Strain-induced structural change and nearly-commensurate diffuse scattering in the model high-temperature superconductor HgBa₂CuO_(4+δ)
Pith reviewed 2026-05-18 04:54 UTC · model grok-4.3
The pith
Strain along the a-axis in underdoped HgBa2CuO4+δ induces short-range nearly-commensurate two-dimensional charge correlations with wave vector near (0.5, 0, 0).
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
The paper reports that mechanical compression along the crystallographic a direction in HgBa2CuO4+δ produces diffuse X-ray scattering from a previously unobserved two-dimensional charge correlation. The modulation is short-range, nearly commensurate, and centered near the wave vector (0.5, 0, 0), with a correlation length of approximately four unit cells. The intensity and position of this signal remain unchanged when the sample passes through the superconducting transition temperature, indicating that the charge correlations are decoupled from superconductivity in this strain state.
What carries the argument
The strain-induced diffuse scattering interpreted as a new type of two-dimensional charge correlation with wave vector close to (0.5, 0, 0) and correlation length of about four unit cells.
If this is right
- The charge correlations remain unchanged across the superconducting transition, showing they are insensitive to the onset of superconductivity.
- The modulation wave vector lies close to (0.5, 0, 0) and the correlation length is limited to roughly four unit cells.
- The observed pattern matches the charge-order state predicted in the phase diagram of the resonating-valence-bond spin-liquid model on a square lattice.
Where Pith is reading between the lines
- Strain may serve as a clean tuning knob to stabilize charge correlations without simultaneously altering the superconducting state in this cuprate.
- The resemblance to RVB-model predictions suggests that similar short-range modulations could be accessed in other square-lattice models by modest lattice distortions.
- Applying strain in different crystallographic directions could test whether other wave vectors become favored or whether the (0.5, 0, 0) feature is unique to a-axis compression.
Load-bearing premise
The diffuse scattering signal is correctly identified as arising from a new type of two-dimensional charge correlation rather than from structural defects, thermal effects, or instrumental artifacts.
What would settle it
A direct simulation or measurement showing that the observed diffuse intensity and wave-vector position can be fully accounted for by thermal diffuse scattering or known defect scattering without invoking any additional charge modulation.
Figures
read the original abstract
We investigate the strain response of underdoped HgBa$_2$CuO$_{4+\delta}$ (Hg1201), by synchrotron X-ray diffraction and corresponding simulations of thermal diffuse scattering. The compression in the crystallographic $a$ direction leads to relatively small expansion in the $b$ and $c$ directions, with Poisson ratios $\nu_{ba}$=0.16 and $\nu_{ca}$=0.11, respectively. However, the Cu-O distance in the $c$ direction exhibits a notable 0.9% increase at 1.1% $a$-axis compression. We further find strain-induced diffuse scattering which corresponds to a new type of two-dimensional charge correlation. Interestingly, this signal is insensitive to the onset of superconductivity and instead corresponds to a short-range, nearly commensurate modulation with a wave vector close to (0.5, 0, 0) and a correlation length of approximately four unit cells. It closely resembles the charge order theoretically predicted in the phase diagram of the spin-liquid model with resonating valence bonds on a square lattice.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript reports synchrotron X-ray diffraction measurements on underdoped HgBa₂CuO₄₊δ under uniaxial a-axis compression. It quantifies the resulting structural response via Poisson ratios ν_ba = 0.16 and ν_ca = 0.11, notes a 0.9% increase in the c-direction Cu-O distance at 1.1% a-compression, and identifies strain-induced diffuse scattering at wave vectors near (0.5, 0, 0) with a correlation length of ~4 unit cells. This signal is interpreted as a new short-range, nearly commensurate two-dimensional charge correlation that is insensitive to the superconducting transition and resembles theoretical charge order in the resonating-valence-bond spin-liquid model on a square lattice. The interpretation is supported by comparison to thermal diffuse scattering simulations.
