Recognition: 2 theorem links
· Lean TheoremNovel five-dimensional rotating Lifshitz black holes with electric and axionic charges
Pith reviewed 2026-05-16 11:31 UTC · model grok-4.3
The pith
Five-dimensional rotating Lifshitz black holes can be supported by both electric and axionic charges.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
The central discovery is a new family of exact five-dimensional charged and rotating asymptotically Lifshitz black holes. The spacetime solves the Einstein equations coupled to a dilaton, two Abelian gauge fields, and axionic scalars supplemented by two generalized Chern-Simons terms. The configuration is characterized by a range of the free dynamical exponent z and possesses nontrivial thermodynamical parameters, where the first law of black hole thermodynamics is verified and the corresponding Smarr relation derived. These solutions provide the first explicit family of five-dimensional rotating Lifshitz black holes supported simultaneously by electric and axionic charges.
What carries the argument
The metric and field ansatz with generalized Chern-Simons terms that admits exact solutions with Lifshitz asymptotics, rotation, and both charges for a continuous range of the dynamical exponent z.
If this is right
- The first law of black hole thermodynamics holds for these solutions.
- A Smarr relation follows from the thermodynamic parameters of the family.
- Increasing the rotation parameter suppresses the scalar condensate in the dual holographic superconductor.
- Increasing the dynamical critical exponent enhances the superconducting order.
Where Pith is reading between the lines
- These backgrounds could model rotating non-relativistic condensed matter systems through holographic duality.
- The rotation-induced suppression of condensation offers a tunable parameter for phase transitions in the dual theory.
- Similar ansatze may yield solutions in other dimensions or with additional matter fields.
Load-bearing premise
A specific metric and field ansatz combined with generalized Chern-Simons terms allows exact solutions with the required Lifshitz scaling and charges for a continuous range of the dynamical exponent.
What would settle it
Direct substitution of the proposed metric and fields into the Einstein equations to verify whether the equations hold identically for a chosen value of the dynamical exponent z.
Figures
read the original abstract
In this work, we construct a new family of exact five-dimensional charged and rotating asymptotically Lifshitz black holes. The spacetime solves Einstein equations coupled to a dilaton, two Abelian gauge fields, and axionic scalars supplemented by two generalized Chern-Simons terms. This configuration is characterized by a range of the free dynamical exponent $z$ and possesses nontrivial thermodynamical parameters, where we verify the first law of black hole thermodynamics and derive the corresponding Smarr relation. As an application of this new gravitational background, we then investigate a holographic superconductor in the rotating Lifshitz background. We study the condensation of the scalar operator and the AC conductivity of the dual system. These results show that increasing the rotation parameter suppresses the condensate and weakens the superconducting phase, while increasing the dynamical critical exponent enhances the superconducting order. To the best of our knowledge, these solutions provide the first explicit family of five-dimensional rotating Lifshitz black holes supported simultaneously by electric and axionic charges.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper constructs a new family of exact five-dimensional rotating asymptotically Lifshitz black holes carrying both electric and axionic charges. The solutions arise from a direct metric and field ansatz in Einstein gravity coupled to a dilaton, two Abelian gauge fields, axionic scalars, and generalized Chern-Simons terms. The configurations are shown to solve the field equations for a continuous range of the dynamical exponent z, to possess a regular horizon, and to satisfy the first law of black-hole thermodynamics together with the corresponding Smarr relation. As an application, the backgrounds are used to study holographic superconductivity, where the effects of the rotation parameter and z on scalar condensation and AC conductivity are analyzed.
Significance. If the explicit solutions are correct, the work supplies the first known family of five-dimensional rotating Lifshitz black holes supported by both electric and axionic charges. This fills a concrete gap in the literature and supplies new gravitational backgrounds for holographic studies of condensed-matter systems with Lifshitz scaling and rotation. The direct verification of thermodynamic consistency and the concrete holographic results on how rotation suppresses condensation while larger z enhances the order parameter constitute clear strengths of the manuscript.
minor comments (2)
- [Section 2] The explicit metric functions, dilaton profile, and gauge-field components obtained after solving the reduced ODEs should be written out in full (perhaps in an appendix) so that independent verification of the Einstein equations and thermodynamic identities is immediate.
