Curriculum Vitaes
Profile Information
- Affiliation
- Assoiciate Professor, Institute of Space and Astronautical Science, Japan Aerospace Exploration AgencyAssociate Professor, School of Physical Sciences, The Graduate University for Advanced Studies
- J-GLOBAL ID
- 200901006137313045
- researchmap Member ID
- 1000253786
- External link
Research Interests
5Research Areas
1Research History
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Jul, 1998 - Sep, 2003
Education
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Apr, 1988 - Mar, 1991
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Apr, 1986 - Mar, 1988
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Apr, 1982 - Mar, 1986
Committee Memberships
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2007 - 2011
Awards
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May, 2009
Papers
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日本航空宇宙学会論文集, 73(3) 109-116, 2025Conventionally, the double-probe method is used to observe the electric field by the sounding rockets. In the double-probe method, two pairs of dipole antennas are equipped to observe the electric field of two orthogonal components in the spin plane perpendicular to the rocket axis. In this study, we establish an electric field analysis method using one pair of dipole antennas and investigate its error in order to reduce the size of the detector and the risk by reducing the number of extensions. The results show that the magnitude of the electric field has an error of ±12% and the direction of the electric field vector has an error of ±4º.
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AIAA SCITECH 2024 FORUM, 2024
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Experimental Astronomy, 54(2-3) 521-559, Dec, 2022 Peer-reviewed
Misc.
130-
電子情報通信学会大会講演論文集, 1(1) 241, Aug 13, 1997
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電子情報通信学会論文誌. B-2, 通信. 2, 無線通信・無線応用 = The Transactions of the Institute of Electronics, Information and Communication Engineers. B-2 / 電子情報通信学会 編, 79(8) 492-494, Aug, 1996
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電子情報通信学会大会講演論文集, 1996(Sogo Pt 4) 159, Mar 11, 1996
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電子情報通信学会大会講演論文集, 1996(Sogo Pt 2) 281, Mar 11, 1996
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電子情報通信学会大会講演論文集, 1996(Sogo Pt 4) 155, Mar 11, 1996
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On the permittivity measurement of unprocessed dielectric material with rectangular cavity resonatorTechnical Report of IEICE, SAT, 96(168) MW97-51, Jul 22, 1996We discuss a new method to measure a permittivity of sample material with the rectangular cavity resonator. A merit of this method is that it is unnesessary to cut the material so as to be inserted fit for the cavity size, and therfore experimental error related to the material dimension is avoidable. Theoretical calculation of the cavity resonant frequency, obtained by the FDTD method, is compared to measured one, for several cases of material width and the permittivity. Both freqiencies are in a reasonable agreement each other within an error of a few percents. The present result suggests that this method is very convetional and effective for the permittivity measurement and it also has a possibility for further application of the permittivity estimation which does not require any processing of the material.
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Physics of Space Plasmas edited by T. Chang and J.R. Jasperse (MIT Center for Theoretical Geo/Cosmo Plasma Physics, Cambridge, MA), 3-14, No.14, 1996
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IEICE technical report. Electromagnetic compatibility, 95(241) 17-24, Sep 20, 1995We present a possible suggestion of a way to measure a permittivity without cutting a sample material by means of the rectangular cavity resonator. The theoretical discussion on the possibility is made in this paper, based on the time variation and the resonance frequency of electromagnetic field inside cavity which is calculated by the FDTD method. The material permittivity estimated from the resonance frequency has a reasonable agreement with theoretical one within an error of a few percents. The present result suggests a possibility for further application of the permittivity estimation which does not require any processing of the material.
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Proceedings of the Society Conference of IEICE, 1995(1) 109, Sep 5, 1995
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電子情報通信学会大会講演論文集, 1995(Society B1) 175-4, Sep 5, 1995Standing-wave method in a rectangular waveguide is a convenient method for measuring the permittivity of the materials. But it is found the error due to the deformation became large when the test sample is deformated. In this paper, we applied FDTD which is powerful tool for solving waveguide problem to evaluate the error due to the deformation. As the results, we can estimate the error as a function of the deformation of sample.
