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Author Kaganov, M. L.; Lifshitz, I. M.; Tanatarov, L. V.
Title Relaxation between electrons and the crystalline lattice Type Journal Article
Year (up) 1957 Publication Sov. Phys. JETP Abbreviated Journal Sov. Phys. JETP
Volume 4 Issue 2 Pages 173-178
Keywords HEB, nonlinear equations, numerical model
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Notes Approved no
Call Number Serial 894
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Author Bardeen, J.; Cooper, L. N.; Schrieffer, J. R.
Title Microscopic theory of superconductivity Type Journal Article
Year (up) 1957 Publication Phys. Rev. Abbreviated Journal Phys. Rev.
Volume 106 Issue Pages 162-164
Keywords BCS
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Notes Approved no
Call Number Serial 900
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Author Bardeen, J.; Cooper, L. N.; Schrieffer, J. R.
Title Theory of superconductivity Type Journal Article
Year (up) 1957 Publication Phys. Rev. Abbreviated Journal Phys. Rev.
Volume 108 Issue 5 Pages 1175-1204
Keywords BCS
Abstract A theory of superconductivity is presented, based on the fact that the interaction between electrons resulting from virtual exchange of phonons is attractive when the energy difference between the electrons states involved is less than the phonon energy, â„<8f>ω. It is favorable to form a superconducting phase when this attractive interaction dominates the repulsive screened Coulomb interaction. The normal phase is described by the Bloch individual-particle model. The ground state of a superconductor, formed from a linear combination of normal state configurations in which electrons are virtually excited in pairs of opposite spin and momentum, is lower in energy than the normal state by amount proportional to an average (â„<8f>ω)2, consistent with the isotope effect. A mutually orthogonal set of excited states in one-to-one correspondence with those of the normal phase is obtained by specifying occupation of certain Bloch states and by using the rest to form a linear combination of virtual pair configurations. The theory yields a second-order phase transition and a Meissner effect in the form suggested by Pippard. Calculated values of specific heats and penetration depths and their temperature variation are in good agreement with experiment. There is an energy gap for individual-particle excitations which decreases from about 3.5kTc at T=0°K to zero at Tc. Tables of matrix elements of single-particle operators between the excited-state superconducting wave functions, useful for perturbation expansions and calculations of transition probabilities, are given.
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Notes Approved no
Call Number Serial 901
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Author Bremer, J. W.; Newhouse, V. L.
Title Type Journal Article
Year (up) 1958 Publication Phys. Rev. Lett. Abbreviated Journal
Volume 1 Issue Pages 282
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Address Bremer, J. W.; Newhouse, V. L.
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Call Number MSPU @ s @ bremer_prl_1958 Serial 215
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Author Bardeen, J; Mattis, D. C.
Title Theory of the anomalous skin effect in normal and superconducting metals Type Journal Article
Year (up) 1958 Publication Phys. Rev. Abbreviated Journal Phys. Rev.
Volume 111 Issue 2 Pages 412-417
Keywords local dirty limit, complex conductivity, HEB
Abstract Chambers' expression for the current density in a normal metal in which the electric field varies over a mean free path is derived from a quantum approach in which use is made of the density matrix in the presence of scattering centers but in the absence of the field. An approximate expression used for the latter is shown to reduce to one derived by Kohn and Luttinger for the case of weak scattering. A general space-and time-varying electromagnetic interaction is treated by first-order perturbation theory. The method is applied to superconductors, and a general expression derived for the kernel of the Pippard integral for fields of arbitrary frequency. The expressions derived can also be used to discuss absorption of electromagnetic radiation in thin superconducting films.
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Notes Approved no
Call Number Serial 937
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