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Bi and Zn co-doped SnTe thermoelectrics: interplay of resonance levels and heavy hole band dominance leading to enhanced performance and a record high room temperature ZT
Lead free SnTe with a tunable electronic structure has become the front runner in eco-friendly thermoelectrics. Herein, we show through first-principles density functional theory calculations that Bi and Zn doping introduces a resonance level in SnTe. The dominance of the heavy hole valence band at...
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Published in: | Journal of materials chemistry. C, Materials for optical and electronic devices Materials for optical and electronic devices, 2020-01, Vol.8 (6), p.2036-2042 |
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container_issue | 6 |
container_start_page | 2036 |
container_title | Journal of materials chemistry. C, Materials for optical and electronic devices |
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creator | Shenoy, U Sandhya Bhat, D Krishna |
description | Lead free SnTe with a tunable electronic structure has become the front runner in eco-friendly thermoelectrics. Herein, we show through first-principles density functional theory calculations that Bi and Zn doping introduces a resonance level in SnTe. The dominance of the heavy hole valence band at room temperature in Bi–Zn co-doped SnTe leads to a record high room temperature
ZT
of ∼0.3 (at 300 K) for SnTe based materials. The increase in the Seebeck coefficient value due to the interaction between the resonance states and formation of the nanoprecipitates leading to an appreciably low lattice thermal conductivity of 0.68 W m
−1
K
−1
results in a peak
ZT
of ∼1.6 at 840 K. A record high
ZT
average
of ∼0.86 with 300 K and 840 K as cold and hot ends, respectively, makes Bi–Zn co-doped SnTe a potential material for thermoelectric applications. This strategy of using two resonant dopants, to not only improve the room temperature
ZT
but also high temperature values, can very well be extended to other systems. |
doi_str_mv | 10.1039/C9TC06490G |
format | article |
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ZT
of ∼0.3 (at 300 K) for SnTe based materials. The increase in the Seebeck coefficient value due to the interaction between the resonance states and formation of the nanoprecipitates leading to an appreciably low lattice thermal conductivity of 0.68 W m
−1
K
−1
results in a peak
ZT
of ∼1.6 at 840 K. A record high
ZT
average
of ∼0.86 with 300 K and 840 K as cold and hot ends, respectively, makes Bi–Zn co-doped SnTe a potential material for thermoelectric applications. This strategy of using two resonant dopants, to not only improve the room temperature
ZT
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ZT
of ∼0.3 (at 300 K) for SnTe based materials. The increase in the Seebeck coefficient value due to the interaction between the resonance states and formation of the nanoprecipitates leading to an appreciably low lattice thermal conductivity of 0.68 W m
−1
K
−1
results in a peak
ZT
of ∼1.6 at 840 K. A record high
ZT
average
of ∼0.86 with 300 K and 840 K as cold and hot ends, respectively, makes Bi–Zn co-doped SnTe a potential material for thermoelectric applications. This strategy of using two resonant dopants, to not only improve the room temperature
ZT
but also high temperature values, can very well be extended to other systems.</description><subject>Bismuth</subject><subject>Carrier density</subject><subject>Chemical potential</subject><subject>Density functional theory</subject><subject>Density of states</subject><subject>Electrical resistivity</subject><subject>Electronic structure</subject><subject>First principles</subject><subject>Heat conductivity</subject><subject>Heat transfer</subject><subject>High temperature</subject><subject>Lead free</subject><subject>Mathematical analysis</subject><subject>Organic chemistry</subject><subject>Performance enhancement</subject><subject>Power factor</subject><subject>Resonance</subject><subject>Room temperature</subject><subject>Seebeck effect</subject><subject>Thermal conductivity</subject><subject>Thermoelectric materials</subject><subject>Thermoelectricity</subject><subject>Valence band</subject><issn>2050-7526</issn><issn>2050-7534</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2020</creationdate><recordtype>article</recordtype><recordid>eNpFkclOwzAQQCMEEhVw4QtG4oYUcGrHdrhBxSZV4kC59BI59rhJldjBTpH6S3wladnmMtvTm8MkyXlGrjJCi-tZsZgRzgryeJBMpiQnqcgpO_yrp_w4OYtxTcaQGZe8mCSfdw0oZ2DpQPvU-B4NvLoFwlBj6Dy2qIfQ6HgDjRsw9K3agrcQMHqnnEZo8QPbuHfUqD62UPsWodr1xnfNL6RM41YweEBX70YGegzWh26_39FqlGofRk2zqiF438GA3UipYRMQlovT5MiqNuLZTz5J3h7uF7OndP7y-Dy7naeaFnJIC1HlrBIciaBWcaqIlJWVma2yimeV4oxZy7URRJopqkKKjFEqhDJSWp0TepJcfHv74N83GIdy7TfBjSfLKc0ZYUyQfKQuvykdfIwBbdmHplNhW2ak3L2j_H8H_QLDzX7x</recordid><startdate>20200101</startdate><enddate>20200101</enddate><creator>Shenoy, U