Layer-By-Layer Magnetic Ordering via Idle Spins and the Optical Signature of Jahn–Teller Cr2+ Ions in Sr2Cr(PO4)2
Blue/turquoise crystals of Sr2CrII(PO4)2 with prismatic shape and edge-length of up to 1 mm were obtained by a vapor-phase moderated solid-state reaction at 1273 K in sealed silica tubes. Its crystal structure was solved and refined from a triply twinned (“trilling”) crystal [Pbca (no. 61), Z = 12,...
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description | Blue/turquoise crystals of Sr2CrII(PO4)2 with prismatic shape and edge-length of up to 1 mm were obtained by a vapor-phase moderated solid-state reaction at 1273 K in sealed silica tubes. Its crystal structure was solved and refined from a triply twinned (“trilling”) crystal [Pbca (no. 61), Z = 12, a = 10.7064(6) Å, b = 9.2730(5) Å, c = 21.2720(7) Å, R 1 = 0.038]. Sr2Cr(PO4)2 belongs to the small family of inorganic solids containing divalent chromium, where the rare Cr2+ ions are stabilized by the inductive effect of the phosphate groups. As expected from its d 4 (S = 2) electronic configuration, the Jahn–Teller effect (JT) is prominent, leading for the two independent Cr2+ ions to square-pyramidal Cr(1)O4+1 and square-planar Cr(2)O4 coordination within a 3D chromium phosphate network [CrII 2(PO4)4]8. Topologically, the Cr(1) and Cr(2) cations are arranged in separate alternating layers stacked along the c axis. In their respective layers, Cr(1) shows a gapped 2D topology and only weak interaction with the adjacent Cr(2) layers. However, below T N1 ∼11.3 K, Cr(1) orders antiferromagnetically into a noncollinear structure, leaving nearly paramagnetic Cr(2) idle spins, strongly frustrated by the Cr(1) moments of the next layers. On further cooling, below T N2 ∼3.6 K, the ordering of Cr(2) occurs via an additional magnetic irreducible representation, which splits the Cr(1) into Cr(1)a and Cr(1)b orbits, thus lifting the frustration on Cr(2). The corresponding P2 1 ca.29.99 magnetic space group forces a crystal symmetry lowering, plausibly signed by a change of the magnetostrictive coefficient from positive to negative below T N2. The optical transitions observed for the JT d 4 ions are in good agreement with our crystal picture from the DFT calculations. A detailed analysis within the angular overlap model explains the surprisingly different d orbital splitting by the ligand field for the chromophores Cr(1)O4+1 and Cr(2)O4. |
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Its crystal structure was solved and refined from a triply twinned (“trilling”) crystal [Pbca (no. 61), Z = 12, a = 10.7064(6) Å, b = 9.2730(5) Å, c = 21.2720(7) Å, R 1 = 0.038]. Sr2Cr(PO4)2 belongs to the small family of inorganic solids containing divalent chromium, where the rare Cr2+ ions are stabilized by the inductive effect of the phosphate groups. As expected from its d 4 (S = 2) electronic configuration, the Jahn–Teller effect (JT) is prominent, leading for the two independent Cr2+ ions to square-pyramidal Cr(1)O4+1 and square-planar Cr(2)O4 coordination within a 3D chromium phosphate network [CrII 2(PO4)4]8. Topologically, the Cr(1) and Cr(2) cations are arranged in separate alternating layers stacked along the c axis. In their respective layers, Cr(1) shows a gapped 2D topology and only weak interaction with the adjacent Cr(2) layers. However, below T N1 ∼11.3 K, Cr(1) orders antiferromagnetically into a noncollinear structure, leaving nearly paramagnetic Cr(2) idle spins, strongly frustrated by the Cr(1) moments of the next layers. On further cooling, below T N2 ∼3.6 K, the ordering of Cr(2) occurs via an additional magnetic irreducible representation, which splits the Cr(1) into Cr(1)a and Cr(1)b orbits, thus lifting the frustration on Cr(2). The corresponding P2 1 ca.29.99 magnetic space group forces a crystal symmetry lowering, plausibly signed by a change of the magnetostrictive coefficient from positive to negative below T N2. The optical transitions observed for the JT d 4 ions are in good agreement with our crystal picture from the DFT calculations. A detailed analysis within the angular overlap model explains the surprisingly different d orbital splitting by the ligand field for the chromophores Cr(1)O4+1 and Cr(2)O4.