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Investigation of the Crystal Structure and the Structural and Magnetic Properties of SrCu2(PO4)2
SrCu2(PO4)2 was prepared by the solid-state method at 1153 K. Its structure was solved by direct methods in the space group Pccn (No. 56) with Z = 8 from synchrotron X-ray powder diffraction data measured at room temperature. Structure parameters were then refined by the Rietveld method to obtain th...
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Published in: | Inorganic chemistry 2005-09, Vol.44 (19), p.6632-6640 |
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creator | Belik, Alexei A Azuma, Masaki Matsuo, Akira Whangbo, Myung-Hwan Koo, Hyun-Joo Kikuchi, Jun Kaji, Tomoyuki Okubo, Susumu Ohta, Hitoshi Kindo, Koichi Takano, Mikio |
description | SrCu2(PO4)2 was prepared by the solid-state method at 1153 K. Its structure was solved by direct methods in the space group Pccn (No. 56) with Z = 8 from synchrotron X-ray powder diffraction data measured at room temperature. Structure parameters were then refined by the Rietveld method to obtain the lattice parameters, a = 7.94217(8) Å, b = 15.36918(14) Å, and c = 10.37036(10) Å. SrCu2(PO4)2 presents a new structure type and is built up from Sr2O16 and Cu1Cu2O8 units with Cu1···Cu2 = 3.256 Å. The magnetic properties of SrCu2(PO4)2 were investigated by magnetic susceptibility, magnetization up to 65 T, Cu nuclear quadrupole resonance (NQR), electron-spin resonance, and specific heat measurements. With spin-dimer analysis, it was shown that the two strongest spin-exchange interactions between Cu sites result from the Cu1−O···O−Cu2 and Cu2−O···O−Cu2 super-superexchange paths with Cu1···Cu2 = 5.861 Å and Cu2···Cu2 = 5.251 Å, and the superexchange associated with the structural dimer Cu1Cu2O8 is negligible. The magnetic susceptibility data were analyzed in terms of a linear four-spin cluster model, Cu1−Cu2−Cu2−Cu1 with −2J 1/k B = 82.4 K for Cu1−Cu2 and −2J 2/k B = 59 K for Cu2−Cu2. A spin gap deduced from this model (Δ/k B = 63 K) is in agreement with that obtained from the Cu NQR data (Δ/k B = 65 K). A one-half magnetization plateau was observed between approximately 50 and 63 T at 1.3 K. Specific heat data show that SrCu2(PO4)2 does not undergo a long-range magnetic ordering down to 0.45 K. SrCu2(PO4)2 melts incongruently at 1189 K. We also report its vibrational properties studied with Raman spectroscopy. |
doi_str_mv | 10.1021/ic051079h |
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Its structure was solved by direct methods in the space group Pccn (No. 56) with Z = 8 from synchrotron X-ray powder diffraction data measured at room temperature. Structure parameters were then refined by the Rietveld method to obtain the lattice parameters, a = 7.94217(8) Å, b = 15.36918(14) Å, and c = 10.37036(10) Å. SrCu2(PO4)2 presents a new structure type and is built up from Sr2O16 and Cu1Cu2O8 units with Cu1···Cu2 = 3.256 Å. The magnetic properties of SrCu2(PO4)2 were investigated by magnetic susceptibility, magnetization up to 65 T, Cu nuclear quadrupole resonance (NQR), electron-spin resonance, and specific heat measurements. With spin-dimer analysis, it was shown that the two strongest spin-exchange interactions between Cu sites result from the Cu1−O···O−Cu2 and Cu2−O···O−Cu2 super-superexchange paths with Cu1···Cu2 = 5.861 Å and Cu2···Cu2 = 5.251 Å, and the superexchange associated with the structural dimer Cu1Cu2O8 is negligible. The magnetic susceptibility data were analyzed in terms of a linear four-spin cluster model, Cu1−Cu2−Cu2−Cu1 with −2J 1/k B = 82.4 K for Cu1−Cu2 and −2J 2/k B = 59 K for Cu2−Cu2. A spin gap deduced from this model (Δ/k B = 63 K) is in agreement with that obtained from the Cu NQR data (Δ/k B = 65 K). A one-half magnetization plateau was observed between approximately 50 and 63 T at 1.3 K. Specific heat data show that SrCu2(PO4)2 does not undergo a long-range magnetic ordering down to 0.45 K. SrCu2(PO4)2 melts incongruently at 1189 K. We also report its vibrational properties studied with Raman spectroscopy.