Matches in DBpedia 2016-04 for { ?s ?p "The Kosterlitz–Thouless transition (KT transition), or Berezinsky–Kosterlitz–Thouless transition (BKT transition), is a phase transition in the two-dimensional (2-D) XY model. It is a transition from bound vortex-antivortex pairs at low temperatures to unpaired vortices and anti-vortices at some critical temperature. The transition is named for condensed matter physicists Vadim L'vovich Berezinskiĭ (Вади́м Льво́вич Берези́нский), John M. Kosterlitz and David J. Thouless. BKT transitions can be found in several 2-D systems in condensed matter physics that are approximated by the XY model, including Josephson junction arrays and thin disordered superconducting granular films. More recently, the term has been applied by the 2-D superconductor insulator transition community to the pinning of Cooper pairs in the insulating regime, due to similarities with the original vortex BKT transition."@en }
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- Kosterlitz–Thouless_transition abstract "The Kosterlitz–Thouless transition (KT transition), or Berezinsky–Kosterlitz–Thouless transition (BKT transition), is a phase transition in the two-dimensional (2-D) XY model. It is a transition from bound vortex-antivortex pairs at low temperatures to unpaired vortices and anti-vortices at some critical temperature. The transition is named for condensed matter physicists Vadim L'vovich Berezinskiĭ (Вади́м Льво́вич Берези́нский), John M. Kosterlitz and David J. Thouless. BKT transitions can be found in several 2-D systems in condensed matter physics that are approximated by the XY model, including Josephson junction arrays and thin disordered superconducting granular films. More recently, the term has been applied by the 2-D superconductor insulator transition community to the pinning of Cooper pairs in the insulating regime, due to similarities with the original vortex BKT transition.".
- Q898780 abstract "The Kosterlitz–Thouless transition (KT transition), or Berezinsky–Kosterlitz–Thouless transition (BKT transition), is a phase transition in the two-dimensional (2-D) XY model. It is a transition from bound vortex-antivortex pairs at low temperatures to unpaired vortices and anti-vortices at some critical temperature. The transition is named for condensed matter physicists Vadim L'vovich Berezinskiĭ (Вади́м Льво́вич Берези́нский), John M. Kosterlitz and David J. Thouless. BKT transitions can be found in several 2-D systems in condensed matter physics that are approximated by the XY model, including Josephson junction arrays and thin disordered superconducting granular films. More recently, the term has been applied by the 2-D superconductor insulator transition community to the pinning of Cooper pairs in the insulating regime, due to similarities with the original vortex BKT transition.".