By Henri Poincaré
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Extra resources for Électricité et optique
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It is readily seen that G(V ) is asymmetrical, contrary to what is appropriate for superconductors . 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.  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  Bilbro, G. and McMillan, W. L. (1976) Theoretical model of superconductivity and the martensitic transformation in A15 compounds, Phys. Rev. B14, 1887– 1892.  Halperin, B.
Électricité et optique by Henri Poincaré