Geometric orthogonal metals: Hidden antiferromagnetism and pseudogap from fluctuating stripes
Pith reviewed 2026-05-23 17:31 UTC · model grok-4.3
The pith
Fluctuating domain walls in doped cuprates generate a geometric orthogonal metal with hidden antiferromagnetic order that produces a small Fermi surface without symmetry breaking.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
The central claim is that an orthogonal metal with geometric origin emerges from the proliferation of domain walls stabilized by charge fluctuations. These domain walls obscure underlying long-range antiferromagnetic order in real-space but preserve order in the reference frame of the background spins. Well-defined fermionic quasiparticles as magnetic polarons couple to Z2 topological excitations of the domain wall string-net condensate, constituting a small Fermi surface. At critical doping, hidden order is lost at a hidden quantum critical point.
What carries the argument
Domain wall string-net condensate whose Z2 topological excitations couple to magnetic polarons to realize hidden order.
If this is right
- Establishes a deep connection between the antiferromagnetic, stripe, and pseudogap phases.
- At a critical doping value hidden order is lost, driving a transition to a regular Fermi liquid at a hidden quantum critical point featuring quantum critical transport properties.
- Suggests a possible unification of superconductivity in electron and hole doped cuprates and heavy fermion compounds.
Where Pith is reading between the lines
- Similar hidden-order mechanisms from fluctuating domain walls could apply to other doped Mott insulators that show small Fermi surfaces.
- Spin-frame-sensitive probes such as certain polarized neutron or NMR experiments might reveal the preserved antiferromagnetic order that is invisible in real-space measurements.
- The framework predicts that electron-doped cuprates should exhibit an analogous hidden quantum critical point separating pseudogap-like behavior from a Fermi liquid.
Load-bearing premise
Charge fluctuations must produce a proliferating domain-wall string-net condensate whose Z2 topological excitations couple to magnetic polarons to yield a small Fermi surface without symmetry breaking.
What would settle it
ARPES measurements showing an abrupt change from small to large Fermi surface without accompanying quantum critical transport signatures at the doping where the pseudogap closes would falsify the hidden-order transition.
Figures
read the original abstract
One of the key features of hole-doped cuprates is the presence of an extended pseudogap phase, whose microscopic origin has been the subject of intense investigation since its discovery and is believed to be crucial for understanding high-temperature superconductivity. Various explanations have been proposed for the pseudogap, including links to symmetry-breaking orders such as stripes or pairing, and the emergence of novel fractionalized Fermi liquid (FL*) and orthogonal metal (OM) phases. The topological nature of FL* and OM phases has been identified as scenarios compatible with a small Fermi surface without symmetry breaking, as suggested experimentally. With recent experimental and numerical studies supporting an intricate relationship between stripe order and the pseudogap phase, we here propose an alternative scenario: an orthogonal metal with a geometric origin (GOM) driven by fluctuating domain walls. The essential mechanism behind our proposal is hidden order, where the proliferation of domain walls stabilized by charge fluctuations obscures the underlying long-range antiferromagnetic order in real-space, but order is preserved in the reference frame of the background spins. As a result, well-defined fermionic quasiparticles in the form of magnetic polarons exist, which couple to $\mathbb{Z}_2$ topological excitations of the domain wall string-net condensate in the ground state and constitute a small Fermi surface. At a critical doping value, we argue that hidden order is lost, driving a transition to a regular Fermi liquid at a hidden quantum critical point (hQCP) featuring quantum critical transport properties. Our GOM framework establishes a deep connection between the antiferromagnetic, stripe, and pseudogap phases, and suggests a possible unification of superconductivity in (electron and hole) doped cuprates and heavy fermion compounds.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript proposes a 'geometric orthogonal metal' (GOM) phase in hole-doped cuprates arising from fluctuating domain walls (stripes) stabilized by charge fluctuations. This produces 'hidden order' in which long-range antiferromagnetism is obscured in real space but preserved in the background-spin reference frame; magnetic polarons then couple to Z2 topological excitations of a domain-wall string-net condensate, yielding a small Fermi surface without symmetry breaking. At a critical doping the hidden order is lost at a hidden quantum critical point (hQCP) that connects to a conventional Fermi liquid, thereby linking the antiferromagnetic, stripe, and pseudogap regimes and suggesting a unification with heavy-fermion superconductivity.
Significance. If the proposed mechanism can be realized in a controlled microscopic model, the GOM scenario would supply a concrete route to a small Fermi surface without symmetry breaking that is tied to stripe fluctuations, offering a unified picture of the pseudogap, hidden order, and quantum criticality across cuprates and heavy-fermion systems. The absence of any explicit Hamiltonian, slave-particle construction, string-net wave function, or spectral-function calculation means the central claim remains a qualitative conjecture rather than a derived result.
major comments (3)
- [Abstract] Abstract (and opening paragraphs): The central claim that charge fluctuations produce a proliferating domain-wall string-net condensate whose Z2 excitations couple to magnetic polarons to generate a small Fermi surface while preserving hidden AF order is asserted but not derived from any microscopic Hamiltonian or effective theory. No slave-particle ansatz, string-net wave function, or spectral-function computation is supplied to demonstrate that the coupling actually produces the claimed small FS without symmetry breaking.
