Recognition: no theorem link
Effective Field Theory for Superconducting Phase Transitions
Pith reviewed 2026-05-13 21:18 UTC · model grok-4.3
The pith
An effective field theory via Schwinger-Keldysh formalism for s-wave superconducting phase transitions reproduces Ginzburg-Landau equations when truncated and is validated holographically with complex relaxation.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
Employing the Schwinger-Keldysh formalism, we formulate an effective field theory for s-wave superconducting phase transition, where the dynamical variables consist of electromagnetic gauge field and complex scalar order parameter. Symmetry-constrained effective action allows systematic handling of dissipations and fluctuations. In particular, we explore the physical implications of higher-order terms, including those involving additional dynamical fields as well as higher time derivatives, on the real-time dynamics near the superconducting critical point. When appropriately truncated, the effective field theory reproduces the phenomenological Ginzburg-Landau equations. Upon crossing the crt
What carries the argument
Symmetry-constrained effective action in the Schwinger-Keldysh formalism for the electromagnetic gauge field and complex scalar order parameter, which encodes dissipations, fluctuations and higher-order terms.
If this is right
- Truncation of the effective action at appropriate order recovers the Ginzburg-Landau equations.
- In the low-temperature phase the order-parameter condensate spontaneously breaks electromagnetic gauge symmetry.
- Near the critical point the Higgs mode appears as an overdamped diffusive mode.
- Phase fluctuations of the order parameter are absorbed into the gauge field via the Higgs mechanism.
- Holographic results fix the Wilsonian coefficients and show a complex relaxation parameter that indicates oscillatory dynamics.
Where Pith is reading between the lines
- The same Schwinger-Keldysh construction could be applied to other continuous phase transitions that involve gauge fields and scalar order parameters.
- Time-resolved experiments that detect oscillatory relaxation near criticality in strongly coupled superconductors would provide a direct test of the holographic coefficients.
- Retaining additional higher-derivative terms may generate new predictions for non-equilibrium transport or collective-mode spectra beyond standard Ginzburg-Landau theory.
- The framework offers a route to connect phenomenological effective theories with microscopic holographic models at quantum critical points.
Load-bearing premise
The symmetry-constrained effective action can be truncated at low orders to recover Ginzburg-Landau dynamics while the retained higher-order terms correctly describe essential real-time behavior, and holographic models furnish unbiased values for the Wilsonian coefficients.
What would settle it
A holographic calculation that returns a purely real relaxation parameter instead of a complex one, or a direct measurement showing strictly overdamped rather than oscillatory relaxation near the critical point in a strongly coupled superconductor, would falsify the claimed structure and coefficients.
Figures
read the original abstract
Employing the Schwinger-Keldysh formalism, we formulate an effective field theory for s-wave superconducting phase transition, where the dynamical variables consist of electromagnetic gauge field and complex scalar order parameter. Symmetry-constrained effective action allows systematic handling of dissipations and fluctuations. In particular, we explore the physical implications of higher-order terms, including those involving additional dynamical fields as well as higher time derivatives, on the real-time dynamics near the superconducting critical point. When appropriately truncated, the effective field theory reproduces the phenomenological Ginzburg-Landau equations. Upon crossing the critical temperature into the low-temperature phase, the electromagnetic gauge symmetry undergoes spontaneous breaking induced by the condensate of the order parameter. Collective excitation analysis reveals that the Higgs mode behaves as an overdamped diffusive mode near the critical point, while the phase fluctuation is absorbed into the gauge field via the Higgs mechanism. Via the holographic Schwinger-Keldysh technique, rigorous validation in a holographic superconductor confirms the structure of the effective action and quantifies the Wilsonian coefficients. Holographic results revaeal a complex relaxation parameter that indicates oscillatory dynamics characteristic of strongly coupled systems.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript develops a symmetry-constrained effective field theory for the s-wave superconducting phase transition within the Schwinger-Keldysh formalism. The dynamical fields are the electromagnetic gauge field and a complex scalar order parameter. The action incorporates dissipation and fluctuations, including higher-order terms with additional fields and higher time derivatives. Appropriate truncation recovers the Ginzburg-Landau equations. Below the critical temperature the gauge symmetry is spontaneously broken by the scalar condensate. Collective mode analysis identifies the Higgs mode as an overdamped diffusive mode near criticality, with the phase mode absorbed into the gauge field. Holographic Schwinger-Keldysh calculations are used to validate the EFT structure and fix the Wilsonian coefficients, yielding a complex relaxation parameter that signals oscillatory dynamics in strongly coupled regimes.
