[
    {
        "id": "authors:k96m5-hfp79",
        "collection": "authors",
        "collection_id": "k96m5-hfp79",
        "cite_using_url": "https://authors.library.caltech.edu/records/k96m5-hfp79",
        "type": "article",
        "title": "Turning excitons to the dark side",
        "author": [
            {
                "family_name": "Han",
                "given_name": "Yuchen",
                "orcid": "0000-0002-9636-7127",
                "clpid": "Han-Yuchen"
            },
            {
                "family_name": "Hsieh",
                "given_name": "David",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            }
        ],
        "abstract": "Hubbard excitons capture the many-body correlations of Mott insulators. Using ultrafast light, their quantum wavefunction can be coherently rotated, opening a path towards optical quantum control and sensing in strongly correlated materials.",
        "doi": "10.1038/s41563-026-02577-8",
        "issn": "1476-1122",
        "publisher": "Nature Publishing Group",
        "publication": "Nature Materials",
        "publication_date": "2026-06",
        "volume": "25",
        "pages": "887-888"
    },
    {
        "id": "authors:8s0zb-96h09",
        "collection": "authors",
        "collection_id": "8s0zb-96h09",
        "cite_using_url": "https://authors.library.caltech.edu/records/8s0zb-96h09",
        "type": "article",
        "title": "2D van der Waals magnets: From fundamental physics to\u00a0applications",
        "author": [
            {
                "family_name": "Park",
                "given_name": "Je-Geun",
                "orcid": "0000-0002-3930-4226"
            },
            {
                "family_name": "Zhang",
                "given_name": "Kai-Xuan",
                "orcid": "0000-0002-9958-6018"
            },
            {
                "family_name": "Cheong",
                "given_name": "Hyeonsik",
                "orcid": "0000-0002-2347-4044"
            },
            {
                "family_name": "Kim",
                "given_name": "Jae Hoon",
                "orcid": "0000-0002-7840-3630"
            },
            {
                "family_name": "Belvin",
                "given_name": "Carina A.",
                "orcid": "0000-0002-6540-1185",
                "clpid": "Belvin-Carina-A"
            },
            {
                "family_name": "Hsieh",
                "given_name": "David",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            },
            {
                "family_name": "Ning",
                "given_name": "Honglie"
            },
            {
                "family_name": "Gedik",
                "given_name": "Nuh",
                "orcid": "0000-0002-6394-4987"
            }
        ],
        "abstract": "<p>Magnetism has played a central role in the long and rich history of modern condensed matter physics, with many foundational insights originating from theoretical studies of two-dimensional (2D) spin systems. The discovery of 2D van der Waals (vdW) magnets has revolutionized this area by providing real, atomically thin magnetic systems for experimental investigation. Since the first experimental reports of antiferromagnetic vdW insulators in 2016&mdash;followed by studies on ferromagnetic vdW systems in 2017&mdash;the field has witnessed rapid and expansive growth, with more than two dozen vdW magnetic materials now identified, including both ferromagnets and antiferromagnets. This review presents a comprehensive overview of the major scientific and technological developments in this rapidly evolving field. These developments include experimental realizations of various 2D spin Hamiltonians, as well as unexpected phenomena such as magnetic excitons, Floquet-engineered states, and light-induced metastable magnetic phases. In parallel, 2D vdW magnets have shown significant promise in spintronics and related applications, offering a new platform for engineering quantum functionalities. This review traces the historical development of the field, synthesizes key milestones, and highlights its broader impact across condensed matter physics and materials science. The review concludes by outlining several promising directions for future research, charting a path forward in this vibrant and still rapidly growing area.</p>",
        "doi": "10.1103/2pff-xy6n",
        "issn": "0034-6861",
        "publisher": "American Physical Society",
        "publication": "Reviews of Modern Physics",
        "publication_date": "2026-05-27",
        "series_number": "2",
        "volume": "98",
        "issue": "2",
        "pages": "025003"
    },
    {
        "id": "authors:q07d1-z4w79",
        "collection": "authors",
        "collection_id": "q07d1-z4w79",
        "cite_using_url": "https://authors.library.caltech.edu/records/q07d1-z4w79",
        "type": "article",
        "title": "High-speed antiferromagnetic domain walls driven by coherent spin waves",
        "author": [
            {
                "family_name": "Seyler",
                "given_name": "Kyle L.",
                "orcid": "0000-0003-1553-4518",
                "clpid": "Seyler-Kyle-L"
            },
            {
                "family_name": "Zhang",
                "given_name": "Hantao",
                "orcid": "0000-0001-6281-6708"
            },
            {
                "family_name": "Van Beveren",
                "given_name": "Daniel"
            },
            {
                "family_name": "Rotundu",
                "given_name": "Costel R.",
                "orcid": "0000-0002-1571-8352"
            },
            {
                "family_name": "Lee",
                "given_name": "Young S.",
                "orcid": "0000-0002-7022-8313"
            },
            {
                "family_name": "Cheng",
                "given_name": "Ran",
                "orcid": "0000-0003-0166-2172"
            },
            {
                "family_name": "Hsieh",
                "given_name": "David",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            }
        ],
        "abstract": "<p>The ability to rapidly manipulate domain walls in magnetic materials is key to developing novel high-speed spintronic memory and computing devices. Antiferromagnetic materials present a particularly promising platform due to their robustness against stray fields and their potential for exceptional domain wall velocities. Among various proposed driving mechanisms, coherent spin waves could potentially propel antiferromagnetic domain walls to the magnon group velocity while minimizing dissipation from Joule heating. However, experimental realization has remained elusive due to the dual challenges of generating coherent antiferromagnetic spin waves near isolated mobile antiferromagnetic domain walls and simultaneously measuring high-speed domain wall dynamics. Here we experimentally realize an approach where ultrafast laser pulses generate coherent spin waves that drive antiferromagnetic domain walls and develop a technique to directly map the spatiotemporal domain wall dynamics. Using the room-temperature antiferromagnetic insulator Sr<sub>2</sub>Cu<sub>3</sub>O<sub>4</sub>Cl<sub>2</sub>, we observe antiferromagnetic domain wall motion with record-high velocities up to ~50 km s<sup>&minus;1</sup>. Remarkably, the direction of domain wall propagation is controllable through both the pump laser helicity and the sign of the domain wall winding number. This bidirectional control can be theoretically explained, and numerically reproduced, by the domain wall dynamics induced by coherent spin waves of the in-plane magnon mode&mdash;a phenomenon unique to magnets with an easy-plane anisotropy. Our work uncovers a novel domain wall propulsion mechanism that is generalizable to a wide range of antiferromagnetic materials, unlocking new opportunities for ultrafast coherent antiferromagnetic spintronics.</p>",
        "doi": "10.1038/s41467-025-64803-2",
        "issn": "2041-1723",
        "publisher": "Nature Publishing Group",
        "publication": "Nature Communications",
        "publication_date": "2025-11-07",
        "series_number": "1",
        "volume": "16",
        "issue": "1",
        "pages": "9836"
    },
    {
        "id": "authors:9st9q-tx308",
        "collection": "authors",
        "collection_id": "9st9q-tx308",
        "cite_using_url": "https://authors.library.caltech.edu/records/9st9q-tx308",
        "type": "article",
        "title": "Twist-programmable superconductivity in spin\u2013orbit-coupled bilayer graphene",
        "author": [
            {
                "family_name": "Zhang",
                "given_name": "Yiran",
                "orcid": "0000-0002-8477-0074",
                "clpid": "Zhang-Yiran"
            },
            {
                "family_name": "Shavit",
                "given_name": "Gal",
                "orcid": "0000-0003-1792-9249",
                "clpid": "Shavit-Gal"
            },
            {
                "family_name": "Ma",
                "given_name": "Huiyang",
                "orcid": "0009-0000-3028-2668"
            },
            {
                "family_name": "Han",
                "given_name": "Youngjoon",
                "clpid": "Han-Youngjoon"
            },
            {
                "family_name": "Siu",
                "given_name": "Chi Wang",
                "clpid": "Siu-Chi-Wang"
            },
            {
                "family_name": "Mukherjee",
                "given_name": "Ankan",
                "clpid": "Mukherjee-Ankan"
            },
            {
                "family_name": "Watanabe",
                "given_name": "Kenji",
                "orcid": "0000-0003-3701-8119"
            },
            {
                "family_name": "Taniguchi",
                "given_name": "Takashi",
                "orcid": "0000-0002-1467-3105"
            },
            {
                "family_name": "Hsieh",
                "given_name": "David",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            },
            {
                "family_name": "Lewandowski",
                "given_name": "Cyprian",
                "orcid": "0000-0002-6944-9805"
            },
            {
                "family_name": "von Oppen",
                "given_name": "Felix",
                "orcid": "0000-0002-2537-7256"
            },
            {
                "family_name": "Oreg",
                "given_name": "Yuval",
                "orcid": "0000-0001-8753-8468"
            },
            {
                "family_name": "Nadj-Perge",
                "given_name": "Stevan",
                "orcid": "0000-0002-2394-9070",
                "clpid": "Nadj-Perge-S"
            }
        ],
        "abstract": "<p>The relative twist angle between layers of near-lattice-matched van der Waals materials is critical for the emergent phenomena associated with moir&eacute; flat bands. However, the concept of angle rotation control is not exclusive to moir&eacute; superlattices in which electrons directly experience a twist-angle-dependent periodic potential. Instead, it can also be used to induce programmable symmetry-breaking perturbations with the goal of stabilizing desired correlated states. Here we experimentally demonstrate 'moir&eacute;less' twist-tuning of superconductivity together with other correlated orders in Bernal bilayer graphene proximitized by tungsten diselenide. The precise alignment between the two materials systematically controls the strength of induced Ising spin&ndash;orbit coupling (SOC), profoundly altering the phase diagram. As Ising SOC is increased, superconductivity onsets at a higher displacement field and features a higher critical temperature, reaching up to 0.5&thinsp;K. Within the main superconducting dome and in the strong Ising SOC limit, we find an unusual phase transition characterized by a nematic redistribution of holes among trigonally warped Fermi pockets and enhanced resilience to in-plane magnetic fields. The superconducting behaviour is theoretically compatible with the prominent role of interband interactions between symmetry-breaking Fermi pockets. Moreover, we identify two additional superconducting regions, one of which descends from an inter-valley coherent normal state and shows a Pauli-limit violation ratio exceeding 40, among the highest for all known superconductors. Our results provide insights into ultraclean graphene superconductors and underscore the potential of utilizing moir&eacute;less-twist engineering across a wide range of van der Waals heterostructures.</p>",
        "doi": "10.1038/s41586-025-08959-3",
        "issn": "0028-0836",
        "publisher": "Nature Publishing Group",
        "publication": "Nature",
        "publication_date": "2025-05-15",
        "series_number": "8063",
        "volume": "641",
        "issue": "8063",
        "pages": "625-631"
    },
    {
        "id": "authors:vej7z-7w929",
        "collection": "authors",
        "collection_id": "vej7z-7w929",
        "cite_using_url": "https://authors.library.caltech.edu/records/vej7z-7w929",
        "type": "article",
        "title": "Time-hidden magnetic order in a multi-orbital Mott insulator",
        "author": [
            {
                "family_name": "Li",
                "given_name": "Xinwei",
                "orcid": "0000-0003-0555-2624",
                "clpid": "Li-Xinwei"
            },
            {
                "family_name": "Esin",
                "given_name": "Iliya",
                "orcid": "0000-0003-2959-0617",
                "clpid": "Esin-Iliya"
            },
            {
                "family_name": "Han",
                "given_name": "Youngjoon",
                "clpid": "Han-Youngjoon"
            },
            {
                "family_name": "Liu",
                "given_name": "Yincheng",
                "orcid": "0000-0002-0283-5111",
                "clpid": "Liu-Yincheng"
            },
            {
                "family_name": "Zhao",
                "given_name": "Hengdi",
                "orcid": "0000-0003-4606-6323"
            },
            {
                "family_name": "Ning",
                "given_name": "Honglie",
                "orcid": "0000-0003-4867-0751",
                "clpid": "Ning-Honglie"
            },
            {
                "family_name": "Barrett",
                "given_name": "Cora"
            },
            {
                "family_name": "Shan",
                "given_name": "Jun-Yi",
                "orcid": "0000-0001-7665-2169",
                "clpid": "Shan-Jun-Yi"
            },
            {
                "family_name": "Seyler",
                "given_name": "Kyle",
                "orcid": "0000-0003-1553-4518",
                "clpid": "Seyler-Kyle"
            },
            {
                "family_name": "Cao",
                "given_name": "Gang",
                "orcid": "0000-0001-9779-430X"
            },
            {
                "family_name": "Refael",
                "given_name": "Gil",
                "orcid": "0009-0007-4566-8441",
                "clpid": "Refael-G"
            },
            {
                "family_name": "Hsieh",
                "given_name": "David",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            }
        ],
        "abstract": "Photo-excited quantum materials can be driven into thermally inaccessible metastable states that exhibit structural, charge, spin, topological and superconducting orders. Metastable states typically emerge on timescales set by the intrinsic electronic and phononic energy scales, ranging from femtoseconds to picoseconds, and can persist for weeks. Therefore, studies have primarily focused on ultrafast or quasi-static limits, leaving the intermediate time window less explored. Here we reveal a metastable state with broken glide-plane symmetry in photo-doped Ca2RuO4 using time-resolved optical second-harmonic generation and birefringence measurements. We find that the metastable state appears long after intralayer antiferromagnetic order has melted and photo-carriers have recombined. Its properties are distinct from all known states in the equilibrium phase diagram and are consistent with intralayer ferromagnetic order. Furthermore, model Hamiltonian calculations reveal that a non-thermal trajectory to this state can be accessed via photo-doping. Our results expand the search space for out-of-equilibrium electronic matter to metastable states emerging at intermediate timescales.",
        "doi": "10.1038/s41567-024-02752-1",
        "issn": "1745-2473",
        "publisher": "Nature Publishing Group",
        "publication": "Nature Physics",
        "publication_date": "2025-03",
        "volume": "21",
        "pages": "451\u2013457"
    },
    {
        "id": "authors:swxwr-smz38",
        "collection": "authors",
        "collection_id": "swxwr-smz38",
        "cite_using_url": "https://authors.library.caltech.edu/records/swxwr-smz38",
        "type": "article",
        "title": "Observation of excitons bound by antiferromagnetic correlations",
        "author": [
            {
                "family_name": "Mehio",
                "given_name": "Omar",
                "orcid": "0000-0001-7923-2178",
                "clpid": "Mehio-Omar"
            },
            {
                "family_name": "Han",
                "given_name": "Yuchen",
                "orcid": "0000-0002-9636-7127",
                "clpid": "Han-Yuchen"
            },
            {
                "family_name": "Li",
                "given_name": "Xinwei",
                "orcid": "0000-0003-0555-2624",
                "clpid": "Li-Xinwei"
            },
            {
                "family_name": "Ning",
                "given_name": "Honglie",
                "orcid": "0000-0003-4867-0751",
                "clpid": "Ning-Honglie"
            },
            {
                "family_name": "Porter",
                "given_name": "Zach",
                "orcid": "0000-0002-2945-9558"
            },
            {
                "family_name": "Wilson",
                "given_name": "Stephen D.",
                "orcid": "0000-0003-3733-930X"
            },
            {
                "family_name": "Hsieh",
                "given_name": "David",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            }
        ],
        "abstract": "<p>Two-dimensional Mott insulators host antiferromagnetic (AFM) correlations that are predicted to enhance the attractive interaction between empty (holons) and doubly occupied (doublons) sites, creating a novel pathway for exciton formation. However, experimental confirmation of this spin-mediated binding mechanism remains elusive. Leveraging the distinct magnetic critical properties of the Mott antiferromagnets Sr\u2082\u2062IrO\u2084 and Sr\u2083Ir\u2082\u2062O\u2087, we show using time-resolved THz spectroscopy that excitons exist only at temperatures below where short-range AFM correlation develops. The excitons remain stable up to photodoping densities approaching the predicted excitonic Mott insulator-to-metal transition, revealing a unique robustness against screening. Our results establish the viability of spin-bound excitons and introduce opportunities for excitonic control through magnetic degrees of freedom.</p>",
        "doi": "10.1103/physrevresearch.7.013114",
        "issn": "2643-1564",
        "publisher": "American Physical Society",
        "publication": "Physical Review Research",
        "publication_date": "2025-01-30",
        "series_number": "1",
        "volume": "7",
        "issue": "1",
        "pages": "013114"
    },
    {
        "id": "authors:p9xn7-cdb83",
        "collection": "authors",
        "collection_id": "p9xn7-cdb83",
        "cite_using_url": "https://authors.library.caltech.edu/records/p9xn7-cdb83",
        "type": "article",
        "title": "Dynamic magnetic phase transition induced by parametric magnon pumping",
        "author": [
            {
                "family_name": "Shan",
                "given_name": "Jun-Yi",
                "orcid": "0000-0001-7665-2169",
                "clpid": "Shan-Jun-Yi"
            },
            {
                "family_name": "Curtis",
                "given_name": "Jonathan B.",
                "orcid": "0000-0001-8544-0555",
                "clpid": "Curtis-Jonathan-B"
            },
            {
                "family_name": "Guo",
                "given_name": "Mingyao",
                "orcid": "0000-0003-1109-2548",
                "clpid": "Guo-Mingyao"
            },
            {
                "family_name": "Roh",
                "given_name": "Chang Jae",
                "orcid": "0009-0009-0369-0311",
                "clpid": "Roh-Chang-Jae"
            },
            {
                "family_name": "Rotundu",
                "given_name": "C. R.",
                "orcid": "0000-0002-1571-8352",
                "clpid": "Rotundu-Costel-R"
            },
            {
                "family_name": "Lee",
                "given_name": "Young S.",
                "clpid": "Lee-Young-S"
            },
            {
                "family_name": "Narang",
                "given_name": "Prineha",
                "orcid": "0000-0003-3956-4594",
                "clpid": "Narang-Prineha"
            },
            {
                "family_name": "Noh",
                "given_name": "Tae Won",
                "orcid": "0000-0003-1905-2321",
                "clpid": "Noh-Tae-Won"
            },
            {
                "family_name": "Demler",
                "given_name": "Eugene",
                "orcid": "0000-0002-2499-632X",
                "clpid": "Demler-Eugene"
            },
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            }
        ],
        "abstract": "<p>Uncovering pathways to optically drive magnetic order-disorder transitions on ultrashort timescales can lead to the realization of novel out-of-equilibrium quantum phenomena. A long-sought pathway is to directly excite a highly nonthermal energy-momentum distribution of magnons, bypassing both charge and lattice degrees of freedom. However, this remains elusive owing to the weak coupling and large momentum mismatch between photons and magnons. Here we demonstrate strong parametric excitation of magnons across the entire Brillouin zone of the antiferromagnetic insulator&nbsp;<span><span><span><span><span><span><span><span>Sr\u2082</span></span></span></span><span><span><span><span>Cu\u2083</span></span></span></span><span><span><span><span>O\u2084</span></span></span></span><span><span><span><span>Cl</span></span></span><span><span><span>\u2082</span></span></span></span></span></span></span></span>&nbsp;by periodically modulating the superexchange interaction with the electric field of light. The excitation efficiency is greatly enhanced by tuning to the van Hove singularity in the magnon spectrum, sufficient to transiently collapse the antiferromagnetic state using a pulsed laser field of&nbsp;<span><span><span><span><span><span><span>10\u2079</span></span></span></span></span></span></span>&nbsp;V/m. The order parameter recovery timescale increases by over 1000 times as a function of excitation density, reflecting a crossover from high- to low-energy magnon dominated decay dynamics. This electric-field induced parametric magnon pumping mechanism is applicable to a broad range of magnetic insulators and opens up the possibility of dynamically engineering magnon distributions by design.</p>",
        "doi": "10.1103/physrevb.109.054302",
        "issn": "2469-9950",
        "publisher": "American Physical Society",
        "publication": "Physical Review B",
        "publication_date": "2024-02-01",
        "series_number": "5",
        "volume": "109",
        "issue": "5",
        "pages": "054302"
    },
    {
        "id": "authors:xzrcg-q7w19",
        "collection": "authors",
        "collection_id": "xzrcg-q7w19",
        "cite_using_url": "https://authors.library.caltech.edu/records/xzrcg-q7w19",
        "type": "article",
        "title": "Nonlinear and Nonreciprocal Transport Effects in Untwinned Thin Films of Ferromagnetic Weyl Metal SrRuO\u2083",
        "author": [
            {
                "family_name": "Kar",
                "given_name": "Uddipta",
                "clpid": "Kar-Uddipta"
            },
            {
                "family_name": "Lu",
                "given_name": "Elisha Cho-Hao",
                "clpid": "Lu-Elisha-Cho-Hao"
            },
            {
                "family_name": "Singh",
                "given_name": "Akhilesh Kr.",
                "clpid": "Singh-Akhilesh-Kr"
            },
            {
                "family_name": "Reddy",
                "given_name": "P.\u2009V. Sreenivasa",
                "orcid": "0000-0003-1460-342X",
                "clpid": "Peram-Venkata-Sreenivasa-Reddy"
            },
            {
                "family_name": "Han",
                "given_name": "Youngjoon",
                "orcid": "0000-0003-1256-9328",
                "clpid": "Han-Youngjoon"
            },
            {
                "family_name": "Li",
                "given_name": "Xinwei",
                "clpid": "Li-Xinwei"
            },
            {
                "family_name": "Cheng",
                "given_name": "Cheng-Tung",
                "orcid": "0000-0002-9117-5783",
                "clpid": "Cheng-Cheng-Tung"
            },
            {
                "family_name": "Yang",
                "given_name": "Song",
                "orcid": "0000-0003-4296-8856",
                "clpid": "Yang-Song"
            },
            {
                "family_name": "Lin",
                "given_name": "Chun-Yen",
                "orcid": "0000-0002-5083-9256",
                "clpid": "Lin-Chun-Yen"
            },
            {
                "family_name": "Cheng",
                "given_name": "I-Chun",
                "orcid": "0000-0003-2209-3298",
                "clpid": "Cheng-I-Chun"
            },
            {
                "family_name": "Hsu",
                "given_name": "Chia-Hung",
                "orcid": "0009-0002-7087-4718",
                "clpid": "Hsu-Chia-Hung"
            },
            {
                "family_name": "Hsieh",
                "given_name": "David",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            },
            {
                "family_name": "Lee",
                "given_name": "Wei-Cheng",
                "orcid": "0000-0002-6140-6448",
                "clpid": "Lee-Wei-Cheng"
            },
            {
                "family_name": "Guo",
                "given_name": "Guang-Yu",
                "orcid": "0000-0003-3097-0916",
                "clpid": "Guo-Guang-Yu"
            },
            {
                "family_name": "Lee",
                "given_name": "Wei-Li",
                "orcid": "0000-0001-7207-1607",
                "clpid": "Lee-Wei-Li"
            }
        ],
