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Synthesis, Structure, and Properties of the Layered Oxyselenide Ba2CuO2Cu2Se2
A new layered oxyselenide, Ba2CuO2Cu2Se2, was synthesized under high-pressure and high-temperature conditions and was characterized via structural, magnetic, and transport measurements. It crystallizes into space group I4/mmm and consists of a square lattice of [CuO2] planes and antifluorite-type [C...
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Published in: | Inorganic chemistry 2018-05, Vol.57 (9), p.5108-5113 |
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container_title | Inorganic chemistry |
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creator | Li, Wenmin Fu, Zhaoming Wang, Xiancheng Zhang, Jun Liu, Min Zhao, Jianfa Jin, Meiling Zhao, Guoqiang Dai, Guangyang Deng, Zheng Zhang, Sijia Feng, Shaomin Hu, Zhiwei Huang, Qingzhen Lin, Hongji Chen, Chien-Te Yang, Yifeng Jin, Changqing |
description | A new layered oxyselenide, Ba2CuO2Cu2Se2, was synthesized under high-pressure and high-temperature conditions and was characterized via structural, magnetic, and transport measurements. It crystallizes into space group I4/mmm and consists of a square lattice of [CuO2] planes and antifluorite-type [Cu2Se2] layers, which are alternately stacked along the c axis. The lattice parameters are obtained as a = b = 4.0885 Å and c = 19.6887 Å. The Cu–O bond length is given by half of the lattice constant a, i.e., 2.0443 Å. Ba2CuO2Cu2Se2 is a semiconductor with a resistivity of ∼18 mΩ·cm at room temperature. No magnetic transition was found in the measured temperature range, and the Curie–Weiss temperature was obtained as −0.2 K, suggesting a very weak exchange interaction. The DFT+U eff calculation demonstrates that the band gap is about 0.2 eV for the supposed antiferromagnetic order, and the density of state near the top of the valence band is mainly contributed from the Se 4p electrons. |
doi_str_mv | 10.1021/acs.inorgchem.8b00171 |
format | article |
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It crystallizes into space group I4/mmm and consists of a square lattice of [CuO2] planes and antifluorite-type [Cu2Se2] layers, which are alternately stacked along the c axis. The lattice parameters are obtained as a = b = 4.0885 Å and c = 19.6887 Å. The Cu–O bond length is given by half of the lattice constant a, i.e., 2.0443 Å. Ba2CuO2Cu2Se2 is a semiconductor with a resistivity of ∼18 mΩ·cm at room temperature. No magnetic transition was found in the measured temperature range, and the Curie–Weiss temperature was obtained as −0.2 K, suggesting a very weak exchange interaction. The DFT+U eff calculation demonstrates that the band gap is about 0.2 eV for the supposed antiferromagnetic order, and the density of state near the top of the valence band is mainly contributed from the Se 4p electrons.</description><identifier>ISSN: 0020-1669</identifier><identifier>EISSN: 1520-510X</identifier><identifier>DOI: 10.1021/acs.inorgchem.8b00171</identifier><language>eng</language><publisher>American Chemical Society</publisher><ispartof>Inorganic chemistry, 2018-05, Vol.57 (9), p.5108-5113</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><orcidid>0000-0001-6263-4963 ; 0000-0002-7674-7309 ; 