• Title/Summary/Keyword: Korean Fims

Search Result 145, Processing Time 0.023 seconds

Global features of the Cygnus Loop observed with FIMS

  • Seon Kwang-Il;Park Jang-Hyun;Lee Dae-Hee;Jin Ho;Yuk In-Soo;Han Wonyong;Nam Uk-Won;Kim Il-Joong;Shinn Jong-Ho;Ryu Kwang-Sun;Min Kyung W.;Edelstein Jerry;Korpela Erick
    • The Bulletin of The Korean Astronomical Society
    • /
    • v.30 no.1
    • /
    • pp.32.1-32.1
    • /
    • 2005
  • PDF

The structural Properties of the Pb$(Zr{_{0.7}}Ti_{0.3})O_3$ Ceramics Thin Films by RF Sputtering method (RF Sputtering method를 이용한 Pb$(Zr{_{0.7}}Ti_{0.3})O_3$ 세라믹스 박막의 구조적 특성)

  • Nam, Sung-Pill;Lee, Sang-Chul;Lim, Sung-Su;Lee, Sung-Gap;Lee, Young-Hie
    • Proceedings of the KIEE Conference
    • /
    • 2003.07c
    • /
    • pp.1586-1588
    • /
    • 2003
  • The Pb$(Zr{_{0.7}}Ti_{0.3})O_3$[PZT(70/30)] thin films were fabricated on Pt/$TiO_2/SiO_2$/Si substrate by RF sputtering method. The effects of Ar/$O_2$ ratio on the structural and dielectric properties of PZT thin fillms were investigated. In the case of the PZT thin films deposited with condition of 50/50$(Ar/O_2) $ ratio, the grain of the PZT thin films were fine and uniform. Increasing of $O_2$ ratio, the dielectric constant was increased. In this case the dielectirc constant and dielectric loss of PZT thin fims were about 627 and 0.010, respectively.

  • PDF

PRELIMINARY FEASIBILITY STUDY OF THE SOLAR OBSERVATION PAYLOADS FOR STSAT-CLASS SATELLITES

  • Moon, Yong-Jae;Cho, Kyung-Seok;Jin, Ho;Chae, Jong-Chul;Lee, Sung-Ho;Seon, Kwang-Il;Kim, Yeon-Han;Park, Young-Deuk
    • Journal of Astronomy and Space Sciences
    • /
    • v.21 no.4
    • /
    • pp.329-342
    • /
    • 2004
  • In this paper, we present preliminary feasibility studies on three types of solar observation payloads for future Korean Science and Technology Satellite (STSAT) programs. The three candidates are (1) an UV imaging telescope, (2) an UV spectrograph, and (3) an X-ray spectrometer. In the case of UV imaging telescope, the most important constraint seems to be the control stability of a satellite in order to obtain a reasonably good spatial resolution. Considering that the current pointing stability estimated from the data of the Far ultraviolet Imaging Spectrograph (FIMS) onboard the Korean STSAT-1, is around 1 arc minutes/sec, we think that it is hard to obtain a spatial resolution sufficient for scientific research by such an UV Imaging Telescope. For solar imaging missions, we realize that an image stabilization system, which is composed of a small guide telescope with limb sensor and a servo controller of secondary mirror, is quite essential for a very good pointing stability of about 0.1 arcsec. An UV spectrograph covering the solar full disk seems to be a good choice in that there is no risk due to poor pointing stability as well as that it can provide us with valuable UV spectral irradiance data valuable for studying their effects on the Earth's atmosphere and satellites. The heritage of the FIMS can be a great advantage of developing the UV spectrograph. Its main disadvantage is that two major missions are in operation or scheduled. Our preliminary investigations show that an X-ray spectrometer for the full disk Sun seems to be the best choice among the three candidates. The reasons are : (1) high temporal and spectral X-ray data are very essential for studying the acceleration process of energetic particles associated with solar flares, (2) we have a good heritage of X-ray detectors including a rocket-borne X-ray detector, (3) in the case of developing countries such as India and Czech, solar X-ray spectrometers were selected as their early stage satellite missions due to their poor pointing stabilities, and (4) there is no planned major mission after currently operating Reuven Ramaty High-Energy Solar Spectroscopic Imager (RHESSI) mission. Finally, we present a preliminary design of a solar X-ray spectrometer covering soft X-ray (2 keV) to gamma ray (10 MeV).

