Skip to content
DraconiticResearch
Search Sources API
197,768 studies31 sourcesUpdated 27 min ago
PreprintCC BY-NC-SA 4.0arXiv

Branching Gaps, Coexistence, and Boundary Influence for the Ising Model on Spherically Symmetric Trees

Abstract

In this paper, we study the ferromagnetic nearest-neighbor Ising model on rooted spherically symmetric trees with one or q children per vertex, according to a prescribed sequence of branching levels. Unbounded runs of one-child levels force uniqueness at every nonzero homogeneous field and every finite inverse temperature. We quantify this effect through the locations of sufficiently long nonbranching stretches. Conversely, uniqueness need not entail any uniform rate: for each prescribed vanishing sequence, we construct a density-one tree whose finite-volume boundary influence decays more slowly along a subsequence. The tree retains branching number q, although its nonzero-field coexistence region disappears. For eventually bounded gaps, we prove an optimal uniform comparison with the periodic tree having the largest allowed gap and obtain an explicit interval of coexistence fields. Thus bounded gaps are equivalent, within this family, to coexistence at some finite temperature and nonzero field. For eventually periodic gaps, Gibbs uniqueness is equivalent to fixed-point uniqueness of the full-period return map. A negative Schwarzian derivative yields a complete classification: in the supercritical regime the map has three fixed points inside a closed coexistence interval, two at its endpoints, and one outside. The nonzero endpoints are automatically nondegenerate folds, with square-root splitting of the merging branches.

Related

  1. Spherically symmetric Finsler metrics satisfying the σT-condition
    Salah G. Elgendi
    arXivPreprintarXiv licenceFull textGeometry & topologyarXiv
  2. Unbounded log-concavity breaks in independence polynomials of spherically symmetric trees
    César Bautista-Ramos
    arXivPreprintCC BY 4.0Full textCombinatorics & discrete mathematicsarXiv
  3. The Vlasov-Maxwell point charge system : study of the spherically symmetric case
    Emile Breton
    arXivPreprintarXiv licenceFull textAnalysis & PDEsarXiv
  4. Static spherically symmetric electroweak models with fermions and gravity
    Marko Sobak
    arXivPreprintCC BY-NC-ND 4.0Full textGeometry & topologyMathematical physicsarXiv
  5. Spherically symmetric inextendibility of weak null singularities with Christoffel symbols in Lsloc
    Peter Cameron, Jan Sbierski
    arXivPreprintCC BY 4.0Full textGeometry & topologyGravitation & general relativityarXiv
BibTeX
@misc{mukhamedov2026branching,
  title = {{Branching Gaps, Coexistence, and Boundary Influence for the Ising Model on Spherically Symmetric Trees}},
  author = {Farrukh Mukhamedov and Otabek Khakimov},
  howpublished = {arXiv},
  year = {2026},
  month = oct,
  doi = {10.48550/arxiv.2610.03941},
  eprint = {2610.03941},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2610.03941},
  note = {CC BY-NC-SA 4.0},
}
RIS
TY  - UNPB
TI  - Branching Gaps, Coexistence, and Boundary Influence for the Ising Model on Spherically Symmetric Trees
AU  - Farrukh Mukhamedov
AU  - Otabek Khakimov
PY  - 2026
DA  - 2026/10/02
PB  - arXiv
DO  - 10.48550/arxiv.2610.03941
UR  - https://arxiv.org/abs/2610.03941
AB  - In this paper, we study the ferromagnetic nearest-neighbor Ising model on rooted spherically symmetric trees with one or q children per vertex, according to a prescribed sequence of branching levels. Unbounded runs of one-child levels force uniqueness at every nonzero homogeneous field and every finite inverse temperature. We quantify this effect through the locations of sufficiently long nonbranching stretches. Conversely, uniqueness need not entail any uniform rate: for each prescribed vanishing sequence, we construct a density-one tree whose finite-volume boundary influence decays more slowly along a subsequence. The tree retains branching number q, although its nonzero-field coexistence region disappears. For eventually bounded gaps, we prove an optimal uniform comparison with the periodic tree having the largest allowed gap and obtain an explicit interval of coexistence fields. Thus bounded gaps are equivalent, within this family, to coexistence at some finite temperature and nonzero field. For eventually periodic gaps, Gibbs uniqueness is equivalent to fixed-point uniqueness of the full-period return map. A negative Schwarzian derivative yields a complete classification: in the supercritical regime the map has three fixed points inside a closed coexistence interval, two at its endpoints, and one outside. The nonzero endpoints are automatically nondegenerate folds, with square-root splitting of the merging branches.
ER  -