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電子情報通信学会大会講演論文集, 1994(Shunki Pt 2), 1994
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電子情報通信学会大会講演論文集, 1994(Shunki Pt 2), 1994
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電子情報通信学会大会講演論文集, 1994(Shunki Pt 2), 1994
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電子情報通信学会大会講演論文集, 1994(Shuki Pt 2) 251, Sep 26, 1994
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IEICE technical report. Electromagnetic compatibility, 93(264) 31-37, Oct 12, 1993In this paper,we discuss on an aplication of the range doppler imaging to measurement of a wave absorbing characteristices without using a wave darkroom.For the 300x3OOmm metal plate,the measureable range of higher than 4O〜5OdB has been obtained.The nor mal incident characteristices of both vertical and porizontal polarization are in close agreement with the theoretial values. These results show that this metod can be applicable to the measurement method of absorbing not in the wave darkroom,but in an usual room.
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電子情報通信学会大会講演論文集, 1993(Shuki Pt 2), 1993
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通信総合研究所季報 / 通信総合研究所企画部研究連携室 編, 38(2) p145-152, Jun, 1992資料形態 : テキストデータ プレーンテキスト
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Vol.1, Comet Halley - A Paramount Communications Company, 1991
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宇宙科学研究所報告 特集, 25(25) 167-184, Jan, 1990Thermal electrons in the upper ionosphere are being studied by means of the scientific satellite "AKEBONO". The measurements are electron temperature, electron density and the distribution of electrons in the energy range of 0∿5eV. An overview of the experiment is given and preliminary results on the protonosphere and field aligned current region are presented.
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23 137-155, Mar, 1989Low energy component of protons in the solar wind was found by means of an observation with the spacecraft "SAKIGAKE". This component is always accompanied by a sudden change in the solar wind parameters such as interplanetary shocks. The difference of bulk speed between the low energy component and normal one amounts to about 60-140km/s, and is strongly affected by the configuration of the interplanetary magnetic field. It is shown that this low energy component was produced by the gyromotion of protons, through an acceleration mechanism, e. g., Fermi process. Furthermore, it seems that there are two types of accelerative process, though these mechanisms are unknown.
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23 179-190, Mar, 1989Numerical simulations of Boltzmann's equation have been carried out in order to investigate the anisotropy of the electron energy distribution in the topside F region ionosphere. The equation contains both electron-electron collisions and electron-ion collisions. The simulations were compared with the observational data obtained with the electron temperature probe on board the Ohzora satellite. The results show that the anisotropy of the electron energy distribution can be generated in the topside F region ionosphere and that the electron energy distribution can differ from the Maxwell distribution, when an electric field or temperature gradient (heat flux) exists in the plasma. The simulations also indicate the dependence of electron density on the anisotropy of the ionospheric electron energy distribution.
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53 1-14, Mar, 1988We investigate the heliographic latitude-longitude structure of solar wind speed between Sept. 1985 and Jan. 1987 through the analysis of the solar wind data obtained by Sakigake, Suisei, and IMP-8. Until Jan. 1986,both polar regians had a high-speed stream extended across the equatorial region. After Feb. 1986,high-speed streams were rarely seen on the equator and low-speed streams were ranged along the equator, although there remained a slight wavy pattern in the latitude-longitude structure. This wavy pattern has been stable till the end of 1986.
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21 61-73, Mar, 198827-day recurrence-associated phenomena of the solar wind (SOW), the plasma wave (PWP), and the interplanetary magnetic field (IMF) were detected by the Sakigake spacecraft. The heliospheric structures, having a neutral (current) sheet of ∿2×10^4km thickness and a "plasmasheet" of ≳7×10^5km thickness, during April, 1985-August, 1986 and September, 1986-July, 1987,were in the excursion and aligned phases, respectively. In the neutral sheet the IMF direction usually reverses in a minute. Using high time-resolution data, the average ion density and temperature in the heliospheric plasma sheet are also found to be ≳60/cc and ∿20×10^4K, respectively.
