| Project/Area Number |
61850006
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| Research Category |
Grant-in-Aid for Developmental Scientific Research
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| Allocation Type | Single-year Grants |
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| Research Field |
Applied materials
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| Research Institution | Department of Physics, Gakushuin University |
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Principal Investigator |
OGAWA Tomoya Department of Physics, Gakushuin University, 理学部, 教授 (50080437)
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| Co-Investigator(Kenkyū-buntansha) |
NANGO Nobuhito Ratoc System Engineering, 代表取締役
KOJIMA Takahiro Department of Physics, Gakushuin University, 商学部, 教授 (50070272)
KAWAI Yoriyoshi Department of Physics, Gakushuin University, 理学部, 研究員 (30158860)
SAKAI Kazufumi Department of Physics, Gakushuin University, 理学部, 助手 (40205703)
大塚 謙一 学習院大学, 理, 助手 (30101588)
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| Project Period (FY) |
1986 – 1988
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| Project Status |
Completed (Fiscal Year 1988)
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| Budget Amount *help |
¥37,000,000 (Direct Cost: ¥37,000,000)
Fiscal Year 1988: ¥5,500,000 (Direct Cost: ¥5,500,000)
Fiscal Year 1987: ¥10,500,000 (Direct Cost: ¥10,500,000)
Fiscal Year 1986: ¥21,000,000 (Direct Cost: ¥21,000,000)
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| Keywords | Infrared Light Scattering / Resonance Scattering / Compound Semiconductors / Lattice defects / Crystal Growth / 光散乱トモグラフィー / 光散乱 / 画像処理 |
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| Research Abstract |
Since scattering intensity of IR light is dependent upon electronic polarization or displacement of electrons cause by the incident light, the light scattering from semiconductors will be classified into the following three items:
1. the polarization induced by electrons traped in electronic centers and/OR defects in semiconductor crystals. Here, the electrons show restoring force against their displacement and then they have their own resonance frequencies which are determined by the mass and restoring force of the electrons.
2. the polarization due to electrons in tiny particles inside semiconductors, which will show a resonance similar to the plasma resonance inside metal particles.
3. Polarization due free carriers, which will mainly contribute to absorption because of no restoring force against displacement of electrons.
The resonance mentioned above the category 1 and 2 will be observed if we abjust temperature of the specimens to be examind or frequency of incident IR light. Unfortunately, we don't have any tuneable laser in the frequency range of 1 micron.
Here, the sample is installed in a cryostat which temperature is changed by a refrigerator from room temperature to 24K. The stability of the temperature is 0.1 K. Thus, we have clearly observed resonance type scattering from an In-doped GaAs crystal at 130 K by 1.15mu m radiation of a He-Ne Laser, which was confirmed experimentally.
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