Significance. If the higher-derivative coefficients can be shown to preserve stability and causality, the framework would supply a systematic real-time EFT that connects phenomenological Ginzburg-Landau theory to holographic results, particularly useful for quantifying dissipation and fluctuations near the superconducting transition in strongly coupled systems. The explicit use of Schwinger-Keldysh contour and holographic matching to determine coefficients is a constructive feature.
major comments (2)
- [Abstract / EFT construction] Abstract and central EFT construction: the symmetry-constrained Schwinger-Keldysh action retains higher time-derivative terms on the gauge field and scalar. These generically produce fourth-order (or higher) equations of motion whose characteristic equation can admit roots with positive real parts, raising Ostrogradsky instabilities or acausal propagation. The manuscript must derive the linearized equations of motion from the full (untruncated) action, extract the dispersion relations for the collective modes, and demonstrate that all physical poles remain stable and causal, especially for the reported complex relaxation parameter.
- [Holographic validation] Holographic validation section: the matching procedure that quantifies the Wilsonian coefficients is performed after truncation to Ginzburg-Landau form. An explicit check is required that the retained higher-derivative coefficients (before truncation) do not destabilize the real-time dynamics on the Schwinger-Keldysh contour; otherwise the holographic results cannot be taken as independent confirmation of the full EFT.
minor comments (1)
- [Abstract] Abstract contains a typographical error: 'revaeal' should read 'reveal'.
Simulated Author's Rebuttal
We thank the referee for the careful reading and constructive comments on our manuscript. We address each major comment below and will revise the manuscript to incorporate the requested analyses.
read point-by-point responses
-
Referee: [Abstract / EFT construction] Abstract and central EFT construction: the symmetry-constrained Schwinger-Keldysh action retains higher time-derivative terms on the gauge field and scalar. These generically produce fourth-order (or higher) equations of motion whose characteristic equation can admit roots with positive real parts, raising Ostrogradsky instabilities or acausal propagation. The manuscript must derive the linearized equations of motion from the full (untruncated) action, extract the dispersion relations for the collective modes, and demonstrate that all physical poles remain stable and causal, especially for the reported complex relaxation parameter.
Authors: We appreciate the referee highlighting the need to verify stability and causality for the untruncated action. In the revised manuscript we will derive the full linearized equations of motion, including all higher time-derivative terms, compute the associated dispersion relations, and explicitly demonstrate that all physical poles have negative real parts (ensuring stability) while satisfying causality bounds. For the complex relaxation parameter extracted from holography, we will show that it produces damped oscillatory behavior without introducing instabilities inside the EFT regime of validity. revision: yes
-
Referee: [Holographic validation] Holographic validation section: the matching procedure that quantifies the Wilsonian coefficients is performed after truncation to Ginzburg-Landau form. An explicit check is required that the retained higher-derivative coefficients (before truncation) do not destabilize the real-time dynamics on the Schwinger-Keldysh contour; otherwise the holographic results cannot be taken as independent confirmation of the full EFT.
Authors: We agree that the holographic matching must be validated for the complete EFT. In the revision we will perform an explicit stability analysis of the higher-derivative coefficients using the holographic values, confirming that the real-time dynamics on the Schwinger-Keldysh contour remain stable and causal. This will allow the holographic results to serve as independent confirmation of the full effective action. revision: yes
Circularity Check
No circularity: symmetry-constrained EFT independently validated by holography
full rationale
The derivation begins from symmetry principles in the Schwinger-Keldysh formalism to write the effective action for the gauge field and scalar, then truncates to recover Ginzburg-Landau dynamics while retaining higher-order terms. Holographic Schwinger-Keldysh computations are invoked only afterward as an external benchmark to confirm the action structure and fix Wilsonian coefficients; this constitutes independent input rather than a self-referential fit or self-citation chain. No equation reduces to its own inputs by construction, and the reported complex relaxation parameter emerges from the holographic matching rather than being presupposed.
