Abstract

We consider a Galilean mathcal{N}=2 supersymmetric theory with F-term couplings in 2 + 1 dimensions, obtained by null reduction of a relativistic Wess-Zumino model. We compute quantum corrections and we check that, as for the relativistic parent theory, the F-term does not receive quantum corrections. Even more, we find evidence that the causal structure of the non-relativistic dynamics together with particle number conservation constrain the theory to be one-loop exact.

Highlights

  • In the relativistic setting the construction of SUSY invariant actions and the study of renormalization properties is better performed in superspace, where fields belonging to the same multiplet are organized in superfields

  • Since the non-relativistic limit via null reduction technique does not modify the grassmannian part of the superfields in the action, R-symmetry works in the same way as in the relativistic case

  • In this paper we studied the renormalization properties of a 2 + 1 dimensional model with S2G Galilean SUSY invariance, obtained by null reduction of the four-dimensional relativistic Wess-Zumino model (see eq (4.1))

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Summary

Non-relativistic supersymmetry algebra

We are interested in studying non-relativistic SUSY theories in 2 + 1 dimensions with S2G invariance This graded generalization of the Galilean algebra contains two complex supercharges and is described by the following non-vanishing (anti)commutators [Pj, Kk] = iδjkM , [Pj, J ] = −i jkPk ,. The central charge M corresponds to the mass or particle number conservation This is the non-relativistic N = 2 SUSY algebra in (2+1) dimensions. While in the relativistic reduction a central term appears in the fermionic part of the algebra when we reduce the number of dimensions, in the non-relativistic case the central charge is produced already in the bosonic sector (without requiring any SUSY extension) and accounts for the physical fact that in non-relativistic theories the particle number is a conserved quantity

Non-relativistic superspace
Review of the relativistic Wess-Zumino model
Renormalization in superspace
Renormalization in components
The non-renormalization theorem
The non-relativistic Wess-Zumino model
Super-Feynman and selection rules
Renormalizability of the theory
Loop corrections to the self-energy
Loop corrections to the vertices
Non-relativistic non-renormalization theorem
Conclusions
A Conventions
B Non-relativistic Wess-Zumino model in components
C Quantum corrections in components
D Example of non-relativistic supergraph calculation
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