By Henri Poincaré

ISBN-10: 2876470284

ISBN-13: 9782876470286

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Rev. Lett. 74, 1657 (1995). [7] P. Fulde, A. Ferrell, Phys. Rev. 135, A550 (1964). [8] A. Larkin, Y. Ovchinnikov, Sov. Phys. JETP 20, 762 (1965). [9] A. I. Buzdin, L. N. Bulaevskii, S. V. Panyukov, JETP Lett. 35, 178 (1982); A. I. Buzdin, M. V. Kuprianov, JETP Lett. 52, 487 (1990). [10] Z. Radovi´c, M. Ledvij, L. Dobrosavljevi´c-Gruji´c, A. I. Buzdin, J. C. Clem, Phys. Rev. B44, 759 (1991). [11] E. A. Demler, G. B. Arnold, M. R. Beasley, Phys. Rev. B55, 15 174 (1997). 16 Fulde-Ferrell-Larkin-Ovchinnikov-like state in FM - SC Proximity System [12] Y.

It is readily seen that G(V ) is asymmetrical, contrary to what is appropriate for superconductors [67]. Mathematically it stems from an almost total compensation between Gd(V ) and Gib(V ) peculiarities at voltages of one sign and their enhancement at voltages of the other sign (for the adopted choice Σ > 0 it means negative and positive V , respectively). In the absence of the external magnetic ﬁeld and spin polarization this result was obtained by us earlier [61, 62]. When H is switched on, the electronic DOS peak splits as in the case of superconductors [1, 18].

And Mathon, G. (1999) Spin polarized tunneling in ferromagnetic junctions, J. Magn. Magn. Materials 200, 248–273. [33] Zhang, X-G. and Butler, W. H. (2003) Band structure, evanescent states, and transport in spin tunnel junctions, J. : Condens. Matter 15, R1603–R1639. 40 Spin-dependent Tunnel Currents for Metals or Superconductors [34] Bilbro, G. and McMillan, W. L. (1976) Theoretical model of superconductivity and the martensitic transformation in A15 compounds, Phys. Rev. B14, 1887– 1892. [35] Halperin, B.

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