Finite size effects in euclidean lattice thermodynamics for non-interacting Bose and Fermi systems

Engels J, Karsch F, Satz H (1982)
Nuclear Physics, B 205(2): 239-252.

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Zeitschriftenaufsatz | Veröffentlicht | Englisch
Abstract / Bemerkung
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 non-interacting 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.
Erscheinungsjahr
Zeitschriftentitel
Nuclear Physics, B
Band
205
Zeitschriftennummer
2
Seite
239-252
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PUB-ID

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Engels J, Karsch F, Satz H. Finite size effects in euclidean lattice thermodynamics for non-interacting Bose and Fermi systems. Nuclear Physics, B. 1982;205(2):239-252.
Engels, J., Karsch, F., & Satz, H. (1982). Finite size effects in euclidean lattice thermodynamics for non-interacting Bose and Fermi systems. Nuclear Physics, B, 205(2), 239-252. doi:10.1016/0550-3213(82)90387-X
Engels, J., Karsch, F., and Satz, H. (1982). Finite size effects in euclidean lattice thermodynamics for non-interacting Bose and Fermi systems. Nuclear Physics, B 205, 239-252.
Engels, J., Karsch, F., & Satz, H., 1982. Finite size effects in euclidean lattice thermodynamics for non-interacting Bose and Fermi systems. Nuclear Physics, B, 205(2), p 239-252.
J. Engels, F. Karsch, and H. Satz, “Finite size effects in euclidean lattice thermodynamics for non-interacting Bose and Fermi systems”, Nuclear Physics, B, vol. 205, 1982, pp. 239-252.
Engels, J., Karsch, F., Satz, H.: Finite size effects in euclidean lattice thermodynamics for non-interacting Bose and Fermi systems. Nuclear Physics, B. 205, 239-252 (1982).
Engels, Jürgen, Karsch, Frithjof, and Satz, Helmut. “Finite size effects in euclidean lattice thermodynamics for non-interacting Bose and Fermi systems”. Nuclear Physics, B 205.2 (1982): 239-252.
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