REVIEW 2 major objections 3 minor 110 references
Non-BCS Pairing by a Singular Dynamical Interaction
T0 review · 2 major / 3 minor · reviewed 2026-06-26 · grok-4.3
Pith's one-line read Singular dynamical interactions produce non-BCS superconductivity with an infinite set of topologically distinct gap solutions.
desk verdict This review organizes how singular dynamical interactions produce infinitely many topological solutions to the T=0 gap equation in the γ-model, but the work is mostly a synthesis of the authors' earlier papers. read the letter →
The pith
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
The reading
What carries the argument
The gamma-model with singular dynamical interaction Gamma(Omega) proportional to 1/|Omega|^gamma, which eliminates energy scale separation and generates multiple solutions to the gap equation.
What would settle it
A numerical solution of the gap equation for the gamma-model that finds only finitely many solutions at T=0, or an experiment on a quantum critical material showing conventional single-gap BCS-like superconductivity without multiple solutions.
Extended reading notes
Core claim
For the gamma-model with dynamical interaction Gamma(Omega) proportional to 1 over absolute value of Omega to the power gamma, the gap equation at T equals zero admits an infinite set of topologically distinct solutions. These solutions vanish one by one when the pairing interaction is made non-singular or massive.
Load-bearing premise
That the electron interaction in real materials near quantum critical points or Mott transitions remains singular down to zero frequency and is faithfully captured by the gamma-model.
Editorial extensions
If this is right
- Superconductivity develops above a certain threshold interaction strength but with an origin distinct from BCS theory.
- The gap equation at zero temperature has infinitely many topologically distinct solutions.
- These solutions disappear successively as the interaction becomes non-singular.
- Pairing competes with non-Fermi liquid behavior in such systems.
Reading between the lines
- Materials near quantum critical points may exhibit multiple distinct superconducting states depending on interaction strength.
- Experimental probes of gap structure in such systems could reveal signatures of these multiple solutions.
- Regularizing the interaction at low frequencies, for example by finite temperature or other cutoffs, would reduce the number of available pairing channels.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript reviews superconductivity in systems with singular dynamical electron-electron interactions, using the universal γ-model with pairing interaction Γ(Ω) ∝ 1/|Ω|^γ. It argues that the singularity destroys the separation of energy scales and invalidates the Cooper logarithm, rendering the BCS framework inapplicable. The central claim is that the T=0 gap equation admits an infinite set of topologically distinct solutions; these solutions disappear successively when the interaction is regularized to become non-singular (massive). The work also addresses the competition with non-Fermi liquid behavior and outlines future directions for systems near QCPs and Mott transitions.
Significance. If the mathematical results on the gap equation hold, the paper identifies a qualitatively distinct pairing mechanism relevant to materials near quantum critical points and localization transitions. The demonstration of an infinite family of topologically distinct solutions constitutes a notable structural result that could generate testable predictions beyond conventional BCS theory. The review synthesizes the underlying physics and gives explicit credit to the model's parameter-free aspects in the singular limit.
major comments (2)
- [§4 (T=0 gap equation)] §4 (T=0 gap equation): the topological classification of the infinite solutions is load-bearing for the central claim, yet the manuscript does not specify the invariant (e.g., winding number or nodal structure) used to establish distinctness; without this, it is unclear whether the solutions are truly topologically inequivalent or merely numerically distinct branches.
- [§3.2 (regularization procedure)] §3.2 (regularization procedure): the statement that solutions 'disappear one by one' when the interaction is made massive relies on a specific cutoff or mass term; the paper should demonstrate that this disappearance is independent of the regularization scheme chosen, as different schemes could alter the counting of solutions.
minor comments (3)
- The abstract contains a grammatical error ('these solution disappear' should read 'these solutions disappear').
- [Introduction] Notation for the interaction strength threshold is introduced without an explicit equation reference in the early sections, making it difficult to track how the threshold is determined from the γ-model.
- [Figure 2] Figure captions for the solution branches should include the specific values of γ used in the plots to allow direct comparison with the analytic claims.
Simulated Author's Rebuttal
We thank the referee for the thorough review and valuable suggestions. We address each major comment below and will revise the manuscript accordingly to strengthen the presentation of our results.
read point-by-point responses
-
Referee: [§4 (T=0 gap equation)] the topological classification of the infinite solutions is load-bearing for the central claim, yet the manuscript does not specify the invariant (e.g., winding number or nodal structure) used to establish distinctness; without this, it is unclear whether the solutions are truly topologically inequivalent or merely numerically distinct branches.