Sandhya</creator><creator>Bhat, D Krishna</creator><general>Royal Society of Chemistry</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7SP</scope><scope>7U5</scope><scope>8FD</scope><scope>L7M</scope><orcidid>https://orcid.org/0000-0003-0383-6017</orcidid><orcidid>https://orcid.org/0000-0002-6786-882X</orcidid></search><sort><creationdate>20200101</creationdate><title>Bi and Zn co-doped SnTe thermoelectrics: interplay of resonance levels and heavy hole band dominance leading to enhanced performance and a record high room temperature ZT</title><author>Shenoy, U Sandhya ; Bhat, D Krishna</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c398t-97b54b76e073fa63a088bf81fb1b61ba644ff6cd708d2ea987143377ad88fc503</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2020</creationdate><topic>Bismuth</topic><topic>Carrier density</topic><topic>Chemical potential</topic><topic>Density functional theory</topic><topic>Density of states</topic><topic>Electrical resistivity</topic><topic>Electronic structure</topic><topic>First principles</topic><topic>Heat conductivity</topic><topic>Heat transfer</topic><topic>High temperature</topic><topic>Lead free</topic><topic>Mathematical analysis</topic><topic>Organic chemistry</topic><topic>Performance enhancement</topic><topic>Power factor</topic><topic>Resonance</topic><topic>Room temperature</topic><topic>Seebeck effect</topic><topic>Thermal conductivity</topic><topic>Thermoelectric materials</topic><topic>Thermoelectricity</topic><topic>Valence band</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Shenoy, U Sandhya</creatorcontrib><creatorcontrib>Bhat, D Krishna</creatorcontrib><collection>CrossRef</collection><collection>Electronics & Communications Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Journal of materials chemistry. C, Materials for optical and electronic devices</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Shenoy, U Sandhya</au><au>Bhat, D Krishna</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Bi and Zn co-doped SnTe thermoelectrics: interplay of resonance levels and heavy hole band dominance leading to enhanced performance and a record high room temperature ZT</atitle><jtitle>Journal of materials chemistry. C, Materials for optical and electronic devices</jtitle><date>2020-01-01</date><risdate>2020</risdate><volume>8</volume><issue>6</issue><spage>2036</spage><epage>2042</epage><pages>2036-2042</pages><issn>2050-7526</issn><eissn>2050-7534</eissn><abstract>Lead free SnTe with a tunable electronic structure has become the front runner in eco-friendly thermoelectrics. Herein, we show through first-principles density functional theory calculations that Bi and Zn doping introduces a resonance level in SnTe. The dominance of the heavy hole valence band at room temperature in Bi–Zn co-doped SnTe leads to a record high room temperature
ZT
of ∼0.3 (at 300 K) for SnTe based materials. The increase in the Seebeck coefficient value due to the interaction between the resonance states and formation of the nanoprecipitates leading to an appreciably low lattice thermal conductivity of 0.68 W m
−1
K
−1
results in a peak
ZT
of ∼1.6 at 840 K. A record high
ZT
average
of ∼0.86 with 300 K and 840 K as cold and hot ends, respectively, makes Bi–Zn co-doped SnTe a potential material for thermoelectric applications. This strategy of using two resonant dopants, to not only improve the room temperature
ZT
but also high temperature values, can very well be extended to other systems.</abstract><cop>Cambridge</cop><pub>Royal Society of Chemistry</pub><doi>10.1039/C9TC06490G</doi><tpages>7</tpages><orcidid>https://orcid.org/0000-0003-0383-6017</orcidid><orcidid>https://orcid.org/0000-0002-6786-882X</orcidid><oa>free_for_read</oa></addata></record> |
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subjects | Bismuth Carrier density Chemical potential Density functional theory Density of states Electrical resistivity Electronic structure First principles Heat conductivity Heat transfer High temperature Lead free Mathematical analysis Organic chemistry Performance enhancement Power factor Resonance Room temperature Seebeck effect Thermal conductivity Thermoelectric materials Thermoelectricity Valence band |
title | Bi and Zn co-doped SnTe thermoelectrics: interplay of resonance levels and heavy hole band dominance leading to enhanced performance and a record high room temperature ZT |
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