Abstract
The full description of a superconductor requires that it has an infinite DC conductivity (or zero electrical resistivity) as well as expels the external magnetic fields. Thus, for any holographic superconductor which is dual to a real superconductor, it is necessary to examine, simultaneously, these two features based on the gauge/gravity duality. In this paper, we explore numerically these two aspects of the higher dimensional holographic superconductors, in the presence of a Power-Maxwell electrodynamics as the gauge field. At first, we calculate the critical temperature, condensation, conductivity, and superconducting gap, in the absence of magnetic field and disclose the effects of both power parameter, $s$, as well as the spacetime dimensions, $d$, on this quantities. Then, we immerse the superconductor into an external magnetic field, $B$, and observe that with increasing the magnetic field, the starting point of condensation occurs at temperature less than the critical temperature, $T_{c}$, in the absence of magnetic field. This implies that at a fixed temperature, we can define a critical magnetic field, above which the critical temperature goes to zero which is similar to the Meissner effect in superconductor. In these indications, we also try to show the distinction of the conformal invariance of the Power-Maxwell Lagrangian that occurs for $s=d/4$.
Highlights
The gauge/gravity correspondence [1,2,3], provides an efficient tool to explore strongly coupled phenomena in the field theory where the perturbational methods are no longer available
We immerse the superconductor into an external magnetic field, B, and observe that with increasing the magnetic field, the starting point of condensation occurs at temperature less than the critical temperature, Tc, in the absence of magnetic field
A version of this duality is called anti–deSitter/ conformal field theory (AdS/CFT) correspondence, which has been applied for investigating various aspects of holographic superconductors, using a gravity dual in a ðd þ 1Þ dimensional bulk for a superconductor which is localized on the d-dimensional boundary of the bulk [4,5]
Summary
The gauge/gravity correspondence [1,2,3], provides an efficient tool to explore strongly coupled phenomena in the field theory where the perturbational methods are no longer available. In the context of Gauss-Bonnet black holes, analytical and numerical studies on the properties of the holographic superconductors with power-Maxwell electrodynamics have been investigated [49,50]. Using the analytical matching method, the upper critical magnetic field of holographic superconductor with conformally invariant power-Maxwell electrodynamics have been explored in [51]. It was argued that in the presence of magnetic field, the physically acceptable phase behavior of the holographic superconductor can be deduced only for s 1⁄4 d=4, which guaranties the conformal invariance of the power-Maxwell Lagrangian. Conductivity as well as the effects of the magnetic field on the properties of the higher dimensional power-Maxwell holographic superconductors have not been explored by using the numerical shooting method.
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