scholarly journals DiPerna–Lions Flow for Relativistic Particles in an Electromagnetic Field

2015 ◽  
Vol 217 (3) ◽  
pp. 1029-1067 ◽  
Author(s):  
P.-E. Jabin ◽  
N. Masmoudi
2013 ◽  
Vol 10 (08) ◽  
pp. 1360007 ◽  
Author(s):  
ANNA MARIA CANDELA ◽  
ALFONSO ROMERO ◽  
MIGUEL SÁNCHEZ

The second-order differential equation [Formula: see text] on a Lorentzian manifold describes, in particular, the dynamics of particles under the action of an electromagnetic field F and a conservative force -∇V. We provide a first study on the extendability of its solutions, by imposing some natural assumptions.


1999 ◽  
Vol 14 (10n11) ◽  
pp. 709-720 ◽  
Author(s):  
A. A. DERIGLAZOV ◽  
D. M. GITMAN

We consider a possibility of describing spin one-half and higher spins of massive relativistic particles by means of commuting spinors. We present two classical gauge models with the variables xμ, ξα, χα, where ξ, χ are commuting Majorana spinors. In the course of quantization both models reproduce Dirac equation. We analyze the possibility of introducing an interaction with an external electromagnetic background into the models and generalizing them to higher spin description. The first model admits a minimal interaction with the external electromagnetic field, but leads to reducible representations of the Poincaré group being generalized for higher spins. The second model turns out to be appropriate for description of the massive higher spins. However, it seems to be difficult to introduce a minimal interaction with an external electromagnetic field into this model. We compare our approach with one, which uses Grassmann variables, and establish a relation between them.


2015 ◽  
Vol 1084 ◽  
pp. 138-146 ◽  
Author(s):  
Gennady A. Naumenko

The formalism of form factors is the basis for the describing the coherent radiation of bunches that comprise relativistic charged particles. The general theory of coherent radiation for synchrotron and bremsstrahlung radiation, when radiation is generated directly by charged particles, but not by the material of a target, was developed long ago. However, there is no general model of coherent radiation for such polarization radiation as transition, diffraction and other types of radiation, when the radiation is generated by the material of a target polarized by the electromagnetic field of relativistic particles. This often causes the misapplication of the form factors of synchrotron radiation to other types of radiation. In this paper, we suggest the simplified algorithm for construction of form factors for different types of polarization radiation of relativistic electrons in the material of a target.


1972 ◽  
Vol 27 (2) ◽  
pp. 339-362
Author(s):  
Wolfgang Ulrici

AbstractStarting with the equations of the center-of-mass motion and spin motion of a particle in a homogeneous electromagnetic field, we derive the Hamiltonian and the wave equation of a relativistic particle with arbitrary spin and arbitrary magnetic moment in this field. We change from the canonical representation to spinor representations with convenient transformation properties, and we find a form of the wave equation which, for the special case of spin 1/2, coincides with the Dirac equation (in the form first given by Feynman). The problems and limitations of this derivation are extensively discussed.


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