Projector augmented wave calculation of x-ray absorption spectra at the L2,3 edges
We develop a technique based on density functional theory and the projector augmented wave method in order to obtain the x-ray absorption cross section at a general edge, both in the electric dipole and quadrupole approximations. The method is a generalization of Taillefumier et al., PRB 66, 195107...
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description | We develop a technique based on density functional theory and the projector augmented wave method in order to obtain the x-ray absorption cross section at a general edge, both in the electric dipole and quadrupole approximations. The method is a generalization of Taillefumier et al., PRB 66, 195107 (2002). We apply the method to the calculation of the Cu L2,3 edges in fcc copper and cuprite (Cu2O), and to the S L2,3 edges in molybdenite (2H-MoS2). The role of core-hole effects, modeled in a supercell approach, as well as the decomposition of the spectrum into different angular momentum channels are studied in detail. In copper we find that the best agreement with experimental data is obtained when core-hole effects are neglected. On the contrary, core-hole effects need to be included both in Cu2O and 2H-MoS2. Finally we show that a non-negligible component of S L2,3 edges in 2H-MoS2 involves transition to states with s character at all energy scales. The inclusion of this angular momentum channel is mandatory to correctly describe the angular dependence of the measured spectra. We believe that transitions to s character states are quantitatively significant at the L2,3 edges of third row elements from Al to Ar. |
doi_str_mv | 10.48550/arxiv.1304.6251 |
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The method is a generalization of Taillefumier et al., PRB 66, 195107 (2002). We apply the method to the calculation of the Cu L2,3 edges in fcc copper and cuprite (Cu2O), and to the S L2,3 edges in molybdenite (2H-MoS2). The role of core-hole effects, modeled in a supercell approach, as well as the decomposition of the spectrum into different angular momentum channels are studied in detail. In copper we find that the best agreement with experimental data is obtained when core-hole effects are neglected. On the contrary, core-hole effects need to be included both in Cu2O and 2H-MoS2. Finally we show that a non-negligible component of S L2,3 edges in 2H-MoS2 involves transition to states with s character at all energy scales. The inclusion of this angular momentum channel is mandatory to correctly describe the angular dependence of the measured spectra. We believe that transitions to s character states are quantitatively significant at the L2,3 edges of third row elements from Al to Ar.</description><identifier>EISSN: 2331-8422</identifier><identifier>DOI: 10.48550/arxiv.1304.6251</identifier><language>eng</language><publisher>Ithaca: Cornell University Library, arXiv.org</publisher><subject>Absorption cross sections ; Absorption spectra ; Angular momentum ; Copper ; Copper oxides ; Density functional theory ; Dependence ; Electric dipoles ; Molybdenite ; Molybdenum disulfide ; Physics - Computational Physics ; Physics - Materials Science ; Quadrupoles ; X ray absorption</subject><ispartof>arXiv.org, 2013-04</ispartof><rights>2013. This work is published under http://arxiv.org/licenses/nonexclusive-distrib/1.0/ (the “License”). 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We believe that transitions to s character states are quantitatively significant at the L2,3 edges of third row elements from Al to Ar.</description><subject>Absorption cross sections</subject><subject>Absorption spectra</subject><subject>Angular momentum</subject><subject>Copper</subject><subject>Copper oxides</subject><subject>Density functional theory</subject><subject>Dependence</subject><subject>Electric dipoles</subject><subject>Molybdenite</subject><subject>Molybdenum disulfide</subject><subject>Physics - Computational Physics</subject><subject>Physics - Materials Science</subject><subject>Quadrupoles</subject><subject>X ray absorption</subject><issn>2331-8422</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2013</creationdate><recordtype>article</recordtype><sourceid>ABUWG</sourceid><sourceid>AFKRA</sourceid><sourceid>AZQEC</sourceid><sourceid>BENPR</sourceid><sourceid>CCPQU</sourceid><sourceid>DWQXO</sourceid><sourceid>GOX</sourceid><recordid>eNotj81LAzEUxIMgWGrvniTg1a1v30u26VGKX1BQpPfl7SapLW2zJru1_vduW08Dw8wwPyFuchgrozU8cDys9uOcQI0L1PmFGCBRnhmFeCVGKa0BAIsJak0D8fkRw9rVbYiSu-XW7Vpn5Q_vnax5U3cbbldhJ4OXhyzyr-QqhdicvNT0tciSW9l-OTnHe5LOLl26FpeeN8mN_nUoFs9Pi9lrNn9_eZs9zjPWOWYe2BrPunKEqrBQIEzZIFWKpl4RganrXJmJZfI1FJXlnsJZhaAACu1pKG7PsyfesomrLcff8shdHrn7wN050MTw3bnUluvQxV1_qUQwaIj0BOkPNV9Z-Q</recordid><startdate>20130423</startdate><enddate>20130423</enddate><creator>Bunau, Oana</creator><creator>Calandra, Matteo</creator><general>Cornell