Subir Sachdev
Born2 December 1961
New Delhi
Alma materMassachusetts Institute of Technology (B.S),
Harvard University (Ph.D)
Known forTheories of critical and topological states of quantum matter;
Sachdev–Ye–Kitaev model
Awards
Scientific career
FieldsCondensed matter theory
ThesisFrustration and Order in Rapidly Cooled Metals (1985)
Doctoral advisorD. R. Nelson
Websiteqpt.physics.harvard.edu/cv.html

Subir Sachdev is Herchel Smith Professor of Physics[1] at Harvard University specializing in condensed matter. He was elected to the U.S. National Academy of Sciences in 2014, received the Lars Onsager Prize from the American Physical Society and the Dirac Medal from the ICTP in 2018, and was elected Foreign Member of the Royal Society ForMemRS in 2023. He was a co-editor of the Annual Review of Condensed Matter Physics 2017–2019, [2][3] and is Editor-in-Chief of Reports on Progress in Physics 2022-.

Sachdev's research describes the consequences of quantum entanglement on the macroscopic properties of natural systems: watch his Institute Lecture at IIT Delhi in January 2024.[4] Sachdev has made extensive contributions to the description of the diverse varieties of entangled states of quantum matter. Many of these contributions have been linked to experiments, especially to the rich phase diagrams of the high temperature superconductors. Sachdev's research has exposed remarkable connections between the nature of quantum entanglement in certain laboratory materials, and the quantum entanglement in astrophysical black holes, and these connections have led to new insights on the entropy and radiation of black holes proposed by Stephen Hawking.

Strange metals and black holes

Extreme examples of complex quantum entanglement arise in metallic states of matter without quasiparticle excitations, often called strange metals. Remarkably, there is an intimate connection between the quantum physics of strange metals found in modern materials (which can be studied in tabletop experiments), and quantum entanglement near black holes of astrophysics.

This connection is most clearly seen by first thinking more carefully about the defining characteristic of a strange metal: the absence of quasiparticles. In practice, given a state of quantum matter, it is difficult to completely rule out the existence of quasiparticles: while one can confirm that certain perturbations do not create single quasiparticle excitations, it is almost impossible to rule out a non-local operator which could create an exotic quasiparticle in which the underlying electrons are non-locally entangled. Sachdev argued[5][6] instead that it is better to examine how rapidly the system loses quantum phase coherence, or reaches local thermal equilibrium in response to general external perturbations. If quasiparticles existed, dephasing would take a long time during which the excited quasiparticles collide with each other. In contrast, states without quasiparticles reach local thermal equilibrium in the fastest possible time, bounded below by a value of order (Planck constant)/((Boltzmann constant) x (absolute temperature)).[5] Sachdev proposed[7][8] a solvable model of a strange metal (a variant of which is now called the Sachdev–Ye–Kitaev (SYK) model), which was shown to saturate such a bound on the time to reach quantum chaos.[9]

We can now make the connection to the quantum theory of black holes: quite generally, black holes also thermalize and reach quantum chaos in a time of order (Planck constant)/((Boltzmann constant) x (absolute temperature)),[10][11] where the absolute temperature is the black hole's Hawking temperature. And this similarity to quantum matter without quasiparticles is not a co-incidence: for the SYK models, Sachdev had argued[12] that the strange metal has a holographic dual description in terms of the quantum theory of black holes in a curved spacetime with 1 space dimension.

This connection, and other related work by Sachdev and collaborators, have led to valuable insights on the properties of electronic quantum matter, and on the nature of Hawking radiation from black holes. Solvable models of strange metals obtained from the gravitational mapping have inspired analyses of more realistic models of strange metals in the high temperature superconductors and other compounds. Such predictions have been connected to experiments, including some[13] that are in good quantitative agreement with observations on graphene.[14][15] These topics are discussed in more detail in Research.

Resonating valence bonds and Z2 quantum spin liquids

P.W. Anderson proposed[16] that Mott insulators realize antiferromagnets which could form resonating valence bond (RVB) or quantum spin liquid states with an energy gap to spin excitations without breaking time-reversal symmetry. It was conjectured that such RVB states have excitations with fractional quantum numbers, such as a fractional spin 1/2. The existence of such RVB ground states, and of the deconfinement of fractionalized excitations was first established by Read and Sachdev[17] and Wen[18] by the connection to a Z2 gauge theory. Sachdev was also the first to show that the RVB state is an odd Z2 gauge theory,[19][20][21] as described in Research. An odd Z2 spin liquid has a background Z2 electric charge on each lattice site (equivalently, translations in the x and y directions anti-commute with each other in the super-selection sector of states associated with a Z2 gauge flux (also known as the m sector)). Sachdev showed that antiferromagnets with half-integer spin form odd Z2 spin liquids, and those with integer spin form even Z2 spin liquids. Using this theory, various universal properties of the RVB state were understood, including constraints on the symmetry transformations of the anyon excitations. Sachdev also obtained many results on the confinement transitions of the RVB state, including restrictions on proximate quantum phases and the nature of quantum phase transitions to them.

Career

Sachdev attended school at St. Joseph's Boys' High School, Bangalore and Kendriya Vidyalaya, ASC, Bangalore. He attended college at Indian Institute of Technology, Delhi for a year. He transferred to Massachusetts Institute of Technology where he received a B.S. in Physics. He received his Ph.D. in theoretical physics from Harvard University. He held professional positions at Bell Labs (1985–1987) and at Yale University (1987–2005), where he was a Professor of Physics, before returning to Harvard, where he is now the Herchel Smith Professor of Physics. He has also held visiting positions as the Cenovus Energy James Clerk Maxwell Chair in Theoretical Physics [22] at the Perimeter Institute for Theoretical Physics, and the Dr. Homi J. Bhabha Chair Professorship[23] at the Tata Institute of Fundamental Research.[citation needed] He has also been on the Physical Sciences jury for the Infosys Prize from 2018.[24]

Honors

Subir Sachdev has made profound contributions to theoretical condensed matter physics research. His main interests have been in quantum magnetism, quantum criticality, and perhaps most innovative of all, links between the nature of quantum entanglement in black holes and strongly interacting electrons in materials.

Professor Subir Sachdev is a world renowned condensed matter theorist, with many seminal contributions to the theory of strongly interacting condensed matter systems. He is a pioneer in the study of systems near quantum phase transitions. He has also pioneered the exploration of the connection between physical properties of modern quantum materials and the nature of quantum entanglement in their many-particle state, elucidating the diverse varieties of entangled states of quantum matter.

Subir Sachdev has made pioneering contributions to many areas of theoretical condensed matter physics. Of particular importance were the development of the theory of quantum critical phenomena in insulators, superconductors and metals; the theory of spin-liquid states of quantum antiferromagnets and the theory of fractionalized phases of matter; the study of novel deconfinement phase transitions; the theory of quantum matter without quasiparticles; and the application of many of these ideas to a priori unrelated problems in black hole physics, including a concrete model of non-Fermi liquids.

for his seminal contributions to the theory of quantum phase transitions, quantum magnetism, and fractionalized spin liquids, and for his leadership in the physics community.

The Dirac Medal was awarded to Professor Sachdev in recognition of his many seminal contributions to the theory of strongly interacting condensed matter systems: quantum phase transitions, including the idea of critical deconfinement and the breakdown of the conventional symmetry based Landau–Ginsburg–Wilson paradigm; the prediction of exotic 'spin-liquid' and fractionalized states; and applications to the theory of high-temperature superconductivity in the cuprate materials.

Sachdev has made seminal advances in the theory of condensed matter systems near a quantum phase transition, which have elucidated the rich variety of static and dynamic behavior in such systems, both at finite temperatures and at T=0. His book, Quantum Phase Transitions,[5] is the basic text of the field.

