Quarks in an External Electric Field in Finite Temperature Large N Gauge Theory
By Tameem Albash, V. Filev, Clifford V. Johnson, Arnab Kundu. 2007
329 citations recorded by the source corpus.
We use a ten dimensional dual string background to study aspects of the physics of large N four dimensional SU(N) gauge theory, where its fundamental quarks are charged under a background electric field. The theory is N = 2 supersymmetric for vanishing temperature and electric field. We work in a limit where the quarks do not back-react. At zero temperature, we observe that the electric field induces a phase transition associated with the dissociation of the mesons into their constituent quarks. This is an analogue of an insulator-metal transition, since the system goes from being an insulator with zero current (in the applied field) to a conductor with free charge carriers (the quarks). At finite temperature this phenomenon persists, and the dissociation transition becomes subsumed into the more familiar meson melting transition. Here, the dissociation phenomenon reduces the critical melting temperature.
Subfields: Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/4cb29d6e51477455c91c963a888aae89f88f5a37
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Citations in the corpus
- Analytic calculation of properties of holographic superconductors (2010, methodology): “In recent years it has been shown using the AdSd+1/CFTd correspondence [3] that for d = 3 and d = 4 we can create a strongly coupled superconducting system from its gravitational dual [4–7], also including an external magnetic field [8, 9].”
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- Supercurrent: Vector hair for an AdS black hole (2008, background): “Various related works discuss other aspects of superconductivity including partial discussions of Meissner effect and the non-abelian case [22, 23, 24, 25, 26, 27, 28].”
- Charged magnetic brane solutions in AdS5 and the fate of the third law of thermodynamics (2009, methodology): “This brane solution is known analytically for all ρ and B; its spectrum of small fluctuations may be obtained systematically, and used to compute physical quantities such as electric and thermal conductivities [1, 2, 3, 4, 5, 6, 7, 8, 9, 11, 12].”
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