        "abstract": "<p>The identification of distinct charge transport features, deriving from nontrivial bulk band and surface states, has been a challenging subject in the field of topological systems. In topological Dirac and Weyl semimetals, nontrivial conical bands with Fermi-arc surface states give rise to negative longitudinal magnetoresistance due to chiral anomaly effect and unusual thickness dependent quantum oscillation from Weyl-orbit effect, which were demonstrated recently in experiments. In this work, we report the experimental observations of large nonlinear and nonreciprocal transport effects for both longitudinal and transverse channels in an untwinned Weyl metal of&nbsp;<span><span><span><span><span><span><span><span><span>SrRuO\u2083</span></span></span></span></span></span></span></span></span>&nbsp;thin film grown on a&nbsp;<span><span><span><span><span><span><span><span><span>SrTiO\u2083</span></span></span></span></span></span></span></span></span>&nbsp;substrate. From rigorous measurements with bias current applied along various directions with respect to the crystalline principal axes, the magnitude of nonlinear Hall signals from the transverse channel exhibits a simple&nbsp;<span><span><span><span><span><span>sin</span></span><span><span>&alpha;</span></span></span></span></span></span>&nbsp;dependence at low temperatures, where&nbsp;<span><span><span><span><span>&alpha;</span></span></span></span></span>&nbsp;is the angle between bias current direction and orthorhombic&nbsp;<span><span><span><span><span><span>[</span></span><span><span>001</span></span><span><span><span><span><span>]</span></span></span></span><span><span><span><span>\u2092</span></span></span></span></span></span></span></span></span>, reaching a maximum when current is along orthorhombic&nbsp;<span><span><span><span><span><span>[</span></span><span><span>1</span></span><span><span><span><span><span><span>&macr;</span></span></span></span><span><span><span><span>1</span></span></span></span></span></span><span><span>0</span></span><span><span><span><span><span>]\u2092</span></span></span></span></span></span></span></span></span>. On the contrary, the magnitude of nonlinear and nonreciprocal signals in the longitudinal channel attains a maximum for bias current along&nbsp;<span><span><span><span><span><span>[</span></span><span><span>001</span></span><span><span><span><span><span>]</span></span></span></span><span><span><span><span>o</span></span></span></span></span></span></span></span></span>, and it vanishes for bias current along&nbsp;<span><span><span><span><span><span>[</span></span><span><span>1</span></span><span><span><span><span><span><span>&macr;</span></span></span></span><span><span><span><span>1</span></span></span></span></span></span><span><span>0</span></span><span><span><span><span><span>]<span><span><span><span>\u2092</span></span></span></span></span></span></span></span></span></span></span></span></span>. The observed&nbsp;<span><span><span><span><span>&alpha;</span></span></span></span></span>-dependent nonlinear and nonreciprocal signals in longitudinal and transverse channels reveal a magnetic Weyl phase with an effective Berry curvature dipole along&nbsp;<span><span><span><span><span><span>[</span></span><span><span>1</span></span><span><span><span><span><span><span>&macr;</span></span></span></span><span><span><span><span>1</span></span></span></span></span></span><span><span>0</span></span><span><span><span><span><span>]\u2092</span></span></span></span></span></span></span></span></span>&nbsp;from surface states, accompanied by 1D chiral edge modes along&nbsp;<span><span><span><span><span><span>[</span></span><span><span>001</span></span><span><span><span><span><span>]</span></span></span></span><span><span><span><span>\u2092</span></span></span></span></span></span></span></span></span>.</p>",
        "doi": "10.1103/physrevx.14.011022",
        "issn": "2160-3308",
        "publisher": "American Physical Society",
        "publication": "Physical Review X",
        "publication_date": "2024-01",
        "series_number": "1",
        "volume": "14",
        "issue": "1",
        "pages": "011022"
    },
    {
        "id": "authors:b8j5v-rrk37",
        "collection": "authors",
        "collection_id": "b8j5v-rrk37",
        "cite_using_url": "https://authors.library.caltech.edu/records/b8j5v-rrk37",
        "type": "article",
        "title": "A coherent phonon-induced hidden quadrupolar ordered state in Ca\u2082RuO\u2084",
        "author": [
            {
                "family_name": "Ning",
                "given_name": "Honglie",
                "orcid": "0000-0003-4867-0751",
                "clpid": "Ning-Honglie"
            },
            {
                "family_name": "Mehio",
                "given_name": "Omar",
                "orcid": "0000-0001-7923-2178",
                "clpid": "Mehio-Omar"
            },
            {
                "family_name": "Li",
                "given_name": "Xinwei",
                "orcid": "0000-0003-0555-2624",
                "clpid": "Li-Xinwei"
            },
            {
                "family_name": "Buchhold",
                "given_name": "Michael",
                "orcid": "0000-0001-5194-9388",
                "clpid": "Buchhold-Michael"
            },
            {
                "family_name": "Driesse",
                "given_name": "Mathias",
                "orcid": "0000-0002-3983-5852",
                "clpid": "Driesse-Mathias"
            },
            {
                "family_name": "Zhao",
                "given_name": "Hengdi",
                "orcid": "0000-0003-4606-6323",
                "clpid": "Zhao-Hengdi"
            },
            {
                "family_name": "Cao",
                "given_name": "Gang",
                "orcid": "0000-0001-9779-430X",
                "clpid": "Cao-Gang"
            },
            {
                "family_name": "Hsieh",
                "given_name": "David",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            }
        ],
        "abstract": "<p>AbstractUltrafast laser excitation provides a means to transiently realize long-range ordered electronic states of matter that are hidden in thermal equilibrium. Recently, this approach has unveiled a variety of thermally inaccessible ordered states in strongly correlated materials, including charge density wave, ferroelectric, magnetic, and intertwined charge-orbital ordered states. However, more exotic hidden states exhibiting higher multipolar ordering remain elusive owing to the challenge of directly manipulating and detecting them with light. Here we demonstrate a method to induce a dynamical transition from a thermally allowed to a thermally forbidden spin-orbit entangled quadrupolar ordered state in Ca\u2082RuO\u2084 by coherently exciting a phonon that is strongly coupled to the order parameter. Combining probe photon energy-resolved coherent phonon spectroscopy measurements with model Hamiltonian calculations, we show that the dynamical transition is manifested through anomalies in the temperature, pump excitation fluence, and probe photon energy dependence of the strongly coupled phonon. With this procedure, we introduce a general pathway to uncover hidden multipolar ordered states and to control their re-orientation on ultrashort timescales.</p>",
        "doi": "10.1038/s41467-023-44021-4",
        "issn": "2041-1723",
        "publisher": "Nature Publishing Group",
        "publication": "Nature Communications",
        "publication_date": "2023-12-13",
        "volume": "14",
        "pages": "8258"
    },
    {
        "id": "authors:8v2db-dxg10",
        "collection": "authors",
        "collection_id": "8v2db-dxg10",
        "cite_using_url": "https://authors.library.caltech.edu/records/8v2db-dxg10",
        "type": "article",
        "title": "Transforming a strain-stabilized ferroelectric into an intrinsic polar metal with light",
        "author": [
            {
                "family_name": "Ron",
                "given_name": "Alon",
                "orcid": "0000-0002-1840-7824",
                "clpid": "Ron-Alon"
            },
            {
                "family_name": "Ahadi",
                "given_name": "Kaveh",
                "orcid": "0000-0003-2280-4037",
                "clpid": "Ahadi-Kaveh"
            },
            {
                "family_name": "Hickox-Young",
                "given_name": "Daniel",
                "orcid": "0000-0002-5411-0497",
                "clpid": "Hickox-Young-Daniel"
            },
            {
                "family_name": "Puggioni",
                "given_name": "Danilo",
                "orcid": "0000-0002-2128-4191",
                "clpid": "Puggioni-Danilo"
            },
            {
                "family_name": "Mehio",
                "given_name": "Omar",
                "orcid": "0000-0001-7923-2178",
                "clpid": "Mehio-Omar"
            },
            {
                "family_name": "Rondinelli",
                "given_name": "James M.",
                "orcid": "0000-0003-0508-2175",
                "clpid": "Rondinelli-James-M"
            },
            {
                "family_name": "Stemmer",
                "given_name": "Susanne",
                "orcid": "0000-0002-3142-4696",
                "clpid": "Stemmer-Susanne"
            },
            {
                "family_name": "Hsieh",
                "given_name": "David",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            }
        ],
        "abstract": "<p>We explore the effects of chemical doping and photodoping in the strain-induced multiferroic&nbsp;<span><span><span><span><span><span><span>EuTiO\u2083</span></span></span></span></span></span></span>&nbsp;grown on&nbsp;<span><span><span><span><span><span><span>DyScO</span></span></span><span><span><span>\u2083</span></span></span></span></span></span></span>&nbsp;substrates. The polar order is probed experimentally using second harmonic generation (SHG) and modeled using&nbsp;<em>ab initio</em>&nbsp;calculations. At low photodoping concentrations, we observe a reduction in SHG signal, indicating a destructive coupling between charge carriers and polar order in accordance with our simulations and expectations for a second-order Jahn-Teller driven ferroelectric. However, under increased photodoping the reduction in SHG plateaus at 84% of its original magnitude, indicating resilience of the polar order in the presence of a high concentration of delocalized electrons. This behavior stands in contrast with our first-principles simulations, indicating that&nbsp;<span><span><span><span><span><span><span>EuTiO\u2083</span></span></span></span></span></span></span>&nbsp;undergoes a transition from ferroelectric to polar metallic character under photodoping. We suggest several hypotheses for the mechanism behind this change in distortion character.</p>",
        "doi": "10.1103/physrevb.108.224308",
        "issn": "2469-9950",
        "publisher": "American Physical Society",
        "publication": "Physical Review B",
        "publication_date": "2023-12-01",
        "series_number": "22",
        "volume": "108",
        "issue": "22",
        "pages": "224308"
    },
    {
        "id": "authors:f2wj0-p4753",
        "collection": "authors",
        "collection_id": "f2wj0-p4753",
        "cite_using_url": "https://authors.library.caltech.edu/records/f2wj0-p4753",
        "type": "article",
        "title": "A Hubbard exciton fluid in a photo-doped antiferromagnetic Mott insulator",
        "author": [
            {
                "family_name": "Mehio",
                "given_name": "Omar",
                "orcid": "0000-0001-7923-2178",
                "clpid": "Mehio-Omar"
            },
            {
                "family_name": "Li",
                "given_name": "Xinwei",
                "orcid": "0000-0003-0555-2624",
                "clpid": "Li-Xinwei"
            },
            {
                "family_name": "Ning",
                "given_name": "Honglie",
                "orcid": "0000-0003-4867-0751",
                "clpid": "Ning-Honglie"
            },
            {
                "family_name": "Lenar\u010di\u010d",
                "given_name": "Zala",
                "orcid": "0000-0001-8374-8011",
                "clpid": "Lenar\u010di\u010d-Zala"
            },
            {
                "family_name": "Han",
                "given_name": "Yuchen",
                "orcid": "0000-0002-9636-7127",
                "clpid": "Han-Yuchen"
            },
            {
                "family_name": "Buchhold",
                "given_name": "Michael",
                "orcid": "0000-0001-5194-9388",
                "clpid": "Buchhold-Michael"
            },
            {
                "family_name": "Porter",
                "given_name": "Zach",
                "orcid": "0000-0002-2945-9558",
                "clpid": "Porter-Zach"
            },
            {
                "family_name": "Laurita",
                "given_name": "Nicholas J.",
                "orcid": "0000-0002-7794-7951",
                "clpid": "Laurita-Nicholas-J"
            },
            {
                "family_name": "Wilson",
                "given_name": "Stephen D.",
                "orcid": "0000-0003-3733-930X",
                "clpid": "Wilson-Stephen-D"
            },
            {
                "family_name": "Hsieh",
                "given_name": "David",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            }
        ],
        "abstract": "<div>\n<div>\n<p>The undoped antiferromagnetic Mott insulator naturally has one charge carrier per lattice site. When it is doped with additional carriers, they are unstable to spin-fluctuation-mediated Cooper pairing as well as other unconventional types of charge, spin and orbital current ordering. Photo-excitation can produce charge carriers in the form of empty (holons) and doubly occupied (doublons) sites that may also exhibit charge instabilities. There is evidence that antiferromagnetic correlations enhance attractive interactions between holons and doublons, which can then form bound pairs known as Hubbard excitons, and that these might self-organize into an insulating Hubbard exciton fluid. However, this out-of-equilibrium phenomenon has not been experimentally detected. Here we report the transient formation of a Hubbard exciton fluid in the antiferromagnetic Mott insulator Sr<sub>2</sub>IrO<sub>4</sub> using ultrafast terahertz conductivity. Following photo-excitation, we observe rapid spectral-weight transfer from a Drude metallic response to an insulating response. The latter is characterized by a finite-energy peak originating from intraexcitonic transitions, whose assignment is corroborated by our numerical simulations of an extended Hubbard model. The lifetime of the peak is short (approximately one picosecond) and scales exponentially with the Mott gap size, implying extremely strong coupling to magnon modes.</p>\n</div>\n</div>",
        "doi": "10.1038/s41567-023-02204-2",
        "issn": "1745-2473",
        "publisher": "Nature Publishing Group",
        "publication": "Nature Physics",
        "publication_date": "2023-12",
        "series_number": "12",
        "volume": "19",
        "issue": "12",
        "pages": "1876-1882"
    },
    {
        "id": "authors:qsbag-6ss50",
        "collection": "authors",
        "collection_id": "qsbag-6ss50",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20221202-906480600.4",
        "type": "article",
        "title": "Light-induced Weyl semiconductor-to-metal transition mediated by Peierls instability",
        "author": [
            {
                "family_name": "Ning",
                "given_name": "Honglie",
                "orcid": "0000-0003-4867-0751",
                "clpid": "Ning-Honglie"
            },
            {
                "family_name": "Mehio",
                "given_name": "Omar",
                "clpid": "Mehio-Omar"
            },
            {
                "family_name": "Lian",
                "given_name": "Chao",
                "clpid": "Lian-Chao"
            },
            {
                "family_name": "Li",
                "given_name": "Xinwei",
                "orcid": "0000-0003-0555-2624",
                "clpid": "Li-Xinwei"
            },
            {
                "family_name": "Zoghlin",
                "given_name": "Eli",
                "orcid": "0000-0002-8160-584X",
                "clpid": "Zoghlin-Eli"
            },
            {
                "family_name": "Zhou",
                "given_name": "Preston",
                "clpid": "Zhou-Preston"
            },
            {
                "family_name": "Cheng",
                "given_name": "Bryan",
                "orcid": "0000-0003-1787-0240",
                "clpid": "Cheng-Bryan"
            },
            {
                "family_name": "Wilson",
                "given_name": "Stephen D.",
                "orcid": "0000-0003-3733-930X",
                "clpid": "Wilson-Stephen-D"
            },
            {
                "family_name": "Wong",
                "given_name": "Bryan M.",
                "orcid": "0000-0002-3477-8043",
                "clpid": "Wong-Bryan-M"
            },
            {
                "family_name": "Hsieh",
                "given_name": "David",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            }
        ],
        "abstract": "Elemental tellurium is a strongly spin-orbit coupled Peierls-distorted semiconductor whose band structure features topologically protected Weyl nodes. Using time-dependent density functional theory calculations, we show that impulsive optical excitation can be used to transiently control the amplitude of the Peierls distortion, realizing a mechanism to switch tellurium between three states: Weyl semiconductor, Weyl metal, and non-Weyl metal. Further, we present experimental evidence of this inverse Peierls distortion using time-resolved optical second harmonic generation measurements. These results provide a pathway to multifunctional ultrafast Weyl devices and introduce Peierls systems as viable hosts of light-induced topological transitions.",
        "doi": "10.1103/physrevb.106.205118",
        "issn": "2469-9950",
        "publisher": "American Physical Society",
        "publication": "Physical Review B",
        "publication_date": "2022-11-15",
        "series_number": "20",
        "volume": "106",
        "issue": "20",
        "pages": "Art. No. 205118"
    },
    {
        "id": "authors:42dpf-6vn98",
        "collection": "authors",
        "collection_id": "42dpf-6vn98",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20221104-609510400.4",
        "type": "article",
        "title": "Direct visualization and control of antiferromagnetic domains and spin reorientation in a parent cuprate",
        "author": [
            {
                "family_name": "Seyler",
                "given_name": "K. L.",
                "orcid": "0000-0003-1553-4518",
                "clpid": "Seyler-Kyle-L"
            },
            {
                "family_name": "Ron",
                "given_name": "A.",
                "orcid": "0000-0002-1840-7824",
                "clpid": "Ron-Alon"
            },
            {
                "family_name": "Van Beveren",
                "given_name": "D.",
                "clpid": "Van-Beveren-Daniel"
            },
            {
                "family_name": "Rotundu",
                "given_name": "C. R.",
                "orcid": "0000-0002-1571-8352",
                "clpid": "Rotundu-Costel-R"
            },
            {
                "family_name": "Lee",
                "given_name": "Y. S.",
                "clpid": "Lee-Young-Sang"
            },
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            }
        ],
        "abstract": "We report magnetic optical second-harmonic generation (SHG) polarimetry and imaging on Sr\u2082Cu\u2083O\u2084Cl\u2082, which allows direct visualization of the mesoscopic antiferromagnetic (AFM) structure of a parent cuprate. Temperature- and magnetic-field-dependent SHG reveals large domains with 90\u00b0 relative orientations that are stabilized by a combination of uniaxial magnetic anisotropy and the Earth's magnetic field. Below a temperature T_R \u223c 97 K, we observe an unusual 90\u00b0 spin-reorientation transition, possibly driven by competing magnetic anisotropies of the two copper sublattices, which swaps the AFM domain states while preserving the domain structure. This allows deterministic switching of the AFM states by thermal or laser heating. Near T_R, the domain walls become exceptionally responsive to an applied magnetic field, with the Earth's field sufficient to completely expel them from the crystal. Our findings unlock opportunities to study the mesoscopic AFM behavior of parent cuprates and explore their potential for AFM technologies.",
        "doi": "10.1103/physrevb.106.l140403",
        "issn": "2469-9950",
        "publisher": "American Physical Society",
        "publication": "Physical Review B",
        "publication_date": "2022-10-01",
        "series_number": "14",
        "volume": "106",
        "issue": "14",
        "pages": "Art. No. L140403"
    },
    {
        "id": "authors:mfkae-eja11",
        "collection": "authors",
        "collection_id": "mfkae-eja11",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20220705-671865000",
        "type": "article",
        "title": "High-pressure control of optical nonlinearity in the polar Weyl semimetal TaAs",
        "author": [
            {
                "family_name": "Li",
                "given_name": "Chen",
                "orcid": "0000-0001-6750-5925",
                "clpid": "Li-Chen"
            },
            {
                "family_name": "Li",
                "given_name": "Xiang",
                "clpid": "Li-Xiang"
            },
            {
                "family_name": "Deshpande",
                "given_name": "T.",
                "orcid": "0000-0003-0326-1372",
                "clpid": "Deshpande-Tejas"
            },
            {
                "family_name": "Li",
                "given_name": "Xinwei",
                "orcid": "0000-0003-0555-2624",
                "clpid": "Li-Xinwei"
            },
            {
                "family_name": "Nair",
                "given_name": "N.",
                "clpid": "Nair-N"
            },
            {
                "family_name": "Analytis",
                "given_name": "J. G.",
                "orcid": "0000-0002-7657-7688",
                "clpid": "Analytis-James-G"
            },
            {
                "family_name": "Silevitch",
                "given_name": "D. M.",
                "orcid": "0000-0002-6347-3513",
                "clpid": "Silevitch-D-M"
            },
            {
                "family_name": "Rosenbaum",
                "given_name": "T. F.",
                "orcid": "0009-0008-6152-666X",
                "clpid": "Rosenbaum-T-F"
            },
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            }
        ],
        "abstract": "The transition metal monopnictide family of Weyl semimetals recently has been shown to exhibit anomalously strong second-order optical nonlinearity, which is theoretically attributed to a highly asymmetric polarization distribution induced by their polar structure. We experimentally test this hypothesis by measuring optical second harmonic generation (SHG) from TaAs across a pressure-tuned polar-to-nonpolar structural phase transition. Despite the high-pressure structure remaining noncentrosymmetric, the SHG yield is reduced by more than 60% by 20 GPa as compared to the ambient pressure value. By examining the pressure dependence of distinct groups of SHG susceptibility tensor elements, we find that the yield is primarily controlled by a single element that governs the response along the polar axis. Our results confirm a connection between the polar axis and the giant optical nonlinearity of Weyl semimetals and demonstrate pressure as a means to tune this effect in situ.",
        "doi": "10.1103/physrevb.106.014101",
        "issn": "2469-9950",
        "publisher": "American Physical Society",
        "publication": "Physical Review B",
        "publication_date": "2022-07-01",
        "series_number": "1",
        "volume": "106",
        "issue": "1",
        "pages": "Art. No. 014101"
    },
    {
        "id": "authors:b81k8-x0402",
        "collection": "authors",
        "collection_id": "b81k8-x0402",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20220525-286273000",
        "type": "article",
        "title": "Keldysh Space Control of Charge Dynamics in a Strongly Driven Mott Insulator",
        "author": [
            {
                "family_name": "Li",
                "given_name": "Xinwei",
                "orcid": "0000-0003-0555-2624",
                "clpid": "Li-Xinwei"
            },
            {
                "family_name": "Ning",
                "given_name": "Honglie",
                "clpid": "Ning-Honglie"
            },
            {
                "family_name": "Mehio",
                "given_name": "Omar",
                "clpid": "Mehio-Omar"
            },
            {
                "family_name": "Zhao",
                "given_name": "Hengdi",
                "orcid": "0000-0003-4606-6323",
                "clpid": "Zhao-Hengdi"
            },
            {
                "family_name": "Lee",
                "given_name": "Min-Cheol",
                "orcid": "0000-0002-9145-9700",
                "clpid": "Lee-Min-Cheol"
            },
            {
                "family_name": "Kim",
                "given_name": "Kyungwan",
                "orcid": "0000-0003-3833-5378",
                "clpid": "Kim-Kyungwan"
            },
            {
                "family_name": "Nakamura",
                "given_name": "Fumihiko",
                "clpid": "Nakamura-Fumihiko"
            },
            {
                "family_name": "Maeno",
                "given_name": "Yoshiteru",
                "orcid": "0000-0002-3467-9416",
                "clpid": "Maeno-Yoshiteru"
            },
            {
                "family_name": "Cao",
                "given_name": "Gang",
                "orcid": "0000-0001-9779-430X",
                "clpid": "Cao-Gang"
            },
            {
                "family_name": "Hsieh",
                "given_name": "David",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            }
        ],
        "abstract": "The fate of a Mott insulator under strong low frequency optical driving conditions is a fundamental problem in quantum many-body dynamics. Using ultrafast broadband optical spectroscopy, we measured the transient electronic structure and charge dynamics of an off-resonantly pumped Mott insulator Ca\u2082RuO\u2084. We observe coherent bandwidth renormalization and nonlinear doublon-holon pair production occurring in rapid succession within a sub-100-fs pump pulse duration. By sweeping the electric field amplitude, we demonstrate continuous bandwidth tuning and a Keldysh crossover from a multiphoton absorption to quantum tunneling dominated pair production regime. Our results provide a procedure to control coherent and nonlinear heating processes in Mott insulators, facilitating the discovery of novel out-of-equilibrium phenomena in strongly correlated systems.",
        "doi": "10.1103/physrevlett.128.187402",
        "issn": "0031-9007",
        "publisher": "American Physical Society",
        "publication": "Physical Review Letters",
        "publication_date": "2022-05-06",
        "series_number": "18",
        "volume": "128",
        "issue": "18",
        "pages": "Art. No. 187402"
    },
    {
        "id": "authors:fdnnj-y1e72",
        "collection": "authors",
        "collection_id": "fdnnj-y1e72",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20220113-234606083",
        "type": "article",
        "title": "Decoupling of static and dynamic criticality in a driven Mott insulator",
        "author": [
            {
                "family_name": "de la Torre",
                "given_name": "Alberto",
                "orcid": "0000-0002-6751-8205",
                "clpid": "de-la-Torre-Alberto"
            },
            {
                "family_name": "Seyler",
                "given_name": "Kyle L.",
                "orcid": "0000-0003-1553-4518",
                "clpid": "Seyler-Kyle-L"
            },
            {
                "family_name": "Buchhold",
                "given_name": "Michael",
                "orcid": "0000-0001-5194-9388",
                "clpid": "Buchhold-Michael"
            },
            {
                "family_name": "Baum",
                "given_name": "Yuval",
                "orcid": "0000-0003-4631-8551",
                "clpid": "Baum-Yuval"
            },
            {
                "family_name": "Zhang",
                "given_name": "Gufeng",
                "orcid": "0000-0001-8188-2559",
                "clpid": "Zhang-Gu-Feng"
            },
            {
                "family_name": "Laurita",
                "given_name": "Nicholas J.",
                "orcid": "0000-0002-7794-7951",
                "clpid": "Lauriita-Nicholas-J"
            },
            {
                "family_name": "Harter",
                "given_name": "John W.",
