Abstract
We revisit supersymmetric nonlinear sigma models on the target manifold $CP^{N-1}$ and $SO(N)/SO(N-2)\times U(1)$ in four dimensions. These models are formulated as gauged linear models, but it is indicated that the Wess-Zumino term should be added to the linear model since the hidden local symmetry is anomalous. Applying a procedure used for quantization of anomalous gauge theories to the nonlinear models, we determine the form of the Wess-Zumino term, by which a global symmetry in the linear model becomes smaller in the action than the conventional one. Moreover, we analyze the resulting linear model in the $1/N$ leading order. Consequently, we find that the model has a critical coupling constant similar to bosonic models. In the weak coupling regime, the $U(1)$ local symmetry is broken but supersymmetry is never broken. In contrast to the bosonic case, it is impossible to find stable vacua in the strong coupling regime as far as in the $1/N$ leading order. These results are straightforwardly generalized to the case of the hermitian symmetric space.
Highlights
A nonlinear sigma model is regarded as a low-energy effective field theory, where the relevant degrees of freedoms are massless Nambu-Goldstone (NG) bosons associated with broken global symmetries
We find that the model has the critical coupling, below which the Uð1Þlocal symmetry is broken and supersymmetry is unbroken
We have shown that the supersymmetric CPN−1 and SOðNÞ=SOðN − 1Þ × Uð1Þ models are formulated as anomalous gauge theories
Summary
A nonlinear sigma model is regarded as a low-energy effective field theory, where the relevant degrees of freedoms are massless Nambu-Goldstone (NG) bosons associated with broken global symmetries. We will explicitly deal with CPN−1 and SOðNÞ=SOðN − 1Þ × Uð1Þ models, but our results can be generalized straightforwardly to other target manifolds, because these models capture typical features of the models without or with F-term constraint [15] Both nonlinear models will be formulated as anomalous gauged linear models. We show that the supersymmetric CPN−1 model is quantumly equivalent to the theory given by the Kähler potential [Eq (2.9)] and the F-term [Eq (2.20)] This F-term reduces the flavor symmetry to SUðN − 1Þ, and so the action of this gauged linear model has the symmetry SUðN − 1Þ × Uð1Þlocal
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.