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      Particle Production in Strong Electromagnetic Fields in Relativistic Heavy-Ion Collisions

      Advances in High Energy Physics
      Hindawi Limited

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          Abstract

          I review the origin and properties of electromagnetic fields produced in heavy-ion collisions. The field strength immediately after a collision is proportional to the collision energy and reaches ~mπ2at RHIC and ~10mπ2at LHC. I demonstrate by explicit analytical calculation that after dropping by about one-two orders of magnitude during the first fm/c of plasma expansion, it freezes out and lasts for as long as quark-gluon plasma lives as a consequence of finite electrical conductivity of the plasma. Magnetic field breaks spherical symmetry in the direction perpendicular to the reaction plane, and therefore all kinetic coefficients are anisotropic. I examine viscosity of QGP and show that magnetic field induces azimuthal anisotropy on plasma flow even in spherically symmetric geometry. Very strong electromagnetic field has an important impact on particle production. I discuss the problem of energy loss and polarization of fast fermions due to synchrotron radiation, consider photon decay induced by magnetic field, elucidateJ/ψdissociation via Lorentz ionization mechanism, and examine electromagnetic radiation by plasma. I conclude thatallprocesses in QGP are affected by strong electromagnetic field and call for experimental investigation.

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          Spontaneously Growing Transverse Waves in a Plasma Due to an Anisotropic Velocity Distribution

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            The order of the quantum chromodynamics transition predicted by the standard model of particle physics

            We determine the nature of the QCD transition using lattice calculations for physical quark masses. Susceptibilities are extrapolated to vanishing lattice spacing for three physical volumes, the smallest and largest of which differ by a factor of five. This ensures that a true transition should result in a dramatic increase of the susceptibilities.No such behaviour is observed: our finite-size scaling analysis shows that the finite-temperature QCD transition in the hot early Universe was not a real phase transition, but an analytic crossover (involving a rapid change, as opposed to a jump, as the temperature varied). As such, it will be difficult to find experimental evidence of this transition from astronomical observations.
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              J/ψ suppression by quark-gluon plasma formation

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                Author and article information

                Journal
                Advances in High Energy Physics
                Advances in High Energy Physics
                Hindawi Limited
                1687-7357
                1687-7365
                2013
                2013
                : 2013
                :
                : 1-34
                Article
                10.1155/2013/490495
                e5144e2a-66d3-4dba-9c26-e869a5bc9940
                © 2013

                http://creativecommons.org/licenses/by/3.0/

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