1982
DOI: 10.1016/0550-3213(82)90387-x
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Finite size effects in euclidean lattice thermodynamics for non-interacting bose and fermi systems

Abstract: In the Monte Carlo simulation of QCD, the euclidean form of the partition function is evaluated on a finite lattice. We use this method to calculate the partition function for noninteracting Bose and Fermi fields. Here the expressions on the lattice can be evaluated in closed form and the continuum limit is well-known; this provides us with a measure for finite lattice size effects in such approaches.

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Cited by 118 publications
(71 citation statements)
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“…One simple exercise consists of calculating the pressure of a free massless boson on the lattice, and comparing it with the continuum Stefan-Boltzmann law [16]. An instructive figure can be found in Fig.…”
Section: Discussionmentioning
confidence: 99%
“…One simple exercise consists of calculating the pressure of a free massless boson on the lattice, and comparing it with the continuum Stefan-Boltzmann law [16]. An instructive figure can be found in Fig.…”
Section: Discussionmentioning
confidence: 99%
“…It is well known that this introduces severe problems in thermodynamic calculations, which in the past made a direct determination of the physics in the continuum limit difficult. Already the thermodynamics of free Bose (gluon) or Fermi (quark) gases deviates strongly from the continuum ideal gas results when calculated on coarse Euclidean lattices [2]. This problem carries over to QCD, where bulk thermodynamic observables like energy density and pressure do rapidly come close to the non-interacting ideal gas limit above the deconfinement phase transition.…”
Section: Introductionmentioning
confidence: 95%
“…We provide here a detailed analysis of mesonic spectral functions in the infinite temperature limit and discuss their cut-off dependence. This provides a basis for discussions of the cut-off dependence of spectral functions at finite temperature and is similar in spirit to studies of the cut-off dependence of the QCD equation of state which have first been performed in the ideal gas (infinite temperature) limit [1].…”
Section: Introductionmentioning
confidence: 99%