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Stability of Holographic Superconductors
High Energy Physics - Theory · Submitted 28 Jul 2010
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim It implies the stability of the superconducting phase.
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The abstract, sentence by sentence
We study the dynamical stability of holographic superconductors. We first classify perturbations around black hole background solutions into vector and scalar sectors by means of a 2-dimensional rotational symmetry. We prove the stability of the vector sector by explicitly constructing the positive definite Hamiltonian. To reveal a mechanism for the stabilization of a superconducting phase, we construct a quadratic action for the scalar sector. From the action, we see the stability of black holes near a critical point is determined by the equation of motion for a charged scalar field. We show the effective mass of the charged scalar field in hairy black holes is always above the Breitenlohner-Freedman bound near the critical point due to the backreaction of a gauge field. It implies the stability of the superconducting phase. We also argue that the stability continues away from the critical point.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We study the dynamical stability of holographic superconductors. | contribution 0.91 | 0.93 | 0.04 | unclear 0.69 |
| s1 | We first classify perturbations around black hole background solutions into vector and scalar sectors by means of a 2-dimensional rotational symmetry. | method 0.97 | 0.95 | 0.02 | asserted 0.99 |
| s2 | We prove the stability of the vector sector by explicitly constructing the positive definite Hamiltonian. | result 0.86 | 0.97 | 0.12 | asserted 1.00 |
| s3 | To reveal a mechanism for the stabilization of a superconducting phase, we construct a quadratic action for the scalar sector. | method 0.78 | 0.96 | 0.04 | asserted 0.92 |
| s4 | From the action, we see the stability of black holes near a critical point is determined by the equation of motion for a charged scalar field. | result 0.90 | 0.92 | 0.11 | asserted 1.00 |
| s5 | We show the effective mass of the charged scalar field in hairy black holes is always above the Breitenlohner-Freedman bound near the critical point due to the backreaction of a gauge field. | result 0.99 | 0.93 | 0.30 | asserted 1.00 |
| s6 | It implies the stability of the superconducting phase. | interpretation 1.00 | 0.80 | 0.50 | asserted 0.65 |
| s7 | We also argue that the stability continues away from the critical point. | result 0.88 | 0.88 | 0.16 | asserted 0.43 |
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The paper
Original abstract
We study the dynamical stability of holographic superconductors. We first classify perturbations around black hole background solutions into vector and scalar sectors by means of a 2-dimensional rotational symmetry. We prove the stability of the vector sector by explicitly constructing the positive definite Hamiltonian. To reveal a mechanism for the stabilization of a superconducting phase, we construct a quadratic action for the scalar sector. From the action, we see the stability of black holes near a critical point is determined by the equation of motion for a charged scalar field. We show the effective mass of the charged scalar field in hairy black holes is always above the Breitenlohner-Freedman bound near the critical point due to the backreaction of a gauge field. It implies the stability of the superconducting phase. We also argue that the stability continues away from the critical point.
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References
How the literature uses it
5 arXiv papers cite this in 5 sentences
Papers citing it · 3 sentences without a confident label
Cites it as background 2 papers
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There has been a great deal of recent work in this area, studying how the system behaves in a variety of different scenarios including altering the scalar mass and spacetime dimension, changing the gauge group and adding an external magnetic field [ref] .
The Rich Structure of Gauss-Bonnet Holographic Superconductors · Introduction · 0.99
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Many aspects of holographic superconductivity are now well understood also in the $(3+1)$-dimensional case, such as their behavior in the presence of an external magnetic field, different scalar masses, potentials and backgrounds; for a (partial) list see [ref] .
Holographic Superconductors and Higher Curvature Corrections · Introduction · 0.97
What it cites · 11 sentences without a confident label
Builds on 5 papers
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For example, it is possible to extend our analysis to the Gauss-Bonnet superconductors [ref] .
Holographic Superconductors with Higher Curvature Corrections · Conclusion · 0.87
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For example, it is possible to extend our analysis to the Gauss-Bonnet superconductors [ref] .
Holographic Superconductors with various condensates in Einstein-Gauss-Bonnet gravity · Conclusion · 0.87
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For example, it is possible to extend our analysis to the Gauss-Bonnet superconductors [ref] .
Holographic Superconductors in 3+1 dimensions away from the probe limit · Conclusion · 0.87
Uses the method or tool of 1 paper
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In this section, we explain a useful method to obtain a quadratic action for black hole perturbations [ref] .
Hawking Radiation from Fluctuating Black Holes · Uses of ADM Formalism · 0.99
Cites as background 6 papers
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In this section, we review the gravity/superconductor correspondence [ref] .
Building an AdS/CFT superconductor · Gravity dual of superconductors · 1.00
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In this section, we review the gravity/superconductor correspondence [ref] .
Holographic Superconductors · Gravity dual of superconductors · 1.00
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It is believed that the AdS/CFT correspondence is useful to study strongly coupled systems [ref] .
The Large N Limit of Superconformal Field Theories and Supergravity · Introduction · 0.99
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