Authors: We agree that an explicit definition of the topological invariant is necessary to substantiate the claim of topologically distinct solutions. The solutions in the γ-model are distinguished by the number of zeros of the gap function on the imaginary axis, which defines a winding number invariant. We will revise §4 to include a clear definition of this invariant and demonstrate its distinct values for each solution. This clarification will be added in the revised version. revision: yes
-
Referee: [§3.2 (regularization procedure)] the statement that solutions 'disappear one by one' when the interaction is made massive relies on a specific cutoff or mass term; the paper should demonstrate that this disappearance is independent of the regularization scheme chosen, as different schemes could alter the counting of solutions.
Authors: The referee correctly notes that robustness to the choice of regularization is important. While our primary results use a mass term, we will include additional analysis in the revised manuscript showing that the successive disappearance of solutions occurs similarly under alternative regularizations, such as frequency cutoffs. This will involve presenting comparative numerical solutions for different schemes to confirm the counting remains the same. revision: yes
Circularity Check
No significant circularity in derivation chain
full rationale
The paper is a review analyzing the γ-model with singular interaction Γ(Ω) ∝ 1/|Ω|^γ and the T=0 gap equation. No load-bearing steps reduce by construction to inputs via self-definition, fitted parameters renamed as predictions, or self-citation chains that substitute for independent derivation. Claims about infinite topologically distinct solutions are presented as outcomes of the model's analysis without the paper's own equations showing equivalence to fitted data or prior self-citations as the sole justification. The work is self-contained as a theoretical exploration with external falsifiability through the model's assumptions.
Assumptions & free parameters
free parameters (1)
- γ
assumptions (1)
- domain assumption The electron-electron interaction remains singular (power-law divergent at zero frequency) and can be approximated by the universal γ-model across the cited physical systems.
Cite this review
Pith. "Pith review of Non-BCS Pairing by a Singular Dynamical Interaction." pith.science (2026). https://pith.science/paper/RHMCMAJA
@misc{pith2026260621731,
author = {Pith},
title = {Pith review of: Non-BCS Pairing by a Singular Dynamical Interaction},
year = {2026},
howpublished = {\url{https://pith.science/paper/RHMCMAJA}},
note = {Machine review of arXiv:2606.21731}
}
abstract
This review examines the theory of superconductivity in systems with {\em singular dynamical} electron-electron interaction and contrasts it with a conventional BCS superconductivity. Examples include metals near a Quantum Critical Point, quantum dots and system near a localization (Mott) transition. We show, that the singular interaction destroys the traditional separation of energy scales, invalidating the significance of Cooper logarithm, and, as the consequence, the whole BCS framework. We explore the universal model with dynamical interaction $\Gamma (\Omega) \propto 1/|\Omega|^\gamma$ (the $\gamma$-model) and analyze the competition/interplay between the tendency towards pairing and towards non-Fermi liquid behavior. We show that superconductivity still develops once the pairing interaction exceeds a certain threshold, but the origin of the pairing is qualitatively different from that in BCS theory. We show that the gap equation at $T=0$ has an infinite set of topologically distinct solutions. These solution disappear one by one once the pairing interaction becomes non-singular (massive). We review the physics underlying these phenomena and outline future directions.
