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							2009Volume 116Issue 6 Pages
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							2009Volume 116Issue 6 Pages
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							2009Volume 116Issue 6 Pages
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							2009Volume 116Issue 6 Pages
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							2009Volume 116Issue 6 Pages
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							2009Volume 116Issue 6 Pages
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							2009Volume 116Issue 6 Pages
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							2009Volume 116Issue 6 Pages
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M. Asakawa, S.A. Bass, B. Mueller, C. Nonaka
						
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							2009Volume 116Issue 6 Pages
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									The presence of a critical point in the QCD phase diagram can deform the trajectories describing the evolution of the expanding fireball in the μ_B-T phase diagram. If the average emission time of hadrons is a function of transverse velocity, as microscopic simulations of the hadronic freezeout dynamics suggest, the deformation of the hydrodynamic trajectories will change the transverse velocity (β_T) dependence of the proton-antiproton ratio when the fireball passes in the vicinity of the critical point. An unusual β_T-dependence of the p^^-/p ratio in a narrow beam energy window would thus signal the presence of the critical point.
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							2009Volume 116Issue 6 Pages
									F39-F41
								
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							2009Volume 116Issue 6 Pages
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							2009Volume 116Issue 6 Pages
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							2009Volume 116Issue 6 Pages
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							2009Volume 116Issue 6 Pages
									F50-F51
								
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Kenji Hotta
						
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							2009Volume 116Issue 6 Pages
									F52-F54
								
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									Atick and Witten have proposed the Hagedorn transition of closed strings via condensation of winding tachyon. But we have not known the stable minimum of this tachyon potential yet. On the other hand, we have previously shown that a phase transition occurs near the Hagedorn temperature and D9-brane-<D9>^^^-brane pairs become stable. We present a conjecture that D9-brane-<D9>^^^-brane pairs are created by the Hagedorn transition of closed strings. We will show some circumstantial evidences for this conjecture.
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							2009Volume 116Issue 6 Pages
									F55-F62
								
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Kenji Maeda, Gordon Baym, Tetsuo Hatsuda
						
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							2009Volume 116Issue 6 Pages
									F63-F65
								
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							2009Volume 116Issue 6 Pages
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							2009Volume 116Issue 6 Pages
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Yoshiya Yamanaka, Masahiko Okumura, Makoto Mine, Tomoka Sunaga, Yusuke ...
						
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							2009Volume 116Issue 6 Pages
									F75-F77
								
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							2009Volume 116Issue 6 Pages
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							2009Volume 116Issue 6 Pages
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							2009Volume 116Issue 6 Pages
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							2009Volume 116Issue 6 Pages
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							2009Volume 116Issue 6 Pages
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Kohtaroh Miura, Noboru Kawamoto, Akira Ohnishi
						
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							2009Volume 116Issue 6 Pages
									F96-F98
								
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									We investigate the phase diagram evolution with the finite coupling 1/g^2 in the color SU(N_c=3) strong coupling lattice QCD with one species of staggered fermions at finite quark chemical potential (μ) and finite temperature (T). We evaluate the next to leading order of the strong coupling expansion, and obtain the following results: (1) The ratio of the critical value (μ_c/T_c)becomes closer to the empirical value. (2) As the coupling decreases, the second order transition on the T axis evolves to the first order, and T_c is found to be consistent with lattice Monte-Carlo simulations. (3) The "Partially Chiral Restored Phase" appears in low temperature and high density region.
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									F99-F106
								
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							2009Volume 116Issue 6 Pages
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							2009Volume 116Issue 6 Pages
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							2009Volume 116Issue 6 Pages
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							2009Volume 116Issue 6 Pages
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[in Japanese], [in Japanese], [in Japanese], Gernot Akemann
						
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							2009Volume 116Issue 6 Pages
									F119-F121
								
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							2009Volume 116Issue 6 Pages
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H. Kouno, Y. Sakai, K. Kashiwa, M. Matsuzaki, M. Yahiro
						
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							2009Volume 116Issue 6 Pages
									F125-F127
								
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									Using the Polyakov extended Nambu-Jona-Lasinio (PNJL) model with imaginary chemical potential, the relation between the Roberge-Weiss (RW) phase transition and the extended Z_3 symmetry is studied. At low temperature, there is approximate continuous symmetry under the phase transformation of the Polyakov loop with the shift of the imaginary chemical potential. Due to this continuous symmetry, the Polyakov loop can oscillate smoothly as the imaginary chemical potential increases. At high temperature, this continuous symmetry is broken to an exact discrete symmetry, the extended Z_3 symmetry, and the Polyakov loop can not oscillate smoothly. This symmetry breaking of the continuous symmetry causes a discontinuity of the Polyakov loop. That is the RW phase transition.
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							2009Volume 116Issue 6 Pages
									F128-F130
								
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							2009Volume 116Issue 6 Pages
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									F137-F138
								
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