Ca and S K‐edge XANES of CaS calculated by different methods: influence of full potential, core hole and Eu doping
Ca and S K‐edge spectra of CaS are calculated by the full‐potential Green's function multiple‐scattering method, by the FLAPW method and by the finite‐difference method. All three techniques lead to similar spectra. Some differences remain close to the edge, both when comparing different calcul...
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Veröffentlicht in: | Journal of synchrotron radiation 2019-01, Vol.26 (1), p.152-158 |
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description | Ca and S K‐edge spectra of CaS are calculated by the full‐potential Green's function multiple‐scattering method, by the FLAPW method and by the finite‐difference method. All three techniques lead to similar spectra. Some differences remain close to the edge, both when comparing different calculations with each other and when comparing the calculations with earlier experimental data. Here it is found that using the full potential does not lead to significant improvement over the atomic spheres approximation and that the effect of the core hole can be limited to the photoabsorbing atom alone. Doping CaS with Eu will not affect the Ca and S K‐edge XANES of CaS significantly but may give rise to a pre‐edge structure not present for clean CaS.
There are differences between theoretical and experimental Ca and S K‐edge XANES of CaS within the first 10 eV above the edge that cannot be explained as full‐potential effects or by the influence of the core hole as accounted for by the final‐state rule. |
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There are differences between theoretical and experimental Ca and S K‐edge XANES of CaS within the first 10 eV above the edge that cannot be explained as full‐potential effects or by the influence of the core hole as accounted for by the final‐state rule.</description><identifier>ISSN: 1600-5775</identifier><identifier>ISSN: 0909-0495</identifier><identifier>EISSN: 1600-5775</identifier><identifier>DOI: 10.1107/S1600577518016144</identifier><identifier>PMID: 30655480</identifier><language>eng</language><publisher>5 Abbey Square, Chester, Cheshire CH1 2HU, England: International Union of Crystallography</publisher><subject>Calcium sulfides ; CaS ; Condensed Matter ; core hole ; Doping ; full potential ; Green's functions ; Materials Science ; Mathematical analysis ; Physics ; XANES</subject><ispartof>Journal of synchrotron radiation, 2019-01, Vol.26 (1), p.152-158</ispartof><rights>International Union of Crystallography, 2019</rights><rights>Copyright Wiley Subscription Services, Inc. Jan 2019</rights><rights>Distributed under a Creative Commons Attribution 4.0 International License</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c4568-aac2d08bbf98fed962c3dd544946711686fc4a1f8eb97163ea11d497c21fbb973</citedby><cites>FETCH-LOGICAL-c4568-aac2d08bbf98fed962c3dd544946711686fc4a1f8eb97163ea11d497c21fbb973</cites><orcidid>0000-0003-4669-5402 ; 0000-0002-1872-6112</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://onlinelibrary.wiley.com/doi/pdf/10.1107%2FS1600577518016144$$EPDF$$P50$$Gwiley$$H</linktopdf><linktohtml>$$Uhttps://onlinelibrary.wiley.com/doi/full/10.1107%2FS1600577518016144$$EHTML$$P50$$Gwiley$$H</linktohtml><link.rule.ids>230,314,780,784,885,1417,11562,27924,27925,45574,45575,46052,46476</link.rule.ids><linktorsrc>$$Uhttps://onlinelibrary.wiley.com/doi/abs/10.1107%2FS1600577518016144$$EView_record_in_Wiley-Blackwell$$FView_record_in_$$GWiley-Blackwell</linktorsrc><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/30655480$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink><backlink>$$Uhttps://hal.science/hal-01980027$$DView record in HAL$$Hfree_for_read</backlink></links><search><creatorcontrib>Šipr, Ondřej</creatorcontrib><creatorcontrib>Khan, Wilayat</creatorcontrib><creatorcontrib>Joly, Yves</creatorcontrib><creatorcontrib>Minár, Ján</creatorcontrib><title>Ca and S K‐edge XANES of CaS calculated by different methods: influence of full potential, core hole and Eu doping</title><title>Journal of synchrotron radiation</title><addtitle>J Synchrotron Radiat</addtitle><description>Ca and S K‐edge spectra of CaS are calculated by the full‐potential Green's function multiple‐scattering method, by the FLAPW method and by the finite‐difference method. All three techniques lead to similar spectra. Some differences remain close to the edge, both when comparing different calculations with each other and when comparing the calculations with earlier experimental data. Here it is found that using the full potential does not lead to significant improvement over the atomic spheres approximation and that the effect of the core hole can be limited to the photoabsorbing atom alone. Doping CaS with Eu will not affect the Ca and S K‐edge XANES of CaS significantly but may give rise to a pre‐edge structure not present for clean CaS.
