English

The spin-3/2 Blume-Capel model with competing short- and long-range interactions

Statistical Mechanics 2016-02-23 v1

Abstract

The phase diagrams of the spin-3/23/2 Blume-Capel model with competing short and long-range interactions were studied through the free energy density obtained by analytical methods. The competition emerges when positive short-range interactions of strength KK arranged in a linear chain tend to establish an anti-parallel spin order, whereas negative long-range interactions J-J tend to align them in parallel. Thus, no ferromagnetic order exists for K/J>0.25K/J > 0.25. So, the phase-diagrams were scanned by varying the values of KK in this interval. As in other similar study done for the spin-1 case, the second-order frontier separating the ferromagnetic and the paramagnetic phases is transformed gradually into a first-order line, when K/JK/J is greater than a certain critical value. Accordingly, there is a subinterval of KK, for which two tricritical points appear restricting the length of the second-order frontier. Nevertheless, for greater values of K/JK/J, the ferromagnetic-paramagnetic frontier becomes wholly of first order. Also, the tipical coexistence line, which divides two different ferromagnetic phases of magnetization m=3/2m=3/2 and m=1/2m=1/2, becomes more complex by giving rise to another line of coexistence with a reentrant behavior that encloses a third ordered phase. In this case, the competition is such that there is a region in the phase diagram, where for each spin ii with Si=3/2S_{i}=3/2 (Si=3/2S_{i}=-3/2), there is another one spin jj with Sj=1/2S_{j}=-1/2 (Sj=1/2S_{j}=1/2), so the absolute value of the magnetization per spin is one.

Keywords

Cite

@article{arxiv.1602.06360,
  title  = {The spin-3/2 Blume-Capel model with competing short- and long-range interactions},
  author = {Octavio D. Rodriguez Salmon and Jose Ricardo de Sousa and Minos A. Neto and Igor T. Padilha and J. Roberto Viana Azevedo and Francisco Dinola Neto},
  journal= {arXiv preprint arXiv:1602.06360},
  year   = {2016}
}
R2 v1 2026-06-22T12:54:11.613Z