Axiom & Free-Parameter Ledger
free parameters (1)
- Wilsonian coefficients
axioms (1)
- domain assumption Symmetry constraints determine the form of the effective action
Forward citations
Cited by 1 Pith paper
-
Schwinger-Keldysh Path Integral for Gauge theories
A manifestly BRST-invariant Schwinger-Keldysh path integral is derived for non-Abelian gauge theories with generic initial states, enabling perturbative Ward-Takahashi-Slavnov-Taylor identities and Open EFT expansions...
Reference graph
Works this paper leans on
-
[1]
Tinkham,Introduction to Superconductivity: Second Edition
M. Tinkham,Introduction to Superconductivity: Second Edition. Dover Books on Physics. Dover Publications, 2004. https://books.google.com.hk/books?id=k6AO9nRYbioC
work page 2004
-
[2]
On the Theory of superconductivity,
V. L. Ginzburg and L. D. Landau, “On the Theory of superconductivity,”Zh. Eksp. Teor. Fiz.20(1950) 1064–1082
work page 1950
-
[3]
On the theory of phase transitions,
L. D. Landau, “On the theory of phase transitions,”Zh. Eksp. Teor. Fiz.7(1937) 19–32
work page 1937
-
[4]
An introduction to the Ginzburg–Landau theory of phase transitions and nonequilibrium patterns,
P. C. Hohenberg and A. P. Krekhov, “An introduction to the Ginzburg–Landau theory of phase transitions and nonequilibrium patterns,”Phys. Rept.572(2015) 1–42
work page 2015
-
[5]
On the Magnetic Properties of Superconductors of the Second Group,
A. A. Abrikosov, “On the Magnetic Properties of Superconductors of the Second Group,”Sov. Phys. JETP5(1957) 1174–1182
work page 1957
-
[6]
Microscopic theory of superconductivity,
J. Bardeen, L. N. Cooper, and J. R. Schrieffer, “Microscopic theory of superconductivity,”Phys. Rev.106(1957) 162
work page 1957
-
[7]
J. Bardeen, L. N. Cooper, and J. R. Schrieffer, “Theory of superconductivity,”Phys. Rev.108(1957) 1175–1204
work page 1957
-
[8]
Bound electron pairs in a degenerate Fermi gas,
L. N. Cooper, “Bound electron pairs in a degenerate Fermi gas,”Phys. Rev.104(1956) 1189–1190
work page 1956
-
[9]
BCS: The scientific “love of my life
P. W. Anderson, “BCS: The scientific “love of my life”,” inBCS: 50 Years, Cooper, L. N. and Feldman, D., ed., pp. 127–142. World Scientific, 2011
work page 2011
-
[10]
H. Bruus and K. Flensberg,Many-Body Quantum Theory in Condensed Matter Physics: An Introduction. Oxford Graduate Texts. Oxford University Press, 2004
work page 2004
-
[11]
Phenomenological theory of unconventional superconductivity,
M. Sigrist and K. Ueda, “Phenomenological theory of unconventional superconductivity,”Rev. Mod. Phys.63(1991) 239–311
work page 1991
-
[12]
Interface high-temperature superconductivity,
L. Wang, X. Ma, and Q.-K. Xue, “Interface high-temperature superconductivity,” Supercond. Sci. Technol.29no. 12, (2016) 123001
work page 2016
-
[13]
H.-H. Wen, “Unconventional superconductivity after the BCS paradigm and empirical rules for the exploration of high temperature superconductors,”J. Phys.: Conf. Ser. 2323no. 1, (2022) 012001. 21
work page 2022
-
[14]
When superconductivity crosses over: From BCS to BEC,
Q. Chen, Z. Wang, R. Boyack, S. Yang, and K. Levin, “When superconductivity crosses over: From BCS to BEC,”Rev. Mod. Phys.96no. 2, (2024) 025002,arXiv:2208.01774 [cond-mat.supr-con]
-
[15]
