Multiplet structure for perovskite-type Ba0.9Ca0.1Ti0.9Zr0.1O3 by core–hole spectroscopies
Core–hole spectroscopies such as x-ray photoelectron spectroscopy (XPS) and high-resolution electron energy loss spectroscopy (HR-EELS) in combination with multiplet calculation are important tools to elucidate the electronic structure of transition metal compounds. This work presents a comparison b...
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creator | Herrera-Pérez, G. Solis-Canto, O. Silva-Vidaurri, G. Pérez-García, S. Borja-Urby, R. Paraguay-Delgado, F. Rojas-George, G. Reyes-Rojas, A. Fuentes-Cobas, L. |
description | Core–hole spectroscopies such as x-ray photoelectron spectroscopy (XPS) and high-resolution electron energy loss spectroscopy (HR-EELS) in combination with multiplet calculation are important tools to elucidate the electronic structure of transition metal compounds. This work presents a comparison between the electronic structure obtained by XPS and HR-EELS for polycrystalline perovskite-type Ba0.9Ca0.1Ti0.9Zr0.1O3. Raman analysis suggests that Ca2+ cations could partly occupy the Ti4+ cations in the B-site of a perovskite structure with the tetragonal phase. A multiplet structure was determined by XPS for Ti 2p and by HR-EELS for Ca L2,3 and Ti L2,3 edges. Octahedral (Oh) symmetry in the crystal field (CF) effects reproduces the local distortion of TiO6 octahedra. The charge transfer (CT) effects were also considered to reproduce L3-edge EELS shoulders and the satellite in the Ti 2p XPS region. CF and CT parameters, 10 Dq, (charge transfer energy) Δ, and (Coulomb repulsion energy) Udd, are reported for future reference. The broadening of the Ti L2-edge suggests the presence of the Coster–Kronig electron decay process. Multiplet calculation in Oh symmetry for the Ca L2,3-edge could support the Raman interpretation. |
doi_str_mv | 10.1063/5.0014496 |
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This work presents a comparison between the electronic structure obtained by XPS and HR-EELS for polycrystalline perovskite-type Ba0.9Ca0.1Ti0.9Zr0.1O3. Raman analysis suggests that Ca2+ cations could partly occupy the Ti4+ cations in the B-site of a perovskite structure with the tetragonal phase. A multiplet structure was determined by XPS for Ti 2p and by HR-EELS for Ca L2,3 and Ti L2,3 edges. Octahedral (Oh) symmetry in the crystal field (CF) effects reproduces the local distortion of TiO6 octahedra. The charge transfer (CT) effects were also considered to reproduce L3-edge EELS shoulders and the satellite in the Ti 2p XPS region. CF and CT parameters, 10 Dq, (charge transfer energy) Δ, and (Coulomb repulsion energy) Udd, are reported for future reference. The broadening of the Ti L2-edge suggests the presence of the Coster–Kronig electron decay process. Multiplet calculation in Oh symmetry for the Ca L2,3-edge could support the Raman interpretation.</description><identifier>ISSN: 0021-8979</identifier><identifier>EISSN: 1089-7550</identifier><identifier>DOI: 10.1063/5.0014496</identifier><identifier>CODEN: JAPIAU</identifier><language>eng</language><publisher>Melville: American Institute of Physics</publisher><subject>Applied physics ; Calcium ions ; Cations ; Charge transfer ; Electron energy loss spectroscopy ; Electronic structure ; Energy dissipation ; Mathematical analysis ; Metal compounds ; Perovskite structure ; Perovskites ; Photoelectrons ; Raman spectroscopy ; Spectrum analysis ; Symmetry ; Titanium ; Transition metal compounds ; X ray photoelectron spectroscopy</subject><ispartof>Journal of applied physics, 2020-08, Vol.128 (6)</ispartof><rights>Author(s)</rights><rights>2020 Author(s). 