Reference graph
Works this paper leans on
-
[1]
1957.Physical Review108(5):1175–1204
Bardeen J, Cooper LN, Schrieffer JR. 1957.Physical Review108(5):1175–1204
1957
-
[2]
1960.Soviet Physics JETP11:696
Eliashberg GM. 1960.Soviet Physics JETP11:696
1960
-
[3]
1998.Nature394(6688):39– 43
Mathur ND, Grosche FM, Julian SR, Walker IR, Freye DM, et al. 1998.Nature394(6688):39– 43
1998
-
[4]
2010.Annual Review of Condensed Matter Physics1:51–70
Taillefer L. 2010.Annual Review of Condensed Matter Physics1:51–70
2010
-
[5]
2012.Rev
Scalapino DJ. 2012.Rev. Mod. Phys.84(4):1383–1417
2012
-
[6]
2014.Annual Review of Condensed Matter Physics 5:113–135
Shibauchi T, Carrington A, Matsuda Y. 2014.Annual Review of Condensed Matter Physics 5:113–135
2014
-
[7]
2020.Annual Review of Condensed Matter Physics11(Volume 11, 2020):213–229
Greene RL, Mandal PR, Poniatowski NR, Sarkar T. 2020.Annual Review of Condensed Matter Physics11(Volume 11, 2020):213–229
2020
-
[8]
2018.Nature556(7699):43–50
Cao Y, Fatemi V, Fang S, Watanabe K, Taniguchi T, et al. 2018.Nature556(7699):43–50
2018
Show all 110 references
-
[9]
2018.Nature556(7699):80–84
Cao Y, Fatemi V, Demir A, Fang S, Tomarken SL, et al. 2018.Nature556(7699):80–84
2018
-
[10]
2021.Nature Reviews Materials6(3):201–206
Andrei E, Efetov D, Jarillo-Herrero P, MacDonald A, Mak K, et al. 2021.Nature Reviews Materials6(3):201–206
2021
-
[11]
Guo Y, Pack J, Swann J, Holtzman L, Cothrine M, et al. 2024. Superconductivity in twisted bilayer wse2 www.annualreviews.org • Non-BCS Superconductivity 19
2024
-
[12]
2024.Nature
Xia Y, Han Z, Watanabe K, Taniguchi T, Shan J, Mak KF. 2024.Nature
2024
-
[13]
2022.Science375(6582):774–778
Zhou H, Holleis L, Saito Y, Cohen L, Huynh W, et al. 2022.Science375(6582):774–778
2022
-
[14]
2022.arXiv preprint arXiv:2205.05087
Zhang Y, Polski R, Thomson A, Lantagne-Hurtubise ´E, Lewandowski C, et al. 2022.arXiv preprint arXiv:2205.05087
2022
-
[15]
2023.arXiv preprint arXiv:2303.00742
Holleis L, Patterson CL, Zhang Y, Yoo HM, Zhou H, et al. 2023.arXiv preprint arXiv:2303.00742
2023
-
[16]
1976.Physical Review B14(3):1165–1184
Hertz JA. 1976.Physical Review B14(3):1165–1184
1976
-
[17]
1993.Physical Review B48(10):7183–7196
Millis AJ. 1993.Physical Review B48(10):7183–7196
1993
-
[18]
2012.Phys
Bergeron D, Chowdhury D, Punk M, Sachdev S, Tremblay AMS. 2012.Phys. Rev. B 86(15):155123
2012
-
[19]
2013.Phys
Wang Y, Chubukov A. 2013.Phys. Rev. B88(2):024516
2013
-
[20]
2025.Phys
Wang Y, Chubukov AV. 2025.Phys. Rev. B111(21):214514
2025
-
[21]
2015.Phys
Raghu S, Torroba G, Wang H. 2015.Phys. Rev. B92(20):205104
2015
-
[22]
2017.Phys
Wang H, Raghu S, Torroba G. 2017.Phys. Rev. B95(16):165137
2017
-
[23]
2005.Phys
Rohe D, Metzner W. 2005.Phys. Rev. B71(11):115116
2005
-
[24]
2006.Phys
Dell’Anna L, Metzner W. 2006.Phys. Rev. B73(4):045127
2006
-
[25]
2016.Phys
Yamase H, Eberlein A, Metzner W. 2016.Phys. Rev. Lett.116(9):096402
2016
-
[26]
1995.Phys
Castellani C, Di Castro C, Grilli M. 1995.Phys. Rev. Lett.75(25):4650–4653
1995
-
[27]
1996.Phys
Perali A, Castellani C, Di Castro C, Grilli M. 1996.Phys. Rev. B54(22):16216–16225
1996
-
[28]
2001.Phys
Andergassen S, Caprara S, Di Castro C, Grilli M. 2001.Phys. Rev. Lett.87(5):056401
2001
-
[29]
2001.EPL (Europhysics Letters)54(4):488
Abanov A, Chubukov AV, Finkel’stein AM. 2001.EPL (Europhysics Letters)54(4):488
2001
-
[30]
2003.Advances in Physics52(3):119–218
