Critical Magnetic Field临界磁场
The superconducting state cannot exist in the presence of a magnetic field greater than a critical value, even at absolute zero. This critical magnetic field is strongly correlated with the critical temperature for the superconductor, which is in turn correlated with the bandgap. Type II superconductors show two critical magnetic field values, one at the onset of a mixed superconducting and normal state and one where superconductivity ceases. 超导态在存在超过临界值的磁场时无法存在,即使在绝对零度下也是如此。这个临界磁场与超导体的临界温度密切相关,而临界温度又与能带隙相关。II型超导体显示出两个临界磁场值,一个是在超导态和正常态开始混合时的值,另一个是超导性消失时的值。
![]() It is the nature of superconductors to exclude magnetic fields (Meissner effect) so long as the applied field does not exceed their critical magnetic field. This critical magnetic field is tabulated for 0K and decreases from that magnitude with increasing temperature, reaching zero at the critical temperature for superconductivity. The critical magnetic field at any temperature below the critical temperature is given by the relationship 超导体的性质是排斥磁场(迈斯纳效应),只要外加磁场不超过其临界磁场。这个临界磁场在0K时被列出,并且随着温度升高而减小,直到临界温度时降为零。在临界温度以下的任何温度,临界磁场由以下关系式给出:
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Index Superconductivity concepts Reference Rohlf,Ch 15 索引 超导概念 参考 Rohlf,第15章 | ||||
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Critical magnetic fields for superconductors超导体的临界磁场
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使超导态破坏所需的临界磁场与超导体的临界温度密切相关。这些参数可以被视为可以以某种方式供给材料的能,这种能会干扰超导机制。这与存在超导态与正常态之间的能隙这一想法是一致的。 |
Index Superconductivity concepts Reference Rohlf,Ch 15 索引 超导概念 参考 Rohlf,第15章 | ||||
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Phase Diagram Examples相图示例
The Type II superconductors have much higher critical magnetic fields than Type I, but for most of that field range they are mixtures of normal and superconducting. II型超导体的临界磁场远高于I型,但在这大部分磁场范围内,它们都是正常态和超导态的混合物。
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Index Superconductivity concepts Reference Rohlf,Ch 15 索引 超导概念 参考 Rohlf,第15章 | ||
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Vortex State for Superconductors超导体的涡流态
Type II superconductors usually exist in a vortex state with normal cores surrounded by superconducting regions. This allows magnetic field penetration. As their critical temperatures are approached, the normal cores are more closely packed and eventually overlap as the superconducting state is lost. II型超导体通常处于一种漩涡态,其中正常区域被超导区域包围。这允许磁场穿透。当接近临界温度时,正常区域更加紧密排列,最终会重叠,当超导态消失时。
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Index Superconductivity concepts Reference Rohlf,Ch 15 索引 超导概念 参考 Rohlf,第15章 | ||
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Vortex State for Superconductors超导体的涡流态
At the lower of the two critical magnetic fields in a Type II superconductor, magnetic fields begin to penetrate through cores of normal material surrounded by superconducting current vortices. As long as these vortices are stationary (pinned), the magnetic fields can penetrate while still maintaining zero electric resistivity paths through the material. A size of about 300 nm is typical for the normal cores. While the Meissner effect is modified to allow magnetic fields through the normal cores, magnetic fields are still excluded from the superconducting regions.
在Type II超导体的两个临界磁场中较低的一个下,磁场均开始穿透正常材料的芯部,这些芯部被超导电流涡旋所包围。只要这些涡旋保持静止(被钉扎),磁场均可以在保持材料中零电阻路径的同时穿透正常材料的芯部。正常芯部的尺寸通常约为300 nm。虽然迈斯纳效应被修改以允许磁场均通过正常芯部,但磁场均仍被排除在超导区域之外。 |
Index Superconductivity concepts Reference Rohlf,Ch 15 索引 超导概念 参考 Rohlf,第15章 | ||
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