Non-Abelian strings
Mikhail A Shifman, Alexei Yung · Cambridge University Press eBooks · 2023
Non-Abelian stringsIn this chapter we discuss a particular class of N = 2 supersymmetric gauge theories in which non-Abelian strings were found.One can pose the question: what is so special about these models that makes an Abelian Z N string become non-Abelian?Models we will dwell on below have both gauge and flavor symmetries broken by the condensation of scalar fields.The common feature of these models is that some global diagonal combination of color and flavor groups survive the breaking.We consider the case when this diagonal group is SU(N) C+F , where the subscript C + F means a combination of global color and flavor groups.The presence of this unbroken subgroup is responsible for the occurrence of the orientational zero modes of the string which entail its non-Abelian nature.Clearly, the presence of supersymmetry is not important for the construction of non-Abelian strings.In particular, while here we focus on the BPS non-Abelian strings in N = 2 supersymmetric gauge theories, in Chapter 5 we review non-Abelian strings in N = 1 supersymmetric theories and in Chapter 6 in nonsupersymmetric theories. Basic model: N = 2 SQCDThe model we will deal with derives from N = 2 SQCD with the gauge group SU(N + 1) and N f = N flavors of the fundamental matter hypermultiplets which we will call quarks [3].At a generic point on the Coulomb branch of this theory, the gauge group is broken down to U(1) N .We will be interested, however, in a particular subspace of the Coulomb branch, on which the gauge group is broken down to SU(N)×U(1).We will enforce this regime by a special choice of the quark mass terms.The breaking SU(N + 1) → SU(N)×U(1) occurs at the scale m which is supposed to lie very high, m SU(N +1) , where SU(N +1) is the scale of the SU(N + 1) theory.Correspondingly, the masses of the gauge bosons from the 85