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Compton profiles of NiO and TiO2 obtained from first principles GWA spectral function
In this work,we first use momentum density studies to understand strongly correlated electron behavior,which is typically seen in transition metal oxides.We observe that correlated electron behavior as seen in bulk NiO is due to the Fermi break located in the middle of overlapping spectral functions...
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Published in: | Chinese physics B 2016-06, Vol.25 (6), p.407-415 |
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creator | Khidzir, S M Halid, M F M Wan Abdullah, W A T |
description | In this work,we first use momentum density studies to understand strongly correlated electron behavior,which is typically seen in transition metal oxides.We observe that correlated electron behavior as seen in bulk NiO is due to the Fermi break located in the middle of overlapping spectral functions obtained from a GW(G is Green’s function and W is the screened Coulomb interaction) approximation(GWA) calculation while in the case of TiO2 we can see that the origin of the constant momentum distribution in lower momenta is due to a pile up of spectra before the Fermi energy.These observations are then used to compare our calculated Compton profiles with previous experimental studies of Fukamachi and Limandri.Our calculations for NiO are observed to follow the same trend as the experimental profile but it is seen to have a wide difference in the case of TiO2 before the Fermi break.The ground state momentum densities differ significantly from the quasiparticle momentum density,thus stressing the importance of the quasiparticle wave function as the input for the study of charge density and the electron localization function.Finally we perform a calculation of the quasiparticle renormalization function,giving a quantitative description of the discontinuity of the GWA momentum density. |
doi_str_mv | 10.1088/1674-1056/25/6/067105 |
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Halid, M F M ; Wan Abdullah, W A T</creator><creatorcontrib>Khidzir, S M ; Halid, M F M ; Wan Abdullah, W A T</creatorcontrib><description>In this work,we first use momentum density studies to understand strongly correlated electron behavior,which is typically seen in transition metal oxides.We observe that correlated electron behavior as seen in bulk NiO is due to the Fermi break located in the middle of overlapping spectral functions obtained from a GW(G is Green’s function and W is the screened Coulomb interaction) approximation(GWA) calculation while in the case of TiO2 we can see that the origin of the constant momentum distribution in lower momenta is due to a pile up of spectra before the Fermi energy.These observations are then used to compare our calculated Compton profiles with previous experimental studies of Fukamachi and Limandri.Our calculations for NiO are observed to follow the same trend as the experimental profile but it is seen to have a wide difference in the case of TiO2 before the Fermi break.The ground state momentum densities differ significantly from the quasiparticle momentum density,thus stressing the importance of the quasiparticle wave function as the input for the study of charge density and the electron localization function.Finally we perform a calculation of the quasiparticle renormalization function,giving a quantitative description of the discontinuity of the GWA momentum density.</description><identifier>ISSN: 1674-1056</identifier><identifier>EISSN: 2058-3834</identifier><identifier>DOI: 10.1088/1674-1056/25/6/067105</identifier><language>eng</language><publisher>IOP Publishing</publisher><subject>borides ; carbides ; chalcogenides ; density functional theory ; elastic and Compton scattering ; elements ; gradient and other corrections ; Green函数 ; local density approximation ; NiO ; nitrides ; oxides ; TiO2 ; 型材 ; 康普顿 ; 第一性原理 ; 谱函数 ; 过渡金属氧化物</subject><ispartof>Chinese physics B, 2016-06, Vol.25 (6), p.407-415</ispartof><rights>2016 Chinese Physical Society and IOP Publishing Ltd</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Uhttp://image.cqvip.com/vip1000/qk/85823A/85823A.jpg</thumbnail><link.rule.ids>314,780,784,27924,27925</link.rule.ids></links><search><creatorcontrib>Khidzir, S M</creatorcontrib><creatorcontrib>Halid, M F M</creatorcontrib><creatorcontrib>Wan Abdullah, W A T</creatorcontrib><title>Compton profiles of NiO and TiO2 obtained from first principles GWA spectral function</title><title>Chinese physics B</title><addtitle>ChinPhysB</addtitle><addtitle>Chinese Physics</addtitle><description>In this work,we first use momentum density studies to understand strongly correlated electron behavior,which is typically seen in transition metal oxides.We observe that correlated electron behavior as seen in bulk NiO is due to the Fermi break located in the middle of overlapping spectral functions obtained from a GW(G is Green’s function and W is the screened Coulomb interaction) approximation(GWA) calculation while in the case of TiO2 we can see that the origin of the constant momentum distribution in lower momenta is due to a pile up of spectra before the Fermi energy.These observations are then used to compare our calculated Compton profiles with previous experimental studies of Fukamachi and Limandri.Our calculations for NiO are observed to follow the same trend as the experimental profile but it is seen to have a wide difference in the case of TiO2 before the Fermi break.The ground state momentum densities differ significantly from the quasiparticle momentum density,thus stressing the importance of the quasiparticle wave function as the input for the study of charge density and the electron localization function.Finally we perform a calculation of the quasiparticle renormalization function,giving a quantitative description of the discontinuity of the GWA momentum density.