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PATH INTEGRAL AND OPERATOR APPROACH FOR THE PODOLSKY-SCHWINGER MODEL
(Springer, 1992-12-01)
We study the role of the thachyonic excitation which emerges from the quantum electrodynamics in two dimensions with Podolsky term. The quantization is performed by using path integral framework and the operator approach.
Comment on symmetric path integrals for stochastic equations with multiplicative noise
(2002)
We recall our approach through discretizations for path integrals and its general results for representations of probability densities. It is shown that the result of Arnold [P. Arnold, Phys. Rev. E 61, 6099 (2000)] is a ...
A path integral approach to the Hodgkin–Huxley model
(Elsevier Science, 2017-11)
To understand how single neurons process sensory information, it is necessary to develop suitable stochastic models to describe the response variability of the recorded spike trains. Spikes in a given neuron are produced ...
Option pricing, stochastic volatility, singular dynamics and constrained path integrals
(Elsevier, 2014)
Stochastic volatility models have been widely studied and used in the financial world. The
Heston model (Heston, 1993) [7] is one of the best known models to deal with this issue.
These stochastic volatility models are ...
Nonpertubative solutions of massless gauged thirring model
(2010-12-01)
We present a nonperturbative quantization of the two-dimensional massless gauged Thirring model by using the path-integral approach. First, we will study the constraint structure of model via the Dirac's formalism and by ...
Quantum propagator for some classes of three-dimensional three-body systems
(2006-05-01)
In this work we solve exactly a class of three-body propagators for the most general quadratic interactions in the coordinates, for arbitrary masses and couplings. This is done both for the constant as the time-dependent ...
Quantum propagator for some classes of three-dimensional three-body systems
(2006-05-01)
In this work we solve exactly a class of three-body propagators for the most general quadratic interactions in the coordinates, for arbitrary masses and couplings. This is done both for the constant as the time-dependent ...