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arXiv · hep-th/0208166

Properties of the Bound States of Super-Yang-Mills-Chern-Simons Theory

J. R. Hiller·S. S. Pinsky·U. Trittmann
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Abstract

We apply supersymmetric discrete light-cone quantization (SDLCQ) to the study of supersymmetric Yang-Mills-Chern-Simons (SYM-CS) theory on R x S^1 x S^1. One of the compact directions is chosen to be light-like and the other to be space-like. Since the SDLCQ regularization explicitly preserves supersymmetry, this theory is totally finite, and thus we can solve for bound-state wave functions and masses numerically without renormalizing. The Chern-Simons term is introduced here to provide masses for the particles while remaining totally within a supersymmetric context. We examine the free, weak and strong-coupling spectrum. The transverse direction is discussed as a model for universal extra dimensions in the gauge sector. The wave functions are used to calculate the structure functions of the lowest mass states. We discuss the properties of Kaluza-Klein states and focus on how they appear at strong coupling. We also discuss a set of anomalously light states which are reflections of the exact Bogomol'nyi-Prasad-Sommerfield states of the underlying SYM theory.

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J. R. Hiller, S. S. Pinsky, U. Trittmann. 2002-08-22. Properties of the Bound States of Super-Yang-Mills-Chern-Simons Theory. https://doi.org/10.1103/physrevd.66.125015

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