K. Yubuta, S. Okada, Y. Miyazaki, I. Terasaki, T. Kajitani
{"title":"High-resolution electron microscopy of thermoelectric compounds Bi-(Sr,Ba)-Rh-O","authors":"K. Yubuta, S. Okada, Y. Miyazaki, I. Terasaki, T. Kajitani","doi":"10.1109/ICT.2006.331286","DOIUrl":null,"url":null,"abstract":"The crystal structures of thermoelectric (TE) compounds Bi<sub>1.91</sub>Sr<sub>2.0</sub>Rh<sub>1.77</sub>O<sub>x</sub> and Bi <sub>2.12</sub>Ba<sub>2.00</sub>Rh<sub>1.95</sub>O<sub>x</sub> are investigated by means of electron diffraction measurements and high-resolution electron microscopy. These compounds have layered structures and consist of two interpenetrating subsystems exhibiting incommensurated periodicities along b-axis. Both subsystems, CdI<sub>2 </sub>-type RhO<sub>2</sub> sheets and a distorted four-layered rock-salt (RS)-type (Bi,(Sr,Ba))O blocks, have common a-, c-axes and beta;-angles. On the other hand, the ratios of two axis lengths, i.e., b <sub>1</sub> (RhO<sub>2</sub> sheet) / b<sub>2</sub> (RS-type block), are irrational. Based on the cation ratio and b<sub>1</sub>/b<sub>2</sub> value, the structural formulae are expressed as [(Bi<sub>1-x></sub>Rh<sub>x</sub>)<sub>2</sub>(Sr<sub>1-y</sub>Bi <sub>y</sub>)<sub>2</sub>O<sub>4+delta</sub>]<sub>0.63</sub>RhO<sub>2 </sub> with x = 0.077, y = 0.016 and delta = 0.46 for the Sr-system and [(Bi<sub>1-x></sub>Rh<sub>x</sub>)<sub>2</sub>(Sr<sub>1-y</sub>Bi <sub>y</sub>)<sub>2</sub>O<sub>4+delta</sub>]<sub>0.56</sub>RhO<sub>2 </sub> with x = 0.037, y = 0.047 and delta = 0.39 for the Ba-system, respectively. Based on the electron diffraction measurements, it is found that these compounds have irrational modulation vectors, q<sub>1 </sub> = -a* + 0.63b<sub>1</sub>* and q<sub>2</sub> = 0.17b<sub>1</sub>* + c for Bi-Sr-Rh-O, and q<sub>1</sub> = -a* + 0.56b<sub>1</sub>* and q <sub>2</sub> = 0.11b<sub>1</sub>* + 0.35c* for Bi-Ba-Rh-O, respectively, being the indications of (3+2) dimensional structures. High-resolution images taken with the incident electron beam parallel to the a- and c-axes clearly exhibit modulated atomic arrangements. These compounds are characterized by the displacement modulations in both RhO<sub>2</sub> layers and the RS-type blocks","PeriodicalId":346555,"journal":{"name":"2006 25th International Conference on Thermoelectrics","volume":"49 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2006-08-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"2006 25th International Conference on Thermoelectrics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/ICT.2006.331286","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
The crystal structures of thermoelectric (TE) compounds Bi1.91Sr2.0Rh1.77Ox and Bi 2.12Ba2.00Rh1.95Ox are investigated by means of electron diffraction measurements and high-resolution electron microscopy. These compounds have layered structures and consist of two interpenetrating subsystems exhibiting incommensurated periodicities along b-axis. Both subsystems, CdI2 -type RhO2 sheets and a distorted four-layered rock-salt (RS)-type (Bi,(Sr,Ba))O blocks, have common a-, c-axes and beta;-angles. On the other hand, the ratios of two axis lengths, i.e., b 1 (RhO2 sheet) / b2 (RS-type block), are irrational. Based on the cation ratio and b1/b2 value, the structural formulae are expressed as [(Bi1-x>Rhx)2(Sr1-yBi y)2O4+delta]0.63RhO2 with x = 0.077, y = 0.016 and delta = 0.46 for the Sr-system and [(Bi1-x>Rhx)2(Sr1-yBi y)2O4+delta]0.56RhO2 with x = 0.037, y = 0.047 and delta = 0.39 for the Ba-system, respectively. Based on the electron diffraction measurements, it is found that these compounds have irrational modulation vectors, q1 = -a* + 0.63b1* and q2 = 0.17b1* + c for Bi-Sr-Rh-O, and q1 = -a* + 0.56b1* and q 2 = 0.11b1* + 0.35c* for Bi-Ba-Rh-O, respectively, being the indications of (3+2) dimensional structures. High-resolution images taken with the incident electron beam parallel to the a- and c-axes clearly exhibit modulated atomic arrangements. These compounds are characterized by the displacement modulations in both RhO2 layers and the RS-type blocks