Schwinger effect and negative differential conductivity in holographic models

被引:17
作者
Chakrabortty, Shankhadeep [1 ,2 ]
Sathiapalan, B. [2 ]
机构
[1] Indian Inst Sci Educ & Res, Pune 411008, Maharashtra, India
[2] Inst Math Sci, Madras 600113, Tamil Nadu, India
关键词
PAIR CREATION; PHOTON;
D O I
10.1016/j.nuclphysb.2014.11.010
中图分类号
O412 [相对论、场论]; O572.2 [粒子物理学];
学科分类号
摘要
The consequences of the Schwinger effect for conductivity are computed for strong coupling systems using holography. The one-loop diagram on the flavor brane introduces an O(lambda/N-c) imaginary part in the effective action for a Maxwell flavor gauge field. This in turn introduces a real conductivity in an otherwise insulating phase of the boundary theory. Moreover, in certain regions of parameter space the differential conductivity is negative. This is computed in the context of the Sakai-Sugimoto model. (C) 2014 The Authors. Published by Elsevier B.V.
引用
收藏
页码:241 / 262
页数:22
相关论文
共 32 条
  • [1] Abramowitz Milton, 2014, APPL MATH SERIES, V55
  • [2] Chiral symmetry breaking and external fields in the Kuperstein-Sonnenschein model
    Alam, M. Sohaib
    Kaplunovsky, Vadim S.
    Kundu, Arnab
    [J]. JOURNAL OF HIGH ENERGY PHYSICS, 2012, (04):
  • [3] Schwinger mechanism and graphene
    Allor, Danielle
    Cohen, Thomas D.
    McGady, David A.
    [J]. PHYSICAL REVIEW D, 2008, 78 (09):
  • [4] [Anonymous], 2011, J HIGH ENERGY PHYS
  • [5] Pair creation by a photon in an electric field
    Baier, V. N.
    Katkov, V. M.
    [J]. PHYSICS LETTERS A, 2010, 374 (22) : 2201 - 2206
  • [6] Pair creation by a photon in a strong magnetic field
    Baier, V. N.
    Katkov, V. M.
    [J]. PHYSICAL REVIEW D, 2007, 75 (07):
  • [7] Bergman O., 2008, JHEP, V0805, P007
  • [8] DITTRICH W, 1985, LECT NOTES PHYS, V220, P1
  • [9] Eisenhart L.P., 1966, RIEMANNIAN GEOMETRY
  • [10] Gil A, 2001, MATH COMPUT, V70, P1183, DOI 10.1090/S0025-5718-00-01268-0