Color superconductivity in dense quark matter
M. G. Alford, A. Schmitt, K. Rajagopal, and T. Sch¨ afer, “Color superconductivity in dense quark matter,”Rev. Mod. Phys.80(2008) 1455–1515,arXiv:0709.4635 [hep-ph]
work page internal anchor Pith review Pith/arXiv arXiv 2008
-
[16]
The structure of a vortex line and the lower critical field in superconducting alloys,
L. Neumann and L. Tewordt, “The structure of a vortex line and the lower critical field in superconducting alloys,”Z. Physik189(1966) 55–66
work page 1966
-
[17]
Temperature dependence of the magnetization in the mixed state of superconducting alloys,
L. Neumann and L. Tewordt, “Temperature dependence of the magnetization in the mixed state of superconducting alloys,”Z. Physik191(1966) 73–80
work page 1966
-
[18]
Extended Ginzburg-Landau Formalism for Two-Band Superconductors,
A. A. Shanenko, M. V. Miloˇ sevi´ c, F. M. Peeters, and A. V. Vagov, “Extended Ginzburg-Landau Formalism for Two-Band Superconductors,”Phys. Rev. Lett.106 (2011) 047005
work page 2011
-
[19]
A. Vagov, A. A. Shanenko, M. V. Miloˇ sevi´ c, V. M. Axt, and F. M. Peeters, “Two-band superconductors: Extended Ginzburg-Landau formalism by a systematic expansion in small deviation from the critical temperature,”Phys. Rev. B86(2012) 144514
work page 2012
-
[20]
A. V. Vagov, A. A. Shanenko, M. V. Miloˇ sevi´ c, V. M. Axt, and F. M. Peeters, “Extended Ginzburg-Landau formalism: Systematic expansion in small deviation from the critical temperature,”Phys. Rev. B85(2012) 014502
work page 2012
-
[21]
A. Schmid, “A time dependent Ginzburg–Landau equation and its applications to a problem of resistivity in the mixed state,”Physik der kondensierten Materie5(1966) 302–317
work page 1966
-
[22]
Extension of the Ginzburg-Landau theory equations for nonstationary problems,
L. P. Gor’kov and G. M. Eliashberg, “Extension of the Ginzburg-Landau theory equations for nonstationary problems,”Soviet Physics JETP27no. 2, (1968) 328–334
work page 1968
-
[23]
Kopnin,Theory of Nonequilibrium Superconductivity
N. Kopnin,Theory of Nonequilibrium Superconductivity. Oxford University Press, 2001
work page 2001
-
[24]
A. V. Harbick and M. K. Transtrum, “Time-dependent Ginzburg-Landau framework for sample-specific simulation of superconductors for radio-frequency applications,”Phys. Rev. B112(2025) 094518
work page 2025
-
[25]
A. Larkin and A. Varlamov,Theory of Fluctuations in Superconductors. Oxford University Press, 2005
work page 2005
-
[26]
Extended Time-Dependent Ginzburg–Landau Theory,
K. V. Grigorishin, “Extended Time-Dependent Ginzburg–Landau Theory,”J. Low Temp. Phys.203no. 3-4, (2021) 262–308
work page 2021
-
[27]
pyTDGL: Time-dependent Ginzburg-Landau in Python,
L. Bishop-Van Horn, “pyTDGL: Time-dependent Ginzburg-Landau in Python,” Comput. Phys. Commun.291(2023) 108799. 22
work page 2023
-
[28]
Microscopic derivation of the Ginzburg-Landau equations in the theory of superconductivity,
L. P. Gor’kov, “Microscopic derivation of the Ginzburg-Landau equations in the theory of superconductivity,”Soviet Physics - JETP (Engl. Transl.)9no. 6, (1959) 1364
work page 1959
-
[29]
Effective actions for anomalous hydrodynamics,
F. M. Haehl, R. Loganayagam, and M. Rangamani, “Effective actions for anomalous hydrodynamics,”JHEP03(2014) 034,arXiv:1312.0610 [hep-th]
