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arXiv:0706.4106 · Annals of Physics

Path-integral quantization of Galilean Fermi fields

M. de Montigny, F.C. Khanna, F.M. Saradzhev

Published Aug 15, 2007• 9 citations
arXivHTMLPDF
DOI
10.1016/j.aop.2007.08.002

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Path-integral quantization of Galilean Fermi fields 1

M. de Montigny, F. C. Khanna, Fuad M. Saradzhev

The Galilei-covariant fermionic field theories are quantized by using the path-integral method and five-dimensional Lorentz-like covariant expressions of non-relativistic field equations. Firstly we review the five-dimensional approach to the Galilean Dirac equation, which leads to the Lévy-Leblond equations, and define the Galilean generating functional and Green’s functions for positive- and negative-energy/mass solutions. Then, as an example of interactions, we consider the quartic self-interacting potential λ(ΨΨ) 2, and we derive expressions for the 2- and 4-point Green’s functions. Our results are compatible with those found in the literature on non-relativistic many-body systems. The extended manifold allows for compact expressions of the contributions in (3 + 1) space-time. This is particularly apparent when we represent the results with diagrams in the extended (4 + 1) manifold, since they usually encompass more diagrams in Galilean (3 + 1) space-time. 1

•Dec 4, 2012•5 citations

Galilean transformation and the path integral propagator for a crossed electric and magnetic field

Carlos Farina de Souza, ALVARO DE SOUZA DUTRA

A Galilean transformation is made in the path integral formalism to obtain the Feynman propagator of a charged particle in the presence of a crossed uniform electromagnetic field in terms of the propagator of a charged particle in the presence of only a magnetic one. Also noted is how the result makes it possible to relate the initial propagator, with E and B, to that of the free particle.

American Journal of Physics•Apr 1, 1989•7 citations
The Galilei-covariant fermionic field theories are quantized by using the path-integral method and five-dimensional Lorentz-like covariant expressions of non-relativistic field equations. Firstly we review the five-dimensional approach to the Galilean Dirac equation, which leads to the Lévy-Leblond equations, and define the Galilean generating functional and Green’s functions for positive- and negative-energy/mass solutions. Then, as an example of interactions, we consider the quartic self-interacting potential λ(ΨΨ) 2, and we derive expressions for the 2- and 4-point Green’s functions. Our results are compatible with those found in the literature on non-relativistic many-body systems. The extended manifold allows for compact expressions of the contributions in (3 + 1) space-time. This is particularly apparent when we represent the results with diagrams in the extended (4 + 1) manifold, since they usually encompass more diagrams in Galilean (3 + 1) space-time. 1