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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author Ekino, T.
Gabovich, A.M.
Voitenko, A.I.
author_facet Ekino, T.
Gabovich, A.M.
Voitenko, A.I.
citation_txt 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.
collection DSpace DC
container_title Физика низких температур
description 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.
first_indexed 2025-11-28T13:39:04Z
format Article
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institution Digital Library of Periodicals of National Academy of Sciences of Ukraine
issn 0132-6414
language English
last_indexed 2025-11-28T13:39:04Z
publishDate 2005
publisher Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України
record_format dspace
spelling Ekino, T.
Gabovich, A.M.
Voitenko, A.I.
2017-06-12T19:36:11Z
2017-06-12T19:36:11Z
2005
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.
0132-6414
PACS: 71.45.Lr, 73.40.Gk, 75.20.En, 75.47.Np
https://nasplib.isofts.kiev.ua/handle/123456789/120777
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.
en
Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України
Физика низких температур
Электpонные свойства металлов и сплавов
Spin-polarized electron tunneling between charge-density-wave metals
Article
published earlier
spellingShingle Spin-polarized electron tunneling between charge-density-wave metals
Ekino, T.
Gabovich, A.M.
Voitenko, A.I.
Электpонные свойства металлов и сплавов
title Spin-polarized electron tunneling between charge-density-wave metals
title_full Spin-polarized electron tunneling between charge-density-wave metals
title_fullStr Spin-polarized electron tunneling between charge-density-wave metals
title_full_unstemmed Spin-polarized electron tunneling between charge-density-wave metals
title_short Spin-polarized electron tunneling between charge-density-wave metals
title_sort spin-polarized electron tunneling between charge-density-wave metals
topic Электpонные свойства металлов и сплавов
topic_facet Электpонные свойства металлов и сплавов
url https://nasplib.isofts.kiev.ua/handle/123456789/120777
work_keys_str_mv AT ekinot spinpolarizedelectrontunnelingbetweenchargedensitywavemetals
AT gabovicham spinpolarizedelectrontunnelingbetweenchargedensitywavemetals
AT voitenkoai spinpolarizedelectrontunnelingbetweenchargedensitywavemetals