- [Abstract] Abstract (paragraph on hidden QCP): The transition at the hidden quantum critical point is described as driving a change from GOM to a regular Fermi liquid with quantum-critical transport, yet no controlled limit, renormalization-group analysis, or numerical evidence is given that establishes the existence or location of this hQCP.
- [Abstract] Abstract (final paragraph): The unification of superconductivity in electron- and hole-doped cuprates with heavy-fermion compounds is suggested on the basis of the GOM framework, but the manuscript contains no explicit comparison of pairing mechanisms, Fermi-surface topologies, or critical exponents that would substantiate the claimed connection.
Simulated Author's Rebuttal
We thank the referee for the detailed report. The manuscript is a conceptual proposal for a geometric orthogonal metal phase in cuprates, and we address the concerns regarding the lack of explicit derivations by clarifying the scope of the work.
read point-by-point responses
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Referee: [Abstract] Abstract (and opening paragraphs): The central claim that charge fluctuations produce a proliferating domain-wall string-net condensate whose Z2 excitations couple to magnetic polarons to generate a small Fermi surface while preserving hidden AF order is asserted but not derived from any microscopic Hamiltonian or effective theory. No slave-particle ansatz, string-net wave function, or spectral-function computation is supplied to demonstrate that the coupling actually produces the claimed small FS without symmetry breaking.
Authors: We acknowledge that our manuscript presents this as a proposed scenario rather than a fully derived result from a microscopic model. The GOM phase is motivated by combining known elements: fluctuating stripes leading to domain walls, hidden antiferromagnetism, magnetic polarons, and Z2 topological excitations in a string-net condensate. We will revise the abstract to emphasize that this is a qualitative conjecture inspired by recent experimental and numerical studies on stripes and the pseudogap, with the explicit construction of the wave function or spectral functions being an important direction for future research. revision: yes
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Referee: [Abstract] Abstract (paragraph on hidden QCP): The transition at the hidden quantum critical point is described as driving a change from GOM to a regular Fermi liquid with quantum-critical transport, yet no controlled limit, renormalization-group analysis, or numerical evidence is given that establishes the existence or location of this hQCP.
Authors: The hQCP is proposed as the point where the hidden order associated with the domain-wall condensate is lost upon increasing doping, leading to a conventional Fermi liquid. This is argued on phenomenological grounds, linking to the known quantum critical doping in cuprates where the pseudogap ends. While we do not provide a new RG analysis here, the concept builds on existing literature on quantum criticality in these systems. We can add a discussion referencing relevant numerical works on the stripe quantum critical point. revision: partial
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Referee: [Abstract] Abstract (final paragraph): The unification of superconductivity in electron- and hole-doped cuprates with heavy-fermion compounds is suggested on the basis of the GOM framework, but the manuscript contains no explicit comparison of pairing mechanisms, Fermi-surface topologies, or critical exponents that would substantiate the claimed connection.
Authors: The unification is suggested as an outlook based on the common appearance of small Fermi surfaces without symmetry breaking and the role of quantum criticality in both classes of materials. We do not claim a detailed mapping of pairing mechanisms or exponents in this work, which focuses on the normal-state physics. We will revise the final paragraph of the abstract to present this as a speculative connection rather than a substantiated unification. revision: yes
Circularity Check
No significant circularity; proposal is qualitative with no explicit derivations or self-referential reductions.
full rationale
The provided abstract and context contain no equations, Hamiltonians, or derivation steps that could be inspected for self-definition, fitted inputs renamed as predictions, or load-bearing self-citations. The GOM mechanism is presented as a conceptual proposal linking existing stripe and OM ideas to a small FS via hidden order, without any reduction of the central claim to its own inputs by construction. This matches the default expectation of a non-circular conceptual paper; the reader's assessment that circularity cannot be assessed from the abstract is consistent with the absence of load-bearing mathematical steps.
Axiom & Free-Parameter Ledger
axioms (1)
- domain assumption Long-range antiferromagnetic order exists in the undoped parent cuprate compound and can be referenced to background spins even when obscured in real space.
invented entities (2)
-
Geometric orthogonal metal (GOM)
no independent evidence
-
hidden quantum critical point (hQCP)
no independent evidence
Lean theorems connected to this paper
-
IndisputableMonolith/Foundation/AlexanderDuality.leanalexander_duality_circle_linking unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
proliferation of domain walls ... couple to Z2 topological excitations of the domain wall string-net condensate ... small Fermi surface ... hidden quantum critical point (hQCP)
What do these tags mean?
