Loading…
Effects of Sc and Y substitution on the structure and thermoelectric properties of Yb14MnSb11
Yb14MnSb11 is the most efficient bulk p-type thermoelectric material for high temperature applications. Materials with Y and Sc substitutions in Yb14MnSb11 were made both in Sn-flux and by ball milling. These small 3+ rare earth (RE) cations were introduced with the goal of providing chemical pressu...
Saved in:
Published in: | Journal of solid state chemistry 2016-10, Vol.242 (P2), p.55-61 |
---|---|
Main Authors: | , , , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
Tags: |
Add Tag
No Tags, Be the first to tag this record!
|
cited_by | cdi_FETCH-LOGICAL-c371t-2d3467d64f4af9f79bb7e81e0ef9d1a5d4395c1533601c799fc8c710f9eb9123 |
---|---|
cites | cdi_FETCH-LOGICAL-c371t-2d3467d64f4af9f79bb7e81e0ef9d1a5d4395c1533601c799fc8c710f9eb9123 |
container_end_page | 61 |
container_issue | P2 |
container_start_page | 55 |
container_title | Journal of solid state chemistry |
container_volume | 242 |
creator | Grebenkemper, Jason H. Klemenz, Sebastian Albert, Barbara Bux, Sabah K. Kauzlarich, Susan M. |
description | Yb14MnSb11 is the most efficient bulk p-type thermoelectric material for high temperature applications. Materials with Y and Sc substitutions in Yb14MnSb11 were made both in Sn-flux and by ball milling. These small 3+ rare earth (RE) cations were introduced with the goal of providing chemical pressure on the structure. The RE3+ cation is smaller than Yb2+ and also donates one additional electron to this p-type semiconductor. In Yb14−xRExMnSb11 (RE = Sc, Y) the maximum x was about 0.5. X-ray diffraction experiments on the single crystals obtained from Sn-flux showed that Sc preferentially substitutes for Yb(1) and Yb(3), and decreases the size of the unit cell by about 0.3%. Y substitutes on all Yb sites and increases the size of the unit cell by about 0.2%. Samples with Yb14−xRExMnSb11 (x~0.3) were prepared via powder metallurgy and spark plasma sintering for transport and thermal conductivity measurements. Electron microprobe of the Sc-substituted sample showed small regions (≤1 μm) containing greater amounts of Sc, and X-ray powder diffraction of the ball milled Sc sample could be fitted as phase pure Yb14−xScxMnSb11. Y-substituted samples showed larger regions of excess Y in electron microprobe, and small amounts of Yb4Sb3 in X-ray powder diffraction. The Sc sample has slightly reduced carrier concentration over optimized Yb14MnSb11, while the Y samples have even lower carrier concentrations. These carrier concentrations lead to comparable resistivity to Yb14MnSb11 in the Sc-substituted material, and higher resistivities in the Y-substituted material. All materials had similar Seebeck coefficients that slightly exceed Yb14MnSb11 at high temperatures, with the Sc-substituted sample having the highest despite having a higher carrier concentration. Sc-substituted samples also had a slightly higher thermal conductivity over the Y-substituted samples, which had comparable thermal conductivity to Yb14MnSb11. The zT values of the Sc and Y substituted samples are similar (zT1000K~0.8), however below that of Yb14MnSb11 due to the compensation of Seebeck and resistivity.
Chemical pressure of the Sc substituted Yb14MnSb11 provides a viable method for enhancing the Seebeck coefficient.
