Surface electromagnetic modes in layered conductors in a magnetic field

A transfer-matrix approach is developed for studies of the collective electromagnetic modes in a semi-infinite layered conductor subjected to a quantizing external magnetic field perpendicular to the layers. The dispersion relations for the surface and bulk modes are derived. It is shown that the su...

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Дата:2000
Автор: Gvozdikov, V.M.
Формат: Стаття
Мова:English
Опубліковано: Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України 2000
Назва видання:Физика низких температур
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Онлайн доступ:http://dspace.nbuv.gov.ua/handle/123456789/129164
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Назва журналу:Digital Library of Periodicals of National Academy of Sciences of Ukraine
Цитувати:Surface electromagnetic modes in layered conductors in a magnetic field / V.M. Gvozdikov // Физика низких температур. — 2000. — Т. 26, № 8. — С. 776-786. — Бібліогр.: 29 назв. — англ.

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Digital Library of Periodicals of National Academy of Sciences of Ukraine
id irk-123456789-129164
record_format dspace
spelling irk-123456789-1291642018-01-17T03:04:52Z Surface electromagnetic modes in layered conductors in a magnetic field Gvozdikov, V.M. Электpонные свойства металлов и сплавов A transfer-matrix approach is developed for studies of the collective electromagnetic modes in a semi-infinite layered conductor subjected to a quantizing external magnetic field perpendicular to the layers. The dispersion relations for the surface and bulk modes are derived. It is shown that the surface mode has a gap in the long-wavelength limit and exists only if the absolute value of the in-plane wave vector q exceeds the threshold value q*=−1/(a ln|Δ|). Depending on the sign of the parameter Δ=(ε−ε₀)/(ε₀+ε), the frequency of the surface mode ωs(q,Δ) goes either above (for Δ>0) or below (for Δ<0) the bulk-mode frequency ω(q,k)=ω(q,k+2π/a) for any value of k. At nonzero magnetic field H the bulk mode has a singular point q₀(H) at which the bulk band twists in such a way that its top and bottom bounds swap. Small variations of q near this point change dramatically the shape of the dispersion function ω(q,k) in the variable k. The surface mode has no dispersion across the layers, since its amplitude decays exponentially into the bulk of the sample. Both bulk and surface modes have in the region qa≫1 a similar asymptotic behavior ω∝q¹/², but ωs(q,Δ) lies above or below ω(q,k), respectively, for Δ>0 and Δ<0 (a is the interlayer separation; ε0 and ε stand for the dielectric constants of the media outside the sample and between the layers; q and k are the components of the wave vector in the plane and perpendicular to the layers, respectively). 2000 Article Surface electromagnetic modes in layered conductors in a magnetic field / V.M. Gvozdikov // Физика низких температур. — 2000. — Т. 26, № 8. — С. 776-786. — Бібліогр.: 29 назв. — англ. 0132-6414 PACS: 73.20.Dx, 73.20.Mf http://dspace.nbuv.gov.ua/handle/123456789/129164 en Физика низких температур Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України
institution Digital Library of Periodicals of National Academy of Sciences of Ukraine
collection DSpace DC
language English
topic Электpонные свойства металлов и сплавов
Электpонные свойства металлов и сплавов
spellingShingle Электpонные свойства металлов и сплавов
Электpонные свойства металлов и сплавов
Gvozdikov, V.M.
Surface electromagnetic modes in layered conductors in a magnetic field
Физика низких температур
description A transfer-matrix approach is developed for studies of the collective electromagnetic modes in a semi-infinite layered conductor subjected to a quantizing external magnetic field perpendicular to the layers. The dispersion relations for the surface and bulk modes are derived. It is shown that the surface mode has a gap in the long-wavelength limit and exists only if the absolute value of the in-plane wave vector q exceeds the threshold value q*=−1/(a ln|Δ|). Depending on the sign of the parameter Δ=(ε−ε₀)/(ε₀+ε), the frequency of the surface mode ωs(q,Δ) goes either above (for Δ>0) or below (for Δ<0) the bulk-mode frequency ω(q,k)=ω(q,k+2π/a) for any value of k. At nonzero magnetic field H the bulk mode has a singular point q₀(H) at which the bulk band twists in such a way that its top and bottom bounds swap. Small variations of q near this point change dramatically the shape of the dispersion function ω(q,k) in the variable k. The surface mode has no dispersion across the layers, since its amplitude decays exponentially into the bulk of the sample. Both bulk and surface modes have in the region qa≫1 a similar asymptotic behavior ω∝q¹/², but ωs(q,Δ) lies above or below ω(q,k), respectively, for Δ>0 and Δ<0 (a is the interlayer separation; ε0 and ε stand for the dielectric constants of the media outside the sample and between the layers; q and k are the components of the wave vector in the plane and perpendicular to the layers, respectively).
format Article
author Gvozdikov, V.M.
author_facet Gvozdikov, V.M.
author_sort Gvozdikov, V.M.
title Surface electromagnetic modes in layered conductors in a magnetic field
title_short Surface electromagnetic modes in layered conductors in a magnetic field
title_full Surface electromagnetic modes in layered conductors in a magnetic field
title_fullStr Surface electromagnetic modes in layered conductors in a magnetic field
title_full_unstemmed Surface electromagnetic modes in layered conductors in a magnetic field
title_sort surface electromagnetic modes in layered conductors in a magnetic field
publisher Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України
publishDate 2000
topic_facet Электpонные свойства металлов и сплавов
url http://dspace.nbuv.gov.ua/handle/123456789/129164
citation_txt Surface electromagnetic modes in layered conductors in a magnetic field / V.M. Gvozdikov // Физика низких температур. — 2000. — Т. 26, № 8. — С. 776-786. — Бібліогр.: 29 назв. — англ.
series Физика низких температур
work_keys_str_mv AT gvozdikovvm surfaceelectromagneticmodesinlayeredconductorsinamagneticfield
first_indexed 2023-10-18T20:57:05Z
last_indexed 2023-10-18T20:57:05Z
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