</description><identifier>ISSN: 0020-1669</identifier><identifier>EISSN: 1520-510X</identifier><identifier>DOI: 10.1021/ic051079h</identifier><identifier>PMID: 16156620</identifier><language>eng</language><publisher>United States: American Chemical Society</publisher><ispartof>Inorganic chemistry, 2005-09, Vol.44 (19), p.6632-6640</ispartof><rights>Copyright © 2005 American Chemical Society</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,777,781,27905,27906</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/16156620$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Belik, Alexei A</creatorcontrib><creatorcontrib>Azuma, Masaki</creatorcontrib><creatorcontrib>Matsuo, Akira</creatorcontrib><creatorcontrib>Whangbo, Myung-Hwan</creatorcontrib><creatorcontrib>Koo, Hyun-Joo</creatorcontrib><creatorcontrib>Kikuchi, Jun</creatorcontrib><creatorcontrib>Kaji, Tomoyuki</creatorcontrib><creatorcontrib>Okubo, Susumu</creatorcontrib><creatorcontrib>Ohta, Hitoshi</creatorcontrib><creatorcontrib>Kindo, Koichi</creatorcontrib><creatorcontrib>Takano, Mikio</creatorcontrib><title>Investigation of the Crystal Structure and the Structural and Magnetic Properties of SrCu2(PO4)2</title><title>Inorganic chemistry</title><addtitle>Inorg. Chem</addtitle><description>SrCu2(PO4)2 was prepared by the solid-state method at 1153 K. Its structure was solved by direct methods in the space group Pccn (No. 56) with Z = 8 from synchrotron X-ray powder diffraction data measured at room temperature. Structure parameters were then refined by the Rietveld method to obtain the lattice parameters, a = 7.94217(8) Å, b = 15.36918(14) Å, and c = 10.37036(10) Å. SrCu2(PO4)2 presents a new structure type and is built up from Sr2O16 and Cu1Cu2O8 units with Cu1···Cu2 = 3.256 Å. The magnetic properties of SrCu2(PO4)2 were investigated by magnetic susceptibility, magnetization up to 65 T, Cu nuclear quadrupole resonance (NQR), electron-spin resonance, and specific heat measurements. With spin-dimer analysis, it was shown that the two strongest spin-exchange interactions between Cu sites result from the Cu1−O···O−Cu2 and Cu2−O···O−Cu2 super-superexchange paths with Cu1···Cu2 = 5.861 Å and Cu2···Cu2 = 5.251 Å, and the superexchange associated with the structural dimer Cu1Cu2O8 is negligible. The magnetic susceptibility data were analyzed in terms of a linear four-spin cluster model, Cu1−Cu2−Cu2−Cu1 with −2J 1/k B = 82.4 K for Cu1−Cu2 and −2J 2/k B = 59 K for Cu2−Cu2. A spin gap deduced from this model (Δ/k B = 63 K) is in agreement with that obtained from the Cu NQR data (Δ/k B = 65 K). A one-half magnetization plateau was observed between approximately 50 and 63 T at 1.3 K. Specific heat data show that SrCu2(PO4)2 does not undergo a long-range magnetic ordering down to 0.45 K. SrCu2(PO4)2 melts incongruently at 1189 K. We also report its vibrational properties studied with Raman spectroscopy.</description><issn>0020-1669</issn><issn>1520-510X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2005</creationdate><recordtype>article</recordtype><recordid>eNo9kU1PwkAQhjdGI4ge_AOmF40eqrNddtsetRHBYMCACbd1aQcoQou7WyP_3kU-Mof5eJ-8ycwQcknhnkJAH_IUOIUwnh2ROuUB-K4bHZM6gKupEHGNnBkzB4CYNcUpqVFBuRAB1Mlnp_hBY_OpsnlZeOXEszP0Er02Vi28gdVVaiuNniqyf2U_ceJm9KamBdo89fq6XKG2OZqNx0AnVXDb7zXvgnNyMlELgxe73CAfredh0va7vZdO8tj1FYPA-hjGY9qEjMccqQi5SsMgihAnXKCLIEbGIpHGaeTELFOgxpCpjLFQNDEWijXIzdZ3pcvvyq0kl7lJcbFQBZaVkSLiIVAGDrzagdV4iZlc6Xyp9Frub-IAfwvkxuLvQVf6S4qQhVwO-wPZar8-wYi_S-b46y2vUiPnZaULt6ekIDe_kYffsD_Fqnzs</recordid><startdate>20050919</startdate><enddate>20050919</enddate><creator>Belik, Alexei A</creator><creator>Azuma, Masaki</creator><creator>Matsuo, Akira</creator><creator>Whangbo, Myung-Hwan</creator><creator>Koo, Hyun-Joo</creator><creator>Kikuchi, Jun</creator><creator>Kaji, Tomoyuki</creator><creator>Okubo, Susumu</creator><creator>Ohta, Hitoshi</creator><creator>Kindo, Koichi</creator><creator>Takano, Mikio</creator><general>American