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This work presents a comparison between the electronic structure obtained by XPS and HR-EELS for polycrystalline perovskite-type Ba0.9Ca0.1Ti0.9Zr0.1O3. Raman analysis suggests that Ca2+ cations could partly occupy the Ti4+ cations in the B-site of a perovskite structure with the tetragonal phase. A multiplet structure was determined by XPS for Ti 2p and by HR-EELS for Ca L2,3 and Ti L2,3 edges. Octahedral (Oh) symmetry in the crystal field (CF) effects reproduces the local distortion of TiO6 octahedra. The charge transfer (CT) effects were also considered to reproduce L3-edge EELS shoulders and the satellite in the Ti 2p XPS region. CF and CT parameters, 10 Dq, (charge transfer energy) Δ, and (Coulomb repulsion energy) Udd, are reported for future reference. The broadening of the Ti L2-edge suggests the presence of the Coster–Kronig electron decay process. Multiplet calculation in Oh symmetry for the Ca L2,3-edge could support the Raman interpretation.</description><subject>Applied physics</subject><subject>Calcium ions</subject><subject>Cations</subject><subject>Charge transfer</subject><subject>Electron energy loss spectroscopy</subject><subject>Electronic structure</subject><subject>Energy dissipation</subject><subject>Mathematical analysis</subject><subject>Metal compounds</subject><subject>Perovskite structure</subject><subject>Perovskites</subject><subject>Photoelectrons</subject><subject>Raman spectroscopy</subject><subject>Spectrum analysis</subject><subject>Symmetry</subject><subject>Titanium</subject><subject>Transition metal compounds</subject><subject>X ray photoelectron spectroscopy</subject><issn>0021-8979</issn><issn>1089-7550</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2020</creationdate><recordtype>article</recordtype><recordid>eNp90M1KAzEQAOAgCtbqwTdY8KSwNb-7m6MW_6DSS72IEHaTWdxam5hkC735Dr6hT2KkRQ-Cl5mB-ZgZBqFjgkcEF-xcjDAmnMtiBw0IrmReCoF30QBjSvJKlnIfHYQwT4hUTA7Q032_iJ1bQMxC9L2OvYestT5z4O0qvHQR8rh2kF3WeCTHKZBZl6pHn6opy5p1pq2Hz_ePZ7uALDjQ0dugresgHKK9tl4EONrmIXq4vpqNb_PJ9OZufDHJNaMs5po2EjfGcMmpkdiUWNIGSCtIYZisChB1qTktNMcGOK2xMBpAQAkVTQ3NhuhkM9d5-9ZDiGpue79MKxXljAleUcmTOt0onQ4MHlrlfPda-7UiWH0_Twm1fV6yZxsbdBfr2NnlD15Z_wuVM-1_-O_kL-i7fS4</recordid><startdate>20200814</startdate><enddate>20200814</enddate><creator>Herrera-Pérez, G.</creator><creator>Solis-Canto, O.</creator><creator>Silva-Vidaurri, G.</creator><creator>Pérez-García, S.</creator><creator>Borja-Urby, R.</creator><creator>Paraguay-Delgado, F.</creator><creator>Rojas-George, G.</creator><creator>Reyes-Rojas, A.</creator><creator>Fuentes-Cobas, L.</creator><general>American Institute of Physics</general><scope>AAYXX</scope><scope>CITATION</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope><orcidid>https://orcid.org/0000-0002-3764-1595</orcidid><orcidid>https://orcid.org/0000-0001-6063-3967</orcidid><orcidid>https://orcid.org/0000-0003-1303-910X</orcidid><orcidid>https://orcid.org/0000-0001-7489-6549</orcidid><orcidid>https://orcid.org/0000-0002-6972-0714</orcidid><orcidid>https://orcid.org/0000-0002-6947-4728</orcidid><orcidid>https://orcid.org/0000-0002-0542-5919</orcidid></search><sort><creationdate>20200814</creationdate><title>Multiplet structure for perovskite-type Ba0.9Ca0.1Ti0.9Zr0.1O3 by core–hole spectroscopies</title><author>Herrera-Pérez, G. ; Solis-Canto, O. ; Silva-Vidaurri, G. ; Pérez-García, S. ; Borja-Urby, R. ; Paraguay-Delgado, F. ; Rojas-George, G. ; Reyes-Rojas, A. ; Fuentes-Cobas, L.