Free-energy formula for the one-dimensional 3-permaspin model

Let c=e2βHc=e^{-2\beta H} and d=e2βJd=e^{-2\beta J}, and consider the one-dimensional 3-permaspin model with couplings JJ and HH. Let zz be the unique root of the cubic

λ3(cd2+c2+2cd+c+1)λ2c(cd3+3c2d+cd2+c2+cd+c+3d+1)(d1)λ+(d2+4d+1)c3(d+1)(d1)3=0\lambda^3-(cd^2+c^2+2cd+c+1)\lambda^2-c(cd^3+3c^2d+cd^2+c^2+cd+c+3d+1)(d-1)\lambda+(d^2+4d+1)c^3(d+1)(d-1)^3=0

whose argument satisfies arg(z)[2π/3,π]\mathbf{\arg}(z)\in[2\pi/3,\pi]. Free-energy formula. The free energy is

f(cddes)(β)=(J+H)1βln(c2d+c2+2cd+c+12Re(z)).f^{(\mathrm{cddes})}(\beta)=-(J+H)-\frac{1}{\beta}\ln\left(c^2d+c^2+2cd+c+1-2\mathbf{Re}(z)\right).

This summarizes the preceding experimental observations and spectral analysis of the transfer matrix. The parser provides no evidence that the formula has been proved, so its status is left open.

Sources & referencesView supporting material

Primary source

Mark Dukes, “An Ising model having permutation spin motivated by a permutation complexity measure”, arXiv:2211.08908 (2023).

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