Baryonic Spectral Functions at Finite Temperature - Physics

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Result for PS channel (η c ) at Finite T η c (p = 0) also disappears between 1.62T c and 1.70T c Asakawa and Hatsuda, PRL 2004 M. Asakawa (Osaka University)
Importance of Understanding Baryons @Finite T Success of Recombination @RHIC v 2 ⎛ p p ⎜ ⎞ 3v ⎛ ⎞ 2 ⎟ ∼ ⎜ 3 ⎟ ⎝ ⎠ ⎝ ⎠ ( p ) ∼ v and v ( p ) M p t B p t 2 t 2 2 t 2 ( x) n 1+ ∼1+ nx • v 2M (p TM ) : v 2 B (p TB ) ~ 2 : 3 for p TM : p T B = 2 : 3 φ dN ⎛ i dN ⎞ = N i2 i0 1 + 2v1cos( − 0) + 2v2 cos 2( − 0) + dydϕ⎜dydϕd p ⎜⎝ ⎠⎟ T ( ϕ ϕ ϕ ϕ ) M. Asakawa (Osaka University)
Page 1 and 2: Baryonic Spectral Functions at Fini
Page 3 and 4: Hadrons above Tc? Hadrons above T c
Page 5 and 6: Photon and Dilepton production rate
Page 7 and 8: QGP is strongly coupled, but... D
Page 9 and 10: Spectral Functions above T c m~m s
Page 11: J/ψ non-dissociation above T c Lat
Page 15 and 16: Baryon Operators • Nucleon curren
Page 17 and 18: Lattice Parameters 1. Lattice Sizes
Page 19 and 20: Stat. and Syst. Error Analyses in M
Page 21 and 22: Below T c : Charm Baryon ccc baryon
Page 23 and 24: @Higher T only symmetric and equall
Page 25 and 26: @Higher T only symmetric and equall
Page 27 and 28: Statistical Analysis: Charm Baryon
Page 29 and 30: Scattering Term (two body case) m 1
Page 31 and 32: Negative parity: a possible interpr
Page 33 and 34: QCD Phase Diagram Quark-antiquark c

Baryonic Spectral Functions at Finite Temperature - Physics

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