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Representations by means of path integrals are used to find spinor and isospinor structure of relativistic particle propagators in external fields. For Dirac propagator in an external electromagnetic field all grassmannian integrations are…

High Energy Physics - Theory · Physics 2009-10-22 D. M. Gitman , Sh. M. Shvartsman

We construct a worldline path integral for the effective action and propagator of a Dirac field in 2+1 dimensions in an Abelian gauge field background. Integrating over an auxiliary gauge group variable we derive a worldline action…

High Energy Physics - Theory · Physics 2008-11-26 C. D. Fosco , J. Sanchez-Guillen , R. A. Vazquez

We consider a simple action for a fractional spin particle and a path integral representation for the propagator is obtained in a gauge such that the constraint embodied in the Lagrangian is not an obstacle. We obtain a propagator for the…

High Energy Physics - Theory · Physics 2007-05-23 Wellington da Cruz

We derive some non-perturbative results in 1+1 and 2+1 dimensions within the context of the particle path-integral representation for a Dirac field propagator in the presence of an external field, in a formulation introduced by Migdal in…

High Energy Physics - Theory · Physics 2009-11-10 C. Fosco , J. Sanchez-Guillen , R. A. Vazquez

A variation to the usual formulation of Grassmann representation path integrals is presented. Time-indexed anticommuting partners are introduced for each Grassmann coherent state variable and a general method for handling the effect of…

Quantum Physics · Physics 2007-05-23 S. Shresta

We simplify and generalize an approach proposed by Di Vecchia and Ravndal to describe a massive Dirac particle in external vector and scalar fields. Two different path integral representations for the propagator are derived systematically…

High Energy Physics - Theory · Physics 2009-10-31 C. Alexandrou , R. Rosenfelder , A. W. Schreiber

We examine the problem of the evaluation of both the propagator and of the partition function of a spinning particle in an external field at the classical as well as the quantum level, in connection with the asserted exactness of the saddle…

Condensed Matter · Physics 2009-10-28 E. Ercolessi , G. Morandi , F. Napoli , P. Pieri

The relativistic Green's function of a free spin-1/2 fermion is derived using the Feynman path integral formalism in spherical coordinates. The Green's function is reduced to an exactly solvable path integral by an appropriate coordinate…

Atomic Physics · Physics 2023-09-26 Sreya Banerjee , Zoltán Harman

We present different non-perturbative calculations within the context of Migdal's representation for the propagator and effective action of quantum particles. We first calculate the exact propagators and effective actions for Dirac, scalar…

High Energy Physics - Theory · Physics 2009-11-11 C. D. Fosco , J. Sanchez-Guillen , R. A. Vazquez

The technique of functional integration over velocities is applied to the calculation of the propagator of a spinning particle with and without anomalous magnetic moment. A representation for the spin factor is obtained in this context for…

High Energy Physics - Theory · Physics 2009-09-25 Wellington da Cruz

The propagator of a spinning particle in external Abelian field and in arbitrary dimensions is presented by means of a path integral. The problem has different solutions in even and odd dimensions. In even dimensions the representation is…

High Energy Physics - Theory · Physics 2009-10-30 D. M. Gitman

For the `classical' formulation of a massive spinning particle, the propagator is obtained along with the spin factor. We treat the system with two kinds of constraints that were recently shown to be concerned with the reparametrization…

High Energy Physics - Theory · Physics 2009-10-28 Jin-Ho Cho , Seungjoon Hyun , Hyuk-Jae Lee

In this paper, we correct an inaccurate result of previous works on the Feynman propagator in position space of a free Dirac field in (3+1)-dimensional spacetime, and we derive the generalized analytic formulas of both the scalar Feynman…

Mathematical Physics · Physics 2010-11-02 Hong-Hao Zhang , Kai-Xi Feng , Si-Wei Qiu , An Zhao , Xue-Song Li

The motion of a particle in the field of dispiration (due to a wedge disclination and a screw dislocation) is studied by path integration. By gauging $SO(2) \otimes T(1)$, first, we derive the metric, curvature, and torsion of the medium of…

Mathematical Physics · Physics 2012-02-03 Akira Inomata , Georg Junker , James Raynolds

Representations of propagators by means of path integrals over velocities are discussed both in nonrelativistic and relativistic quantum mechanics. It is shown that all the propagators can only be expressed through bosonic path integrals…

High Energy Physics - Theory · Physics 2007-05-23 D. M. Gitman , Sh. M. Shvartsman

Electromagnetic interactions of the spin 3/2 particle are investigated while allowing the propagation of the transverse spin 1/2 component present in the reducible Rarita-Schwinger vector-spinor. This is done by allowing a more general form…

High Energy Physics - Theory · Physics 2011-11-23 Konstantin G. Savvidy

The concept of a propagator is useful and is a well-known object in diffusion NMR experiments. Here, we investigate the related concept; the propagator for the magnetisation or the Green's function of the Torrey-Bloch equations. The…

Statistical Mechanics · Physics 2015-03-25 Robin A. Damion

We introduce the spinor parallel propagator for maximally symmetric spaces in any dimension. Then, the Dirac spinor Green's functions in the maximally symmetric spaces R^n, S^n and H^n are calculated in terms of intrinsic geometric objects.…

High Energy Physics - Theory · Physics 2008-11-26 Wolfgang Mück

Polyakov's spin factor enters as a weight in the path-integral description of particle-like modes propagating in Euclidean space-times, accounting for particle spin. The Fock-Feynman-Schwinger path integral applied to QCD accomodates…

High Energy Physics - Theory · Physics 2009-10-31 A. I. Karanikas , C. N. Ktorides

In the path integral formulation of quantum mechanics, the phase factor Exp[iS(x[t])] is associated with every path x[t]. Summing this factor over all paths yields Feynman's propagator as a sum-over-paths. In the original formulation, the…

Quantum Physics · Physics 2007-05-23 G. N. Ord , J. A. Gualtieri , R. B. Mann
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