Through more detailed calculations on QED$_{1+1}$ and QED$_{3+1}$ employing a new treatment of Feynman Amplitudes, we attribute the regularization independent and hence definite origin of chiral anomaly in perturbation theory to an unambiguous term which is a rational function in momentum space. Some relevant remarks are presented
We propose to use rich informations on pi p total cross sections below N=10 GeV in order to investig...
AbstractWe prove a general identity for a F23 hypergeometric function over a finite field Fq, where ...
AbstractIn this paper, we deal with a class of pseudoparabolic problems with integral boundary condi...
AbstractWe introduce multiple q-Mahler measures and we calculate some specific examples, where multi...
Exact path integration for the one dimensional potential $V=b^2\cos 2q$ which describes the finite a...
Final state quark-antiquark interactions give origin to non zero values of the off-diagonal element ...
Results of the work of S. Bruce [{\it Nuovo Cimento} {\bf 110}B (1995) 115] are compared with those ...
The formulation of the relativistic spinless path integral on the general affine space is presented....
We consider the fate of 1/N expansions in unstable many-body quantum systems, as realized by a quenc...
We consider the fate of 1/N expansions in unstable many-body quantum systems, as realized by a quenc...
AbstractThis is the second part of a study of the inversion for a Sturm–Liouville difference equatio...
AbstractA singular integral equation with a Holderian second member function on [a,b] is considered ...
AbstractWe study asymptotic properties (as n→∞) of polynomials Qn(x)=xn+⋯, orthogonal with respect t...
5 pagesIt is suggested that Schwinger's (1951) vacuum persistence probability against pair productio...
Introduction/purpose: The problem of quantum corrections to propagators in Quantum Electrodynamics (...
We propose to use rich informations on pi p total cross sections below N=10 GeV in order to investig...
AbstractWe prove a general identity for a F23 hypergeometric function over a finite field Fq, where ...
AbstractIn this paper, we deal with a class of pseudoparabolic problems with integral boundary condi...
AbstractWe introduce multiple q-Mahler measures and we calculate some specific examples, where multi...
Exact path integration for the one dimensional potential $V=b^2\cos 2q$ which describes the finite a...
Final state quark-antiquark interactions give origin to non zero values of the off-diagonal element ...
Results of the work of S. Bruce [{\it Nuovo Cimento} {\bf 110}B (1995) 115] are compared with those ...
The formulation of the relativistic spinless path integral on the general affine space is presented....
We consider the fate of 1/N expansions in unstable many-body quantum systems, as realized by a quenc...
We consider the fate of 1/N expansions in unstable many-body quantum systems, as realized by a quenc...
AbstractThis is the second part of a study of the inversion for a Sturm–Liouville difference equatio...
AbstractA singular integral equation with a Holderian second member function on [a,b] is considered ...
AbstractWe study asymptotic properties (as n→∞) of polynomials Qn(x)=xn+⋯, orthogonal with respect t...
5 pagesIt is suggested that Schwinger's (1951) vacuum persistence probability against pair productio...
Introduction/purpose: The problem of quantum corrections to propagators in Quantum Electrodynamics (...
We propose to use rich informations on pi p total cross sections below N=10 GeV in order to investig...
AbstractWe prove a general identity for a F23 hypergeometric function over a finite field Fq, where ...
AbstractIn this paper, we deal with a class of pseudoparabolic problems with integral boundary condi...