A range of flavour number at which the N=1 supersymmetric QCD becomes a superconformal field theory . The exact Novikov-Shifman-Vainshtein-Zakharov beta function of the N=1 supersymmetric QCD shows that the theory may have a nontrivial infrared fixed point [1]. The beta function vanishes at the fixed point , so the N=1 supersymmetric QCD becomes a superconformal quantum field theory , since the trace of the energy-momentum tensor is proportional to the beta function [2]. The theory can now have a dual magnetic description in the sense that it describes the same physics as N=1 supersymmetric QCD , but the gauge coupling reverses. The dynamics of the N=1 supersymmetric QCD is very sensitive to the flavour number N f and color number N c . With different choices of the flavour and color numbers , the theory can be in distinct dynamical phases [3]. Therefore, the N = 1 superconformal symmetry does not occur for an arbitrary...
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Lozano, Y. et al. (2004). Seiberg Conformal Window. In: Duplij, S., Siegel, W., Bagger, J. (eds) Concise Encyclopedia of Supersymmetry. Springer, Dordrecht. https://doi.org/10.1007/1-4020-4522-0_480
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