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超导物理的发展

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发信人: Solo (solo~~戴着枷锁跳舞), 信区: Physics/ T1 X5 a8 Z1 _8 p' ] 标 题: 超导物理的发展 & Q# M- P% z! L( W发信站: 异域桃源 (Thu Jan 31 21:58:35 2002), 转信4 u) w: r) [) n! X1 I2 ]3 R; W % R2 j+ p6 _8 `6 f 顾名思义,超导体是指在低温下(一个临界温度,$T_C$,以下)电阻为零的一类导体 O5 \0 ?/ I$ Z5 Q* A7 i5 \+ g' B# \( n/ \1 R4 x 在Kamerlingh Onnes发现Hg的超导电性之后,又接连发现多种金属、% F/ W3 O* H. A6 X8 w 合金在低温下都有这种超导现象产生。因此,零电阻(完全导体)成为超导体的第一个4 {! m. Y2 O1 Y3 B& ` 标志。 & a- |+ h8 k z第二个被发现的特征标志是超导体的完全抗磁性,也就是Meissner效应。& A8 W" R N' A5 D" i; x8 q 即使超导体在正常态时就处于磁场之中,当温度降低进入超导态时,磁力线也不会存在6 a5 R; s+ l2 |0 ~0 ? 于超* D- N7 L% ~6 N 导体穿透深度($\lambda$,典型值在500$\AA$左右)以内的部分。如果磁场大于一个临 + \) B% o# B. z* Y G$ s界磁场时,( R' m( }0 \; G7 G4 F" s 超导态就被破坏。从热力学的角度来看,也就是超导态的自由能比正常态的自由能要低 , F8 X8 \; u$ D \0 C+ V( `1 f* M/ Z! Y% m- I) B9 h* @/ G\begin{equation} 7 s" u" }) |' r{{H_C}^2(T) \over {8 \pi}} = f_n(T)-f_s(T) : h. }0 d) J5 D\end{equation}9 n) A7 T* I$ ^ 这里,$f_n$和$f_s$分别是零场下的正常态、超导态的单位体积的Helmholtz自由能。并! K. T. n. {2 R2 x- j6 b 且, ]5 X# F0 U# `% C$H_C(T)$与温度的关系可以用一个二次函数的经验公式来表述: - C' `7 R& K# R\begin{equation} ! E3 i- q1 R6 [! ~9 A) i3 c! z{H_C}(T) \approx H_C(0)[1-(T/T_C)^2]5 D; r5 u( u ]# A3 } \end{equation}

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    根据哲学,我猜测有低温超导,也有高温超导。

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    请问高温状态下有没有类似的现象?有没有这方面的研究报告?

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    超导常用链接

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    Pictures/Graphics/Animations:

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  • Micro-photographs of Superconducting Materials | FSU Gallery ; J1 X) ?: e/ B) `% T- |3 G1 t" R! t1 ]" _$ z: P5 ~. I$ x
  • Micro-photographs of Flux Lattices | Bell Labs Gallery Z; Y+ m2 ]* Z. W4 w( n6 W" f8 z& e/ L
  • Superconductor Animations and 3-D Figures | University of Texas at Austin 9 i8 W" c. v% x( K ) m, c8 t) u/ H( f9 m
  • Stripes and Vortices in Motion | University of Michigan 5 c( c7 S$ y5 f& Y9 f) R ) j E# N/ c: ?+ A9 c
  • Perovskite Structures | Center for Computational Materials Science s8 m0 f( w; C9 g; M) P Z, O" @ ) w8 J+ Y' |9 q
  • Figures of Superconductor Molecules | ILL Research Institute - France 6 l6 r" X# `; v1 M. @0 g 8 N/ l" D% K( d
  • Crystal Atomic Lattice Viewer | University of Leicester - UK 1 [! U4 J; |+ F* ~1 ], Z7 _7 B2 J' M/ s
  • Type 2 Vortex Twisters | IGA Nanomechanics - Switzerland $ S7 y* j- |1 O+ B3 Q1 G9 P' [* u& O- H
  • Scanning Squid Images | IBM Research (slow - graphics intensive) " K. k6 } p: V# E: Y & S2 Y- `% K/ y7 o% Q
  • Perovskite & Other Structures | University of Oxford (slow - graphics intensive) - UK u; F N; |2 K! y2 l1 } : t( q% p; b# t% j
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  • Superconductivity In Its Simplest Form | Oxford University : c+ l$ ?3 A# c # y$ G6 y" e8 f
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  • Oxide Superconductors Tutorial | by Bob Cava of Princeton University for the American Ceramic Society , p* x% e9 }& s, w G4 p 8 A/ ]1 E0 y( O- d4 d
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  • NIST Superconducting Materials Database | National Institute of Standards and Technology - ]* s$ ]7 ?5 A+ M / ?/ F1 {1 h1 V7 S5 K
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    Research Groups and Institutions:

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  • International Workshop on High Temperature Superconductors | June 24 - 30, 2001, Moscow, Russia + P: Y( H) Q( ?+ t6 [2 `( ~+ k : P5 P) U; q D; V
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