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We present a direct path integral derivation of the propagator in the presence of a step potential. The derivation makes use of the Path Decomposition Expansion (PDX), and also of the definition of the propagator as a limit of lattice…

Quantum Physics · Physics 2015-05-13 James M. Yearsley

This paper presents an analytical treatment of the path integral formalism for time-dependent quantum systems within the framework of Wigner-Dunkl mechanics, emphasizing systems with varying masses and time-dependent potentials. By…

Quantum Physics · Physics 2026-01-01 A. Benchikha , B. Hamil , B. C. Lütfüoğlu

We present an analytical closed form expression, which gives a good approximate propagator for diffusion on the sphere. Our formula is the spherical counterpart of the Gaussian propagator for diffusion on the plane. While the analytical…

Statistical Mechanics · Physics 2016-10-05 Abhijit Ghosh , Joseph Samuel , Supurna Sinha

We present a complete derivation of the semiclassical limit of the coherent state propagator in one dimension, starting from path integrals in phase space. We show that the arbitrariness in the path integral representation, which follows…

Quantum Physics · Physics 2009-11-07 M. Baranger , M. A. M. de Aguiar , F. Keck , H. J. Korsch , B. Schellhaass

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

To reduce general relativity to the canonical Hamiltonian formalism and construct the path (functional) integral in a simpler and, especially in the discrete case, less singular way, one extends the configuration superspace, as in the…

General Relativity and Quantum Cosmology · Physics 2019-01-25 V. M. Khatsymovsky

A path-integral representation for the kernel of the evolution operator of general Hamiltonian systems is reviewed. We study the models with bosonic and fermionic degrees of freedom. A general scheme for introducing boundary conditions in…

High Energy Physics - Theory · Physics 2007-05-23 A. T. Filippov , A. P. Isaev

See hep-th/9907179.

High Energy Physics - Theory · Physics 2016-08-25 Shyamoli Chaudhuri

We construct the action-angle variables of a classical integrable model defined on complex projective phase space and calculate the quantum mechanical propagator in the coherent state path integral representation using the stationary phase…

High Energy Physics - Theory · Physics 2015-06-26 Phillial Oh , Myung-Ho Kim

An ordinary unambiguous integral representation for the finite propagator of a quantum system is found by starting of a privileged skeletonization of the functional action in phase space, provided by the complete solution of the…

Quantum Physics · Physics 2007-05-23 Rafael Ferraro

Feynman's path integral in adelic quantum mechanics is considered. The propagator K(x'',t'';x',t') for one-dimensional adelic systems with quadratic Lagrangians is analytically evaluated. Obtained exact general formula has the form which is…

High Energy Physics - Theory · Physics 2014-11-18 G. S. Djordjevic , B. Dragovich , L. Nesic

We construct a representation of the coherent state path integral using the Weyl symbol of the Hamiltonian operator. This representation is very different from the usual path integral forms suggested by Klauder and Skagerstan in…

Quantum Physics · Physics 2009-11-13 L. C. dos Santos , M. A. M. de Aguiar

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 present an Initial Value Representation for the semiclassical coherent state propagator based on complex trajectories. We map the complex phase space into a real phase space with twice as many dimensions and use a simple procedure to…

Quantum Physics · Physics 2009-08-14 Marcus A. M. de Aguiar , Silvio A. Vitiello , Adriano Grigolo

We study the Cauchy problem for an evolution equation of Schr\"odinger type. The Hamiltonian is the Weyl quantization of a real homogeneous quadratic form with a pseudodifferential perturbation of negative order from Shubin's class. We…

Analysis of PDEs · Mathematics 2019-03-06 Marco Cappiello , René Schulz , Patrik Wahlberg

A path integral representation of the evolution operator for the four-dimensional Dirac equation is proposed. A quadratic form of the canonical momenta regularizes the original representation of the path integral in the electron phase…

General Relativity and Quantum Cosmology · Physics 2009-11-11 Alexander S. Lukyanenko , Inna A. Lukyanenko

In the first part of this paper, we extend the d-dimensional unitarity cut method of hep-ph/0609191 to cases with massive propagators. We present formulas for integral reduction with which one can obtain coefficients of all pentagon, box,…

High Energy Physics - Phenomenology · Physics 2008-11-26 Ruth Britto , Bo Feng

By considering the most general metric which can occur on a contractable two dimensional symplectic manifold, we find the most general Hamiltonians on a two dimensional phase space to which equivariant localization formulas for the…

High Energy Physics - Theory · Physics 2009-10-22 Richard J. Szabo , Gordon W. Semenoff

The propagator associated to the potential barrier $V=V_{0}\cosh ^{-2}(\omega x)$ is obtained by solving path integrals. The method of delta functionals based on canonical and other transformations is used to reduce the path integral for…

Quantum Physics · Physics 2007-05-23 L. Guechi , T. F. Hammann

Path-integral expressions for one-particle propagators in scalar and fermionic field theories are derived, for arbitrary mass. This establishes a direct connection between field theory and specific classical point-particle models. The role…

High Energy Physics - Theory · Physics 2010-11-22 J. W. van Holten
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