[Display omitted]
•Yb14−xRExMnSb11 (RE=Sc, Y) were synthesized from Sn flux and stoichiometric powders.•Sc substitution decreases the size of the unit cell while Y increases it.•Sc substitution slightly reduces carrier concentration and Y decreases it further.•Y substitution results |
doi_str_mv | 10.1016/j.jssc.2016.03.015 |
format | article |
fullrecord | <record><control><sourceid>elsevier_osti_</sourceid><recordid>TN_cdi_osti_scitechconnect_1434060</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><els_id>S0022459616300883</els_id><sourcerecordid>S0022459616300883</sourcerecordid><originalsourceid>FETCH-LOGICAL-c371t-2d3467d64f4af9f79bb7e81e0ef9d1a5d4395c1533601c799fc8c710f9eb9123</originalsourceid><addsrcrecordid>eNp9kE9LAzEQxYMoWKtfwFPwvmtmk91twIuU-gcqHtqDPUjYzU5oSrspSVbw25u1noWBGYb3ezweIbfAcmBQ3e_yXQg6L9KdM54zKM_IBJgss7qoPs7JhLGiyEQpq0tyFcKOMYByJibkc2EM6hioM3SladN3dEPD0IZo4xCt62mauEUaoh90HDz-atLHHxzuE-qtpkfvjuijxV-fTQvirV-1ANfkwjT7gDd_e0rWT4v1_CVbvj-_zh-XmeY1xKzouKjqrhJGNEaaWrZtjTNAhkZ20JSd4LLUUHJeMdC1lEbPdA3MSGwlFHxK7k62LsVWQduIeqtd36d4CgQXrGJJVJxE2rsQPBp19PbQ-G8FTI0lqp0aS1RjiYpxlUpM0MMJwpT-y6If3bHX2Fk_mnfO_of_AHJxevc</addsrcrecordid><sourcetype>Open Access Repository</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype></control><display><type>article</type><title>Effects of Sc and Y substitution on the structure and thermoelectric properties of Yb14MnSb11</title><source>Elsevier</source><creator>Grebenkemper, Jason H. ; Klemenz, Sebastian ; Albert, Barbara ; Bux, Sabah K. ; Kauzlarich, Susan M.</creator><creatorcontrib>Grebenkemper, Jason H. ; Klemenz, Sebastian ; Albert, Barbara ; Bux, Sabah K. ; Kauzlarich, Susan M.</creatorcontrib><description>Yb14MnSb11 is the most efficient bulk p-type thermoelectric material for high temperature applications. Materials with Y and Sc substitutions in Yb14MnSb11 were made both in Sn-flux and by ball milling. These small 3+ rare earth (RE) cations were introduced with the goal of providing chemical pressure on the structure. The RE3+ cation is smaller than Yb2+ and also donates one additional electron to this p-type semiconductor. In Yb14−xRExMnSb11 (RE = Sc, Y) the maximum x was about 0.5. X-ray diffraction experiments on the single crystals obtained from Sn-flux showed that Sc preferentially substitutes for Yb(1) and Yb(3), and decreases the size of the unit cell by about 0.3%. Y substitutes on all Yb sites and increases the size of the unit cell by about 0.2%. Samples with Yb14−xRExMnSb11 (x~0.3) were prepared via powder metallurgy and spark plasma sintering for transport and thermal conductivity measurements. Electron microprobe of the Sc-substituted sample showed small regions (≤1 μm) containing greater amounts of Sc, and X-ray powder diffraction of the ball milled Sc sample could be fitted as phase pure Yb14−xScxMnSb11. Y-substituted samples showed larger regions of excess Y in electron microprobe, and small amounts of Yb4Sb3 in X-ray powder diffraction. The Sc sample has slightly reduced carrier concentration over optimized Yb14MnSb11, while the Y samples have even lower carrier concentrations. These carrier concentrations lead to comparable resistivity to Yb14MnSb11 in the Sc-substituted material, and higher resistivities in the Y-substituted material. All materials had similar Seebeck coefficients that slightly exceed Yb14MnSb11 at high temperatures, with the Sc-substituted sample having the highest despite having a higher carrier concentration. Sc-substituted samples also had a slightly higher thermal conductivity over the Y-substituted samples, which had comparable thermal conductivity to Yb14MnSb11. The zT values of the Sc and Y substituted samples are similar (zT1000K~0.8), however below that of Yb14MnSb11 due to the compensation of Seebeck and resistivity.
Chemical pressure of the Sc substituted Yb14MnSb11 provides a viable method for enhancing the Seebeck coefficient.
