N = 1 supersymmetric quantum chromodynamics : How confined non-Abelian monopoles emerge from quark condensation

N = 1 supersymmetric quantum chromodynamics : How confined non-Abelian monopoles emerge from quark condensation
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N = 1 超对称量子色动力学:夸克凝聚如何产生受限非阿贝尔单极子

DOI:
10.1103/physrevd.75.065032
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发表时间:
2007
期刊:
影响因子:
5
通讯作者:
A. Yung
A. Yung
中科院分区:
物理与天体物理2区
文献类型:
--
作者:
A. Gorsky;M. Shifman;A. Yung;A. Yung

文献摘要

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本文考虑N=1超对称QCD,其规范群为U(N),夸克味数为N{sub f}=N。为了摆脱平坦的方向,我们添加了一个介子超场。该理论没有伴随场,因此在准经典极限下没有Hooft-Polyakov单极。我们观察到一个非阿贝尔迈斯纳效应:色荷(方)的凝聚产生受限的单极子。在没有伴随标量的N=1超对称QCD中,它们的存在这一事实以前是未知的。我们的分析是分析的,是基于这样一个事实,即考虑中的N=1理论可以从N=2 SQCD开始获得,其中t Hooft-Polyakov单极子确实存在,通过一定的限制程序,使我们能够跟踪这些单极子在各个阶段的状态。单极子被Bogomol'nyi-Prasad-Sommerfield(BPS)非阿贝尔弦(通量管)限制。弦取向零模的动力学行为用弦世界片上的超对称CP(N-1)σ模型描述。如果能找到一个N=1的SQCD的对偶,它具有规范群U(N)和N{sub f}=N夸克味,那么在这个对偶理论中,我们的证明就等价于非阿贝尔对偶Meissner效应的证明。
We consider N=1 supersymmetric QCD with the gauge group U(N) and N{sub f}=N quark flavors. To get rid of flat directions we add a meson superfield. The theory has no adjoint fields and, therefore, no 't Hooft-Polyakov monopoles in the quasiclassical limit. We observe a non-Abelian Meissner effect: condensation of color charges (squarks) gives rise to confined monopoles. The very fact of their existence in N=1 supersymmetric QCD without adjoint scalars was not known previously. Our analysis is analytic and is based on the fact that the N=1 theory under consideration can be obtained starting from N=2 SQCD in which the 't Hooft-Polyakov monopoles do exist, through a certain limiting procedure allowing us to track the status of these monopoles at various stages. Monopoles are confined by Bogomol'nyi-Prasad-Sommerfield (BPS) non-Abelian strings (flux tubes). Dynamics of string orientational zero modes are described by a supersymmetric CP(N-1) sigma model on the string world sheet. If a dual of N=1 SQCD with the gauge group U(N) and N{sub f}=N quark flavors could be identified, in this dual theory our demonstration would be equivalent to the proof of the non-Abelian dual Meissner effect.