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<ref>[http://www.jetp.ac.ru/cgi-bin/e/index/e/34/3/p610?a=list V. L. Berezinskii "Destruction of Long-range Order in One-dimensional and Two-dimensional Systems Possessing a Continuous Symmetry Group. II. Quantum Systems", Journal of Experimental and Theoretical Physics '''34''' pp. 610 (1972)]</ref>
<ref>[http://www.jetp.ac.ru/cgi-bin/e/index/e/34/3/p610?a=list V. L. Berezinskii "Destruction of Long-range Order in One-dimensional and Two-dimensional Systems Possessing a Continuous Symmetry Group. II. Quantum Systems", Journal of Experimental and Theoretical Physics '''34''' pp. 610 (1972)]</ref>
<ref>[http://dx.doi.org/10.1088/0022-3719/5/11/002  J. M. Kosterlitz and D. J. Thouless "Long range order and metastability in two dimensional solids and superfluids. (Application of dislocation theory)", Journal of Physics C: Solid State Physics '''5''' pp. L124-L126 (1972)]</ref>
<ref>[http://dx.doi.org/10.1088/0022-3719/5/11/002  J. M. Kosterlitz and D. J. Thouless "Long range order and metastability in two dimensional solids and superfluids. (Application of dislocation theory)", Journal of Physics C: Solid State Physics '''5''' pp. L124-L126 (1972)]</ref>
<ref name="KT_1">[http://dx.doi.org/10.1088/0022-3719/6/7/010  J. M. Kosterlitz and D. J. Thouless "Ordering, metastability and phase transitions in two-dimensional systems", Journal of Physics C: Solid State Physics '''6''' pp. 1181-1203 (1973)]</ref> is a [[phase transitions | phase transition]]
<ref>[http://dx.doi.org/10.1088/0022-3719/6/7/010  J. M. Kosterlitz and D. J. Thouless "Ordering, metastability and phase transitions in two-dimensional systems", Journal of Physics C: Solid State Physics '''6''' pp. 1181-1203 (1973)]</ref> is a [[phase transitions | phase transition]]
found in the two-dimensional [[XY model]]. Below the transition temperature, <math>T_{KT}</math>, the system plays host to a 'liquid' of vortex-antivortex pairs that have zero total vorticity. Above <math>T_{KT}</math> these pairs break up into a gas of independent vortices.
found in the two-dimensional [[XY model]].
 
For the XY model the critical temperature is given by (Eq.4 in <ref name="KT_1"></ref>):
 
:<math>T_c = \frac{\pi J}{k_B}</math>
 
where <math>J</math> is the spin-spin coupling constant. This can be obtained as (Eq.58 in <ref name="KT_1"></ref>):
 
:<math>\frac{\pi J}{k_BT_c}-1 \approx \pi \tilde{y}_c(0) \exp\left(\frac{-\pi^2J}{k_BT_c} \right) \approx 0.12</math>
==See also==
*[[Universality classes#XY | XY universality class]]
==References==
==References==
<references/>
<references/>
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*[http://dx.doi.org/10.1088/0953-8984/14/9/321 Kurt Binder, Surajit Sengupta and Peter Nielaba "The liquid-solid transition of hard discs: first-order transition or Kosterlitz-Thouless-Halperin-Nelson-Young scenario?", Journal of Physics: Condensed Matter '''14''' pp. 2323-2333 (2002)]
*[http://dx.doi.org/10.1088/0953-8984/14/9/321 Kurt Binder, Surajit Sengupta and Peter Nielaba "The liquid-solid transition of hard discs: first-order transition or Kosterlitz-Thouless-Halperin-Nelson-Young scenario?", Journal of Physics: Condensed Matter '''14''' pp. 2323-2333 (2002)]
* "40 Years of Berezinskii–Kosterlitz–Thouless Theory" (Ed. Jorge V José) World Scientific Publishing (2013) ISBN 978-981-4417-63-1
* "40 Years of Berezinskii–Kosterlitz–Thouless Theory" (Ed. Jorge V José) World Scientific Publishing (2013) ISBN 978-981-4417-63-1
*[http://www.nobelprize.org/nobel_prizes/physics/laureates/2016/advanced-physicsprize2016.pdf Nobel Prize in Physics 2016 'Scientific Background']


[[category: phase transitions]]
[[category: phase transitions]]
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