Koichiro Misu
Mitsubishi Electric
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Publication
Featured researches published by Koichiro Misu.
Japanese Journal of Applied Physics | 1997
Akira Yamada; Chisako Maeda; Toshio Umemura; Fusaoki Uchikawa; Koichiro Misu; Shusou Wadaka; Takahide Ishikawa
Film bulk acoustic wave resonators (FBAWRs) at the GHz band were successfully fabricated using piezoelectric lead titanate, PbTiO 3 (PT) films on GaAs substrates by a process similar to that used in microwave integrated circuit (MIC) fabrication. PT films deposited on Pt/Ti bottom electrodes by RF magnetron sputtering oriented preferentially along the (111) crystal direction. Resonances of the bulk acoustic mode were observed around 1.9 GHz. The effective electromechanical coupling coefficient (k t 2 ) and electrical Q were estimated to be ∼9.4% and ∼65, respectively. The relationship between residual stress in the PT films and Q was investigated. It was found that stress in the PT film exerted a large influence on Q.
Japanese Journal of Applied Physics | 1999
Akira Yamada; Chisako Maeda; Fusaoki Uchikawa; Koichiro Misu; Toshihiko Honma
Bulk acoustic wave (BAW) resonators with 5-wt%-La2O3-doped PbTiO3 (PT) piezoelectric films were fabricated. The La-doped PT films had a dense, homogeneous morphology, as well as high crystallinity caused by the use of bottom electrodes with pure Pt-like surface layers. These PT films had remanent polarization of 110 mC/m2 at 200°C. Resonant frequencies of the fabricated devices were 1.4 GHz and 2.0 GHz. The electromechanical coupling coefficient (kt2) was estimated to be 11% at 1.4 GHz and 9.4% at 2.0 GHz, respectively. The PT films had superior kt2 in the GHz band. The capability of the RF devices with broad bandwidth was investigated.
international symposium on electromagnetic compatibility | 2009
Naoto Oka; Takefumi Kumamoto; Koichiro Misu; Shuichi Nitta
This study experimentally clarifies the relationship between the common mode noise induced on the cable connected to the signal trace of PCB and the differential mode noise on signal trace, converted from the common mode noise, due to the unbalance of differential signal trace by applying the measurement method that Test baluns are used as a load of the cable and a signal source. In this study, S13 (Differential mode noise) and S23 (Common mode noise) are measured by the network analyzer for evaluation. Finally, the effectiveness of the common mode choke on signal trace and the shielding for the cable for both common mode and differential mode noise reduction are evaluated.
international symposium on electromagnetic compatibility | 2012
Fujiyuki Nakamoto; Takeshi Uchida; Chiharu Miyazaki; Naoto Oka; Koichiro Misu
We studied a CMC model with a one-turn toroidal core, which is easily used in 3D field simulators. The calculation model of a CMC differs from the actual shape, so we need to correct the CMCs characteristics. When we calculated the noise-suppressing effect of the CMC, we used relative permeability, which differs from the actual value, to approximate the actual characteristics of a CMC. From the comparison of calculated results with measurement results, the calculated results were comparable to the measurement results. We confirmed the validity of our model.
international symposium on electromagnetic compatibility | 2009
Takeshi Uchida; Chiharu Miyazaki; Naoto Oka; Koichiro Misu; Yoshihiko Konishi
We examined about the electromagnetic field immunity test system applying the array antenna technology. This system is able to get the electric field uniformity and the high power electric field near the antenna, in a wideband, by the beam forming technology. We constructed an electromagnetic field immunity test system consisting of 64 elements array antenna as a prototype. In this paper, we calculated the electric field uniformity near electromagnetic field immunity test system. We measured electric distributions and compared with the calculated value and the measured value. From these results, the validity of the calculation method of the electric field uniformity near the test system was confirmed.
Integrated Ferroelectrics | 1998
Akira Yamada; Chisako Maeda; Takehiko Sato; Toshio Umemura; Fusaoki Uchikawa; Koichiro Misu; Shusou Wadaka
Abstract The bulk acoustic wave filters at GHz bands were fabricated using lead titanate, PbTiO3 (PT) piezoelectric films which were deposited by RF magnetron sputtering and were oriented along crystal direction. To improve the quality of PT films, the bottom electrodes which had the Ti-diffusion suppressible layers were designed and prepared. X-ray diffraction intensity of the PT(111) became 5 times larger and degree of crystal orientation became 2 times stronger in comparison with those of the former PT films. The filters using the improved PT films had the insertion loss of -14dB. The PT film had effective electromechanical coupling coefficient (k) of 31% and electrical Q of 50. This k value was superior to those of well-known ZnO and AlN piezoelectric films.
REVIEW OF PROGRESS IN QUANTITATIVE NONDESTRUCTIVE EVALUATION: Volume 20 | 2001
Tomonori Kimura; Shumpei Kameyama; Koichiro Misu; Shusou Wadaka; H. Tanaka
A design is presented for a probe, used for automatic ultrasonic testing for a round bar using the angle beam immersion technique, to improve a signal to noise ratio. It is defined based on a flaw echo height and a spurious echo height, taking into consideration of a time gate and variation of the flaw echo height along with a rotation of the probe round the bar. The result of the design is in good agreement with that of experiments.
Archive | 1996
Shusou Wadaka; Tsutomu Nagatsuka; Koichiro Misu; Tomonori Kimura; Mitsuhiro Koike; H. Ichikawa
In recent years, so called “digital ultrasonic test instruments” have been commercially available. These conventional instruments employ electrical impulse excitation of ultrasonic probes. In this configuration, waveforms of ultrasonic pulses into a test object are determined only by the characteristics of probes. This means that variation of probe characteristics causes variation of evaluated results and reproducibility of evaluation is poor. Furthermore, some of the conventional instruments do not provide enough information required for quantitative nondestructive evaluation (QNDE) about a test object, since ultrasonic echo signals are A/D converted after an envelope detector in a receiver and only information of echo height and position is obtained.
Archive | 1997
Shusou Wadaka; Koichiro Misu; Tsutomu Nagatsuka; Tomonori Kimura; Shumpei Kameyama
Archive | 2000
Koichiro Misu; Kenji Yoshida; Koji Ibata; Shusou Wadaka; Tsutomu Nagatsuka; Fusaoki Uchikawa; Akira Yamada; Chisako Maeda
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National Institute of Information and Communications Technology
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