Significance. If the attribution of the diffuse intensity holds, the work supplies direct experimental evidence that uniaxial strain can induce tunable, short-range charge correlations in a model cuprate, offering a potential bridge to theoretical phase diagrams of charge order within resonating-valence-bond states. The explicit combination of high-resolution diffraction data with thermal diffuse scattering simulations is a methodological strength that helps separate lattice from electronic contributions and could inform strain-engineering strategies in high-Tc materials.
major comments (1)
- [Diffuse scattering analysis] Diffuse scattering analysis section: The thermal diffuse scattering simulations are performed on the unstrained or average structure. The manuscript reports a 0.9% c-axis expansion together with anisotropic Poisson ratios under 1.1% a-compression; without re-computing the phonon spectrum or diffuse intensity on the measured strained lattice (including possible local strain gradients), the residual intensity at Q ≈ (0.5, 0, 0) cannot be unambiguously assigned to electronic charge correlations rather than modified thermal or defect scattering. This distinction is load-bearing for the central claim of a new two-dimensional charge correlation.
minor comments (2)
- [Abstract] The abstract states that the diffuse signal is 'insensitive to the onset of superconductivity' but does not specify the temperature range or how the comparison was performed; a brief statement in the results would clarify this point.
- [Results] Notation for the wave vector (0.5, 0, 0) should explicitly indicate reciprocal-lattice units and the Brillouin-zone centering to avoid ambiguity with possible incommensurate shifts.
Simulated Author's Rebuttal
We thank the referee for the careful and constructive review of our manuscript. We address the single major comment below, providing clarification on our methodology while acknowledging the value of additional discussion to strengthen the interpretation.
read point-by-point responses
-
Referee: Diffuse scattering analysis section: The thermal diffuse scattering simulations are performed on the unstrained or average structure. The manuscript reports a 0.9% c-axis expansion together with anisotropic Poisson ratios under 1.1% a-compression; without re-computing the phonon spectrum or diffuse intensity on the measured strained lattice (including possible local strain gradients), the residual intensity at Q ≈ (0.5, 0, 0) cannot be unambiguously assigned to electronic charge correlations rather than modified thermal or defect scattering. This distinction is load-bearing for the central claim of a new two-dimensional charge correlation.
Authors: We appreciate this observation. Our thermal diffuse scattering simulations incorporated the lattice parameters of the strained crystal as refined from the measured Bragg reflections under applied compression, including the reported 0.9% c-axis expansion and the anisotropic Poisson ratios. However, we did not perform a full recalculation of the phonon dispersion on the strained lattice or explicitly model possible local strain gradients. Given the modest strain magnitude (1.1%), we anticipate only small modifications to the phonon spectrum, and the simulated TDS intensity remains concentrated near integer Bragg positions with a three-dimensional character, in contrast to the observed short-range, nearly-commensurate two-dimensional signal. To address the referee's concern directly, we will revise the manuscript to include a quantitative estimate of the expected TDS intensity variation under the measured strain (using the elastic constants and Poisson ratios) and a brief discussion ruling out local gradients as the origin of the diffuse feature. This addition will reinforce the assignment to electronic charge correlations without altering the central conclusions. revision: yes
Circularity Check
No circularity: results are direct experimental observations and comparisons
full rationale
The paper reports synchrotron X-ray diffraction measurements under uniaxial compression, extracted Poisson ratios from observed lattice expansions, and diffuse scattering signals compared against thermal diffuse scattering simulations. These steps rely on raw diffraction data and standard simulation protocols applied to the measured average structure; no parameter is fitted to a subset and then relabeled as a prediction, no central claim reduces to a self-citation chain, and no ansatz or uniqueness theorem is imported to force the interpretation. The resemblance to a spin-liquid model is presented as a qualitative similarity rather than a derived equivalence. The derivation chain is therefore self-contained against external benchmarks.
Axiom & Free-Parameter Ledger
axioms (2)
- standard math Poisson ratios are defined as the negative ratio of transverse strain to axial strain under uniaxial compression.
- domain assumption Diffuse scattering can be simulated from thermal vibrations to distinguish charge-correlation signals from background.
Lean theorems connected to this paper
-
IndisputableMonolith/Foundation/AlexanderDuality.leanalexander_duality_circle_linking unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
strain-induced diffuse scattering … wave vector close to (0.5, 0, 0) and a correlation length of approximately four unit cells. It closely resembles the charge order theoretically predicted in the phase diagram of the spin-liquid model with resonating valence bonds on a square lattice.
