7–12 Sept 2014
St. Petersburg
Europe/Moscow timezone

Session

Parallel IV: D4 Deconfinement

5
9 Sept 2014, 16:30
St. Petersburg

St. Petersburg

Conveners

Parallel IV: D4 Deconfinement: Strong Magnetic Fields + ...

  • Peter Arnold (University of Virginia)

Presentation materials

There are no materials yet.

  1. Prof. Gunnar Bali (University of Regensburg)
    09/09/2014, 16:30
    Section D: Deconfinement
    We present recent lattice results of magnetic properties of QCD matter obtained with 1+1+1 sea quarks at physical mass and several lattice spacings at zero and at non-zero temperatures. The results include the phase diagram, the magnetization and the equation of state.
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  2. Prof. Domènec Espriu (ICCUB - Universitat de Barcelona)
    09/09/2014, 17:00
    Section D: Deconfinement
    We investigate how local parity breaking due to fluctuations of the topological charge may affect hadron physics in heavy ion collisions. A distorted dispersion relation is derived for the lightest vector mesons ρ and ω and compared to the experimental results. The main characteristic of LPB is an invariant mass splitting that depends on the polarization. We present a detailed analysis of the...
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  3. Mr Kei Suzuki (Tokyo Institute of Technology)
    09/09/2014, 17:20
    Section D: Deconfinement
    Quantum chromodynamics (QCD) in strong magnetic field is one of the most exciting topic in hadron physics. Especially, one can expect that hadrons are modified by strong magnetic fields such as that produced in ultrarelativistic heavy-ion collisions. In this study, we investigate the properties of the heavy-light (D) meson in magnetic field. QCD sum rule (QCDSR) is a method to investigate the...
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  4. Sergey Bondarenko (Ariel University)
    09/09/2014, 17:40
    Section D: Deconfinement
    In our work we consider calculations of distribution function of the charged droplet in the electric field of another, relativistically moving charged drop. Namely, we consider rotating charged droplet in transverse plane which was created during the very first stage of interaction of two neutral objects in high-energy scattering. Due the small droplet's size, the thermalization of this...
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