- [Section 4] In the holographic-superconductor section, the precise boundary conditions imposed on the scalar field and the definition of the order parameter should be stated explicitly, together with the numerical method used to extract the critical temperature.
Simulated Author's Rebuttal
We thank the referee for the careful reading and positive evaluation of our manuscript. The referee summary accurately captures our main results: the construction of the first known family of five-dimensional rotating asymptotically Lifshitz black holes carrying both electric and axionic charges, the direct verification that the solutions satisfy the field equations for a range of z, the confirmation of the first law and Smarr relation, and the holographic superconductivity analysis demonstrating that rotation suppresses scalar condensation while larger z enhances the order parameter. Since no specific major comments were raised, we have no individual points to address.
Circularity Check
No significant circularity in derivation chain
full rationale
The paper constructs its five-dimensional rotating Lifshitz black hole solutions via an explicit metric and field ansatz (including dilaton, two gauge fields, axions, and generalized Chern-Simons terms) that directly reduces the modified Einstein equations to solvable ODEs, yielding exact expressions with Lifshitz asymptotics, regular horizons, and independent charges for a continuous range of z. Thermodynamic relations such as the first law and Smarr formula are then verified by direct substitution of the obtained quantities rather than by any redefinition or fitting procedure. No load-bearing steps reduce to self-definition, fitted inputs renamed as predictions, or self-citation chains; the derivation remains self-contained against the input ansatz and the field equations.
Axiom & Free-Parameter Ledger
free parameters (1)
- dynamical exponent z
axioms (1)
- domain assumption Einstein equations coupled to a dilaton, two Abelian gauge fields, axionic scalars and two generalized Chern-Simons terms
Lean theorems connected to this paper
-
IndisputableMonolith/Foundation/AlexanderDuality.leanalexander_duality_circle_linking unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
five-dimensional rotating asymptotically Lifshitz black holes... metric ansatz (8) with f(r), N(r), N_x1(r) for z ∈ (2,3]
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]
Dimensional Reduction in Quantum Gravity
G. ’t Hooft, Conf. Proc. C 930308 (1993), 284-296 [arXiv:gr-qc/9310026 [gr-qc]]
work page internal anchor Pith review Pith/arXiv arXiv 1993
-
[2]
L. Susskind, J. Math. Phys. 36 (1995), 6377-6396 doi:10.1063/1.531249 [arXiv:hep-th/9409089 [hep-th]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1063/1.531249 1995
-
[3]
J. M. Maldacena, Adv. Theor. Math. Phys. 2, 231- 252 (1998) doi:10.4310/ATMP.1998.v2.n2.a1 [arXiv:hep- th/9711200 [hep-th]]
-
[4]
Anti De Sitter Space And Holography
E. Witten, Adv. Theor. Math. Phys.2 (1998), 253-291 doi:10.4310/ATMP.1998.v2.n2.a2 [arXiv:hep-th/9802150 [hep-th]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.4310/atmp.1998.v2.n2.a2 1998
-
[5]
S. S. Gubser, I. R. Klebanov and A. M. Polyakov, Phys. Lett. B 428 (1998), 105-114 doi:10.1016/S0370- 2693(98)00377-3 [arXiv:hep-th/9802109 [hep-th]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1016/s0370- 1998
-
[6]
S. S. Gubser, Phys. Rev. D 78, 065034 (2008) doi:10.1103/PhysRevD.78.065034 [arXiv:0801.2977 [hep- th]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1103/physrevd.78.065034 2008
