Study the effect of tin on the energy density of states of Se60Te40-XSnx chalcogenide glass
In this paper, Se60Te40-xSnx chalcogenide glasses with different concentrations of Tin (x=0, 5, 10, 15 and 20) were prepared) by melting point method. The electrical properties, i.e. electrical conductivity as a function of temperature, were studied. The activation energy was calculated and was foun...
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description | In this paper, Se60Te40-xSnx chalcogenide glasses with different concentrations of Tin (x=0, 5, 10, 15 and 20) were prepared) by melting point method. The electrical properties, i.e. electrical conductivity as a function of temperature, were studied. The activation energy was calculated and was found that at the extended state it changes from 0.223 to 0.281, local state, the activation energy changes from 0.159 to 0.306 and at the Fermi level; it is found that it changes from 0.151 to 0.231. As for the width of energy tails, they are decreasing, and this indicates that the randomness of the compound is decreased, meaning that it has become more crystalline. The Energy density of state the extended, localized, at Fermi energy and the effect of adding Sn on it also was calculated. The increase in Tin (Sn) concentration led to a change in the density of extended, localized, and at Fermi level. it was found that the extended levels changed from 1.650x1024 to 6.226x1025, localize state, they change from 2.881x1020 to 2.113x1024, as for Fermi level, the density of states changed from 5.033x1021 to 1.942x1023 when the Tin concentration increased from 0 to 20. |
doi_str_mv | 10.1063/5.0129373 |
format | Conference Proceeding |
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The electrical properties, i.e. electrical conductivity as a function of temperature, were studied. The activation energy was calculated and was found that at the extended state it changes from 0.223 to 0.281, local state, the activation energy changes from 0.159 to 0.306 and at the Fermi level; it is found that it changes from 0.151 to 0.231. As for the width of energy tails, they are decreasing, and this indicates that the randomness of the compound is decreased, meaning that it has become more crystalline. The Energy density of state the extended, localized, at Fermi energy and the effect of adding Sn on it also was calculated. The increase in Tin (Sn) concentration led to a change in the density of extended, localized, and at Fermi level. it was found that the extended levels changed from 1.650x1024 to 6.226x1025, localize state, they change from 2.881x1020 to 2.113x1024, as for Fermi level, the density of states changed from 5.033x1021 to 1.942x1023 when the Tin concentration increased from 0 to 20.</description><identifier>ISSN: 0094-243X</identifier><identifier>EISSN: 1551-7616</identifier><identifier>DOI: 10.1063/5.0129373</identifier><identifier>CODEN: APCPCS</identifier><language>eng</language><publisher>Melville: American Institute of Physics</publisher><subject>Activation energy ; Chalcogenides ; Density of states ; Electrical properties ; Electrical resistivity ; Energy ; Fermi level ; Mathematical analysis ; Melting points ; Tin</subject><ispartof>AIP conference proceedings, 2023, Vol.2769 (1)</ispartof><rights>Author(s)</rights><rights>2023 Author(s). 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The electrical properties, i.e. electrical conductivity as a function of temperature, were studied. The activation energy was calculated and was found that at the extended state it changes from 0.223 to 0.281, local state, the activation energy changes from 0.159 to 0.306 and at the Fermi level; it is found that it changes from 0.151 to 0.231. As for the width of energy tails, they are decreasing, and this indicates that the randomness of the compound is decreased, meaning that it has become more crystalline. The Energy density of state the extended, localized, at Fermi energy and the effect of adding Sn on it also was calculated. The increase in Tin (Sn) concentration led to a change in the density of extended, localized, and at Fermi level. it was found that the extended levels changed from 1.650x1024 to 6.226x1025, localize state, they change from 2.881x1020 to 2.113x1024, as for Fermi level, the density of states changed from 5.033x1021 to 1.942x1023 when the Tin concentration increased from 0 to 20.