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By Thomas James Dolan

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On the other hand, a reason of shift can be an interference term in the total Bs cross-section that was not taken into account. And if an IP is heavy or ultrarelativistic, the expected value of shift should be small due to the smallness of the interference summand in these cases. For an ultrarelativistic IP the theory results in an additional possibility of interest: the value of shift of the Bs frequency maximum relative to the potential of ionization of a corresponding atomic subshell sharply depends on the angle of photon emission, which is caused by essentially different patterns of the static and polarization Bs channels in the ultrarelativistic case.

F ðiÞ. Otherwise in these expressions it is necessary to take into account the line width for corresponding transitions. It is well seen that the obtained expression for the PBs amplitude (Eq. 30) corresponds to its interpretation as a process of scattering of the incident particle eigenfield by atomic electrons to a bremsstrahlung photon. Now let us calculate the amplitude of static (ordinary) bremsstrahlung (due to emission of a photon by an incident particle) taking into account possible excitation of atomic electrons.

55 and the relation ai ðoÞ ! a1 ðoÞ ¼ ÀN e2 m o2 to estimate the spectral PBs cross-section in a high-frequency range, we find for three spectral 34 2 Quantum-Electrodynamics Approach to Description of Bremsstrahlung. . Fig. u. 1 rel. u. 58) are low-sensitive to a specific type of nucleus screening by atomic electrons. 51) since in this frequency range the dipole approximation for interaction of an IP with an atomic core (and especially with a photon) is still true. 57) is presented in Fig. 2 for two values of the relativistic factor g.

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