Building a holographic superconductor.

By S. Hartnoll, Christopher P. Herzog, G. Horowitz. Physical Review Letters, 2008

1,775 citations recorded by the source corpus.

Subfields: Astronomy and Astrophysics, Nuclear and High Energy Physics, Statistical and Nonlinear Physics

View Paper: https://www.semanticscholar.org/paper/971acc9e5806bcf5bdfafe5dfeb80afc40b722ce

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Citations in the corpus

Holography of charged dilaton black holes (2009, background): “(3)In the context of holographic superconductors [10, 11], another class of black branes with vanishing entropy at T = 0 was recently found in [12, 13, 14].”
What Can Gauge-Gravity Duality Teach Us about Condensed Matter Physics? (2011, background): “This indicates that the holographic superfluids [74, 75] are not conventional superfluids at T = 0, and perhaps co-exist with a non-Fermi liquid sector.”
Analytical study on holographic superconductors in external magnetic field (2010, background): “considered a neutral black hole with a charged scalar and the only Maxwell sector A = At and they captured the essence in this limit and showed that the properties of a (2+1)-dimensional superconductor can indeed be reproduced [6].”
Superconductivity from gauge/gravity duality with flavor (2008, background): “in [6, 7, 8], as well as a realization of a superconducting current from a top-down (super-) gravity model, rather than in a phenomenological bottom-up AdS/QCD model.”
Holographic endpoint of spatially modulated phase transition (2010, background): “dratic terms in the equations of motion (3.10) and the fact that we consider the gravity system classically. The mean eld behavior is also observed in the holographic description of superconductivity [2, 4]. 4 Quantum Corrections We found that the phase transition is of the second order in the class”
Holographic Duality with a View Toward Many-Body Physics (2009, background): “If we put a charged boson in this geometry, we find the holographic superconductor phenomenon ([57, 58, 59], for a review see [60]).”
Thermodynamics of Rotating Black Holes and Black Rings: Phase Transitions and Thermodynamic Volume (2014, background): “For a charged scalar field coupled to Einstein–Maxwell theory a similar situation occurs: at small temperatures charged scalar hair forms and the resulting “hairy black holes” are thermodynamically preferred [90–97].”
Lectures on holographic non-Fermi liquids and quantum phase transitions (2011, background): “For a charged scalar the condensed phase is the well-studied holographic superconductor [93, 94]; for reviews see [51, 52].”
Introduction to holographic superconductor models (2015, methodology): “1 The Abelian-Higgs model In this subsection, we begin with the Abelian-Higgs model [11] by introducing a complex scalar field Ψ, with mass m and charge q, into the (3 + 1) dimensional Einstein-Maxwell theory with a negative cosmological constant.”
Gauge gravity duality for d-wave superconductors: prospects and challenges (2010, methodology): “Indeed, given the similarity between our condensing spin two field and the Abelian Higgs model of [10], the behavior of the fermion correlator in the condensed phase will be identical to that of the s-wave superconductor studied in [43, 44].”
Spatially modulated instabilities of magnetic black branes (2011, background): “Such superfluid black branes were first analysed in phenomenological theories of gravity [1, 2, 3] and then in consistent truncations of D = 10, 11 supergravity [4, 5, 6, 7].”
Holographic striped phases (2011, background): “These instabilities and the back reacted black branes were first studied in a bottom up context in [1][2][3] and then subsequently embedded into D=11 and D=10 supergravity in [4][5][6][7].”
Holographic superconductors with various condensates (2008, methodology): “It has recently been shown that a simple Einstein-Maxwell theory coupled to a charged scalar provides a holographically dual description of a superconductor [1, 2].”