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1.10 Type I superconductors
Superconductors can be categorized into two classes, type I and type II. The ratio(1.7.5)of the penetration depthλto the superconducting coherence length ξ is called as the Ginzburg-Landau(GL)parameterκ,which determines whether a material is type I or type II superconductor.For type I superconductors this ratio is
![](https://epubservercos.yuewen.com/F84C83/15279429905177406/epubprivate/OEBPS/Images/figure1_0030_0043.jpg?sign=1739258806-PGnJek6pumhqurDh5FnpzYvklq9QO9my-0-49cc93e8502b480b9d57b66b8905c1a3)
and for type II superconductors,
![](https://epubservercos.yuewen.com/F84C83/15279429905177406/epubprivate/OEBPS/Images/figure1_0030_0044.jpg?sign=1739258806-AYxJ3OBKCzWkqy0b5NQcZqZtfRCMsM8O-0-ed863170f6a7a50039d285f5e1cbf4fc)
Most pure elemental superconductors, except niobium and carbon nanotubes, are type I superconductors, while almost all impure and compound superconductors are type II superconductors. Type 1.5 superconductor refers to a multicomponent superconductor which is characterized by two or more coherence lengths, and ξ 1 <
Superconducting materials that completely expel magnetic flux until they be come completely normal are called as type I superconductors. The superconduc tor is in the Meissner-Ochsenfeld state at small magnetic field.The Meissner Ochsenfeld state breaks down when the applied magnetic field has a certain larger value.