Abstract
Recently, Merca presented characterizations of the parities on \(R_s(n)\) and \(R_t^{*}(n)\) with \(s\in \{2,4\}\) and \(t\in \{1,3\}\), where \(R_s(n)\) counts the number of partitions of n into odd parts or congruent to \(0, \pm s\ (\textrm{mod}\ 10)\) and \(R_t^{*}(n)\) counts the number of partitions of n into parts not congruent to \( 0, \pm t\ (\textrm{mod} 10)\) and \(10 \pm 2t\ (\textrm{mod} \ 20)\). The generating function of \(R_s(n)\) arises naturally in regime III of Baxter’s solution of the hard-hexagon model of statistical mechanics and the generating function of \(R_t^{*} (n)\) arises naturally in regime IV of Baxter’s solution of the hard-hexagon model of statistical mechanics. In this paper, we prove some congruences modulo 4 and 8. In particular, we establish several infinite families of congruences modulo 4 and 8 for \(R_s(n)\) and \(R_t^{*}(n)\) and prove that \(\frac{R_s(n)}{8}\) and \(\frac{R_t^{*}(n)}{8}\) take integer values with probability 1 for \(n\ge 0\).
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Acknowledgements
This work was supported by the Natural Science Foundation of Jiangsu Province of China (no. BK20221383) and the National Natural Science Foundation of China (no. 11971203).
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Yao, O.X.M. New congruences involving statistical mechanics partition functions in regime III and IV of Baxter’s solution of the hard-hexagon model. Rev. Real Acad. Cienc. Exactas Fis. Nat. Ser. A-Mat. 117, 62 (2023). https://doi.org/10.1007/s13398-023-01394-x
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DOI: https://doi.org/10.1007/s13398-023-01394-x