Stress Tensor of Static Dipoles in strongly coupled $\mathcal{N}$=4 Gauge Theory

Abstract

In the context of the AdS/CFT correspondence we calculate the induced stress tensor of static dipoles (electric-electric and electric-magnetic) in a strongly coupled $\mathcal{N}=4$ SYM gauge theory, by solving the linearized Einstein equation with Maldecena string as a source. Analytic expressions are given for the far-field and a near-field close to one charge, and compared to what one has in weak coupling. The result can be compared to lattice results for QCD-like theories in a deconfined but strongly coupled regime.

References in corpus (7)

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• Strongly coupled plasma with electric and magnetic charges
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• The stress tensor of a quark moving through N=4 thermal plasma
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Cited by in corpus (7)

• Light quark energy loss in strongly-coupled N = 4 supersymmetric Yang-Mills plasma
• The stress-energy tensor of a quark moving through a strongly-coupled N=4 supersymmetric Yang-Mills plasma: comparing hydrodynamics and AdS/CFT
• Toward the AdS/CFT Gravity Dual for High Energy Collisions: II. The Stress Tensor on the Boundary
• Universality of the diffusion wake in the gauge-string duality
• Shock waves from heavy-quark mesons in AdS/CFT
• On the critical condition in gravitational shock wave collision and heavy ion collisions
• Gravity Dual Corrections to the Heavy Quark Potential at Finite-Temperature