Electronic States in Zinc Magnesium Oxide Alloy Semiconductors: Hard X-ray Photoemission Spectroscopy and Density Functional Theory Calculations

被引:12
作者
Ohsawa, Takeo [2 ]
Adachi, Yutaka [1 ,3 ]
Sakaguchi, Isao [1 ,3 ]
Matsumoto, Kenji [2 ,4 ]
Haneda, Hajime [2 ,4 ]
Ueda, Shigenori [5 ]
Yoshikawa, Hideki [5 ]
Kobayashi, Keisuke [5 ]
Ohashi, Naoki [1 ,3 ,4 ]
机构
[1] Natl Inst Mat Sci, Int Ctr Mat Nanoarchitecton MANA, Optron Mat Ctr, Tsukuba, Ibaraki 3050044, Japan
[2] Natl Inst Mat Sci, Sensor Mat Ctr, Tsukuba, Ibaraki 3050044, Japan
[3] Natl Inst Mat Sci, Optron Mat Ctr, Tsukuba, Ibaraki 3050044, Japan
[4] Kyushu Univ, Dept Appl Sci Elect & Mat ASEM, Fukuoka 8168580, Japan
[5] NIMS Beamline Stn SPring 8, Sayo, Hyogo 6795148, Japan
关键词
PHOTOELECTRON-SPECTROSCOPY; POPULATION ANALYSIS; VALENCE-BAND; THIN-FILMS; WAVE; SOLIDS;
D O I
10.1021/cm802467n
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
The electronic states of zinc magnesium oxide (Zn1-xMgx)O thin films were determined exactly by hard X-ray photoemission spectroscopy (HX-PES) using synchrotron radiation. The Zn 2p core level was shifted to a higher binding energy along with widening of the bandgap by alloying with MgO, whereas the shift of the 0 Is peak was less than that of the Zn 2p peak. Density functional theory (DFT) calculations revealed that the electronic state of an 0 ion bonding with an adjacent Mg ion is remarkably different from that not bonding with a Mg ion. As a result, the energy shift observed in the 0 Is peak results from a combination of the expansion of the bandgap energy and the chemical shift due to a change in the ionicity. The Fermi level is always situated just below the conduction band; this suggests that a shallow donor can be added, even in the alloy film with very high MgO fraction, for example, x = 0.47.
引用
收藏
页码:144 / 150
页数:7
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