Research

Quantum phases of antiferromagnets

Sachdev has worked extensively on the quantum theory of antiferromagnetism, especially in two-dimensional lattices. Some of the spin liquid states of antiferromagnets can be described by examining the quantum phase transitions out of magnetically ordered states. Such an approach leads to a theory of emergent gauge fields and excitations in the spin liquid states. It is convenient to consider two classes of magnetic order separately: those with collinear and non-collinear spin order. For the case of collinear antiferromagnetism (as in the Néel state), the transition leads to a spin liquid with a U(1) gauge field, while non-collinear antiferromagnetism has a transition to a spin liquid with a Z2 gauge field.

Sachdev was the first to identify [19][20][21] that Z2 spin liquids come in two classes: `even' and `odd'. Half-integer-spin antiferromagnets can only realize odd Z2 spin liquids, which therefore provide a theory for Anderson's RVB state. Odd Z2 spin liquids have (what is now called) an anomaly which constrains the symmetry transformations of the anyon excitations, and modifies the anyon condensation transition. An important consequence is that half-integer-spin antiferromagnets (and odd Ising gauge theories) do not have a trivial confining phase, as is required by extensions of the Lieb–Schultz–Mattis theorems. These results apply also to quantum dimer models[20] and closely related models of bosons on the square lattice.[43][44] This work is now the starting point of research in symmetry enriched topological (SET) order.

These results agree with numerous numerical studies of model quantum spin systems in two dimensions.

Turning to experiments, VBS order was predicted[45] by this mechanism in SrCu2(BO3)2, and has been observed by neutron scattering.[46] A particular Z2 spin liquid state proposed for the kagome lattice antiferromagnet[42] agrees well with a tensor network analysis,[47] and has been proposed[48] to describe neutron scattering and NMR experiments on herbertsmithite.[49][50] A gapped spin liquid state has also been observed[51][52] in the kagome lattice compound Cu3Zn(OH)6FBr, and is likely to be a Z2 spin liquid.[53]

Quantum criticality

Sachdev proposed that the anomalous dynamic properties of the cuprate superconductors, and other correlated electron compounds, could be understood by proximity to a quantum critical fixed point. In the quantum critical regime of a non-trivial renormalization group fixed point (in higher than one spatial dimension) the dynamics is characterized by the absence of quasiparticles, and a local equilibration time of order ħ/(kBT). This time was proposed to be the shortest possible such time in all quantum systems.[5] Transport measurements have since shown that this bound is close to saturation in many correlated metals.[54] Sachdev has made numerous contributions to quantum field theories of quantum criticality in insulators, superconductors, and metals.[5]

Confinement transitions of gauge theories, and deconfined criticality

Traditionally, classical and quantum phase transitions, have been described in terms of the Landau–Ginzburg–Wilson paradigm. The broken symmetry in one of the phases identifies as order parameter; the action for the order parameter is expressed as a field theory which controls fluctuations at and across the critical point. Deconfined critical points describe a new class of phase transitions in which the field theory is not expressed in terms of the order parameter. Broken symmetry and order parameters, or topological order, are present in one or both of the adjacent phases. The critical field theory is expressed in terms of deconfined fractionalized degrees of freedom that cannot exist in isolation outside the sample.

Ising gauge theories: Franz Wegner introduced[55] Ising lattice gauge theories, and their transition between confining and deconfined phases, signaled by a change in the value of the Wilson loop of the gauge field from area law to perimeter law. Wegner also argued that confinement transition of this theory had no local order parameter, but was instead described by a dual Ising model in 3 dimensions. This conclusion turns out to need a crucial extension. One of the implications of Sachdev's work on emergent gauge fields in two-dimensional antiferromagnets[17][41][19] was that the deconfined phase of the 2+1 dimensional Ising gauge theory had Z2 topological order. The presence of topological order in one of the phases implies that this is an Ising* transition, in which we only select states and operators which are invariant under global Ising inversion; see a recent numerical study[56] for observable consequences of this restriction. The Ising field represents a fractionalized excitation of the deconfined phase, the "vison" (or the m particle) carrying a quantum of Z2 gauge flux, and visons can only be created in pairs. The confinement transition is driven by the condensation of deconfined visons, and so this is an example of a deconfined quantum critical point, although there is no gapless gauge field.

Odd Ising gauge theories: The notion of deconfined criticality becomes more crucial in studying the confinement transitions of RVB states. These are described by deconfined phases of "odd" Ising gauge theories[19][20][21] with Z2 topological order. (Wegner's Z2 gauge theory, which is "even", is not a satisfactory theory of the RVB state.) Now the critical theory has fractionalized excitations and a gapless gauge field. In the context of two-dimensional antiferromagnets with half-integer spin per unit cell, the effective description in terms of Ising gauge theories requires a background static electric charge on each site: this is the odd Ising gauge theory. We can write the Ising gauge theory as the strong coupling limit of a compact U(1) gauge theory in the presence of a charge 2 Higgs field.[57] The presence of the background electric charges implies that the monopoles of the U(1) field carry Berry phases,[19] and transform non-trivially under the space group of the lattice. As the monopoles condense in the confining phase, an immediate consequence is that the confining phase must break the space group by the development of valence bond solid (VBS) order. Furthermore, the Berry phases lead to suppression of monopoles at the critical point, so that, on the square lattice, the critical theory has a deconfined U(1) gauge field coupled to a critical charged scalar.[58] Note that the critical theory is not expressed in terms of the VBS order as would be required by the LGW paradigm (which ignores the Z2 topological order in the deconfined phase). Instead, a dual version of the U(1) gauge theory is written in terms of a "square root" of the VBS order.[19]

Onset of non-collinear antiferromagnetism: Another example of deconfined criticality in two dimensional antiferromagnets appears in the condensation of particles with electric charges (the e particle, or the spinon) from the deconfined phase of the Z2 gauge theory. As the spinon also carries quantum numbers of global spin rotations, this leads to a "Higgs" phase of the Z2 gauge theory with antiferromagnetic order and broken spin rotation symmetry;[59] here the antiferromagnetic order parameter has SO(3) symmetry, and so should the LGW critical theory; but the deconfined critical theory for the spinons has an exact SU(2) symmetry (which is further enlarged to O(4) after neglecting irrelevant terms).

Néel-VBS transition: A more subtle class of deconfined critical points has confining phases on both sides, and the fractionalized excitations present only at the critical point.[58][60][61][62] The best studied examples of this class are quantum antiferromagnets with SU(N) symmetry on the square lattice. These exhibit a phase transition from a state with collinear antiferromagnetic order to a valence bond solid,[39][40] but the critical theory is expressed in terms of spinons coupled to an emergent U(1) gauge field.[58][60][63] The study of this transition involved the first computation[64] of the scaling dimension of a monopole operator in a conformal field theory in 2+1 dimensions; more precise computations[65][66] to order 1/N are in good accord with numerical studies[67] of the Néel-VBS transition.

SYK model of non-Fermi liquids and black holes

Sachdev, and his first graduate student Jinwu Ye, proposed[7] an exactly solvable model of a non-Fermi liquid, a variant of which is now called the Sachdev–Ye–Kitaev model. Its fermion correlators have a power-law decay,[7] which was found[68] to extend to a conformally invariant form at non-zero temperatures. The SYK model was also found [69] to have a non-zero entropy per site in the limit of vanishing temperature (this is not equivalent to an exponentially large ground state degeneracy: instead, it is due to an exponentially small many-body level spacing, which extends across the spectrum down to the lowest energies). Based on these observations, Sachdev first proposed[12][8] that the model is holographically dual to quantum gravity on AdS2, and identified its low temperature entropy with the Bekenstein–Hawking black hole entropy. Unlike previous models of quantum gravity, it appears that the SYK model is solvable in a regime which accounts for the subtle non-thermal correlations in the Hawking radiation.

