Loading…

Generalized Maxwell Garnett equations for rough surfaces

An optical model of a rough surface is made up of a layer of metal particles of sizes much smaller than a wavelength, dispersed in a dielectric medium. The metal particles are approximated by a layer of dipoles of identical dipole moment arranged in square or hexagonal planar array. The two-dimensio...

Full description

Saved in:
Bibliographic Details
Published in:Journal of applied physics 1974-11, Vol.45 (11), p.5004-5007
Main Authors: Chan, E. C., Marton, J. P.
Format: Article
Language:English
Citations: Items that this one cites
Items that cite this one
Online Access:Get full text
Tags: Add Tag
No Tags, Be the first to tag this record!
cited_by cdi_FETCH-LOGICAL-c293t-93efb87ddff15ed5cd98828dceab97ee93fe36fccba2f8f11ee2fe77ea6f06563
cites cdi_FETCH-LOGICAL-c293t-93efb87ddff15ed5cd98828dceab97ee93fe36fccba2f8f11ee2fe77ea6f06563
container_end_page 5007
container_issue 11
container_start_page 5004
container_title Journal of applied physics
container_volume 45
creator Chan, E. C.
Marton, J. P.
description An optical model of a rough surface is made up of a layer of metal particles of sizes much smaller than a wavelength, dispersed in a dielectric medium. The metal particles are approximated by a layer of dipoles of identical dipole moment arranged in square or hexagonal planar array. The two-dimensional dipole-dipole interaction results in surface anisotropy represented by a pair of Maxwell Garnett-type equations. This surface anisotropy due to surface geometry may be a good indication of the degree of roughness of a given surface.
doi_str_mv 10.1063/1.1663173
format article
fullrecord <record><control><sourceid>crossref</sourceid><recordid>TN_cdi_crossref_primary_10_1063_1_1663173</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>10_1063_1_1663173</sourcerecordid><originalsourceid>FETCH-LOGICAL-c293t-93efb87ddff15ed5cd98828dceab97ee93fe36fccba2f8f11ee2fe77ea6f06563</originalsourceid><addsrcrecordid>eNotz8tKxDAUgOEgCtbRhW-QrYuOOQm5LWXQKoy4mVmXNDlHK7XVpMXL04s4q3_3w8fYJYg1CKOuYQ3GKLDqiFUgnK-t1uKYVUJIqJ23_pSdlfIqBIBTvmKuwRFzGPofTPwxfH3iMPAm5BHnmePHEuZ-GgunKfM8Lc8vvCyZQsRyzk4oDAUvDl2x_d3tbnNfb5-ah83Nto7Sq7n2CqlzNiUi0Jh0TN456VLE0HmL6BWhMhRjFyQ5AkCUhNZiMCSMNmrFrv6_MU-lZKT2PfdvIX-3INo_cgvtgax-ATe8Smo</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype></control><display><type>article</type><title>Generalized Maxwell Garnett equations for rough surfaces</title><source>AIP Digital Archive</source><creator>Chan, E. C. ; Marton, J. P.</creator><creatorcontrib>Chan, E. C. ; Marton, J. P.</creatorcontrib><description>An optical model of a rough surface is made up of a layer of metal particles of sizes much smaller than a wavelength, dispersed in a dielectric medium. The metal particles are approximated by a layer of dipoles of identical dipole moment arranged in square or hexagonal planar array. The two-dimensional dipole-dipole interaction results in surface anisotropy represented by a pair of Maxwell Garnett-type equations. This surface anisotropy due to surface geometry may be a good indication of the degree of roughness of a given surface.</description><identifier>ISSN: 0021-8979</identifier><identifier>EISSN: 1089-7550</identifier><identifier>DOI: 10.1063/1.1663173</identifier><language>eng</language><ispartof>Journal of applied physics, 1974-11, Vol.45 (11), p.5004-5007</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c293t-93efb87ddff15ed5cd98828dceab97ee93fe36fccba2f8f11ee2fe77ea6f06563</citedby><cites>FETCH-LOGICAL-c293t-93efb87ddff15ed5cd98828dceab97ee93fe36fccba2f8f11ee2fe77ea6f06563</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></links><search><creatorcontrib>Chan, E. C.</creatorcontrib><creatorcontrib>Marton, J. P.