Abstract

We formulate four-dimensional $\mathcal{N} = 1$ supersymmetric nonlinear sigma models on Hermitian symmetric spaces with higher derivative terms, free from the auxiliary field problem and the Ostrogradski's ghosts, as gauged linear sigma models. We then study Bogomol'nyi-Prasad-Sommerfield equations preserving 1/2 or 1/4 supersymmetries. We find that there are distinct branches, that we call canonical ($F=0$) and non-canonical ($F\neq 0$) branches, associated with solutions to auxiliary fields $F$ in chiral multiplets. For the ${\mathbb C}P^N$ model, we obtain a supersymmetric ${\mathbb C}P^N$ Skyrme-Faddeev model in the canonical branch while in the non-canonical branch the Lagrangian consists of solely the ${\mathbb C}P^N$ Skyrme-Faddeev term without a canonical kinetic term. These structures can be extended to the Grassmann manifold $G_{M,N} = SU(M)/[SU(M-N)\times SU(N) \times U(1)]$. For other Hermitian symmetric spaces such as the quadric surface $Q^{N-2}=SO(N)/[SO(N-2) \times U(1)])$, we impose F-term (holomorphic) constraints for embedding them into ${\mathbb C}P^{N-1}$ or Grassmann manifold. We find that these constraints are consistent in the canonical branch but yield additional constraints on the dynamical fields thus reducing the target spaces in the non-canonical branch.

Highlights

  • Nonlinear sigma models are typical examples of lowenergy effective theories

  • For other Hermitian symmetric spaces such as the quadric surface QN−2 1⁄4 SOðNÞ=1⁄2SOðN − 2Þ × Uð1ފÞ, we impose F-term constraints for embedding them into CPN−1 or Grassmann manifold. We find that these constraints are consistent in the canonical branch but yield additional constraints on the dynamical fields, reducing the target spaces in the noncanonical branch

  • The purpose of this paper is to present higher derivative supersymmetric nonlinear sigma models with a wider class of target spaces—Hermitian symmetric spaces, CPN−1 1⁄4 SUðNÞ=1⁄2SUðN − 1Þ × Uð1ފ; GM;N 1⁄4 UðMÞ=1⁄2UðM − NÞ × UðNފ; QN−2 1⁄4 SOðNÞ=1⁄2SOðN − 2Þ × Uð1ފ; SOð2NÞ=UðNÞ; SpðNÞ=UðNÞ; E6=1⁄2SOð10Þ × Uð1ފ; E7=1⁄2E6 × Uð1ފ; ð1:1Þ

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Summary

INTRODUCTION

Nonlinear sigma models are typical examples of lowenergy effective theories. When a global symmetry G is spontaneously broken down to its subgroup H, there appear massless Nambu-Goldstone bosons dominant at low energy, and their low-energy dynamics can be described by nonlinear sigma model whose target space is a coset space G=H [1,2]. In the noncanonical branch, the bosonic part of the Lagrangian consists of only the fourderivative term of the Skyrme-Faddeev type [43] (that is without fourth order time derivatives) without any canonical kinetic term This admits a compact baby Skyrmion [45] which is a BPS state preserving 1=4 supersymmetry [27]. In the case without higher derivative terms, supersymmetric nonlinear sigma models on Hermitian symmetric spaces can be constructed by imposing supersymmetric constraints on gauged linear sigma models [27] This formulation is found to help us to solve auxiliary field equations even with higher derivative terms. As for a superfield notation, we follow the Wess-Bagger convention [50]

SUPERSYMMETRIC HIGHER DERIVATIVE TERMS IN THE CHIRAL MODEL
NONLINEAR SIGMA MODELS WITH D-TERM CONSTRAINTS
Canonical branch
Noncanonical branch
NONLINEAR SIGMA MODELS WITH D- AND F-TERM CONSTRAINTS
BOGOMOL’NYI-PRASAD-SOMMERFIELD STATES
BPS states in canonical branch
BPS states in noncanonical branch
COMMENT ON FERMIONIC INTERACTIONS
CONCLUSION AND DISCUSSIONS
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