One-dimensional quantum systems with an energy gap

Sachdev and collaborators developed a formally exact theory for the non-zero temperature dynamics and transport of one-dimensional quantum systems with an energy gap.[70][71][72] The diluteness of the quasiparticle excitations at low temperature allowed the use of semi-classical methods. The results were in good quantitative agreement with NMR[73] and subsequent neutron scattering[74] observations on S=1 spin chains, and with NMR[75] on the Transverse Field Ising chain compound CoNb2O6

Quantum impurities

The traditional Kondo effect involves a local quantum degree of freedom interacting with a Fermi liquid or Luttinger liquid in the bulk. Sachdev described cases where the bulk was a strongly-interacting critical state without quasiparticle excitations.[76][77][78] The impurity was characterized by a Curie susceptibility of an irrational spin, and a boundary entropy of an irrational number of states.

Ultracold atoms

Sachdev predicted[79] density wave order and 'magnetic' quantum criticality in tilted lattices of ultracold atoms. This was subsequently observed in experiments.[80][81] The modeling of tilted lattices inspired a more general model of interacting bosons in which a coherent external source can create and annihilate bosons on each site.[82] This model exhibits density waves of multiple periods, along with gapless incommensurate phases, and has been realized in experiments on trapped Rydberg atoms.[83]

Metals with fractionalization and emergent gauge fields

Sachdev and collaborators proposed[84][85] a new metallic state, the fractionalized Fermi liquid (FL*): this has electron-like quasiparticles around a Fermi surface, enclosing a volume distinct from that required by Luttinger's theorem. A general argument was given that any such state must have very low energy excitations on a torus, not related to the low energy quasiparticles: these excitations are generally related to the emergent gauge fields of an associated spin liquid state. In other words, a non-Luttinger Fermi surface volume necessarily requires topological order.[85][86] The FL* phase must be separated from the conventional Fermi liquid (FL) by a quantum phase transition; this transition need not involve any broken symmetry, and examples were presented involving confinement/Higgs transitions of the gauge field. Such a quantum phase transition has been observed in CeCoIn5.[87]

Quantum critical transport

Sachdev developed the theory of quantum transport at non-zero temperatures in the simplest model system without quasiparticle excitations: a conformal field theory in 2+1 dimensions, realized by the superfluid-insulator transitions of ultracold bosons in an optical lattice. A comprehensive picture emerged from quantum-Boltzmann equations,[6] the operator product expansion,[88] and holographic methods.[89][90][91][92] The latter mapped the dynamics to that in the vicinity of the horizon of a black hole. These were the first proposed connections between condensed matter quantum critical systems, hydrodynamics, and quantum gravity. These works eventually led to the theory of hydrodynamic transport in graphene, and the successful experimental predictions[15] described below.

Quantum matter without quasiparticles

Sachdev developed the theory of magneto-thermoelectric transport in 'strange' metals: these are states of quantum matter with variable density without quasiparticle excitations. Such metals are found, most famously, near optimal doping in the hole-doped cuprates, but also appear in numerous other correlated electron compounds. For strange metals in which momentum is approximately conserved, a set of hydrodynamic equations were proposed in 2007,[93] describing two-component transport with momentum drag component and a quantum-critical conductivity. This formulation was connected to the holography of charged black holes, memory functions, and new field-theoretic approaches.[94] These equations are valid when the electron-electron scattering time is much shorter than the electron-impurity scattering time, and they lead to specific predictions for the density, disorder, temperature, frequency, and magnetic field dependence of transport properties. Strange metal behavior obeying these hydrodynamic equations was predicted in graphene,[13][95] in the 'quantum critical' regime of weak disorder and moderate temperatures near the Dirac density. The theory quantitatively describes measurements of thermal and electrical transport in graphene,[15] and points to a regime of viscous, rather than Ohmic, electron flow. Extensions of this theory to Weyl metals pointed out the relevance of the axial-gravitational anomaly,[96] and made predictions for thermal transport which were confirmed in observations[97][98] (and highlighted in the New York Times).

Phases of the high temperature superconductors

High temperature superconductivity appears upon changing the electron density away from a two-dimensional antiferromagnet. Much attention has focused on the intermediate regime between the antiferromagnet and the optimal superconductor, where additional competing orders are found at low temperatures, and a "pseudogap" metal appears in the hole-doped cuprates. Sachdev's theories for the evolution of the competing order with magnetic field,[99][100] density, and temperature have been successfully compared with experiments.[101][102] Sachdev and collaborators proposed[103] a sign-problem free Monte Carlo method for studying the onset of antiferromagnetic order in metals: this yields a phase diagram with high temperature superconductivity similar to that found in many materials, and has led to much subsequent work describing the origin of high temperature superconductivity in realistic models of various materials. Nematic order was predicted for the iron-based superconductors,[104] and a new type of charge density wave, a d-form factor density wave, was predicted[105] for the hole-doped cuprates; both have been observed in numerous experiments.[106][107][108][109][110] The pseudogap metal of the hole-doped cuprates was argued[111] to be a metal with topological order, as discussed above, based partly on its natural connection to the d-form factor density wave. Soon after, the remarkable experiments of Badoux et al.[112] displayed evidence for a small Fermi surface state with topological order near optimal doping in YBCO, consistent with the overall theoretical picture presented in Sachdev's work.[113][114][115]

