Magnetic instability in AdS/CFT : Schwinger effect and Euler-Heisenberg Lagrangian of Supersymmetric QCD
arXiv:1403.6336 · doi:10.1007/JHEP06(2014)085
Abstract
To reveal the Schwinger effect for quarks, i.e., pair creation process of quarks and antiquarks, we derive the vacuum decay rate at strong coupling using AdS/CFT correspondence. Magnetic fields, in addition to the electric field responsible for the pair creation, causes prominent effects on the rate, and is important also in experiments such as RHIC/LHC heavy ion collisions. In this paper, through the gravity dual we obtain the full Euler-Heisenberg Lagrangian of N=2 supersymmetric QCD and study the Schwinger mechanism with not only a constant electric field but also a constant magnetic field as external fields. We determine the quark mass and temperature dependence of the Lagrangian. In sharp contrast with the zero magnetic field case, we find that the imaginary part, and thus the vacuum decay rate, diverges in the massless zero-temperature limit. This may be related to a strong instability of the QCD vacuum in strong magnetic fields. The real part of the Lagrangian serves as a generating function for non-linear electro-magnetic responses, and is found such that the Cotton-Mouton effect vanishes. Interestingly, our results of the Schwinger / Cotton-Mouton effects coincide precisely with those of N=2 supersymmetric QED.
21 pages. v2:references added, footnotes added
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Cited by in corpus (7)
- The melting of charmonium in a magnetic field from an effective AdS/QCD model
- A holographic description of the Schwinger effect in a confining gauge theory
- Electric Field Quench in AdS/CFT
- Effect of gluon condensate on holographic Schwinger effect
- Holographic Schwinger effect in a rotating strongly coupled medium
- Electromagnetic instability in holographic QCD
- Universal turbulence on branes in holography