Electronic structures, elastic properties, and minimum thermal conductivities of cermet M sub(3)AlN
The electronic structures and elastic anisotropies of cubic Ti sub(3)AlN, Zr sub(3)AlN, and Hf sub(3)AlN are investigated by pseudopotential plane-wave method based on density functional theory. At the Fermi level, the electronic structures of these compounds are successive with no energy gap betwee...
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Veröffentlicht in: | Journal of solid state chemistry 2014-08, Vol.216, p.1-8 |
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description | The electronic structures and elastic anisotropies of cubic Ti sub(3)AlN, Zr sub(3)AlN, and Hf sub(3)AlN are investigated by pseudopotential plane-wave method based on density functional theory. At the Fermi level, the electronic structures of these compounds are successive with no energy gap between conduct and valence bands, and exhibit metallicity in ground states. In valence band of each partial density of states, the different orbital electrons indicate interaction of corresponding atoms. In addition, the anisotropy of Hf sub(3)AlN is found to be significantly different from that of Ti sub(3)AlN and Zr sub(3)AlN, which involve the differences in the bonding strength. It is notable that Hf sub(3)AlN is a desired thermal barrier material with the lowest thermal conductivity at high temperature among the three compounds. |
doi_str_mv | 10.1016/j.jssc.2014.04.008 |
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At the Fermi level, the electronic structures of these compounds are successive with no energy gap between conduct and valence bands, and exhibit metallicity in ground states. In valence band of each partial density of states, the different orbital electrons indicate interaction of corresponding atoms. In addition, the anisotropy of Hf sub(3)AlN is found to be significantly different from that of Ti sub(3)AlN and Zr sub(3)AlN, which involve the differences in the bonding strength. It is notable that Hf sub(3)AlN is a desired thermal barrier material with the lowest thermal conductivity at high temperature among the three compounds.</description><identifier>ISSN: 0022-4596</identifier><identifier>DOI: 10.1016/j.jssc.2014.04.008</identifier><language>eng</language><subject>Anisotropy ; Elastic anisotropy ; Electronic structure ; Ground state ; Heat transfer ; Orbitals ; Thermal conductivity ; Valence band</subject><ispartof>Journal of solid state chemistry, 2014-08, Vol.216, p.1-8</ispartof><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>314,776,780,27903,27904</link.rule.ids></links><search><creatorcontrib>Wang, Jin</creatorcontrib><creatorcontrib>Chen, ZhiQian</creatorcontrib><creatorcontrib>Li, ChunMei</creatorcontrib><creatorcontrib>Li, Feng</creatorcontrib><creatorcontrib>Nie, ChaoYin</creatorcontrib><title>Electronic structures, elastic properties, and minimum thermal conductivities of cermet M sub(3)AlN</title><title>Journal of solid state chemistry</title><description>The electronic structures and elastic anisotropies of cubic Ti sub(3)AlN, Zr sub(3)AlN, and Hf sub(3)AlN are investigated by pseudopotential plane-wave method based on density functional theory. At the Fermi level, the electronic structures of these compounds are successive with no energy gap between conduct and valence bands, and exhibit metallicity in ground states. In valence band of each partial density of states, the different orbital electrons indicate interaction of corresponding atoms. In addition, the anisotropy of Hf sub(3)AlN is found to be significantly different from that of Ti sub(3)AlN and Zr sub(3)AlN, which involve the differences in the bonding strength. It is notable that Hf sub(3)AlN is a desired thermal barrier material with the lowest thermal conductivity at high temperature among the three compounds.</description><subject>Anisotropy</subject><subject>Elastic anisotropy</subject><subject>Electronic structure</subject><subject>Ground state</subject><subject>Heat transfer</subject><subject>Orbitals</subject><subject>Thermal conductivity</subject><subject>Valence band</subject><issn>0022-4596</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2014</creationdate><recordtype>article</recordtype><recordid>eNqVTstqQjEUzEKhPvoDrs5Sod6eXHOtXYpY3LSr7iXGI-aSh-Yk_f5G6A8UBgbmxQgxk9hIlOvXvumZTdOiVA1W4GYgRohtu1Td-_pJjJl7RCm7jRoJs3dkcorBGuCcisklEb8AOc25arcUb5SyfWg6nMHbYH3xkK-UvHZgYjjXkv2xjwzEC5hqUIZP4HKarxZb9zUVw4t2TM9_PBHzj_337rCs4_dCnI_esiHndKBY-Ci7-lO9yU6t_hH9BWxxT8U</recordid><startdate>20140801</startdate><enddate>20140801</enddate><creator>Wang, Jin</creator><creator>Chen, ZhiQian</creator><creator>Li, ChunMei</creator><creator>Li, Feng</creator><creator>Nie, ChaoYin</creator><scope>7QF</scope><scope>7QQ</scope><scope>7U5</scope><scope>8FD</scope><scope>JG9</scope><scope>L7M</scope></search><sort><creationdate>20140801</creationdate><title>Electronic structures, elastic properties, and minimum thermal conductivities of cermet M sub(3)AlN</title><author>Wang, Jin ; Chen, ZhiQian ; Li, ChunMei ; Li, Feng ; Nie, ChaoYin</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-proquest_miscellaneous_15596471543</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2014</creationdate><topic>Anisotropy</topic><topic>Elastic anisotropy</topic><topic>Electronic structure</topic><topic>Ground state</topic><topic>Heat transfer</topic><topic>Orbitals</topic><topic>Thermal conductivity</topic><topic>Valence band</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Wang, Jin</creatorcontrib><creatorcontrib>Chen, ZhiQian</creatorcontrib><creatorcontrib>Li, ChunMei</creatorcontrib><creatorcontrib>Li, Feng</creatorcontrib><creatorcontrib>Nie, ChaoYin</creatorcontrib><collection>Aluminium Industry Abstracts</collection><collection>Ceramic Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Journal of solid state chemistry</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Wang, Jin</au><au>Chen, ZhiQian</au><au>Li, ChunMei</au><au>Li, Feng</au><au>Nie, ChaoYin</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Electronic structures, elastic properties, and minimum thermal conductivities of cermet M sub(3)AlN</atitle><jtitle>Journal of solid state chemistry</jtitle><date>2014-08-01</date><risdate>2014</risdate><volume>216</volume><spage>1</spage><epage>8</epage><pages>1-8</pages><issn>0022-4596</issn><abstract>The electronic structures and elastic anisotropies of cubic Ti sub(3)AlN, Zr sub(3)AlN, and Hf sub(3)AlN are investigated by pseudopotential plane-wave method based on density functional theory. At the Fermi level, the electronic structures of these compounds are successive with no energy gap between conduct and valence bands, and exhibit metallicity in ground states. In valence band of each partial density of states, the different orbital electrons indicate interaction of corresponding atoms. In addition, the anisotropy of Hf sub(3)AlN is found to be significantly different from that of Ti sub(3)AlN and Zr sub(3)AlN, which involve the differences in the bonding strength. It is notable that Hf sub(3)AlN is a desired thermal barrier material with the lowest thermal conductivity at high temperature among the three compounds.</abstract><doi>10.1016/j.jssc.2014.04.008</doi></addata></record> |
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subjects | Anisotropy Elastic anisotropy Electronic structure Ground state Heat transfer Orbitals Thermal conductivity Valence band |
title | Electronic structures, elastic properties, and minimum thermal conductivities of cermet M sub(3)AlN |
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