- matches
- The paper's claim is directly supported by a theorem in the formal canon.
- supports
- The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
- extends
- The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
- uses
- The paper appears to rely on the theorem as machinery.
- contradicts
- The paper's claim conflicts with a theorem or certificate in the canon.
- unclear
- Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.
Reference graph
Works this paper leans on
-
[1]
Possible high Tc superconductivity in the Ba-La-Cu-O system,
“Possible high Tc superconductivity in the Ba-La-Cu-O system,” Zeitschrift f¨ ur Physik B Condensed Matter64, 189–193 (1986)
work page 1986
-
[2]
Doping a Mott insulator: Physics of high-temperature superconductiv- ity,
P. A. Lee, N. Nagaosa, and X.-G. Wen, “Doping a Mott insulator: Physics of high-temperature superconductiv- ity,” Rev. Mod. Phys. 78, 17–85 (2006)
work page 2006
-
[3]
From quantum matter to high- temperature superconductivity in copper oxides,
B. Keimer, S. A. Kivelson, M. R. Norman, S. Uchida, and J. Zaanen, “From quantum matter to high- temperature superconductivity in copper oxides,” Na- ture 518, 179–186 (2015)
work page 2015
-
[4]
The pseudogap in high- temperature superconductors: an experimental survey,
T. Timusk and B. Statt, “The pseudogap in high- temperature superconductors: an experimental survey,” Reports on Progress in Physics 62, 61 (1999)
work page 1999
-
[5]
The pseudo- gap: friend or foe of high Tc ?
M. R. Norman, D. Pines, and C. Kallin, “The pseudo- gap: friend or foe of high Tc ?” Advances in Physics 54, 715–733 (2005)
work page 2005
-
[6]
The Enigma of the Pseudogap Phase of the Cuprate Superconductors,
D. Chowdhury and S. Sachdev, “The Enigma of the Pseudogap Phase of the Cuprate Superconductors,” in Quantum Criticality in Condensed Matter , pp. 1–43
-
[7]
Nodal Quasiparticles and Antinodal Charge Ordering in Ca2−xNaxCuO2Cl2,
K. M. Shen, F. Ronning, D. H. Lu, F. Baumberger, N. J. C. Ingle, W. S. Lee, W. Meevasana, Y. Kohsaka, M. Azuma, M. Takano, H. Takagi, and Z.-X. Shen, “Nodal Quasiparticles and Antinodal Charge Ordering in Ca2−xNaxCuO2Cl2,” Science 307, 901–904 (2005)
work page 2005
-
[8]
Evolution of the pseudogap from Fermi arcs to the nodal liquid,
A. Kanigel, M. R. Norman, M. Randeria, U. Chatterjee, S. Souma, A. Kaminski, H. M. Fretwell, S. Rosenkranz, M. Shi, T. Sato, T. Takahashi, Z. Z. Li, H. Raffy, K. Kadowaki, D. Hinks, L. Ozyuzer, and J. C. Cam- puzano, “Evolution of the pseudogap from Fermi arcs to the nodal liquid,” Nature Physics 2, 447–451 (2006)
work page 2006
-
[9]
Reconstructed Fermi Surface of Underdoped Bi2Sr2CaCu2O8+δ Cuprate Superconductors,
H.-B. Yang, J. D. Rameau, Z.-H. Pan, G. D. Gu, P. D. Johnson, H. Claus, D. G. Hinks, and T. E. Kidd, “Reconstructed Fermi Surface of Underdoped Bi2Sr2CaCu2O8+δ Cuprate Superconductors,” Phys. Rev. Lett. 107, 047003 (2011)
work page 2011
-
[10]
Unveiling phase diagram of the lightly doped high-Tc cuprate superconductors with disorder removed,
K. Kurokawa, S. Isono, Y. Kohama, S. Kunisada, S. Sakai, R. Sekine, M. Okubo, M. D. Watson, T. K. Kim, C. Cacho, S. Shin, T. Tohyama, K. Tokiwa, and T. Kondo, “Unveiling phase diagram of the lightly doped high-Tc cuprate superconductors with disorder removed,” Nature Communications 14, 4064 (2023)
work page 2023
-
[11]
Quantum oscillations and the Fermi surface in an underdoped high-Tc superconduc- tor,
N. Doiron-Leyraud, C. Proust, D. LeBoeuf, J. Leval- lois, J.-B. Bonnemaison, R. Liang, D. A. Bonn, W. N. Hardy, and L. Taillefer, “Quantum oscillations and the Fermi surface in an underdoped high-Tc superconduc- tor,” Nature 447, 565–568 (2007)
work page 2007
-
[12]