Abanov A, Chubukov AV, Schmalian J. 2003.Advances in Physics52(3):119–218
2003
-
[31]
2008.Phys
Abanov A, Chubukov AV, Norman MR. 2008.Phys. Rev. B78(22):220507
2008
-
[32]
2010.Phys
Metlitski MA, Sachdev S. 2010.Phys. Rev. B82(7):075128
2010
-
[33]
2010.Phys
Metlitski MA, Sachdev S. 2010.Phys. Rev. B82(7):075127
2010
-
[34]
2011.Phys
Hartnoll SA, Hofman DM, Metlitski MA, Sachdev S. 2011.Phys. Rev. B84(12):125115
2011
-
[35]
2015.Phys
Metlitski MA, Mross DF, Sachdev S, Senthil T. 2015.Phys. Rev. B91(11):115111
2015
-
[36]
2018.Annual Review of Condensed Matter Physics9(Volume 9, 2018):227–244
Lee SS. 2018.Annual Review of Condensed Matter Physics9(Volume 9, 2018):227–244
2018
-
[37]
2020.Rev
Varma CM. 2020.Rev. Mod. Phys.92(3):031001
2020
-
[38]
2020.Physical Review B102(2):024524
Abanov A, Chubukov AV. 2020.Physical Review B102(2):024524
2020
-
[39]
2025.Phys
Shi ZD, Goldman H, Dong Z, Senthil T. 2025.Phys. Rev. B111(12):125154
2025
-
[40]
2023.Phys
Wu TC, Lee PA, Foster MS. 2023.Phys. Rev. B108(21):214506
2023
-
[41]
2013.Phys
Chowdhury D, Swingle B, Berg E, Sachdev S. 2013.Phys. Rev. Lett.111(15):157004
2013
-
[42]
2014.Phys
Chowdhury D, Sachdev S. 2014.Phys. Rev. B90(24):245136
2014
-
[43]
2022.Rev
Chowdhury D, Georges A, Parcollet O, Sachdev S. 2022.Rev. Mod. Phys.94(3):035004
2022
-
[44]
2020.Phys
Chowdhury D, Berg E. 2020.Phys. Rev. Res.2(1):013301
2020
-
[45]
2026.Annual Review of Condensed Matter Physics17(1):419–448
Esterlis I, Schmalian J. 2026.Annual Review of Condensed Matter Physics17(1):419–448
2026
-
[46]
2019.Physical Review B100(11):115132
Esterlis I, Schmalian J. 2019.Physical Review B100(11):115132
2019
-
[47]
2020.Annals of Physics:168120
Hauck D, Klug MJ, Esterlis I, Schmalian J. 2020.Annals of Physics:168120
2020
-
[48]
2021.Physical Review B104(12):125120
Classen L, Chubukov A. 2021.Physical Review B104(12):125120
2021
-
[49]
2020.Physical Review Research2(3):033084
Wang Y, Chubukov AV. 2020.Physical Review Research2(3):033084
2020
-
[50]
2020.Physical review letters124(1):017002
Wang Y. 2020.Physical review letters124(1):017002
2020
-
[51]
2021.Phys
Kim J, Altman E, Cao X. 2021.Phys. Rev. B103(8):L081113
2021
-
[52]
2026.Phys
Stangier VC, Scheurer MS, Sheehy DE, Schmalian J. 2026.Phys. Rev. Lett.136(17):176501
2026
-
[53]
2026.Phys
Stangier VC, Sheehy DE, Schmalian J. 2026.Phys. Rev. B113(8):085119
2026
-
[54]
1996.Rev
Georges A, Kotliar G, Krauth W, Rozenberg MJ. 1996.Rev. Mod. Phys.68(1):13–125
1996
-
[55]
2019.Phys
Simard O, H´ ebert CD, Foley A, S´ en´ echal D, Tremblay AMS. 2019.Phys. Rev. B100(9):094506
2019
-
[56]
2009.Rev
Capone M, Fabrizio M, Castellani C, Tosatti E. 2009.Rev. Mod. Phys.81(2):943–958
2009
-
[57]
2023.Phys
Chatzieleftheriou M, Kowalski A, Berovi´ c M, Amaricci A, Capone M, et al. 2023.Phys. Rev. Lett.130(6):066401
2023
-
[58]
2026.Communications Physics 20 Abanov•Chubukov 9(1):179
Malcolms MO, Menke H, Tseng YT, Jacob E, Held K, et al. 2026.Communications Physics 20 Abanov•Chubukov 9(1):179
2026
-
[59]
2022.Annual Review of Condensed Matter Physics 13(Volume 13, 2022):239–274
Arovas DP, Berg E, Kivelson SA, Raghu S. 2022.Annual Review of Condensed Matter Physics 13(Volume 13, 2022):239–274
2022
-
[60]
Abrikosov AA, Gorkov LP, Dzyaloshinski IE. 1965. Methods of quantum feld theory in statis- tical physics. Pergamon Oxford
1965
-
[61]
Ramshaw BJ, Kivelson SA. 2026. Superconductivity in overdoped cuprates can be understood from a bcs perspective!
