5 research outputs found
HOT SCALAR ELECTRODYNAMICS AS A TOY MODEL FOR HOT QCD
Hot scalar electrodynamics is adopted as a toy model for a hot gluon plasma
to display some aspects of the compulsory resummation of hard thermal loops
when next-to-leading order quantities at soft momentum scales are to be
calculated. [Talk given by A.K.R. at a one-day meeting dedicated to the memory
of Tanguy ALTHERR, held on November 4, 1994 at CERN, Geneva. To appear in a
Gedenkschrift published by World Scientific.]Comment: 11 pages, LaTeX, uses epsf.sty, 1 uuencoded postscript figur
Hard thermal loops and the entropy of supersymmetric Yang-Mills theories
We apply the previously proposed scheme of approximately self-consistent
hard-thermal-loop resummations in the entropy of high-temperature QCD to N=4
supersymmetric Yang-Mills (SYM) theories and compare with a (uniquely
determined) R[4,4] Pad\'e approximant that interpolates accurately between the
known perturbative result and the next-to-leading order strong-coupling result
obtained from AdS/CFT correspondence. We find good agreement up to couplings
where the entropy has dropped to about 85% of the Stefan-Boltzmann value. This
is precisely the regime which in purely gluonic QCD corresponds to temperatures
above 2.5 times the deconfinement temperature and for which this method of
hard-thermal-loop resummation has given similar good agreement with lattice QCD
results. This suggests that in this regime the entropy of both QCD and N=4 SYM
is dominated by effectively weakly coupled hard-thermal-loop quasiparticle
degrees of freedom. In N=4 SYM, strong-coupling contributions to the
thermodynamic potential take over when the entropy drops below 85% of the
Stefan-Boltzmann value.Comment: 14 pages, 2 figures, JHEP3. v2: revised and expanded, with unchanged
HTL results but corrected NLO strong-coupling result from AdS/CFT (which is
incorrectly reproduced in almost all previous papers comparing weak and
strong coupling results of N=4 SYM) and novel (unique) Pade approximant
interpolating between weak and strong coupling result