Koichi Izumi
University of Tokyo
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Featured researches published by Koichi Izumi.
Review of Scientific Instruments | 1992
Tetsuya Ishikawa; Yoshitaka Yoda; Koichi Izumi; Carlos K. Suzuki; Xiaowei Zhang; Masami Ando; Seishi Kikuta
A versatile precision diffractometer for nuclear Bragg scattering was designed and constructed at the Photon Factory. Standardized component goniometers can be arranged to address various requirements of incident beam conditioning for nuclear Bragg scattering, including a high‐energy resolution monochromator with wide angular acceptance as well as a circularly polarized incident beam.
Japanese Journal of Applied Physics | 1991
Keiichi Hirano; Koichi Izumi; Tetsuya Ishikawa; Shoichi Annaka; Seishi Kikuta
An X-ray phase plate using two-beam Bragg case diffraction is proposed. The variation of the polarization state of the transmitted (forward-diffracted) beam through the incident angle was observed. Left-handed and right-handed circular polarizations whose degree of circular polarizations were ±0.90 were experimentally produced.
Hyperfine Interactions | 1992
Seishi Kikuta; Yoshitaka Yoda; Yuji Hasegawa; Koichi Izumi; Tetsuya Ishikawa; X. W. Zhang; Shunji Kishimoto; Hiroshi Sugiyama; T. Matsushita; Masami Ando; Carlos K. Suzuki; Makoto Seto; Hideo Ohno; Humihiko Takei
Experiments of nuclear Resonant scattering carried out at PF and TRISTAN-AR of KEK are described, which include nuclear Bragg scattering in time domain as well as energy domain, time-resolved nuclear resonant forward scattering, and interferometric studies.
Japanese Journal of Applied Physics | 1991
Seishi Kikuta; Yoshitaka Yoda; Yoshihiro Kudo; Koichi Izumi; Tetsuya Ishikawa; Carlos Kenichi Suzuki; Hideo Ohno; Humihiko Takei; Kan Nakayama; Xiaowei Zhang; Tadashi Matsushita; Shunji Kishimoto; Masami Ando
Nuclear Bragg scattering from a synthesized α-57Fe2O3 crystal was observed with 450 cps at beamline 16 of the Photon Factory. Mossbauer absorption spectra of the scattered beam were measured by oscillating the scatterer crystal while maintaining its Bragg condition. Time distribution of the scattered beam was measured with 300 ps resolution.
Surface Science | 1987
Toshio Takahashi; Koichi Izumi; Tetsuya Ishikawa; Seishi Kikuta
The structure of the 3 x 3 structure on the Si(111) clean surface has been studied using X-ray diffraction under the nearly normal incidence condition. A thin substrate crystal, about 5 μm in thickness, was used to reduce the background scattering. From the analysis of the intensity distribution of diffraction patterns, evidence for a trimer of Bi atoms was obtained and the distance between Bi atoms forming the trimer was found to be 3.10±0.1 A.
Japanese Journal of Applied Physics | 1992
Vitali V. Aristov; Yuri A. Basov; Timour E. Goureev; A. Snigirev; Tetsuya Ishikawa; Koichi Izumi; Seishi Kikuta
Hard X-ray focusing by a linear phase Bragg-Fresnel crystal lens was performed with an efficiency close to 30%. The phase shift of an incident beam was controlled by deviating the crystal lens from the exact Bragg condition. Analytical expressions for the intensity and the image contrast at the focal point was presented.
Japanese Journal of Applied Physics | 1989
Koichi Izumi; Toshio Takahashi; Seishi Kikuta
The atomic structure of Si(111) √3×√3-In was investigated by low energy ion scattering spectroscopy with 1 keV He+ ions. Azimuthal angular distributions of scattered ions suggest that the In atoms are located in the three-fold sites on top of the second layer Si atoms. Comparing the experimental distribution as a function of the incident angle with the calculation using the Thomas-Fermi-Moliere potential taking of the thermal vibrations, the Debye temperature of the surface In atoms and the bond length between the In atom and the first layer Si atom were estimated.
Japanese Journal of Applied Physics | 1995
Koichi Izumi; Takaya Mitsui; Makoto Seto; Yoshitaka Yoda; Tetsuya Ishikawa; Xiaowei Zhang; Masami Ando; Seishi Kikuta
Interferometry of the nuclear Bragg scattered X-rays from 57Fe2O3 (777) with the optical path difference of 2.4 mm was reported. In order to carry out this measurement, a new X-ray interferometer of the wavefront-dividing type was designed and fabricated. The interference pattern was observed using this X-ray interferometer, since the temporal coherence length of the nuclear resonantly scattered X-rays is much longer than the optical path difference. From the visibility of the interference pattern, the vertical size of the X-ray source was estimated to be 50 µ m.
Review of Scientific Instruments | 1992
Carlos K. Suzuki; Hideo Ohno; Humihiko Takei; Fumiko Sakai; Yoshitaka Yoda; Yoshihiro Kudo; Koichi Izumi; Tetsuya Ishikawa; Seishi Kikuta; Xiao W. Zhang; Tadashi Matsushita; Masami Ando
High quality single crystals or thin films containing Mossbauer isotopes are the main x‐ray optical component for nuclear Bragg scattering (NBS) with synchrotron radiation. For this purpose, flux grown α‐57Fe2O3 (hematite) single crystals prepared in two growth runs have been characterized by plane wave x‐ray topography, which indicated the most suitable sample. Measurements of (111), (333), (555), (777), and (999) pure nuclear‐reflection profiles showed a good agreement of relative reflectivity with the values calculated from theory. At the beamline NE‐3, accumulation ring of TRISTAN, a Mossbauer event rate as high as 13 000 cps for (777) reflection was observed.
Japanese Journal of Applied Physics | 2002
Shigeru Kimura; Yasushi Kagoshima; Kenji Kobayashi; Koichi Izumi; Yasutaka Sakata; S. Sudo; Yoshiyuki Yokoyama; Toshihiro Niimi; Yoshiyuki Tsusaka; Junji Matsui
We developed a micro-area X-ray diffraction system using a sub-µm X-ray beam of 10 keV energy that was produced by a phase zone plate made of tantalum. Using this system, we were able to measure the lattice strain distribution in InGaAsP metalorganic vapor phase epitaxial layers selectively grown on InP stripe regions a few µm in width between a pair of SiO2 mask stripes, with strain sensitivity of about 1×10-4. We found that the strain distribution in a 3-µm-wide stripe layer is almost completely uniform, while that in a 4-µm-wide layer is not.