On the role of magnetic field in photon excess in heavy ion collisions
Kirill Tuchin

TL;DR
This paper investigates how magnetic fields influence the excess of photons observed in heavy-ion collisions, attributing a significant part of the excess to synchrotron radiation and analyzing its anisotropic properties.
Contribution
It provides a detailed calculation of synchrotron photon spectra considering realistic magnetic field structures in heavy-ion collisions, highlighting their role in photon excess.
Findings
Synchrotron radiation accounts for a significant photon excess at 1-3 GeV.
The azimuthal anisotropy coefficients are v2=4/7 and v4=1/10, independent of photon momentum and centrality.
Magnetic field effects are crucial in understanding photon production in heavy-ion collisions.
Abstract
Synchrotron photon spectrum in heavy-ion collisions is computed taking into account the spatial and temporal structure of magnetic field. It is found that a significant fraction of photon excess in heavy-ion collisions in the region GeV can be attributed to the synchrotron radiation. Azimuthal anisotropy of the synchrotron photon spectrum is characterized by the Fourier coefficients and that are independent of photon momentum and centrality.
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