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On the theory of superconducitivity. (English) Zbl 0067.23504

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[1] F. London:Superfluids, vol. I (1950).
[2] V. L. Ginzburg andL. D. Landau:Žu. Eksper. Teor. Fiz.,20, 1064 (1950).
[3] V. L. Ginzburg:Usp. Fiz. Nauk,42, 169, 333 (1950). Translation inAbhandlungen aus der sowjetischen Physik, Folge II (Berlin, 1951), p. 135.
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[8] A. V. Gurevič:Žu. Eksper. Teor. Fiz.,27, 195 (1954).
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[10] L. D. Landau andE. M. Lifšic:Statistical Physics (Moscow, 1951), chap. XIV.
[11] V. L. Ginzburg:Journ. of Phys. USSR,10, 107 (1946);Žu. Eksper. Teor. Fiz.,17, 883 (1947);19, 36 (1949);Usp. Fiz. Nauk,38, 490 (1949).
[12] The condition (11) automatically follows from the variation principle if no auxiliary conditions restricts \(\psi\) on the boundary: that is the case considered here (2).
[13] J. Bardeen:Phys. Rev.,94, 554 (1954). · Zbl 0059.22501 · doi:10.1103/PhysRev.94.554
[14] The casex is being considered here; about corrections containingx see (8). Forx 0 in the film \(\psi\)=\(\psi\)0=const, i.e. \(\psi\) is independent ofz.
[15] N. V. Zavarickij:Dokl. Akad. Nauk SSSR,78, 665 (1951);85, 749 (1952).
[16] A. B. Pippard:Proc. Roy. Soc., A.216, 547 (1953);Physica,19, 765 (1953).
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[19] V. L. Ginzburg:Žu. Eksper. Teor. Fiz.,21, 979 (1951).
[20] A. A. Abrikosov:Dokl. Akad. Nauk SSSR,86, 43 (1952).
[21] The relation (34) can be obtained from experimental facts even without verifying the validity of equation (1) from which the expression (34) follows directly (see (4) and (29)).
[22] V. L. Ginzburg andG. P. Motulevič:Usp. Fiz. Nauk,55, 469 (1955).
[23] According to (20). for tin\(\lambda\) c<0.83 cm; measurements for lower wave lengths and for other metals are not available although the corresponding experiments are quite possible and their importance was emphasized over 10 years ago (see (21)).
[24] E. Fawcett:Proc. Phys. Soc., A66, 1071 (1953).
[25] V. L. Ginzburg:Žu. Eksper. Teor. Fiz.,14, 134 (1944).
[26] V. L. Ginzburg:Usp. Fiz. Nauk,48, 25 (1952); Translation inFortschritte der Physik (Berlin),1, 101 (1953). · Zbl 0053.48203
[27] H. Koppe:Erg. der exakten Naturwiss.,23, 283 (1950). · doi:10.1007/BFb0109284
[28] M. R. Schafroth:Phys. Rev.,96, 1149, 1442 (1954). · doi:10.1103/PhysRev.96.1149
[29] H. Fröhlich:Phys. Rev.,79, 845 (1950);Proc. Phys. Soc., A64, 129 (1951). · Zbl 0037.43003 · doi:10.1103/PhysRev.79.845
[30] J. Bardeen:Rev. Mod. Phys.,23, 261 (1951). · Zbl 0044.45204 · doi:10.1103/RevModPhys.23.261
[31] M. R. Schafroth:Helv. Phys. Acta,24, 667 (1951);Nuovo Cimento,9, 291 (1952).
[32] An exclusion in this respect is the investigation ofH. Fröhlich:Proc. Roy. Soc.,223, 296 (1954) in which, however, only the one-dimensional case is considered. · Zbl 0055.44105 · doi:10.1098/rspa.1954.0116
[33] W. S. Corak, B. B. Goodman, G. B. Satterthwaite andA. Wexler:Phys. Rev.,96, 1442 (1954). · doi:10.1103/PhysRev.96.1442.2
[34] L. D. Landau:Journ. of Phys. USSR,5, 71 (1941);11, 91 (1947).
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