2016
DOI: 10.1103/physreve.94.032140
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Competing nematic interactions in a generalizedXYmodel in two and three dimensions

Abstract: We study a generalization of the XY model with an additional nematic-like term through extensive numerical simulations and finite-size techniques, both in two and three dimensions. While the original model favors local alignment, the extra term induces angles of 2π/q between neighboring spins. We focus here on the q = 8 case (while presenting new results for other values of q as well) whose phase diagram is much richer than the well-known q = 2 case. In particular, the model presents not only continuous, stand… Show more

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Cited by 40 publications
(41 citation statements)
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“…For q > 3, the results in Refs [61,62] suggest the existence of new phases at intermediate values of ∆ that do not appear for either ∆ = 0 or 1. Since the existence and/or nature of some of those transitions are still disputed, it would be interesting to see the outcome of the neural networks in those cases.…”
Section: Q=8mentioning
confidence: 95%
“…For q > 3, the results in Refs [61,62] suggest the existence of new phases at intermediate values of ∆ that do not appear for either ∆ = 0 or 1. Since the existence and/or nature of some of those transitions are still disputed, it would be interesting to see the outcome of the neural networks in those cases.…”
Section: Q=8mentioning
confidence: 95%
“…Nevertheless, such investigations by MC simulations would require immense computational effort and it is out of the present scope. Furthermore, in the light of the recently found new phases in the model involving only two terms with q = 1 and q ≥ 5 [18,19], it would be interesting to explore the possibility of the existence of additional phases in the generalized XY model involving multiple terms with the q-values ranging between q min = 1 and q max ≥ 5.…”
Section: Summary and Discussionmentioning
confidence: 99%
“…Surprisingly, recent studies revealed that the model involving the q = 1 and q ≥ 5 terms displays a qualitatively different phase diagram featuring additional phases [18,19]. The latter appeared due to the competition between the respective couplings and the resulting phase transitions were determined to belong to different (Potts, Ising, or BKT) universality classes.…”
Section: Introductionmentioning
confidence: 99%
“…We can imagine this as an interaction between the spins considered as headless rods: spins which are parallel contribute less energy, even if they point in opposite directions. The T -∆ phase dia- gram of this model is explored in [47][48][49], and we see that at our chosen ∆ = 0.15, it undergoes two phase transitions as temperature increases. The first is an Ising-type transition from a magnetic phase to a nematic phase at T ≈ 0.3314 (as estimated using the magnetic susceptibility) resulting in (anti)vortices (which remain bound into vortex-antivortex pairs) stretching into domain walls with a half-(anti)vortex at each end; across the wall the spins flip by π.…”
Section: Nematic Xy Modelmentioning
confidence: 94%