The Far-ultraviolet Spectrum Study of Comet C/2001 Q4 (NEAT)

  • Lim, Yeo-Myeong;Min, Kyoung-Wook;Feldman, Paul D.;Han, Wanyong;Edelstein, Jerry
    • The Bulletin of The Korean Astronomical Society
    • /
    • v.39 no.1
    • /
    • pp.68.1-68.1
    • /
    • 2014
  • We present the results of far-ultraviolet (FUV) observations of comet C/2001 Q4 (NEAT) obtained with Far-ultraviolet Imaging Spectrograph (FIMS) on board the Korean microsatellite STSAT-1, which operated at an altitude of 700 km in a sun-synchronous orbit. FIMS is a dual channel imaging spectrograph (S-channel 900-1150 ${\AA}$, L-channel 1350-1710 ${\AA}$, and ${\lambda}/{\Delta}{\lambda}$ ~ 550 for both channels) with large image fields of view (S-channel $4.0^{\circ}{\times}4.6^{\prime}$, L-channel $7.5^{\circ}{\times}4.3^{\prime}$, and angular resolution ~ $5-10^{\prime}$) optimized for the observation of diffuse emission of astrophysical radiation. Comet C/2001 Q4 (NEAT) were made in two campaigns during its perihelion approach between May 8 and 15, 2004. Based on the scanning mode observations in the wavelength band of 1400-1700 ${\AA}$, we have constructed an image of the comet with an angular size of $5^{\circ}{\times}5^{\circ}$, which corresponds to the central coma region. Several important fluorescence emission lines were detected including S I multiplets at 1429 and 1479 ${\AA}$, C I multiplets at 1561 and 1657 ${\AA}$, and the CO $A^1{\Pi}-X^1{\Sigma}^+$ Fourth Positive system; we have estimated the production rates of the corresponding species from the fluxes of these emission lines. The estimated production rate of CO was $Q_{CO}=(2.65{\pm}0.63){\times}10^{28}s^{-1}$, which is 6.2-7.4% of the water production rate and is consistent with earlier predictions. The average carbon production rate was estimated to be $Q_C={\sim}1.59{\times}10^{28}s^{-1}$, which is ~60% of the CO production rate. However, the observed carbon profile was steeper than that predicted using the two-component Haser model in the inner coma region, while it was consistent with the model in the outer region. The average sulfur production rate was $Q_S=(4.03{\pm}1.03){\times}10^{27}s^{-1}$, which corresponds to ~1% of the water production rate.

  • PDF

A Study on Chinese Characters Represented in Korean Films from under Japanese Colonial Period to the 2000s (한국 영화에 재현된 중국인 형상의 역사적 고찰)

  • Kim, Jongsoo
    • Cross-Cultural Studies
    • /
    • v.27
    • /
    • pp.105-122
    • /
    • 2012
  • This article aims that Chinese characters represented in Korean films have been explored for historical consideration of Korean's viewpoint on Chinese from early modern to the present day. During Japanese colonial period, Chinese had been hateful and feared by most of Korean because Korean had been acted high-handedly by chinese in early modern time and had covertly regarded chinese as threatening competitors in economical part of the colony, refered to the chinese characters represented in the films, For the Lover(1928) and Secret of Chinese Street(1928). Chinese had been called as enemy forces in Korean movies, such as Marines are Gone(1963), Dragon competed with tiger(1974) made with Korean battle field setting and Manchuria setting developed a Korean independence movement, after Korean War in the 1960-70s maintained the cold war system in the World. According to analyzing chinese characters depicted in Failan(2001), A Good Rain Knows(2010), Korean public have a friendly attitude with contemporary Chinese as China has been the great trade partner of Korea with interdependent relationship after 1992, the year of Korea have established diplomatic ties with China.