Quantum oscillations in an overdoped high-tc superconductor,
B. Vignolle, A. Carrington, R. A. Cooper, M. M. J. French, A. P. Mackenzie, C. Jaudet, D. Vignolles, C. Proust, and N. E. Hussey, “Quantum oscillations in an overdoped high-tc superconductor,” Nature 455, 952–955 (2008)
work page 2008
-
[13]
Quantum Oscillations in the Underdoped Cuprate YBa2Cu4O8,
E. A. Yelland, J. Singleton, C. H. Mielke, N. Harri- son, F. F. Balakirev, B. Dabrowski, and J. R. Cooper, “Quantum Oscillations in the Underdoped Cuprate YBa2Cu4O8,” Phys. Rev. Lett. 100, 047003 (2008)
work page 2008
-
[14]
B. J. Ramshaw, B. Vignolle, J. Day, R. Liang, W. N. Hardy, C. Proust, and D. A. Bonn, “Angle depen- dence of quantum oscillations in YBa2Cu3O6.59 shows free-spin behaviour of quasiparticles,” Nature Physics 7, 234–238 (2011)
work page 2011
-
[15]
Y. Ando, Y. Kurita, S. Komiya, S. Ono, and K. Segawa, “Evolution of the Hall Coefficient and the Peculiar Electronic Structure of the Cuprate Superconductors,” Phys. Rev. Lett. 92, 197001 (2004)
work page 2004
-
[16]
Change of carrier density at the pseudogap critical point of a cuprate superconductor,
S. Badoux, W. Tabis, F. Lalibert´ e, G. Grissonnanche, B. Vignolle, D. Vignolles, J. B´ eard, D. A. Bonn, W. N. Hardy, R. Liang, N. Doiron-Leyraud, L. Taillefer, and C. Proust, “Change of carrier density at the pseudogap critical point of a cuprate superconductor,” Nature531, 210–214 (2016)
work page 2016
-
[17]
C. Collignon, S. Badoux, S. A. A. Afshar, B. Mi- chon, F. Lalibert´ e, O. Cyr-Choini` ere, J.-S. Zhou, S. Lic- 15 ciardello, S. Wiedmann, N. Doiron-Leyraud, and L. Taillefer, “Fermi-surface transformation across the pseudogap critical point of the cuprate superconductor la1.6−xnd0.4srxcuo4,” Phys. Rev. B 95, 224517 (2017)
work page 2017
-
[18]
S. I. Mirzaei, D. Stricker, J. N. Hancock, C. Berthod, A. Georges, E. van Heumen, M. K. Chan, X. Zhao, Y. Li, M. Greven, N. Bariˇ si´ c, and D. van der Marel, “Spectroscopic evidence for Fermi liquid-like energy and temperature dependence of the relaxation rate in the pseudogap phase of the cuprates,” Proceedings of the National Academy of Sciences 110, 5...
work page 2013
-
[19]
In-Plane Magnetoresistance Obeys Kohler’s Rule in the Pseudogap Phase of Cuprate Superconductors,
M. K. Chan, M. J. Veit, C. J. Dorow, Y. Ge, Y. Li, W. Tabis, Y. Tang, X. Zhao, N. Bariˇ si´ c, and M. Greven, “In-Plane Magnetoresistance Obeys Kohler’s Rule in the Pseudogap Phase of Cuprate Superconductors,” Phys. Rev. Lett. 113, 177005 (2014)
work page 2014
-
[20]
Fermi Surface and Some Simple Equi- librium Properties of a System of Interacting Fermions,
J. M. Luttinger, “Fermi Surface and Some Simple Equi- librium Properties of a System of Interacting Fermions,” Phys. Rev. 119, 1153–1163 (1960)
work page 1960
-
[21]
Sachdev, Quantum Phases of Matter (Cambridge University Press, Cambridge, 2023)
S. Sachdev, Quantum Phases of Matter (Cambridge University Press, Cambridge, 2023)
work page 2023
-
[22]
Test- ing the itinerancy of spin dynamics in superconducting Bi2Sr2CaCu2O8+δ,
G. Xu, G. D. Gu, M. H¨ ucker, B. Fauqu´ e, T. G. Per- ring, L. P. Regnault, and J. M. Tranquada, “Test- ing the itinerancy of spin dynamics in superconducting Bi2Sr2CaCu2O8+δ,” Nature Physics5, 642–646 (2009)
work page 2009
-
[23]
In- tense paramagnon excitations in a large family of high- temperature superconductors,
M. Le Tacon, G. Ghiringhelli, J. Chaloupka, M. M. Sala, V. Hinkov, M. W. Haverkort, M. Minola, M. Bakr, K. J. Zhou, S. Blanco-Canosa, C. Monney, Y. T. Song, G. L. Sun, C. T. Lin, G. M. De Luca, M. Salluzzo, G. Khal- iullin, T. Schmitt, L. Braicovich, and B. Keimer, “In- tense paramagnon excitations in a large family of high- temperature superconductors,” ...
