{"title":"Thermoelectric properties of ternary and Al-containing quaternary Ru1−xRexSiy chimney–ladder compounds","authors":"Kyosuke Kishida, Akira Ishida, Tatsuya Koyama, Shunta Harada, Norihiko L. Okamoto, Katsushi Tanaka, Haruyuki Inui","doi":"10.1016/j.actamat.2008.12.039","DOIUrl":null,"url":null,"abstract":"<div><p>The thermoelectric properties of ternary and Al-containing quaternary Ru<sub>1−</sub><em><sub>x</sub></em>Re<em><sub>x</sub></em>Si<em><sub>y</sub></em> chimney–ladder phases have been studied as a function of the Re concentration with the use of directionally solidified alloys. The Ru<sub>1−</sub><em><sub>x</sub></em>Re<em><sub>x</sub></em>Si<em><sub>y</sub></em> chimney–ladder phases exhibit n- and p-type semiconducting behaviors, respectively, at low and high Re concentrations, at which the X(=Si)/M(=Ru<!--> <!-->+<!--> <!-->Re) ratios are respectively, larger and smaller than those expected from the VEC (valence electron concentration)<!--> <!-->=<!--> <!-->14 rule. The absolute values of both Seebeck coefficient and electrical resistivity increase as the extent of the deviation from the VEC<!--> <!-->=<!--> <!-->14 rule increases, i.e. as the alloy composition deviates from that corresponding to the p–n transition (<em>x</em> <!-->≈<!--> <!-->0.5), indicating that the carrier concentration can be controlled by changing the extent of compositional deviation from the ideal VEC<!--> <!-->=<!--> <!-->14 composition. The highest values of the dimensionless figure of merit obtained are 0.47 for ternary (<em>x</em> <!-->=<!--> <!-->0.60) and 0.56 for Al-containing quaternary alloys. The reasons for the systematic compositional deviation from the ideal VEC<!--> <!-->=<!--> <!-->14 compositions observed for a series of chimney–ladder phases are discussed in terms of atomic packing.</p></div>","PeriodicalId":238,"journal":{"name":"Acta Materialia","volume":"57 6","pages":"Pages 2010-2019"},"PeriodicalIF":9.3000,"publicationDate":"2009-04-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/j.actamat.2008.12.039","citationCount":"21","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Acta Materialia","FirstCategoryId":"88","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S1359645409000172","RegionNum":1,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"MATERIALS SCIENCE, MULTIDISCIPLINARY","Score":null,"Total":0}
引用次数: 21
Abstract
The thermoelectric properties of ternary and Al-containing quaternary Ru1−xRexSiy chimney–ladder phases have been studied as a function of the Re concentration with the use of directionally solidified alloys. The Ru1−xRexSiy chimney–ladder phases exhibit n- and p-type semiconducting behaviors, respectively, at low and high Re concentrations, at which the X(=Si)/M(=Ru + Re) ratios are respectively, larger and smaller than those expected from the VEC (valence electron concentration) = 14 rule. The absolute values of both Seebeck coefficient and electrical resistivity increase as the extent of the deviation from the VEC = 14 rule increases, i.e. as the alloy composition deviates from that corresponding to the p–n transition (x ≈ 0.5), indicating that the carrier concentration can be controlled by changing the extent of compositional deviation from the ideal VEC = 14 composition. The highest values of the dimensionless figure of merit obtained are 0.47 for ternary (x = 0.60) and 0.56 for Al-containing quaternary alloys. The reasons for the systematic compositional deviation from the ideal VEC = 14 compositions observed for a series of chimney–ladder phases are discussed in terms of atomic packing.
期刊介绍:
Acta Materialia serves as a platform for publishing full-length, original papers and commissioned overviews that contribute to a profound understanding of the correlation between the processing, structure, and properties of inorganic materials. The journal seeks papers with high impact potential or those that significantly propel the field forward. The scope includes the atomic and molecular arrangements, chemical and electronic structures, and microstructure of materials, focusing on their mechanical or functional behavior across all length scales, including nanostructures.