Speaker
Dr
Kouji Kashiwa
(Yukawa Institute for Theoretical Physics, Kyoto University)
Description
We propose a new determination of the confinement-deconfinement transition by using the imaginary chemical potential. The imaginary chemical potential can be interpreted as the Aharonov-Bohm phase and then an analogy of the topological-order suggests that the Roberge-Weiss endpoint would define the deconfinement temperature. Based on the topological property, we can construct a new quantity which describes the confinement-deconfinement transition. This quantity is defined as the integral of the quark number susceptibility along the closed loop of $\theta$ where $\theta$ is the dimensionless imaginary chemical potential. Expected behavior of it at finite temperature is discussed and its asymptotic behaviors are shown.
Primary author
Dr
Kouji Kashiwa
(Yukawa Institute for Theoretical Physics, Kyoto University)
Co-author
Prof.
Akira Ohnishi
(Yukawa Institute for Theoretical Physics, Kyoto University)