2026
-
[62]
2020.Phys
Wu YM, Abanov A, Chubukov AV. 2020.Phys. Rev. B102(9):094516
2020
-
[63]
2021.Physical Review B103(2):024522
Wu YM, Zhang SS, Abanov A, Chubukov AV. 2021.Physical Review B103(2):024522
2021
-
[64]
2021.Phys
Wu YM, Zhang SS, Abanov A, Chubukov AV. 2021.Phys. Rev. B103(18):184508
2021
-
[65]
2021.Phys
Zhang SS, Wu YM, Abanov A, Chubukov AV. 2021.Phys. Rev. B104(14):144509
2021
-
[66]
Yu Y, Chubukov AV. 2026. Topologically non-trivial gap function and topology-induced time- reversal symmetry breaking in a superconductor with singular dynamical interaction
2026
-
[67]
1958.Soviet Physics JETP7:996
Migdal AB. 1958.Soviet Physics JETP7:996
1958
-
[68]
2003.Phys
Haslinger R, Chubukov AV. 2003.Phys. Rev. B68(21):214508
2003
-
[69]
2026.Annual Review of Condensed Matter Physics17(Volume 17, 2026):419–448
Esterlis I, Schmalian J. 2026.Annual Review of Condensed Matter Physics17(Volume 17, 2026):419–448
2026
-
[70]
1999.Phys
Son DT. 1999.Phys. Rev. D59(9):094019
1999
-
[71]
2005.Phys
Chubukov AV, Schmalian J. 2005.Phys. Rev. B72(17):174520
2005
-
[72]
2010.Phys
Mross DF, McGreevy J, Liu H, Senthil T. 2010.Phys. Rev. B82(4):045121
2010
-
[73]
2015.Phys
Fitzpatrick AL, Kachru S, Kaplan J, Raghu S, Torroba G, Wang H. 2015.Phys. Rev. B 92(4):045118
2015
-
[74]
2009.Journal of Physics: Condensed Matter21(7):075303
Khveshchenko DV. 2009.Journal of Physics: Condensed Matter21(7):075303
2009
-
[75]
1995.Phys
Altshuler BL, Ioffe LB, Millis AJ. 1995.Phys. Rev. B52(8):5563–5572
1995
-
[76]
1996.Phys
Bonesteel NE, McDonald IA, Nayak C. 1996.Phys. Rev. Lett.77(14):3009–3012
1996
-
[77]
2015.Phys
Lederer S, Schattner Y, Berg E, Kivelson SA. 2015.Phys. Rev. Lett.114(9):097001
2015
-
[78]
2001.Phys
Wang Z, Mao W, Bedell K. 2001.Phys. Rev. Lett.87(25):257001
2001
-
[79]
2001.Phys
Roussev R, Millis AJ. 2001.Phys. Rev. B63(14):140504
2001
-
[80]
2003.Phys
Chubukov AV, Finkel’stein AM, Haslinger R, Morr DK. 2003.Phys. Rev. Lett.90(7):077002
2003
-
[81]
2018.Phys
Klein A, Chubukov A. 2018.Phys. Rev. B98(22):220501
2018
-
[82]
2020.Phys
Klein A, Chubukov AV, Schattner Y, Berg E. 2020.Phys. Rev. X10(3):031053
2020
-
[83]
2022.Phys
Liu Y, Jiang W, Klein A, Wang Y, Sun K, et al. 2022.Phys. Rev. B105(4):L041111
2022
-
[84]
1992.Physical Review B46(9):5621–5639
Lee PA, Nagaosa N. 1992.Physical Review B46(9):5621–5639
1992
-
[85]
2007.Phys
Haule K, Kotliar G. 2007.Phys. Rev. B76(10):104509
2007
-
[86]
1995.Phys
Combescot R. 1995.Phys. Rev. B51(17):11625–11634
1995
-
[87]
Bergmann G, Rainer D. 1973.Z. Physik263:59–68
1973
-
[88]
1991.Nature349:396 EP –
Allen PB, Rainer D. 1991.Nature349:396 EP –
1991
-
[89]
1975.Phys
Allen PB, Dynes RC. 1975.Phys. Rev. B12(3):905–922
1975
-
[90]
1988.Phys
Marsiglio F, Schossmann M, Carbotte JP. 1988.Phys. Rev. B37(10):4965–4969
1988
-
[91]
Electron-Phonon Superconductivity
Marsiglio F, Carbotte JP. 1991.Phys. Rev. B43(7):5355–5363. For more recent results see F. Marsiglio and J.P. Carbotte, “Electron-Phonon Superconductivity”, in “The Physics of Con- ventional and Unconventional Superconductors”, Bennemann and Ketterson eds., Springer- Verlag, (...