[Display omitted]
•Yb14−xRExMnSb11 (RE=Sc, Y) were synthesized from Sn flux and stoichiometric powders.•Sc substitution decreases the size of the unit cell while Y increases it.•Sc substitution slightly reduces carrier concentration and Y decreases it further.•Y substitution results in significantly higher resistivity.•Both substitutions result in similar Seebeck coefficients and zT values.</description><identifier>ISSN: 0022-4596</identifier><identifier>EISSN: 1095-726X</identifier><identifier>DOI: 10.1016/j.jssc.2016.03.015</identifier><language>eng</language><publisher>United States: Elsevier Inc</publisher><subject>Chemical pressure ; Rare earth compounds ; Thermoelectric material ; Zintl</subject><ispartof>Journal of solid state chemistry, 2016-10, Vol.242 (P2), p.55-61</ispartof><rights>2016 Elsevier Inc.</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c371t-2d3467d64f4af9f79bb7e81e0ef9d1a5d4395c1533601c799fc8c710f9eb9123</citedby><cites>FETCH-LOGICAL-c371t-2d3467d64f4af9f79bb7e81e0ef9d1a5d4395c1533601c799fc8c710f9eb9123</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>230,314,776,780,881,27903,27904</link.rule.ids><backlink>$$Uhttps://www.osti.gov/biblio/1434060$$D View this record in Osti.gov$$Hfree_for_read</backlink></links><search><creatorcontrib>Grebenkemper, Jason H.</creatorcontrib><creatorcontrib>Klemenz, Sebastian</creatorcontrib><creatorcontrib>Albert, Barbara</creatorcontrib><creatorcontrib>Bux, Sabah K.</creatorcontrib><creatorcontrib>Kauzlarich, Susan M.</creatorcontrib><title>Effects of Sc and Y substitution on the structure and thermoelectric properties of Yb14MnSb11</title><title>Journal of solid state chemistry</title><description>Yb14MnSb11 is the most efficient bulk p-type thermoelectric material for high temperature applications. Materials with Y and Sc substitutions in Yb14MnSb11 were made both in Sn-flux and by ball milling. These small 3+ rare earth (RE) cations were introduced with the goal of providing chemical pressure on the structure. The RE3+ cation is smaller than Yb2+ and also donates one additional electron to this p-type semiconductor. In Yb14−xRExMnSb11 (RE = Sc, Y) the maximum x was about 0.5. X-ray diffraction experiments on the single crystals obtained from Sn-flux showed that Sc preferentially substitutes for Yb(1) and Yb(3), and decreases the size of the unit cell by about 0.3%. Y substitutes on all Yb sites and increases the size of the unit cell by about 0.2%. Samples with Yb14−xRExMnSb11 (x~0.3) were prepared via powder metallurgy and spark plasma sintering for transport and thermal conductivity measurements. Electron microprobe of the Sc-substituted sample showed small regions (≤1 μm) containing greater amounts of Sc, and X-ray powder diffraction of the ball milled Sc sample could be fitted as phase pure Yb14−xScxMnSb11. Y-substituted samples showed larger regions of excess Y in electron microprobe, and small amounts of Yb4Sb3 in X-ray powder diffraction. The Sc sample has slightly reduced carrier concentration over optimized Yb14MnSb11, while the Y samples have even lower carrier concentrations. These carrier concentrations lead to comparable resistivity to Yb14MnSb11 in the Sc-substituted material, and higher resistivities in the Y-substituted material. All materials had similar Seebeck coefficients that slightly exceed Yb14MnSb11 at high temperatures, with the Sc-substituted sample having the highest despite having a higher carrier concentration. Sc-substituted samples also had a slightly higher thermal conductivity over the Y-substituted samples, which had comparable thermal conductivity to Yb14MnSb11. The zT values of the Sc and Y substituted samples are similar (zT1000K~0.8), however below that of Yb14MnSb11 due to the compensation of Seebeck and resistivity.
Chemical pressure of the Sc substituted Yb14MnSb11 provides a viable method for enhancing the Seebeck coefficient.