Books

References

  1. ^ "Subir Sachdev. Herchel Smith Professor of Physics, Harvard University". Official website.
  2. ^ "Annual Review of Condensed Matter Physics, Planning Editorial Committee – Volume 8, 2017". Annual Reviews Directory. Retrieved 14 September 2021.
  3. ^ "Annual Review of Condensed Matter Physics, Planning Editorial Committee – Volume 10, 2019". Annual Reviews Directory. Retrieved 14 September 2021.
  4. ^ "Quantum Entanglement in Nature". YouTube Video.
  5. ^ a b c d e Sachdev, Subir (1999). Quantum phase transitions. Cambridge University Press. ISBN 0-521-00454-3.
  6. ^ a b Damle, Kedar; Sachdev, Subir (1997). "Nonzero-temperature transport near quantum critical points". Physical Review B. 56 (14): 8714–8733. arXiv:cond-mat/9705206. Bibcode:1997PhRvB..56.8714D. doi:10.1103/PhysRevB.56.8714. ISSN 0163-1829. S2CID 16703727.
  7. ^ a b c Sachdev, Subir; Ye, Jinwu (1993). "Gapless spin-fluid ground state in a random quantum Heisenberg magnet". Physical Review Letters. 70 (21): 3339–3342. arXiv:cond-mat/9212030. Bibcode:1993PhRvL..70.3339S. doi:10.1103/PhysRevLett.70.3339. ISSN 0031-9007. PMID 10053843. S2CID 1103248.
  8. ^ a b Sachdev, Subir (2015). "Bekenstein-Hawking Entropy and Strange Metals". Physical Review X. 5 (4): 041025. arXiv:1506.05111. Bibcode:2015PhRvX...5d1025S. doi:10.1103/PhysRevX.5.041025. ISSN 2160-3308. S2CID 35748649.
  9. ^ Maldacena, Juan; Shenker, Stephen H.; Stanford, Douglas (2016). "A bound on chaos". Journal of High Energy Physics. 2016 (8): 106. arXiv:1503.01409. Bibcode:2016JHEP...08..106M. doi:10.1007/JHEP08(2016)106. ISSN 1029-8479. S2CID 84832638.
  10. ^ Dray, Tevian; 't Hooft, Gerard (1985). "The gravitational shock wave of a massless particle". Nuclear Physics B. 253: 173–188. Bibcode:1985NuPhB.253..173D. doi:10.1016/0550-3213(85)90525-5. hdl:1874/4758. ISSN 0550-3213.
  11. ^ Shenker, Stephen H.; Stanford, Douglas (2014). "Black holes and the butterfly effect". Journal of High Energy Physics. 2014 (3): 67. arXiv:1306.0622. Bibcode:2014JHEP...03..067S. doi:10.1007/JHEP03(2014)067. ISSN 1029-8479. S2CID 54184366.
  12. ^ a b Sachdev, Subir (2010). "Holographic Metals and the Fractionalized Fermi Liquid". Physical Review Letters. 105 (15): 151602. arXiv:1006.3794. Bibcode:2010PhRvL.105o1602S. doi:10.1103/PhysRevLett.105.151602. ISSN 0031-9007. PMID 21230891. S2CID 1773630.
  13. ^ a b Müller, Markus; Sachdev, Subir (2008). "Collective cyclotron motion of the relativistic plasma in graphene". Physical Review B. 78 (11): 115419. arXiv:0801.2970. Bibcode:2008PhRvB..78k5419M. doi:10.1103/PhysRevB.78.115419. ISSN 1098-0121. S2CID 20437676.
  14. ^ Bandurin, D. A.; Torre, I.; Kumar, R. K.; Ben Shalom, M.; Tomadin, A.; Principi, A.; Auton, G. H.; Khestanova, E.; Novoselov, K. S.; Grigorieva, I. V.; Ponomarenko, L. A.; Geim, A. K.; Polini, M. (2016). "Negative local resistance caused by viscous electron backflow in graphene". Science. 351 (6277): 1055–1058. arXiv:1509.04165. Bibcode:2016Sci...351.1055B. doi:10.1126/science.aad0201. ISSN 0036-8075. PMID 26912363. S2CID 45538235.
  15. ^ a b c Crossno, J.; Shi, J. K.; Wang, K.; Liu, X.; Harzheim, A.; Lucas, A.; Sachdev, S.; Kim, P.; Taniguchi, T.; Watanabe, K.; Ohki, T. A.; Fong, K. C. (2016). "Observation of the Dirac fluid and the breakdown of the Wiedemann-Franz law in graphene". Science. 351 (6277): 1058–1061. arXiv:1509.04713. Bibcode:2016Sci...351.1058C. doi:10.1126/science.aad0343. ISSN 0036-8075. PMID 26912362. S2CID 206641575.
  16. ^ Anderson, P.W. (1973). "Resonating valence bonds: A new kind of insulator?". Materials Research Bulletin. 8 (2): 153–160. doi:10.1016/0025-5408(73)90167-0. ISSN 0025-5408.
  17. ^ a b c Read, N.; Sachdev, Subir (1991). "Large-Nexpansion for frustrated quantum antiferromagnets". Physical Review Letters. 66 (13): 1773–1776. Bibcode:1991PhRvL..66.1773R. doi:10.1103/PhysRevLett.66.1773. ISSN 0031-9007. PMID 10043303.
  18. ^ a b Wen, X. G. (1991). "Mean-field theory of spin-liquid states with finite energy gap and topological orders". Physical Review B. 44 (6): 2664–2672. Bibcode:1991PhRvB..44.2664W. doi:10.1103/PhysRevB.44.2664. ISSN 0163-1829. PMID 9999836.
  19. ^ a b c d e f Jalabert, Rodolfo A.; Sachdev, Subir (1991). "Spontaneous alignment of frustrated bonds in an anisotropic, three-dimensional Ising model". Physical Review B. 44 (2): 686–690. Bibcode:1991PhRvB..44..686J. doi:10.1103/PhysRevB.44.686. ISSN 0163-1829. PMID 9999168.
  20. ^ a b c d Sachdev, S.; Vojta, M. (1999). "Translational symmetry breaking in two-dimensional antiferromagnets and superconductors". J. Phys. Soc. Jpn. 69, Supp. B: 1. arXiv:cond-mat/9910231. Bibcode:1999cond.mat.10231S.
  21. ^ a b c Sachdev, Subir (2019). "Topological order, emergent gauge fields, and Fermi surface reconstruction". Reports on Progress in Physics. 82 (1): 014001. arXiv:1801.01125. Bibcode:2019RPPh...82a4001S. doi:10.1088/1361-6633/aae110. ISSN 0034-4885. PMID 30210062. S2CID 52197314.
  22. ^ "Subir Sachdev, Perimeter Institute".
  23. ^ "Endowment Chairs at TIFR".
  24. ^ "Infosys Prize – Jury 2020". www.infosys-science-foundation.com. Retrieved 10 December 2020.
  25. ^ "New 2019 Academy Members Announced". 17 April 2019.
  26. ^ "IAS honorary fellows".
  27. ^ "INSA Foreign Fellows elected".
  28. ^ "ICTP – Dirac Medallists 2018". www.ictp.it.
  29. ^ "2018 Lars Onsager Prize Recipient".
  30. ^ "Dirac Medal awarded to Professor Subir Sachdev".
  31. ^ "Subir Sachdev NAS member".
  32. ^ "Condensed matter physicist Subir Sachdev to deliver Salam Distinguished Lectures 2014".
  33. ^ "Lorentz Chair".
  34. ^ "Nine Leading Researchers Join Stephen Hawking as Distinguished Research Chairs at PI". Perimeter Institute for Theoretical Physics.
  35. ^ "All Fellows – John Simon Guggenheim Memorial Foundation". John Simon Guggenheim Memorial Foundation. Retrieved 26 January 2010.
  36. ^ "APS Fellow archive". APS. Retrieved 21 September 2020.
  37. ^ "Past Fellows". sloan.org. Retrieved 23 October 2018.
  38. ^ "LeRoy Apker Award Recipient". American Physical Society. Retrieved 30 June 2010.