                "orcid": "0000-0002-7146-9370",
                "clpid": "Harter-John-W"
            },
            {
                "family_name": "Zhao",
                "given_name": "Liuyan",
                "orcid": "0000-0001-9512-3537",
                "clpid": "Zhao-Liuyan"
            },
            {
                "family_name": "Phinney",
                "given_name": "Isabelle",
                "clpid": "Phinney-Isabelle"
            },
            {
                "family_name": "Chen",
                "given_name": "Xiang",
                "orcid": "0000-0003-3997-8148",
                "clpid": "Chen-Xiang"
            },
            {
                "family_name": "Wilson",
                "given_name": "Stephen D.",
                "orcid": "0000-0003-3733-930X",
                "clpid": "Wilson-Stephen-D"
            },
            {
                "family_name": "Cao",
                "given_name": "Gang",
                "orcid": "0000-0001-9779-430X",
                "clpid": "Cao-Gang"
            },
            {
                "family_name": "Averitt",
                "given_name": "Richard D.",
                "orcid": "0000-0003-0451-1935",
                "clpid": "Averitt-Richard-D"
            },
            {
                "family_name": "Refael",
                "given_name": "Gil",
                "clpid": "Refael-G"
            },
            {
                "family_name": "Hsieh",
                "given_name": "David",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            }
        ],
        "abstract": "Strongly driven antiferromagnetic Mott insulators have the potential to exhibit exotic transient phenomena that are forbidden in thermal equilibrium. However, such far-from-equilibrium regimes, where conventional time-dependent Ginzburg-Landau descriptions fail, are experimentally challenging to prepare and to probe especially in solid state systems. Here we use a combination of time-resolved second harmonic optical polarimetry and coherent magnon spectroscopy to interrogate n-type photo-doping induced ultrafast magnetic order parameter dynamics in the antiferromagnetic Mott insulator Sr\u2082IrO\u2084. We find signatures of an unusual far-from-equilibrium critical regime in which the divergences of the magnetic correlation length and relaxation time are decoupled. This violation of conventional thermal critical behavior arises from the interplay of photo-doping and non-thermal magnon population induced demagnetization effects. Our findings, embodied in a non-equilibrium phase diagram, provide a blueprint for engineering the out-of-equilibrium properties of quantum matter, with potential applications to terahertz spintronics technologies.",
        "doi": "10.1038/s42005-022-00813-6",
        "issn": "2399-3650",
        "publisher": "Nature Publishing Group",
        "publication": "Communications Physics",
        "publication_date": "2022-02-04",
        "volume": "5",
        "pages": "Art. No. 35"
    },
    {
        "id": "authors:kea1a-b9h37",
        "collection": "authors",
        "collection_id": "kea1a-b9h37",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20211209-456366000",
        "type": "article",
        "title": "Giant modulation of optical nonlinearity by Floquet engineering",
        "author": [
            {
                "family_name": "Shan",
                "given_name": "Jun-Yi",
                "orcid": "0000-0001-7665-2169",
                "clpid": "Shan-Jun-Yi"
            },
            {
                "family_name": "Ye",
                "given_name": "M.",
                "clpid": "Ye-M"
            },
            {
                "family_name": "Chu",
                "given_name": "H.",
                "orcid": "0000-0002-1989-9517",
                "clpid": "Chu-Hao"
            },
            {
                "family_name": "Lee",
                "given_name": "Sungmin",
                "clpid": "Lee-Sungmin"
            },
            {
                "family_name": "Park",
                "given_name": "Je-Geun",
                "orcid": "0000-0002-3930-4226",
                "clpid": "Park-Je-Geun"
            },
            {
                "family_name": "Balents",
                "given_name": "L.",
                "orcid": "0000-0002-2377-2711",
                "clpid": "Balents-Leon"
            },
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            }
        ],
        "abstract": "Strong periodic driving with light offers the potential to coherently manipulate the properties of quantum materials on ultrafast timescales. Recently, strategies have emerged to drastically alter electronic and magnetic properties by optically inducing non-trivial band topologies, emergent spin interactions and even superconductivity. However, the prospects and methods of coherently engineering optical properties on demand are far less understood. Here we demonstrate coherent control and giant modulation of optical nonlinearity in a van der Waals layered magnetic insulator, manganese phosphorus trisulfide (MnPS\u2083). By driving far off-resonance from the lowest on-site manganese d\u2013d transition, we observe a coherent on\u2013off switching of its optical second harmonic generation efficiency on the timescale of 100\u2009femtoseconds with no measurable dissipation. At driving electric fields of the order of 10\u2079\u2009volts per metre, the on\u2013off ratio exceeds 10, which is limited only by the sample damage threshold. Floquet theory calculations based on a single-ion model of MnPS\u2083 are able to reproduce the measured driving field amplitude and polarization dependence of the effect. Our approach can be applied to a broad range of insulating materials and could lead to dynamically designed nonlinear optical elements.",
        "doi": "10.1038/s41586-021-04051-8",
        "issn": "0028-0836",
        "publisher": "Nature Publishing Group",
        "publication": "Nature",
        "publication_date": "2021-12-09",
        "series_number": "7888",
        "volume": "600",
        "issue": "7888",
        "pages": "235-239"
    },
    {
        "id": "authors:2z4ad-dps41",
        "collection": "authors",
        "collection_id": "2z4ad-dps41",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20211130-215730151",
        "type": "article",
        "title": "Magnetic order, disorder, and excitations under pressure in the Mott Insulator Sr\u2082IrO\u2084",
        "author": [
            {
                "family_name": "Li",
                "given_name": "Xiang",
                "orcid": "0000-0002-3780-7735",
                "clpid": "Li-Xiang"
            },
            {
                "family_name": "Cooper",
                "given_name": "S. E.",
                "clpid": "Cooper-S-E"
            },
            {
                "family_name": "Krishnadas",
                "given_name": "A.",
                "clpid": "Krishnadas-A"
            },
            {
                "family_name": "de la Torre",
                "given_name": "A.",
                "orcid": "0000-0002-6751-8205",
                "clpid": "de-la-Torre-Alberto"
            },
            {
                "family_name": "Perry",
                "given_name": "R. S.",
                "clpid": "Perry-R-S"
            },
            {
                "family_name": "Baumberger",
                "given_name": "F.",
                "orcid": "0000-0001-7104-7541",
                "clpid": "Baumberger-Felix"
            },
            {
                "family_name": "Silevitch",
                "given_name": "D. M.",
                "orcid": "0000-0002-6347-3513",
                "clpid": "Silevitch-D-M"
            },
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            },
            {
                "family_name": "Rosenbaum",
                "given_name": "T. F.",
                "orcid": "0009-0008-6152-666X",
                "clpid": "Rosenbaum-T-F"
            },
            {
                "family_name": "Feng",
                "given_name": "Yejun",
                "orcid": "0000-0003-3667-056X",
                "clpid": "Feng-Yejun"
            }
        ],
        "abstract": "Protected by the interplay of on-site Coulomb interactions and spin-orbit coupling, Sr\u2082IrO\u2084 at high pressure is a rare example of a Mott insulator with a paramagnetic ground state. Here, using optical Raman scattering, we measure both the phonon and magnon evolution in Sr\u2082IrO\u2084 under pressure, and identify three different magnetically-ordered phases, culminating in a spin-disordered state beyond 18 GPa. A strong first-order structural phase transition drives the magnetic evolution at \u223c10 GPa with reduced structural anisotropy in the IrO\u2086 cages, leading to increasingly isotropic exchange interactions between the Heisenberg spins and a spin-flip transition to c-axis-aligned antiferromagnetic order. In the disordered phase of Heisenberg J_(eff) = 1/2 pseudospins, the spin excitations are quasi-elastic and continuous to 10 meV, potentially hosting a gapless quantum spin liquid in Sr\u2082IrO\u2084.",
        "doi": "10.1103/PhysRevB.104.L201111",
        "issn": "2469-9950",
        "publisher": "American Physical Society",
        "publication": "Physical Review B",
        "publication_date": "2021-11-15",
        "series_number": "20",
        "volume": "114",
        "issue": "20",
        "pages": "Art. No. L201111"
    },
    {
        "id": "authors:crc7y-x7328",
        "collection": "authors",
        "collection_id": "crc7y-x7328",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20210406-142159297",
        "type": "article",
        "title": "Implications of second harmonic generation for hidden order in Sr\u2082CuO\u2082Cl\u2082",
        "author": [
            {
                "family_name": "de la Torre",
                "given_name": "A.",
                "orcid": "0000-0002-6751-8205",
                "clpid": "de-la-Torre-Alberto"
            },
            {
                "family_name": "Di Matteo",
                "given_name": "S.",
                "orcid": "0000-0001-5746-0057",
                "clpid": "Di-Matteo-Sergio"
            },
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            },
            {
                "family_name": "Norman",
                "given_name": "M. R.",
                "orcid": "0000-0002-9459-078X",
                "clpid": "Norman-Michael-R"
            }
        ],
        "abstract": "Sr\u2082CuO\u2082Cl\u2082 (SCOC) is a model undoped cuprate with I4/mmm crystallographic symmetry, and a simple magnetic space group C_Amca with associated magnetic point group mmm1\u2032. However, recent second harmonic spectroscopy in the antiferromagnetic phase has challenged this picture, suggesting instead a magnetic point group 4/mm\u2032m\u2032 that coexists with the antiferromagnetism and breaks the two orthogonal mirror planes containing the tetragonal c axis. Here, we analyze the symmetry of SCOC in light of the second harmonic results, and discuss possible ground states that are consistent with the data.",
        "doi": "10.1103/PhysRevB.104.035138",
        "issn": "2469-9950",
        "publisher": "American Physical Society",
        "publication": "Physical Review B",
        "publication_date": "2021-07-15",
        "series_number": "3",
        "volume": "104",
        "issue": "3",
        "pages": "Art. No. 035138"
    },
    {
        "id": "authors:x1as9-6rk47",
        "collection": "authors",
        "collection_id": "x1as9-6rk47",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20200909-101851261",
        "type": "article",
        "title": "Mirror symmetry breaking in a model insulating cuprate",
        "author": [
            {
                "family_name": "de la Torre",
                "given_name": "A.",
                "clpid": "de-la-Torre-A"
            },
            {
                "family_name": "Seyler",
                "given_name": "K. L.",
                "orcid": "0000-0003-1553-4518",
                "clpid": "Seyler-Kyle-L"
            },
            {
                "family_name": "Zhao",
                "given_name": "L.",
                "clpid": "Zhao-L"
            },
            {
                "family_name": "Di Matteo",
                "given_name": "S.",
                "clpid": "Di-Matteo-S"
            },
            {
                "family_name": "Scheurer",
                "given_name": "M. S.",
                "clpid": "Scheurer-M-S"
            },
            {
                "family_name": "Li",
                "given_name": "Y.",
                "orcid": "0000-0003-0886-2919",
                "clpid": "Li-Yangmu"
            },
            {
                "family_name": "Yu",
                "given_name": "B.",
                "clpid": "Yu-B"
            },
            {
                "family_name": "Greven",
                "given_name": "M.",
                "orcid": "0000-0002-8055-4358",
                "clpid": "Greven-Martin"
            },
            {
                "family_name": "Sachdev",
                "given_name": "S.",
                "orcid": "0000-0002-2432-7070",
                "clpid": "Sachdev-Subir"
            },
            {
                "family_name": "Norman",
                "given_name": "M. R.",
                "orcid": "0000-0002-9459-078X",
                "clpid": "Norman-Michael-R"
            },
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            }
        ],
        "abstract": "Among the most actively studied issues in the cuprates are the natures of the pseudogap and strange metal states and their relationship to superconductivity1. There is general agreement that the low-energy physics of the Mott-insulating parent state is well captured by a two-dimensional spin S\u2009=\u20091/2 antiferromagnetic Heisenberg model. However, recent observations of a large thermal Hall conductivity in several parent cuprates appear to defy this simple model and suggest proximity to a magneto-chiral state that breaks all mirror planes that are perpendicular to the CuO\u2082 layers. Here we use optical second harmonic generation to directly resolve the point group symmetries of the model parent cuprate Sr\u2082CuO\u2082Cl\u2082. We report evidence of an order parameter that breaks all perpendicular mirror planes and is consistent with a magneto-chiral state in zero magnetic field. Although this order is clearly coupled to the antiferromagnetism, we are unable to realize its time-reversed partner by thermal cycling through the antiferromagnetic transition temperature or by sampling different spatial locations. This suggests that the order onsets above the N\u00e9el temperature and may be relevant to the mechanism of pseudogap formation.",
        "doi": "10.1038/s41567-021-01210-6",
        "issn": "1745-2473",
        "publisher": "Nature Publishing Group",
        "publication": "Nature Physics",
        "publication_date": "2021-07",
        "series_number": "7",
        "volume": "17",
        "issue": "7",
        "pages": "777-781"
    },
    {
        "id": "authors:s0af3-zdd95",
        "collection": "authors",
        "collection_id": "s0af3-zdd95",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20210506-140539872",
        "type": "article",
        "title": "Topology and Symmetry of Quantum Materials via Nonlinear Optical Responses",
        "author": [
            {
                "family_name": "Orenstein",
                "given_name": "J.",
                "clpid": "Orenstein-J"
            },
            {
                "family_name": "Moore",
                "given_name": "J. E.",
                "clpid": "Moore-J-E"
            },
            {
                "family_name": "Morimoto",
                "given_name": "T.",
                "clpid": "Morimoto-T"
            },
            {
                "family_name": "Torchinsky",
                "given_name": "D. H.",
                "clpid": "Torchinsky-Darius-H"
            },
            {
                "family_name": "Harter",
                "given_name": "J. W.",
                "orcid": "0000-0002-7146-9370",
                "clpid": "Harter-John-W"
            },
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            }
        ],
        "abstract": "We review recent progress in the study of photogalvanic effects and optical second-harmonic generation in topological and noncentrosymmetric metals.",
        "doi": "10.1146/annurev-conmatphys-031218-013712",
        "issn": "1947-5454",
        "publisher": "Annual Reviews",
        "publication": "Annual Review of Condensed Matter Physics",
        "publication_date": "2021-03",
        "volume": "12",
        "pages": "247-272"
    },
    {
        "id": "authors:5tzpp-vvv59",
        "collection": "authors",
        "collection_id": "5tzpp-vvv59",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20201224-090002408",
        "type": "article",
        "title": "Signatures of Ultrafast Reversal of Excitonic Order in Ta\u2082NiSe\u2085",
        "author": [
            {
                "family_name": "Ning",
                "given_name": "H.",
                "clpid": "Ning-Honglie"
            },
            {
                "family_name": "Mehio",
                "given_name": "O.",
                "clpid": "Mehio-Omar"
            },
            {
                "family_name": "Buchhold",
                "given_name": "M.",
                "orcid": "0000-0001-5194-9388",
                "clpid": "Buchhold-Michael"
            },
            {
                "family_name": "Kurumaji",
                "given_name": "T.",
                "orcid": "0000-0002-2157-3727",
                "clpid": "Kurumaji-Takashi"
            },
            {
                "family_name": "Refael",
                "given_name": "G.",
                "clpid": "Refael-G"
            },
            {
                "family_name": "Checkelsky",
                "given_name": "J.\u2009G.",
                "orcid": "0000-0003-0325-5204",
                "clpid": "Checkelsky-Joseph-G"
            },
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            }
        ],
        "abstract": "In the presence of electron-phonon coupling, an excitonic insulator harbors two degenerate ground states described by an Ising-type order parameter. Starting from a microscopic Hamiltonian, we derive the equations of motion for the Ising order parameter in the phonon coupled excitonic insulator Ta\u2082NiSe\u2085 and show that it can be controllably reversed on ultrashort timescales using appropriate laser pulse sequences. Using a combination of theory and time-resolved optical reflectivity measurements, we report evidence of such order parameter reversal in Ta\u2082NiSe\u2085 based on the anomalous behavior of its coherently excited order-parameter-coupled phonons. Our Letter expands the field of ultrafast order parameter control beyond spin and charge ordered materials.",
        "doi": "10.1103/physrevlett.125.267602",
        "issn": "0031-9007",
        "publisher": "American Physical Society",
        "publication": "Physical Review Letters",
        "publication_date": "2020-12-31",
        "series_number": "26",
        "volume": "125",
        "issue": "26",
        "pages": "Art. No. 267602"
    },
    {
        "id": "authors:sj520-zwr83",
        "collection": "authors",
        "collection_id": "sj520-zwr83",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20201113-100152383",
        "type": "article",
        "title": "Spin-orbit-enhanced magnetic surface second-harmonic generation in Sr\u2082IrO\u2084",
        "author": [
            {
                "family_name": "Seyler",
                "given_name": "K. L.",
                "orcid": "0000-0003-1553-4518",
                "clpid": "Seyler-Kyle-L"
            },
            {
                "family_name": "de la Torre",
                "given_name": "A.",
                "clpid": "de-la-Torre-Alberto"
            },
            {
                "family_name": "Porter",
                "given_name": "Z.",
                "clpid": "Porter-Z"
            },
            {
                "family_name": "Zoghlin",
                "given_name": "E.",
                "orcid": "0000-0002-8160-584X",
                "clpid": "Zoghlin-Eli"
            },
            {
                "family_name": "Polski",
                "given_name": "R.",
                "orcid": "0000-0003-0887-8099",
                "clpid": "Polski-Robert-M"
            },
            {
                "family_name": "Nguyen",
                "given_name": "M.",
                "clpid": "Nguyen-Mai"
            },
            {
                "family_name": "Nadj-Perge",
                "given_name": "S.",
                "orcid": "0000-0002-2394-9070",
                "clpid": "Nadj-Perge-S"
            },
            {
                "family_name": "Wilson",
                "given_name": "S. D.",
                "clpid": "Wilson-Stephen-D"
            },
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            }
        ],
        "abstract": "An anomalous optical second-harmonic generation (SHG) signal was previously reported in Sr\u2082IrO\u2084 and attributed to a hidden odd-parity bulk magnetic state. Here we investigate the origin of this SHG signal using a combination of bulk magnetic susceptibility, magnetic-field-dependent SHG rotational anisotropy, and overlapping wide-field SHG imaging and atomic force microscopy measurements. We find that the anomalous SHG signal exhibits a twofold rotational symmetry as a function of in-plane magnetic field orientation that is associated with a crystallographic distortion. We also show a change in SHG signal across step edges that tracks the bulk antiferromagnetic stacking pattern. While we do not rule out the existence of hidden order in Sr\u2082IrO\u2084, our results altogether show that the anomalous SHG signal in parent Sr\u2082IrO\u2084 originates instead from a surface-magnetization-induced electric-dipole process that is enhanced by strong spin-orbit coupling.",
        "doi": "10.1103/physrevb.102.201113",
        "issn": "2469-9950",
        "publisher": "American Physical Society",
        "publication": "Physical Review B",
        "publication_date": "2020-11-15",
        "series_number": "20",
        "volume": "102",
        "issue": "20",
        "pages": "Art. No. 201113(R)"
    },
    {
        "id": "authors:zqxn5-ecv65",
        "collection": "authors",
        "collection_id": "zqxn5-ecv65",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20191217-085020547",
        "type": "article",
        "title": "Ultrafast Enhancement of Ferromagnetic Spin Exchange Induced by Ligand-to-Metal Charge Transfer",
        "author": [
            {
                "family_name": "Ron",
                "given_name": "A.",
                "orcid": "0000-0002-1840-7824",
                "clpid": "Ron-Alon"
            },
            {
                "family_name": "Chaudhary",
                "given_name": "S.",
                "clpid": "Chaudhary-Swati"
            },
            {
                "family_name": "Zhang",
                "given_name": "G.",
                "clpid": "Zhang-Gufeng"
            },
            {
                "family_name": "Ning",
                "given_name": "H.",
                "clpid": "Ning-Honglie"
            },
            {
                "family_name": "Zoghlin",
                "given_name": "E.",
                "orcid": "0000-0002-8160-584X",
                "clpid": "Zoghlin-E"
            },
            {
                "family_name": "Wilson",
                "given_name": "S. D.",
                "clpid": "Wilson-S-D"
            },
            {
                "family_name": "Averitt",
                "given_name": "R. D.",
                "orcid": "0000-0003-0451-1935",
                "clpid": "Averitt-R-D"
            },
            {
                "family_name": "Refael",
                "given_name": "G.",
                "clpid": "Refael-G"
            },
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            }
        ],
        "abstract": "We theoretically predict and experimentally demonstrate a nonthermal pathway to optically enhance superexchange interaction energies in a material based on exciting ligand-to-metal charge-transfer transitions, which introduces lower-order virtual hopping contributions that are absent in the ground state. We demonstrate this effect in the layered ferromagnetic insulator CrSiTe\u2083 by exciting Te-to-Cr charge-transfer transitions using ultrashort laser pulses and detecting coherent phonon oscillations that are impulsively generated by superexchange enhancement via magneto-elastic coupling. This mechanism kicks in below the temperature scale where short-range in-plane spin correlations begin to develop and disappears when the excitation energy is tuned away from the charge-transfer resonance, consistent with our predictions.",
        "doi": "10.1103/PhysRevLett.125.197203",
        "issn": "0031-9007",
        "publisher": "American Physical Society",
        "publication": "Physical Review Letters",
        "publication_date": "2020-11-06",
        "series_number": "19",
        "volume": "125",
        "issue": "19",
        "pages": "Art. No. 197203"
    },
    {
        "id": "authors:ceyaw-k8w85",
        "collection": "authors",
        "collection_id": "ceyaw-k8w85",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20200731-134646814",
        "type": "article",
        "title": "Evidence for an extended critical fluctuation region above the polar ordering transition in LiOsO\u2083",
        "author": [
            {
                "family_name": "Shan",
                "given_name": "Jun-Yi",
                "orcid": "0000-0001-7665-2169",
                "clpid": "Shan-Jun-Yi"
            },
            {
                "family_name": "de la Torre",
                "given_name": "A.",
                "clpid": "de-la-Torre-A"
            },
            {
                "family_name": "Laurita",
                "given_name": "N. J.",
                "clpid": "Laurita-N-J"
            },
            {
                "family_name": "Zhao",
                "given_name": "L.",
                "clpid": "Zhao-L"
            },
            {
                "family_name": "Dashwood",
                "given_name": "C. D.",
                "clpid": "Dashwood-C-D"
            },
            {
                "family_name": "Puggioni",
                "given_name": "D.",
                "orcid": "0000-0002-2128-4191",
                "clpid": "Puggioni-D"
            },
            {
                "family_name": "Wang",
                "given_name": "C. X.",
                "orcid": "0000-0003-2072-2759",
                "clpid": "Wang-Cuixiang"
            },
            {
                "family_name": "Yamaura",
                "given_name": "K.",
                "orcid": "0000-0003-0390-8244",
                "clpid": "Yamaura-Kazunari"
            },
            {
                "family_name": "Shi",
                "given_name": "Y.",
                "clpid": "Shi-Y"
            },
            {
                "family_name": "Rondinelli",
                "given_name": "J. M.",
                "orcid": "0000-0003-0508-2175",
                "clpid": "Rondinelli-J-M"
            },
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            }
        ],
        "abstract": "Metallic LiOsO\u2083 undergoes a continuous ferroelectric-like structural phase transition below T_c=140K to realize a polar metal. To understand the microscopic interactions that drive this transition, we study its critical behavior above T_c via electromechanical coupling\u2014distortions of the lattice induced by short-range dipole-dipole correlations arising from Li off-center displacements. By mapping the full angular distribution of second harmonic electric-quadrupole radiation from LiOsO\u2083 and performing a simplified hyper-polarizable bond model analysis, we uncover subtle symmetry-preserving lattice distortions over a broad temperature range extending from T_c up to around 230 K, characterized by nonuniform changes in the short and long Li-O bond lengths. Such an extended region of critical fluctuations may explain anomalous features reported in specific heat and Raman scattering data and suggests the presence of competing interactions that are not accounted for in existing theoretical treatments. More broadly, our results showcase how electromechanical effects serve as a probe of critical behavior near inversion symmetry-breaking transitions in metals.",
