{ "id": "2501.18569", "version": "v1", "published": "2025-01-30T18:39:44.000Z", "updated": "2025-01-30T18:39:44.000Z", "title": "Derivation of the free energy, entropy and specific heat for planar Ising models: Application to Archimedean lattices and their duals", "authors": [ "Laurent Pierre", "Bernard Bernu", "Laura Messio" ], "comment": "22 pages, 48 with the appendices, 10 figures, 5 tables", "categories": [ "cond-mat.stat-mech" ], "abstract": "The 2d ferromagnetic Ising model was solved by Onsager on the square lattice in 1944, and an explicit expression of the free energy density $f$ is presently available for some other planar lattices. An exact derivation of the critical temperature $T_c$ only requires a partial derivation of $f$ and has been performed on many lattices, including the 11 Archimedean lattices. We give general expressions of the free energy, energy, entropy and specific heat for planar lattices with a single type of non-crossing links. The specific heat exhibits a logarithmic singularity at $T_c$: $c_V(T)\\sim -A\\ln|1-T_c/T|$, in all the ferromagnetic and some antiferromagnetic cases. While the non-universal weight $A$ of the leading term has often been evaluated, this is not the case for the sub-leading order term $B$ such that $c_V(T)+A\\ln|1-T_c/T|\\sim B$, despite its strong impact on $c_V(T)$ values in the vicinity of $T_c$, particularly important in experimental measurements. Explicit values of these thermodynamic quantities and of $A$ and $B$ are given for the Archimedean lattices and their dual for both ferromagnetic and antiferromagnetic interactions.", "revisions": [ { "version": "v1", "updated": "2025-01-30T18:39:44.000Z" } ], "analyses": { "keywords": [ "specific heat", "archimedean lattices", "planar ising models", "derivation", "application" ], "note": { "typesetting": "TeX", "pages": 22, "language": "en", "license": "arXiv", "status": "editable" } } }