Chiral Thirring-Wess model with Faddeevian Regularization

Abstract

Replacing vector type of interaction of the Thirring-Wess model by the chiral type a new model is presented which is termed here as chiral Thirring-Wess model. Ambiguity parameters of regularization is so chosen that the model falls into the Faddeevian class. The resulting Faddeevian class of model in general do not possess Lorentz invariance. However we can exploit the arbitrariness admissible in the ambiguity parameters to relate the quantum mechanically generated ambiguity parameters with the classical parameter involved in the masslike term of the gauge field which helps to maintain physical Lorentz invariance instead of the absence of manifestly lorentz covariance of the model. The the phase space structure and the theoretical spectrum of this class of model has been determined through Dirac's method of quantization of constraint system.

9 pages latex, submitted to Ann. Phys

References in corpus (5)

• Schwinger Model In Noncommutating Space-Time
• On the mass spectrum of noncommutative Schwinger model in Euclidean ${\mathbb{R}}^2$ space
• Nonperturbative solution of the Nonconfining Schwinger Model with a generalized regularization
• Unparticle in (1+1) dimension with one loop correction
• The Thirring-Wess Model Revisited: A Functional Integral Approach

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• Role of Faddeevian anomaly in the s-wave scattering of chiral fermion off dilaton black holes towards preservation of information
• Chiral Thirring-Wess Model
• On the Poincaré and Gauge symmetry of a model where vector and axial vector interaction get mixed up with different weight
• On the indistinguishability of Chiral QED with parameter-free Faddeevian anomaly and QED under a chiral constraint