        "doi": "10.1103/physrevresearch.2.033174",
        "issn": "2643-1564",
        "publisher": "American Physical Society",
        "publication": "Physical Review Research",
        "publication_date": "2020-07",
        "series_number": "3",
        "volume": "2",
        "issue": "3",
        "pages": "Art. No. 033174"
    },
    {
        "id": "authors:k8e59-84091",
        "collection": "authors",
        "collection_id": "k8e59-84091",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20200116-131511286",
        "type": "article",
        "title": "Linear Magnetoelectric Phase in Ultrathin MnPS\u2083 Probed by Optical Second Harmonic Generation",
        "author": [
            {
                "family_name": "Chu",
                "given_name": "Hao",
                "orcid": "0000-0002-1989-9517",
                "clpid": "Chu-Hao"
            },
            {
                "family_name": "Roh",
                "given_name": "Chang Jae",
                "clpid": "Roh-Chang-Jae"
            },
            {
                "family_name": "Island",
                "given_name": "Joshua O.",
                "clpid": "Island-J-O"
            },
            {
                "family_name": "Li",
                "given_name": "Chen",
                "clpid": "Li-Chen"
            },
            {
                "family_name": "Lee",
                "given_name": "Sungmin",
                "clpid": "Lee-Sungmin"
            },
            {
                "family_name": "Chen",
                "given_name": "Jingjing",
                "clpid": "Chen-Jingjing"
            },
            {
                "family_name": "Park",
                "given_name": "Je-Geun",
                "clpid": "Park-Je-Geun"
            },
            {
                "family_name": "Young",
                "given_name": "Andrea F.",
                "clpid": "Young-Andrea-F"
            },
            {
                "family_name": "Lee",
                "given_name": "Jong Seok",
                "clpid": "Lee-Jong-Seok"
            },
            {
                "family_name": "Hsieh",
                "given_name": "David",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            }
        ],
        "abstract": "The transition metal thiophosphates MPS\u2083 (M=Mn, Fe, Ni) are a class of van der Waals stacked insulating antiferromagnets that can be exfoliated down to the ultrathin limit. MnPS\u2083 is particularly interesting because its N\u00e9el ordered state breaks both spatial-inversion and time-reversal symmetries, allowing for a linear magnetoelectric phase that is rare among van der Waals materials. However, it is unknown whether this unique magnetic structure of bulk MnPS\u2083 remains stable in the ultrathin limit. Using optical second harmonic generation rotational anisotropy, we show that long-range linear magnetoelectric type N\u00e9el order in MnPS\u2083 persists down to at least 5.3 nm thickness. However an unusual mirror symmetry breaking develops in ultrathin samples on SiO\u2082 substrates that is absent in bulk materials, which is likely related to substrate induced strain.",
        "doi": "10.1103/physrevlett.124.027601",
        "issn": "0031-9007",
        "publisher": "American Physical Society",
        "publication": "Physical Review Letters",
        "publication_date": "2020-01-17",
        "series_number": "2",
        "volume": "124",
        "issue": "2",
        "pages": "Art. No. 027601"
    },
    {
        "id": "authors:g6y56-69550",
        "collection": "authors",
        "collection_id": "g6y56-69550",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20200116-095411449",
        "type": "article",
        "title": "Valence bond phases of herbertsmithite and related copper kagome materials",
        "author": [
            {
                "family_name": "Norman",
                "given_name": "M. R.",
                "orcid": "0000-0002-9459-078X",
                "clpid": "Norman-M-R"
            },
            {
                "family_name": "Laurita",
                "given_name": "N. J.",
                "clpid": "Laurita-N-J"
            },
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            }
        ],
        "abstract": "Recent evidence from magnetic torque, electron spin resonance, and second harmonic generation indicate that the prototypical quantum spin liquid candidate, herbertsmithite, has a symmetry lower than its x-ray refined trigonal space group. Here we consider known and possible distortions of this mineral class, along with related copper kagome oxides and fluorides, relate these to possible valence bond patterns, and comment on their relevance to the physics of these interesting materials.",
        "doi": "10.1103/physrevresearch.2.013055",
        "issn": "2643-1564",
        "publisher": "American Physical Society",
        "publication": "Physical Review Research",
        "publication_date": "2020-01",
        "series_number": "1",
        "volume": "2",
        "issue": "1",
        "pages": "Art. No. 013055"
    },
    {
        "id": "authors:jk5ad-65w58",
        "collection": "authors",
        "collection_id": "jk5ad-65w58",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20190520-132243974",
        "type": "article",
        "title": "Orbital Floquet Engineering of Exchange Interactions in Magnetic Materials",
        "author": [
            {
                "family_name": "Chaudhary",
                "given_name": "Swati",
                "clpid": "Chaudhary-Swati"
            },
            {
                "family_name": "Hsieh",
                "given_name": "David",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            },
            {
                "family_name": "Refael",
                "given_name": "Gil",
                "clpid": "Refael-G"
            }
        ],
        "abstract": "We present a scheme to control the spin-exchange interactions by manipulating the orbital degrees of freedom using a periodic drive. We discuss two different protocols for orbital Floquet engineering. In one case, a periodic drive modifies the properties of the ligand orbitals which mediate magnetic interactions between transition-metal ions. In the other case, we consider drive-induced mixing of d orbitals on each magnetic ion. We first find that an AC Stark shift of orbitals induces a change comparable to that induced from photoinduced hopping schemes, but expands the applicable frequency ranges. Next, we find that radiatively induced coherent vibrations provide a realistic path for Floquet orbital engineering with short pulses of electric fields weaker than 0.5 V/\u00c5 producing 5%\u201310% changes in the magnetic coupling of Mott insulators such as the rare-earth titanates.",
        "doi": "10.1103/PhysRevB.100.220403",
        "issn": "2469-9950",
        "publisher": "American Physical Society",
        "publication": "Physical Review B",
        "publication_date": "2019-12-01",
        "series_number": "22",
        "volume": "100",
        "issue": "22",
        "pages": "Art. No. 220403"
    },
    {
        "id": "authors:ne2g5-mym09",
        "collection": "authors",
        "collection_id": "ne2g5-mym09",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20190719-102955020",
        "type": "article",
        "title": "Evidence for the weakly coupled electron mechanism in an Anderson-Blount polar metal",
        "author": [
            {
                "family_name": "Laurita",
                "given_name": "N. J.",
                "clpid": "Laurita-N-J"
            },
            {
                "family_name": "Ron",
                "given_name": "A.",
                "orcid": "0000-0002-1840-7824",
                "clpid": "Ron-Alon"
            },
            {
                "family_name": "Shan",
                "given_name": "Jun-Yi",
                "orcid": "0000-0001-7665-2169",
                "clpid": "Shan-Jun-Yi"
            },
            {
                "family_name": "Puggioni",
                "given_name": "D.",
                "orcid": "0000-0002-2128-4191",
                "clpid": "Puggioni-Danilo"
            },
            {
                "family_name": "Koocher",
                "given_name": "N. Z.",
                "clpid": "Koocher-N-Z"
            },
            {
                "family_name": "Yamaura",
                "given_name": "K.",
                "orcid": "0000-0003-0390-8244",
                "clpid": "Yamaura-K"
            },
            {
                "family_name": "Shi",
                "given_name": "Y.",
                "clpid": "Shi-Y"
            },
            {
                "family_name": "Rondinelli",
                "given_name": "J. M.",
                "orcid": "0000-0003-0508-2175",
                "clpid": "Rondinelli-James-M"
            },
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            }
        ],
        "abstract": "Over 50 years ago, Anderson and Blount proposed that ferroelectric-like structural phase transitions may occur in metals, despite the expected screening of the Coulomb interactions that often drive polar transitions. Recently, theoretical treatments have suggested that such transitions require the itinerant electrons be decoupled from the soft transverse optical phonons responsible for polar order. However, this decoupled electron mechanism (DEM) has yet to be experimentally observed. Here we utilize ultrafast spectroscopy to uncover evidence of the DEM in LiOsO_3, the first known band metal to undergo a thermally driven polar phase transition (T_c\u2009\u2248\u2009140\u2009K). We demonstrate that intra-band photo-carriers relax by selectively coupling to only a subset of the phonon spectrum, leaving as much as 60% of the lattice heat capacity decoupled. This decoupled heat capacity is shown to be consistent with a previously undetected and partially displacive TO polar mode, indicating the DEM in LiOsO_3.",
        "doi": "10.1038/s41467-019-11172-2",
        "pmcid": "PMC6642157",
        "issn": "2041-1723",
        "publisher": "Nature Publishing Group",
        "publication": "Nature Communications",
        "publication_date": "2019-07-19",
        "volume": "10",
        "pages": "Art. No. 3217"
    },
    {
        "id": "authors:fkybh-d3e86",
        "collection": "authors",
        "collection_id": "fkybh-d3e86",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20190410-093027160",
        "type": "article",
        "title": "Dimensional crossover in a layered ferromagnet detected by spin correlation driven distortions",
        "author": [
            {
                "family_name": "Ron",
                "given_name": "A.",
                "orcid": "0000-0002-1840-7824",
                "clpid": "Ron-Alon"
            },
            {
                "family_name": "Zoghlin",
                "given_name": "E.",
                "clpid": "Zoghlin-E"
            },
            {
                "family_name": "Balents",
                "given_name": "L.",
                "clpid": "Balents-L"
            },
            {
                "family_name": "Wilson",
                "given_name": "S. D.",
                "clpid": "Wilson-S-D"
            },
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            }
        ],
        "abstract": "Magneto-elastic distortions are commonly detected across magnetic long-range ordering (LRO) transitions. In principle, they are also induced by the magnetic short-range ordering (SRO) that precedes a LRO transition, which contains information about short-range correlations and energetics that are essential for understanding how LRO is established. However these distortions are difficult to resolve because the associated atomic displacements are exceedingly small and do not break symmetry. Here we demonstrate high-multipole nonlinear optical polarimetry as a sensitive and mode selective probe of SRO induced distortions using CrSiTe_3 as a testbed. This compound is composed of weakly bonded sheets of nearly isotropic ferromagnetically interacting spins that, in the Heisenberg limit, would individually be impeded from LRO by the Mermin-Wagner theorem. Our results show that CrSiTe_3 evades this law via a two-step crossover from two- to three-dimensional magnetic SRO, manifested through two successive and previously undetected totally symmetric distortions above its Curie temperature.",
        "doi": "10.1038/s41467-019-09663-3",
        "pmcid": "PMC6458139",
        "issn": "2041-1723",
        "publisher": "Nature Publishing Group",
        "publication": "Nature Communications",
        "publication_date": "2019-04-10",
        "volume": "10",
        "pages": "Art. No. 1654"
    },
    {
        "id": "authors:t31vy-7dm36",
        "collection": "authors",
        "collection_id": "t31vy-7dm36",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20180508-105825258",
        "type": "article",
        "title": "Inversion symmetry and bulk Rashba effect in methylammonium lead iodide perovskite single crystals",
        "author": [
            {
                "family_name": "Frohna",
                "given_name": "Kyle",
                "orcid": "0000-0002-2259-6154",
                "clpid": "Frohna-Kyle"
            },
            {
                "family_name": "Deshpande",
                "given_name": "Tejas",
                "orcid": "0000-0003-0326-1372",
                "clpid": "Deshpande-Tejas"
            },
            {
                "family_name": "Harter",
                "given_name": "John",
                "orcid": "0000-0002-7146-9370",
                "clpid": "Harter-John-W"
            },
            {
                "family_name": "Peng",
                "given_name": "Wei",
                "clpid": "Peng-Wei"
            },
            {
                "family_name": "Barker",
                "given_name": "Bradford A.",
                "clpid": "Barker-Bradford-A"
            },
            {
                "family_name": "Neaton",
                "given_name": "Jeffrey B.",
                "orcid": "0000-0001-7585-6135",
                "clpid": "Neaton-Jeffrey-B"
            },
            {
                "family_name": "Louie",
                "given_name": "Steven G.",
                "clpid": "Louie-Steven-G"
            },
            {
                "family_name": "Bakr",
                "given_name": "Osman M.",
                "clpid": "Bakr-Osman-M"
            },
            {
                "family_name": "Hsieh",
                "given_name": "David",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            },
            {
                "family_name": "Bernardi",
                "given_name": "Marco",
                "orcid": "0000-0001-7289-9666",
                "clpid": "Bernardi-Marco"
            }
        ],
        "abstract": "Methylammonium lead iodide perovskite (MAPbI_3) exhibits long charge carrier lifetimes that are linked to its high efficiency in solar cells. Yet, the mechanisms governing these unusual carrier dynamics are not completely understood. A leading hypothesis\u2014disproved in this work\u2014is that a large, static bulk Rashba effect slows down carrier recombination. Here, using second harmonic generation rotational anisotropy measurements on MAPbI_3 crystals, we demonstrate that the bulk structure of tetragonal MAPbI_3 is centrosymmetric with I4/mcmspace group. Our calculations show that a significant Rashba splitting in the bandstructure requires a non-centrosymmetric lead iodide framework, and that incorrect structural relaxations are responsible for the previously predicted large Rashba effect. The small Rashba splitting allows us to compute effective masses in excellent agreement with experiment. Our findings rule out the presence of a large static Rashba effect in bulk MAPbI_3, and our measurements find no evidence of dynamic Rashba effects.",
        "doi": "10.1038/s41467-018-04212-w",
        "pmcid": "PMC5940805",
        "issn": "2041-1723",
        "publisher": "Nature Publishing Group",
        "publication": "Nature Communications",
        "publication_date": "2018-05-08",
        "volume": "9",
        "pages": "Art. No. 1829"
    },
    {
        "id": "authors:v2873-34b69",
        "collection": "authors",
        "collection_id": "v2873-34b69",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20180313-161721314",
        "type": "article",
        "title": "Floquet Engineering in Quantum Chains",
        "author": [
            {
                "family_name": "Kennes",
                "given_name": "D. M.",
                "clpid": "Kennes-D-M"
            },
            {
                "family_name": "de la Torre",
                "given_name": "A.",
                "clpid": "de-la-Torre-A"
            },
            {
                "family_name": "Ron",
                "given_name": "A.",
                "orcid": "0000-0002-1840-7824",
                "clpid": "Ron-Alon"
            },
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            },
            {
                "family_name": "Millis",
                "given_name": "A. J.",
                "clpid": "Mills-A-J"
            }
        ],
        "abstract": "We consider a one-dimensional interacting spinless fermion model, which displays the well-known Luttinger liquid (LL) to charge density wave (CDW) transition as a function of the ratio between the strength of the interaction \nU\n and the hopping \nJ\n. We subject this system to a spatially uniform drive which is ramped up over a finite time interval and becomes time periodic in the long-time limit. We show that by using a density matrix renormalization group approach formulated for infinite system sizes, we can access the large-time limit even when the drive induces finite heating. When both the initial and long-time states are in the gapless (LL) phase, the final state has power-law correlations for all ramp speeds. However, when the initial and final state are gapped (CDW phase), we find a pseudothermal state with an effective temperature that depends on the ramp rate, both for the Magnus regime in which the drive frequency is very large compared to other scales in the system and in the opposite limit where the drive frequency is less than the gap. Remarkably, quantum defects (instantons) appear when the drive tunes the system through the quantum critical point, in a realization of the Kibble-Zurek mechanism.",
        "doi": "10.1103/PhysRevLett.120.127601",
        "issn": "0031-9007",
        "publisher": "American Physical Society",
        "publication": "Physical Review Letters",
        "publication_date": "2018-03-23",
        "series_number": "12",
        "volume": "120",
        "issue": "12",
        "pages": "Art. No. 127601"
    },
    {
        "id": "authors:dmv84-6kv75",
        "collection": "authors",
        "collection_id": "dmv84-6kv75",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20180131-160608890",
        "type": "article",
        "title": "Evidence of an Improper Displacive Phase Transition in Cd_2Re_2O_7 via Time-Resolved Coherent Phonon Spectroscopy",
        "author": [
            {
                "family_name": "Harter",
                "given_name": "J. W.",
                "orcid": "0000-0002-7146-9370",
                "clpid": "Harter-J-W"
            },
            {
                "family_name": "Kennes",
                "given_name": "D. M.",
                "clpid": "Kennes-D-M"
            },
            {
                "family_name": "Chu",
                "given_name": "H.",
                "orcid": "0000-0002-1989-9517",
                "clpid": "Chu-Hao"
            },
            {
                "family_name": "de la Torre",
                "given_name": "A.",
                "clpid": "de-la-Torre-A"
            },
            {
                "family_name": "Zhao",
                "given_name": "Z. Y.",
                "clpid": "Zhao-Z-Y"
            },
            {
                "family_name": "Yan",
                "given_name": "J.-Q.",
                "orcid": "0000-0001-6625-4706",
                "clpid": "Yan-Jiaqiang"
            },
            {
                "family_name": "Mandrus",
                "given_name": "D. G.",
                "clpid": "Mandrus-D-G"
            },
            {
                "family_name": "Millis",
                "given_name": "A. J.",
                "clpid": "Millis-A-J"
            },
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            }
        ],
        "abstract": "We have used a combination of ultrafast coherent phonon spectroscopy, ultrafast thermometry, and time-dependent Landau theory to study the inversion symmetry breaking phase transition at T_c=200\u2009\u2009K in the strongly spin-orbit coupled correlated metal Cd_2Re_2O_7. We establish that the structural distortion at T_c is a secondary effect through the absence of any softening of its associated phonon mode, which supports a purely electronically driven mechanism. However, the phonon lifetime exhibits an anomalously strong temperature dependence that decreases linearly to zero near T_c. We show that this behavior naturally explains the spurious appearance of phonon softening in previous Raman spectroscopy experiments and should be a prevalent feature of correlated electron systems with linearly coupled order parameters.",
        "doi": "10.1103/PhysRevLett.120.047601",
        "issn": "0031-9007",
        "publisher": "American Physical Society",
        "publication": "Physical Review Letters",
        "publication_date": "2018-01-26",
        "series_number": "4",
        "volume": "120",
        "issue": "4",
        "pages": "Art. No. 047601"
    },
    {
        "id": "authors:rpxwr-tvg04",
        "collection": "authors",
        "collection_id": "rpxwr-tvg04",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20170922-102739878",
        "type": "article",
        "title": "Towards properties on demand in quantum materials",
        "author": [
            {
                "family_name": "Basov",
                "given_name": "D. N.",
                "clpid": "Basov-D-N"
            },
            {
                "family_name": "Averitt",
                "given_name": "R. D.",
                "clpid": "Averitt-R-D"
            },
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            }
        ],
        "abstract": "The past decade has witnessed an explosion in the field of quantum materials, headlined by the predictions and discoveries of novel Landau-symmetry-broken phases in correlated electron systems, topological phases in systems with strong spin\u2013orbit coupling, and ultra-manipulable materials platforms based on two-dimensional van der Waals crystals. Discovering pathways to experimentally realize quantum phases of matter and exert control over their properties is a central goal of modern condensed-matter physics, which holds promise for a new generation of electronic/photonic devices with currently inaccessible and likely unimaginable functionalities. In this Review, we describe emerging strategies for selectively perturbing microscopic interaction parameters, which can be used to transform materials into a desired quantum state. Particular emphasis will be placed on recent successes to tailor electronic interaction parameters through the application of intense fields, impulsive electromagnetic stimulation, and nanostructuring or interface engineering. Together these approaches outline a potential roadmap to an era of quantum phenomena on demand.",
        "doi": "10.1038/NMAT5017",
        "issn": "1476-1122",
        "publisher": "Nature Publishing Group",
        "publication": "Nature Materials",
        "publication_date": "2017-11",
        "series_number": "11",
        "volume": "16",
        "issue": "11",
        "pages": "1077-1088"
    },
    {
        "id": "authors:pm8rq-ds434",
        "collection": "authors",
        "collection_id": "pm8rq-ds434",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20170530-122910588",
        "type": "article",
        "title": "Doping-driven structural distortion in the bilayer iridate \n (Sr_(1\u2212x)La_x)_3Ir_2O_7",
        "author": [
            {
                "family_name": "Hogan",
                "given_name": "Tom",
                "clpid": "Hogan-T"
            },
            {
                "family_name": "Wang",
                "given_name": "Xiaoping",
                "orcid": "0000-0001-7143-8112",
                "clpid": "Wang-Xiaoping"
            },
            {
                "family_name": "Chu",
                "given_name": "H.",
                "orcid": "0000-0002-1989-9517",
                "clpid": "Chu-Hao"
            },
            {
                "family_name": "Hsieh",
                "given_name": "David",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            },
            {
                "family_name": "Wilson",
                "given_name": "Stephen D.",
                "clpid": "Wilson-Stephen-D"
            }
        ],
        "abstract": "Neutron single-crystal diffraction and rotational anisotropy optical second harmonic generation data are presented resolving the nature of the structural distortion realized in electron-doped (Sr_(1\u2212x)La_x)_3Ir_2O_7 with x = 0.035 and x = 0.071. Once electrons are introduced into the bilayer spin-orbit assisted Mott insulator Sr_2Ir_2O_7, previous studies have identified the appearance of a low-temperature structural distortion and have suggested the presence of a competing electronic instability in the phase diagram of this material. Our measurements resolve a lowering of the structural symmetry from monoclinic C2/c to monoclinic P2_1/c and the creation of two unique Ir sites within the chemical unit cell as the lattice distorts below a critical temperature T_S. Details regarding the modifications to oxygen octahedral rotations and tilting through the transition are discussed as well as the evolution of the low-temperature distorted lattice as a function of carrier substitution.",
        "doi": "10.1103/PhysRevB.95.174109",
        "issn": "2469-9950",
        "publisher": "American Physical Society",
        "publication": "Physical Review B",
        "publication_date": "2017-05-01",
        "series_number": "17",
        "volume": "95",
        "issue": "17",
        "pages": "Art. No. 174109"
    },
    {
        "id": "authors:d54e3-e7d91",
        "collection": "authors",
        "collection_id": "d54e3-e7d91",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20170420-145037343",
        "type": "article",
        "title": "A parity-breaking electronic nematic phase transition in the spin-orbit coupled metal Cd\u2082Re\u2082O\u2087",
        "author": [
            {
                "family_name": "Harter",
                "given_name": "J. W.",
                "orcid": "0000-0002-7146-9370",
                "clpid": "Harter-John-W"
            },
            {
                "family_name": "Zhao",
                "given_name": "Z. Y.",
                "orcid": "0000-0002-7878-8972",
                "clpid": "Zhao-Zhiying"
            },
            {
                "family_name": "Yan",
                "given_name": "J.-Q.",
                "orcid": "0000-0001-6625-4706",
                "clpid": "Yan-Jiaqiang"
            },
            {
                "family_name": "Mandrus",
                "given_name": "D. G.",
                "orcid": "0000-0003-3616-7104",
                "clpid": "Mandrus-David-G"
            },
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            }
        ],
