Exact renormalization group at finite temperature

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THE TWO-LOOP ENTROPY -effectively a one-loop expression; residual interactions start at order three-loop -manifestly ultraviolet finite -perturbatively correct up to order g 3
State of the art pure-glue SU(3) Yang-Mills theory • J.-P. B., E. Iancu, A. Rebhan: Phys.Rev.D63:065003,2001 • G. Boyd et al., Nucl. Phys. B469, 419 (1996). from J.-P. B., E. Iancu, A. Rebhan: Nucl.Phys.A698:404-407,2002
Page 1 and 2: Exact renormalisation group at fini
Page 3 and 4: Hot QCD
Page 5 and 6: Pressure for SU(3) YM theory at (ve
Page 7 and 8: Weak coupling techniques (non pertu
Page 9 and 10: Similar difficulty in scalar theory
Page 12 and 13: Skeleton expansion Phi-derivable ap
Page 16 and 17: Large N f
Page 18 and 19: Entropy in large N f Good agreement
Page 20: Leading order correction S S 0 = 3
Page 23 and 24: Scales, fluctuations and degrees of
Page 25 and 26: Non perturbative renormalization gr
Page 27 and 28: Beyond the local potential approxim
Page 30 and 31: Flow of coupling constant (LPA) wea
Page 33 and 34: Pressure versus m/T g^3 g^3 g^4 g^4
Page 35: Summary •While strict perturbatio

Exact renormalization group at finite temperature

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