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c323t-c2b90bdd4942d90d7092be1f516d3986e5a7c426c40de42a05dcee5e7e827c4c3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2020</creationdate><topic>Applied physics</topic><topic>Calcium ions</topic><topic>Cations</topic><topic>Charge transfer</topic><topic>Electron energy loss spectroscopy</topic><topic>Electronic structure</topic><topic>Energy dissipation</topic><topic>Mathematical analysis</topic><topic>Metal compounds</topic><topic>Perovskite structure</topic><topic>Perovskites</topic><topic>Photoelectrons</topic><topic>Raman spectroscopy</topic><topic>Spectrum analysis</topic><topic>Symmetry</topic><topic>Titanium</topic><topic>Transition metal compounds</topic><topic>X ray photoelectron spectroscopy</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Herrera-Pérez, G.</creatorcontrib><creatorcontrib>Solis-Canto, O.</creatorcontrib><creatorcontrib>Silva-Vidaurri, G.</creatorcontrib><creatorcontrib>Pérez-García, S.</creatorcontrib><creatorcontrib>Borja-Urby, R.</creatorcontrib><creatorcontrib>Paraguay-Delgado, F.</creatorcontrib><creatorcontrib>Rojas-George, G.</creatorcontrib><creatorcontrib>Reyes-Rojas, A.</creatorcontrib><creatorcontrib>Fuentes-Cobas, L.</creatorcontrib><collection>CrossRef</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Journal of applied physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Herrera-Pérez, G.</au><au>Solis-Canto, O.</au><au>Silva-Vidaurri, G.</au><au>Pérez-García, S.</au><au>Borja-Urby, R.</au><au>Paraguay-Delgado, F.</au><au>Rojas-George, G.</au><au>Reyes-Rojas, A.</au><au>Fuentes-Cobas, L.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Multiplet structure for perovskite-type Ba0.9Ca0.1Ti0.9Zr0.1O3 by core–hole spectroscopies</atitle><jtitle>Journal of applied physics</jtitle><date>2020-08-14</date><risdate>2020</risdate><volume>128</volume><issue>6</issue><issn>0021-8979</issn><eissn>1089-7550</eissn><coden>JAPIAU</coden><abstract>Core–hole spectroscopies such as x-ray photoelectron spectroscopy (XPS) and high-resolution electron energy loss spectroscopy (HR-EELS) in combination with multiplet calculation are important tools to elucidate the electronic structure of transition metal compounds. This work presents a comparison between the electronic structure obtained by XPS and HR-EELS for polycrystalline perovskite-type Ba0.9Ca0.1Ti0.9Zr0.1O3. Raman analysis suggests that Ca2+ cations could partly occupy the Ti4+ cations in the B-site of a perovskite structure with the tetragonal phase. A multiplet structure was determined by XPS for Ti 2p and by HR-EELS for Ca L2,3 and Ti L2,3 edges. Octahedral (Oh) symmetry in the crystal field (CF) effects reproduces the local distortion of TiO6 octahedra. The charge transfer (CT) effects were also considered to reproduce L3-edge EELS shoulders and the satellite in the Ti 2p XPS region. CF and CT parameters, 10 Dq, (charge transfer energy) Δ, and (Coulomb repulsion energy) Udd, are reported for future reference. The broadening of the Ti L2-edge suggests the presence of the Coster–Kronig electron decay process. 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subjects | Applied physics Calcium ions Cations Charge transfer Electron energy loss spectroscopy Electronic structure Energy dissipation Mathematical analysis Metal compounds Perovskite structure Perovskites Photoelectrons Raman spectroscopy Spectrum analysis Symmetry Titanium Transition metal compounds X ray photoelectron spectroscopy |
title | Multiplet structure for perovskite-type Ba0.9Ca0.1Ti0.9Zr0.1O3 by core–hole spectroscopies |
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