-
IndisputableMonolith/Cost/FunctionalEquation.leanwashburn_uniqueness_aczel unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
simulations of the diffuse scattering induced by the thermal population of phonons … dynamical matrices … PBESOL … 4×4×2 momentum grid
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]
F. Hardy, N. J. Hillier, C. Meingast, D. Colson, Y. Li, N. Barišić, G. Yu, X. Zhao, M. Greven, and J. S. Schilling, Enhancement of the Critical Temperature of HgBa2CuO4+δ by Applying Uniaxial and Hydrostatic Pressure: Implications for a Universal Trend in Cuprate Superconductors, Phys. Rev. Lett.105, 167002 (2010)
work page 2010
-
[2]
C. W. Hicks, D. O. Brodsky, E. A. Yelland, A. S. Gibbs, J.A.N.Bruin, M.E.Barber, S.D.Edkins, K.Nishimura, S. Yonezawa, Y. Maeno, and A. P. Mackenzie, Strong In- crease ofT c of Sr2RuO4 Under Both Tensile and Com- pressive Strain, Science344, 283 (2014)
work page 2014
-
[3]
A. Steppke, L. Zhao, M. E. Barber, T. Scaffidi, F. Jerzembeck, H. Rosner, A. S. Gibbs, Y. Maeno, S. H. Simon, A. P. Mackenzie, and C. W. Hicks, Strong peak inT c of Sr2RuO4 under uniaxial pressure, Science355, 148 (2017)
work page 2017
-
[4]
M. Mito, K. Ogata, H. Goto, K. Tsuruta, K. Nakamura, H.Deguchi, T.Horide, K.Matsumoto, T.Tajiri, H.Hara, T. Ozaki, H. Takeya, and Y. Takano, Uniaxial strain ef- fects on the superconducting transition in re-doped hg- 1223 cuprate superconductors, Phys. Rev. B95, 064503 (2017)
work page 2017
-
[5]
H.-H. Kim, S. M. Souliou, M. E. Barber, E. Lefrançois, M. Minola, M. Tortora, R. Heid, N. Nandi, R. A. Borzi, G. Garbarino, A. Bosak, J. Porras, T. Loew, M. König, P. J. W. Moll, A. P. Mackenzie, B. Keimer, C. W. Hicks, and M. L. Tacon, Uniaxial pressure control of compet- ing orders in a high-temperature superconductor, Science 362, 1040 (2018)
work page 2018
-
[6]
H.-H. Kim, E. Lefrançois, K. Kummer, R. Fumagalli, N. B. Brookes, D. Betto, S. Nakata, M. Tortora, J. Por- ras, T. Loew, M. E. Barber, L. Braicovich, A. P. Mackenzie, C. W. Hicks, B. Keimer, M. Minola, and M. Le Tacon, Charge Density Waves inYBa2Cu3O6.67 Probed by Resonant X-Ray Scattering under Uniaxial Compression, Phys. Rev. Lett.126, 037002 (2021)
work page 2021
-
[7]
M. E. Barber, H.-h. Kim, T. Loew, M. Le Tacon, M. Mi- nola, M. Konczykowski, B. Keimer, A. P. Mackenzie, and C. W. Hicks, Dependence ofTc ofYBa 2Cu3O6.67 on in- plane uniaxial stress, Phys. Rev. B106, 184516 (2022)
work page 2022
-
[8]
T. J. Boyle, M. Walker, A. Ruiz, E. Schierle, Z. Zhao, F. Boschini, R. Sutarto, T. D. Boyko, W. Moore, N. Tamura, F. He, E. Weschke, A. Gozar, W. Peng, A. C. Komarek, A. Damascelli, C. Schüßler-Langeheine, A. Frano, E. H. da Silva Neto, and S. Blanco-Canosa, Large response of charge stripes to uniaxial stress in La1.475Nd0.4Sr0.125CuO4, Phys. Rev. Res.3, ...
work page 2021
- [9]
-
[10]
H.-H. Kim, K. Ueda, S. Nakata, P. Wochner, A. Macken- zie, C. Hicks, G. Khaliullin, H. Liu, B. Keimer, and M. Minola, Giant stress response of terahertz magnons in a spin-orbit mott insulator, Nature Communications 13, 6674 (2022)
work page 2022
-
[11]
I. Vinograd, S. M. Souliou, A. A. Haghighirad, T. Lac- mann, Y. Caplan, M. Frachet, M. Merz, G. Garbarino, Y. Liu, S. Nakata, K. Ishida, H. M. L. Noad, M. Minola, B. Keimer, D. Orgad, C. W. Hicks, and M. Le Tacon, Using strain to uncover the interplay between two- and three-dimensional charge density waves in high- temperature superconducting YBa2Cu3Oy, N...