-
[7]
S. A. Hartnoll, C. P. Herzog and G. T. Horowitz, Phys. Rev. Lett. 101, 031601 (2008) doi:10.1103/PhysRevLett.101.031601 [arXiv:0803.3295 [hep-th]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1103/physrevlett.101.031601 2008
-
[8]
Critical magnetic field in AdS/CFT superconductor
E. Nakano and W. Y. Wen, Phys. Rev. D 78, 046004 (2008) doi:10.1103/PhysRevD.78.046004 [arXiv:0804.3180 [hep-th]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1103/physrevd.78.046004 2008
-
[9]
S. A. Hartnoll, C. P. Herzog and G. T. Horowitz, JHEP 12, 015 (2008) doi:10.1088/1126-6708/2008/12/015 [arXiv:0810.1563 [hep-th]]. 10
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1088/1126-6708/2008/12/015 2008
-
[10]
The Holographic Superconductor Vortex
M. Montull, A. Pomarol and P. J. Silva, Phys. Rev. Lett. 103, 091601(2009)doi:10.1103/PhysRevLett.103.091601 [arXiv:0906.2396 [hep-th]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1103/physrevlett.103.091601 2009
-
[11]
Emergent Gauge Fields in Holographic Superconductors
O. Domenech, M. Montull, A. Pomarol, A. Salvio and P. J. Silva, JHEP 08, 033 (2010) doi:10.1007/JHEP08(2010)033 [arXiv:1005.1776 [hep- th]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1007/jhep08(2010)033 2010
-
[12]
Flux Periodicities and Quantum Hair on Holographic Superconductors
M. Montull, O. Pujolas, A. Salvio and P. J. Silva, Phys. Rev. Lett. 107, 181601 (2011) doi:10.1103/PhysRevLett.107.181601 [arXiv:1105.5392 [hep-th]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1103/physrevlett.107.181601 2011
-
[13]
Magnetic Response in the Holographic Insulator/Superconductor Transition
M. Montull, O. Pujolas, A. Salvio and P. J. Silva, JHEP 04, 135 (2012) doi:10.1007/JHEP04(2012)135 [arXiv:1202.0006 [hep-th]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1007/jhep04(2012)135 2012
-
[14]
Holographic Superfluids and Superconductors in Dilaton-Gravity
A. Salvio, JHEP 09, 134 (2012) doi:10.1007/JHEP09(2012)134 [arXiv:1207.3800 [hep- th]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1007/jhep09(2012)134 2012
-
[15]
Transitions in Dilaton Holography with Global or Local Symmetries
A. Salvio, JHEP 03, 136 (2013) doi:10.1007/JHEP03(2013)136 [arXiv:1302.4898 [hep- th]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1007/jhep03(2013)136 2013
-
[16]
Vortex lattice for a holographic superconductor
K. Maeda, M. Natsuume and T. Okamura, Phys. Rev. D 81, 026002 (2010) doi:10.1103/PhysRevD.81.026002 [arXiv:0910.4475 [hep-th]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1103/physrevd.81.026002 2010
-
[17]
A. Donos, J. P. Gauntlett and C. Pantelidou, JHEP 07, 095 (2020) doi:10.1007/JHEP07(2020)095 [arXiv:2001.11510 [hep-th]]
-
[18]
C. Y. Xia, H. B. Zeng, Y. Tian, C. M. Chen and J. Zaanen, Phys. Rev. D 105, no.2, L021901 (2022) doi:10.1103/PhysRevD.105.L021901 [arXiv:2111.07718 [hep-th]]
-
[19]
M. de la Cruz-López, J. A. Herrera-Mendoza, R. Cartas- Fuentevilla and A. Herrera-Aguilar, Eur. Phys. J. Plus 139 (2024) no.9, 786 doi:10.1140/epjp/s13360-024- 05585-2 [arXiv:2402.12476 [hep-th]]
-
[20]
M. de la Cruz-López, A. Herrera-Aguilar, D. Martínez- Carbajal and S. Patiño-López, Eur. Phys. J. C 85, no.10, 1103 (2025) doi:10.1140/epjc/s10052-025-14642-8 [arXiv:2411.05259 [hep-th]]
-
[21]
Gravity Duals of Lifshitz-like Fixed Points
S. Kachru, X. Liu and M. Mulligan, Phys. Rev. D 78, 106005 (2008) doi:10.1103/PhysRevD.78.106005 [arXiv:0808.1725 [hep-th]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1103/physrevd.78.106005 2008
-
[22]
