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Area Superconductivity / Superconducting properties

IEV ref815-10-34

Symbol
κGL

en
Ginzburg-Landau parameter
G-L parameter
ratio of penetration depth, λ, to coherence length, ξ

κ GL =λ/ξ MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garmWu51MyVXgaruWqVvNCPvMCG4uz 3bqee0evGueE0jxyaibaieYdi9WrpeeC0lXdi9qqqj=hEeeu0lXdbb a9frFj0xb9Lqpepeea0xd9s8qiYRWxGi6xij=hbba9q8aq0=yq=He9 q8qiLsFr0=vr0=vr0db8meaabaGacmGadiWaaiWabiabciaafiaake aacqaH6oWAdaWgaaWcbaGaae4raiaabYeaaeqaaOGaeyypa0ZaaSGb aeaacqaH7oaBaeaacqaH+oaEaaaaaa@41A7@

Note 1 to entry: For a type II superconductor, κ GL >1/ 2 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garmWu51MyVXgaruWqVvNCPvMCG4uz 3bqee0evGueE0jxyaibaieYdi9WrpeeC0lXdi9qqqj=hEeeu0lXdbb a9frFj0xb9Lqpepeea0xd9s8qiYRWxGi6xij=hbba9q8aq0=yq=He9 q8qiLsFr0=vr0=vr0db8meaabaGacmGadiWaaiWabiabciaafiaake aacqaH6oWAdaWgaaWcbaGaae4raiaabYeaaeqaaOGaeyOpa4ZaaSGb aeaacaqGXaaabaWaaOaaaeaacaqGYaaaleqaaaaaaaa@3FB6@ ; κ GL = H c2 / ( 2 H c ) MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garmWu51MyVXgaruWqVvNCPvMCG4uz 3bqee0evGueE0jxyaibaieYdi9WrpeeC0lXdi9qqqj=hEeeu0lXdbb a9frFj0xb9Lqpepeea0xd9s8qiYRWxGi6xij=hbba9q8aq0=yq=He9 q8qiLsFr0=vr0=vr0db8meaabaGacmGadiWaaiWabiabciaafiaake aacqaH6oWAdaWgaaWcbaGaae4raiaabYeaaeqaaOGaeyypa0ZaaSGb aeaacaWGibWaaSbaaSqaaiaabogacaqGYaaabeaaaOqaamaabmaaba WaaOaaaeaacaqGYaaaleqaaOGaamisamaaBaaaleaacaqGJbaabeaa aOGaayjkaiaawMcaaaaaaaa@451A@ , where H c2 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garmWu51MyVXgaruWqVvNCPvMCG4uz 3bqee0evGueE0jxyaibaieYdi9WrpeeC0lXdi9qqqj=hEeeu0lXdbb a9frFj0xb9Lqpepeea0xd9s8qiYRWxGi6xij=hbba9q8aq0=yq=He9 q8qiLsFr0=vr0=vr0db8meaabaGacmGadiWaaiWabiabciaafiaake aacaWGibWaaSbaaSqaaiaabogaaeqaaaaa@3B72@ is the upper critical field strength and H c MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garmWu51MyVXgaruWqVvNCPvMCG4uz 3bqee0evGueE0jxyaibaieYdi9WrpeeC0lXdi9qqqj=hEeeu0lXdbb a9frFj0xb9Lqpepeea0xd9s8qiYRWxGi6xij=hbba9q8aq0=yq=He9 q8qiLsFr0=vr0=vr0db8meaabaGacmGadiWaaiWabiabciaafiaake aacaWGibWaaSbaaSqaaiaabogaaeqaaaaa@3B72@ is the critical field strength.

Note 2 to entry: For a type I superconductor, κ GL <1/ 2 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garmWu51MyVXgaruWqVvNCPvMCG4uz 3bqee0evGueE0jxyaibaieYdi9WrpeeC0lXdi9qqqj=hEeeu0lXdbb a9frFj0xb9Lqpepeea0xd9s8qiYRWxGi6xij=hbba9q8aq0=yq=He9 q8qiLsFr0=vr0=vr0db8meaabaGacmGadiWaaiWabiabciaafiaake aacqaH6oWAdaWgaaWcbaGaae4raiaabYeaaeqaaOGaeyipaWZaaSGb aeaacaqGXaaabaWaaOaaaeaacaqGYaaaleqaaaaaaaa@3FB2@ .


fr
paramètre de Ginzburg-Landau, m
rapport de la profondeur de pénétration λ à la longueur de cohérence ξ

