Abstract
AbstractThe paper presents the low temperature expansion of the 2D Ising model in the presence of the magnetic field in powers of $$x=\exp (-J/(kT))$$
x
=
exp
(
-
J
/
(
k
T
)
)
and $$z=\exp (B/(kT))$$
z
=
exp
(
B
/
(
k
T
)
)
with full polynomials in z up to $$x^{88}$$
x
88
and full polynomials in $$x^4$$
x
4
up to $$z^{-60}$$
z
-
60
, in the latter case the polynomials are explicitly given. The new result presented in the paper is an expansion not in inverse powers of z but in $$(z^2+x^8)^{-k}$$
(
z
2
+
x
8
)
-
k
where the subsequent coefficients (polynomials in $$x^4$$
x
4
) turn out to be divisible by increasing powers of $$(1-x^4)$$
(
1
-
x
4
)
. This result gives a hint about the intriguing ‘off-diagonal’ correlations in the Ising model mixing the $$B\ne 0$$
B
≠
0
contributions with the usual low temperature $$B=0$$
B
=
0
expansion what may be useful on the road to find the full analytic expression for the partition function of the Ising model with non-vanishing magnetic field. The paper describes both the analytic expansions of the partition function and the efficient combinatorial methods to get the coefficients of the expansion.
Publisher
Springer Science and Business Media LLC
Subject
Mathematical Physics,Statistical and Nonlinear Physics
Reference10 articles.
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