15.–18. Sept. 2025
University of Ioannina - Conference Center "Karolos Papoulias"
Europe/Berlin Zeitzone

Depolarization of Radiation of High Energy Electron Bunch in a Strong Magnetic Field

18.09.2025, 10:20
20m
University of Ioannina - Conference Center "Karolos Papoulias"

University of Ioannina - Conference Center "Karolos Papoulias"

Talk Session 9

Sprecher

Oleksandr Novak (The Institute of Applied Physics NAS of Ukraine)

Beschreibung

Synchotron radiation is widely used to generate intense beams of hard photons [1]. Of particular intrest is the case of electron propagation in a strong magnetic field comparable to the critical Schwinger field, $H_c \approx 4.41 \cdot 10^{13}$ G. In this regime, rapid radiative self-polarization, accompanied by intense emission, is expected to occur on a timescale of femtoseconds. Recently, the generation of a strong magnetic field of approximately $4 \cdot 10^{9}$ G has been proposed via the collision of a dense high-energy electron bunch with a solid target at a grazing angle [2,3].

In this contibution, we perform simulation of propagation of an bunch electron in a strong uniform magnetic field. Energy loss due to radiation and the consequent emission of multiple photons are taken into account. We numerically solve the balance equation to determine the time evolution of the spin-resolved energy distribution of the electron beam. This, in turn, allows us to evaluate the polarization of the emitted radiation as a function of time and photon energy.

We consider the dependence of radiation polarization on the dimensionless parameter $\varepsilon = (E/mc^2)(H/H_c)$, where $E$ is the electron energy and $H$ is the magnetic field strength. For $\varepsilon \ll 1$, we reproduce the well-known result that radiation is predominantly polarized perpendicular to the magnetic field [4]. However, when $\varepsilon \gg 1$, the spectral maximum shifts toward the emission of high-energy photons, resulting in a substantial decrease in radiation polarization. The most notable case arises for electrons with spins aligned parallel to the magnetic field. In this regime, significant or nearly complete depolarization of the synchrotron radiation is observed.

References
[1] François Méot, Haixin Huang, Vadim Ptitsyn, Fanglei Lin. Polarized Beam Dynamics and Instrumentation in Particle Accelerators // USPAS Summer 2021 Spin Class Lectures. Springer, 2021.
[2] Xing-Long Zhu et al., Efficient generation of collimated multi-GeV gamma-rays along solid surfaces. Optica, 2023, Vol. 10, No. 1, p. 118.
[3] Xing-Long Zhu et al., Generation of relativistic polarized electron beams via collective beam-target interactions. arXiv:2408.05768.
[4] A.A. Sokolov, I.M. Ternov. Radiation from relativistic electrons. New York: American Institute of Physics, 1986, 312 p.

Autoren

Mykhailo Diachenko (Institute of Applied Physics, National Academy of Sciences of Ukraine) Oleksandr Novak (The Institute of Applied Physics NAS of Ukraine)

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