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Journal of High Energy Physics

, 2010:151 | Cite as

Effective holographic theories for low-temperature condensed matter systems

  • Christos Charmousis
  • Blaise Goutéraux
  • Bom Soo Kim
  • Elias Kiritsis
  • Rene Meyer
Open Access
Article

Abstract

The IR dynamics of effective holographic theories capturing the interplay between charge density and the leading relevant scalar operator at strong coupling are analyzed. Such theories are parameterized by two real exponents (γ, δ) that control the IR dynamics. By studying the thermodynamics, spectra and conductivities of several classes of charged dilatonic black hole solutions that include the charge density back reaction fully, the landscape of such theories in view of condensed matter applications is characterized. Several regions of the (γ, δ) plane can be excluded as the extremal solutions have unacceptable singularities. The classical solutions have generically zero entropy at zero temperature, except when γ = δ where the entropy at extremality is finite. The general scaling of DC resistivity with temperature at low temperature, and AC conductivity at low frequency and temperature across the whole (γ, δ) plane, is found. There is a codimension-one region where the DC resistivity is linear in the temperature. For massive carriers, it is shown that when the scalar operator is not the dilaton, the DC resistivity scales as the heat capacity (and entropy) for planar (3d) systems. Regions are identified where the theory at finite density is a Mott-like insulator at T = 0. We also find that at low enough temperatures the entropy due to the charge carriers is generically larger than at zero charge density.

Keywords

Black Holes in String Theory AdS-CFT Correspondence Black Holes 

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© The Author(s) 2010

Open Access This article is distributed under the terms of the Creative Commons Attribution License which permits any use, distribution and reproduction in any medium, provided the original author(s) and source are credited.

Authors and Affiliations

  • Christos Charmousis
    • 1
    • 2
  • Blaise Goutéraux
    • 1
  • Bom Soo Kim
    • 3
    • 4
  • Elias Kiritsis
  • Rene Meyer
    • 4
  1. 1.Univ. Paris-Sud, Laboratoire de Physique ThéoriqueOrsayFrance
  2. 2.LMPT, Parc de GrandmontUniversité Francois RabelaisToursFrance
  3. 3.IESL-FORTHHeraklionGreece
  4. 4.Crete Center for Theoretical Physics, Department of PhysicsUniversity of CreteHeraklionGreece

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