  39. ^ a b Read, N.; Sachdev, Subir (1989). "Valence-bond and spin-Peierls ground states of low-dimensional quantum antiferromagnets". Physical Review Letters. 62 (14): 1694–1697. Bibcode:1989PhRvL..62.1694R. doi:10.1103/PhysRevLett.62.1694. ISSN 0031-9007. PMID 10039740.
  40. ^ a b Read, N.; Sachdev, Subir (1990). "Spin-Peierls, valence-bond solid, and Néel ground states of low-dimensional quantum antiferromagnets". Physical Review B. 42 (7): 4568–4589. Bibcode:1990PhRvB..42.4568R. doi:10.1103/PhysRevB.42.4568. ISSN 0163-1829. PMID 9995989.
  41. ^ a b Sachdev, Subir; Read, N. (1991). "Large N Expansion for Frustrated and Doped Quantum Antiferromagnets". International Journal of Modern Physics B. 05 (1n02): 219–249. arXiv:cond-mat/0402109. Bibcode:1991IJMPB...5..219S. doi:10.1142/S0217979291000158. ISSN 0217-9792. S2CID 18042838.
  42. ^ a b Sachdev, Subir (1992). "Kagome and triangular-lattice Heisenberg antiferromagnets: Ordering from quantum fluctuations and quantum-disordered ground states with unconfined bosonic spinons". Physical Review B. 45 (21): 12377–12396. Bibcode:1992PhRvB..4512377S. doi:10.1103/PhysRevB.45.12377. ISSN 0163-1829. PMID 10001275.
  43. ^ Senthil, T.; Motrunich, O. (2002). "Microscopic models for fractionalized phases in strongly correlated systems". Physical Review B. 66 (20): 205104. arXiv:cond-mat/0201320. Bibcode:2002PhRvB..66t5104S. doi:10.1103/PhysRevB.66.205104. ISSN 0163-1829. S2CID 44027950.
  44. ^ Motrunich, O. I.; Senthil, T. (2002). "Exotic Order in Simple Models of Bosonic Systems". Physical Review Letters. 89 (27): 277004. arXiv:cond-mat/0205170. Bibcode:2002PhRvL..89A7004M. doi:10.1103/PhysRevLett.89.277004. ISSN 0031-9007. PMID 12513235. S2CID 9496517.
  45. ^ Chung, C. H.; Marston, J. B.; Sachdev, Subir (2001). "Quantum phases of the Shastry–Sutherland antiferromagnet: Application toSrCu2(BO3)2". Physical Review B. 64 (13): 134407. arXiv:cond-mat/0102222. Bibcode:2001PhRvB..64m4407C. doi:10.1103/PhysRevB.64.134407. ISSN 0163-1829. S2CID 115132482.
  46. ^ Zayed, M. E.; Rüegg, Ch.; Larrea J., J.; Läuchli, A. M.; Panagopoulos, C.; Saxena, S. S.; Ellerby, M.; McMorrow, D. F.; Strässle, Th.; Klotz, S.; Hamel, G.; Sadykov, R. A.; Pomjakushin, V.; Boehm, M.; Jiménez–Ruiz, M.; Schneidewind, A.; Pomjakushina, E.; Stingaciu, M.; Conder, K.; Rønnow, H. M. (2017). "4-spin plaquette singlet state in the Shastry–Sutherland compound SrCu2(BO3)2". Nature Physics. 13 (10): 962–966. arXiv:1603.02039. Bibcode:2017NatPh..13..962Z. doi:10.1038/nphys4190. ISSN 1745-2473. S2CID 59402393.
  47. ^ Mei, Jia-Wei; Chen, Ji-Yao; He, Huan; Wen, Xiao-Gang (2017). "Gapped spin liquid with Z2 topological order for the kagome Heisenberg model". Physical Review B. 95 (23): 235107. arXiv:1606.09639. Bibcode:2017PhRvB..95w5107M. doi:10.1103/PhysRevB.95.235107. ISSN 2469-9950. S2CID 119215027.
  48. ^ Punk, Matthias; Chowdhury, Debanjan; Sachdev, Subir (2014). "Topological excitations and the dynamic structure factor of spin liquids on the kagome lattice". Nature Physics. 10 (4): 289–293. arXiv:1308.2222. Bibcode:2014NatPh..10..289P. doi:10.1038/nphys2887. ISSN 1745-2473. S2CID 106398490.
  49. ^ Han, Tian-Heng; Helton, Joel S.; Chu, Shaoyan; Nocera, Daniel G.; Rodriguez-Rivera, Jose A.; Broholm, Collin; Lee, Young S. (2012). "Fractionalized excitations in the spin-liquid state of a kagome-lattice antiferromagnet". Nature. 492 (7429): 406–410. arXiv:1307.5047. Bibcode:2012Natur.492..406H. doi:10.1038/nature11659. ISSN 0028-0836. PMID 23257883. S2CID 4344923.
  50. ^ Fu, M.; Imai, T.; Han, T.-H.; Lee, Y. S. (2015). "Evidence for a gapped spin-liquid ground state in a kagome Heisenberg antiferromagnet". Science. 350 (6261): 655–658. arXiv:1511.02174. Bibcode:2015Sci...350..655F. doi:10.1126/science.aab2120. ISSN 0036-8075. PMID 26542565. S2CID 22287797.
  51. ^ Feng, Zili; Li, Zheng; Meng, Xin; Yi, Wei; Wei, Yuan; Zhang, Jun; Wang, Yan-Cheng; Jiang, Wei; Liu, Zheng; Li, Shiyan; Liu, Feng; Luo, Jianlin; Li, Shiliang; Zheng, Guo-qing; Meng, Zi Yang; Mei, Jia-Wei; Shi, Youguo (2017). "Gapped Spin-1/2 Spinon Excitations in a New Kagome Quantum Spin Liquid Compound Cu3Zn(OH)6FBr". Chinese Physics Letters. 34 (7): 077502. arXiv:1702.01658. Bibcode:2017ChPhL..34g7502F. doi:10.1088/0256-307X/34/7/077502. ISSN 0256-307X. S2CID 29531269.
  52. ^ Wei, Yuan; Feng, Zili; Lohstroh, Wiebke; dela Cruz, Clarina; Yi, Wei; Ding, Z.F.; Zhang, J.; Tan, Cheng; Shu, Lei; Wang, Yang-Cheng; Luo, Jianlin; Mei, Jia-Wei; Meng, Zi Yang; Shi, Youguo; Li, Shiliang (2017). "Evidence for a Z2 topological ordered quantum spin liquid in a kagome-lattice antiferromagnet". arXiv:1710.02991 [cond-mat.str-el].
  53. ^ Wen, Xiao-Gang (2017). "Discovery of Fractionalized Neutral Spin-1/2 Excitation of Topological Order". Chinese Physics Letters. 34 (9): 090101. Bibcode:2017ChPhL..34i0101W. doi:10.1088/0256-307X/34/9/090101. hdl:1721.1/124012. S2CID 250908913.
  54. ^ Bruin, J. A. N.; Sakai, H.; Perry, R. S.; Mackenzie, A. P. (2013). "Similarity of Scattering Rates in Metals Showing T-Linear Resistivity". Science. 339 (6121): 804–807. Bibcode:2013Sci...339..804B. doi:10.1126/science.1227612. ISSN 0036-8075. PMID 23413351. S2CID 206544038.
  55. ^ Wegner, Franz J. (1971). "Duality in Generalized Ising Models and Phase Transitions without Local Order Parameters". Journal of Mathematical Physics. 12 (10): 2259–2272. Bibcode:1971JMP....12.2259W. doi:10.1063/1.1665530. ISSN 0022-2488.
  56. ^ Schuler, Michael; Whitsitt, Seth; Henry, Louis-Paul; Sachdev, Subir; Läuchli, Andreas M. (2016). "Universal Signatures of Quantum Critical Points from Finite-Size Torus Spectra: A Window into the Operator Content of Higher-Dimensional Conformal Field Theories". Physical Review Letters. 117 (21): 210401. arXiv:1603.03042. Bibcode:2016PhRvL.117u0401S. doi:10.1103/PhysRevLett.117.210401. ISSN 0031-9007. PMID 27911517. S2CID 6860115.
  57. ^ Fradkin, Eduardo; Shenker, Stephen H. (1979). "Phase diagrams of lattice gauge theories with Higgs fields". Physical Review D. 19 (12): 3682–3697. Bibcode:1979PhRvD..19.3682F. doi:10.1103/PhysRevD.19.3682. ISSN 0556-2821.