There are differences between theoretical and experimental Ca and S K‐edge XANES of CaS within the first 10 eV above the edge that cannot be explained as full‐potential effects or by the influence of the core hole as accounted for by the final‐state rule.</description><subject>Calcium sulfides</subject><subject>CaS</subject><subject>Condensed Matter</subject><subject>core hole</subject><subject>Doping</subject><subject>full potential</subject><subject>Green's functions</subject><subject>Materials Science</subject><subject>Mathematical analysis</subject><subject>Physics</subject><subject>XANES</subject><issn>1600-5775</issn><issn>0909-0495</issn><issn>1600-5775</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2019</creationdate><recordtype>article</recordtype><recordid>eNqFkc2KFDEUhYMozo8-gBsJuFGwNbcqlR93TdM6zjQKloquilRyM11DutLWz0jvfASfcZ5kUvY4iC5c3XD4zrk3HEIeAXsBwOTLEgRjhZQFKAYCOL9DDidpNml3_3gfkKO-v2AJkll-nxzkTBQFV-yQDAtDTetoSc-ufvxEd470y_zdsqTR04UpqTXBjsEM6Gi9o67xHjtsB7rBYR1d_4o2rQ8jthYnhx9DoNs4JKIx4Tm1sUO6jgF_7ViO1MVt054_IPe8CT0-vJnH5NPr5cfFyWz1_s3bxXw1s7wQamaMzRxTde218ui0yGzuXMG55kICCCW85Qa8wlpLEDkaAMe1tBn4Okn5MXm2z12bUG27ZmO6XRVNU53MV9WkMdCKsUxeQmKf7tltF7-N2A_VpukthmBajGNfZSA1B674FPvkL_Qijl2bfpIooSBXkmWJgj1lu9j3HfrbC4BVU33VP_Ulz-Ob5LHeoLt1_O4rAXoPfG8C7v6fWJ2WX7MPnwumVX4NQWyjFA</recordid><startdate>201901</startdate><enddate>201901</enddate><creator>Šipr, Ondřej</creator><creator>Khan, Wilayat</creator><creator>Joly, Yves</creator><creator>Minár, Ján</creator><general>International Union of Crystallography</general><general>John Wiley & Sons, Inc</general><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7U5</scope><scope>8FD</scope><scope>JQ2</scope><scope>L7M</scope><scope>7X8</scope><scope>1XC</scope><scope>VOOES</scope><orcidid>https://orcid.org/0000-0003-4669-5402</orcidid><orcidid>https://orcid.org/0000-0002-1872-6112</orcidid></search><sort><creationdate>201901</creationdate><title>Ca and S K‐edge XANES of CaS calculated by different methods: influence of full potential, core hole and Eu doping</title><author>Šipr, Ondřej ; Khan, Wilayat ; Joly, Yves ; Minár, Ján</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c4568-aac2d08bbf98fed962c3dd544946711686fc4a1f8eb97163ea11d497c21fbb973</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2019</creationdate><topic>Calcium sulfides</topic><topic>CaS</topic><topic>Condensed Matter</topic><topic>core hole</topic><topic>Doping</topic><topic>full potential</topic><topic>Green's functions</topic><topic>Materials Science</topic><topic>Mathematical analysis</topic><topic>Physics</topic><topic>XANES</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Šipr, Ondřej</creatorcontrib><creatorcontrib>Khan, Wilayat</creatorcontrib><creatorcontrib>Joly, Yves</creatorcontrib><creatorcontrib>Minár, Ján</creatorcontrib><collection>PubMed</collection><collection>CrossRef</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>ProQuest Computer Science Collection</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>MEDLINE - Academic</collection><collection>Hyper Article en Ligne (HAL)</collection><collection>Hyper Article en Ligne (HAL) (Open Access)</collection><jtitle>Journal of synchrotron radiation</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Šipr, Ondřej</au><au>Khan, Wilayat</au><au>Joly, Yves</au><au>Minár, Ján</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Ca and S K‐edge XANES of CaS calculated by different methods: influence of full potential, core hole and Eu doping</atitle><jtitle>Journal of synchrotron radiation</jtitle><addtitle>J Synchrotron Radiat</addtitle><date>2019-01</date><risdate>2019</risdate><volume>26</volume><issue>1</issue><spage>152</spage><epage>158</epage><pages>152-158</pages><issn>1600-5775</issn><issn>0909-0495</issn><eissn>1600-5775</eissn><abstract>Ca and S K‐edge spectra of CaS are calculated by the full‐potential Green's function multiple‐scattering method, by the FLAPW method and by the finite‐difference method. All three techniques lead to similar spectra. Some differences remain close to the edge, both when comparing different calculations with each other and when comparing the calculations with earlier experimental data. Here it is found that using the full potential does not lead to significant improvement over the atomic spheres approximation and that the effect of the core hole can be limited to the photoabsorbing atom alone. Doping CaS with Eu will not affect the Ca and S K‐edge XANES of CaS significantly but may give rise to a pre‐edge structure not present for clean CaS.
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subjects | Calcium sulfides CaS Condensed Matter core hole Doping full potential Green's functions Materials Science Mathematical analysis Physics XANES |
title | Ca and S K‐edge XANES of CaS calculated by different methods: influence of full potential, core hole and Eu doping |
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