</description><subject>borides</subject><subject>carbides</subject><subject>chalcogenides</subject><subject>density functional theory</subject><subject>elastic and Compton scattering</subject><subject>elements</subject><subject>gradient and other corrections</subject><subject>Green函数</subject><subject>local density approximation</subject><subject>NiO</subject><subject>nitrides</subject><subject>oxides</subject><subject>TiO2</subject><subject>型材</subject><subject>康普顿</subject><subject>第一性原理</subject><subject>谱函数</subject><subject>过渡金属氧化物</subject><issn>1674-1056</issn><issn>2058-3834</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2016</creationdate><recordtype>article</recordtype><recordid>eNo9kE1Lw0AQhhdRMFZ_grB4j5n93hxL0SoUe2nxuGw22bql3Y1JevDfmxDxNAw87wzPi9AjgWcCWhdEKp4TELKgopAFSDUuVyijIHTONOPXKPtnbtFd3x8BJAHKMrRfpXM7pIjbLvlwanqcPP4IW2xjjXdhS3GqBhtiU2PfpTP2oeuHEQ7RhXbC159L3LeNGzp7wv4S3RBSvEc33p765uFvLtD-9WW3ess32_X7arnJHaV8yEtvlauFdV54BppzUtNKKEut9rWrKlJKbonyDWGSK8GB65J4oWotKCWj2QKR-W5IrTmmSxfHb4aAmXoxk7OZnA0VRpq5lzHzNGfcV4qH7xAPZtQ52-7HSKlLxQQA-wWr-2Cq</recordid><startdate>20160601</startdate><enddate>20160601</enddate><creator>Khidzir, S M</creator><creator>Halid, M F M</creator><creator>Wan Abdullah, W A T</creator><general>IOP Publishing</general><scope>2RA</scope><scope>92L</scope><scope>CQIGP</scope><scope>~WA</scope></search><sort><creationdate>20160601</creationdate><title>Compton profiles of NiO and TiO2 obtained from first principles GWA spectral function</title><author>Khidzir, S M ; Halid, M F M ; Wan Abdullah, W A T</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c224t-9fa7cd5acf5f308441d2b57a2a8fdcbb1964a17fe136475404891f57d85221383</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2016</creationdate><topic>borides</topic><topic>carbides</topic><topic>chalcogenides</topic><topic>density functional theory</topic><topic>elastic and Compton scattering</topic><topic>elements</topic><topic>gradient and other corrections</topic><topic>Green函数</topic><topic>local density approximation</topic><topic>NiO</topic><topic>nitrides</topic><topic>oxides</topic><topic>TiO2</topic><topic>型材</topic><topic>康普顿</topic><topic>第一性原理</topic><topic>谱函数</topic><topic>过渡金属氧化物</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Khidzir, S M</creatorcontrib><creatorcontrib>Halid, M F M</creatorcontrib><creatorcontrib>Wan Abdullah, W A T</creatorcontrib><collection>维普_期刊</collection><collection>中文科技期刊数据库-CALIS站点</collection><collection>维普中文期刊数据库</collection><collection>中文科技期刊数据库- 镜像站点</collection><jtitle>Chinese physics B</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Khidzir, S M</au><au>Halid, M F M</au><au>Wan Abdullah, W A T</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Compton profiles of NiO and TiO2 obtained from first principles GWA spectral function</atitle><jtitle>Chinese physics B</jtitle><stitle>ChinPhysB</stitle><addtitle>Chinese Physics</addtitle><date>2016-06-01</date><risdate>2016</risdate><volume>25</volume><issue>6</issue><spage>407</spage><epage>415</epage><pages>407-415</pages><issn>1674-1056</issn><eissn>2058-3834</eissn><abstract>In this work,we first use momentum density studies to understand strongly correlated electron behavior,which is typically seen in transition metal oxides.We observe that correlated electron behavior as seen in bulk NiO is due to the Fermi break located in the middle of overlapping spectral functions obtained from a GW(G is Green’s function and W is the screened Coulomb interaction) approximation(GWA) calculation while in the case of TiO2 we can see that the origin of the constant momentum distribution in lower momenta is due to a pile up of spectra before the Fermi energy.These observations are then used to compare our calculated Compton profiles with previous experimental studies of Fukamachi and Limandri.Our calculations for NiO are observed to follow the same trend as the experimental profile but it is seen to have a wide difference in the case of TiO2 before the Fermi break.The ground state momentum densities differ significantly from the quasiparticle momentum density,thus stressing the importance of the quasiparticle wave function as the input for the study of charge density and the electron localization function.Finally we perform a calculation of the quasiparticle renormalization function,giving a quantitative description of the discontinuity of the GWA momentum density.</abstract><pub>IOP Publishing</pub><doi>10.1088/1674-1056/25/6/067105</doi><tpages>9</tpages></addata></record> |
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subjects | borides carbides chalcogenides density functional theory elastic and Compton scattering elements gradient and other corrections Green函数 local density approximation NiO nitrides oxides TiO2 型材 康普顿 第一性原理 谱函数 过渡金属氧化物 |
title | Compton profiles of NiO and TiO2 obtained from first principles GWA spectral function |
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