Electrical and optical properties of epitaxial YHx switchable mirrors
In 1996, Huiberts et al. discovered that polycrystalline Y and La films, covered with a thin Pd layer, switch reversibly from shiny metallic to transparent semiconductors upon H absorption. Epitaxial YHx switchable mirrors are characterized by micrometer-size domains delineated by a self-organized t...
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Veröffentlicht in: | Journal of alloys and compounds 2005-07, Vol.397 (1-2), p.9-16 |
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container_title | Journal of alloys and compounds |
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creator | ENACHE, S LEEUWERINK, T HOEKSTRA, A. F. Th REMHOF, A KOEMAN, N. J DAM, B GRIESSEN, R |
description | In 1996, Huiberts et al. discovered that polycrystalline Y and La films, covered with a thin Pd layer, switch reversibly from shiny metallic to transparent semiconductors upon H absorption. Epitaxial YHx switchable mirrors are characterized by micrometer-size domains delineated by a self-organized triangular network of ridges. On a macroscopic scale, the epitaxial films exhibit similar optical switching properties as the polycrystalline ones constituted of nanometer-size domains, although the microscopic domains switch independently. Their electrical transport properties are, however, different from those of polycrystalline films. Near the trihydride state, although the optical gaps of epitaxial and polycrystalline films are essentially the same, the electrical resistivity of epitaxial films is much lower. This is due to the metallic ridges in the epitaxial films, which are also responsible for a large in-plane anisotropy of the Hall voltage (i.e., up to 35% at 3 K in YH,3). In the dihydride state, the temperature dependence of the optical transmission of both films is reminiscent of that exhibited by their electrical conductivity, Q(T). These features can be understood in a Drude model for free electrons, in which the only temperature-dependent parameter is the scattering time, r. |
doi_str_mv | 10.1016/j.jallcom.2005.01.039 |
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F. Th ; REMHOF, A ; KOEMAN, N. J ; DAM, B ; GRIESSEN, R</creator><creatorcontrib>ENACHE, S ; LEEUWERINK, T ; HOEKSTRA, A. F. Th ; REMHOF, A ; KOEMAN, N. J ; DAM, B ; GRIESSEN, R</creatorcontrib><description>In 1996, Huiberts et al. discovered that polycrystalline Y and La films, covered with a thin Pd layer, switch reversibly from shiny metallic to transparent semiconductors upon H absorption. Epitaxial YHx switchable mirrors are characterized by micrometer-size domains delineated by a self-organized triangular network of ridges. On a macroscopic scale, the epitaxial films exhibit similar optical switching properties as the polycrystalline ones constituted of nanometer-size domains, although the microscopic domains switch independently. Their electrical transport properties are, however, different from those of polycrystalline films. Near the trihydride state, although the optical gaps of epitaxial and polycrystalline films are essentially the same, the electrical resistivity of epitaxial films is much lower. This is due to the metallic ridges in the epitaxial films, which are also responsible for a large in-plane anisotropy of the Hall voltage (i.e., up to 35% at 3 K in YH,3). In the dihydride state, the temperature dependence of the optical transmission of both films is reminiscent of that exhibited by their electrical conductivity, Q(T). These features can be understood in a Drude model for free electrons, in which the only temperature-dependent parameter is the scattering time, r.</description><identifier>ISSN: 0925-8388</identifier><identifier>EISSN: 1873-4669</identifier><identifier>DOI: 10.1016/j.jallcom.2005.01.039</identifier><language>eng</language><publisher>Lausanne: Elsevier</publisher><subject>Condensed matter: electronic structure, electrical, magnetic, and optical properties ; Exact sciences and technology ; Optical properties and condensed-matter spectroscopy and other interactions of matter with particles and radiation ; Physics</subject><ispartof>Journal of alloys and compounds, 2005-07, Vol.397 (1-2), p.9-16</ispartof><rights>2005 INIST-CNRS</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c314t-26604cecf1394fd15e0c3e7bca699231bde35a97e9cdd366581aff8911df4bb23</citedby><cites>FETCH-LOGICAL-c314t-26604cecf1394fd15e0c3e7bca699231bde35a97e9cdd366581aff8911df4bb23</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27924,27925</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=16885429$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>ENACHE, S</creatorcontrib><creatorcontrib>LEEUWERINK, T</creatorcontrib><creatorcontrib>HOEKSTRA, A. 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Near the trihydride state, although the optical gaps of epitaxial and polycrystalline films are essentially the same, the electrical resistivity of epitaxial films is much lower. This is due to the metallic ridges in the epitaxial films, which are also responsible for a large in-plane anisotropy of the Hall voltage (i.e., up to 35% at 3 K in YH,3). In the dihydride state, the temperature dependence of the optical transmission of both films is reminiscent of that exhibited by their electrical conductivity, Q(T). These features can be understood in a Drude model for free electrons, in which the only temperature-dependent parameter is the scattering time, r.</description><subject>Condensed matter: electronic structure, electrical, magnetic, and optical properties</subject><subject>Exact sciences and technology</subject><subject>Optical properties and condensed-matter spectroscopy and other interactions of matter with particles and radiation</subject><subject>Physics</subject><issn>0925-8388</issn><issn>1873-4669</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2005</creationdate><recordtype>article</recordtype><recordid>eNpFkEFLxDAQhYMouK7-BKEXvbVmmjZNjrJUV1jwogdPIU0nmJJua9LF9d_bdRc8zTC8N_PmI-QWaAYU-EOXddp7M_RZTmmZUcgok2dkAaJiacG5PCcLKvMyFUyIS3IVY0cpBclgQerao5mCM9onetsmwzj99WMYRgyTw5gMNsHRTXrv5vnHep_EbzeZT914THoXwhDiNbmw2ke8OdUleX-q31brdPP6_LJ63KSGQTGlOee0MGgsMFnYFkqkhmHVGM2lzBk0LbJSywqlaVvGeSlAWyskQGuLpsnZktwf987xvnYYJ9W7aNB7vcVhF1U-f1yArGZheRSaMMQY0KoxuF6HHwVUHaCpTp2gqQM0RUHN0Gbf3emAjjMGG_TWuPhv5kKURS7ZL09UcI4</recordid><startdate>20050719</startdate><enddate>20050719</enddate><creator>ENACHE, S</creator><creator>LEEUWERINK, T</creator><creator>HOEKSTRA, A. 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Their electrical transport properties are, however, different from those of polycrystalline films. Near the trihydride state, although the optical gaps of epitaxial and polycrystalline films are essentially the same, the electrical resistivity of epitaxial films is much lower. This is due to the metallic ridges in the epitaxial films, which are also responsible for a large in-plane anisotropy of the Hall voltage (i.e., up to 35% at 3 K in YH,3). In the dihydride state, the temperature dependence of the optical transmission of both films is reminiscent of that exhibited by their electrical conductivity, Q(T). These features can be understood in a Drude model for free electrons, in which the only temperature-dependent parameter is the scattering time, r.</abstract><cop>Lausanne</cop><pub>Elsevier</pub><doi>10.1016/j.jallcom.2005.01.039</doi><tpages>8</tpages></addata></record> |
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subjects | Condensed matter: electronic structure, electrical, magnetic, and optical properties Exact sciences and technology Optical properties and condensed-matter spectroscopy and other interactions of matter with particles and radiation Physics |
title | Electrical and optical properties of epitaxial YHx switchable mirrors |
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