        "abstract": "Strong electron interactions can drive metallic systems toward a variety of well-known symmetry-broken phases, but the instabilities of correlated metals with strong spin-orbit coupling have only recently begun to be explored. We uncovered a multipolar nematic phase of matter in the metallic pyrochlore Cd\u2082Re\u2082O\u2087 using spatially resolved second-harmonic optical anisotropy measurements. Like previously discovered electronic nematic phases, this multipolar phase spontaneously breaks rotational symmetry while preserving translational invariance. However, it has the distinguishing property of being odd under spatial inversion, which is allowed only in the presence of spin-orbit coupling. By examining the critical behavior of the multipolar nematic order parameter, we show that it drives the thermal phase transition near 200 kelvin in Cd\u2082Re\u2082O\u2087 and induces a parity-breaking lattice distortion as a secondary order.",
        "doi": "10.1126/science.aad1188",
        "issn": "0036-8075",
        "publisher": "American Association for the Advancement of Science",
        "publication": "Science",
        "publication_date": "2017-04-21",
        "series_number": "6335",
        "volume": "356",
        "issue": "6335",
        "pages": "295-299"
    },
    {
        "id": "authors:h2txk-8af81",
        "collection": "authors",
        "collection_id": "h2txk-8af81",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20161014-080142438",
        "type": "article",
        "title": "A global inversion-symmetry-broken phase inside the pseudogap region of YBa_2Cu_3O_y",
        "author": [
            {
                "family_name": "Zhao",
                "given_name": "L.",
                "clpid": "Zhao-Liyuan"
            },
            {
                "family_name": "Belvin",
                "given_name": "C. A.",
                "clpid": "Belvin-C-A"
            },
            {
                "family_name": "Liang",
                "given_name": "R.",
                "clpid": "Liang-R"
            },
            {
                "family_name": "Bonn",
                "given_name": "D. A.",
                "clpid": "Bonn-D-A"
            },
            {
                "family_name": "Hardy",
                "given_name": "W. N.",
                "clpid": "Hardy-W-N"
            },
            {
                "family_name": "Armitage",
                "given_name": "N. P.",
                "clpid": "Armitage-N-P"
            },
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            }
        ],
        "abstract": "The phase diagram of cuprate high-temperature superconductors features an enigmatic pseudogap region that is characterized by a partial suppression of low-energy electronic excitations. Polarized neutron diffraction Nernst effect, terahertz polarimetry and ultrasound measurements on YBa_2Cu_3O_y suggest that the pseudogap onset below a temperature T^\u2217 coincides with a bona fide thermodynamic phase transition that breaks time-reversal, four-fold rotation and mirror symmetries respectively. However, the full point group above and below T^\u2217 has not been resolved and the fate of this transition as T^\u2217 approaches the superconducting critical temperature T_c is poorly understood. Here we reveal the point group of YBa_2Cu_3O_y inside its pseudogap and neighbouring regions using high-sensitivity linear and second-harmonic optical anisotropy measurements. We show that spatial inversion and two-fold rotational symmetries are broken below T^\u2217 while mirror symmetries perpendicular to the Cu\u2013O plane are absent at all temperatures. This transition occurs over a wide doping range and persists inside the superconducting dome, with no detectable coupling to either charge ordering or superconductivity. These results suggest that the pseudogap region coincides with an odd-parity order that does not arise from a competing Fermi surface instability and exhibits a quantum phase transition inside the superconducting dome.",
        "doi": "10.1038/nphys3962",
        "issn": "1745-2473",
        "publisher": "Nature Publishing Group",
        "publication": "Nature Physics",
        "publication_date": "2017-03",
        "series_number": "3",
        "volume": "13",
        "issue": "3",
        "pages": "250-254"
    },
    {
        "id": "authors:ffng7-fj792",
        "collection": "authors",
        "collection_id": "ffng7-fj792",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20161110-133754241",
        "type": "article",
        "title": "A charge density wave-like instability in a doped spin-orbit assisted weak Mott insulator",
        "author": [
            {
                "family_name": "Chu",
                "given_name": "H.",
                "orcid": "0000-0002-1989-9517",
                "clpid": "Chu-Hao"
            },
            {
                "family_name": "Zhao",
                "given_name": "L.",
                "clpid": "Zhao-L"
            },
            {
                "family_name": "de la Torre",
                "given_name": "A.",
                "clpid": "de-la-Torre-A"
            },
            {
                "family_name": "Hogan",
                "given_name": "T.",
                "clpid": "Hogan-T"
            },
            {
                "family_name": "Wilson",
                "given_name": "S. D.",
                "clpid": "Wilson-S-D"
            },
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            }
        ],
        "abstract": "Layered perovskite iridates realize a rare class of Mott insulators that are predicted to be strongly spin\u2013orbit coupled analogues of the parent state of cuprate high-temperature superconductors. Recent discoveries of pseudogap, magnetic multipolar ordered6 and possible d-wave superconducting phases in doped Sr_2IrO_4 have reinforced this analogy among the single layer variants. However, unlike the bilayer cuprates, no electronic instabilities have been reported in the doped bilayer iridate Sr_3Ir_2O_7. Here we show that Sr_3Ir_2O_7 realizes a weak Mott state with no cuprate analogue by using ultrafast time-resolved optical reflectivity to uncover an intimate connection between its insulating gap and antiferromagnetism. However, we detect a subtle charge density wave-like Fermi surface instability in metallic electron doped Sr_3Ir_2O_7 at temperatures (T_(DW)) close to 200\u2009K via the coherent oscillations of its collective modes, which is reminiscent of that observed in cuprates. The absence of any signatures of a new spatial periodicity below T_(DW) from diffraction, scanning tunnelling and photoemission based probes suggests an unconventional and possibly short-ranged nature of this density wave order.",
        "doi": "10.1038/NMAT4836",
        "issn": "1476-1122",
        "publisher": "Nature Publishing Group",
        "publication": "Nature Materials",
        "publication_date": "2017-02",
        "series_number": "2",
        "volume": "16",
        "issue": "2",
        "pages": "200-203"
    },
    {
        "id": "authors:abb6x-st040",
        "collection": "authors",
        "collection_id": "abb6x-st040",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20160525-143627761",
        "type": "article",
        "title": "Structural investigation of the bilayer iridate Sr_3Ir_2O_7",
        "author": [
            {
                "family_name": "Hogan",
                "given_name": "Tom",
                "clpid": "Hogan-T"
            },
            {
                "family_name": "Bjaalie",
                "given_name": "Lars",
                "clpid": "Bjaalie-L"
            },
            {
                "family_name": "Zhao",
                "given_name": "Liuyan",
                "clpid": "Zhao-Liuyan"
            },
            {
                "family_name": "Belvin",
                "given_name": "Carina",
                "clpid": "Belvin-C"
            },
            {
                "family_name": "Wang",
                "given_name": "Xiaoping",
                "orcid": "0000-0001-7143-8112",
                "clpid": "Wang-Xiaoping"
            },
            {
                "family_name": "Van de Walle",
                "given_name": "Chris G.",
                "clpid": "Van-de-Walle-C-G"
            },
            {
                "family_name": "Hsieh",
                "given_name": "David",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            },
            {
                "family_name": "Wilson",
                "given_name": "Stephen D.",
                "clpid": "Wilson-S-D"
            }
        ],
        "abstract": "A complete structural solution of the bilayer iridate compound Sr_3Ir_2O_7 presently remains outstanding. Previously reported structures for this compound vary and all fail to explain weak structural violations observed in neutron scattering measurements as well as the presence of a net ferromagnetic moment in the basal plane. In this paper, we present single crystal neutron diffraction and rotational anisotropy second harmonic generation measurements unveiling a lower, monoclinic symmetry inherent to Sr_3Ir_2O_7. Combined with density functional theory, our measurements identify the correct structural space group as No. 15 (C2/c) and provide clarity regarding the local symmetry of Ir^(4+) cations within this spin-orbit Mott material.",
        "doi": "10.1103/PhysRevB.93.134110",
        "issn": "2469-9950",
        "publisher": "American Physical Society",
        "publication": "Physical Review B",
        "publication_date": "2016-04-01",
        "series_number": "13",
        "volume": "93",
        "issue": "13",
        "pages": "Art. No. 134110"
    },
    {
        "id": "authors:4qbrp-cjf05",
        "collection": "authors",
        "collection_id": "4qbrp-cjf05",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20160401-095101047",
        "type": "article",
        "title": "Nonlinear and time-resolved optical study of the 112-type iron-based superconductor parent Ca_(1\u2212x)La_xFeAs_2 across its structural phase transition",
        "author": [
            {
                "family_name": "Harter",
                "given_name": "J. W.",
                "orcid": "0000-0002-7146-9370",
                "clpid": "Harter-J-W"
            },
            {
                "family_name": "Chu",
                "given_name": "H.",
                "orcid": "0000-0002-1989-9517",
                "clpid": "Chu-Hao"
            },
            {
                "family_name": "Jiang",
                "given_name": "S.",
                "clpid": "Jiang-S"
            },
            {
                "family_name": "Ni",
                "given_name": "N.",
                "clpid": "Ni-N"
            },
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            }
        ],
        "abstract": "The newly discovered 112-type ferropnictide superconductors contain chains of As atoms that break the tetragonal symmetry between the \u0251 and b axes. This feature eliminates the need for uniaxial strain that is usually required to stabilize large single domains in the electronic nematic state that exists in the vicinity of magnetic order in the iron-based superconductors. We report detailed structural symmetry measurements of 112-type Ca_(0.73)La_(0.27)FeAs_2 using rotational anisotropy optical second-harmonic generation. This technique is complementary to diffraction experiments and enables a precise determination of the point-group symmetry of a crystal. By combining our measurements with density functional theory calculations, we uncover a strong optical second-harmonic response of bulk electric dipole origin from the Fe and Ca 3d-derived states that enables us to assign C_2 as the crystallographic point group. This makes the 112-type materials high-temperature superconductors without a center of inversion, allowing for the possible mixing of singlet and triplet Cooper pairs in the superconducting state. We also perform pump-probe transient reflectivity experiments that reveal a 4.6-THz phonon mode associated with the out-of-plane motion of As atoms in the FeAs layers. We do not observe any suppression of the optical second-harmonic response or shift in the phonon frequency upon cooling through the reported monoclinic-to-triclinic transition at 58 K. This allows us to identify C_1 as the low-temperature crystallographic point group but suggests that structural changes induced by long-range magnetic order are subtle and do not significantly affect electronic states near the Fermi level.",
        "doi": "10.1103/PhysRevB.93.104506",
        "issn": "1098-0121",
        "publisher": "American Physical Society",
        "publication": "Physical Review B",
        "publication_date": "2016-03-07",
        "series_number": "10",
        "volume": "93",
        "issue": "10",
        "pages": "Art. No. 104506"
    },
    {
        "id": "authors:gnrnh-z3m69",
        "collection": "authors",
        "collection_id": "gnrnh-z3m69",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20150914-110119511",
        "type": "article",
        "title": "Evidence of an odd-parity hidden order in a spin\u2013orbit coupled correlated iridate",
        "author": [
            {
                "family_name": "Zhao",
                "given_name": "L.",
                "clpid": "Zhao-Liyuan"
            },
            {
                "family_name": "Torchinsky",
                "given_name": "D. H.",
                "clpid": "Torchinsky-D-H"
            },
            {
                "family_name": "Chu",
                "given_name": "H.",
                "orcid": "0000-0002-1989-9517",
                "clpid": "Chu-Hao"
            },
            {
                "family_name": "Ivanov",
                "given_name": "V.",
                "clpid": "Ivanov-V-M"
            },
            {
                "family_name": "Lifshitz",
                "given_name": "R.",
                "orcid": "0000-0002-8829-5506",
                "clpid": "Lifshitz-R"
            },
            {
                "family_name": "Flint",
                "given_name": "R.",
                "clpid": "Flint-R"
            },
            {
                "family_name": "Qi",
                "given_name": "T.",
                "clpid": "Qi-Tongfei"
            },
            {
                "family_name": "Cao",
                "given_name": "G.",
                "clpid": "Cao-Gang"
            },
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            }
        ],
        "abstract": "A rare combination of strong spin\u2013orbit coupling and electron\u2013electron correlations makes the iridate Mott insulator Sr_2IrO_4 a promising host for novel electronic phases of matter. The resemblance of its crystallographic, magnetic and electronic structures to La_2CuO_4, as well as the emergence on doping of a pseudogap region and a low-temperature d-wave gap, has particularly strengthened analogies to cuprate high-T_c superconductors. However, unlike the cuprate phase diagram, which features a plethora of broken symmetry phases in a pseudogap region that includes charge density wave, stripe, nematic and possibly intra-unit-cell loop-current orders, no broken symmetry phases proximate to the parent antiferromagnetic Mott insulating phase in Sr_2IrO_4 have been observed so far, making the comparison of iridate to cuprate phenomenology incomplete. Using optical second-harmonic generation, we report evidence of a hidden non-dipolar magnetic order in Sr_2IrO_4 that breaks both the spatial inversion and rotational symmetries of the underlying tetragonal lattice. Four distinct domain types corresponding to discrete 90\u00b0-rotated orientations of a pseudovector order parameter are identified using nonlinear optical microscopy, which is expected from an electronic phase that possesses the symmetries of a magneto-electric loop-current order. The onset temperature of this phase is monotonically suppressed with bulk hole doping, albeit much more weakly than the N\u00e9el temperature, revealing an extended region of the phase diagram with purely hidden order. Driving this hidden phase to its quantum critical point may be a path to realizing superconductivity in Sr_2IrO_4.",
        "doi": "10.1038/nphys3517",
        "issn": "1745-2473",
        "publisher": "Nature Publishing Group",
        "publication": "Nature Physics",
        "publication_date": "2016-01",
        "series_number": "1",
        "volume": "12",
        "issue": "1",
        "pages": "32-36"
    },
    {
        "id": "authors:hbdc2-7qs03",
        "collection": "authors",
        "collection_id": "hbdc2-7qs03",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20151207-094335828",
        "type": "article",
        "title": "High-speed measurement of rotational anisotropy nonlinear optical harmonic generation using position-sensitive detection",
        "author": [
            {
                "family_name": "Harter",
                "given_name": "J. W.",
                "orcid": "0000-0002-7146-9370",
                "clpid": "Harter-J-W"
            },
            {
                "family_name": "Niu",
                "given_name": "L.",
                "clpid": "Niu-L"
            },
            {
                "family_name": "Woss",
                "given_name": "A. J.",
                "clpid": "Woss-A-J"
            },
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            }
        ],
        "abstract": "We present a method of performing high-speed rotational anisotropy nonlinear optical harmonic generation experiments at rotational frequencies of several hertz by projecting the harmonic light reflected at different angles from a sample onto a stationary position-sensitive detector. The high rotational speed of the technique, 103 to 104 times larger than existing methods, permits precise measurements of the crystallographic and electronic symmetries of samples by averaging over low frequency laser-power, beam-pointing, and pulse-width fluctuations. We demonstrate the sensitivity of our technique by resolving the bulk fourfold rotational symmetry of GaAs about its [001] axis using second-harmonic generation.",
        "doi": "10.1364/OL.40.004671",
        "issn": "0146-9592",
        "publisher": "Optical Society of America",
        "publication": "Optics Letters",
        "publication_date": "2015-10-15",
        "series_number": "20",
        "volume": "40",
        "issue": "20",
        "pages": "4671-4674"
    },
    {
        "id": "authors:mbrcb-1ky55",
        "collection": "authors",
        "collection_id": "mbrcb-1ky55",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20141117-101456748",
        "type": "article",
        "title": "Structural Distortion-Induced Magnetoelastic Locking in Sr_2IrO_4 Revealed through Nonlinear Optical Harmonic Generation",
        "author": [
            {
                "family_name": "Torchinsky",
                "given_name": "D. H.",
                "clpid": "Torchinsky-D-H"
            },
            {
                "family_name": "Chu",
                "given_name": "H.",
                "orcid": "0000-0002-1989-9517",
                "clpid": "Chu-Hao"
            },
            {
                "family_name": "Zhao",
                "given_name": "L.",
                "clpid": "Zhao-L"
            },
            {
                "family_name": "Perkins",
                "given_name": "N. B.",
                "clpid": "Perkins-N-B"
            },
            {
                "family_name": "Sizyuk",
                "given_name": "Y.",
                "clpid": "Sizyuk-Y"
            },
            {
                "family_name": "Qi",
                "given_name": "T.",
                "clpid": "Qi-Tongfei"
            },
            {
                "family_name": "Cao",
                "given_name": "G.",
                "clpid": "Cao-Gang"
            },
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            }
        ],
        "abstract": "We report a global structural distortion in Sr2IrO4 using spatially resolved optical second and third harmonic generation rotational anisotropy measurements. A symmetry lowering from an I4_1/acd to I4_1/a space group is observed both above and below the N\u00e9el temperature that arises from a staggered tetragonal distortion of the oxygen octahedra. By studying an effective superexchange Hamiltonian that accounts for this lowered symmetry, we find that perfect locking between the octahedral rotation and magnetic moment canting angles can persist even in the presence of large noncubic local distortions. Our results explain the origin of the forbidden Bragg peaks recently observed in neutron diffraction experiments and reconcile the observations of strong tetragonal distortion and perfect magnetoelastic locking in Sr_2IrO_4.",
        "doi": "10.1103/PhysRevLett.114.096404",
        "issn": "0031-9007",
        "publisher": "American Physical Society",
        "publication": "Physical Review Letters",
        "publication_date": "2015-03-06",
        "series_number": "9",
        "volume": "114",
        "issue": "9",
        "pages": "Art. No. 096404"
    },
    {
        "id": "authors:bhh69-yt438",
        "collection": "authors",
        "collection_id": "bhh69-yt438",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140717-142502645",
        "type": "article",
        "title": "A Low Temperature Nonlinear Optical Rotational Anisotropy Spectrometer for the Determination of Crystallographic and Electronic Symmetries",
        "author": [
            {
                "family_name": "Torchinsky",
                "given_name": "Darius H.",
                "clpid": "Torchinsky-D-H"
            },
            {
                "family_name": "Chu",
                "given_name": "Hao",
                "orcid": "0000-0002-1989-9517",
                "clpid": "Chu-Hao"
            },
            {
                "family_name": "Qi",
                "given_name": "Tongfei",
                "clpid": "Qi-Tongfei"
            },
            {
                "family_name": "Cao",
                "given_name": "Gang",
                "clpid": "Cao-Gang"
            },
            {
                "family_name": "Hsieh",
                "given_name": "David",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            }
        ],
        "abstract": "Nonlinear optical generation from a crystalline material can reveal the symmetries of both its lattice structure and underlying ordered electronic phases and can therefore be exploited as a complementary technique to diffraction based scattering probes. Although this technique has been successfully used to study the lattice and magnetic structures of systems such as semiconductor surfaces, multiferroic crystals, magnetic thin films, and multilayers, challenging technical requirements have prevented its application to the plethora of complex electronic phases found in strongly correlated electron systems. These requirements include an ability to probe small bulk single crystals at the \u03bcm length scale, a need for sensitivity to the entire nonlinear optical susceptibility tensor, oblique light incidence reflection geometry, and incident light frequency tunability among others. These measurements are further complicated by the need for extreme sample environments such as ultra low temperatures, high magnetic fields, or high pressures. In this review we present a novel experimental construction using a rotating light scattering plane that meets all the aforementioned requirements. We demonstrate the efficacy of our scheme by making symmetry measurements on a \u03bcm scale facet of a small bulk single crystal of Sr_2IrO_4 using optical second and third harmonic generation.",
        "doi": "10.1063/1.4891417",
        "issn": "0034-6748",
        "publisher": "American Institute of Physics",
        "publication": "Review of Scientific Instruments",
        "publication_date": "2014-08",
        "series_number": "8",
        "volume": "85",
        "issue": "8",
        "pages": "Art. No. 083102"
    },
    {
        "id": "authors:2vwm6-2xb11",
        "collection": "authors",
        "collection_id": "2vwm6-2xb11",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140813-105943474",
        "type": "article",
        "title": "Measurement of Intrinsic Dirac Fermion Cooling on the Surface of the Topological Insulator Bi_2Se_3 Using Time-Resolved and Angle-Resolved Photoemission Spectroscopy",
        "author": [
            {
                "family_name": "Wang",
                "given_name": "Y. H.",
                "clpid": "Wang-Y-H"
            },
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            },
            {
                "family_name": "Sie",
                "given_name": "E. J.",
                "clpid": "Sie-E-J"
            },
            {
                "family_name": "Steinberg",
                "given_name": "H.",
                "clpid": "Steinberg-H"
            },
            {
                "family_name": "Gardner",
                "given_name": "D. R.",
                "clpid": "Gardner-D-R"
            },
            {
                "family_name": "Lee",
                "given_name": "Y. S.",
                "clpid": "Lee-Y-S"
            },
            {
                "family_name": "Jarillo-Herrero",
                "given_name": "P.",
                "clpid": "Jarillo-Herrero-P"
            },
            {
                "family_name": "Gedik",
                "given_name": "N.",
                "clpid": "Gedik-N"
            }
        ],
        "abstract": "We perform time- and angle-resolved photoemission spectroscopy of a prototypical topological insulator (TI) Bi_2Se_3 to study the ultrafast dynamics of surface and bulk electrons after photoexcitation. By analyzing the evolution of surface states and bulk band spectra, we obtain their electronic temperature and chemical potential relaxation dynamics separately. These dynamics reveal strong phonon-assisted surface-bulk coupling at high lattice temperature and total suppression of inelastic scattering between the surface and the bulk at low lattice temperature. In this low temperature regime, the unique cooling of Dirac fermions in TI by acoustic phonons is manifested through a power law dependence of the surface temperature decay rate on carrier density.",
        "doi": "10.1103/PhysRevLett.109.127401",
        "issn": "0031-9007",
        "publisher": "American Physical Society",
        "publication": "Physical Review Letters",
        "publication_date": "2012-09-21",
        "series_number": "12",
        "volume": "109",
        "issue": "12",
        "pages": "Art. No. 127401"
    },
    {
        "id": "authors:magf8-qq882",
        "collection": "authors",
        "collection_id": "magf8-qq882",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140813-113900066",
        "type": "article",
        "title": "Observation of a metal-to-insulator transition with both Mott-Hubbard and Slater characteristics in Sr_2IrO_4 from time-resolved photocarrier dynamics",
        "author": [
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            },
            {
                "family_name": "Mahmood",
                "given_name": "F.",
                "clpid": "Mahmood-F"
            },
            {
                "family_name": "Torchinsky",
                "given_name": "D. H.",
                "clpid": "Torchinsky-D-H"
            },
            {
                "family_name": "Cao",
                "given_name": "G.",
                "clpid": "Cao-Gang"
            },
            {
                "family_name": "Gedik",
                "given_name": "N.",
                "clpid": "Gedik-N"
            }
        ],