A study on the formation of ITO by reactive DC cylindrical sputtering (DC 원통형 반응성 스파트링을 이용한 ITO 형성에 관한 연구)

  • 조정수;박정후;하홍주;곽병구;이우근
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
    • /
    • 1995.05a
    • /
    • pp.35-38
    • /
    • 1995
  • Indium Tin Oxide(ITO) thin film is transparent to visible ray and conductive in electricity. It is seen that the samples made by the sputtering process have high transmission rate to visible ray and high adhesion , but the planar type magnetron sputtering process with is very well known in industrial region have a defect of partial erosion on the surface of target and a high loss of target and also since the substrate is positioned in plasma, the damage on thin film surface is caused by the reaction with plasma. In cylindrical magnetron sputtering system. it is known that the loss of target is little , the damage of thin film is very little and the adhesion of thin film with substrate is strong. In this study, we have made ITO thin film in the cylindrical DC magnetron system with the variable of substrate temperature , magnetic field, vacuum condution and the applied voltage. The general temperature for formation on ITO is asked at 350 $^{\circ}C$~400$^{\circ}C$ but we have made ITO is low temperature(80-150$^{\circ}C$) By studing electrical and optical properties of ITO thin fims made by varing several condition, we have searched the optimal condition for formation in the best ITO in low temperature.

  • PDF

Magnetic and Electrical Properties of Mn-Zn Ferrite Thin Films Deposited by Ion Beam Sputtering (이온빔 스퍼터링에 의해 증착된 Mn-Zn 페라이트 박막의 자기 및 전기적 특성)

  • 조해석;하상기;이대형;주한용;김형준;김경용;제해준;유병두
    • Journal of the Korean Ceramic Society
    • /
    • v.32 no.3
    • /
    • pp.313-320
    • /
    • 1995
  • We investigated the preferred orientation, electrical and magnetic properties of the Mn-Zn ferrite thin films deposited on SiO2/Si(100) by ion beam sputtering. The Cu-added Mn-Zn ferrite thin films had a preferred orientation of (111) with a weak orientation, (311). While the Zn-added one had a strong (111) preferred orientation. The saturation magnetization of the Cu- or Zn-doped Mn-Zn ferrite films increased with increasing substrate temperature (Ts) due to the increase of grain size and the enhancement of crystallinity. For the same reason the coercivity of Cu- or Zn-doped Mn-Zn ferrite films deposited at low Ts increased with increasing Ts, but those of the films deposited at high Ts slightly decreased not only because the defect density of the films decreases but because more grains have multi-domains with increasing Ts. The resistivity of Cu- or Zn-added Mn-Zn ferrite thin fims measured by complex impedance method decreased with increasing Ts due to the ehhancement of crystallinity as well as due to the increase of grain size.

  • PDF

Effect of Deposition Temperature on the Electrical Performance of SiZnSnO Thin Film Transistors Fabricated by RF Magnetron Sputtering (스퍼터 공정을 이용한 SiZnSnO 산화물 반도체 박막 트랜지스터의 증착 온도에 따른 특성)

  • Ko, Kyung Min;Lee, Sang Yeol
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
    • /
    • v.27 no.5
    • /
    • pp.282-285
    • /
    • 2014
  • We have investigated the structural and electrical properties of Si-Zn-Sn-O (SZTO) thin films deposited by RF magnetron sputtering at various deposition temperatures from RT to $350^{\circ}C$. All the SZTO thin fims are amorphous structure. The mobility of SZTO thin film has been changed depending on the deposition temperature. SZTO thin film transistor shows mobility of 8.715 $cm^2/Vs$ at room temperature. We performed the electrical stress test by applying gate and drain voltage. SZTO thin film transistor shows good stability deposited at room temperature while showing poor stability deposited at $350^{\circ}C$. As a result, the electrical performance and stability have been changed depending on deposition temperature mainly because high deposition temperature loosened the amorphous structure generating more oxygen vacancies.

Structural and optical properties of $TiO_2$ thin film fabricated by reactive sputtering (반응성 스퍼터링법에 의한 $TiO_2$ 박막의 구조적 및 광학적 특성)

  • Yang, Hyeon-Hun;Jeong, Woon-Jo;Park, Gye-Choon
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
    • /
    • 2008.04c
    • /
    • pp.58-61
    • /
    • 2008
  • $TiO_2$ is a wide band-gap semiconductor (3.4 eV) and can only absorb about 5% of sun light in the ultraviolet light region, which largely limits its practical applications because of the lower utility of sun light and quantum yield. In order to move the absorption edge of $TiO_2$ fims to visible spectrum range, we have made the impurity level within a band-gap of $TiO_2$ thin film by introduction of oxygen vacancy. Oxygen-defected $TiO_2$ thin film have prepared by reactive sputtering with the partial pressure of $Ar:O_2=10:90{\sim}99.33:0.66$ ratio. As a result, we could have the impurity level of about 2.75 eV on condition that oxygen partial pressure is below 7%.

  • PDF