※一部利用できない機能があります
1.
図書 |
酒井忠司 [ほか] 編集委員, 宮﨑照宣編集協力委員
|
|||||||
2.
図書 |
関東学院大学材料・表面工学研究所編
|
|||||||
3.
図書 |
澤彰仁著
|
|||||||
4.
図書 |
隅山兼治著
|
|||||||
5.
図書 |
表面技術協会編
|
|||||||
6.
電子ブック |
日本学術振興会薄膜第131委員会編集企画 ; 吉田貞史, 近藤高志編著
|
|||||||
7.
図書 |
日本学術振興会薄膜第131委員会編集企画 ; 吉田貞史, 近藤高志編著
|
|||||||
8.
図書 |
小島啓安著
|
|||||||
9.
論文 |
オチ, ケイタ ; オクサワ, マコト ; Ochi, Keita ; Okusawa, Makoto ; 越智, 啓太 ; 奥沢, 誠
概要:
Departmental Bulletin Paper<br />Eight Fe-films with a thickness different from one another have been prepared by deposi
…
ted on clean Sm surfaces with accuracy of 0.1 nm (Fe(d nm)/Sm(10.0nm)(d=0.3,0.5,0.7,1.0,1.5,2.0,5.0,10.0)),and the\nFe 2p3/2XPS spectra of the films have been,in situ,measured at about 8K and room temperature. A shift in the binding energy position of the Fe 2p3/2lines is found to depend on the film thickness and the temperature.\nAt both temperatures,the shift from a peak position of the Fe 2p3/2line in Fe(10.0nm)/Sm(10.0nm)is hardly found in the range of~1-10 nm,whereas it increases monotonously to the low binding energy side as the film\nthickness decreases in the range of 0.1-~1nm. The value of the shift at about 8K seems to be larger than that at room temperature slightly in the range of 0.1-~1nm. Comparing with the case of Sm(d nm)/Fe(10.0nm)\nfrom Chihiro IIJIMA and Makoto OKUSAWA (2010),this suggests that a change in an electronic state takes place in the vicinity of a Fe-Sm interface,and that a charge density on the Fe side becomes large and that on\nthe Sm side small. Detailed discussion will be presented elsewher.
続きを見る
|
|||||||
10.
図書 |
日本学術振興会透明酸化物光・電子材料第166委員会編
|