Spin-polarized electron tunneling between charge-density-wave metals

For junctions between metals partially gapped by charge density waves (CDWs), the quasiparticle tunnel currents J(V) and conductances G(V) in external magnetic fields H are calculated as functions of H, the bias voltage V, temperature T, the dielectric gaps ∑, and the gapped portions
 μ of t...

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Published in:Физика низких температур
Date:2005
Main Authors: Ekino, T., Gabovich, A.M., Voitenko, A.I.
Format: Article
Language:English
Published: Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України 2005
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Online Access:https://nasplib.isofts.kiev.ua/handle/123456789/120777
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Journal Title:Digital Library of Periodicals of National Academy of Sciences of Ukraine
Cite this:Spin-polarized electron tunneling between charge-density-wave metals / T. Ekino, A.M. Gabovich, and A.I. Voitenko // Физика низких температур. — 2005. — Т. 31, № 1. — С. 77-93. — Бібліогр.: 93 назв. — англ.

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Digital Library of Periodicals of National Academy of Sciences of Ukraine
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Summary:For junctions between metals partially gapped by charge density waves (CDWs), the quasiparticle tunnel currents J(V) and conductances G(V) in external magnetic fields H are calculated as functions of H, the bias voltage V, temperature T, the dielectric gaps ∑, and the gapped portions
 μ of the Fermi surface (FS). The paramagnetic effect of H is taken into account, whereas orbital
 effects are neglected. General expressions are obtained for different CDW metal electrodes.
 Analytical formulas are obtained for T = 0. Explicit numerical calculations are carried out for symmetrical
 junctions. The results are substantially unlike those for junctions between superconductors.
 It is shown that due to the interplay between quasiparticles from nested and non-nested FS
 sections the junction properties involve features appropriate to both symmetrical and asymmetrical
 setups. In particular, for H = 0 discontinuities at eV = ±2∑ and square-root singularities at eV = ±∑
 should coexist. Here e is the elementary charge. For H ≠ 0 the former remain intact, while the latter
 split. It is suggested to use the splitting as a verification of the CDW nature of the pseudogap
 in high-Tc superconducting oxides.
ISSN:0132-6414