  58. ^ a b c Senthil, T.; Balents, Leon; Sachdev, Subir; Vishwanath, Ashvin; Fisher, Matthew P. A. (2004). "Quantum criticality beyond the Landau-Ginzburg-Wilson paradigm". Physical Review B. 70 (14): 144407. arXiv:cond-mat/0312617. Bibcode:2004PhRvB..70n4407S. doi:10.1103/PhysRevB.70.144407. ISSN 1098-0121. S2CID 13489712.
  59. ^ Chubukov, Andrey V.; Senthil, T.; Sachdev, Subir (1994). "Universal magnetic properties of frustrated quantum antiferromagnets in two dimensions". Physical Review Letters. 72 (13): 2089–2092. arXiv:cond-mat/9311045. Bibcode:1994PhRvL..72.2089C. doi:10.1103/PhysRevLett.72.2089. ISSN 0031-9007. PMID 10055785. S2CID 18732398.
  60. ^ a b Senthil, T.; Vishwanath, Ashvin; Balents, Leon; Sachdev, Subir; Fisher, Matthew P. A. (2004). "Deconfined Quantum Critical Points". Science. 303 (5663): 1490–1494. arXiv:cond-mat/0311326. Bibcode:2004Sci...303.1490S. doi:10.1126/science.1091806. ISSN 0036-8075. PMID 15001771. S2CID 7023655.
  61. ^ Fradkin, Eduardo; Huse, David A.; Moessner, R.; Oganesyan, V.; Sondhi, S. L. (2004). "Bipartite Rokhsar–Kivelson points and Cantor deconfinement". Physical Review B. 69 (22): 224415. arXiv:cond-mat/0311353. Bibcode:2004PhRvB..69v4415F. doi:10.1103/PhysRevB.69.224415. ISSN 1098-0121. S2CID 119328669.
  62. ^ Vishwanath, Ashvin; Balents, L.; Senthil, T. (2004). "Quantum criticality and deconfinement in phase transitions between valence bond solids". Physical Review B. 69 (22): 224416. arXiv:cond-mat/0311085. Bibcode:2004PhRvB..69v4416V. doi:10.1103/PhysRevB.69.224416. ISSN 1098-0121. S2CID 118819626.
  63. ^ Chubukov, Andrey V.; Sachdev, Subir; Ye, Jinwu (1994). "Theory of two-dimensional quantum Heisenberg antiferromagnets with a nearly critical ground state". Physical Review B. 49 (17): 11919–11961. arXiv:cond-mat/9304046. Bibcode:1994PhRvB..4911919C. doi:10.1103/PhysRevB.49.11919. ISSN 0163-1829. PMID 10010065. S2CID 10371761.
  64. ^ Murthy, Ganpathy; Sachdev, Subir (1990). "Action of hedgehog instantons in the disordered phase of the (2 + 1)-dimensional CPN−1 model". Nuclear Physics B. 344 (3): 557–595. Bibcode:1990NuPhB.344..557M. doi:10.1016/0550-3213(90)90670-9. ISSN 0550-3213.
  65. ^ Dyer, Ethan; Mezei, Márk; Pufu, Silviu S.; Sachdev, Subir (2015). "Scaling dimensions of monopole operators in the CPN-1 theory in 2 + 1 dimensions". Journal of High Energy Physics. 2015 (6): 37. arXiv:1504.00368. Bibcode:2015JHEP...06..037D. doi:10.1007/JHEP06(2015)037. ISSN 1029-8479. S2CID 9724456.
  66. ^ Dyer, Ethan; Mezei, Márk; Pufu, Silviu S.; Sachdev, Subir (2016). "Erratum to: Scaling dimensions of monopole operators in the CPN-1 theory in 2 + 1 dimensions". Journal of High Energy Physics. 2016 (3): 111. arXiv:1504.00368. Bibcode:2016JHEP...03..111D. doi:10.1007/JHEP03(2016)111. ISSN 1029-8479. S2CID 195304831.
  67. ^ Block, Matthew S.; Melko, Roger G.; Kaul, Ribhu K. (2013). "Fate of CPN-1 Fixed Points with q Monopoles". Physical Review Letters. 111 (13): 137202. arXiv:1307.0519. Bibcode:2013PhRvL.111m7202B. doi:10.1103/PhysRevLett.111.137202. ISSN 0031-9007. PMID 24116811. S2CID 23088057.
  68. ^ Parcollet, Olivier; Georges, Antoine (1999). "Non-Fermi-liquid regime of a doped Mott insulator". Physical Review B. 59 (8): 5341–5360. arXiv:cond-mat/9806119. Bibcode:1999PhRvB..59.5341P. doi:10.1103/PhysRevB.59.5341. ISSN 0163-1829. S2CID 16912120.
  69. ^ Georges, A.; Parcollet, O.; Sachdev, S. (2001). "Quantum fluctuations of a nearly critical Heisenberg spin glass". Physical Review B. 63 (13): 134406. arXiv:cond-mat/0009388. Bibcode:2001PhRvB..63m4406G. doi:10.1103/PhysRevB.63.134406. ISSN 0163-1829. S2CID 10445601.
  70. ^ Sachdev, Subir; Young, A. P. (1997). "Low Temperature Relaxational Dynamics of the Ising Chain in a Transverse Field". Physical Review Letters. 78 (11): 2220–2223. arXiv:cond-mat/9609185. Bibcode:1997PhRvL..78.2220S. doi:10.1103/PhysRevLett.78.2220. ISSN 0031-9007. S2CID 31110608.
  71. ^ Sachdev, Subir; Damle, Kedar (1997). "Low Temperature Spin Diffusion in the One-Dimensional QuantumO(3)NonlinearσModel". Physical Review Letters. 78 (5): 943–946. arXiv:cond-mat/9610115. Bibcode:1997PhRvL..78..943S. doi:10.1103/PhysRevLett.78.943. ISSN 0031-9007. S2CID 51363066.
  72. ^ Damle, Kedar; Sachdev, Subir (1998). "Spin dynamics and transport in gapped one-dimensional Heisenberg antiferromagnets at nonzero temperatures". Physical Review B. 57 (14): 8307–8339. arXiv:cond-mat/9711014. Bibcode:1998PhRvB..57.8307D. doi:10.1103/PhysRevB.57.8307. ISSN 0163-1829. S2CID 15363782.
  73. ^ Takigawa, M.; Asano, T.; Ajiro, Y.; Mekata, M.; Uemura, Y. J. (1996). "Dynamics in theS=1One-Dimensional Antiferromagnet AgVP2S6 via 31P and 51V NMR". Physical Review Letters. 76 (12): 2173–2176. Bibcode:1996PhRvL..76.2173T. doi:10.1103/PhysRevLett.76.2173. ISSN 0031-9007. PMID 10060624.
  74. ^ Xu, G.; Broholm, C.; Soh, Y.-A.; Aeppli, G.; DiTusa, J. F.; Chen, Y.; Kenzelmann, M.; Frost, C. D.; Ito, T.; Oka, K.; Takagi, H. (2007). "Mesoscopic Phase Coherence in a Quantum Spin Fluid". Science. 317 (5841): 1049–1052. arXiv:0804.0211. Bibcode:2007Sci...317.1049X. doi:10.1126/science.1143831. ISSN 0036-8075. PMID 17656685. S2CID 46317974.
  75. ^ Kinross, A. W.; Fu, M.; Munsie, T. J.; Dabkowska, H. A.; Luke, G. M.; Sachdev, Subir; Imai, T. (2014). "Evolution of Quantum Fluctuations Near the Quantum Critical Point of the Transverse Field Ising Chain System CoNb2O6". Physical Review X. 4 (3): 031008. arXiv:1401.6917. Bibcode:2014PhRvX...4c1008K. doi:10.1103/PhysRevX.4.031008. ISSN 2160-3308. S2CID 53464054.
  76. ^ Sachdev, S.; Buragohain, C.; Vojta, M. (1999). "Quantum Impurity in a Nearly Critical Two-Dimensional Antiferromagnet". Science. 286 (5449): 2479–2482. arXiv:cond-mat/0004156. doi:10.1126/science.286.5449.2479. ISSN 0036-8075. PMID 10617456. S2CID 33160119.
  77. ^ Kolezhuk, Alexei; Sachdev, Subir; Biswas, Rudro R.; Chen, Peiqiu (2006). "Theory of quantum impurities in spin liquids". Physical Review B. 74 (16): 165114. arXiv:cond-mat/0606385. Bibcode:2006PhRvB..74p5114K. doi:10.1103/PhysRevB.74.165114. ISSN 1098-0121. S2CID 119375810.
  78. ^ Kaul, Ribhu K.; Melko, Roger G.; Metlitski, Max A.; Sachdev, Subir (2008). "Imaging Bond Order near Nonmagnetic Impurities in Square-Lattice Antiferromagnets". Physical Review Letters. 101 (18): 187206. arXiv:0808.0495. Bibcode:2008PhRvL.101r7206K. doi:10.1103/PhysRevLett.101.187206. ISSN 0031-9007. PMID 18999862. S2CID 13624296.
