Roberge-Weiss phase transition and its endpoint
arXiv:0904.0925 · doi:10.1088/0954-3899/36/11/115010
Abstract
The Roberge-Weiss (RW) phase transition in the imaginary chemical potential region is analyzed by the Polyakov-loop extended Nambu--Jona-Lasinio (PNJL) model. In the RW phase transition, the charge-conjugation symmetry is spontaneously broken, while the extended Z3 symmetry (the RW periodicity) is preserved. The RW transition is of second order at the endpoint. At the zero chemical potential, a crossover deconfinement transition appears as a remnant of the second-order RW phase transition at the endpoint, while the charge-conjugation symmetry is always preserved.
24 pages, 19 figures. Journal version. Some sentences have been revised and added. Fig. 9 has been revised. (New panels have been added.)
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Cited by in corpus (45)
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- Entanglement between deconfinement transition and chiral symmetry restoration
- The order of the Roberge-Weiss endpoint (finite size transition) in QCD
- The critical line of two-flavor QCD at finite isospin or baryon densities from imaginary chemical potentials
- The Roberge-Weiss endpoint in N_f = 2 QCD
- Imaginary Chemical Potential Approach for the Pseudo-Critical Line in the QCD Phase Diagram with Clover-Improved Wilson Fermions
- Roberge-Weiss endpoint at the physical point of QCD
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