</creatorcontrib><title>Generalized Maxwell Garnett equations for rough surfaces</title><title>Journal of applied physics</title><description>An optical model of a rough surface is made up of a layer of metal particles of sizes much smaller than a wavelength, dispersed in a dielectric medium. The metal particles are approximated by a layer of dipoles of identical dipole moment arranged in square or hexagonal planar array. The two-dimensional dipole-dipole interaction results in surface anisotropy represented by a pair of Maxwell Garnett-type equations. This surface anisotropy due to surface geometry may be a good indication of the degree of roughness of a given surface.</description><issn>0021-8979</issn><issn>1089-7550</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1974</creationdate><recordtype>article</recordtype><recordid>eNotz8tKxDAUgOEgCtbRhW-QrYuOOQm5LWXQKoy4mVmXNDlHK7XVpMXL04s4q3_3w8fYJYg1CKOuYQ3GKLDqiFUgnK-t1uKYVUJIqJ23_pSdlfIqBIBTvmKuwRFzGPofTPwxfH3iMPAm5BHnmePHEuZ-GgunKfM8Lc8vvCyZQsRyzk4oDAUvDl2x_d3tbnNfb5-ah83Nto7Sq7n2CqlzNiUi0Jh0TN456VLE0HmL6BWhMhRjFyQ5AkCUhNZiMCSMNmrFrv6_MU-lZKT2PfdvIX-3INo_cgvtgax-ATe8Smo</recordid><startdate>19741101</startdate><enddate>19741101</enddate><creator>Chan, E. C.</creator><creator>Marton, J. P.</creator><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>19741101</creationdate><title>Generalized Maxwell Garnett equations for rough surfaces</title><author>Chan, E. C. ; Marton, J. P.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c293t-93efb87ddff15ed5cd98828dceab97ee93fe36fccba2f8f11ee2fe77ea6f06563</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1974</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Chan, E. C.</creatorcontrib><creatorcontrib>Marton, J. P.</creatorcontrib><collection>CrossRef</collection><jtitle>Journal of applied physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Chan, E. C.</au><au>Marton, J. P.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Generalized Maxwell Garnett equations for rough surfaces</atitle><jtitle>Journal of applied physics</jtitle><date>1974-11-01</date><risdate>1974</risdate><volume>45</volume><issue>11</issue><spage>5004</spage><epage>5007</epage><pages>5004-5007</pages><issn>0021-8979</issn><eissn>1089-7550</eissn><abstract>An optical model of a rough surface is made up of a layer of metal particles of sizes much smaller than a wavelength, dispersed in a dielectric medium. The metal particles are approximated by a layer of dipoles of identical dipole moment arranged in square or hexagonal planar array. The two-dimensional dipole-dipole interaction results in surface anisotropy represented by a pair of Maxwell Garnett-type equations. This surface anisotropy due to surface geometry may be a good indication of the degree of roughness of a given surface.</abstract><doi>10.1063/1.1663173</doi><tpages>4</tpages></addata></record>
fulltext fulltext
identifier ISSN: 0021-8979
ispartof Journal of applied physics, 1974-11, Vol.45 (11), p.5004-5007
issn 0021-8979
1089-7550
language eng
recordid cdi_crossref_primary_10_1063_1_1663173
source AIP Digital Archive
title Generalized Maxwell Garnett equations for rough surfaces
url http://sfxeu10.hosted.exlibrisgroup.com/loughborough?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-01-07T19%3A08%3A31IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-crossref&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Generalized%20Maxwell%20Garnett%20equations%20for%20rough%20surfaces&rft.jtitle=Journal%20of%20applied%20physics&rft.au=Chan,%20E.%20C.&rft.date=1974-11-01&rft.volume=45&rft.issue=11&rft.spage=5004&rft.epage=5007&rft.pages=5004-5007&rft.issn=0021-8979&rft.eissn=1089-7550&rft_id=info:doi/10.1063/1.1663173&rft_dat=%3Ccrossref%3E10_1063_1_1663173%3C/crossref%3E%3Cgrp_id%3Ecdi_FETCH-LOGICAL-c293t-93efb87ddff15ed5cd98828dceab97ee93fe36fccba2f8f11ee2fe77ea6f06563%3C/grp_id%3E%3Coa%3E%3C/oa%3E%3Curl%3E%3C/url%3E&rft_id=info:oai/&rft_id=info:pmid/&rfr_iscdi=true