  79. ^ Sachdev, Subir; Sengupta, K.; Girvin, S. M. (2002). "Mott insulators in strong electric fields". Physical Review B. 66 (7): 075128. arXiv:cond-mat/0205169. Bibcode:2002PhRvB..66g5128S. doi:10.1103/PhysRevB.66.075128. ISSN 0163-1829. S2CID 119478443.
  80. ^ Simon, Jonathan; Bakr, Waseem S.; Ma, Ruichao; Tai, M. Eric; Preiss, Philipp M.; Greiner, Markus (2011). "Quantum simulation of antiferromagnetic spin chains in an optical lattice". Nature. 472 (7343): 307–312. arXiv:1103.1372. Bibcode:2011Natur.472..307S. doi:10.1038/nature09994. ISSN 0028-0836. PMID 21490600. S2CID 3790620.
  81. ^ Meinert, F.; Mark, M. J.; Kirilov, E.; Lauber, K.; Weinmann, P.; Daley, A. J.; Nägerl, H.-C. (2013). "Quantum Quench in an Atomic One-Dimensional Ising Chain". Physical Review Letters. 111 (5): 053003. arXiv:1304.2628. Bibcode:2013PhRvL.111e3003M. doi:10.1103/PhysRevLett.111.053003. ISSN 0031-9007. PMID 23952393. S2CID 27242806.
  82. ^ Fendley, Paul; Sengupta, K.; Sachdev, Subir (2004). "Competing density-wave orders in a one-dimensional hard-boson model". Physical Review B. 69 (7): 075106. arXiv:cond-mat/0309438. Bibcode:2004PhRvB..69g5106F. doi:10.1103/PhysRevB.69.075106. ISSN 1098-0121. S2CID 51063893.
  83. ^ Bernien, Hannes; Schwartz, Sylvain; Keesling, Alexander; Levine, Harry; Omran, Ahmed; Pichler, Hannes; Choi, Soonwon; Zibrov, Alexander S.; Endres, Manuel; Greiner, Markus; Vuletić, Vladan; Lukin, Mikhail D. (2017). "Probing many-body dynamics on a 51-atom quantum simulator". Nature. 551 (7682): 579–584. arXiv:1707.04344. Bibcode:2017Natur.551..579B. doi:10.1038/nature24622. ISSN 0028-0836. PMID 29189778. S2CID 205261845.
  84. ^ Senthil, T.; Sachdev, Subir; Vojta, Matthias (2003). "Fractionalized Fermi Liquids". Physical Review Letters. 90 (21): 216403. arXiv:cond-mat/0209144. Bibcode:2003PhRvL..90u6403S. doi:10.1103/PhysRevLett.90.216403. ISSN 0031-9007. PMID 12786577. S2CID 16211890.
  85. ^ a b Senthil, T.; Vojta, Matthias; Sachdev, Subir (2004). "Weak magnetism and non-Fermi liquids near heavy-fermion critical points". Physical Review B. 69 (3): 035111. arXiv:cond-mat/0305193. Bibcode:2004PhRvB..69c5111S. doi:10.1103/PhysRevB.69.035111. ISSN 1098-0121. S2CID 28588064.
  86. ^ Paramekanti, Arun; Vishwanath, Ashvin (2004). "Extending Luttinger's theorem to Z2 fractionalized phases of matter". Physical Review B. 70 (24): 245118. arXiv:cond-mat/0406619. Bibcode:2004PhRvB..70x5118P. doi:10.1103/PhysRevB.70.245118. ISSN 1098-0121. S2CID 119509835.
  87. ^ Maksimovic, Nikola; Analytis, James (2021). "Evidence for a delocalization quantum phase transition without symmetry breaking in CeCoIn5". Science. 375 (6576): 76–81. doi:10.1126/science.aaz4566. OSTI 1856508. PMID 34855511. S2CID 245828322.
  88. ^ Katz, Emanuel; Sachdev, Subir; Sørensen, Erik S.; Witczak-Krempa, William (2014). "Conformal field theories at nonzero temperature: Operator product expansions, Monte Carlo, and holography". Physical Review B. 90 (24): 245109. arXiv:1409.3841. Bibcode:2014PhRvB..90x5109K. doi:10.1103/PhysRevB.90.245109. ISSN 1098-0121. S2CID 7679342.
  89. ^ Herzog, Christopher P.; Kovtun, Pavel; Sachdev, Subir; Son, Dam Thanh (2007). "Quantum critical transport, duality, and M theory". Physical Review D. 75 (8): 085020. arXiv:hep-th/0701036. Bibcode:2007PhRvD..75h5020H. doi:10.1103/PhysRevD.75.085020. ISSN 1550-7998. S2CID 51192704.
  90. ^ Myers, Robert C.; Sachdev, Subir; Singh, Ajay (2011). "Holographic quantum critical transport without self-duality". Physical Review D. 83 (6): 066017. arXiv:1010.0443. Bibcode:2011PhRvD..83f6017M. doi:10.1103/PhysRevD.83.066017. ISSN 1550-7998. S2CID 8917892.
  91. ^ Witczak-Krempa, William; Sørensen, Erik S.; Sachdev, Subir (2014). "The dynamics of quantum criticality revealed by quantum Monte Carlo and holography" (PDF). Nature Physics. 10 (5): 361–366. arXiv:1309.2941. Bibcode:2014NatPh..10..361W. doi:10.1038/nphys2913. ISSN 1745-2473. S2CID 53623028.
  92. ^ Witczak-Krempa, William; Sachdev, Subir (2012). "Quasinormal modes of quantum criticality". Physical Review B. 86 (23): 235115. arXiv:1210.4166. Bibcode:2012PhRvB..86w5115W. doi:10.1103/PhysRevB.86.235115. ISSN 1098-0121. S2CID 44049139.
  93. ^ Hartnoll, Sean A.; Kovtun, Pavel K.; Müller, Markus; Sachdev, Subir (2007). "Theory of the Nernst effect near quantum phase transitions in condensed matter and in dyonic black holes". Physical Review B. 76 (14): 144502. arXiv:0706.3215. Bibcode:2007PhRvB..76n4502H. doi:10.1103/PhysRevB.76.144502. ISSN 1098-0121. S2CID 50832996.
  94. ^ Lucas, Andrew; Sachdev, Subir (2015). "Memory matrix theory of magnetotransport in strange metals". Physical Review B. 91 (19): 195122. arXiv:1502.04704. Bibcode:2015PhRvB..91s5122L. doi:10.1103/PhysRevB.91.195122. ISSN 1098-0121. S2CID 58941656.
  95. ^ Müller, Markus; Fritz, Lars; Sachdev, Subir (2008). "Quantum-critical relativistic magnetotransport in graphene". Physical Review B. 78 (11): 115406. arXiv:0805.1413. Bibcode:2008PhRvB..78k5406M. doi:10.1103/PhysRevB.78.115406. ISSN 1098-0121. S2CID 2501609.
  96. ^ Lucas, Andrew; Davison, Richard A.; Sachdev, Subir (2016). "Hydrodynamic theory of thermoelectric transport and negative magnetoresistance in Weyl semimetals". Proceedings of the National Academy of Sciences. 113 (34): 9463–9468. arXiv:1604.08598. Bibcode:2016PNAS..113.9463L. doi:10.1073/pnas.1608881113. ISSN 0027-8424. PMC 5003291. PMID 27512042.
  97. ^ Gooth, Johannes; Niemann, Anna C.; Meng, Tobias; Grushin, Adolfo G.; Landsteiner, Karl; Gotsmann, Bernd; Menges, Fabian; Schmidt, Marcus; Shekhar, Chandra; Süß, Vicky; Hühne, Ruben; Rellinghaus, Bernd; Felser, Claudia; Yan, Binghai; Nielsch, Kornelius (2017). "Experimental signatures of the mixed axial–gravitational anomaly in the Weyl semimetal NbP". Nature. 547 (7663): 324–327. arXiv:1703.10682. Bibcode:2017Natur.547..324G. doi:10.1038/nature23005. ISSN 0028-0836. PMID 28726829. S2CID 205257613.
  98. ^ Ball, Philip (2017). "Big Bang gravitational effect observed in lab crystal". Nature. doi:10.1038/nature.2017.22338. ISSN 1476-4687.