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52 1-14, Dec, 1987Periodic components were picked up by applying maximum entropy method to the visual brightness of comet Halley which was measured from the ground. 2.22 days' period appears between November 1985 and February 1986. This period is the same as obtained by using Planet-A and Vega imaging experiments. This rotational period shifts to 2.33 days after April 1986. 7.4 days' period is detected from March to April 1986. Millis and Schleicher also indicate that the rotational period of the comet is near 7.4 days. Between March and May 1986,3.4 days' period appears, which can be explained by assuming that 2.33 days' period is modulated by the period of 7.4 days.
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19 103-110, Mar, 1987Solar wind parameters measured by SAKIGAKE around the time of encounter with Halley comet are discussed Sakigake was in or near the neutral sheet of Heliomagnetosphere and therefore the solar wind velocily was comparatively slow. Interplanetary space was in a small disturbance period. Although a firm evidence does not exist that solar wind velocity was decelerated by Halley's comet, frequency spectrum analysis of the solar wind parameters shows the exisistence of water group ions.
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14 3-17, Mar, 1986Electron temperature was measured with planar plobes boarding on ISAS 10th scientific satellite "OHZORA". The simultaneous measurments of electrons moving along geomagnetic line of force with those moving perpendicularly revealed anisotropy of the electron temperature. In the region of geomagnetic latitude above 20 degrees, electron temperature measured with the probe which surface is perpendicular to the geomagnetic line of force, T_⫽ is, in most cases, higher than that measured with the one parallel to geomagnetic field, T_⊥. Below 20 degree, T_⊥ was higher than T_⫽ with some exceptions. A celear local time dependence can be seen; in night time the events that T_⫽ was higher than T_⊥ were more frequently observed than those that T_⫽ was lower than T_⊥. No correlation between temperature anisotropy and Kp index was observed. The anisotropy of electron temperature will interpret some discripancies of electron temperature measured so far.
Books and Other Publications
2Presentations
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2026 URSI-Japan Radio Science Meeting, Mar 2, 2026
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2026 URSI-Japan Radio Science Meeting, Mar 2, 2026
Teaching Experience
1-
Jun, 2005 - Present惑星大気科学特論 (総合研究)
Professional Memberships
3Research Projects
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Grants-in-Aid for Scientific Research, Japan Society for the Promotion of Science, Apr, 2023 - Mar, 2026
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Grants-in-Aid for Scientific Research, Japan Society for the Promotion of Science, Apr, 2018 - Mar, 2021
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Grants-in-Aid for Scientific Research Grant-in-Aid for Scientific Research (B), Japan Society for the Promotion of Science, Apr, 2012 - Mar, 2015
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Grants-in-Aid for Scientific Research Grant-in-Aid for Scientific Research (B), Japan Society for the Promotion of Science, Apr, 2010 - Mar, 2014
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Grants-in-Aid for Scientific Research Grant-in-Aid for Scientific Research (B), Japan Society for the Promotion of Science, 2008 - 2010
● 指導学生等の数
2-
Fiscal Year2021年度(FY2021)Master’s program4Students under Commissioned Guidance Student System4Students under Skills Acquisition System1
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Fiscal Year2020年度(FY2020)Master’s program3Students under Commissioned Guidance Student System3Students under Skills Acquisition System2
● 専任大学名
1-
Affiliation (university)総合研究大学院大学(SOKENDAI)
● 所属する所内委員会
3-
ISAS Committee理学委員会
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ISAS Committee観測ロケット専門委員会
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ISAS Committeeスペースチェンバー専門委員会