-
[30]
The Fluid Manifesto: Emergent symmetries, hydrodynamics, and black holes,
F. M. Haehl, R. Loganayagam, and M. Rangamani, “The Fluid Manifesto: Emergent symmetries, hydrodynamics, and black holes,”JHEP01(2016) 184,arXiv:1510.02494 [hep-th]
-
[31]
Topological sigma models & dissipative hydrodynamics,
F. M. Haehl, R. Loganayagam, and M. Rangamani, “Topological sigma models & dissipative hydrodynamics,”JHEP04(2016) 039,arXiv:1511.07809 [hep-th]
-
[32]
Effective field theory of dissipative fluids,
M. Crossley, P. Glorioso, and H. Liu, “Effective field theory of dissipative fluids,”JHEP 09(2017) 095,arXiv:1511.03646 [hep-th]
-
[33]
P. Glorioso, M. Crossley, and H. Liu, “Effective field theory of dissipative fluids (II): classical limit, dynamical KMS symmetry and entropy current,”JHEP09(2017) 096, arXiv:1701.07817 [hep-th]
-
[34]
Effective Action for Relativistic Hydrodynamics: Fluctuations, Dissipation, and Entropy Inflow,
F. M. Haehl, R. Loganayagam, and M. Rangamani, “Effective Action for Relativistic Hydrodynamics: Fluctuations, Dissipation, and Entropy Inflow,”JHEP10(2018) 194, arXiv:1803.11155 [hep-th]
-
[35]
Lectures on non-equilibrium effective field theories and fluctuating hydrodynamics
H. Liu and P. Glorioso, “Lectures on non-equilibrium effective field theories and fluctuating hydrodynamics,”PoSTASI2017(2018) 008,arXiv:1805.09331 [hep-th]
work page Pith review arXiv 2018
-
[36]
Universal time-dependent Ginzburg-Landau theory,
A. Kapustin and L. Mrini, “Universal time-dependent Ginzburg-Landau theory,”Phys. Rev. B107no. 14, (2023) 144514,arXiv:2209.03391 [cond-mat.supr-con]
-
[37]
Nearly critical superfluids in Keldysh-Schwinger formalism,
A. Donos and P. Kailidis, “Nearly critical superfluids in Keldysh-Schwinger formalism,” JHEP01(2024) 110,arXiv:2304.06008 [hep-th]
-
[38]
Nearly critical superfluid: effective field theory and holography,
Y. Bu, H. Gao, X. Gao, and Z. Li, “Nearly critical superfluid: effective field theory and holography,”JHEP07(2024) 104,arXiv:2401.12294 [hep-th]
-
[39]
Critical Dynamics of Superfluids,
A. Donos and P. Kailidis, “Critical Dynamics of Superfluids,”arXiv:2510.20750 [hep-th]
-
[40]
L. D. Landau, L. P. Pitaevskii, and E. M. Lifshitz,Electrodynamics of Continuous Media. Butterworth-Heinemann, 2 ed., 1984
work page 1984
-
[41]
Strong-field magnetohydrodynamics for neutron stars,
S. Vardhan, S. Grozdanov, S. Leutheusser, and H. Liu, “Strong-field magnetohydrodynamics for neutron stars,”Phys. Rev. Res.6no. 4, (2024) L042050, arXiv:2207.01636 [astro-ph.HE]
-
[42]
A systematic formulation of chiral anomalous magnetohydrodynamics,
M. J. Landry and H. Liu, “A systematic formulation of chiral anomalous magnetohydrodynamics,”arXiv:2212.09757 [hep-ph]. 23
-
[43]
Towards an effective action for chiral magnetohydrodynamics,
A. Das, N. Iqbal, and N. Poovuttikul, “Towards an effective action for chiral magnetohydrodynamics,”arXiv:2212.09787 [hep-th]
-
[44]
An Open Effective Field Theory for light in a medium,
S. A. Salcedo, T. Colas, and E. Pajer, “An Open Effective Field Theory for light in a medium,”JHEP03(2025) 138,arXiv:2412.12299 [hep-th]
-
[45]
Gauging Open EFTs from the top down,
