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- The high-temperature disordered phase of the XY model is peculiar because12:
- It is characterized by topological defects, leading to a vortex-unbinding transition.
- These defects cannot be removed by continuous transformations of the spin orientation.
- In two dimensions, the XY model exhibits the Kosterlitz-Thouless transition, which is of infinite order and has exponential spin correlations above the transition temperature TKT3.
Learn more:✕This summary was generated using AI based on multiple online sources. To view the original source information, use the "Learn more" links.Topological defects in the XY model leads to a vortex-unbinding transition from the low-temperature phase to the high-temperature disordered phase.www.chemeurope.com/en/encyclopedia/XY+model…The peculiar nature of the disordering mechanism causing this phase transition, is that these disorders cannot be removed by any continuous transformations of the spin orientation.web.mit.edu/8.334/www/grades/projects/projects12…Thus the XY-model cannot have an ordered phase at low temperature like the Ising model does. Yet in two dimensions it does show the very peculiar Kosterlitz-Thouless (KT) transition, which is very soft, of infinite order. Above the transition temperature TKT, correlations between spins decay exponentially as usual, with some correlation length ξ.itp.tugraz.at/MML/isingxy/isingxy.pdf - People also ask
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Classical XY model | Wikipedia
This is what makes them peculiar from other phase transitions which are always accompanied with a symmetry breaking. Topological defects in the XY model lead to a vortex-unbinding transition from the low-temperature phase to the high-temperature disordered phase. See more
The classical XY model (sometimes also called classical rotor (rotator) model or O(2) model) is a lattice model of statistical mechanics. In general, the XY model can be seen as a specialization of Stanley's n-vector model for … See more
Given a D-dimensional lattice Λ, per each lattice site j ∈ Λ there is a two-dimensional, unit-length vector sj = (cos θj, sin θj)
The spin … See moreAs mentioned above in one dimension the XY model does not have a phase transition, while in two dimensions it has the Berezinski-Kosterlitz-Thouless transition between … See more
• H. E. Stanley, Introduction to Phase Transitions and Critical Phenomena, (Oxford University Press, Oxford and New York 1971); See more
• The existence of the thermodynamic limit for the free energy and spin correlations were proved by Ginibre, extending to this case the Griffiths inequality.
• Using … See moreWikipedia text under CC-BY-SA license Disordered XY model: Effective medium theory and beyond
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