Abstract

It was recently discovered that for a boundary system in the presence of a background magnetic field, the quantum fluctuation of the vacuum would create a non-uniform magnetization density for the vacuum and a magnetization current is induced in the vacuum [1]. It was also shown that this “magnetic Casimir effect” of the vacuum is closely related to another quantum effect of the vacuum, the Weyl anomaly. Furthermore, the phenomena can be understood in terms of the holography of the boundary system [2]. In this paper, we generalize this four dimensional effect to six dimensions. We use the AdS/BCFT holography to show that in the presence of a 3-form magnetic field strength H, a string current is induced in a six dimensional boundary conformal field theory. This allows us to determine the gauge field contribution to the Weyl anomaly in six dimensional conformal field theory in a H-flux background. For the (2,0) superconformal field theory of N M5-branes, the current has a magnitude proportional to N3 for large N. This suggests that the degree of freedoms scales as N3 in the (2,0) superconformal theory of N multiple M5-branes. The prediction we have for the Weyl anomaly is a new criteria that the (2,0) theory should satisfy.

Highlights

  • JHEP07(2019)151 the S duality of the N = 4 supersymmetric Yang-Mills theory [41]

  • It was shown that this “magnetic Casimir effect” of the vacuum is closely related to another quantum effect of the vacuum, the Weyl anomaly

  • We use the AdS/BCFT holography to show that in the presence of a 3-form magnetic field strength H, a string current is induced in a six dimensional boundary conformal field theory

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Summary

Boundary string current

Consider a boundary conformal field theory (BCFT) defined on a manifold M with boundary P. In (2.4), · · · denotes terms that are regular at x = 0, and Jμ(1ν) and Jμ(0ν) are functions of dimension 3 and 4 respectively Their form are constrained by (2.5) and the Lorentz and gauge symmetries of the theory. In [1] it was shown that, for four dimensions, the near boundary asymptotic form of the standard current Jμ is completely determined by the background field strength of the Weyl anomaly. It was shown in [2] that the near boundary current can be determined using the AdS/BCFT holography. Let us proceed first with the holographic analysis and determine the near boundary current using boundary holography

Holographic boundary current
Weyl anomaly from boundary current
Discussion
B Holographic Weyl anomaly
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