work page 2011
-
[24]
M. P. M. Dean, G. Dellea, R. S. Springell, F. Yakhou- Harris, K. Kummer, N. B. Brookes, X. Liu, Y.-J. Sun, J. Strle, T. Schmitt, L. Braicovich, G. Ghiringhelli, I. Boˇ zovi´ c, and J. P. Hill, “Persistence of magnetic ex- citations in La2-xSrxCuO4 from the undoped insulator to the heavily overdoped non-superconducting metal,” Nature Materials 12, 1019–1023 (2013)
work page 2013
-
[25]
Anisotropic softening of magnetic excitations along the nodal direction in superconducting cuprates,
M. Guarise, B. D. Piazza, H. Berger, E. Giannini, T. Schmitt, H. M. Rønnow, G. A. Sawatzky, J. van den Brink, D. Altenfeld, I. Eremin, and M. Grioni, “Anisotropic softening of magnetic excitations along the nodal direction in superconducting cuprates,” Nature Communications 5, 5760 (2014)
work page 2014
-
[26]
Stripe phases in high-temperature superconductors,
V. J. Emery, S. A. Kivelson, and J. M. Tranquada, “Stripe phases in high-temperature superconductors,” Proceedings of the National Academy of Sciences 96, 8814–8817 (1999)
work page 1999
-
[27]
How to detect fluctuating stripes in the high-temperature su- perconductors,
S. A. Kivelson, I. P. Bindloss, E. Fradkin, V. Oganesyan, J. M. Tranquada, A. Kapitulnik, and C. Howald, “How to detect fluctuating stripes in the high-temperature su- perconductors,” Rev. Mod. Phys. 75, 1201–1241 (2003)
work page 2003
-
[28]
Lattice symmetry breaking in cuprate super- conductors: stripes, nematics, and superconductivity,
M. Vojta, “Lattice symmetry breaking in cuprate super- conductors: stripes, nematics, and superconductivity,” Advances in Physics 58, 699–820 (2009)
work page 2009
-
[29]
Evidence for stripe correlations of spins and holes in copper oxide superconductors,
J. M. Tranquada, B. J. Sternlieb, J. D. Axe, Y. Naka- mura, and S. Uchida, “Evidence for stripe correlations of spins and holes in copper oxide superconductors,” Nature 375, 561–563 (1995)
work page 1995
-
[30]
Neutron-scattering study of stripe-phase order of holes and spins in La1.48Nd0.4Sr0.12CuO4,
J. M. Tranquada, J. D. Axe, N. Ichikawa, Y. Naka- mura, S. Uchida, and B. Nachumi, “Neutron-scattering study of stripe-phase order of holes and spins in La1.48Nd0.4Sr0.12CuO4,” Phys. Rev. B 54, 7489–7499 (1996)
work page 1996
-
[31]
Spatially modulated ’Mot- tness’ in La2-xBaxCuO4,
P. Abbamonte, A. Rusydi, S. Smadici, G. D. Gu, G. A. Sawatzky, and D. L. Feng, “Spatially modulated ’Mot- tness’ in La2-xBaxCuO4,” Nature Physics 1, 155–158 (2005)
work page 2005
-
[32]
Periodic density-of-states modulations in superconducting Bi 2Sr2CaCu2O8+δ,
C. Howald, H. Eisaki, N. Kaneko, M. Greven, and A. Kapitulnik, “Periodic density-of-states modulations in superconducting Bi 2Sr2CaCu2O8+δ,” Phys. Rev. B 67, 014533 (2003)
work page 2003
-
[33]
Local Ordering in the Pseudogap State of the High-Tc Superconductor Bi2Sr2CaCu2O8+ δ,
M. Vershinin, S. Misra, S. Ono, Y. Abe, Y. Ando, and A. Yazdani, “Local Ordering in the Pseudogap State of the High-Tc Superconductor Bi2Sr2CaCu2O8+ δ,” Sci- ence 303, 1995–1998 (2004)
work page 1995
-
[34]
Fluctuating stripes at the onset of the pseudogap in the high-Tc superconductor Bi2Sr2CaCu2O8+x,
C. V. Parker, P. Aynajian, E. H. da Silva Neto, A. Pushp, S. Ono, J. Wen, Z. Xu, G. Gu, and A. Yaz- dani, “Fluctuating stripes at the onset of the pseudogap in the high-Tc superconductor Bi2Sr2CaCu2O8+x,” Nature 468, 677–680 (2010)
work page 2010
-
[35]
Magnetic-field-induced charge- stripe order in the high-temperature superconductor YBa2Cu3Oy,
T. Wu, H. Mayaffre, S. Kr¨ amer, M. Horvati´ c, C. Berthier, W. N. Hardy, R. Liang, D. A. Bonn, and M.-H. Julien, “Magnetic-field-induced charge- stripe order in the high-temperature superconductor YBa2Cu3Oy,” Nature 477, 191–194 (2011)
work page 2011
-
[36]
J. Chang, N. B. Christensen, C. Niedermayer, K. Lef- mann, H. M. Rønnow, D. F. McMorrow, A. Schnei- dewind, P. Link, A. Hiess, M. Boehm, R. Mottl, S. Pailh´ es, N. Momono, M. Oda, M. Ido, and J. Mesot, “Magnetic-Field-Induced Soft-Mode Quantum Phase Transition in the High-Temperature Superconductor La1.855Sr0.145CuO4: An Inelastic Neutron-Scattering Study...