work page 2024
-
[12]
C. Lin, A. Consiglio, O. K. Forslund, J. Küspert, M. M. Denner, H. Lei, A. Louat, M. D. Watson, T. K. Kim, C.Cacho, D.Carbone, M.Leandersson, C.Polley, T.Bal- asubramanian, D. D. Sante, R. Thomale, Z. Guguchia, G. Sangiovanni, T. Neupert, and J. Chang, Uniaxial strain tuning of charge modulation and singularity in a kagome superconductor, Nature Communica...
work page 2024
-
[13]
J. Küspert, I. Biało, R. Frison, A. Morawietz, L. Mar- tinelli, J. Choi, D. Bucher, O. Ivashko, M. v Zimmer- mann, N. B. Christensen, D. G. Mazzone, G. Simutis, A. A. Turrini, L. Thomarat, D. W. Tam, M. Janoschek, T. Kurosawa, N. Momono, M. Oda, Q. Wang, and J. Chang, Engineering phase competition between stripe order and superconductivity in La1.88Sr0.12...
work page 2024
-
[14]
T.Wu, H.Mayaffre, S.Krämer, M.Horvatić, 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, Nature477, 191 (2011)
work page 2011
-
[15]
S. Gerber, H. Jang, H. Nojiri, S. Matsuzawa, H. Ya- sumura, D. A. Bonn, R. Liang, W. N. Hardy, Z. Islam, A. Mehta, S. Song, M. Sikorski, D. Stefanescu, Y. Feng, S. A. Kivelson, T. P. Devereaux, Z.-X. Shen, C.-C. Kao, W.-S. Lee, D. Zhu, and J.-S. Lee, Three-dimensional charge density wave order in YBa2Cu3O6.67 at high mag- netic fields, Science350, 949 (2015)
work page 2015
-
[16]
Y. Caplan and D. Orgad, Dimensional crossover of charge-density wave correlations in the cuprates, Phys. Rev. Lett.119, 107002 (2017)
work page 2017
-
[17]
N. Barišić, Y. Li, X. Zhao, Y.-C. Cho, G. Chabot- Couture, G. Yu, and M. Greven, Demonstrating the model nature of the high-temperature superconductor HgBa2CuO4+δ, Phys. Rev. B78, 054518 (2008)
work page 2008
-
[18]
W. Tabis, B. Yu, I. Bialo, M. Bluschke, T. Kolodziej, A. Kozlowski, E. Blackburn, K. Sen, E. M. Forgan, M. v. Zimmermann, Y. Tang, E. Weschke, B. Vig- nolle, M. Hepting, H. Gretarsson, R. Sutarto, F. He, M. Le Tacon, N. Barišić, G. Yu, and M. Greven, Syn- chrotron x-ray scattering study of charge-density-wave order inHgBa2CuO4+δ, Phys. Rev. B96, 134510 (2017)
work page 2017
-
[19]
B. Yu, W. Tabis, I. Bialo, F. Yakhou, N. B. Brookes, Z. Anderson, Y. Tang, G. Yu, and M. Greven, Un- usualDynamicChargeCorrelationsinSimple-Tetragonal HgBa2CuO4+δ, Physical Review X10, 021059 (2020)
work page 2020
-
[20]
H. Murayama, Y. Sato, R. Kurihara, S. Kasahara, Y. Mizukami, Y. Kasahara, H. Uchiyama, A. Ya- mamoto, E. G. Moon, J. Cai, J. Freyermuth, M. Greven, T. Shibauchi, and Y. Matsuda, Diagonal nematicity in the pseudogap phase of HgBa2CuO4+δ, Nature Commu- nications10, 3282 (2019)
work page 2019
-
[21]
X. Zhao, G. Yu, Y.-C. Cho, G. Chabot-Couture, N. Bar- išić, P. Bourges, N. Kaneko, Y. Li, L. Lu, E. M. Mo- toyama, O. P. Vajk, and M. Greven, Crystal Growth and Characterization of the Model High-Temperature Super- conductor HgBa2CuO4+δ, Advanced Materials18, 3243 8 (2006)