G. Kaplanek, M. Mylova, and A. J. Tolley, “Gauging Open EFTs from the top down,” arXiv:2512.17089 [hep-th]
-
[46]
The probe limit in MHD and its implications for magnetic transport,
G. Frangi, M. Bajec, G. K. Buza, A. Soloviev, and S. Grozdanov, “The probe limit in MHD and its implications for magnetic transport,”arXiv:2510.12352 [hep-th]
-
[47]
Effective field theory for dissipative photons from higher-form symmetries,
G. Yoshimura, Y. Akamatsu, and Y. Hirono, “Effective field theory for dissipative photons from higher-form symmetries,”arXiv:2601.00605 [hep-th]
-
[48]
Kamenev,Field Theory of Non-Equilibrium Systems
A. Kamenev,Field Theory of Non-Equilibrium Systems. Cambridge University Press, 2 ed., 2023
work page 2023
-
[49]
The second law of thermodynamics from symmetry and unitarity,
P. Glorioso and H. Liu, “The second law of thermodynamics from symmetry and unitarity,”arXiv:1612.07705 [hep-th]
-
[50]
Theory of dynamic critical phenomena,
P. C. Hohenberg and B. I. Halperin, “Theory of dynamic critical phenomena,”Rev. Mod. Phys.49(Jul, 1977) 435–479. https://link.aps.org/doi/10.1103/RevModPhys.49.435
-
[51]
Holographic Schwinger-Keldysh field theory of SU(2) diffusion,
Y. Bu, X. Sun, and B. Zhang, “Holographic Schwinger-Keldysh field theory of SU(2) diffusion,”JHEP08(2022) 223,arXiv:2205.00195 [hep-th]
-
[52]
Critical and near-critical relaxation of holographic superfluids,
M. Flory, S. Grieninger, and S. Morales-Tejera, “Critical and near-critical relaxation of holographic superfluids,”Phys. Rev. D110no. 2, (2024) 026019,arXiv:2209.09251 [hep-th]
-
[53]
Equilibration rates in a strongly coupled nonconformal quark-gluon plasma,
A. Buchel, M. P. Heller, and R. C. Myers, “Equilibration rates in a strongly coupled nonconformal quark-gluon plasma,”Phys. Rev. Lett.114no. 25, (2015) 251601, arXiv:1503.07114 [hep-th]
-
[54]
Holographic D-brane constructions with dynamical gauge fields
Y. Ahn, M. Baggioli, H.-S. Jeong, and M. Matsumoto, “Holographic D-brane constructions with dynamical gauge fields,”JHEP03(2026) 118,arXiv:2506.09461 [hep-th]
work page internal anchor Pith review Pith/arXiv arXiv 2026
-
[55]
Collective dynamics and the Anderson-Higgs mechanism in a bona fide holographic superconductor,
H.-S. Jeong, M. Baggioli, K.-Y. Kim, and Y.-W. Sun, “Collective dynamics and the Anderson-Higgs mechanism in a bona fide holographic superconductor,”JHEP03(2023) 206,arXiv:2302.02364 [hep-th]
-
[56]
Breaking an Abelian gauge symmetry near a black hole horizon,
S. S. Gubser, “Breaking an Abelian gauge symmetry near a black hole horizon,”Phys. Rev. D78(2008) 065034,arXiv:0801.2977 [hep-th]
-
[57]
S. A. Hartnoll, C. P. Herzog, and G. T. Horowitz, “Holographic Superconductors,” JHEP12(2008) 015,arXiv:0810.1563 [hep-th]. 24
-
[58]
Building an AdS/CFT superconductor
S. A. Hartnoll, C. P. Herzog, and G. T. Horowitz, “Building a Holographic Superconductor,”Phys. Rev. Lett.101(2008) 031601,arXiv:0803.3295 [hep-th]
work page internal anchor Pith review Pith/arXiv arXiv 2008
-
[59]
Lectures on Holographic Superfluidity and Superconductivity
C. P. Herzog, “Lectures on Holographic Superfluidity and Superconductivity,”J. Phys. A42(2009) 343001,arXiv:0904.1975 [hep-th]
work page internal anchor Pith review Pith/arXiv arXiv 2009
-
[60]
Introduction to Holographic Superconductor Models,
