A010367 High-temperature spin-1/2 Ising model series for second derivative of susceptibility with respect to magnetic field for hyper-body-centered-cubic lattice.

2, 128, 9792, 886784, 92722944, 11014965248, 1465369976832, 215937597784064, 34916329300783104, 6147843514432913408, 1170908043876450435072

Offset

1,1

Comments

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

Links

Table of n, a(n) for n=1..11.

George A. Baker Jr. and John M. Kincaid, The continuous-spin Ising model, g0:phi4:d field theory and the renormalization group. J. Statist. Phys. 24 (1981), no. 3, 469-528. See Eq. (4.27).

M. A. Moore, Critical Behavior of the Four-Dimensional Ising Ferromagnet and the Breakdown of Scaling, Phys. Rev. B 1, 2238-2240 (1970).

Index entries for sequences related to D_4 lattice

Crossrefs

Cf. A010047, A010559, A010560, A010564.

Sequence in context: A202748 A322308 A277757 * A024344 A012673 A358486

Adjacent sequences: A010364 A010365 A010366 * A010368 A010369 A010370

Keyword

nonn,more,changed

Author

N. J. A. Sloane

Extensions

Edited by Andrey Zabolotskiy, Aug 01 2022 and Nov 26 2024

Status

approved