Synchrotron radiation of a magnetic moment in classical electrodynamics

1982 ◽  
Vol 25 (2) ◽  
pp. 83-87 ◽  
Author(s):  
I. M. Ternov ◽  
V. A. Bordovitsyn ◽  
G. K. Razina
2010 ◽  
Vol 25 (supp01) ◽  
pp. 128-135 ◽  
Author(s):  
HIDEO NITTA

Radiations from a crystal irradiated with relativistic charged particles are reviewed with the emphasis on their fundamental processes. As their "compound processes" diffraction of both channeling radiation and coherent bremsstrahlung are considered. Coherent polarization radiation from neutral particles with magnetic moment is discussed within the framework of classical electrodynamics.


1990 ◽  
Vol 33 (6) ◽  
pp. 478-481
Author(s):  
I. M. Ternov ◽  
V. A. Bordovitsyn ◽  
V. Ya. �pp

1994 ◽  
Vol 09 (26) ◽  
pp. 4581-4600 ◽  
Author(s):  
ALEXANDER V. KURILIN

We calculate the probabilities of slepton and photino production via a charged lepton decay induced by an arbitrary electromagnetic wave or by a constant homogeneous external field, Fμν. This allows us to estimate the domains where this reaction could be significant. Comparing the process [Formula: see text] with the synchrotron radiation we conclude that for all values of the background field parameter [Formula: see text], with pν being the lepton’s momentum, the following estimate holds: [Formula: see text]. We also study the impact of the intense field on radiative corrections to the lepton’s anomalous magnetic moment. It is found that, when χ exceeds the cube of the masses’ ratios, [Formula: see text], [Formula: see text], the sparticle’s contribution to the anomalous magnetic moment is of the same order as the QED correction. In this region the magnitude of the anomalous magnetic moment of the lepton is very sensitive to the masses of the slepton and the photino.


1950 ◽  
Vol 28a (3) ◽  
pp. 336-338
Author(s):  
F. A. Kaempffer

It is shown that not only the rest-mass of the electron but its spin as well is carried by the surrounding electromagnetic field. The ratio of magnetic moment and angular momentum (g-factor) of the electron is determined. The law of conservation of angular momentum is checked.


Symmetry ◽  
2020 ◽  
Vol 12 (7) ◽  
pp. 1095
Author(s):  
Vladislav Bagrov ◽  
Anna Kasatkina ◽  
Alexey Pecheritsyn

An exact analytical expression for the effective angle is determined for an arbitrary energy value of a radiating particle. An effective angle of instantaneous power is defined for synchrotron radiation in the framework of classical electrodynamics. This definition explicitly contains the most symmetric distribution of half the total of the instantaneous power of synchrotron radiation. Two exact analytical expressions for the effective angle are considered for the arbitrary energy values of a radiating particle, and the second expression brings to light the exact asymptotics of the effective angle in the ultrarelativistic limit.


1974 ◽  
Vol 10 (2) ◽  
pp. 517-525 ◽  
Author(s):  
Antonio F. Rañada ◽  
Manuel F. Rañada ◽  
Mario Soler ◽  
Luis Vázquez

1990 ◽  
Vol 33 (5) ◽  
pp. 420-422 ◽  
Author(s):  
I. M. Ternov ◽  
V. A. Bordovitsyn ◽  
V. Ya. �pp

Author(s):  
B. Jouffrey ◽  
D. Dorignac ◽  
A. Bourret

Since the early works on GP zones and the model independently proposed by Preston and Guinier on the first steps of precipitation in supersaturated solid solution of aluminium containing a few percent of copper, many works have been performed to understand the structure of different stages in the sequence of precipitation.The scheme which is generally admitted can be drawn from a work by Phillips.In their original model Guinier and Preston analysed a GP zone as composed of a single (100) copperrich plane surrounded by aluminum atomic planes with a slightly shorter distance from the original plane than in the solid solution.From X-ray measurements it has also been shown that GP1 zones were not only copper monolayer zones. They could be up to a few atomic planes thick. Different models were proposed by Guinier, Gerold, Toman. Using synchrotron radiation, proposals have been recently made.


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