Thermoelectric properties of antiperovskite calcium oxides Ca3PbO and Ca3SnO
We report the thermoelectric properties of polycrystalline samples of Ca3Pb1− x Bi x O (x = 0, 0.1, 0.2) and Ca3SnO, both crystallizing in a cubic antiperovskite-type structure. The Ca3SnO sample shows metallic resistivity and its thermoelectric power approaches 100 μV K−1 at room temperature, resul...
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creator | Okamoto, Y. Sakamaki, A. Takenaka, K. |
description | We report the thermoelectric properties of polycrystalline samples of Ca3Pb1−
x
Bi
x
O (x = 0, 0.1, 0.2) and Ca3SnO, both crystallizing in a cubic antiperovskite-type structure. The Ca3SnO sample shows metallic resistivity and its thermoelectric power approaches 100 μV K−1 at room temperature, resulting in the thermoelectric power factor of Ca3SnO being larger than that of Ca3Pb1−
x
Bi
x
O. On the basis of Hall and Sommerfeld coefficients, the Ca3SnO sample is found to be a p-type metal with a carrier density of ∼1019 cm−3, a mobility of ∼80 cm2 V−1 s−1, both comparable to those in degenerated semiconductors, and a moderately large hole carrier effective mass. The coexistence of moderately high mobility and large effective mass observed in Ca3SnO, as well as possible emergence of a multivalley electronic structure with a small band gap at low-symmetry points in k-space, suggests that the antiperovskite Ca oxides have strong potential as a thermoelectric material. |
doi_str_mv | 10.1063/1.4952393 |
format | Article |
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x
Bi
x
O (x = 0, 0.1, 0.2) and Ca3SnO, both crystallizing in a cubic antiperovskite-type structure. The Ca3SnO sample shows metallic resistivity and its thermoelectric power approaches 100 μV K−1 at room temperature, resulting in the thermoelectric power factor of Ca3SnO being larger than that of Ca3Pb1−
x
Bi
x
O. On the basis of Hall and Sommerfeld coefficients, the Ca3SnO sample is found to be a p-type metal with a carrier density of ∼1019 cm−3, a mobility of ∼80 cm2 V−1 s−1, both comparable to those in degenerated semiconductors, and a moderately large hole carrier effective mass. The coexistence of moderately high mobility and large effective mass observed in Ca3SnO, as well as possible emergence of a multivalley electronic structure with a small band gap at low-symmetry points in k-space, suggests that the antiperovskite Ca oxides have strong potential as a thermoelectric material.</description><identifier>ISSN: 0021-8979</identifier><identifier>EISSN: 1089-7550</identifier><identifier>DOI: 10.1063/1.4952393</identifier><identifier>CODEN: JAPIAU</identifier><language>eng</language><publisher>Melville: American Institute of Physics</publisher><subject>Applied physics ; Calcium oxide ; Carrier density ; Electronic structure ; Lime ; Power factor ; Thermoelectric materials ; Thermoelectricity</subject><ispartof>Journal of applied physics, 2016-05, Vol.119 (20)</ispartof><rights>Author(s)</rights><rights>2016 Author(s). Published by AIP Publishing.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c393t-a49c28d46d9fa3cc50d114d440bf8e47c7be1c167ab5427a78c7aba43590513a3</citedby><cites>FETCH-LOGICAL-c393t-a49c28d46d9fa3cc50d114d440bf8e47c7be1c167ab5427a78c7aba43590513a3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://pubs.aip.org/jap/article-lookup/doi/10.1063/1.4952393$$EHTML$$P50$$Gscitation$$H</linktohtml><link.rule.ids>314,780,784,794,4512,27924,27925,76384</link.rule.ids></links><search><creatorcontrib>Okamoto, Y.</creatorcontrib><creatorcontrib>Sakamaki, A.</creatorcontrib><creatorcontrib>Takenaka, K.</creatorcontrib><title>Thermoelectric properties of antiperovskite calcium oxides Ca3PbO and Ca3SnO</title><title>Journal of applied physics</title><description>We report the thermoelectric properties of polycrystalline samples of Ca3Pb1−
x
Bi
x
O (x = 0, 0.1, 0.2) and Ca3SnO, both crystallizing in a cubic antiperovskite-type structure. The Ca3SnO sample shows metallic resistivity and its thermoelectric power approaches 100 μV K−1 at room temperature, resulting in the thermoelectric power factor of Ca3SnO being larger than that of Ca3Pb1−
x
Bi
x