κ GL =λ/ξ MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garmWu51MyVXgaruWqVvNCPvMCG4uz 3bqee0evGueE0jxyaibaieYdi9WrpeeC0lXdi9qqqj=hEeeu0lXdbb a9frFj0xb9Lqpepeea0xd9s8qiYRWxGi6xij=hbba9q8aq0=yq=He9 q8qiLsFr0=vr0=vr0db8meaabaGacmGadiWaaiWabiabciaafiaake aacqaH6oWAdaWgaaWcbaGaae4raiaabYeaaeqaaOGaeyypa0ZaaSGb aeaacqaH7oaBaeaacqaH+oaEaaaaaa@41A7@

Note 1 à l’article: Pour un supraconducteur de type II, κ GL >1/ 2 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garmWu51MyVXgaruWqVvNCPvMCG4uz 3bqee0evGueE0jxyaibaieYdi9WrpeeC0lXdi9qqqj=hEeeu0lXdbb a9frFj0xb9Lqpepeea0xd9s8qiYRWxGi6xij=hbba9q8aq0=yq=He9 q8qiLsFr0=vr0=vr0db8meaabaGacmGadiWaaiWabiabciaafiaake aacqaH6oWAdaWgaaWcbaGaae4raiaabYeaaeqaaOGaeyOpa4ZaaSGb aeaacaqGXaaabaWaaOaaaeaacaqGYaaaleqaaaaaaaa@3FB6@ ; κ GL = H c2 / ( 2 H c ) MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garmWu51MyVXgaruWqVvNCPvMCG4uz 3bqee0evGueE0jxyaibaieYdi9WrpeeC0lXdi9qqqj=hEeeu0lXdbb a9frFj0xb9Lqpepeea0xd9s8qiYRWxGi6xij=hbba9q8aq0=yq=He9 q8qiLsFr0=vr0=vr0db8meaabaGacmGadiWaaiWabiabciaafiaake aacqaH6oWAdaWgaaWcbaGaae4raiaabYeaaeqaaOGaeyypa0ZaaSGb aeaacaWGibWaaSbaaSqaaiaabogacaqGYaaabeaaaOqaamaabmaaba WaaOaaaeaacaqGYaaaleqaaOGaamisamaaBaaaleaacaqGJbaabeaa aOGaayjkaiaawMcaaaaaaaa@451A@ , où H c2 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garmWu51MyVXgaruWqVvNCPvMCG4uz 3bqee0evGueE0jxyaibaieYdi9WrpeeC0lXdi9qqqj=hEeeu0lXdbb a9frFj0xb9Lqpepeea0xd9s8qiYRWxGi6xij=hbba9q8aq0=yq=He9 q8qiLsFr0=vr0=vr0db8meaabaGacmGadiWaaiWabiabciaafiaake aacaWGibWaaSbaaSqaaiaabogaaeqaaaaa@3B72@ est le champ magnétique critique supérieur et H c MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garmWu51MyVXgaruWqVvNCPvMCG4uz 3bqee0evGueE0jxyaibaieYdi9WrpeeC0lXdi9qqqj=hEeeu0lXdbb a9frFj0xb9Lqpepeea0xd9s8qiYRWxGi6xij=hbba9q8aq0=yq=He9 q8qiLsFr0=vr0=vr0db8meaabaGacmGadiWaaiWabiabciaafiaake aacaWGibWaaSbaaSqaaiaabogaaeqaaaaa@3B72@ le champ magnétique critique.

Note 2 à l’article: Pour un supraconducteur de type I, κ GL <1/ 2 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garmWu51MyVXgaruWqVvNCPvMCG4uz 3bqee0evGueE0jxyaibaieYdi9WrpeeC0lXdi9qqqj=hEeeu0lXdbb a9frFj0xb9Lqpepeea0xd9s8qiYRWxGi6xij=hbba9q8aq0=yq=He9 q8qiLsFr0=vr0=vr0db8meaabaGacmGadiWaaiWabiabciaafiaake aacqaH6oWAdaWgaaWcbaGaae4raiaabYeaaeqaaOGaeyipaWZaaSGb aeaacaqGXaaabaWaaOaaaeaacaqGYaaaleqaaaaaaaa@3FB2@ .


de
Ginzburg-Landau-Parameter, m
GL-Parameter, m

es
parámetro de orden Ginzburg-Landau

ko
긴즈버그-란다우 매개변수

ja
ギンツブルグ-ランダウ・パラメータ
G-Lパラメータ

pl
parametr Ginzburga-Landaua, m
parametr G-L, m

pt
parâmetro de Ginzburg-Landau

zh
金兹堡-朗道参数
G-L参数

Publication date: 2015-11
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