• Title/Summary/Keyword: Optical spectrograph

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Current Status and Improvement of the Fast Imaging Solar Spectrograph of the 1.6m telescope at Big Bear Solar Observatory

  • Park, Hyungmin;Chae, Jongchul;Song, Donguk;Yang, Heesu;Jang, Bi-Ho;Park, Young-Deuk;Nah, Jakyoung;Cho, Kyung-Suk;Ahn, Kwangsu
    • The Bulletin of The Korean Astronomical Society
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    • v.37 no.2
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    • pp.112.2-112.2
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    • 2012
  • For the study of fine-scale structure and dynamics in the solar chromosphere, the Fast Imaging Solar Spectrograph (FISS) was installed in 1.6m New Solar Telescope at Big Bear Solar Observatory in 2010. The instrument, installed at a vertical table of the Coude lab, is properly working and producing data for science. From the analysis of the data, however, we noticed that a couple of problems exist that deteriorate image quality : lower light level and poorer resolution of the CaII band data. After several tests, we found that the relay optics at the right position is crucial role for the spatial resolution of raster-scan images. By using resolution target, we re-aligned relay optics and other components of the spectrograph. Here we present the result of optical test and new data taken by the FISS.

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TOLERANCE ANALYSIS OF FIMS OPTICAL SYSTEM (과학위성 1호 원자외선 분광기 광학부의 TOLERANCE 분석)

  • ;;;;;;;;Jerry Edelstein
    • Journal of Astronomy and Space Sciences
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    • v.17 no.1
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    • pp.67-76
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    • 2000
  • Far-ultraviolet IMaging Spectrograph(FIMS) is the main payload of the first Korean scientific satellite, KAISTSTA-4, which will be launched in 2002. The optical system of FIMS consists of parabolic cylinder mirror, slit, ellipsoidal reflection grating, and MCP to get spatial information as well as spectral information. Allowed ranges of manufacturing and positioning error are derived for each optical components to achieve the astronomical goals. In the procedure, graphical simplification is dedicated to understand sensitivity table and to derive range and precision of manipulation for each optical component. The result shows that precision of ${\mu}m$ for linear and of 2' for angular manipulation fulfills optical requirements.

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Preliminary Design of the G-CLEF Flexure Control Camera System

  • Oh, Jae Sok;Park, Chan;Park, Sung-Joon;Kim, Kang-Min;Chun, Moo-Young;Yu, Young Sam;Lee, Sungho;Szentgyorgyi, Andrew;Norton, Timothy;Podgorski, William;Evans, Ian;Mueller, Mark;McMuldroch, Stuart;Uomoto, Alan;Crane, Jeffrey;Hare, Tyson
    • The Bulletin of The Korean Astronomical Society
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    • v.40 no.2
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    • pp.56.1-56.1
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    • 2015
  • The GMT-Consortium Large Earth Finder (G-CLEF) is the very first light instrument of the Giant Magellan Telescope (GMT) and an optical-band echelle spectrograph. The Flexure Control Camera (FCC) is one of the major contributions of KASI's for the spectrograph project. FCC system includes the Fiber Mirror monitoring and the on- and off-slit mode auto-guidance algorithm. In this study, we present the modified design of the FCC optics and opto-mechanics after the G-CLEF Preliminary Design Review (PDR) held in Cambridge in April 2015.

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BAFFLE DESIGN OF FIMS (과학기술위성 1호 원자외선 분광기 FIMS의 배플 설계)

  • Yuk, I.S.;Seon, K.I.;Ryu, K.S.;Jin, H.;Park, J.H;Nam, U.W.;Lee, D.H.;Oh, S.H.;Rhee, J.G.;Han, W.Y.;Min, K.W.;Edelstein, Jerry;Korpela, Eric
    • Publications of The Korean Astronomical Society
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    • v.18 no.1
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    • pp.87-95
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    • 2003
  • FIMS (Far-ultraviolet IMaging Spectrograph) is the main payload of STSAT-1 satellite which was successfully launched on September 27, 2003. The optical system of FIMS consists of two sets of parabolic cylinder mirror, slit, ellipsoidal reflection grating, and baffle system. We designed two types of baffle system for the FIMS: FOV baffle and order baffle. FOV baffle in the mirror house controls the field of view, and the order baffle in the vacuum box blocks the rays reflected rays by different orders.

The Emission-line Properties of Young Radio Galaxies

  • Son, Dong-Hoon;Woo, Jong-Hak;Bennert, Vardha N.;Fu, Hai;Nagao, Tohru;Park, Dae-Seong
    • The Bulletin of The Korean Astronomical Society
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    • v.36 no.2
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    • pp.71.2-71.2
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    • 2011
  • To investigate the properties of the narrow-line regions and the accretion disks of YRGs, we study a sample of 28 young radio galaxies (YRGs) observed with the Kast Double Spectrograph at the Shane 3-m telescope and with the DBSP (Double Spectrograph for the Palomar 200-inch Telescope) at Palomar observatory. In addition we collect an addition sample of 15 YRGs with the optical spectra from the SDSS archive. We present the measured narrow-line region properties based on the various emission line ratios, i.e., [O III]/$H{\beta}$, [N II]/$H{\alpha}$, [S II] 6716/6731, [O I]/[O III], [O II]/[O III] and [Ar III]/[O III], which are useful to constrain the gas properties and the states of the accretion disk. We will discuss the characteristics of YRG.