</description><subject>Activation energy</subject><subject>Chalcogenides</subject><subject>Density of states</subject><subject>Electrical properties</subject><subject>Electrical resistivity</subject><subject>Energy</subject><subject>Fermi level</subject><subject>Mathematical analysis</subject><subject>Melting points</subject><subject>Tin</subject><issn>0094-243X</issn><issn>1551-7616</issn><fulltext>true</fulltext><rsrctype>conference_proceeding</rsrctype><creationdate>2023</creationdate><recordtype>conference_proceeding</recordtype><recordid>eNp9kE1LAzEQhoMoWKsH_0HAm7A139k9SvELCh62h4KHkG4m7ZaarJtU3H9vSwvePM0w87zzMi9Ct5RMKFH8QU4IZRXX_AyNqJS00IqqczQipBIFE3xxia5S2hDCKq3LEfqo884NOK8Bg_fQZBw9zm3AMRyHAfrVgB2E1ObhsEzZZkiHrgZF5iBIsajDD27WdtvEFYTWAV5tbUrX6MLbbYKbUx2j-vlpPn0tZu8vb9PHWdFVpS90SbVassZLL8DZRgL1pLKicU4y5RmAsppzYX259FzqpbDOcS0sdUxZwcfo7ni16-PXDlI2m7jrw97QsJIIykpa6j11f6RS0-4faGMwXd9-2n4w37E30pxiM53z_8GUmEPOfwL-CxB7bx0</recordid><startdate>20230421</startdate><enddate>20230421</enddate><creator>Khudhair, Nawal Hassan</creator><creator>Jasim, Kareem Ali</creator><general>American Institute of Physics</general><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope></search><sort><creationdate>20230421</creationdate><title>Study the effect of tin on the energy density of states of Se60Te40-XSnx chalcogenide glass</title><author>Khudhair, Nawal Hassan ; Jasim, Kareem Ali</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-p98f-78176b2cf5f4edac5e1f09a4cdd526f2ee6a7334af8bf357b4add374a1d26a43</frbrgroupid><rsrctype>conference_proceedings</rsrctype><prefilter>conference_proceedings</prefilter><language>eng</language><creationdate>2023</creationdate><topic>Activation energy</topic><topic>Chalcogenides</topic><topic>Density of states</topic><topic>Electrical properties</topic><topic>Electrical resistivity</topic><topic>Energy</topic><topic>Fermi level</topic><topic>Mathematical analysis</topic><topic>Melting points</topic><topic>Tin</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Khudhair, Nawal Hassan</creatorcontrib><creatorcontrib>Jasim, Kareem Ali</creatorcontrib><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Khudhair, Nawal Hassan</au><au>Jasim, Kareem Ali</au><au>Julian, Maya</au><au>Salamé, Chafic-Touma</au><au>Jabur, Akram R.</au><au>Shaban, Auday</au><format>book</format><genre>proceeding</genre><ristype>CONF</ristype><atitle>Study the effect of tin on the energy density of states of Se60Te40-XSnx chalcogenide glass</atitle><btitle>AIP conference proceedings</btitle><date>2023-04-21</date><risdate>2023</risdate><volume>2769</volume><issue>1</issue><issn>0094-243X</issn><eissn>1551-7616</eissn><coden>APCPCS</coden><abstract>In this paper, Se60Te40-xSnx chalcogenide glasses with different concentrations of Tin (x=0, 5, 10, 15 and 20) were prepared) by melting point method. The electrical properties, i.e. electrical conductivity as a function of temperature, were studied. The activation energy was calculated and was found that at the extended state it changes from 0.223 to 0.281, local state, the activation energy changes from 0.159 to 0.306 and at the Fermi level; it is found that it changes from 0.151 to 0.231. As for the width of energy tails, they are decreasing, and this indicates that the randomness of the compound is decreased, meaning that it has become more crystalline. The Energy density of state the extended, localized, at Fermi energy and the effect of adding Sn on it also was calculated. The increase in Tin (Sn) concentration led to a change in the density of extended, localized, and at Fermi level. it was found that the extended levels changed from 1.650x1024 to 6.226x1025, localize state, they change from 2.881x1020 to 2.113x1024, as for Fermi level, the density of states changed from 5.033x1021 to 1.942x1023 when the Tin concentration increased from 0 to 20.</abstract><cop>Melville</cop><pub>American Institute of Physics</pub><doi>10.1063/5.0129373</doi><tpages>7</tpages></addata></record> |
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subjects | Activation energy Chalcogenides Density of states Electrical properties Electrical resistivity Energy Fermi level Mathematical analysis Melting points Tin |
title | Study the effect of tin on the energy density of states of Se60Te40-XSnx chalcogenide glass |
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