Magnetic Brane Solutions in AdS

By E. D’Hoker, Per Kraus. 2009

213 citations recorded by the source corpus.

We construct asymptotically AdS5 solutions of Einstein-Maxwell theory dual to = 4 SYM theory on 3,1 in the presence of a background magnetic field. The solutions interpolate between AdS5 and a near horizon AdS3 × T2. The central charge of the near horizon region, and hence low temperature entropy of the solution, is found to be (4/3)1/2 times that of free = 4 SYM theory. The entropy vanishes at zero temperature. We also present the generalization of these solutions to arbitrary spacetime dimensionality.

Subfields: Astronomy and Astrophysics, Nuclear and High Energy Physics

View Paper: https://www.semanticscholar.org/paper/2cc3e29d317e96e9c13b5bcf76867b980c3065cf

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Citations in the corpus

Generalized global symmetries and dissipative magnetohydrodynamics (2016, background): “[43], and our theory could be tested by studying perturbations around this background.”
Charged magnetic brane solutions in AdS5 and the fate of the third law of thermodynamics (2009, background): “Even the special case of ρ = 0 at zero temperature (and B 6= 0) does not lend itself to a full analytical solution [23].”
Thermodynamics and instabilities of a strongly coupled anisotropic plasma (2011, background): “Previous holographic studies of anisotropic plasmas include solutions dual to non-commutative SYM theories at finite temperature [10, 11, 12, 13, 14], gravity duals of p-wave superconductors[15, 16, 17, 18, 19, 20, 21], solutions dual to N = 4 SYM theory coupled to electromagnetic fields with [22, 2”
Holographic Fermi surfaces and entanglement entropy (2011, background): “A good example will be the magnetic quantum critical point found in an asymptotically AdS5 geometry [38–40], as pointed out in [41].”
Introduction to Holographic Superconductors (2010, background): “Are the holographic superconductors still type II? The new magnetic brane solutions in [13] may be useful.”
Spatially modulated instabilities of magnetic black branes (2011, background): “The special case when the skew eigenvalues of the two-form field strength are all equal was discussed in [16] and the solutions are similar to the D = 4, 5 cases depending on whether D is even or odd, respectively.”