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Design of IGRINS Wavelength Calibration System

  • Oh, Hee-Young;Pak, Soo-Jong;Yuk, In-Soo;Park, Chan;Lee, Sang-On;Chun, Moo-Young;Kim, Kang-Min;Lee, Sung-Ho;Pyo, Tae-Soo;Jaffe, Daniel T.
    • The Bulletin of The Korean Astronomical Society
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    • v.35 no.1
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    • pp.41.1-41.1
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    • 2010
  • IGRINS (the Immersion GRating Infrared Spectrograph) is a high resolution infrared spectrograph which is being developed by a collaboration of the University of Texas, the Korea Astronomy and Space Science Institute, and Kyung Hee University. The wavelength calibration unit of IGRINS will be situated between the telescope flange and IGRINS dewar. It will include Th-Ar hallow cathode lamp, optical elements, and gas absorption cell for the case that requires precise calibration (e.g., radial velocity observation). The system will also use a tungsten halogen lamp in an integrating sphere as a blackbody source for the flat-field imaging. IGRINS will be placed initially on the McDonald 2.7m Harlan J. Smith telescope and later on 4-8m class telescopes. We present an overview of the plan for the wavelength calibration sources and of the development process for the optical and mechanical design of the IGRINS calibration system.

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2-dimensional Mapping of Sulfur Dioxide and Bromine Oxide at the Sakurajima Volcano with a Ground Based Scanning Imaging Spectrograph System

  • Lee, Han-Lim;Kim, J.-Hoon;Ryu, Jae-Yong;Kwon, Soon-Chul;Noh, Young-Min;Gu, Myo-Jeong
    • Journal of the Optical Society of Korea
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    • v.14 no.3
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    • pp.204-208
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    • 2010
  • A scanning imaging spectrograph system was used in this study to retrieve readings of the 2-D distribution of $SO_2$ and BrO around the crater of the Sakurajima volcano in Japan. The measurement was carried out during the daytime on November 2, 2005. Measurements were made at the surface of the site, located 5 km from the Sakurajima crater. One hundred horizontal scans were performed. Each column scanned by the system consists of 64 vertical pixels in order to retrieve the spatial distributions of BrO and $SO_2$ in the plume in terms of slant column densities (SCDs). Measured spectra were analyzed to identify and quantify $SO_2$ and BrO in the volcanic plume utilizing the plume's specific absorption features in the ultra violet region. Two-dimensional BrO and $SO_2$ distributions in SCD were retrieved horizontally covering the upwind, crater and downwind areas, and vertically, including the plume in the center of the scanned image. Both horizontal and vertical dispersions of $SO_2$ SCD from the crater were successfully measured to be from $10^{17}$ to $4.5{\times}10^{18}$ molecules $cm^{-2}$. However, BrO was measured below $10^{15}$ molecules $cm^{-2}$, which is considered its background level.

Spectroscopic Studies of Wolf-Rayet galaxies

  • Kim, Myunghak;Shim, Hyunjin
    • The Bulletin of The Korean Astronomical Society
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    • v.40 no.1
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    • pp.72.2-72.2
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    • 2015
  • Wolf-Rayet galaxies, galaxies which show spectral features produced by Wolf-Rayet stars, are thought to be the place of recent massive star formation since the Wolf-Rayet phase covers relatively short timescale in the life of massive O and B type stars. Studying these galaxies provides a unique chance to understand how massive star formation occurs in a galaxy within a short timescale. In this work, we present the intermediate resolution optical spectra of 12 Wolf-Rayet galaxies obtained using longslit spectrograph on Bohyunsan Optical Astronomy Observatory. We derived the emission line ratios for a number of star-forming knots in each Wolf-Rayet galaxy. Star formation properties in these galaxies are discussed.

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SPECTROSCOPIC STUDY OF ACTIVE PROMINENCE (활동홍염의 분광분석 연구)

  • PARK YOUNG DEUK;YUN HONG SIK;MOON YONG-JAE
    • Publications of The Korean Astronomical Society
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    • v.13 no.1 s.14
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    • pp.1-16
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    • 1998
  • A quantitative analysis has been made to estimate the horizontal variation of physical parameters in a loop type active prominence by analyzing Call H&K and $H_{\varepsilon}{\ldots}$ spectra taken from such an active prominence (appeared on May 23, 1981 with position angle 251 degree) with Littrow type spectrograph attached to 25cm coronagraph at Norikura Coronal Station of National Astronomical Observatory of Japan. The spectral resolution is 1.12A/mm and the spatial resolution is 25'/mm for Call H&K lines. The present study shows that the turbulent velocity ranges from 10km/s to 20 km/s in the loop prominence, which are in good agreement with those of Hirayama (1989). It is also found that the temperature of the loop prominence is higher than that of quiescent prominences$(\~8,000 K)$ by about 4,000 K, whose temperature deviation seems very high.

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STUDY OF DOPPLER VELOCITY DISTRIBUTION IN AN ACTIVE PROMINENCE (CCD 분광 관측에 의한 활동홍염의 도플러 시선속도분포 연구)

  • PARK YOUNG DEUK;YUN HONG SIK;MOON YONG-JAE
    • Publications of The Korean Astronomical Society
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    • v.13 no.1 s.14
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    • pp.17-30
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    • 1998
  • To study kinematics of solar prominences, we have made Ha spectrographic study of an eruptive prominence which appeared on the 27th of August, 1992 with a position angle of 270 deg. The observation was carried out by a Littrow type spectrograph and a G1 CCD camera attached to the 25cm coronagraph at Norikura Coronal Station. In taking the spectral data the slit was placed in parallel to the solar limb at 7 different heights, each being separated by 5 arcsec with a time step of 30 sec. The observed eruptive prominence shows a wide range of line of sight Doppler velocity, spanning from $V_{dopp}=-17.5km/s\;to\;V_{dopp}=58.2km/s$. It is also found that the velocity increases with height at the rate of ${\Delta}V= 0.86 km/s/arcsec$.

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