1991
-
[92]
1991.Solid State Communications79(4):329 – 335
Karakozov A, Maksimov E, Mikhailovsky A. 1991.Solid State Communications79(4):329 – 335
1991
-
[93]
2009.Phys
Sachdev S, Metlitski MA, Qi Y, Xu C. 2009.Phys. Rev. B80(15):155129
2009
-
[94]
2010.Journal of Low Temperature Physics161(1):263–281
Moon EG, Chubukov A. 2010.Journal of Low Temperature Physics161(1):263–281
2010
-
[95]
1993.Phys
Sachdev S, Ye J. 1993.Phys. Rev. Lett.70(21):3339–3342
1993
-
[96]
2015.Talks at KITP
Kitaev A. 2015.Talks at KITP
2015
-
[97]
2000.Phys
Georges A, Parcollet O, Sachdev S. 2000.Phys. Rev. Lett.85(4):840–843
2000
-
[98]
2010.Phys
Sachdev S. 2010.Phys. Rev. Lett.105(15):151602 www.annualreviews.org • Non-BCS Superconductivity 21
2010
-
[99]
2018.Journal of High Energy Physics2018(5):183
Kitaev A, Suh SJ. 2018.Journal of High Energy Physics2018(5):183
2018
-
[100]
2025.Phys
Abanov A, Zhang SS, Chubukov AV. 2025.Phys. Rev. B111(7):075157
2025
-
[101]
1972.Soviet Physics Uspekhi14(6):673
Zeldovich YB, Popov VS. 1972.Soviet Physics Uspekhi14(6):673
1972
-
[102]
Aharony O, Cuomo G, Komargodski Z, Mezei M, Raviv-Moshe A. 2023. Phases of wilson lines: Conformality and screening
2023
-
[103]
1988.Phys
Millis AJ, Sachdev S, Varma CM. 1988.Phys. Rev. B37(10):4975–4986
1988
-
[104]
2020.Annals of Physics:168142
Chubukov AV, Abanov A, Wang Y, Wu YM. 2020.Annals of Physics:168142
2020
-
[105]
2012.Phys
Chubukov AV, Maslov DL. 2012.Phys. Rev. B86(15):155136
2012
-
[106]
2016.Physical Review Letters117(15):157001
Wang Y, Abanov A, Altshuler BL, Yuzbashyan EA, Chubukov AV. 2016.Physical Review Letters117(15):157001
2016
-
[107]
2020.Phys
Wu YM, Abanov A, Wang Y, Chubukov AV. 2020.Phys. Rev. B102(2):024525
2020
-
[108]
2020.Annals of Physics417:168142Eliashberg theory at 60: Strong-coupling superconductivity and beyond
Chubukov AV, Abanov A, Wang Y, Wu YM. 2020.Annals of Physics417:168142Eliashberg theory at 60: Strong-coupling superconductivity and beyond
2020
-
[109]
2025.Journal of Statistical Physics192:69
Kiessling MKH, Altshuler BL, Yuzbashyan EA. 2025.Journal of Statistical Physics192:69
2025
-
[110]
Elezaby A, Abanov A. 2025. Superconductivity near a quantum critical point: Bounds on the transition temperature in theγ-model 22 Abanov•Chubukov
2025
Reviewed June 26, 2026 · model on record in the stance chip above.
Discussion (0). Continue with ORCID to comment.