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Article type: Cover
2009 Volume 116 Issue 6 Pages
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Article type: Appendix
2009 Volume 116 Issue 6 Pages
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Article type: Appendix
2009 Volume 116 Issue 6 Pages
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2009 Volume 116 Issue 6 Pages
F5-F12
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2009 Volume 116 Issue 6 Pages
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2009 Volume 116 Issue 6 Pages
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2009 Volume 116 Issue 6 Pages
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2009 Volume 116 Issue 6 Pages
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2009 Volume 116 Issue 6 Pages
F30-F32
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2009 Volume 116 Issue 6 Pages
F33-F35
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M. Asakawa, S.A. Bass, B. Mueller, C. Nonaka
Article type: Article
2009 Volume 116 Issue 6 Pages
F36-F38
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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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Article type: Article
2009 Volume 116 Issue 6 Pages
F39-F41
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2009 Volume 116 Issue 6 Pages
F42-F44
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2009 Volume 116 Issue 6 Pages
F45-F47
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2009 Volume 116 Issue 6 Pages
F48-F49
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2009 Volume 116 Issue 6 Pages
F50-F51
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Kenji Hotta
Article type: Article
2009 Volume 116 Issue 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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Article type: Article
2009 Volume 116 Issue 6 Pages
F55-F62
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Kenji Maeda, Gordon Baym, Tetsuo Hatsuda
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2009 Volume 116 Issue 6 Pages
F63-F65
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2009 Volume 116 Issue 6 Pages
F66-F68
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2009 Volume 116 Issue 6 Pages
F69-F71
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2009 Volume 116 Issue 6 Pages
F72-F74
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Yoshiya Yamanaka, Masahiko Okumura, Makoto Mine, Tomoka Sunaga, Yusuke ...
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2009 Volume 116 Issue 6 Pages
F75-F77
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2009 Volume 116 Issue 6 Pages
F78-F80
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Article type: Article
2009 Volume 116 Issue 6 Pages
F81-F83
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2009 Volume 116 Issue 6 Pages
F84-F86
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2009 Volume 116 Issue 6 Pages
F87-F92
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2009 Volume 116 Issue 6 Pages
F93-F95
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Kohtaroh Miura, Noboru Kawamoto, Akira Ohnishi
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2009 Volume 116 Issue 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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2009 Volume 116 Issue 6 Pages
F99-F106
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2009 Volume 116 Issue 6 Pages
F107-F109
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Article type: Article
2009 Volume 116 Issue 6 Pages
F110-F112
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2009 Volume 116 Issue 6 Pages
F113-F115
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2009 Volume 116 Issue 6 Pages
F116-F118
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[in Japanese], [in Japanese], [in Japanese], Gernot Akemann
Article type: Article
2009 Volume 116 Issue 6 Pages
F119-F121
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2009 Volume 116 Issue 6 Pages
F122-F124
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H. Kouno, Y. Sakai, K. Kashiwa, M. Matsuzaki, M. Yahiro
Article type: Article
2009 Volume 116 Issue 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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Article type: Article
2009 Volume 116 Issue 6 Pages
F128-F130
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Article type: Article
2009 Volume 116 Issue 6 Pages
F131-F133
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2009 Volume 116 Issue 6 Pages
F134-F136
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Article type: Appendix
2009 Volume 116 Issue 6 Pages
F137-F138
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Article type: Appendix
2009 Volume 116 Issue 6 Pages
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Article type: Index
2009 Volume 116 Issue 6 Pages
192-193
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Article type: Index
2009 Volume 116 Issue 6 Pages
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Article type: Index
2009 Volume 116 Issue 6 Pages
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Article type: Index
2009 Volume 116 Issue 6 Pages
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Article type: Appendix
2009 Volume 116 Issue 6 Pages
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Article type: Cover
2009 Volume 116 Issue 6 Pages
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2009 Volume 116 Issue 6 Pages
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