Hybridization of Cr 3d-N 2p-Ga 4s in the wide band-gap diluted magnetic semiconductor Ga1-xCrxN
Inquiry number
SOL-0000000942
Beamline
BL47XU (Micro-CT)
Scientific keywords
A. Sample category | inorganic material |
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B. Sample category (detail) | semiconductor, magnetic material |
C. Technique | photoemission, photoionization |
D. Technique (detail) | photoelectron spectra |
E. Particular condition | interface |
F. Photon energy | X-ray (4-40 keV) |
G. Target information | function, electronic state, spin/magnetism |
Industrial keywords
level 1---Application area | Semiconductor |
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level 2---Target | compound semiconductor |
level 3---Target (detail) | electric rod |
level 4---Obtainable information | electronic state, chemical state |
level 5---Technique | XPS |
Classification
A40.40 surface・interface chemistry, A80.12 semiconductor, A80.14 magnetic materials, M50.10 photoelectron spectroscopy
Body text
Hole-mediated ferromagnetism has produced reliable estimates of Curie temperature (Tc) for diluted magnetic semiconductors (DMS) such as GaMnAs and predicts that GaMnN will have a Tc above room temperature (RT). However, since doped transition metals introduce deep levels in wide band gap semiconductors like GaN and carriers are localized in these states, it may be difficult to apply the hole-mediated ferromagnetism model to wide band gap GaN-based DMS. Therefore, a different mechanism for magnetism will play a role in GaN-based DMS rather than hole-mediated ferromagnetism. In order to get insight into the mechanism of the magnetism, an electronic structure investigation of GaN-based DMS is necessary. In this research, we have investigated the electronic structure of Cr-doped GaN observed by bulk sensitive hard X-ray photoemission spectroscopy at the excitation energy of 5.95keV. Figure shows the normalized energy distribution curves (EDC’s) of undoped GaN, that of Ga0.899Cr0.101N, and the difference spectrum between them, respectively. The Cr-doping does introduce, clearly, new electronic levels in the band gap (C) and causes some change in the valence band structure (A and B). Considering atomic subshell cross section at the excitation energy, the main contribution of the valence band spectra is Ga 4s. The decrease of the intensity in the valence band spectrum by Cr-doping is not only due to the decrease of Ga content but also to the effect of Cr-doping. Namely, the Cr-doping effect on the valence band of GaN and make the in-gap energy state by hybridization between Cr 3d and the second neighbor Ga 4s via the formation of Cr-N bonds. In the Ga 2p core level study, we also observed that the Cr doping influences the second neighbor Ga via the formation of Cr-N bonds. The strong hybridization between Cr 3d and the second neighbor Ga 4s induce the long range interaction between Cr 3d electrons and may an important role in the ferromagnetism of Ga1-xCrxN.
The normalized energy distribution curves (EDC’s) of undoped GaN, that of Ga0.899Cr0.101N, and the difference spectrum between them, respectively.
[ J.-J. Kim, H. Makino, K. Kobayashi, Y. Takata, T. Yamamoto, T. Hanada, M.-W. Cho, E. Ikenaga, M. Yabashi, D. Miwa, Y. Nishino, K. Tamasaku, T. Ishikawa, S. Shin and T. Yao, Physical Review B 70, 161315(R) (2004), Fig. 1,
©2004 American Physical Society ]
Source of the figure
Original paper/Journal article
Journal title
Phys.Rev.B70, 161315(R)(2004)
Figure No.
Technique
In this research, we have investigated the electronic structure of Cr-doped GaN observed by bulk sensitive hard X-ray photoemission spectroscopy at the excitation energy of 5.95 keV.
Source of the figure
Original paper/Journal article
Journal title
Phys.Rev.B70, 161315(R) (2004)
Figure No.
Required time for experimental setup
1 shift(s)
Instruments
Instrument | Purpose | Performance |
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Hard X-ray Photoemission Spectroscopy System | Analysis of electronic states in solid and/or interface | Total Energy Resolution: 85meV |
References
Related experimental techniques
Questionnaire
The measurement was possible only in SPring-8. Impossible or very difficult in other facilities.
This solution is an application of a main instrument of the beamline.
This solution is application of a new instrument installed in the past two years.
Ease of measurement
Easy
Ease of analysis
Middle
How many shifts were needed for taking whole data in the figure?
Four-nine shifts