2015
DOI: 10.1088/1742-5468/2015/07/p07004
|View full text |Cite
|
Sign up to set email alerts
|

The hypergeometric series for the partition function of the 2D Ising model

Abstract: Abstract. In 1944 Onsager published the formula for the partition function of the Ising model for the infinite square lattice. He was able to express the internal energy in terms of a special function, but he left the free energy as a definite integral. Seven decades later, the partition function and free energy have yet to be written in closed form, even with the aid of special functions. Here we evaluate the definite integral explicitly, using hypergeometric series. Let β denote the reciprocal temperature, J… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
1

Citation Types

0
21
0

Year Published

2015
2015
2021
2021

Publication Types

Select...
5

Relationship

1
4

Authors

Journals

citations
Cited by 10 publications
(21 citation statements)
references
References 46 publications
0
21
0
Order By: Relevance
“…We see that, in contrast to the low-temperature expansion, a simple rational function like χ (1) H yielding polynomial expressions modulo 2, 4, 8, 16, 32 cannot give rise to the emergence of lacunary series like (35) and (37). For high-temperature series, one must therefore rather ask whether, modulo 2 r , one can distinguish between the full susceptibility χ H and χ (1)…”
Section: The High-temperature Susceptibilitymentioning
confidence: 90%
See 4 more Smart Citations
“…We see that, in contrast to the low-temperature expansion, a simple rational function like χ (1) H yielding polynomial expressions modulo 2, 4, 8, 16, 32 cannot give rise to the emergence of lacunary series like (35) and (37). For high-temperature series, one must therefore rather ask whether, modulo 2 r , one can distinguish between the full susceptibility χ H and χ (1)…”
Section: The High-temperature Susceptibilitymentioning
confidence: 90%
“…and χ As must be the case, the coefficients are the same up to v 14 for the low-temperature series, and up to v 8 for the high-temperature series, and, beyond, the ratio of the coefficients for χ L (v) and χ (2) L (v) (resp. χ H (v) and χ (1) H (v)) are very close to 1. For the low-temperature series expansion the difference between χ L (v) and χ…”
mentioning
confidence: 81%
See 3 more Smart Citations