2012
DOI: 10.1007/jhep01(2012)094
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Holographic Fermi and non-Fermi liquids with transitions in dilaton gravity

Abstract: Abstract:We study the two-point function for fermionic operators in a class of strongly coupled systems using the gauge-gravity correspondence. The gravity description includes a gauge field and a dilaton which determines the gauge coupling and the potential energy. Extremal black brane solutions in this system typically have vanishing entropy. By analyzing a charged fermion in these extremal black brane backgrounds we calculate the two-point function of the corresponding boundary fermionic operator. We find t… Show more

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Cited by 158 publications
(250 citation statements)
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References 80 publications
(236 reference statements)
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“…These results agree with the electric branes discussed in [85]. On the other hand, if the magnetic charge is nonzero, it always dominates over the electric charge, yielding parameters…”
Section: Jhep10(2013)126supporting
confidence: 88%
“…These results agree with the electric branes discussed in [85]. On the other hand, if the magnetic charge is nonzero, it always dominates over the electric charge, yielding parameters…”
Section: Jhep10(2013)126supporting
confidence: 88%
“…The challenge for the future is to describe the phases of Sections V and VI using the dual gravity theory, in a manner which captures their expected properties of finite-range models in d = 2 and d = 3 respectively, and there have been recent studies in this direction [10,[12][13][14][15][16][17][18]20]. In particular, the d = 3 model of Gubser and Rocha [10] is a promising model for future study.…”
Section: Discussionmentioning
confidence: 99%
“…Thus the superfluid condensate has charge Q = 4. The condensate cannot carry a net SU(2) gauge charge [63], and so we should have 20) which is realized in mean field theory by a real ∆ 1 . Actually the restriction is on total gauge charge neutrality, including the contributions of the fermions.…”
Section: A Phase Diagrammentioning
confidence: 99%
“…We follow the notation of [43] and [32] except for the assignment of γ µ (this difference is necessary to see the diagonalization as for fermion components, see below). The notation for the indices are: M = 0, 1, 2, z, and µ = 0, 1, 2.…”
Section: A Bulk Fermion Eigen-statesmentioning
confidence: 99%