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XQCD 2019 (The 17th International Conference on QCD in Extreme Conditions)

24–26 Jun 2019
Bunkyo School Building, Tokyo Campus, University of Tsukuba
Japan timezone

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Session

Session 9

26 Jun 2019, 09:00
122, 134 (Bunkyo School Building, Tokyo Campus, University of Tsukuba)

122, 134

Bunkyo School Building, Tokyo Campus, University of Tsukuba

3-29-1 Otsuka Bunkyo-ku Tokyo 112-0012 Japan

Conveners

Session 9

  • Jens Oluf Andersen (Norwegian University of Science and Technology)

Presentation materials

There are no materials yet.

  1. 16. Lattice with external fields and rotation
    Dr Arata Yamamoto (University of Tokyo)
    26/06/2019, 09:00
    Invited talk
    Extreme environments, such as strong electromagnetic force and fast rotation, induce interesting quantum phenomena. They are relevant both for high energy experiments and for condensed matter experiments. From a theoretical point of view, we need reliable computational frameworks to investigate them. I would like to review such endeavors in lattice gauge theory.
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  2. 6. Conductivity of quark-gluon plasma in the presence of external magnetic field
    Dr Aleksandr Nikolaev (Swansea University)
    26/06/2019, 09:45
    Oral talk
    We examine the electric conductivity of quark-gluon plasma in the presence of external magnetic field B within LQCD formulation for few temperatures in the deconfinement phase. Ensembles are generated with dynamical staggered 2+1 quarks at physical quark masses. At first we measure the electromagnetic current-current Euclidean correlators along and perpendicular to the magnetic field, then...
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  3. 65. The order of phase transition in three flavor QCD with background magnetic field in crossover regime
    Dr Akio Tomiya (RIKEN-BNL)
    26/06/2019, 10:10
    Oral talk
    We investigate the order of phase transition in three flavor QCD with a background U(1) magnetic field using the standard staggered action with the plaquette gauge action. We perform simulations for three volumes $N_\sigma=8,16,24$ with fixed mass $ma=0.030$ and temporal extent $N_\tau=4$, which is expected to show crossover for vanishing magnetic field. We apply physically same magnitude of...
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