        "abstract": "We perform a time-resolved optical study of Sr_2IrO_4 to understand the influence of magnetic ordering on the low energy electronic structure of a strongly spin-orbit coupled J_(eff) = 1/2 Mott insulator. By studying the recovery dynamics of photoexcited carriers, we find that upon cooling through the N\u00e9el temperature T_N the system evolves continuously from a metal-like phase with fast (\u223c50 fs) and excitation density independent relaxation dynamics to a gapped phase characterized by slower (\u223c500 fs) excitation density-dependent bimolecular recombination dynamics, which is a hallmark of a Slater-type metal-to-insulator transition. However our data indicate that the high energy reflectivity associated with optical transitions into the unoccupied J_(eff) = 1/2 band undergoes the sharpest upturn at TN, which is consistent with a Mott-Hubbard type metal-to-insulator transition involving spectral weight transfer into an upper Hubbard band. These findings show Sr_2IrO_4 to be a unique system in which Slater- and Mott-Hubbard-type behaviors coexist and naturally explain the absence of anomalies at T_N in transport and thermodynamic measurements.",
        "doi": "10.1103/PhysRevB.86.035128",
        "issn": "1098-0121",
        "publisher": "American Physical Society",
        "publication": "Physical Review B",
        "publication_date": "2012-07-15",
        "series_number": "3",
        "volume": "86",
        "issue": "3",
        "pages": "035128"
    },
    {
        "id": "authors:52bw6-gm871",
        "collection": "authors",
        "collection_id": "52bw6-gm871",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140813-113027377",
        "type": "article",
        "title": "Theoretical and experimental study of second harmonic generation from the surface of the topological insulator Bi_2Se_3",
        "author": [
            {
                "family_name": "McIver",
                "given_name": "J. W.",
                "clpid": "McIver-J-W"
            },
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            },
            {
                "family_name": "Drapcho",
                "given_name": "S. G.",
                "clpid": "Drapcho-S-G"
            },
            {
                "family_name": "Torchinsky",
                "given_name": "D. H.",
                "clpid": "Torchinsky-D-H"
            },
            {
                "family_name": "Gardner",
                "given_name": "D. R.",
                "clpid": "Gardner-D-R"
            },
            {
                "family_name": "Lee",
                "given_name": "Y. S.",
                "clpid": "Lee-Y-S"
            },
            {
                "family_name": "Gedik",
                "given_name": "N.",
                "clpid": "Gedik-N"
            }
        ],
        "abstract": "We develop a theoretical model that describes the second harmonic generation of light from the surface of the topological insulator Bi_2Se_3 and experimentally demonstrate that the technique is sensitive to the surface electrons. By performing a crystal symmetry analysis of Bi_2Se_3 (111) we determine the nonlinear electric susceptibility tensor elements that give rise to second harmonic generation. Using these results, we present a phenomenological model that shows that the relative magnitudes of these tensor elements can be determined by measuring the polarization and intensity of the radiated second harmonic light as a function of the in-plane crystal orientation and incident laser polarization. We describe optical techniques capable of isolating second harmonic light and, using these techniques, we measure the first-order linear optical and second-order nonlinear optical responses as a function of crystal orientation and laser polarization on bulk single crystals of Bi_2Se_3 (111). The experimental results are consistent with our theoretical description. By comparing the data to our theoretical model we determine that a portion of the measured second harmonic light originates from the accumulation region of Bi_2Se_3 (111), which we confirm by performing surface doping-dependent studies. Our results show that second harmonic generation is a promising tool for spectroscopic studies of topological surfaces and buried interfaces.",
        "doi": "10.1103/PhysRevB.86.035327",
        "issn": "1098-0121",
        "publisher": "American Physical Society",
        "publication": "Physical Review B",
        "publication_date": "2012-07-15",
        "series_number": "3",
        "volume": "86",
        "issue": "3",
        "pages": "Art. No. 035327"
    },
    {
        "id": "authors:psb5d-1v056",
        "collection": "authors",
        "collection_id": "psb5d-1v056",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140813-115757588",
        "type": "article",
        "title": "Control over topological insulator photocurrents with light polarization",
        "author": [
            {
                "family_name": "McIver",
                "given_name": "J. W.",
                "clpid": "McIver-J-W"
            },
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            },
            {
                "family_name": "Steinberg",
                "given_name": "H.",
                "clpid": "Steinberg-H"
            },
            {
                "family_name": "Jarillo-Herrero",
                "given_name": "P.",
                "clpid": "Jarillo-Herrero-P"
            },
            {
                "family_name": "Gedik",
                "given_name": "N.",
                "clpid": "Gedik-N"
            }
        ],
        "abstract": "Three-dimensional topological insulators represent a new\nquantum phase of matter with spin-polarized surface states \nthat are protected from backscattering. The static electronic\nproperties of these surface states have been comprehensively\nimaged by both photoemission and tunnelling spectroscopies. Theorists have proposed that topological surface states can also exhibit novel electronic responses to light, such as topological quantum phase transitions and spin-polarized electrical currents. However, the effects of optically driving a topological insulator out of equilibrium have remained largely unexplored experimentally, and no photocurrents have been measured. Here, we show that illuminating the topological insulator Bi_2Se_3 with circularly polarized light generates a\nphotocurrent that originates from topological helical Dirac fermions, and that reversing the helicity of the light reverses the direction of the photocurrent. We also observe a photocurrent that is controlled by the linear polarization of light and argue that it may also have a topological surface state origin. This approach may allow the probing of dynamic properties of topological insulators and lead to novel opto-spintronic devices.",
        "doi": "10.1038/nnano.2011.214",
        "issn": "1748-3387",
        "publisher": "Nature Publishing Group",
        "publication": "Nature Nanotechnology",
        "publication_date": "2012-02",
        "series_number": "2",
        "volume": "7",
        "issue": "2",
        "pages": "96-100"
    },
    {
        "id": "authors:sk98s-2xw20",
        "collection": "authors",
        "collection_id": "sk98s-2xw20",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140813-121709306",
        "type": "article",
        "title": "Observation of a Warped Helical Spin Texture in Bi_2Se_3 from Circular Dichroism Angle-Resolved Photoemission Spectroscopy",
        "author": [
            {
                "family_name": "Wang",
                "given_name": "Y. H.",
                "clpid": "Wang-Y-H"
            },
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            },
            {
                "family_name": "Pilon",
                "given_name": "D.",
                "clpid": "Pilon-D"
            },
            {
                "family_name": "Fu",
                "given_name": "L.",
                "clpid": "Fu-L"
            },
            {
                "family_name": "Gardner",
                "given_name": "D. R.",
                "clpid": "Gardner-D-R"
            },
            {
                "family_name": "Lee",
                "given_name": "Y. S.",
                "clpid": "Lee-Y-S"
            },
            {
                "family_name": "Gedik",
                "given_name": "N.",
                "clpid": "Gedik-N"
            }
        ],
        "abstract": "A differential coupling of topological surface states to left- versus right-circularly polarized light is the basis of many optospintronics applications of topological insulators. Here we report direct evidence of circular dichroism from the surface states of Bi_2Se_3 using laser-based time-of-flight angle-resolved photoemission spectroscopy. By employing a novel sample rotational analysis, we resolve unusual modulations in the circular dichroism photoemission pattern as a function of both energy and momentum, which perfectly mimic the predicted but hitherto unobserved three-dimensional warped spin texture of the surface states. By developing a microscopic theory of photoemission from topological surface states, we show that this correlation is a natural consequence of spin-orbit coupling. These results suggest that our technique may be a powerful probe of the spin texture of spin-orbit coupled materials in general.",
        "doi": "10.1103/PhysRevLett.107.207602",
        "issn": "0031-9007",
        "publisher": "American Physical Society",
        "publication": "Physical Review Letters",
        "publication_date": "2011-11-11",
        "series_number": "20",
        "volume": "107",
        "issue": "20",
        "pages": "Art. No. 207602"
    },
    {
        "id": "authors:pqwqz-0wp34",
        "collection": "authors",
        "collection_id": "pqwqz-0wp34",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140815-104401227",
        "type": "article",
        "title": "Nonequilibrium quasiparticle relaxation dynamics in single crystals of hole- and electron-doped BaFe_2As_2",
        "author": [
            {
                "family_name": "Torchinsky",
                "given_name": "D. H.",
                "clpid": "Torchinsky-D-H"
            },
            {
                "family_name": "McIver",
                "given_name": "James  W.",
                "clpid": "McIver-J-W"
            },
            {
                "family_name": "Hsieh",
                "given_name": "David",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            },
            {
                "family_name": "Chen",
                "given_name": "G. F.",
                "clpid": "Chen-G-F"
            },
            {
                "family_name": "Luo",
                "given_name": "J. L.",
                "clpid": "Luo-J-L"
            },
            {
                "family_name": "Wang",
                "given_name": "N. L.",
                "clpid": "Wang-N-L"
            },
            {
                "family_name": "Gedik",
                "given_name": "Nuh",
                "clpid": "Gedik-N"
            }
        ],
        "abstract": "We report on the nonequilibrium quasiparticle dynamics in BaFe_2As_2 on both the hole-doped (Ba_(1\u2212x)K_xFe_2As_2) and electron-doped (BaFe2\u2212yCoyAs2) sides of the phase diagram using ultrafast pump-probe spectroscopy. Below Tc, measurements conducted at low photoinjected quasiparticle densities in the optimally and overdoped Ba1\u2212xKxFe2As2 samples reveal two distinct relaxation processes: a fast component whose decay rate increases linearly with excitation density and a slow component with an excitation density independent decay rate. We argue that these two processes reflect the recombination of quasiparticles in the two hole bands through intraband and interband processes. We also find that the thermal recombination rate of quasiparticles increases quadratically with temperature in these samples. The temperature and excitation density dependence of the decays indicates fully gapped hole bands and nodal or very anisotropic electron bands. At higher excitation densities and lower hole dopings, the dependence of the dynamics on quasiparticle density disappears as the data are more readily understood in terms of a model which accounts for the quasiequilibrium temperature attained by the sample. In the BaFe_(2\u2212y)Co_yAs_2 samples, dependence of the recombination rate on quasiparticle density at low dopings (i.e., y=0.12) is suppressed upon submergence of the inner hole band and quasiparticle relaxation occurs in a slow, density-independent manner.",
        "doi": "10.1103/PhysRevB.84.104518",
        "issn": "1098-0121",
        "publisher": "American Physical Society",
        "publication": "Physical Review B",
        "publication_date": "2011-09-01",
        "series_number": "10",
        "volume": "84",
        "issue": "10",
        "pages": "Art. No. 104518"
    },
    {
        "id": "authors:ehzt6-mh158",
        "collection": "authors",
        "collection_id": "ehzt6-mh158",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140815-110459643",
        "type": "article",
        "title": "Selective Probing of Photoinduced Charge and Spin Dynamics in the Bulk and Surface of a Topological Insulator",
        "author": [
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            },
            {
                "family_name": "Mahmood",
                "given_name": "F.",
                "clpid": "Mahmood-F"
            },
            {
                "family_name": "McIver",
                "given_name": "J. W.",
                "clpid": "McIver-J-W"
            },
            {
                "family_name": "Gardner",
                "given_name": "D. R.",
                "clpid": "Gardner-D-R"
            },
            {
                "family_name": "Lee",
                "given_name": "Y. S.",
                "clpid": "Lee-Y-S"
            },
            {
                "family_name": "Gedik",
                "given_name": "N.",
                "clpid": "Gedik-N"
            }
        ],
        "abstract": "Topological insulators possess completely different spin-orbit coupled bulk and surface electronic spectra that are each predicted to exhibit exotic responses to light. Here we report time-resolved fundamental and second harmonic optical pump-probe measurements on the topological insulator Bi_2Se_3 to independently measure its photoinduced charge and spin dynamics with bulk and surface selectivity. Our results show that a transient net spin density can be optically induced in both the bulk and surface, which may drive spin transport in topological insulators. By utilizing a novel rotational anisotropy analysis we are able to separately resolve the spin depolarization, intraband cooling, and interband recombination processes following photoexcitation, which reveal that spin and charge degrees of freedom relax on very different time scales owing to strong spin-orbit coupling.",
        "doi": "10.1103/PhysRevLett.107.077401",
        "issn": "0031-9007",
        "publisher": "American Physical Society",
        "publication": "Physical Review Letters",
        "publication_date": "2011-08-12",
        "series_number": "7",
        "volume": "107",
        "issue": "7",
        "pages": "Art. No. 077401"
    },
    {
        "id": "authors:0sgwr-8vb22",
        "collection": "authors",
        "collection_id": "0sgwr-8vb22",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140815-131510654",
        "type": "article",
        "title": "Nonlinear Optical Probe of Tunable Surface Electrons on a Topological Insulator",
        "author": [
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            },
            {
                "family_name": "McIver",
                "given_name": "J. W.",
                "clpid": "McIver-J-W"
            },
            {
                "family_name": "Torchinsky",
                "given_name": "D. H.",
                "clpid": "Torchinsky-D-H"
            },
            {
                "family_name": "Gardner",
                "given_name": "D. R.",
                "clpid": "Gardner-D-R"
            },
            {
                "family_name": "Lee",
                "given_name": "Y. S.",
                "clpid": "Lee-Y-S"
            },
            {
                "family_name": "Gedik",
                "given_name": "N.",
                "clpid": "Gedik-N"
            }
        ],
        "abstract": "We use ultrafast laser pulses to experimentally demonstrate that the second-order optical response of bulk single crystals of the topological insulator Bi_2Se_3 is sensitive to its surface electrons. By performing surface doping dependence measurements as a function of photon polarization and sample orientation we show that second harmonic generation can simultaneously probe both the surface crystalline structure and the surface charge of Bi_2Se_3. Furthermore, we find that second harmonic generation using circularly polarized photons reveals the time-reversal symmetry properties of the system and is surprisingly robust against surface charging, which makes it a promising tool for spectroscopic studies of topological surfaces and buried interfaces.",
        "doi": "10.1103/PhysRevLett.106.057401",
        "issn": "0031-9007",
        "publisher": "American Physical Society",
        "publication": "Physical Review Letters",
        "publication_date": "2011-02-04",
        "series_number": "5",
        "volume": "106",
        "issue": "5",
        "pages": "Art. No. 057401"
    },
    {
        "id": "authors:6wh9p-e2h21",
        "collection": "authors",
        "collection_id": "6wh9p-e2h21",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140815-133452212",
        "type": "article",
        "title": "A topological insulator surface under strong Coulomb, magnetic and disorder perturbations",
        "author": [
            {
                "family_name": "Wray",
                "given_name": "L. Andrew",
                "clpid": "Wray-L-A"
            },
            {
                "family_name": "Xu",
                "given_name": "Su-Yang",
                "clpid": "Xu-Su-Yang"
            },
            {
                "family_name": "Xia",
                "given_name": "Yuqi",
                "clpid": "Xia-Yuqi"
            },
            {
                "family_name": "Hsieh",
                "given_name": "David",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            },
            {
                "family_name": "Fedorov",
                "given_name": "Alexei V.",
                "clpid": "Fedorov-A-V"
            },
            {
                "family_name": "Hor",
                "given_name": "Yew San",
                "clpid": "Hor-Yew-San"
            },
            {
                "family_name": "Cava",
                "given_name": "Robert J.",
                "clpid": "Cava-Robert-J"
            },
            {
                "family_name": "Bansil",
                "given_name": "Arun",
                "clpid": "Bansil-Arun"
            },
            {
                "family_name": "Lin",
                "given_name": "Hsin",
                "clpid": "Lin-Hsin"
            },
            {
                "family_name": "Hasan",
                "given_name": "M. Zahid",
                "clpid": "Hasan-M-Zahid"
            }
        ],
        "abstract": "Topological insulators embody a state of bulk matter characterized by spin-momentum-locked surface states that span the bulk bandgap. This highly unusual surface spin environment provides a rich ground for uncovering new phenomena. Understanding the response of a topological surface to strong Coulomb perturbations represents a frontier in discovering the interacting and emergent many-body physics of topological surfaces. Here we present the first controlled study of topological insulator surfaces under Coulomb and magnetic perturbations. We have used time-resolved deposition of iron, with a large Coulomb charge and significant magnetic moment, to systematically modify the topological spin structure of the Bi_2Se_3 surface. We observe that such perturbation leads to the creation of odd multiples of Dirac fermions and that magnetic interactions break time-reversal symmetry in the presence of band hybridizations. We present a theoretical model to account for the observed electron dynamics of the topological surface. Taken collectively, these results are a critical guide in controlling electron mobility and quantum behaviour of topological surfaces, not only for device applications but also in setting the stage for creating exotic particles such as axions or imaging monopoles on the surface.",
        "doi": "10.1038/nphys1838",
        "issn": "1745-2473",
        "publisher": "Nature Publishing Group",
        "publication": "Nature Physics",
        "publication_date": "2011-01",
        "series_number": "1",
        "volume": "7",
        "issue": "1",
        "pages": "32-37"
    },
    {
        "id": "authors:pzm39-zh383",
        "collection": "authors",
        "collection_id": "pzm39-zh383",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140815-135044188",
        "type": "article",
        "title": "Direct observation of spin-polarized surface states in the parent compound of a topological insulator using spin- and angle-resolved photoemission spectroscopy in a Mott-polarimetry mode",
        "author": [
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            },
            {
                "family_name": "Wray",
                "given_name": "L.",
                "clpid": "Wray-L-A"
            },
            {
                "family_name": "Qian",
                "given_name": "D.",
                "clpid": "Qian-Dong"
            },
            {
                "family_name": "Xia",
                "given_name": "Y.",
                "clpid": "Xia-Yuqi"
            },
            {
                "family_name": "Dil",
                "given_name": "J. H.",
                "clpid": "Dil-J-H"
            },
            {
                "family_name": "Meier",
                "given_name": "F.",
                "clpid": "Meier-F"
            },
            {
                "family_name": "Patthey",
                "given_name": "L.",
                "clpid": "Patthey-L"
            },
            {
                "family_name": "Osterwalder",
                "given_name": "J.",
                "clpid": "Osterwalder-J"
            },
            {
                "family_name": "Bihlmayer",
                "given_name": "G.",
                "orcid": "0000-0002-6615-1122",
                "clpid": "Bihlmayer-G"
            },
            {
                "family_name": "Hor",
                "given_name": "Y. S.",
                "clpid": "Hor-Yew-San"
            },
            {
                "family_name": "Cava",
                "given_name": "R. J.",
                "clpid": "Cava-Robert-J"
            },
            {
                "family_name": "Hasan",
                "given_name": "M. Z.",
                "clpid": "Hasan-M-Zihad"
            }
        ],
        "abstract": "We report high-resolution spin-resolved photoemission spectroscopy (spin-ARPES) measurements on the parent compound Sb of the recently discovered three-dimensional topological insulator Bi_(1\u2013x)Sb_x (Hsieh et al 2008 Nature 452 970, Hsieh et al 2009 Science 323 919). By modulating the incident photon energy, we are able to map both the bulk and the (111) surface band structure, from which we directly demonstrate that the surface bands are spin polarized by the spin\u2013orbit interaction and connect the bulk valence and conduction bands in a topologically non-trivial way. A unique asymmetric Dirac surface state gives rise to a k-splitting of its spin-polarized electronic channels. These results complement our previously published works on this class of materials and re-confirm our discovery of topological insulator states in the Bi_(1\u2013x)Sb_x series.",
        "doi": "10.1088/1367-2630/12/12/125001",
        "issn": "1367-2630",
        "publisher": "IOP",
        "publication": "New Journal of Physics",
        "publication_date": "2010-12",
        "series_number": "12",
        "volume": "12",
        "issue": "12",
        "pages": "Art. No. 125001"
    },
    {
        "id": "authors:71zsm-wb886",
        "collection": "authors",
        "collection_id": "71zsm-wb886",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140815-144158820",
        "type": "article",
        "title": "Development of ferromagnetism in the doped topological insulator Bi_(2\u2212x)Mn_xTe_3",
        "author": [
            {
                "family_name": "Hor",
                "given_name": "Y. S.",
                "clpid": "Hor-Yew-San"
            },
            {
                "family_name": "Roushan",
                "given_name": "P.",
                "clpid": "Roushan-P"
            },
            {
                "family_name": "Beidenhopf",
                "given_name": "H.",
                "clpid": "Beidenkopf-H"
            },
            {
                "family_name": "Seo",
                "given_name": "J.",
                "orcid": "0000-0002-0442-288X",
                "clpid": "Seo-Jungpil"
            },
            {
                "family_name": "Qu",
                "given_name": "D.",
                "clpid": "Qu-D"
            },
            {
                "family_name": "Checkelsky",
                "given_name": "J. G.",
                "clpid": "Checkelsky-J-G"
            },
            {
                "family_name": "Wray",
                "given_name": "L. A.",
                "clpid": "Wray-L-A"
            },
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            },
            {
                "family_name": "Xia",
                "given_name": "Y.",
                "clpid": "Xia-Yuqi"
            },
            {
                "family_name": "Xu",
                "given_name": "S.-Y.",
                "clpid": "Xu-Su-Yang"
            },
            {
                "family_name": "Qian",
                "given_name": "D.",
                "clpid": "Qian-Dong"
            },
            {
                "family_name": "Hasan",
                "given_name": "M. Z.",
                "clpid": "Hasan-M-Zihad"
            },
            {
                "family_name": "Ong",
                "given_name": "N. P.",
                "clpid": "Ong-N-P"
            },
            {
                "family_name": "Yazdani",
                "given_name": "A.",
                "clpid": "Yazdani-Ali"
            },
            {
                "family_name": "Cava",
                "given_name": "R. J.",
                "clpid": "Cava-Robert-J"
            }
        ],
        "abstract": "The development of ferromagnetism in Mn-doped Bi_2Te_3 is characterized through measurements on a series of single crystals with different Mn content. Scanning tunneling microscopy analysis shows that the Mn substitutes on the Bi sites, forming compounds of the type Bi_(2\u2212x)Mn_xTe_3, and that the Mn substitutions are randomly distributed, not clustered. Mn doping first gives rise to local magnetic moments with Curie-like behavior, but by the compositions Bi_(1.96)Mn_(0.04)Te_3 and Bi_(1.91)Mn_(0.09)Te_3, a second-order ferromagnetic transition is observed, with T_C\u223c9\u201312\u2002K. The easy axis of magnetization in the ferromagnetic phase is perpendicular to the Bi2Te3 basal plane. Thermoelectric power and Hall effect measurements show that the Mn-doped Bi_2Te_3 crystals are p-type. Angle-resolved photoemission spectroscopy measurements show that the topological surface states that are present in pristine Bi_2Te_3 are also present at 15 K in ferromagnetic Mn-doped Bi2\u2212xMnxTe3 and that the dispersion relations of the surface states are changed in a subtle fashion.",
        "doi": "10.1103/PhysRevB.81.195203",
        "issn": "1098-0121",
        "publisher": "American Physical Society",
        "publication": "Physical Review B",
        "publication_date": "2010-05-15",
        "series_number": "19",
        "volume": "81",
        "issue": "19",
        "pages": "Art. No. 195203"
    },
    {
        "id": "authors:m48dc-xtt51",
        "collection": "authors",
        "collection_id": "m48dc-xtt51",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140828-154214025",
        "type": "article",
        "title": "Observation of Time-Reversal-Protected Single-Dirac-Cone Topological-Insulator States in Bi_2Te_3 and Sb_2Te_3",
