@article{oai:kyutech.repo.nii.ac.jp:00005075,
 author = {宍戸, 統悦 and Shishido, Toetsu and 湯葢, 邦夫 and Yubuta, Kunio and 森, 孝雄 and Mori, Takao and 田中, 雅彦 and Tanaka, Masahiko and 工藤, 邦男 and Kudou, Kunio and 岡田, 繁 and Okada, Shigeru and 野村, 明子 and Nomura, Akiko and 菅原, 孝昌 and Sugawara, Takamasa and 佐原, 亮二 and Sahara, Ryoji and 林, 好一 and Hayashi, Koichi and Kohiki, Shigemi and 古曵, 重美 and 澤田, 豊 and Sawada, Yutaka and 手嶋, 勝弥 and Teshima, Katsuya and 大石, 修治 and Oishi, Shuji and 川添, 良幸 and Kawazoe, Yoshiyuki and 吉川, 彰 and Yoshikawa, Akira},
 issue = {1},
 journal = {Journal of Flux Growth},
 month = {Jun},
 note = {Polycrystalline samples ofYRh3Bx are prepared by the arc melting synthetic method. Perovskite-type cubic phase (space group : Pm3m) of YRh3 Bx exists in the range of 0.50 ≤x≤1. Lattice parameterαof YRh3Bx depends on x, and varies linearly from a = 0.416347(4) nm (x = 1.000) to 0.408776(7) nm (x = 0.500). The value of Vickers microhardness ofYRh3Bx ranges from 7.7 to 2.7 GPa. Hardness decreases with decreasing of boron content x. The TEM observation reveals that the anomalous softening of hardness in the vicinity of x = 0.5 for YRh3 Bx is caused by the appearance of the modulated structure. By the TG-DTA, oxidation of YRh3B1.ooo starts at 541 K. The weight gain by oxidation is 11.4 %. The oxidized product is mixed phase of YB03 and Rh. The densi!Y of states at the Fermi level, D (EF), of YRh3 B1 .ooo (20 at.%B) is indicated to be slightly larger than that of YRh3B0.706(15 at.%B).},
 pages = {12--17},
 title = {ぺロブスカイト型YRh3Bのホウ素不定比と性質に関する研究},
 volume = {8},
 year = {2013},
 yomi = {コヒキ, シゲミ}
}