A010367 - OEIS

%I #19 Nov 26 2024 18:10:49

%S 2,128,9792,886784,92722944,11014965248,1465369976832,215937597784064,

%T 34916329300783104,6147843514432913408,1170908043876450435072

%N High-temperature spin-1/2 Ising model series for second derivative of susceptibility with respect to magnetic field for hyper-body-centered-cubic lattice.

%C Moore defines two four-dimensional lattices called hbcc ("hyper-body-centered-cubic") and hfcc. They have essentially the same arrangement of sites, up to a similarity transformation. (That set of sites forms the D_4 lattice.) However the sets of bonds are different: each site of hfcc is connected to all 24 of its nearest neighbors, while each site of hbcc is connected only to 16 of them, specifically those which have relative position vector (+-1, +-1, +-1, +-1), but not (+-2, 0, 0, 0) or its permutations. - _Andrey Zabolotskiy_, Nov 26 2024

%H George A. Baker Jr. and John M. Kincaid, <a href="https://doi.org/10.1007/BF01012818">The continuous-spin Ising model, g0:phi4:d field theory and the renormalization group</a>. J. Statist. Phys. 24 (1981), no. 3, 469-528. See Eq. (4.27).

%H M. A. Moore, <a href="https://doi.org/10.1103/PhysRevB.1.2238">Critical Behavior of the Four-Dimensional Ising Ferromagnet and the Breakdown of Scaling</a>, Phys. Rev. B 1, 2238-2240 (1970).

%H <a href="/index/Da#D4">Index entries for sequences related to D_4 lattice</a>

%Y Cf. A010047, A010559, A010560, A010564.

%K nonn,more

%O 1,1

%A _N. J. A. Sloane_

%E Edited by _Andrey Zabolotskiy_, Aug 01 2022 and Nov 26 2024