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arXiv 1807.01700hep-th
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石墨烯和边界中心荷的超共形模型

Superconformal Models for Graphene and Boundary Central Charges

Christopher P. Herzog, Kuo-Wei Huang, Itamar Shamir, Julio Virrueta

摘要:

在边界共形场论的背景下,我们研究了在超对称性存在的情况下,边界迹反常是否依赖于边界方向。最近,人们发现具有四维体光子和三维边界电子的类石墨烯非超对称共形场论具有两个边界中心荷,它们依赖于一个精确的边缘方向,即规范耦合。在这项工作中,我们supersymmetrize这个理论,特别注意所需的超对称性的边界条件。我们研究的模型与4,8,和16庞加莱超荷的散装,其中一半被打破的边界。在所有情况下,我们发现,在所有阶微扰理论,规范耦合是不重整化,提供了强有力的证据,这些理论是边界共形场论。此外,边界中心荷取决于耦合。这种对边缘方向的依赖性的一个可能的例外是,在最大超对称情况下,两个电荷之间的差异在一个环路处是耦合独立的。在我们的分析中,一个可能的边界Chern-Simons项是由一个散装$θ$ -长期。

英文摘要:

In the context of boundary conformal field theory, we investigate whether the boundary trace anomaly can depend on marginal directions in the presence of supersymmetry. Recently, it was found that a graphene-like non-supersymmetric conformal field theory with a four-dimensional bulk photon and a three-dimensional boundary electron has two boundary central charges that depend on an exactly marginal direction, namely the gauge coupling. In this work, we supersymmetrize this theory, paying special attention to the boundary terms required by supersymmetry. We study models with 4, 8, and 16 Poincaré supercharges in the bulk, half of which are broken by the boundary. In all cases, we find that at all orders in perturbation theory, the gauge coupling is not renormalized, providing strong evidence that these theories are boundary conformal field theories. Moreover, the boundary central charges depend on the coupling. One possible exception to this dependence on marginal directions is that the difference between the two charges is coupling independent at one-loop in the maximally supersymmetric case. In our analysis, a possible boundary Chern-Simons term is incorporated by a bulk $θ$-term.

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