work page 2009
-
[37]
Stripes and electronic quasiparticles in the pseudogap state of cuprate superconductors,
M. Vojta, “Stripes and electronic quasiparticles in the pseudogap state of cuprate superconductors,” Physica C: Superconductivity 481, 178–188 (2012)
work page 2012
-
[38]
Hidden magnetism at the pseudogap critical point of a cuprate superconduc- tor,
M. Frachet, I. Vinograd, R. Zhou, S. Benhabib, S. Wu, H. Mayaffre, S. Kr¨ amer, S. K. Ramakrishna, A. P. Reyes, J. Debray, T. Kurosawa, N. Momono, M. Oda, S. Komiya, S. Ono, M. Horio, J. Chang, C. Proust, D. LeBoeuf, and M.-H. Julien, “Hidden magnetism at the pseudogap critical point of a cuprate superconduc- tor,” Nature Physics 16, 1064–1068 (2020)
work page 2020
-
[39]
I. Vinograd, R. Zhou, H. Mayaffre, S. Kr¨ amer, S. K. Ramakrishna, A. P. Reyes, T. Kurosawa, N. Momono, M. Oda, S. Komiya, S. Ono, M. Horio, J. Chang, and M.-H. Julien, “Competition between spin order- ing and superconductivity near the pseudogap boundary in La 2−xSrxCuO4: Insights from NMR,” Phys. Rev. B 106, 054522 (2022)
work page 2022
-
[40]
Spin- stripe order tied to the pseudogap phase in La1.8- xEu0.2SrxCuO4,
A. Missiaen, H. Mayaffre, S. Kr¨ amer, D. Zhao, Y. B. Zhou, T. Wu, X. H. Chen, S. Pyon, T. Takayama, H. Takagi, D. LeBoeuf, and M. H. Julien, “Spin- stripe order tied to the pseudogap phase in La1.8- xEu0.2SrxCuO4,” (2024), arXiv:2411.01907
-
[41]
Origin and fate of the pseudogap in the doped Hubbard model,
F. ˇSimkovic, R. Rossi, A. Georges, and M. Ferrero, “Origin and fate of the pseudogap in the doped Hubbard model,” Science 385 (2024)
work page 2024
-
[42]
H. Xu, H. Shi, E. Vitali, M. Qin, and S. Zhang, “Stripes and spin-density waves in the doped two-dimensional Hubbard model: Ground state phase diagram,” Phys. Rev. Res. 4, 013239 (2022)
work page 2022
-
[43]
Antiphase stripe order as the origin of electron pockets observed in 1/8-hole- doped cuprates,
A. J. Millis and M. R. Norman, “Antiphase stripe order as the origin of electron pockets observed in 1/8-hole- doped cuprates,” Phys. Rev. B 76, 220503 (2007). 16
work page 2007
-
[44]
I. Dimov, P. Goswami, X. Jia, and S. Chakravarty, “Competing order, Fermi surface reconstruction, and quantum oscillations in underdoped high-temperature superconductors,” Phys. Rev. B 78, 134529 (2008)
work page 2008
-
[45]
Lifshitz transi- tion in underdoped cuprates,
M. R. Norman, J. Lin, and A. J. Millis, “Lifshitz transi- tion in underdoped cuprates,” Phys. Rev. B 81, 180513 (2010)
work page 2010
-
[46]
Fermi-surface re- construction in a smectic phase of a high-temperature superconductor,
H. Yao, D.-H. Lee, and S. Kivelson, “Fermi-surface re- construction in a smectic phase of a high-temperature superconductor,” Phys. Rev. B 84, 012507 (2011)
work page 2011
-
[47]
Singular Quasiparticle Scattering in the Proximity of Charge In- stabilities,
C. Castellani, C. Di Castro, and M. Grilli, “Singular Quasiparticle Scattering in the Proximity of Charge In- stabilities,” Phys. Rev. Lett. 75, 4650–4653 (1995)
work page 1995
-
[48]
Elec- tronic liquid-crystal phases of a doped Mott insulator,
S. A. Kivelson, E. Fradkin, and V. J. Emery, “Elec- tronic liquid-crystal phases of a doped Mott insulator,” Nature 393, 550–553 (1998)
work page 1998
-
[49]
Quantum dimer model for the pseudogap metal,
M. Punk, A. Allais, and S. Sachdev, “Quantum dimer model for the pseudogap metal,” Proceedings of the Na- tional Academy of Sciences 112 (2015)
work page 2015
-
[50]
Nernst effect in high- Tc superconductors,
Y. Wang, L. Li, and N. P. Ong, “Nernst effect in high- Tc superconductors,” Phys. Rev. B 73, 024510 (2006)
work page 2006
-
[51]
Emergence of preformed Cooper pairs from the doped Mott insulating state in Bi2Sr2CaCu2O8+δ,