M. Taylor, [arXiv:0812.0530 [hep-th]]
work page internal anchor Pith review Pith/arXiv arXiv
-
[23]
Holographic superconductors with $z=2$ Lifshitz scaling
Y. Bu, Phys. Rev. D 86, 046007 (2012) doi:10.1103/PhysRevD.86.046007 [arXiv:1211.0037 [hep-th]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1103/physrevd.86.046007 2012
-
[24]
J. W. Lu, Y. B. Wu, P. Qian, Y. Y. Zhao and X. Zhang, Nucl. Phys. B 887, 112-135 (2014) doi:10.1016/j.nuclphysb.2014.08.001 [arXiv:1311.2699 [hep-th]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1016/j.nuclphysb.2014.08.001 2014
-
[25]
Z. Zhao, Q. Pan and J. Jing, Phys. Lett. B 735, 438-444 (2014) doi:10.1016/j.physletb.2014.06.065 [arXiv:1311.6260 [hep-th]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1016/j.physletb.2014.06.065 2014
-
[26]
J. A. Herrera-Mendoza, D. F. Higuita-Borja, J. A. Méndez-Zavaleta, A. Herrera-Aguilar and F. Pérez- Rodríguez, Phys. Rev. D 106 (2022) no.8, L081902 doi:10.1103/PhysRevD.106.L081902 [arXiv:2208.05988 [hep-th]]
-
[27]
Holographic Superconductors in a Rotating Spacetime
K. Lin and E. Abdalla, Eur. Phys. J. C 74, no.11, 3144 (2014) doi:10.1140/epjc/s10052-014-3144-4 [arXiv:1403.7407 [hep-th]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1140/epjc/s10052-014-3144-4 2014
-
[28]
Analytic investigation of rotating holographic superconductors
A. Srivastav and S. Gangopadhyay, Eur. Phys. J. C 79, no.4, 340 (2019) doi:10.1140/epjc/s10052-019-6834-0 [arXiv:1902.01628 [hep-th]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1140/epjc/s10052-019-6834-0 2019
- [29]
-
[30]
A new rotating axionic AdS$_4$ black hole dressed with a scalar field
M. Bravo-Gaete, F. F. Santos, J. A. Herrera-Mendoza and D. F. Higuita-Borja, [arXiv:2504.17081 [hep-th]]
work page internal anchor Pith review Pith/arXiv arXiv
-
[31]
D. Z. Freedman and A. Van Proeyen, Cambridge Univ. Press, 2012, ISBN 978-1-139-36806-3, 978-0-521-19401-3 doi:10.1017/CBO9781139026833
-
[32]
M. Bravo-Gaete, A. Cisterna, M. Hassaine and D. Kubiznak, Phys. Lett. B 868 (2025), 139721 doi:10.1016/j.physletb.2025.139721 [arXiv:2506.04854 [hep-th]]
-
[33]
R. Deshpande and O. Lunin, JHEP 06 (2025), 066 doi:10.1007/JHEP06(2025)066 [arXiv:2411.01795 [hep- th]]
-
[34]
T. Hale, B. R. Hull, D. Kubizňák, R. B. Mann and J. Menšíková, Class. Quant. Grav. 42 (2025) no.9, 09LT01 doi:10.1088/1361-6382/adc9f2 [arXiv:2412.04329 [gr-qc]]
-
[35]
Black holes and black branes in Lifshitz spacetimes
J. Tarrio and S. Vandoren, JHEP 09 (2011), 017 doi:10.1007/JHEP09(2011)017 [arXiv:1105.6335 [hep- th]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1007/jhep09(2011)017 2011
-
[36]
G. W. Gibbons and S. W. Hawking, Phys. Rev. D15, 2752 (1977)
work page 1977
-
[37]
T. Regge and C. Teitelboim, Role of Surface Inte- grals in the Hamiltonian Formulation of General Rel- ativity, Annals Phys. 88, 286 (1974) doi:10.1016/0003- 4916(74)90404-7
-
[38]
M. Ortaggio and A. Srinivasan, Phys. Rev. D 110 (2024) no.4, 4 doi:10.1103/PhysRevD.110.044035 [arXiv:2309.02900 [gr-qc]]
-
[39]
Here we note that, as was shown in [35], the integration constant µ is fixed to ensure consistency with the desired Lifshitz asymptotic behavior
-
[40]
Here, it is important to note that the two Chern–Simons generalized terms do not appear in the Euclidean action due to their topological structure
-
[41]
For this situation, as before, the integration constantµ is fixed to ensure consistency with the desired asymptotic behavior, and the electric charge comes from the second vector field
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.