[Display omitted]
•Yb14−xRExMnSb11 (RE=Sc, Y) were synthesized from Sn flux and stoichiometric powders.•Sc substitution decreases the size of the unit cell while Y increases it.•Sc substitution slightly reduces carrier concentration and Y decreases it further.•Y substitution results in significantly higher resistivity.•Both substitutions result in similar Seebeck coefficients and zT values.</description><subject>Chemical pressure</subject><subject>Rare earth compounds</subject><subject>Thermoelectric material</subject><subject>Zintl</subject><issn>0022-4596</issn><issn>1095-726X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2016</creationdate><recordtype>article</recordtype><recordid>eNp9kE9LAzEQxYMoWKtfwFPwvmtmk91twIuU-gcqHtqDPUjYzU5oSrspSVbw25u1noWBGYb3ezweIbfAcmBQ3e_yXQg6L9KdM54zKM_IBJgss7qoPs7JhLGiyEQpq0tyFcKOMYByJibkc2EM6hioM3SladN3dEPD0IZo4xCt62mauEUaoh90HDz-atLHHxzuE-qtpkfvjuijxV-fTQvirV-1ANfkwjT7gDd_e0rWT4v1_CVbvj-_zh-XmeY1xKzouKjqrhJGNEaaWrZtjTNAhkZ20JSd4LLUUHJeMdC1lEbPdA3MSGwlFHxK7k62LsVWQduIeqtd36d4CgQXrGJJVJxE2rsQPBp19PbQ-G8FTI0lqp0aS1RjiYpxlUpM0MMJwpT-y6If3bHX2Fk_mnfO_of_AHJxevc</recordid><startdate>201610</startdate><enddate>201610</enddate><creator>Grebenkemper, Jason H.</creator><creator>Klemenz, Sebastian</creator><creator>Albert, Barbara</creator><creator>Bux, Sabah K.</creator><creator>Kauzlarich, Susan M.</creator><general>Elsevier Inc</general><general>Elsevier</general><scope>AAYXX</scope><scope>CITATION</scope><scope>OTOTI</scope></search><sort><creationdate>201610</creationdate><title>Effects of Sc and Y substitution on the structure and thermoelectric properties of Yb14MnSb11</title><author>Grebenkemper, Jason H. ; Klemenz, Sebastian ; Albert, Barbara ; Bux, Sabah K. ; Kauzlarich, Susan M.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c371t-2d3467d64f4af9f79bb7e81e0ef9d1a5d4395c1533601c799fc8c710f9eb9123</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2016</creationdate><topic>Chemical pressure</topic><topic>Rare earth compounds</topic><topic>Thermoelectric material</topic><topic>Zintl</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Grebenkemper, Jason H.</creatorcontrib><creatorcontrib>Klemenz, Sebastian</creatorcontrib><creatorcontrib>Albert, Barbara</creatorcontrib><creatorcontrib>Bux, Sabah K.</creatorcontrib><creatorcontrib>Kauzlarich, Susan M.</creatorcontrib><collection>CrossRef</collection><collection>OSTI.GOV</collection><jtitle>Journal of solid state chemistry</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Grebenkemper, Jason H.</au><au>Klemenz, Sebastian</au><au>Albert, Barbara</au><au>Bux, Sabah K.</au><au>Kauzlarich, Susan M.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Effects of Sc and Y substitution on the structure and thermoelectric properties of Yb14MnSb11</atitle><jtitle>Journal of solid state chemistry</jtitle><date>2016-10</date><risdate>2016</risdate><volume>242</volume><issue>P2</issue><spage>55</spage><epage>61</epage><pages>55-61</pages><issn>0022-4596</issn><eissn>1095-726X</eissn><abstract>Yb14MnSb11 is the most efficient bulk p-type thermoelectric material for high temperature applications. Materials with Y and Sc substitutions in Yb14MnSb11 were made both in Sn-flux and by ball milling. These small 3+ rare earth (RE) cations were introduced with the goal of providing chemical pressure on the structure. The RE3+ cation is smaller than Yb2+ and also donates one additional electron to this p-type semiconductor. In Yb14−xRExMnSb11 (RE = Sc, Y) the maximum x was about 0.5. X-ray diffraction experiments on the