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VxMo₁-xO₂系の1373Kにおける相関係
http://hdl.handle.net/10076/4737
http://hdl.handle.net/10076/4737632780ae-22c5-4be0-8cf5-ace07a7d52ee
| 名前 / ファイル | ライセンス | アクション |
|---|---|---|
AN002341990360010.PDF (241.0 kB)
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| Item type | 紀要論文 / Departmental Bulletin Paper(1) | |||||
|---|---|---|---|---|---|---|
| 公開日 | 2007-07-02 | |||||
| タイトル | ||||||
| タイトル | VxMo₁-xO₂系の1373Kにおける相関係 | |||||
| 言語 | ja | |||||
| 言語 | ||||||
| 言語 | jpn | |||||
| 資源タイプ | ||||||
| 資源タイプ識別子 | http://purl.org/coar/resource_type/c_6501 | |||||
| 資源タイプ | departmental bulletin paper | |||||
| 著者 |
新居, 淳二
× 新居, 淳二× 大森, 雅彦 |
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| 抄録 | ||||||
| 内容記述タイプ | Abstract | |||||
| 内容記述 | Phase relations in the VxMo₁-xO₂ system were investigated by a powder X-ray diffractometry for samples quenched from 1373K. The results are shown in Fig. 4 together with those reported by Marinder. Two types of crystal structures were found in this system. One was MoO₂-type(M¹) and another was rutile-type (R) structure. Boundary of M₁ and R was estimated as x=0.32 by X-ray diffraction patterns of the samples (Fig.1). At x=0.20, two phases with same MoO₂-type structure coexisted, and the two-phase region was estimated as 0.18≦x≦0.22(Fig.2). Lattice parameters for M₁ and R are illustrated as functions of composition in Fig.3. Variation of c-parameter in R was explained by the cation distribution in the VxMo₁-x O₂ and interaction of d-electrons in the cations. | |||||
| 書誌情報 |
三重大学教育学部研究紀要. 自然科学 巻 36, p. 53-56, 発行日 1985-03-01 |
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| ISSN | ||||||
| 収録物識別子タイプ | PISSN | |||||
| 収録物識別子 | 0389-9225 | |||||
| 書誌レコードID | ||||||
| 収録物識別子タイプ | NCID | |||||
| 収録物識別子 | AN00234199 | |||||
| フォーマット | ||||||
| 内容記述タイプ | Other | |||||
| 内容記述 | application/pdf | |||||
| 著者版フラグ | ||||||
| 出版タイプ | VoR | |||||
| 出版タイプResource | http://purl.org/coar/version/c_970fb48d4fbd8a85 | |||||
| その他のタイトル | ||||||
| 言語 | en | |||||
| 値 | Phase Relations in the VxMO₁-xO₂ System at 1373K | |||||
| 出版者 | ||||||
| 出版者 | 三重大学教育学部 | |||||
| 資源タイプ（三重大） | ||||||
| 値 | Departmental Bulletin Paper / 紀要論文 | |||||