work page 2006
-
[22]
M. Ye, T. Lacmann, M. Frachet, I. Vinograd, G. Gar- barino, and A.-A. Haghighirad, Stress-induced structural changes and diffuse scattering in high-temperature su- perconductor hbco (version 1) [dataset], 10.15151/ESRF- DC-1511962937(2024),EuropeanSynchrotronRadiation Facility
-
[23]
G. M. Sheldrick, Crystal structure refinement with SHELXL, Acta Cryst. C71, 3 (2015)
work page 2015
-
[24]
V. Petříček, M. Dušek, and L. Palatinus, Crystallo- graphic computing system jana2006: General features, Z. Kristallogr.229, 345 (2014)
work page 2014
-
[25]
The Supplemental Material contains representative re- finements of the synchrotron x-ray diffraction data
-
[26]
B. Wehinger, A. Bosak, and P. T. Jochym, Soft phonon modes in rutileTiO2, Phys. Rev. B93, 014303 (2016)
work page 2016
- [27]
-
[28]
R. Heid and K. P. Bohnen, Linear response in a density- functionalmixed-basisapproach,Phys.Rev.B60,R3709 (1999)
work page 1999
-
[29]
J. P. Perdew, A. Ruzsinszky, G. I. Csonka, O. A. Vydrov, G. E. Scuseria, L. A. Constantin, X. Zhou, and K. Burke, Restoring the density-gradient expansion for exchange in solids and surfaces, Phys. Rev. Lett.100, 136406 (2008)
work page 2008
-
[30]
G. N. Greaves, A. L. Greer, R. S. Lakes, and T. Rouxel, Poisson’s ratio and modern materials, Nature Materials 10, 823 (2011)
work page 2011
-
[31]
E. Pavarini, I. Dasgupta, T. Saha-Dasgupta, O. Jepsen, and O. K. Andersen, Band-Structure Trend in Hole- Doped Cuprates and Correlation withT max c , Physical Review Letters87, 047003 (2001)
work page 2001
-
[32]
Y.Y.Peng, G.Dellea, M.Minola, M.Conni, A.Amorese, D. Di Castro, G. M. De Luca, K. Kummer, M. Sal- luzzo, X. Sun, X. J. Zhou, G. Balestrino, M. Le Tacon, B. Keimer, L. Braicovich, N. B. Brookes, and G. Ghir- inghelli, Influence of apical oxygen on the extent of in- plane exchange interaction in cuprate superconductors, Nature Physics13, 1201 (2017)
work page 2017
-
[33]
Z. W. Anderson, M. Spaić, N. Biniskos, L. Thompson, B. Yu, J. Zwettler, Y. Liu, F. Ye, G. E. Granroth, M. Krogstad, R. Osborn, D. Pelc, and M. Greven, Nanoscale structural correlations in a model cuprate su- perconductor, Phys. Rev. B110, 214519 (2024)
work page 2024
- [34]
-
[35]
M. Izquierdo, S. Megtert, D. Colson, V. Honkimäki, A. Forget, H. Raffy, and R. Comès, One dimensional ordering of doping oxygen in HgBa2CuO4+δ supercon- ductors evidenced by X-ray diffuse scattering, Journal of Physics and Chemistry of Solids72, 545 (2011)
work page 2011
-
[36]
W. Tabis, Y. Li, M. Le Tacon, L. Braicovich, A. Kreyssig, M. Minola, G. Dellea, E. Weschke, M. J. Veit, M. Ra- mazanoglu, A. I. Goldman, T. Schmitt, G. Ghiringhelli, N. Barišić, M. K. Chan, C. J. Dorow, G. Yu, X. Zhao, B. Keimer, and M. Greven, Charge order and its con- nection with fermi-liquid charge transport in a pristine high-tc cuprate, Nature Commu...
