Non-Lorentzian electromagnetic quadripotentials for the field of a classical point particle

1979 ◽  
Vol 51 (4) ◽  
pp. 532-538
Author(s):  
F. Miglietta
2019 ◽  
Vol 100 (5) ◽  
Author(s):  
K. Kajantie ◽  
Larry D. McLerran ◽  
Risto Paatelainen

2014 ◽  
Vol 90 (3) ◽  
pp. 769-772
Author(s):  
V. A. Malyshev ◽  
S. A. Pirogov

2020 ◽  
Vol 101 (5) ◽  
Author(s):  
K. Kajantie ◽  
Larry D. McLerran ◽  
Risto Paatelainen

2010 ◽  
Vol 32 (3) ◽  
Author(s):  
R De Luca

A two-dimensional annular billiard consisting of a region confined within two concentric circumferences, the outer of radius R and the inner of radius r, is considered. The escape time of a point particle projected at a given angle within this billiard is numerically evaluated in terms of the size of the opening in the billiard. The problem is solved by means of classical mechanics and can be of interest for advanced high school physics students or undergraduate college physics students


1992 ◽  
Vol 07 (32) ◽  
pp. 3023-3028 ◽  
Author(s):  
J.L. MATHEUS-VALLE ◽  
MARCO A.R. MONTEIRO

Following the generalization of the Grassmann Algebra provided by Quantum Groups, we introduce an extension of fermionic coordinates and an action for the classical point particle mechanics which has a symmetry that resembles a supersymmetric transformation.


2008 ◽  
Vol 26 (2) ◽  
pp. 287-294
Author(s):  
O. Keller

AbstractA microscopic eikonal theory based on photon wave mechanics is established. The diamagnetic (solid state) field-plasma interaction is shown to play a central role in the theory, and this interaction enables one to introduce a massive transverse photon concept. This quasi-particle enters the eikonal theory in manner similar to the one in which the classical point particle enters Newtonian Mechanics in the Hamilton-Jacobi formulation. When the spatial fluctuations in the stationary-state plasma density are of importance the microscopic eikonal theory becomes a spatially nonlocal theory, and the nonlocality, originating in the coupling of longitudinal and scalar photons to the massive transverse photon, extends over near-field distances.


2001 ◽  
Vol 79 (6) ◽  
pp. 879-906
Author(s):  
M Mattes ◽  
S Rupp ◽  
M Sorg

The Relativistic Schrödinger Theory (RST) is applied to a system of N particles with electromagnetic interactions. The gauge group is U(1) × U(1)... × U(1). By exploiting the mathematical structure of fibre bundles, the energy-momentum content of the gauge field can be defined in such a way that no infinite self-energy of point charges can arise. However, the picture of classical point particles becomes insufficient in any case in view of the exchange and overlap effects occurring in RST. The presence of overlap currents seems to be necessary to remedy certain pathological features of the classical point-particle theories. PACS Nos.: 03.65Pm, 03.65Ge, 03.65Ta


2021 ◽  
Vol 2021 (3) ◽  
Author(s):  
Colby DeLisle ◽  
Jordan Wilson-Gerow ◽  
Philip Stamp

Abstract Soft factorization has been shown to hold to sub-leading order in QED and to sub-sub-leading order in perturbative quantum gravity, with various loop and non-universal corrections that can be found. Here we show that all terms factorizing at tree level can be uniquely identified as boundary terms that exist already in the classical expressions for the electric current and stress tensor of a point particle. Further, we show that one cannot uniquely identify such boundary terms beyond the sub-leading or sub-sub-leading orders respectively, providing evidence that the factorizability of the tree level soft factor only holds to these orders. Finally, we show that these boundary terms factor out of all tree level amplitudes as expected, in a theory where gravitons couple to a scalar field.


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