        "author": [
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            },
            {
                "family_name": "Xia",
                "given_name": "Y.",
                "clpid": "Xia-Yuqi"
            },
            {
                "family_name": "Qian",
                "given_name": "D.",
                "clpid": "Qian-Dong"
            },
            {
                "family_name": "Wray",
                "given_name": "L.",
                "clpid": "Wray-L-A"
            },
            {
                "family_name": "Meier",
                "given_name": "F.",
                "clpid": "Meier-F"
            },
            {
                "family_name": "Dil",
                "given_name": "J. H.",
                "clpid": "Dil-J-H"
            },
            {
                "family_name": "Osterwalder",
                "given_name": "J.",
                "clpid": "Osterwalder-J"
            },
            {
                "family_name": "Patthey",
                "given_name": "L.",
                "clpid": "Patthey-L"
            },
            {
                "family_name": "Fedorov",
                "given_name": "A. V.",
                "clpid": "Fedorov-A-V"
            },
            {
                "family_name": "Lin",
                "given_name": "H.",
                "clpid": "Lin-Hsin"
            },
            {
                "family_name": "Bansil",
                "given_name": "A.",
                "clpid": "Bansil-Arun"
            },
            {
                "family_name": "Grauer",
                "given_name": "D.",
                "clpid": "Grauer-D"
            },
            {
                "family_name": "Hor",
                "given_name": "Y. S.",
                "clpid": "Hor-Yew-San"
            },
            {
                "family_name": "Cava",
                "given_name": "R. J.",
                "clpid": "Cava-Robert-J"
            },
            {
                "family_name": "Hasan",
                "given_name": "M. Z.",
                "clpid": "Hasan-M-Zihad"
            }
        ],
        "abstract": "We show that the strongly spin-orbit coupled materials Bi_2Te_3 and Sb_2Te_3 and their derivatives belong to the Z_2 topological-insulator class. Using a combination of first-principles theoretical calculations and photoemission spectroscopy, we directly show that Bi_2Te_3 is a large spin-orbit-induced indirect bulk band gap (\u03b4\u223c150\u2009\u2009meV) semiconductor whose surface is characterized by a single topological spin-Dirac cone. The electronic structure of self-doped Sb_2Te_3 exhibits similar Z_2 topological properties. We demonstrate that the dynamics of spin-Dirac fermions can be controlled through systematic Mn doping, making these materials classes potentially suitable for topological device applications.",
        "doi": "10.1103/PhysRevLett.103.146401",
        "issn": "0031-9007",
        "publisher": "American Physical Society",
        "publication": "Physical Review Letters",
        "publication_date": "2009-10-02",
        "series_number": "14",
        "volume": "103",
        "issue": "14",
        "pages": "Art. No. 146401"
    },
    {
        "id": "authors:p0ene-ahg23",
        "collection": "authors",
        "collection_id": "p0ene-ahg23",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140911-161926592",
        "type": "article",
        "title": "Topological surface states protected from backscattering by chiral spin texture",
        "author": [
            {
                "family_name": "Roushan",
                "given_name": "Pedram",
                "clpid": "Roushan-P"
            },
            {
                "family_name": "Seo",
                "given_name": "Jungpil",
                "orcid": "0000-0002-0442-288X",
                "clpid": "Seo-Jungpil"
            },
            {
                "family_name": "Parker",
                "given_name": "Colin V.",
                "clpid": "Parker-C-V"
            },
            {
                "family_name": "Hor",
                "given_name": "Y. S.",
                "clpid": "Hor-Yew-San"
            },
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            },
            {
                "family_name": "Qian",
                "given_name": "Dong",
                "clpid": "Qian-Dong"
            },
            {
                "family_name": "Richardella",
                "given_name": "Anthony",
                "clpid": "Richardella-Anthny"
            },
            {
                "family_name": "Hasan",
                "given_name": "M. Z.",
                "clpid": "Hasan-M-Zihad"
            },
            {
                "family_name": "Cava",
                "given_name": "R. J.",
                "clpid": "Cava-Robert-J"
            },
            {
                "family_name": "Yazdani",
                "given_name": "Ali",
                "clpid": "Yazdani-Ali"
            }
        ],
        "abstract": "Topological insulators are a new class of insulators in which a bulk gap for electronic excitations is generated because of the strong spin\u2013orbit coupling inherent to these systems. These materials are distinguished from ordinary insulators by the presence of gapless metallic surface states, resembling chiral edge modes in quantum Hall systems, but with unconventional spin textures. A key predicted feature of such spin-textured boundary states is their insensitivity to spin-independent scattering, which is thought to protect them from backscattering and localization. Recently, experimental and theoretical efforts have provided strong evidence for the existence of both two- and three-dimensional classes of such topological insulator materials in semiconductor quantum well structures and several bismuth-based compounds, but so far experiments have not probed the sensitivity of these chiral states to scattering. Here we use scanning tunnelling spectroscopy and angle-resolved photoemission spectroscopy to visualize the gapless surface states in the three-dimensional topological insulator Bi_(1-x)Sb_x, and examine in detail the influence of scattering from disorder caused by random alloying in this compound. We show that, despite strong atomic scale disorder, backscattering between states of opposite momentum and opposite spin is absent. Our observations demonstrate that the chiral nature of these states protects the spin of the carriers. These chiral states are therefore potentially useful for spin-based electronics, in which long spin coherence is critical, and also for quantum computing applications, where topological protection can enable fault-tolerant information processing.",
        "doi": "10.1038/nature08308",
        "issn": "0028-0836",
        "publisher": "Nature Publishing Group",
        "publication": "Nature",
        "publication_date": "2009-08-27",
        "series_number": "7259",
        "volume": "460",
        "issue": "7259",
        "pages": "1106-1109"
    },
    {
        "id": "authors:xbv5y-vge71",
        "collection": "authors",
        "collection_id": "xbv5y-vge71",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140909-135533013",
        "type": "article",
        "title": "A tunable topological insulator in the spin helical Dirac transport regime",
        "author": [
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            },
            {
                "family_name": "Xia",
                "given_name": "Y.",
                "clpid": "Xia-Yuqi"
            },
            {
                "family_name": "Qian",
                "given_name": "D.",
                "clpid": "Qian-Dong"
            },
            {
                "family_name": "Wray",
                "given_name": "L.",
                "clpid": "Wray-L-A"
            },
            {
                "family_name": "Dil",
                "given_name": "J. H.",
                "clpid": "Dil-J-H"
            },
            {
                "family_name": "Meier",
                "given_name": "F.",
                "clpid": "Meier-F"
            },
            {
                "family_name": "Osterwalder",
                "given_name": "J.",
                "clpid": "Osterwalder-J"
            },
            {
                "family_name": "Patthey",
                "given_name": "L.",
                "clpid": "Patthey-L"
            },
            {
                "family_name": "Checkelsky",
                "given_name": "J. G.",
                "clpid": "Checkelsky-J-G"
            },
            {
                "family_name": "Ong",
                "given_name": "N. P.",
                "clpid": "Ong-N-P"
            },
            {
                "family_name": "Fedorov",
                "given_name": "A. V.",
                "clpid": "Fedorov-A-V"
            },
            {
                "family_name": "Lin",
                "given_name": "H.",
                "clpid": "Lin-Hsin"
            },
            {
                "family_name": "Bansil",
                "given_name": "A.",
                "clpid": "Bansil-Arun"
            },
            {
                "family_name": "Grauer",
                "given_name": "D.",
                "clpid": "Grauer-D"
            },
            {
                "family_name": "Hor",
                "given_name": "Y. S.",
                "clpid": "Hor-Yew-San"
            },
            {
                "family_name": "Cava",
                "given_name": "R. J.",
                "clpid": "Cava-Robert-J"
            },
            {
                "family_name": "Hasan",
                "given_name": "M. Z.",
                "clpid": "Hasan-M-Zihad"
            }
        ],
        "abstract": "Helical Dirac fermions\u2014charge carriers that behave as massless relativistic particles with an intrinsic angular momentum (spin) locked to its translational momentum\u2014are proposed to be the key to realizing fundamentally new phenomena in condensed matter physics. Prominent examples include the anomalous quantization of magneto-electric coupling, half-fermion states that are their own antiparticle, and charge fractionalization in a Bose\u2013 Einstein condensate, all of which are not possible with conventional Dirac fermions of the graphene variety. Helical Dirac fermions have so far remained elusive owing to the lack of necessary spin-sensitive measurements and because such fermions are forbidden to exist in conventional materials harbouring relativistic electrons, such as graphene or bismuth. It has recently\nbeen proposed that helical Dirac fermions may exist at the edges of certain types of topologically ordered insulators\u2014materials with a bulk insulating gap of spin\u2013orbit origin and surface states protected against scattering by time-reversal symmetry\u2014and that their peculiar properties may be accessed provided the insulator is tuned into the so-called topological transport regime. However, helical Dirac fermions have not been observed in existing topological insulators. Here we report the realization and characterization of a tunable topological insulator in a bismuthbased class of material by combining spin-imaging and\nmomentum-resolved spectroscopies, bulk charge compensation,\nHall transport measurements and surface quantum control. Our\nresults reveal a spin-momentum locked Dirac cone carrying a nontrivial\nBerry's phase that is nearly 100 per cent spin-polarized,\nwhich exhibits a tunable topological fermion density in the vicinity\nof the Kramers point and can be driven to the long-sought\ntopological spin transport regime. The observed topological nodal\nstate is shown to be protected even up to 300 K. Our demonstration\nof room-temperature topological order and non-trivial spintexture\nin stoichiometric Bi_2Se_3.M_x (M_x indicates surface doping\nor gating control) paves the way for future graphene-like studies of\ntopological insulators, and applications of the observed spinpolarized\nedge channels in spintronic and computing technologies\npossibly at room temperature.",
        "doi": "10.1038/nature08234",
        "issn": "0028-0836",
        "publisher": "Nature Publishing Group",
        "publication": "Nature",
        "publication_date": "2009-08-20",
        "series_number": "7259",
        "volume": "460",
        "issue": "7259",
        "pages": "1101-1105"
    },
    {
        "id": "authors:xq5gw-5mr43",
        "collection": "authors",
        "collection_id": "xq5gw-5mr43",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140828-183436105",
        "type": "article",
        "title": "Fermi Surface Topology and Low-Lying Quasiparticle Dynamics of Parent Fe_(1+x)Te/Se Superconductor",
        "author": [
            {
                "family_name": "Xia",
                "given_name": "Y.",
                "clpid": "Xia-Yuqi"
            },
            {
                "family_name": "Qian",
                "given_name": "D.",
                "clpid": "Qian-Dong"
            },
            {
                "family_name": "Wray",
                "given_name": "L.",
                "clpid": "Wray-L-A"
            },
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            },
            {
                "family_name": "Chen",
                "given_name": "G. F.",
                "clpid": "Chen-G-F"
            },
            {
                "family_name": "Luo",
                "given_name": "J. L.",
                "clpid": "Luo-J-L"
            },
            {
                "family_name": "Wang",
                "given_name": "N. L.",
                "clpid": "Wang-N-L"
            },
            {
                "family_name": "Hasan",
                "given_name": "M. Z.",
                "clpid": "Hasan-M-Zihad"
            }
        ],
        "abstract": "We report the first photoemission study of Fe_(1+x) Te\u2014the host compound of the newly discovered iron-chalcogenide superconductors (maximum T_c\u223c27\u2009\u2009K). Our results reveal a pair of nearly electron-hole compensated Fermi pockets, strong Fermi velocity renormalization, and an absence of a spin-density-wave gap. A shadow hole pocket is observed at the \"X\" point of the Brillouin zone which is consistent with a long-range ordered magnetostructural ground state. No signature of Fermi surface nesting instability associated with Q=(\u03c0/2,\u03c0/2) is observed. Our results collectively reveal that the Fe_(1+x)Te series is different from the undoped phases of the high Tc pnictides and likely harbor an unusual mechanism for superconductivity and magnetic order.",
        "doi": "10.1103/PhysRevLett.103.037002",
        "issn": "0031-9007",
        "publisher": "American Physical Society",
        "publication": "Physical Review Letters",
        "publication_date": "2009-07-17",
        "series_number": "3",
        "volume": "103",
        "issue": "3",
        "pages": "Art. No. 037002"
    },
    {
        "id": "authors:a0wsf-sf607",
        "collection": "authors",
        "collection_id": "a0wsf-sf607",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140912-131757767",
        "type": "article",
        "title": "Observation of a large-gap topological-insulator class with a single Dirac cone on the surface",
        "author": [
            {
                "family_name": "Xia",
                "given_name": "Y.",
                "clpid": "Xia-Yuqi"
            },
            {
                "family_name": "Qian",
                "given_name": "D.",
                "clpid": "Qian-Dong"
            },
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            },
            {
                "family_name": "Wray",
                "given_name": "L.",
                "clpid": "Wray-L-A"
            },
            {
                "family_name": "Pal",
                "given_name": "A.",
                "clpid": "Pal-A"
            },
            {
                "family_name": "Lin",
                "given_name": "H.",
                "clpid": "Lin-Hsin"
            },
            {
                "family_name": "Bansil",
                "given_name": "A.",
                "clpid": "Bansil-Arun"
            },
            {
                "family_name": "Grauer",
                "given_name": "D.",
                "clpid": "Grauer-D"
            },
            {
                "family_name": "Hor",
                "given_name": "Y. S.",
                "clpid": "Hor-Yew-San"
            },
            {
                "family_name": "Cava",
                "given_name": "R. J.",
                "clpid": "Cava-Robert-J"
            },
            {
                "family_name": "Hasan",
                "given_name": "M. Z.",
                "clpid": "Hasan-M-Zihad"
            }
        ],
        "abstract": "Recent experiments and theories have suggested that strong spin\u2013orbit coupling effects in certain band insulators can give rise to a new phase of quantum matter, the so-called topological insulator, which can show macroscopic quantum-entanglement effects. Such systems feature two-dimensional surface states whose electrodynamic properties are described not by the conventional Maxwell equations but rather by an attached axion field, originally proposed to describe interacting quarks. It has been proposed that a topological insulator with a single Dirac cone interfaced with a superconductor can form the most elementary unit for performing fault-tolerant quantum computation. Here we present an angle-resolved photoemission spectroscopy study that reveals the first observation of such a topological state of matter featuring a single surface Dirac cone realized in the naturally occurring Bi_2Se_3 class of materials. Our results, supported by our theoretical calculations, demonstrate that undoped Bi_2Se_3 can serve as the parent matrix compound for the long-sought topological device where in-plane carrier transport would have a purely quantum topological origin. Our study further suggests that the undoped compound reached via n-to-p doping should show topological transport phenomena even at room temperature.",
        "doi": "10.1038/nphys1274",
        "issn": "1745-2473",
        "publisher": "Nature Publishing Group",
        "publication": "Nature Physics",
        "publication_date": "2009-05-10",
        "series_number": "6",
        "volume": "5",
        "issue": "6",
        "pages": "398-402"
    },
    {
        "id": "authors:ztrtj-yjc40",
        "collection": "authors",
        "collection_id": "ztrtj-yjc40",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140915-100302653",
        "type": "article",
        "title": "Observation of Unconventional Quantum Spin Textures in Topological Insulators",
        "author": [
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            },
            {
                "family_name": "Xia",
                "given_name": "Y.",
                "clpid": "Xia-Yuqi"
            },
            {
                "family_name": "Wray",
                "given_name": "L.",
                "clpid": "Wray-L-A"
            },
            {
                "family_name": "Qian",
                "given_name": "D.",
                "clpid": "Qian-Dong"
            },
            {
                "family_name": "Pal",
                "given_name": "A.",
                "clpid": "Pal-A"
            },
            {
                "family_name": "Dil",
                "given_name": "J. H.",
                "clpid": "Dil-J-H"
            },
            {
                "family_name": "Osterwalder",
                "given_name": "J.",
                "clpid": "Osterwalder-J"
            },
            {
                "family_name": "Meier",
                "given_name": "F.",
                "clpid": "Meier-F"
            },
            {
                "family_name": "Bihlmayer",
                "given_name": "G.",
                "orcid": "0000-0002-6615-1122",
                "clpid": "Bihlmayer-G"
            },
            {
                "family_name": "Kane",
                "given_name": "C. L.",
                "clpid": "Kane-C-L"
            },
            {
                "family_name": "Hor",
                "given_name": "Y. S.",
                "clpid": "Hor-Yew-San"
            },
            {
                "family_name": "Cava",
                "given_name": "R. J.",
                "clpid": "Cava-Robert-J"
            },
            {
                "family_name": "Hasan",
                "given_name": "M. Z.",
                "clpid": "Hasan-M-Zihad"
            }
        ],
        "abstract": "A topologically ordered material is characterized by a rare quantum organization of electrons that evades the conventional spontaneously broken symmetry\u2013based classification of condensed matter. Exotic spin-transport phenomena, such as the dissipationless quantum spin Hall effect, have been speculated to originate from a topological order whose identification requires a spin-sensitive measurement, which does not exist to this date in any system. Using Mott polarimetry, we probed the spin degrees of freedom and demonstrated that topological quantum numbers are completely determined from spin texture\u2013imaging measurements. Applying this method to Sb and Bi_(1\u2013x)Sb_x, we identified the origin of its topological order and unusual chiral properties. These results taken together constitute the first observation of surface electrons collectively carrying a topological quantum Berry's phase and definite spin chirality, which are the key electronic properties component for realizing topological quantum computing bits with intrinsic spin Hall\u2013like topological phenomena.",
        "doi": "10.1126/science.1167733",
        "issn": "0036-8075",
        "publisher": "American Association for the Advancement of Science",
        "publication": "Science",
        "publication_date": "2009-02-13",
        "series_number": "5916",
        "volume": "323",
        "issue": "5916",
        "pages": "912-922"
    },
    {
        "id": "authors:g0swa-2p704",
        "collection": "authors",
        "collection_id": "g0swa-2p704",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140915-122713242",
        "type": "article",
        "title": "Magnetic excitations in triangular lattice NaCrO_2",
        "author": [
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            },
            {
                "family_name": "Qian",
                "given_name": "D.",
                "clpid": "Qian-Dong"
            },
            {
                "family_name": "Berger",
                "given_name": "R. F.",
                "clpid": "Berger-R-F"
            },
            {
                "family_name": "Cava",
                "given_name": "R. J.",
                "clpid": "Cava-Robert-J"
            },
            {
                "family_name": "Lynn",
                "given_name": "J. W.",
                "orcid": "0000-0003-3626-4932",
                "clpid": "Lynn-J-W"
            },
            {
                "family_name": "Huang",
                "given_name": "Q.",
                "clpid": "Huang-Q"
            },
            {
                "family_name": "Hasan",
                "given_name": "M. Z.",
                "clpid": "Hasan-M-Zihad"
            }
        ],
        "abstract": "We report the first inelastic neutron scattering measurements on the rhombohedrally stacked triangular antiferromagnet NaCrO_2 which has recently been shown via \u03bcSR and NMR measurements to exhibit an unusually broad fluctuating cross-over regime extending far below the onset of spin freezing at T_c. Our results show that strong spin fluctuations persist far below T_c and that dispersive spin wave excitations only appear near the cross-over temperature 0.75T_c.",
        "doi": "10.1016/j.jpcs.2008.06.124",
        "issn": "0022-3697",
        "publisher": "Elsevier",
        "publication": "Journal of Physics and Chemistry of Solids",
        "publication_date": "2008-12",
        "series_number": "12",
        "volume": "69",
        "issue": "12",
        "pages": "3174-3175"
    },
    {
        "id": "authors:qe8f2-pyb58",
        "collection": "authors",
        "collection_id": "qe8f2-pyb58",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140908-100342412",
        "type": "article",
        "title": "Momentum dependence of superconducting gap, strong-coupling dispersion kink, and tightly bound Cooper pairs in the high-T_c (Sr,Ba)_(1\u2212x)(K,Na)_xFe_2As_2 superconductors",
        "author": [
            {
                "family_name": "Wray",
                "given_name": "L.",
                "clpid": "Wray-L-A"
            },
            {
                "family_name": "Qian",
                "given_name": "D.",
                "clpid": "Qian-Dong"
            },
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            },
            {
                "family_name": "Xia",
                "given_name": "Y.",
                "clpid": "Xia-Yuqi"
            },
            {
                "family_name": "Li",
                "given_name": "L.",
                "clpid": "Li-L"
            },
            {
                "family_name": "Checkelsky",
                "given_name": "J. G.",
                "clpid": "Checkelsky-J-G"
            },
            {
                "family_name": "Pasupathy",
                "given_name": "A.",
                "clpid": "Pasupathy-A"
            },
            {
                "family_name": "Gomes",
                "given_name": "K. K.",
                "clpid": "Gomes-K-K"
            },
            {
                "family_name": "Parker",
                "given_name": "C. V.",
                "clpid": "Parker-C-V"
            },
            {
                "family_name": "Fedorov",
                "given_name": "A. V.",
                "clpid": "Fedorov-A-V"
            },
            {
                "family_name": "Chen",
                "given_name": "G. F.",
                "clpid": "Chen-G-F"
            },
            {
                "family_name": "Luo",
                "given_name": "J. L.",
                "clpid": "Luo-J-L"
            },
            {
                "family_name": "Yazdani",
                "given_name": "A.",
                "clpid": "Yazdani-Ali"
            },
            {
                "family_name": "Ong",
                "given_name": "N. P.",
                "clpid": "Ong-N-P"
            },
            {
                "family_name": "Wang",
                "given_name": "N. L.",
                "clpid": "Wang-N-L"
            },
            {
                "family_name": "Hasan",
                "given_name": "M. Z.",
                "clpid": "Hasan-M-Zihad"
            }
        ],
        "abstract": "We present a systematic angle-resolved photoemission spectroscopic study of the high-Tc superconductor class (Sr/Ba)_(1\u2212x)K_xFe_2As_2. By utilizing a photon-energy-modulation contrast and scattering geometry we report the Fermi surface and the momentum dependence of the superconducting gap, \u0394(k\u20d7 ). A prominent quasiparticle dispersion kink reflecting strong scattering processes is observed in a binding-energy range of 25\u201355 meV in the superconducting state, and the coherence length or the extent of the Cooper pair wave function is found to be about 20\u2002\u00c5, which is uncharacteristic of a superconducting phase realized by the BCS-phonon-retardation mechanism. The observed 40\u00b115\u2002meV kink likely reflects contributions from the frustrated spin excitations in a J_1-J_2 magnetic background and scattering from the soft phonons. Results taken collectively provide direct clues to the nature of the pairing potential including an internal phase-shift factor in the superconducting order parameter which leads to a Brillouin zone node in a strong-coupling setting.",
        "doi": "10.1103/PhysRevB.78.184508",
        "issn": "1098-0121",
        "publisher": "American Physical Society",
        "publication": "Physical Review B",
        "publication_date": "2008-11-01",
        "series_number": "18",
        "volume": "78",
        "issue": "18",
        "pages": "Art. No. 184508"