work page 2014
-
[37]
L. Wang, B. Yu, R. Jing, X. Luo, J. Zeng, J. Li, I. Bialo, M. Bluschke, Y. Tang, J. Freyermuth, G. Yu, R. Sutarto, F. He, E. Weschke, W. Tabis, M. Greven, and Y. Li, Doping-dependent phonon anomaly and charge-order phenomena in theHgBa2CuO4+δ andHgBa 2CaCu2O6+δ superconductors, Phys. Rev. B101, 220509 (2020)
work page 2020
-
[38]
X. Zhou, M. Cardona, C. Chu, Q. Lin, S. Loureiro, and M. Marezio, Raman study of HgBa2Can−1CunO2n+2+δ (n=1,2,3,4 and 5) superconductors, Physica C: Supercon- ductivity270, 193 (1996)
work page 1996
-
[39]
X. Zhou, M. Cardona, C. W. Chu, Q. M. Lin, S. M. Loureiro, and M. Marezio, Raman spectra of hg-based superconductors: Effect of oxygen defects, Phys. Rev. B 54, 6137 (1996)
work page 1996
-
[40]
W. Hayes and R. Loudon,Scattering of Light by Crystals (John Wiley and Sons, New York, 1978)
work page 1978
-
[41]
I.-S. Yang, H.-S. Shin, H.-G. Lee, S.-J. Jeon, H.-S. Ahn, J. Yu, S. Lee, S.-I. Lee, and N. H. Hur, Micro-raman study of the role of pressure in mercury-based supercon- ductors, Phys. Rev. B51, 644 (1995)
work page 1995
- [42]
-
[43]
S. Wang, J. Zhang, J. Yan, X.-J. Chen, V. Struzhkin, W. Tabis, N. Barišić, M. K. Chan, C. Dorow, X. Zhao, M.Greven, W.L.Mao,andT.Geballe,Strainderivatives ofT c in HgBa2CuO4+δ: The CuO 2 plane alone is not enough, Phys. Rev. B89, 024515 (2014)
work page 2014
-
[44]
R. Comin and A. Damascelli, Resonant x-ray scattering studies of charge order in cuprates, Annual Review of Condensed Matter Physics7, 369 (2016)
work page 2016
-
[45]
Y. Li, V. Balédent, G. Yu, N. Barišić, K. Hradil, R. A. Mole, Y. Sidis, P. Steffens, X. Zhao, P. Bourges, and M. Greven, Hidden magnetic excitation in the pseudo- gap phase of a high-tc superconductor, Nature468, 283 (2010)
work page 2010
-
[46]
G. Yu, Y. Li, E. M. Motoyama, X. Zhao, N. Bar- išić, Y. Cho, P. Bourges, K. Hradil, R. A. Mole, and M. Greven, Magnetic resonance in the model high- temperature superconductor HgBa2CuO4+δ, Phys. Rev. B81, 064518 (2010)
work page 2010
-
[47]
M. K. Chan, Y. Tang, C. J. Dorow, J. Jeong, L. Mangin- Thro, M. J. Veit, Y. Ge, D. L. Abernathy, Y. Sidis, P. Bourges, and M. Greven, Hourglass Dispersion and Resonance of Magnetic Excitations in the Superconduct- ing State of the Single-Layer CuprateHgBa 2CuO4+δ Near Optimal Doping, Phys. Rev. Lett.117, 277002 (2016)
work page 2016
-
[48]
M. K. Chan, C. J. Dorow, L. Mangin-Thro, Y. Tang, Y. Ge, M. J. Veit, G. Yu, X. Zhao, A. D. Christian- son, J. T. Park, Y. Sidis, P. Steffens, D. L. Abernathy, P. Bourges, and M. Greven, Commensurate antiferro- magnetic excitations as a signature of the pseudogap in the tetragonal high-Tc cuprateHgBa 2CuO4+δ, Nature Communications7, 10819 (2016)
work page 2016
-
[49]
Sachdev, Colloquium: Order and quantum phase tran- sitions in the cuprate superconductors, Rev
S. Sachdev, Colloquium: Order and quantum phase tran- sitions in the cuprate superconductors, Rev. Mod. Phys. 75, 913 (2003)
work page 2003
-
[50]
M. Christos, Z.-X. Luo, H. Shackleton, Y.-H. Zhang, M.S. Scheurer,and S.Sachdev, Amodelofd-wavesuper- conductivity, antiferromagnetism, and charge order on the square lattice, Proceedings of the National Academy of Sciences120, e2302701120 (2023)
work page 2023
-
[51]
S. Sachdev, The foot, the fan, and the cuprate phase diagram: Fermi-volume-changing quantum phase transi- 9 tions, Physica C: Superconductivity and its Applications 633, 1354707 (2025)
work page 2025
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.