Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Possible splitting of a phase transition in a 2D XY model

S. E. Korshunov

Published Mar 10, 1985• 8 citations
OpenAlex

Related papers

First-order transition in 2D classical XY-model

Snehadri Bihari Ota, Smita Ota

Bulletin of the American Physical Society•Mar 12, 2008•0 citations

The low temperature phase in the 2D quantum XY model

J. Szṅajd, J. Zittartz

Journal of Magnetism and Magnetic Materials•Feb 1, 1992•0 citations

Phase Transition in the 2D XY Model with 3-Fold Nematic Interactions

Nguyễn Thị Minh Huyền, Lưu Bích Linh, Bui Thi Toan Thu +5 more

In this work the results of the study on a generalization of the XY model with an additional q-fold nematic-like term through Monte Carlo simulations in two dimensions (2D) have been presented. While the conventional 2D XY model has only integer vortexes, the generalized 2D XY model has both integer and non-integer 1/q vortexes, making the phase diagram of the generalized 2D XY model is much richer than that of the conventional 2D XY model. Here, we located the phase transition between the disordered phase (P), the quasi-long-range order phase (F), and the nematic phase (N) for the case of q = 3. We provided the numerical evidence to clarify the N−F phase transition of either the first-ordered or second-ordered phase transition. The results showed that the N−F phase transition is the second-ordered, not the first-order phase transition.

VNU Journal of Science Mathematics - Physics•Jun 24, 2022•0 citations

Phase transition in the two-dimensional classical XY model

Jae-Kwon Kim

arXiv:hep-lat/9502002•Physics Letters A•Dec 1, 1996•13 citations

The 2D J 1 − J 2 XY and XY-Ising models

Pascal Simon

We consider the 2D J 1 − J 2 classical XY model on a square lattice. In the frustrated phase corresponding to J 2 > J 1 /2, an Ising order parameter emerges by an "order due to disorder" effect. This leads to a discrete symmetry plus the O (2) global one. We formulate the problem in a Coulomb gas language and show by a renormalization group analysis that only two phases are still possible: a locked phase at low temperature and a disordered one at high temperature. The transition is characterized by the loss of Ising and XY order at the same point. This analysis suggests that the 2D J 1 − J 2 XY model is in the same universality class as XY-Ising models.

arXiv:cond-mat/9706078•Europhysics Letters (EPL)•Jul 15, 1997•14 citations

Quantum-phase transition in a XY model

Antonio S. T. Pires

Physica A Statistical Mechanics and its Applications•Sep 8, 2006•40 citations
In this work the results of the study on a generalization of the XY model with an additional q-fold nematic-like term through Monte Carlo simulations in two dimensions (2D) have been presented. While the conventional 2D XY model has only integer vortexes, the generalized 2D XY model has both integer and non-integer 1/q vortexes, making the phase diagram of the generalized 2D XY model is much richer than that of the conventional 2D XY model. Here, we located the phase transition between the disordered phase (P), the quasi-long-range order phase (F), and the nematic phase (N) for the case of q = 3. We provided the numerical evidence to clarify the N−F phase transition of either the first-ordered or second-ordered phase transition. The results showed that the N−F phase transition is the second-ordered, not the first-order phase transition.
We consider the 2D J 1 − J 2 classical XY model on a square lattice. In the frustrated phase corresponding to J 2 > J 1 /2, an Ising order parameter emerges by an "order due to disorder" effect. This leads to a discrete symmetry plus the O (2) global one. We formulate the problem in a Coulomb gas language and show by a renormalization group analysis that only two phases are still possible: a locked phase at low temperature and a disordered one at high temperature. The transition is characterized by the loss of Ising and XY order at the same point. This analysis suggests that the 2D J 1 − J 2 XY model is in the same universality class as XY-Ising models.