Chemical Society</general><scope>BSCLL</scope><scope>NPM</scope><scope>7X8</scope></search><sort><creationdate>20050919</creationdate><title>Investigation of the Crystal Structure and the Structural and Magnetic Properties of SrCu2(PO4)2</title><author>Belik, Alexei A ; Azuma, Masaki ; Matsuo, Akira ; Whangbo, Myung-Hwan ; Koo, Hyun-Joo ; Kikuchi, Jun ; Kaji, Tomoyuki ; Okubo, Susumu ; Ohta, Hitoshi ; Kindo, Koichi ; Takano, Mikio</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a302t-e79b140d595e1675ac7288eef56e6e629e3386c9c8675dda0ab0dad33764e96a3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2005</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Belik, Alexei A</creatorcontrib><creatorcontrib>Azuma, Masaki</creatorcontrib><creatorcontrib>Matsuo, Akira</creatorcontrib><creatorcontrib>Whangbo, Myung-Hwan</creatorcontrib><creatorcontrib>Koo, Hyun-Joo</creatorcontrib><creatorcontrib>Kikuchi, Jun</creatorcontrib><creatorcontrib>Kaji, Tomoyuki</creatorcontrib><creatorcontrib>Okubo, Susumu</creatorcontrib><creatorcontrib>Ohta, Hitoshi</creatorcontrib><creatorcontrib>Kindo, Koichi</creatorcontrib><creatorcontrib>Takano, Mikio</creatorcontrib><collection>Istex</collection><collection>PubMed</collection><collection>MEDLINE - Academic</collection><jtitle>Inorganic chemistry</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Belik, Alexei A</au><au>Azuma, Masaki</au><au>Matsuo, Akira</au><au>Whangbo, Myung-Hwan</au><au>Koo, Hyun-Joo</au><au>Kikuchi, Jun</au><au>Kaji, Tomoyuki</au><au>Okubo, Susumu</au><au>Ohta, Hitoshi</au><au>Kindo, Koichi</au><au>Takano, Mikio</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Investigation of the Crystal Structure and the Structural and Magnetic Properties of SrCu2(PO4)2</atitle><jtitle>Inorganic chemistry</jtitle><addtitle>Inorg. Chem</addtitle><date>2005-09-19</date><risdate>2005</risdate><volume>44</volume><issue>19</issue><spage>6632</spage><epage>6640</epage><pages>6632-6640</pages><issn>0020-1669</issn><eissn>1520-510X</eissn><abstract>SrCu2(PO4)2 was prepared by the solid-state method at 1153 K. Its structure was solved by direct methods in the space group Pccn (No. 56) with Z = 8 from synchrotron X-ray powder diffraction data measured at room temperature. Structure parameters were then refined by the Rietveld method to obtain the lattice parameters, a = 7.94217(8) Å, b = 15.36918(14) Å, and c = 10.37036(10) Å. SrCu2(PO4)2 presents a new structure type and is built up from Sr2O16 and Cu1Cu2O8 units with Cu1···Cu2 = 3.256 Å. The magnetic properties of SrCu2(PO4)2 were investigated by magnetic susceptibility, magnetization up to 65 T, Cu nuclear quadrupole resonance (NQR), electron-spin resonance, and specific heat measurements. With spin-dimer analysis, it was shown that the two strongest spin-exchange interactions between Cu sites result from the Cu1−O···O−Cu2 and Cu2−O···O−Cu2 super-superexchange paths with Cu1···Cu2 = 5.861 Å and Cu2···Cu2 = 5.251 Å, and the superexchange associated with the structural dimer Cu1Cu2O8 is negligible. The magnetic susceptibility data were analyzed in terms of a linear four-spin cluster model, Cu1−Cu2−Cu2−Cu1 with −2J 1/k B = 82.4 K for Cu1−Cu2 and −2J 2/k B = 59 K for Cu2−Cu2. A spin gap deduced from this model (Δ/k B = 63 K) is in agreement with that obtained from the Cu NQR data (Δ/k B = 65 K). A one-half magnetization plateau was observed between approximately 50 and 63 T at 1.3 K. Specific heat data show that SrCu2(PO4)2 does not undergo a long-range magnetic ordering down to 0.45 K. SrCu2(PO4)2 melts incongruently at 1189 K. We also report its vibrational properties studied with Raman spectroscopy.</abstract><cop>United States</cop><pub>American Chemical Society</pub><pmid>16156620</pmid><doi>10.1021/ic051079h</doi><tpages>9</tpages></addata></record> |
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title | Investigation of the Crystal Structure and the Structural and Magnetic Properties of SrCu2(PO4)2 |
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