Quantum and Classical Radiation Reaction from Lightfront QED

2014 ◽  
Vol 55 (5-7) ◽  
pp. 501-506
Author(s):  
Greger Torgrimsson
1982 ◽  
Vol 26 (10) ◽  
pp. 2707-2712 ◽  
Author(s):  
Arnold Rosenblum ◽  
Ronald E. Kates ◽  
Peter Havas

1978 ◽  
Vol 46 (3) ◽  
pp. 244-248 ◽  
Author(s):  
David J. Griffiths ◽  
Ellen W. Szeto

2016 ◽  
Vol 204 ◽  
pp. 141-151 ◽  
Author(s):  
M. Vranic ◽  
J.L. Martins ◽  
R.A. Fonseca ◽  
L.O. Silva

2019 ◽  
Vol 34 (15) ◽  
pp. 1950077 ◽  
Author(s):  
Janos Polonyi

The Abraham–Lorentz force is a finite remnant of the UV singular structure of the self-interaction of a point charge with its own field. The satisfactory description of such an interaction needs a relativistic regulator. This turns out to be a problematic point because the energy of regulated relativistic cutoff theories is unbounded from below. However, one can construct point-splitting regulators which keep the Abraham–Lorentz force stable. The classical language can be reconciled with QED by pointing out that the effective quantum theory for the electric charge supports a saddle point producing the classical radiation reaction forces.


2008 ◽  
Author(s):  
M. Dorigo ◽  
M. Tessarott ◽  
P. Nicolini ◽  
A. Beklemishev ◽  
Takashi Abe

1977 ◽  
Vol 32 (7) ◽  
pp. 685-691
Author(s):  
W. Heudorfer ◽  
M. Sorg

Abstract Numerical solutions of the recently proposed equations of motion for the classically radiating electron are obtained for the case where the particle moves in a one-dimensional Coulomb potential (both attractive and repulsive). The solutions are discussed and found to be meaningful also in that case, where the well-known Lorentz-Dirac equation fails (attractive Coulomb force). Discrete, stationary states are found in a non-singular version of the Coulomb potential. During the transition between those stationary states the particle looses energy by emission of radiation, which results in a smaller amplitude of the stationary oscillations.


2016 ◽  
Author(s):  
M. Vranic ◽  
T. Grismayer ◽  
J. L. Martins ◽  
R. A. Fonseca ◽  
L. O. Silva

2017 ◽  
Vol 83 (3) ◽  
Author(s):  
B. Manuel Hegelich ◽  
Lance Labun ◽  
Ou Z. Labun

The long-standing challenge to describing charged particle dynamics in strong classical electromagnetic fields is how to incorporate classical radiation, classical radiation reaction and quantized photon emission into a consistent unified framework. The current, semiclassical methods to describe the dynamics of quantum particles in strong classical fields also provide the theoretical framework for fundamental questions in gravity and hadron–hadron collisions, including Hawking radiation, cosmological particle production and thermalization of particles created in heavy-ion collisions. However, as we show, these methods break down for highly relativistic particles propagating in strong fields. They must therefore be improved and adapted for the description of laser–plasma experiments that typically involve the acceleration of electrons. Theory developed from quantum electrodynamics, together with dedicated experimental efforts, offer the best controllable context to establish a robust, experimentally validated foundation for the fundamental theory of quantum effects in strong classical potentials.


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