On the role of magnetic field in photon excess in heavy ion collisions
arXiv:1406.5097 · doi:10.1103/PhysRevC.91.014902
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.
9 pages, 3 figures
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Cited by in corpus (18)
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- Photon polarization tensor in a magnetized plasma: Absorptive part
- Photon production and elliptic flow from momentum-anisotropic quark-gluon plasma
- Polarization tensor of magnetized quark-gluon plasma at nonzero baryon density
- Gluon polarization tensor and dispersion relation in a weakly magnetized medium
- Gluon polarization tensor in a magnetized medium: Analytic approach starting from the sum over Landau levels
- Anisotropic photon emission from gluon fusion and splitting in a strong magnetic background I: The two-gluon one-photon vertex
- Synchrotron radiation by slowly rotating fermions
- Synchrotron contribution to photon emission from quark-gluon plasma
- Electromagnetic radiation at extreme angular velocity
- Photon and dilepton emission anisotropy for a magnetized quark-gluon plasma
- Scalar boson emission from a magnetized relativistic plasma
- Phenomenology of collinear photon emission from quark-gluon plasma in collisions
- Two-gluon one-photon vertex in a magnetic field and its explicit one-loop approximation in the intermediate field strength regime
- Rotating synchrotron radiation: Photon emission from magnetized and rotating quark-gluon plasma