This is the authors' abstract. We don't add key points for this paper.
A previously developed method for diagrammatic expansion of the Ising-model partition function and pair distribution function is applied to calculation of the field-free quadruplet spin averages 〈μ₁μ₂μ₃μ₄〉. The central four-vertex function Q generated by these averages is topologically analyzed in standard fashion in terms of an irreducible four-vertex quantity e. Several rigorously necessary conditions that must be satisfied by Q are listed. It is furthermore pointed out that the existence of a logarithmic specific-heat anomaly puts an additional constraint on quadruplet averages (which is verified in an Appendix by direct calculation on the Ising-Onsager two-dimensional square lattice). Upon making a simplifying functional assumption for Q, this latter quantity may be entirely determined above Tc by one of the necessary conditions. This leads at Tc to a kd/2 spectrum (d=dimensionality) and above Tc to a logarithmic specific heat, both of which were adduced by Abe's Ising-model version of the He⁴ speculative analysis due to Patashinskii and Pokrovskii (but for different reasons from those in the present analysis). Sinec the Abe-Patashinskii-Pokrovskii spectrum almost certainly exhibits an incorrect exponent, an alternative and more powerful functional assumption for Q is suggested which still yields a soluble theory in principle, but construction of the solution is not attempted here.
Answers are grounded in this paper and cite their sources.
No takes yet. Share an insight, caveat, or question.
Frank H. Stillinger (1966) studied this question.
Synapse has enriched 10 related papers. Consider them for comparative context: