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Area Superconductivity / Superconducting properties

IEV ref 815-20-27

en
surface superconductivity
phenomenon in which a superconducting state appears within about one coherence length from the surface of a material, even under a magnetic field strength above the upper critical field strength H c2 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garmWu51MyVXgarqqtubsr4rNCHbGe aGqipG0dh9qqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm 0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9ad baqaaiGaciGacmaaceqaaeaacaabaaGcbaGaamisamaaBaaaleaaii aacaWFJbacbaGaa4Nmaaqabaaaaa@35A9@

Note 1 to entry: If the magnetic field is parallel to the surface of the sample, surface superconductivity appears within a range of a magnetic field strength from H c2 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garmWu51MyVXgarqqtubsr4rNCHbGe aGqipG0dh9qqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm 0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9ad baqaaiGaciGacmaaceqaaeaacaabaaGcbaqcaaKaamisaOWaaSbaaK qaafaaiiaacaWFJbacbaGaa4Nmaaqabaaaaa@363B@ to H c3 1,695 H c2 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garmWu51MyVXgarqqtubsr4rNCHbGe aGqipG0dh9qqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm 0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9ad baqaaiGaciGacmaaceqaaeaacaabaaGcbaqcaaKaamisaOWaaSbaaK qaafaaiiaacaWFJbacbaGaa43maaqabaqcaaKaeyisISRaaGymaiaa cYcacaaI2aGaaGyoaiaaiwdacaaMc8UaamisaOWaaSbaaKqaafaaca WFJbGaa4Nmaaqabaaaaa@4046@ for type II superconductors, and from H c MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garmWu51MyVXgarqqtubsr4rNCHbGe aGqipG0dh9qqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm 0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9ad baqaaiGaciGacmaaceqaaeaacaabaaGcbaqcaaKaamisaOWaaSbaaK qaafaaiiaacaWFJbaabeaaaaa@3580@ to H c3 2,40 H c MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garmWu51MyVXgarqqtubsr4rNCHbGe aGqipG0dh9qqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm 0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9ad baqaaiGaciGacmaaceqaaeaacaabaaGcbaqcaaKaamisaOWaaSbaaK qaafaaiiaacaWFJbacbaGaa43maaqabaqcaaKaeyisISRaaGOmaiaa cYcacaaI0aGaaGimaiaaykW7caWGibGcdaWgaaqcbauaaiaa=ngaae qaaaaa@3ECB@ for type I superconductors.

Note 2 to entry: This entry was numbered 815-10-41 in IEC 60050-815:2015.


fr
supraconductivité de surface, f
supraconduction de surface, f
phénomène qui se manifeste par l'apparition d’un supraconducteur à la surface d’un matériau sur une distance d’environ une fois la longueur de cohérence, même lorsque ce dernier est soumis à un champ magnétique supérieur au champ magnétique critique supérieur H c2 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garmWu51MyVXgarqqtubsr4rNCHbGe aGqipG0dh9qqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm 0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9ad baqaaiGaciGacmaaceqaaeaacaabaaGcbaGaamisamaaBaaaleaaii aacaWFJbacbaGaa4Nmaaqabaaaaa@35A9@

Note 1 à l’article: Si le champ magnétique est parallèle à la surface de l'échantillon, la supraconductivité de surface apparaît dans une plage de champs magnétiques allant de H c2 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garmWu51MyVXgarqqtubsr4rNCHbGe aGqipG0dh9qqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm 0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9ad baqaaiGaciGacmaaceqaaeaacaabaaGcbaqcaaKaamisaOWaaSbaaK qaafaaiiaacaWFJbacbaGaa4Nmaaqabaaaaa@363B@ à H c3 1,695 H c2 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garmWu51MyVXgarqqtubsr4rNCHbGe aGqipG0dh9qqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm 0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9ad baqaaiGaciGacmaaceqaaeaacaabaaGcbaqcaaKaamisaOWaaSbaaK qaafaaiiaacaWFJbacbaGaa43maaqabaqcaaKaeyisISRaaGymaiaa cYcacaaI2aGaaGyoaiaaiwdacaaMc8UaamisaOWaaSbaaKqaafaaca WFJbGaa4Nmaaqabaaaaa@4046@ pour des supraconducteurs de type II et de H c MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garmWu51MyVXgarqqtubsr4rNCHbGe aGqipG0dh9qqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm 0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9ad baqaaiGaciGacmaaceqaaeaacaabaaGcbaqcaaKaamisaOWaaSbaaK qaafaaiiaacaWFJbaabeaaaaa@3580@ à H c3 2,40 H c MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garmWu51MyVXgarqqtubsr4rNCHbGe aGqipG0dh9qqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm 0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9ad baqaaiGaciGacmaaceqaaeaacaabaaGcbaqcaaKaamisaOWaaSbaaK qaafaaiiaacaWFJbacbaGaa43maaqabaqcaaKaeyisISRaaGOmaiaa cYcacaaI0aGaaGimaiaaykW7caWGibGcdaWgaaqcbauaaiaa=ngaae qaaaaa@3ECB@ pour des supraconducteurs de type I.

Note 2 à l’article: Cet article était numéroté 815-10-41 dans l’IEC 60050-815:2015.


ar
موصلية فائقة سطحية

de
Oberflächensupraleitung, f

es
superconductividad superficial, f

it
superconduttività di superficie

ja
表面超電導

pl
nadprzewodnictwo powierzchniowe, n

pt
supercondutividade de superfície

zh
表面超导电性

Publication date: 2024-08
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