</description><identifier>ISSN: 0020-1669</identifier><identifier>ISSN: 1520-510X</identifier><identifier>EISSN: 1520-510X</identifier><identifier>DOI: 10.1021/acs.inorgchem.4c02544</identifier><language>eng</language><publisher>American Chemical Society</publisher><ispartof>Inorganic chemistry, 2024-11, Vol.63 (44), p.21000-21011</ispartof><rights>2024 The Authors. Published by American Chemical Society</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><orcidid>0000-0002-1822-6003 ; 0000-0002-8745-4990 ; 0000-0001-5805-1466 ; 0000-0003-1332-7929</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://pubs.acs.org/doi/pdf/10.1021/acs.inorgchem.4c02544$$EPDF$$P50$$Gacs$$H</linktopdf><linktohtml>$$Uhttps://pubs.acs.org/doi/10.1021/acs.inorgchem.4c02544$$EHTML$$P50$$Gacs$$H</linktohtml><link.rule.ids>314,776,780,27053,27901,27902,56713,56763</link.rule.ids></links><search><creatorcontrib>Nimoh, Hicham</creatorcontrib><creatorcontrib>Mentré, Olivier</creatorcontrib><creatorcontrib>Hammer, Eva-Maria</creatorcontrib><creatorcontrib>Jähnig, Maximilian</creatorcontrib><creatorcontrib>Dittrich, Volker</creatorcontrib><creatorcontrib>Minaud, Claire</creatorcontrib><creatorcontrib>Colin, Claire V.</creatorcontrib><creatorcontrib>Arevalo-Lopéz, Angel</creatorcontrib><creatorcontrib>Glaum, Robert</creatorcontrib><title>Layer-By-Layer Magnetic Ordering via Idle Spins and the Optical Signature of Jahn–Teller Cr2+ Ions in Sr2Cr(PO4)2</title><title>Inorganic chemistry</title><addtitle>Inorg. Chem</addtitle><description>Blue/turquoise crystals of Sr2CrII(PO4)2 with prismatic shape and edge-length of up to 1 mm were obtained by a vapor-phase moderated solid-state reaction at 1273 K in sealed silica tubes. Its crystal structure was solved and refined from a triply twinned (“trilling”) crystal [Pbca (no. 61), Z = 12, a = 10.7064(6) Å, b = 9.2730(5) Å, c = 21.2720(7) Å, R 1 = 0.038]. Sr2Cr(PO4)2 belongs to the small family of inorganic solids containing divalent chromium, where the rare Cr2+ ions are stabilized by the inductive effect of the phosphate groups. As expected from its d 4 (S = 2) electronic configuration, the Jahn–Teller effect (JT) is prominent, leading for the two independent Cr2+ ions to square-pyramidal Cr(1)O4+1 and square-planar Cr(2)O4 coordination within a 3D chromium phosphate network [CrII 2(PO4)4]8. Topologically, the Cr(1) and Cr(2) cations are arranged in separate alternating layers stacked along the c axis. In their respective layers, Cr(1) shows a gapped 2D topology and only weak interaction with the adjacent Cr(2) layers. However, below T N1 ∼11.3 K, Cr(1) orders antiferromagnetically into a noncollinear structure, leaving nearly paramagnetic Cr(2) idle spins, strongly frustrated by the Cr(1) moments of the next layers. On further cooling, below T N2 ∼3.6 K, the ordering of Cr(2) occurs via an additional magnetic irreducible representation, which splits the Cr(1) into Cr(1)a and Cr(1)b orbits, thus lifting the frustration on Cr(2). The corresponding P2 1 ca.29.99 magnetic space group forces a crystal symmetry lowering, plausibly signed by a change of the magnetostrictive coefficient from positive to negative below T N2. The optical transitions observed for the JT d 4 ions are in good agreement with our crystal picture from the DFT calculations. A detailed analysis within the angular overlap model explains the surprisingly different d orbital splitting by the ligand field for the chromophores Cr(1)O4+1 and Cr(2)O4.</description><issn>0020-1669</issn><issn>1520-510X</issn><issn>1520-510X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2024</creationdate><recordtype>article</recordtype><recordid>eNo9kM1Kw0AUhQdRsFYfQZhlRVLvzeRvlhr8qVQitIK7MJ1M0pR0UmcSoTvfwTf0SZza4uoeLuccDh8hlwhjBB9vhLTjWremkku1HgcS_DAIjsgAQx-8EOH9mAwAnMYo4qfkzNoVAHAWRANip2KrjHe39f4EfRGVVl0taWYKZWpd0c9a0EnRKDrb1NpSoQvaLRXNNs4lGjqrKy263ijalvRZLPXP1_dcNY3rSo1_TSetC9WazoyfmtFrFlz55-SkFI1VF4c7JG8P9_P0yZtmj5P0duoJjKDz4lgUUDCVSM4XARQh8wshQYRcsDBexFyVQVwisCRWDAOJGIeIC5BJhEomJRuS0b53Y9qPXtkuX9dWum1Cq7a3OUPksY8hT5wV91bHMl-1vdFuWI6Q7wDnu-c_4PwAmP0Cenlxlw</recordid><startdate>20241104</startdate><enddate>20241104</enddate><creator>Nimoh, Hicham</creator><creator>Mentré, Olivier</creator><creator>Hammer, Eva-Maria</creator><creator>Jähnig, Maximilian</creator><creator>Dittrich, Volker</creator><creator>Minaud, Claire</creator><creator>Colin, Claire V.