  99. ^ Demler, Eugene; Sachdev, Subir; Zhang, Ying (2001). "Spin-Ordering Quantum Transitions of Superconductors in a Magnetic Field". Physical Review Letters. 87 (6): 067202. arXiv:cond-mat/0103192. Bibcode:2001PhRvL..87f7202D. doi:10.1103/PhysRevLett.87.067202. ISSN 0031-9007. PMID 11497851. S2CID 1423617.
  100. ^ Zhang, Ying; Demler, Eugene; Sachdev, Subir (2002). "Competing orders in a magnetic field: Spin and charge order in the cuprate superconductors". Physical Review B. 66 (9): 094501. arXiv:cond-mat/0112343. Bibcode:2002PhRvB..66i4501Z. doi:10.1103/PhysRevB.66.094501. ISSN 0163-1829. S2CID 13856528.
  101. ^ Lake, B.; Rønnow, H. M.; Christensen, N. B.; Aeppli, G.; Lefmann, K.; McMorrow, D. F.; Vorderwisch, P.; Smeibidl, P.; Mangkorntong, N.; Sasagawa, T.; Nohara, M.; Takagi, H.; Mason, T. E. (2002). "Antiferromagnetic order induced by an applied magnetic field in a high-temperature superconductor". Nature. 415 (6869): 299–302. arXiv:cond-mat/0201349. Bibcode:2002Natur.415..299L. doi:10.1038/415299a. ISSN 0028-0836. PMID 11797002. S2CID 4354661.
  102. ^ Khaykovich, B.; Wakimoto, S.; Birgeneau, R. J.; Kastner, M. A.; Lee, Y. S.; Smeibidl, P.; Vorderwisch, P.; Yamada, K. (2005). "Field-induced transition between magnetically disordered and ordered phases in underdopedLa2−xSrxCuO4". Physical Review B. 71 (22): 220508. arXiv:cond-mat/0411355. Bibcode:2005PhRvB..71v0508K. doi:10.1103/PhysRevB.71.220508. ISSN 1098-0121. S2CID 118979811.
  103. ^ Berg, E.; Metlitski, M. A.; Sachdev, S. (2012). "Sign-Problem-Free Quantum Monte Carlo of the Onset of Antiferromagnetism in Metals". Science. 338 (6114): 1606–1609. arXiv:1206.0742. Bibcode:2012Sci...338.1606B. doi:10.1126/science.1227769. ISSN 0036-8075. PMID 23258893. S2CID 20745901.
  104. ^ Xu, Cenke; Müller, Markus; Sachdev, Subir (2008). "Ising and spin orders in the iron-based superconductors". Physical Review B. 78 (2): 020501. arXiv:0804.4293. Bibcode:2008PhRvB..78b0501X. doi:10.1103/PhysRevB.78.020501. ISSN 1098-0121. S2CID 6815720.
  105. ^ Sachdev, Subir; La Placa, Rolando (2013). "Bond Order in Two-Dimensional Metals with Antiferromagnetic Exchange Interactions". Physical Review Letters. 111 (2): 027202. arXiv:1303.2114. Bibcode:2013PhRvL.111b7202S. doi:10.1103/PhysRevLett.111.027202. ISSN 0031-9007. PMID 23889434. S2CID 14248654.
  106. ^ Fujita, K.; Hamidian, M. H.; Edkins, S. D.; Kim, C. K.; Kohsaka, Y.; Azuma, M.; Takano, M.; Takagi, H.; Eisaki, H.; Uchida, S.-i.; Allais, A.; Lawler, M. J.; Kim, E.-A.; Sachdev, S.; Davis, J. C. S. (2014). "Direct phase-sensitive identification of a d-form factor density wave in underdoped cuprates". Proceedings of the National Academy of Sciences. 111 (30): E3026–E3032. arXiv:1404.0362. Bibcode:2014PNAS..111E3026F. doi:10.1073/pnas.1406297111. ISSN 0027-8424. PMC 4121838. PMID 24989503.
  107. ^ Comin, R.; Sutarto, R.; He, F.; da Silva Neto, E. H.; Chauviere, L.; Fraño, A.; Liang, R.; Hardy, W. N.; Bonn, D. A.; Yoshida, Y.; Eisaki, H.; Achkar, A. J.; Hawthorn, D. G.; Keimer, B.; Sawatzky, G. A.; Damascelli, A. (2015). "Symmetry of charge order in cuprates". Nature Materials. 14 (8): 796–800. arXiv:1402.5415. Bibcode:2015NatMa..14..796C. doi:10.1038/nmat4295. ISSN 1476-1122. PMID 26006005. S2CID 11830487.
  108. ^ Hamidian, M. H.; Edkins, S. D.; Kim, Chung Koo; Davis, J. C.; Mackenzie, A. P.; Eisaki, H.; Uchida, S.; Lawler, M. J.; Kim, E.-A.; Sachdev, S.; Fujita, K. (2016). "Atomic-scale electronic structure of the cuprate d-symmetry form factor density wave state". Nature Physics. 12 (2): 150–156. arXiv:1507.07865. Bibcode:2016NatPh..12..150H. doi:10.1038/nphys3519. ISSN 1745-2473. S2CID 117974569.
  109. ^ Forgan, E. M.; Blackburn, E.; Holmes, A. T.; Briffa, A. K. R.; Chang, J.; Bouchenoire, L.; Brown, S. D.; Liang, Ruixing; Bonn, D.; Hardy, W. N.; Christensen, N. B.; Zimmermann, M. V.; Hücker, M.; Hayden, S. M. (2015). "The microscopic structure of charge density waves in underdoped YBa2Cu3O6.54 revealed by X-ray diffraction". Nature Communications. 6: 10064. Bibcode:2015NatCo...610064F. doi:10.1038/ncomms10064. ISSN 2041-1723. PMC 4682044. PMID 26648114.
  110. ^ Chu, J.-H.; Kuo, H.-H.; Analytis, J. G.; Fisher, I. R. (2012). "Divergent Nematic Susceptibility in an Iron Arsenide Superconductor". Science. 337 (6095): 710–712. arXiv:1203.3239. Bibcode:2012Sci...337..710C. doi:10.1126/science.1221713. ISSN 0036-8075. PMID 22879513. S2CID 8777939.
  111. ^ Chowdhury, Debanjan; Sachdev, Subir (2014). "Density-wave instabilities of fractionalized Fermi liquids". Physical Review B. 90 (24): 245136. arXiv:1409.5430. Bibcode:2014PhRvB..90x5136C. doi:10.1103/PhysRevB.90.245136. ISSN 1098-0121. S2CID 44966610.
  112. ^ Badoux, S.; Tabis, W.; Laliberté, F.; Grissonnanche, G.; Vignolle, B.; Vignolles, D.; Béard, J.; Bonn, D. A.; Hardy, W. N.; Liang, R.; Doiron-Leyraud, N.; Taillefer, Louis; Proust, Cyril (2016). "Change of carrier density at the pseudogap critical point of a cuprate superconductor". Nature. 531 (7593): 210–214. arXiv:1511.08162. Bibcode:2016Natur.531..210B. doi:10.1038/nature16983. ISSN 0028-0836. PMID 26901870. S2CID 205247746.
  113. ^ Sachdev, Subir (2016). "Emergent gauge fields and the high-temperature superconductors". Philosophical Transactions of the Royal Society A: Mathematical, Physical and Engineering Sciences. 374 (2075): 20150248. arXiv:1512.00465. Bibcode:2016RSPTA.37450248S. doi:10.1098/rsta.2015.0248. ISSN 1364-503X. PMID 27458260. S2CID 19630107.
  114. ^ Sachdev, Subir; Chowdhury, Debanjan (2016). "The novel metallic states of the cuprates: Topological Fermi liquids and strange metals". Progress of Theoretical and Experimental Physics. 2016 (12): 12C102. arXiv:1605.03579. Bibcode:2016PTEP.2016lC102S. doi:10.1093/ptep/ptw110. ISSN 2050-3911. S2CID 119275712.
  115. ^ Sachdev, Subir; Metlitski, Max A.; Qi, Yang; Xu, Cenke (2009). "Fluctuating spin density waves in metals". Physical Review B. 80 (15): 155129. arXiv:0907.3732. Bibcode:2009PhRvB..80o5129S. doi:10.1103/PhysRevB.80.155129. ISSN 1098-0121. S2CID 28060808.

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