0000-0002-6697-1630</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,776,780,27903,27904</link.rule.ids></links><search><creatorcontrib>Li, Wenmin</creatorcontrib><creatorcontrib>Fu, Zhaoming</creatorcontrib><creatorcontrib>Wang, Xiancheng</creatorcontrib><creatorcontrib>Zhang, Jun</creatorcontrib><creatorcontrib>Liu, Min</creatorcontrib><creatorcontrib>Zhao, Jianfa</creatorcontrib><creatorcontrib>Jin, Meiling</creatorcontrib><creatorcontrib>Zhao, Guoqiang</creatorcontrib><creatorcontrib>Dai, Guangyang</creatorcontrib><creatorcontrib>Deng, Zheng</creatorcontrib><creatorcontrib>Zhang, Sijia</creatorcontrib><creatorcontrib>Feng, Shaomin</creatorcontrib><creatorcontrib>Hu, Zhiwei</creatorcontrib><creatorcontrib>Huang, Qingzhen</creatorcontrib><creatorcontrib>Lin, Hongji</creatorcontrib><creatorcontrib>Chen, Chien-Te</creatorcontrib><creatorcontrib>Yang, Yifeng</creatorcontrib><creatorcontrib>Jin, Changqing</creatorcontrib><title>Synthesis, Structure, and Properties of the Layered Oxyselenide Ba2CuO2Cu2Se2</title><title>Inorganic chemistry</title><addtitle>Inorg. Chem</addtitle><description>A new layered oxyselenide, Ba2CuO2Cu2Se2, was synthesized under high-pressure and high-temperature conditions and was characterized via structural, magnetic, and transport measurements. It crystallizes into space group I4/mmm and consists of a square lattice of [CuO2] planes and antifluorite-type [Cu2Se2] layers, which are alternately stacked along the c axis. The lattice parameters are obtained as a = b = 4.0885 Å and c = 19.6887 Å. The Cu–O bond length is given by half of the lattice constant a, i.e., 2.0443 Å. Ba2CuO2Cu2Se2 is a semiconductor with a resistivity of ∼18 mΩ·cm at room temperature. No magnetic transition was found in the measured temperature range, and the Curie–Weiss temperature was obtained as −0.2 K, suggesting a very weak exchange interaction. The DFT+U eff calculation demonstrates that the band gap is about 0.2 eV for the supposed antiferromagnetic order, and the density of state near the top of the valence band is mainly contributed from the Se 4p electrons.</description><issn>0020-1669</issn><issn>1520-510X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2018</creationdate><recordtype>article</recordtype><recordid>eNo9kE1Lw0AQhhdRsFZ_grBHD02d2c3uJkctfkGlQhW8LdvsxKakSd1NwP57Iy0ehhmGh5eXh7FrhCmCwFtXxGnVtOGrWNN2mq0A0OAJG6ESkCiEz1M2Ahhu1Do_ZxcxbgAgl6kesdflvunWFKs44csu9EXXB5pw13j-Ftodha6iyNuSDxCfuz0F8nzxs49UU1N54vdOzPrFMGJJ4pKdla6OdHXcY_bx-PA-e07mi6eX2d08cUJCl2SUl8ZrlDlqyFZFis4LKCAvMwUOnFYrMkIJSUb6FDBDQ2UqnVdaICojx-zmkLsL7XdPsbPbKhZU166hto9WgJApGJHqAcUDOliym7YPzVDMItg_dfbv-a_OHtXJX8DhY-Y</recordid><startdate>20180507</startdate><enddate>20180507</enddate><creator>Li, Wenmin</creator><creator>Fu, Zhaoming</creator><creator>Wang, Xiancheng</creator><creator>Zhang, Jun</creator><creator>Liu, Min</creator><creator>Zhao, Jianfa</creator><creator>Jin, Meiling</creator><creator>Zhao, Guoqiang</creator><creator>Dai, Guangyang</creator><creator>Deng, Zheng</creator><creator>Zhang, Sijia</creator><creator>Feng, Shaomin</creator><creator>Hu, Zhiwei</creator><creator>Huang, Qingzhen</creator><creator>Lin, Hongji</creator><creator>Chen, Chien-Te</creator><creator>Yang, Yifeng</creator><creator>Jin, Changqing</creator><general>American Chemical Society</general><scope>7X8</scope><orcidid>https://orcid.org/0000-0001-6263-4963</orcidid><orcidid>https://orcid.org/0000-0002-7674-7309</orcidid><orcidid>https://orcid.org/0000-0002-6697-1630</orcidid></search><sort><creationdate>20180507</creationdate><title>Synthesis, Structure, and Properties of the Layered Oxyselenide Ba2CuO2Cu2Se2</title><author>Li, Wenmin ; Fu, Zhaoming ; Wang, Xiancheng ; Zhang, Jun ; Liu, Min ; Zhao, Jianfa ; Jin, Meiling ; Zhao, Guoqiang ; Dai, Guangyang ; Deng, Zheng ; Zhang, Sijia ; Feng, Shaomin ; Hu, Zhiwei ; Huang, Qingzhen ; Lin, Hongji ; Chen, Chien-Te ; Yang, Yifeng ; Jin, Changqing</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a230t-8e9f7d61391608bc41ad20c09f850a0a65be72523e73d401817ef43ad56211573</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2018</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Li, Wenmin</creatorcontrib><creatorcontrib>Fu, Zhaoming</creatorcontrib><creatorcontrib>Wang, Xiancheng</creatorcontrib><creatorcontrib>Zhang, Jun</creatorcontrib><creatorcontrib>Liu, Min</creatorcontrib><creatorcontrib>Zhao, Jianfa</creatorcontrib><creatorcontrib>Jin, Meiling</creatorcontrib><creatorcontrib>Zhao, Guoqiang</creatorcontrib><creatorcontrib>Dai, Guangyang</creatorcontrib><creatorcontrib>Deng, Zheng</creatorcontrib><creatorcontrib>Zhang, Sijia</creatorcontrib><creatorcontrib>Feng, Shaomin</creatorcontrib><creatorcontrib>Hu, Zhiwei</creatorcontrib><creatorcontrib>Huang, Qingzhen</creatorcontrib><creatorcontrib>Lin, Hongji</creatorcontrib><creatorcontrib>Chen, Chien-Te</creatorcontrib><creatorcontrib>Yang, Yifeng</creatorcontrib><creatorcontrib>Jin, Changqing</creatorcontrib><collection>MEDLINE - Academic</collection><jtitle>Inorganic chemistry</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Li, Wenmin</au><au>Fu, Zhaoming</au><au>Wang, Xiancheng</au><au>Zhang, Jun</au><au>Liu, Min</au><au>Zhao, Jianfa</au><au>Jin, Meiling</au><au>Zhao, Guoqiang</au><au>Dai, Guangyang</au><au>Deng, Zheng</au><au>Zhang, Sijia</au><au>Feng, Shaomin</au><au>Hu, Zhiwei</au><au>Huang, Qingzhen</au><au>Lin, Hongji</au><au>Chen, Chien-Te</au><au>Yang, Yifeng</au><au>Jin, Changqing</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Synthesis, Structure, and Properties of the Layered Oxyselenide Ba2CuO2Cu2Se2</atitle><jtitle>Inorganic chemistry</jtitle><addtitle>Inorg. Chem</addtitle><date>2018-05-07</date><risdate>2018</risdate><volume>57</volume><issue>9</issue><spage>5108</spage><epage>5113</epage><pages>5108-5113</pages><issn>0020-1669</issn><eissn>1520-510X</eissn><abstract>A new layered oxyselenide, Ba2CuO2Cu2Se2, was synthesized under high-pressure and high-temperature conditions and was characterized via structural, magnetic, and transport measurements. It crystallizes into space group I4/mmm and consists of a square lattice of [CuO2] planes and antifluorite-type [Cu2Se2] layers, which are alternately stacked along the c axis. The lattice parameters are obtained as a = b = 4.0885 Å and c = 19.6887 Å. The Cu–O bond length is given by half of the lattice constant a, i.e., 2.0443 Å. Ba2CuO2Cu2Se2 is a semiconductor with a resistivity of ∼18 mΩ·cm at room temperature. No magnetic transition was found in the measured temperature range, and the Curie–Weiss temperature was obtained as −0.2 K, suggesting a very weak exchange interaction. The DFT+U eff calculation demonstrates that the band gap is about 0.2 eV for the supposed antiferromagnetic order, and the density of state near the top of the valence band is mainly contributed from the Se 4p electrons.</abstract><pub>American Chemical Society</pub><doi>10.1021/acs.inorgchem.8b00171</doi><tpages>6</tpages><orcidid>https://orcid.org/0000-0001-6263-4963</orcidid><orcidid>https://orcid.org/0000-0002-7674-7309</orcidid><orcidid>https://orcid.org/0000-0002-6697-1630</orcidid></addata></record> |
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title | Synthesis, Structure, and Properties of the Layered Oxyselenide Ba2CuO2Cu2Se2 |
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