H. B. Yang, J. D. Rameau, P. D. Johnson, T. Valla, A. Tsvelik, and G. D. Gu, “Emergence of preformed Cooper pairs from the doped Mott insulating state in Bi2Sr2CaCu2O8+δ,” Nature 456, 77–80 (2008)
work page 2008
-
[52]
A. Kanigel, U. Chatterjee, M. Randeria, M. R. Norman, G. Koren, K. Kadowaki, and J. C. Campuzano, “Evi- dence for Pairing above the Transition Temperature of Cuprate Superconductors from the Electronic Disper- sion in the Pseudogap Phase,” Phys. Rev. Lett. 101, 137002 (2008)
work page 2008
-
[53]
Equivalence of pseudogap and pairing energy in a cuprate high-temperature superconductor,
J. Niu, M. O. Larrazabal, T. Gozlinski, Y. Sato, K. M. Bastiaans, T. Benschop, J.-F. Ge, Y. M. Blanter, G. Gu, I. Swart, et al. , “Equivalence of pseudogap and pairing energy in a cuprate high-temperature superconductor,” arXiv:2409.15928 (2024)
-
[54]
Universality of pseudogap and emergent order in lightly doped Mott insulators,
I. Battisti, K. M. Bastiaans, V. Fedoseev, A. de la Torre, N. Iliopoulos, A. Tamai, E. C. Hunter, R. S. Perry, J. Za- anen, F. Baumberger, and M. P. Allan, “Universality of pseudogap and emergent order in lightly doped Mott insulators,” Nature Physics 13, 21–25 (2017)
work page 2017
-
[55]
Carrier den- sity crossover and quasiparticle mass enhancement in a doped 5d Mott insulator,
Y.-T. Hsu, A. Rydh, M. Berben, C. Duffy, A. de la Torre, R. S. Perry, and N. E. Hussey, “Carrier den- sity crossover and quasiparticle mass enhancement in a doped 5d Mott insulator,” Nature Physics (2024), 10.1038/s41567-024-02564-3
-
[56]
Density-wave instabil- ities of fractionalized Fermi liquids,
D. Chowdhury and S. Sachdev, “Density-wave instabil- ities of fractionalized Fermi liquids,” Phys. Rev. B 90, 245136 (2014)
work page 2014
-
[57]
T. Senthil, S. Sachdev, and M. Vojta, “Fractionalized fermi liquids,” Phys. Rev. Lett. 90, 216403 (2003)
work page 2003
-
[58]
Large-N expansion for frus- trated quantum antiferromagnets,
N. Read and S. Sachdev, “Large-N expansion for frus- trated quantum antiferromagnets,” Phys. Rev. Lett.66, 1773–1776 (1991)
work page 1991
-
[59]
Mean-field theory of spin-liquid states with finite energy gap and topological orders,
X. G. Wen, “Mean-field theory of spin-liquid states with finite energy gap and topological orders,” Phys. Rev. B 44, 2664–2672 (1991)
work page 1991
-
[60]
Hole dynamics in an antiferromagnet across a deconfined quantum critical point,
R. K. Kaul, A. Kolezhuk, M. Levin, S. Sachdev, and T. Senthil, “Hole dynamics in an antiferromagnet across a deconfined quantum critical point,” Phys. Rev. B 75, 235122 (2007)
work page 2007
-
[61]
Effective theory of Fermi pock- ets in fluctuating antiferromagnets,
Y. Qi and S. Sachdev, “Effective theory of Fermi pock- ets in fluctuating antiferromagnets,” Phys. Rev. B 81, 115129 (2010)
work page 2010
-
[62]
Underdoped cuprates as fractionalized Fermi liquids: Transition to superconduc- tivity,
E. G. Moon and S. Sachdev, “Underdoped cuprates as fractionalized Fermi liquids: Transition to superconduc- tivity,” Phys. Rev. B 83, 224508 (2011)
work page 2011
-
[63]
Luttinger-volume violating fermi liquid in the pseudogap phase of the cuprate superconductors,
J.-W. Mei, S. Kawasaki, G.-Q. Zheng, Z.-Y. Weng, and X.-G. Wen, “Luttinger-volume violating fermi liquid in the pseudogap phase of the cuprate superconductors,” Phys. Rev. B 85, 134519 (2012)
work page 2012
-
[64]
M. Punk and S. Sachdev, “Fermi surface reconstruction in hole-doped t − J models without long-range antifer- romagnetic order,” Phys. Rev. B 85, 195123 (2012)
work page 2012
-
[65]
The novel metallic states of the cuprates: Topological Fermi liquids and strange metals,