R.-G. Cai, L. Li, L.-F. Li, and R.-Q. Yang, “Introduction to Holographic Superconductor Models,”Sci. China Phys. Mech. Astron.58no. 6, (2015) 060401,arXiv:1502.00437 [hep-th]
-
[61]
Emergent Gauge Fields in Holographic Superconductors,
O. Domenech, M. Montull, A. Pomarol, A. Salvio, and P. J. Silva, “Emergent Gauge Fields in Holographic Superconductors,”JHEP08(2010) 033,arXiv:1005.1776 [hep-th]
-
[62]
U(1) quasi-hydrodynamics: Schwinger-Keldysh effective field theory and holography,
M. Baggioli, Y. Bu, and V. Ziogas, “U(1) quasi-hydrodynamics: Schwinger-Keldysh effective field theory and holography,”JHEP09(2023) 019,arXiv:2304.14173 [hep-th]
-
[63]
Generalized symmetries and 2-groups via electromagnetic duality inAdS/CF T,
O. DeWolfe and K. Higginbotham, “Generalized symmetries and 2-groups via electromagnetic duality inAdS/CF T,”Phys. Rev. D103no. 2, (2021) 026011, arXiv:2010.06594 [hep-th]
-
[64]
Holography and magnetohydrodynamics with dynamical gauge fields,
Y. Ahn, M. Baggioli, K.-B. Huh, H.-S. Jeong, K.-Y. Kim, and Y.-W. Sun, “Holography and magnetohydrodynamics with dynamical gauge fields,”JHEP02(2023) 012, arXiv:2211.01760 [hep-th]
-
[65]
An Analytic Holographic Superconductor,
C. P. Herzog, “An Analytic Holographic Superconductor,”Phys. Rev. D81(2010) 126009,arXiv:1003.3278 [hep-th]
-
[66]
Holographic systems far from equilibrium: a review,
H. Liu and J. Sonner, “Holographic systems far from equilibrium: a review,”Rept. Prog. Phys.83no. 1, (2019) 016001,arXiv:1810.02367 [hep-th]
-
[67]
A prescription for holographic Schwinger-Keldysh contour in non-equilibrium systems
P. Glorioso, M. Crossley, and H. Liu, “A prescription for holographic Schwinger-Keldysh contour in non-equilibrium systems,”arXiv:1812.08785 [hep-th]
-
[68]
Off-shell hydrodynamics from holography,
M. Crossley, P. Glorioso, H. Liu, and Y. Wang, “Off-shell hydrodynamics from holography,”JHEP02(2016) 124,arXiv:1504.07611 [hep-th]
-
[69]
Ginzburg-Landau effective action for a fluctuating holographic superconductor,
Y. Bu, M. Fujita, and S. Lin, “Ginzburg-Landau effective action for a fluctuating holographic superconductor,”JHEP09(2021) 168,arXiv:2106.00556 [hep-th]
-
[70]
Vortex shedding patterns in holographic superfluids at finite temperature,
P. Yang, S. Lan, Y. Tian, Y.-K. Yan, and H. Zhang, “Vortex shedding patterns in holographic superfluids at finite temperature,”Phys. Rev. D112no. 2, (2025) 026032, arXiv:2412.18320 [hep-th]
-
[71]
Giant vortex in a fast rotating holographic superfluid,
J.-H. Su, C.-Y. Xia, W.-C. Yang, and H.-B. Zeng, “Giant vortex in a fast rotating holographic superfluid,”Phys. Rev. D107no. 2, (2023) 026006,arXiv:2208.14172 [hep-th]. 25
-
[72]
Generation of vortices and stabilization of vortex lattices in holographic superfluids,
X. Li, Y. Tian, and H. Zhang, “Generation of vortices and stabilization of vortex lattices in holographic superfluids,”JHEP02(2020) 104,arXiv:1904.05497 [hep-th]
-
[73]
Vortices in holographic superfluids and superconductors as conformal defects,
´O. J. C. Dias, G. T. Horowitz, N. Iqbal, and J. E. Santos, “Vortices in holographic superfluids and superconductors as conformal defects,”JHEP04(2014) 096, arXiv:1311.3673 [hep-th]. 26
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.