single crystals obtained from Sn-flux showed that Sc preferentially substitutes for Yb(1) and Yb(3), and decreases the size of the unit cell by about 0.3%. Y substitutes on all Yb sites and increases the size of the unit cell by about 0.2%. Samples with Yb14−xRExMnSb11 (x~0.3) were prepared via powder metallurgy and spark plasma sintering for transport and thermal conductivity measurements. Electron microprobe of the Sc-substituted sample showed small regions (≤1 μm) containing greater amounts of Sc, and X-ray powder diffraction of the ball milled Sc sample could be fitted as phase pure Yb14−xScxMnSb11. Y-substituted samples showed larger regions of excess Y in electron microprobe, and small amounts of Yb4Sb3 in X-ray powder diffraction. The Sc sample has slightly reduced carrier concentration over optimized Yb14MnSb11, while the Y samples have even lower carrier concentrations. These carrier concentrations lead to comparable resistivity to Yb14MnSb11 in the Sc-substituted material, and higher resistivities in the Y-substituted material. All materials had similar Seebeck coefficients that slightly exceed Yb14MnSb11 at high temperatures, with the Sc-substituted sample having the highest despite having a higher carrier concentration. Sc-substituted samples also had a slightly higher thermal conductivity over the Y-substituted samples, which had comparable thermal conductivity to Yb14MnSb11. The zT values of the Sc and Y substituted samples are similar (zT1000K~0.8), however below that of Yb14MnSb11 due to the compensation of Seebeck and resistivity.
Chemical pressure of the Sc substituted Yb14MnSb11 provides a viable method for enhancing the Seebeck coefficient.
[Display omitted]
•Yb14−xRExMnSb11 (RE=Sc, Y) were synthesized from Sn flux and stoichiometric powders.•Sc substitution decreases the size of the unit cell while Y increases it.•Sc substitution slightly reduces carrier concentration and Y decreases it further.•Y substitution results in significantly higher resistivity.•Both substitutions result in similar Seebeck coefficients and zT values.</abstract><cop>United States</cop><pub>Elsevier Inc</pub><doi>10.1016/j.jssc.2016.03.015</doi><tpages>7</tpages><oa>free_for_read</oa></addata></record> |
fulltext | fulltext |
identifier | ISSN: 0022-4596 |
ispartof | Journal of solid state chemistry, 2016-10, Vol.242 (P2), p.55-61 |
issn | 0022-4596 1095-726X |
language | eng |
recordid | cdi_osti_scitechconnect_1434060 |
source | Elsevier |
subjects | Chemical pressure Rare earth compounds Thermoelectric material Zintl |
title | Effects of Sc and Y substitution on the structure and thermoelectric properties of Yb14MnSb11 |
url | http://sfxeu10.hosted.exlibrisgroup.com/loughborough?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-01-27T16%3A14%3A09IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-elsevier_osti_&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Effects%20of%20Sc%20and%20Y%20substitution%20on%20the%20structure%20and%20thermoelectric%20properties%20of%20Yb14MnSb11&rft.jtitle=Journal%20of%20solid%20state%20chemistry&rft.au=Grebenkemper,%20Jason%20H.&rft.date=2016-10&rft.volume=242&rft.issue=P2&rft.spage=55&rft.epage=61&rft.pages=55-61&rft.issn=0022-4596&rft.eissn=1095-726X&rft_id=info:doi/10.1016/j.jssc.2016.03.015&rft_dat=%3Celsevier_osti_%3ES0022459616300883%3C/elsevier_osti_%3E%3Cgrp_id%3Ecdi_FETCH-LOGICAL-c371t-2d3467d64f4af9f79bb7e81e0ef9d1a5d4395c1533601c799fc8c710f9eb9123%3C/grp_id%3E%3Coa%3E%3C/oa%3E%3Curl%3E%3C/url%3E&rft_id=info:oai/&rft_id=info:pmid/&rfr_iscdi=true |