</creator><creator>Arevalo-Lopéz, Angel</creator><creator>Glaum, Robert</creator><general>American Chemical Society</general><scope>7X8</scope><orcidid>https://orcid.org/0000-0002-1822-6003</orcidid><orcidid>https://orcid.org/0000-0002-8745-4990</orcidid><orcidid>https://orcid.org/0000-0001-5805-1466</orcidid><orcidid>https://orcid.org/0000-0003-1332-7929</orcidid></search><sort><creationdate>20241104</creationdate><title>Layer-By-Layer Magnetic Ordering via Idle Spins and the Optical Signature of Jahn–Teller Cr2+ Ions in Sr2Cr(PO4)2</title><author>Nimoh, Hicham ; Mentré, Olivier ; Hammer, Eva-Maria ; Jähnig, Maximilian ; Dittrich, Volker ; Minaud, Claire ; Colin, Claire V. ; Arevalo-Lopéz, Angel ; Glaum, Robert</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a160t-77ad0d3e8c99b40d532dac0a59a357b79ef47f10387e314c117511b0c861ec8f3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2024</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Nimoh, Hicham</creatorcontrib><creatorcontrib>Mentré, Olivier</creatorcontrib><creatorcontrib>Hammer, Eva-Maria</creatorcontrib><creatorcontrib>Jähnig, Maximilian</creatorcontrib><creatorcontrib>Dittrich, Volker</creatorcontrib><creatorcontrib>Minaud, Claire</creatorcontrib><creatorcontrib>Colin, Claire V.</creatorcontrib><creatorcontrib>Arevalo-Lopéz, Angel</creatorcontrib><creatorcontrib>Glaum, Robert</creatorcontrib><collection>MEDLINE - Academic</collection><jtitle>Inorganic chemistry</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Nimoh, Hicham</au><au>Mentré, Olivier</au><au>Hammer, Eva-Maria</au><au>Jähnig, Maximilian</au><au>Dittrich, Volker</au><au>Minaud, Claire</au><au>Colin, Claire V.</au><au>Arevalo-Lopéz, Angel</au><au>Glaum, Robert</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Layer-By-Layer Magnetic Ordering via Idle Spins and the Optical Signature of Jahn–Teller Cr2+ Ions in Sr2Cr(PO4)2</atitle><jtitle>Inorganic chemistry</jtitle><addtitle>Inorg. Chem</addtitle><date>2024-11-04</date><risdate>2024</risdate><volume>63</volume><issue>44</issue><spage>21000</spage><epage>21011</epage><pages>21000-21011</pages><issn>0020-1669</issn><issn>1520-510X</issn><eissn>1520-510X</eissn><abstract>Blue/turquoise crystals of Sr2CrII(PO4)2 with prismatic shape and edge-length of up to 1 mm were obtained by a vapor-phase moderated solid-state reaction at 1273 K in sealed silica tubes. Its crystal structure was solved and refined from a triply twinned (“trilling”) crystal [Pbca (no. 61), Z = 12, a = 10.7064(6) Å, b = 9.2730(5) Å, c = 21.2720(7) Å, R 1 = 0.038]. Sr2Cr(PO4)2 belongs to the small family of inorganic solids containing divalent chromium, where the rare Cr2+ ions are stabilized by the inductive effect of the phosphate groups. As expected from its d 4 (S = 2) electronic configuration, the Jahn–Teller effect (JT) is prominent, leading for the two independent Cr2+ ions to square-pyramidal Cr(1)O4+1 and square-planar Cr(2)O4 coordination within a 3D chromium phosphate network [CrII 2(PO4)4]8. Topologically, the Cr(1) and Cr(2) cations are arranged in separate alternating layers stacked along the c axis. In their respective layers, Cr(1) shows a gapped 2D topology and only weak interaction with the adjacent Cr(2) layers. However, below T N1 ∼11.3 K, Cr(1) orders antiferromagnetically into a noncollinear structure, leaving nearly paramagnetic Cr(2) idle spins, strongly frustrated by the Cr(1) moments of the next layers. On further cooling, below T N2 ∼3.6 K, the ordering of Cr(2) occurs via an additional magnetic irreducible representation, which splits the Cr(1) into Cr(1)a and Cr(1)b orbits, thus lifting the frustration on Cr(2). The corresponding P2 1 ca.29.99 magnetic space group forces a crystal symmetry lowering, plausibly signed by a change of the magnetostrictive coefficient from positive to negative below T N2. The optical transitions observed for the JT d 4 ions are in good agreement with our crystal picture from the DFT calculations. A detailed analysis within the angular overlap model explains the surprisingly different d orbital splitting by the ligand field for the chromophores Cr(1)O4+1 and Cr(2)O4.</abstract><pub>American Chemical Society</pub><doi>10.1021/acs.inorgchem.4c02544</doi><tpages>12</tpages><orcidid>https://orcid.org/0000-0002-1822-6003</orcidid><orcidid>https://orcid.org/0000-0002-8745-4990</orcidid><orcidid>https://orcid.org/0000-0001-5805-1466</orcidid><orcidid>https://orcid.org/0000-0003-1332-7929</orcidid></addata></record> |
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title | Layer-By-Layer Magnetic Ordering via Idle Spins and the Optical Signature of Jahn–Teller Cr2+ Ions in Sr2Cr(PO4)2 |
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