O. On the basis of Hall and Sommerfeld coefficients, the Ca3SnO sample is found to be a p-type metal with a carrier density of ∼1019 cm−3, a mobility of ∼80 cm2 V−1 s−1, both comparable to those in degenerated semiconductors, and a moderately large hole carrier effective mass. The coexistence of moderately high mobility and large effective mass observed in Ca3SnO, as well as possible emergence of a multivalley electronic structure with a small band gap at low-symmetry points in k-space, suggests that the antiperovskite Ca oxides have strong potential as a thermoelectric material.</description><subject>Applied physics</subject><subject>Calcium oxide</subject><subject>Carrier density</subject><subject>Electronic structure</subject><subject>Lime</subject><subject>Power factor</subject><subject>Thermoelectric materials</subject><subject>Thermoelectricity</subject><issn>0021-8979</issn><issn>1089-7550</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2016</creationdate><recordtype>article</recordtype><recordid>eNqd0E1LAzEQBuAgCtbqwX-w4ElhayYfTXKU4hcUKljPIZvNYmq7WZO06L830oJ3TzMDDzPDi9Al4AngKb2FCVOcUEWP0AiwVLXgHB-jEcYEaqmEOkVnKa0wBpBUjdB8-e7iJri1szl6Ww0xDC5m71IVusr02Zcx7NKHz66yZm39dlOFL98WMDP0pVkU1P62r_3iHJ10Zp3cxaGO0dvD_XL2VM8Xj8-zu3lty2O5NkxZIls2bVVnqLUctwCsZQw3nXRMWNE4sDAVpuGMCCOkLa1hlCvMgRo6Rlf7veXbz61LWa_CNvblpCZAQCjCpSrqeq9sDClF1-kh-o2J3xqw_g1Lgz6EVezN3ibrs8k-9P_DuxD_oB7ajv4ALup3ag</recordid><startdate>20160528</startdate><enddate>20160528</enddate><creator>Okamoto, Y.</creator><creator>Sakamaki, A.</creator><creator>Takenaka, K.</creator><general>American Institute of Physics</general><scope>AAYXX</scope><scope>CITATION</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope></search><sort><creationdate>20160528</creationdate><title>Thermoelectric properties of antiperovskite calcium oxides Ca3PbO and Ca3SnO</title><author>Okamoto, Y. ; Sakamaki, A. ; Takenaka, K.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c393t-a49c28d46d9fa3cc50d114d440bf8e47c7be1c167ab5427a78c7aba43590513a3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2016</creationdate><topic>Applied physics</topic><topic>Calcium oxide</topic><topic>Carrier density</topic><topic>Electronic structure</topic><topic>Lime</topic><topic>Power factor</topic><topic>Thermoelectric materials</topic><topic>Thermoelectricity</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Okamoto, Y.</creatorcontrib><creatorcontrib>Sakamaki, A.</creatorcontrib><creatorcontrib>Takenaka, K.</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>Okamoto, Y.</au><au>Sakamaki, A.</au><au>Takenaka, K.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Thermoelectric properties of antiperovskite calcium oxides Ca3PbO and Ca3SnO</atitle><jtitle>Journal of applied physics</jtitle><date>2016-05-28</date><risdate>2016</risdate><volume>119</volume><issue>20</issue><issn>0021-8979</issn><eissn>1089-7550</eissn><coden>JAPIAU</coden><abstract>We report the thermoelectric properties of polycrystalline samples of Ca3Pb1−
x
Bi
x
O (x = 0, 0.1, 0.2) and Ca3SnO, both crystallizing in a cubic antiperovskite-type structure. The Ca3SnO sample shows metallic resistivity and its thermoelectric power approaches 100 μV K−1 at room temperature, resulting in the thermoelectric power factor of Ca3SnO being larger than that of Ca3Pb1−
x
Bi
x
O. On the basis of Hall and Sommerfeld coefficients, the Ca3SnO sample is found to be a p-type metal with a carrier density of ∼1019 cm−3, a mobility of ∼80 cm2 V−1 s−1, both comparable to those in degenerated semiconductors, and a moderately large hole carrier effective mass. The coexistence of moderately high mobility and large effective mass observed in Ca3SnO, as well as possible emergence of a multivalley electronic structure with a small band gap at low-symmetry points in k-space, suggests that the antiperovskite Ca oxides have strong potential as a thermoelectric material.</abstract><cop>Melville</cop><pub>American Institute of Physics</pub><doi>10.1063/1.4952393</doi><tpages>5</tpages></addata></record> |
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subjects | Applied physics Calcium oxide Carrier density Electronic structure Lime Power factor Thermoelectric materials Thermoelectricity |
title | Thermoelectric properties of antiperovskite calcium oxides Ca3PbO and Ca3SnO |
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