S. Sachdev and D. Chowdhury, “The novel metallic states of the cuprates: Topological Fermi liquids and strange metals,” Progress of Theoretical and Experi- mental Physics 2016, 12C102 (2016)
work page 2016
-
[66]
Superexchange mechanism and d-wave superconductivity,
G. Kotliar and J. Liu, “Superexchange mechanism and d-wave superconductivity,” Phys. Rev. B38, 5142–5145 (1988)
work page 1988
-
[67]
Topological Approach to Luttinger’s Theorem and the Fermi Surface of a Kondo Lattice,
M. Oshikawa, “Topological Approach to Luttinger’s Theorem and the Fermi Surface of a Kondo Lattice,” Phys. Rev. Lett. 84, 3370–3373 (2000)
work page 2000
-
[68]
Z2-slave-spin theory for strongly correlated fermions,
A. R¨ uegg, S. D. Huber, and M. Sigrist, “ Z2-slave-spin theory for strongly correlated fermions,” Phys. Rev. B 81, 155118 (2010)
work page 2010
-
[69]
Orthogonal metals: The simplest non-Fermi liquids,
R. Nandkishore, M. A. Metlitski, and T. Senthil, “Orthogonal metals: The simplest non-Fermi liquids,” Phys. Rev. B 86, 045128 (2012)
work page 2012
-
[70]
Fermi Surface Reconstruction without Symmetry Breaking,
S. Gazit, F. F. Assaad, and S. Sachdev, “Fermi Surface Reconstruction without Symmetry Breaking,” Phys. Rev. X 10, 041057 (2020)
work page 2020
-
[71]
The geometric order of stripes and Luttinger liquids,
J. Zaanen, O. Y. Osman, H. V. Kruis, Z. Nussinov, and J. Tworzydlo, “The geometric order of stripes and Luttinger liquids,” Philosophical Magazine B 81, 1485– 1531 (2001)
work page 2001
-
[72]
Many-body physics with ultracold gases,
I. Bloch, J. Dalibard, and W. Zwerger, “Many-body physics with ultracold gases,” Rev. Mod. Phys.80, 885– 964 (2008)
work page 2008
-
[73]
Fermi-Hubbard Physics with Atoms in an Optical Lattice,
T. Esslinger, “Fermi-Hubbard Physics with Atoms in an Optical Lattice,” Annual Review of Condensed Matter Physics 1, 129–152 (2010)
work page 2010
-
[74]
Quan- tum simulations with ultracold quantum gases,
I. Bloch, J. Dalibard, and S. Nascimb` ene, “Quan- tum simulations with ultracold quantum gases,” Nature Physics 8, 267–276 (2012)
work page 2012
-
[75]
Site-Resolved Imaging of Fermionic 6Li in an Optical Lattice,
M. F. Parsons, F. Huber, A. Mazurenko, C. S. Chiu, W. Setiawan, K. Wooley-Brown, S. Blatt, and M. Greiner, “Site-Resolved Imaging of Fermionic 6Li in an Optical Lattice,” Phys. Rev. Lett. 114, 213002 (2015)
work page 2015
-
[76]
Quantum-Gas Microscope for Fermionic Atoms,
L. W. Cheuk, M. A. Nichols, M. Okan, T. Gersdorf, V. V. Ramasesh, W. S. Bakr, T. Lompe, and M. W. Zwierlein, “Quantum-Gas Microscope for Fermionic Atoms,” Phys. Rev. Lett. 114, 193001 (2015)
work page 2015
-
[77]
Single-atom imaging of fermions in a quantum-gas microscope,
E. Haller, J. Hudson, A. Kelly, D. A. Cotta, B. Peaude- cerf, G. D. Bruce, and S. Kuhr, “Single-atom imaging of fermions in a quantum-gas microscope,” Nature Physics 11, 738–742 (2015)
work page 2015
-
[78]
Quantum simulations with ul- tracold atoms in optical lattices,
C. Gross and I. Bloch, “Quantum simulations with ul- tracold atoms in optical lattices,” Science357, 995–1001 (2017)
work page 2017
-
[79]
Exploration of doped quantum magnets with ultracold atoms,
A. Bohrdt, L. Homeier, C. Reinmoser, E. Demler, and F. Grusdt, “Exploration of doped quantum magnets with ultracold atoms,” Annals of Physics 435, 168651 (2021), special issue on Philip W. Anderson
work page 2021
-
[80]
Short-Range Quantum Magnetism of Ul- 17 tracold Fermions in an Optical Lattice,
D. Greif, T. Uehlinger, G. Jotzu, L. Tarruell, and T. Esslinger, “Short-Range Quantum Magnetism of Ul- 17 tracold Fermions in an Optical Lattice,” Science 340, 1307–1310 (2013)
work page 2013
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