    },
    {
        "id": "authors:ypwn3-se064",
        "collection": "authors",
        "collection_id": "ypwn3-se064",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140908-095501791",
        "type": "article",
        "title": "X-ray imaging of dispersive charge modes in a doped Mott insulator near the antiferromagnet/superconductor transition",
        "author": [
            {
                "family_name": "Li",
                "given_name": "Y. W.",
                "clpid": "Li-Y-W"
            },
            {
                "family_name": "Qian",
                "given_name": "D.",
                "clpid": "Qian-Dong"
            },
            {
                "family_name": "Wray",
                "given_name": "L.",
                "clpid": "Wray-L-A"
            },
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            },
            {
                "family_name": "Xia",
                "given_name": "Y.",
                "clpid": "Xia-Yuqi"
            },
            {
                "family_name": "Kaga",
                "given_name": "Y.",
                "clpid": "Kaga-Y"
            },
            {
                "family_name": "Sasagawa",
                "given_name": "T.",
                "clpid": "Sasagawa-T"
            },
            {
                "family_name": "Takagi",
                "given_name": "H.",
                "clpid": "Takagi-H"
            },
            {
                "family_name": "Markiewicz",
                "given_name": "R. S.",
                "clpid": "Markiewicz-R-S"
            },
            {
                "family_name": "Bansil",
                "given_name": "A.",
                "clpid": "Bansil-Arun"
            },
            {
                "family_name": "Eisaki",
                "given_name": "H.",
                "clpid": "Eisaki-H"
            },
            {
                "family_name": "Uchida",
                "given_name": "S.",
                "clpid": "Uchda-S"
            },
            {
                "family_name": "Hasan",
                "given_name": "M. Z.",
                "clpid": "Hasan-M-Zihad"
            }
        ],
        "abstract": "Momentum-resolved inelastic resonant x-ray scattering is used to map the doping evolution of bulk electronic modes in the doped Mott insulator class Nd_(2\u2212x)Ce_xCuO_4. As the doping induced antiferromagnet/superconductor (AFM/SC) transition is approached, we observe an anisotropic redistribution of the spectral weight of collective excitations over a large energy scale along the \u0393\u2192(\u03c0,\u03c0) direction, whereas the modes exhibit broadening (\u223c1\u2002eV) with relatively little softening along \u0393\u2192(\u03c0,0) with respect to the parent Mott state (x=0). Our study reveals a closing of the charge gap in the vicinity of the zone center even though the mode softening and spectral redistribution involve an unusually large energy scale over the full Brillouin zone. The collective behavior of modes in the vicinity of the AFM/SC critical transition is demonstrated.",
        "doi": "10.1103/PhysRevB.78.073104",
        "issn": "1098-0121",
        "publisher": "American Physical Society",
        "publication": "Physical Review B",
        "publication_date": "2008-08-15",
        "series_number": "7",
        "volume": "78",
        "issue": "7",
        "pages": "Art. No. 073104"
    },
    {
        "id": "authors:jskr0-teb70",
        "collection": "authors",
        "collection_id": "jskr0-teb70",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140917-083918043",
        "type": "article",
        "title": "A topological Dirac insulator in a quantum spin Hall phase",
        "author": [
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            },
            {
                "family_name": "Qian",
                "given_name": "D.",
                "clpid": "Qian-Dong"
            },
            {
                "family_name": "Wray",
                "given_name": "L.",
                "clpid": "Wray-L-A"
            },
            {
                "family_name": "Xia",
                "given_name": "Y.",
                "clpid": "Xia-Yuqi"
            },
            {
                "family_name": "Hor",
                "given_name": "Y. S.",
                "clpid": "Hor-Yew-San"
            },
            {
                "family_name": "Cava",
                "given_name": "R. J.",
                "clpid": "Cava-Robert-J"
            },
            {
                "family_name": "Hasan",
                "given_name": "M. Z.",
                "clpid": "Hasan-M-Zihad"
            }
        ],
        "abstract": "When electrons are subject to a large external magnetic field, the conventional charge quantum Hall effect dictates that an electronic excitation gap is generated in the sample bulk, but metallic conduction is permitted at the boundary. Recent theoretical models suggest that certain bulk insulators with large spin\u2013orbit interactions may also naturally support conducting topological boundary states in the quantum limit, which opens up the possibility for studying unusual quantum Hall-like phenomena in zero external magnetic fields. Bulk Bi_(1-x)Sb_x single crystals are predicted to be prime candidates for one such unusual Hall phase of matter known as the topological insulator. The hallmark of a topological insulator is the existence of metallic surface states that are higher-dimensional analogues of the edge states that characterize a quantum spin Hall insulator. In addition to its interesting boundary states, the bulk of Bi_(1-x)Sb_x is predicted to exhibit three-dimensional Dirac particles, another topic of heightened current interest following the new findings in two-dimensional graphene and charge quantum Hall fractionalization observed in pure bismuth. However, despite numerous transport and magnetic measurements on the Bi_(1-x)Sb_x family since the 1960s, no direct evidence of either topological Hall states or bulk Dirac particles has been found. Here, using incident-photon-energy-modulated angle-resolved photoemission spectroscopy (IPEM-ARPES), we report the direct observation of massive Dirac particles in the bulk of Bi_(0.9)Sb_(0.1), locate the Kramers points at the sample's boundary and provide a comprehensive mapping of the Dirac insulator's gapless surface electron bands. These findings taken together suggest that the observed surface state on the boundary of the bulk insulator is a realization of the 'topological metal'. They also suggest that this material has potential application in developing next-generation quantum computing devices that may incorporate 'light-like' bulk carriers and spin-textured surface currents.",
        "doi": "10.1038/nature06843",
        "issn": "0028-0836",
        "publisher": "Nature Publishing Group",
        "publication": "Nature",
        "publication_date": "2008-04-24",
        "series_number": "7190",
        "volume": "452",
        "issue": "7190",
        "pages": "970-974"
    },
    {
        "id": "authors:szg57-qxg22",
        "collection": "authors",
        "collection_id": "szg57-qxg22",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140917-085305545",
        "type": "article",
        "title": "Unconventional spin order in the triangular lattice system NaCrO_2: A neutron scattering study",
        "author": [
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            },
            {
                "family_name": "Qian",
                "given_name": "D.",
                "clpid": "Qian-Dong"
            },
            {
                "family_name": "Berger",
                "given_name": "R. F.",
                "clpid": "Berger-R-F"
            },
            {
                "family_name": "Cava",
                "given_name": "R. J.",
                "clpid": "Cava-Robert-J"
            },
            {
                "family_name": "Lynn",
                "given_name": "J. W.",
                "orcid": "0000-0003-3626-4932",
                "clpid": "Lynn-J-W"
            },
            {
                "family_name": "Huang",
                "given_name": "Q.",
                "clpid": "Huang-Q"
            },
            {
                "family_name": "Hasan",
                "given_name": "M. Z.",
                "clpid": "Hasan-M-Zihad"
            }
        ],
        "abstract": "We report high resolution neutron scattering measurements on the rhombohedrally stacked triangular antiferromagnet NaCrO_2 which has recently been shown to exhibit an unusually broad fluctuating cross-over regime extending far below the onset of spin freezing at T_c. Our results show that at T_c purely two-dimensional quasi-static spin correlations of the 120\u00b0 type exist. Below some cross-over temperature (T\u223c0.75T_c) a small incommensuration develops which helps resolve the inter-layer spin frustration and drives short-range three-dimensional magnetic order. This incommensuration assisted dimensional cross-over suggests that inter-layer frustration is responsible for stabilizing the rare 2D correlated phase above 0.75T_c.",
        "doi": "10.1016/j.physb.2007.10.295",
        "issn": "0921-4526",
        "publisher": "Elsevier",
        "publication": "Physica B",
        "publication_date": "2008-04-01",
        "series_number": "5-9",
        "volume": "403",
        "issue": "5-9",
        "pages": "1341-1343"
    },
    {
        "id": "authors:hgh9e-kwx29",
        "collection": "authors",
        "collection_id": "hgh9e-kwx29",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140828-192348141",
        "type": "article",
        "title": "Anomalous Metallic State of Cu_(0.07)TiSe_2: An Optical Spectroscopy Study",
        "author": [
            {
                "family_name": "Li",
                "given_name": "G.",
                "clpid": "Li-G"
            },
            {
                "family_name": "Hu",
                "given_name": "W. Z.",
                "clpid": "Hu-W-Z"
            },
            {
                "family_name": "Dong",
                "given_name": "J.",
                "clpid": "Dong-J"
            },
            {
                "family_name": "Qian",
                "given_name": "D.",
                "clpid": "Qian-Dong"
            },
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            },
            {
                "family_name": "Hasan",
                "given_name": "M. Z.",
                "clpid": "Hasan-M-Zihad"
            },
            {
                "family_name": "Morosan",
                "given_name": "E.",
                "clpid": "Morosan-E"
            },
            {
                "family_name": "Cava",
                "given_name": "R. J.",
                "clpid": "Cava-Robert-J"
            },
            {
                "family_name": "Wang",
                "given_name": "N. L.",
                "clpid": "Wang-N-L"
            }
        ],
        "abstract": "We report an optical spectroscopy study on the newly discovered superconductor Cu_(0.07)TiSe_2. Consistent with the development from a semimetal or semiconductor with a very small indirect energy gap upon doping TiSe_2, it is found that the compound has a low carrier density. Most remarkably, the study reveals a substantial shift of the screened plasma edge in reflectance towards high energy with decreasing temperature. This phenomenon, rarely seen in metals, indicates either a sizable increase of the conducting carrier concentration or/and a decrease of the effective mass of carriers with reducing temperature. We attribute the shift primarily to the latter effect.",
        "doi": "10.1103/PhysRevLett.99.167002",
        "issn": "0031-9007",
        "publisher": "American Physical Society",
        "publication": "Physical Review Letters",
        "publication_date": "2007-10-19",
        "series_number": "16",
        "volume": "99",
        "issue": "16",
        "pages": "Art. No. 167002"
    },
    {
        "id": "authors:ytg85-76c94",
        "collection": "authors",
        "collection_id": "ytg85-76c94",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140908-094730650",
        "type": "article",
        "title": "Dispersive collective charge modes in an incommensurately modulated cuprate Mott insulator",
        "author": [
            {
                "family_name": "Wray",
                "given_name": "L.",
                "clpid": "Wray-L-A"
            },
            {
                "family_name": "Qian",
                "given_name": "D.",
                "clpid": "Qian-Dong"
            },
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            },
            {
                "family_name": "Xia",
                "given_name": "Y.",
                "clpid": "Xia-Yuqi"
            },
            {
                "family_name": "Eisaki",
                "given_name": "H.",
                "clpid": "Eisaki-H"
            },
            {
                "family_name": "Hasan",
                "given_name": "M. Z.",
                "clpid": "Hasan-M-Zihad"
            }
        ],
        "abstract": "We report measurement of collective charge modes of insulating Sr_(14)Cu_(24)O_(41) using inelastic resonant x-ray scattering over the complete Brillouin zone. Our results show that the intense excitation modes at the charge gap edge predominantly originate from ladder-containing planar substructures. The observed modes are found to be dispersive for momentum transfers along the \"legs\" (\u210fQ\u20d7 \u2225\u2225\u0109 ) but nearly localized along the \"rungs\" (\u210fQ\u20d7 \u2225\u2225\u00e2 ). We show that the dispersion and peak width characteristics of the modes can be understood in the strong-coupling quantum limit (Hubbard U\u2aa2t_(ladder)&gt;t_(chain), where t is the hopping parameter). Quite generally, we demonstrate that the momentum tunability (Q\u20d7  resolution) of inelastic x-ray scattering can be utilized to resolve mode contributions in multicomponent incommensurate quantum electron systems.",
        "doi": "10.1103/PhysRevB.76.100507",
        "issn": "1098-0121",
        "publisher": "American Physical Society",
        "publication": "Physical Review B",
        "publication_date": "2007-09-19",
        "volume": "76",
        "pages": "Art. No. 100507(R)"
    },
    {
        "id": "authors:7chf9-52w22",
        "collection": "authors",
        "collection_id": "7chf9-52w22",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140908-082820675",
        "type": "article",
        "title": "Semimetal-to-Semimetal Charge Density Wave Transition in 1T-TiSe_2",
        "author": [
            {
                "family_name": "Li",
                "given_name": "G.",
                "clpid": "Li-G"
            },
            {
                "family_name": "Hu",
                "given_name": "Z.",
                "clpid": "Hu-Z"
            },
            {
                "family_name": "Qian",
                "given_name": "D.",
                "clpid": "Qian-Dong"
            },
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            },
            {
                "family_name": "Hasan",
                "given_name": "M. Z.",
                "clpid": "Hasan-M-Zihad"
            },
            {
                "family_name": "Morosan",
                "given_name": "E.",
                "clpid": "Morosan-E"
            },
            {
                "family_name": "Cava",
                "given_name": "R. J.",
                "clpid": "Cava-Robert-J"
            },
            {
                "family_name": "Wang",
                "given_name": "N. L.",
                "clpid": "Wang-N-L"
            }
        ],
        "abstract": "We report an infrared study on 1T-TiSe_2, the parent compound of the newly discovered superconductor Cu_xTiSe_2. Previous studies of this compound have not conclusively resolved whether it is a semimetal or a semiconductor\u2014information that is important in determining the origin of its unconventional charge density wave (CDW) transition. Here we present optical spectroscopy results that clearly reveal that the compound is metallic in both the high-temperature normal phase and the low-temperature CDW phase. The carrier scattering rate is dramatically different in the normal and CDW phases and the carrier density is found to change with temperature. We conclude that the observed properties can be explained within the scenario of an Overhauser-type CDW mechanism.",
        "doi": "10.1103/PhysRevLett.99.027404",
        "issn": "0031-9007",
        "publisher": "American Physical Society",
        "publication": "Physical Review Letters",
        "publication_date": "2007-07-13",
        "series_number": "2",
        "volume": "99",
        "issue": "2",
        "pages": "Art. No. 027404"
    },
    {
        "id": "authors:pyqq6-72941",
        "collection": "authors",
        "collection_id": "pyqq6-72941",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140908-093938696",
        "type": "article",
        "title": "Emergence of Fermi Pockets in a New Excitonic Charge-Density-Wave Melted Superconductor",
        "author": [
            {
                "family_name": "Qian",
                "given_name": "D.",
                "clpid": "Qian-Dong"
            },
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            },
            {
                "family_name": "Wray",
                "given_name": "L.",
                "clpid": "Wray-L-A"
            },
            {
                "family_name": "Morosan",
                "given_name": "E.",
                "clpid": "Morosan-E"
            },
            {
                "family_name": "Wang",
                "given_name": "N. L.",
                "clpid": "Wang-N-L"
            },
            {
                "family_name": "Xia",
                "given_name": "Y.",
                "clpid": "Xia-Yuqi"
            },
            {
                "family_name": "Cava",
                "given_name": "R. J.",
                "clpid": "Cava-Robert-J"
            },
            {
                "family_name": "Hasan",
                "given_name": "M. Z.",
                "clpid": "Hasan-M-Zihad"
            }
        ],
        "abstract": "A superconducting state (T_c\u223c4.2\u2009\u2009K) has very recently been observed upon successful doping of the charge-density-wave (CDW) ordered triangular lattice TiSe_2, with copper. Using state-of-the-art photoemission spectroscopy we identify, for the first time, momentum-space locations of doped electrons that form the Fermi sea of the superconductor. With doping, we find that kinematic nesting volume increases, whereas coherence of the CDW collective order sharply drops. In superconducting doping, as chemical potential rises, we observe the emergence of a large density of states in the form of a narrow electron pocket near the L point of the Brillouin zone with d-like character. The k-space spectral evolution directly demonstrates, for the first time, that the CDW order parameter microscopically competes with superconductivity in the same band.",
        "doi": "10.1103/PhysRevLett.98.117007",
        "issn": "0031-9007",
        "publisher": "American Physical Society",
        "publication": "Physical Review Letters",
        "publication_date": "2007-03-16",
        "series_number": "11",
        "volume": "98",
        "issue": "11",
        "pages": "Art. No. 117007"
    },
    {
        "id": "authors:c06x3-mj246",
        "collection": "authors",
        "collection_id": "c06x3-mj246",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140908-085009835",
        "type": "article",
        "title": "Complete d-Band Dispersion Relation in Sodium Cobaltates",
        "author": [
            {
                "family_name": "Qian",
                "given_name": "D.",
                "clpid": "Qian-Dong"
            },
            {
                "family_name": "Wray",
                "given_name": "L.",
                "clpid": "Wray-L-A"
            },
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            },
            {
                "family_name": "Viciu",
                "given_name": "L.",
                "clpid": "Viciu-L"
            },
            {
                "family_name": "Cava",
                "given_name": "R. J.",
                "clpid": "Cava-Robert-J"
            },
            {
                "family_name": "Luo",
                "given_name": "J. L.",
                "clpid": "Luo-J-L"
            },
            {
                "family_name": "Wu",
                "given_name": "D.",
                "clpid": "Wu-D"
            },
            {
                "family_name": "Wang",
                "given_name": "N. L.",
                "clpid": "Wang-N-L"
            },
            {
                "family_name": "Hasan",
                "given_name": "M. Z.",
                "clpid": "Hasan-M-Zihad"
            }
        ],
        "abstract": "We utilize fine-tuned polarization selection coupled with excitation-energy variation of photoelectron signal to image the complete d-band dispersion relation in sodium cobaltates. A hybridization gap anticrossing is observed along the Brillouin zone corner and the full quasiparticle band is found to emerge as a many-body entity lacking a pure orbital polarization. At low dopings, the quasiparticle bandwidth (Fermion scale, many-body E_F\u223c0.25\u2009\u2009eV) is found to be smaller than most known oxide metals. The low-lying density of states is found to be in agreement with bulk-sensitive thermodynamic measurements for nonmagnetic dopings where the 2D Luttinger theorem is also observed to be satisfied.",
        "doi": "10.1103/PhysRevLett.97.186405",
        "issn": "0031-9007",
        "publisher": "American Physical Society",
        "publication": "Physical Review Letters",
        "publication_date": "2006-11-03",
        "series_number": "18",
        "volume": "97",
        "issue": "18",
        "pages": "Art. No. 186405"
    },
    {
        "id": "authors:g486c-pnt10",
        "collection": "authors",
        "collection_id": "g486c-pnt10",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140908-085720745",
        "type": "article",
        "title": "Low-Lying Quasiparticle States and Hidden Collective Charge Instabilities in Parent Cobaltate Superconductors",
        "author": [
            {
                "family_name": "Qian",
                "given_name": "D.",
                "clpid": "Qian-Dong"
            },
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            },
            {
                "family_name": "Wray",
                "given_name": "L.",
                "clpid": "Wray-L-A"
            },
            {
                "family_name": "Chuang",
                "given_name": "Y.-D.",
                "clpid": "Chuang-Y-D"
            },
            {
                "family_name": "Fedorov",
                "given_name": "A.",
                "clpid": "Fedorov-A"
            },
            {
                "family_name": "Wu",
                "given_name": "D.",
                "clpid": "Wu-D"
            },
            {
                "family_name": "Luo",
                "given_name": "J. L.",
                "clpid": "Luo-J-L"
            },
            {
                "family_name": "Wang",
                "given_name": "N. L.",
                "clpid": "Wang-N-L"
            },
            {
                "family_name": "Viciu",
                "given_name": "L.",
                "clpid": "Viciu-L"
            },
            {
                "family_name": "Cava",
                "given_name": "R. J.",
                "clpid": "Cava-Robert-J"
            },
            {
                "family_name": "Hasan",
                "given_name": "M. Z.",
                "clpid": "Hasan-M-Zihad"
            }
        ],
        "abstract": "We report a state-of-the-art photoemission (angle-resolved photoemission spectroscopy) study of high quality single crystals of the Na_xCoO_2 series focusing on the fine details of the low-energy states. The Fermi velocity is found to be small (&lt;0.5\u2009\u200a\u200aeV\u2009\u2009\u200a\u200a\u00c5) and only weakly anisotropic over the Fermi surface at all dopings, setting the size of the pair wave function to be on the order of 10\u201320 nm. In the low-doping regime, the exchange interlayer splitting vanishes and two-dimensional collective instabilities such as 120\u00b0-type fluctuations become kinematically allowed. Our results suggest that the unusually small Fermi velocity and the unique symmetry of kinematic instabilities distinguish cobaltates from most other oxide superconductors.",
        "doi": "10.1103/PhysRevLett.96.216405",
        "issn": "0031-9007",
        "publisher": "American Physical Society",
        "publication": "Physical Review Letters",
        "publication_date": "2006-06-02",
        "series_number": "21",
        "volume": "96",
        "issue": "21",
        "pages": "Art. No. 216405"
    },
    {
        "id": "authors:m03ve-svd88",
        "collection": "authors",
        "collection_id": "m03ve-svd88",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140908-092120910",
        "type": "article",
        "title": "Quasiparticle Dynamics in the Vicinity of Metal-Insulator Phase Transition in Na_xCoO_2",
        "author": [
            {
                "family_name": "Qian",
                "given_name": "D.",
                "clpid": "Qian-Dong"
            },
            {
                "family_name": "Wray",
                "given_name": "L.",
                "clpid": "Wray-L-A"
            },
            {
                "family_name": "Hsieh",
                "given_name": "D.",
                "orcid": "0000-0002-0812-955X",
                "clpid": "Hsieh-David"
            },
            {
                "family_name": "Wu",
                "given_name": "D.",
                "clpid": "Wu-D"
            },
            {
                "family_name": "Luo",
                "given_name": "J. L.",
                "clpid": "Luo-J-L"
            },
            {
                "family_name": "Wang",
                "given_name": "N. L.",
                "clpid": "Wang-N-L"
            },
            {
                "family_name": "Kuprin",
                "given_name": "A.",
                "clpid": "Kuprin-A"
            },
            {
                "family_name": "Fedorov",
                "given_name": "A.",
                "clpid": "Fedorov-A"
            },
            {
                "family_name": "Cava",
                "given_name": "R. J.",
                "clpid": "Cava-Robert-J"
            },
            {
                "family_name": "Viciu",
                "given_name": "L.",
                "clpid": "Viciu-L"
            },
            {
                "family_name": "Hasan",
                "given_name": "M. Z.",
                "clpid": "Hasan-M-Zihad"
            }
        ],
        "abstract": "Layered cobaltates embody novel realizations of correlated matter on a spin-1/2 triangular lattice. We report a high-resolution systematic photoemission study of the insulating cobaltates. The observation of a single-particle gap opening and band folding provides direct evidence of anisotropic particle-hole instability on the Fermi surface due to its unique topology. Overlap of the measured Fermi surface is observed with the 3\u221a\u00d7 3\u221a charge-order Brillouin zone near x = 1/3 but not at x = 1/2 where the insulating transition is actually observed. Unlike conventional density waves, charge stripes, or band insulators, the onset of the gap depends on the quasiparticle's quantum coherence which is found to occur well below the disorder-order symmetry breaking temperature of the crystal (the first known example of its kind).",
        "doi": "10.1103/PhysRevLett.96.046407",
        "issn": "0031-9007",
        "publisher": "American Physical Society",
        "publication": "Physical Review Letters",
        "publication_date": "2006-02-03",
        "series_number": "4",
        "volume": "96",
        "issue": "4",
        "pages": "Art. No. 046407"
    }
]