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title: "Criticality of the Discrete N-Vector Ferromagnet in Planar Self-Dual Lattices • CBPF Index"
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> Index of every page on this site: [llms.txt](https://index.cbpf.br/llms.txt)

**Nota de Física****Publicado**

# **Criticality of the Discrete N-Vector Ferromagnet in Planar Self-Dual Lattices**

**C. Tsallis; A. M. Mariz; A. Stella; L. R. Silva**

1989

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## **Datos de la publicación**

<dl>

<dt>Autores</dt>
<dd>C. Tsallis; A. M. Mariz; A. Stella; L. R. Silva</dd>

<dt>Tipo</dt>
<dd>Nota de Física</dd>

<dt>Estado</dt>
<dd>Publicado</dd>

<dt>Fecha de publicación</dt>
<dd>1989</dd>

<dt>Descripción</dt>
<dd>We study an extended version of the discrete N-vector (or cubic) ferromagnetic model within a real space renormalization group approach which preserves the two-spin correlation function. The N−evolution (for ''real'' values of N) of the Wheatstone-bridge hierarchical lattice phase diagram, which presents paramagnetic, intermediate (nematic-like) and ferromagnetic phases, as well as of the thermal (&lt;math&gt;\nu &lt;/math&gt;) and crossover (&lt;math&gt;\varnothing &lt;/math&gt;) critical exponents, is presented. The self-avoiding walk problem is recovered in the N &lt;math&gt; \to &lt;/math&gt; 0 limit, and the so called "corner-rule" is reobtained in a larger context. The Ising, N- and 2N-state Potts ferromagnets are recovered as particular cases. An interchange of stability occurs at N = N* &lt;math&gt;\simeq &lt;/math&gt; 6.9 in such a way that the 2N-state Potts special point (where all three existing phases join) is a multicritical one if N &lt; N* but only a critical one if N &gt; N* (consistently &lt;math&gt;\varnothing &lt;/math&gt;(N*)=0). For the cubic model, &lt;math&gt;\nu &lt;/math&gt;(N) presents a maximum at N = N&lt;sub&gt;max&lt;/sub&gt; &lt;math&gt;\simeq &lt;/math&gt;1.5. The results are exact, for all N, for the Wheatstone-bridge hierarchical lattice, and approximate, for N &lt;math&gt; \leqslant &lt;/math&gt; 2, for the square lattice. Last but not least, we discuss the connection between the present approach and the phenomenological renormalization group.</dd>

<dt>Año</dt>
<dd>1989</dd>

<dt>Número</dt>
<dd>CBPF-NF-017/89</dd>

<dt>Vínculo con tesis</dt>
<dd>No</dd>

<dt>Vínculo con beca</dt>
<dd>No</dd>

</dl>

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