University Library, arXiv.org</general><scope>8FE</scope><scope>8FG</scope><scope>ABJCF</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>HCIFZ</scope><scope>L6V</scope><scope>M7S</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><scope>PTHSS</scope><scope>GOX</scope></search><sort><creationdate>20130423</creationdate><title>Projector augmented wave calculation of x-ray absorption spectra at the L2,3 edges</title><author>Bunau, Oana ; Calandra, Matteo</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a512-f0ad8fa5be3246d06209a823b439f43308cc1487da3fc06bda233ed42040065f3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2013</creationdate><topic>Absorption cross sections</topic><topic>Absorption spectra</topic><topic>Angular momentum</topic><topic>Copper</topic><topic>Copper oxides</topic><topic>Density functional theory</topic><topic>Dependence</topic><topic>Electric dipoles</topic><topic>Molybdenite</topic><topic>Molybdenum disulfide</topic><topic>Physics - Computational Physics</topic><topic>Physics - Materials Science</topic><topic>Quadrupoles</topic><topic>X ray absorption</topic><toplevel>online_resources</toplevel><creatorcontrib>Bunau, Oana</creatorcontrib><creatorcontrib>Calandra, Matteo</creatorcontrib><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>Materials Science & Engineering Collection</collection><collection>ProQuest Central (Alumni Edition)</collection><collection>ProQuest Central UK/Ireland</collection><collection>ProQuest Central Essentials</collection><collection>ProQuest Central</collection><collection>Technology Collection</collection><collection>ProQuest One Community College</collection><collection>ProQuest Central Korea</collection><collection>SciTech Premium Collection</collection><collection>ProQuest Engineering Collection</collection><collection>Engineering Database</collection><collection>Publicly Available Content Database</collection><collection>ProQuest One Academic Eastern Edition (DO NOT USE)</collection><collection>ProQuest One Academic</collection><collection>ProQuest One Academic UKI Edition</collection><collection>ProQuest Central China</collection><collection>Engineering Collection</collection><collection>arXiv.org</collection><jtitle>arXiv.org</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Bunau, Oana</au><au>Calandra, Matteo</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Projector augmented wave calculation of x-ray absorption spectra at the L2,3 edges</atitle><jtitle>arXiv.org</jtitle><date>2013-04-23</date><risdate>2013</risdate><eissn>2331-8422</eissn><abstract>We develop a technique based on density functional theory and the projector augmented wave method in order to obtain the x-ray absorption cross section at a general edge, both in the electric dipole and quadrupole approximations. The method is a generalization of Taillefumier et al., PRB 66, 195107 (2002). We apply the method to the calculation of the Cu L2,3 edges in fcc copper and cuprite (Cu2O), and to the S L2,3 edges in molybdenite (2H-MoS2). The role of core-hole effects, modeled in a supercell approach, as well as the decomposition of the spectrum into different angular momentum channels are studied in detail. In copper we find that the best agreement with experimental data is obtained when core-hole effects are neglected. On the contrary, core-hole effects need to be included both in Cu2O and 2H-MoS2. Finally we show that a non-negligible component of S L2,3 edges in 2H-MoS2 involves transition to states with s character at all energy scales. The inclusion of this angular momentum channel is mandatory to correctly describe the angular dependence of the measured spectra. We believe that transitions to s character states are quantitatively significant at the L2,3 edges of third row elements from Al to Ar.</abstract><cop>Ithaca</cop><pub>Cornell University Library, arXiv.org</pub><doi>10.48550/arxiv.1304.6251</doi><oa>free_for_read</oa></addata></record> |
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subjects | Absorption cross sections Absorption spectra Angular momentum Copper Copper oxides Density functional theory Dependence Electric dipoles Molybdenite Molybdenum disulfide Physics - Computational Physics Physics - Materials Science Quadrupoles X ray absorption |
title | Projector augmented wave calculation of x-ray absorption spectra at the L2,3 edges |
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