• Title/Summary/Keyword: radio lines:atomic

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Radio-sensitivity Analysis and Selection of Useful Mutants of Rape (Brassica napus L.) by Gamma Irradiation (방사선 처리에 의한 유채의 생육 및 감수성 조사)

  • Goh, Eun Jeong;Kim, Wook-Jin;Kim, Jin-Baek;Kim, Dong Sub;Kim, Sang Hoon;Kang, Si-Yong
    • Journal of Radiation Industry
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    • v.4 no.3
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    • pp.277-283
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    • 2010
  • Rape (Brassica napus L.) plants are one of the major oilseed crops. The main components of rapeseed are oil (35 to 47%) and protein (15 to 32%). For the biodiesel production, the development of a new variety of rape plant with high biomass and/or oleic acid contents is required. In order to determine the optimum dose of gamma-ray irradiation, the rape seeds of cvs. Hanra (Hr), Youngsan (Ys), Tammi (Tm), and Tamra (Tr) were irradiated with a 100~4,000 Gy dose range of gamma-rays. Considering the growth factors, the optimum doses were determined to be within the range of 600~1,000 Gy for the selection of useful mutant lines. Six-hundred and eighty-eight (688) $M_2$ mutant lines were obtained from 600~1,000 Gy gamma-ray-irradiated $M_1$ plants through selfing. The growth characteristics, leaf shape, early flowering, and flower color were all investigated. The selected mutant numbers of early flowering, leaf shape, and flower color were 34, 52, and 3 from the four cultivars, respectively. These mutant lines will be used for the development of a new variety of rape plant with high biomass and oleic acid contents.

ATOMIC CARBON IN THE W 3 GIANT MOLECULAR CLOUD

  • SAKAI TAKESHI;OKA TOMOHARU;YAMAMOTO SATOSHI
    • Journal of The Korean Astronomical Society
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    • v.38 no.2
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    • pp.257-260
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    • 2005
  • We have mapped the W 3 giant molecular cloud in the $C^o\;^3P_1-^3 P_o$ ([CI]) line with the Mount Fuji Submillimeter-wave Telescope. The [CI] emission is extended over the molecular cloud, having peaks at three star forming clouds; W 3(Main), W 3(OH), and AFGL 333. The [CI] emission is found to be strong in the AFGL 333 cloud. We have also observed the $C^{18}O,\;CCS,\;N_2H^+$, and $H^{13}CO^+$ lines by using the Nobeyama Radio Observatory 45 m telescope. In the AFGL 333 cloud, we find two massive cores, which are highly gravitationally bound and have no sign of active star formation. The high [$C^o$]/[CO] and [CCS]/[$N_2H^+$] abundance ratios suggest that the AFGL 333 cloud is younger than the W 3(Main) and W 3(OH) clouds.

HCO+ Observations toward Compact Radio Continuum Sources Using the KVN 21-m Telescopes to Trace Dark Molecular Gas

  • Park, Geumsook;Koo, Bon-Chul;Kim, Kee-Tae;Byun, Do-Young;Heiles, Carl
    • The Bulletin of The Korean Astronomical Society
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    • v.40 no.2
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    • pp.52.3-53
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    • 2015
  • It has been known that there is "dark gas" invisible either in 21-cm HI or 2.6-mm CO emission which are general tracers of atomic and molecular gas, respectively. Many researchers consider that the dark gas is "Dark Molecular Gas (DMG)" composed of CO-free $H_2$ in the intermediate zone between atomic and full-fledged molecular gas and that HCO+ and OH molecules are good tracers of the DMG since they can form in much lower $H_2$ column densities where CO does not. We have carried out HCO+ J=1-0 absorption observations toward nine bright extragalactic radio continuum sources using the KVN 21-m telescopes as single dishes. We detected HCO+ absorption lines toward two sources. We derive HCO+ and $H_2$ column densities or their limits, and discuss the implications of our results.

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THE HI MOSAIC OF THE LARGE MAGELLANIC CLOUD

  • KIM SUNGEUN
    • Journal of The Korean Astronomical Society
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    • v.29 no.spc1
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    • pp.95-95
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    • 1996
  • We present the recent results of an HI aperture synthesis mosaic of the Large Magellanic Cloud(LMC), made by combining data from 1344 separate pointing centers using the Australia Telescope Compact Array(ATCA). The resolution of the mosaiced images is 1'.0 (15 pc, using a distance to the LMC of 50 kpc). In contrast with its appearance at other wavelengths, the LMC is remarkably symmetric in HI on the largest scales, with the bulk of the HI residing in a disk of diameter 7.3 kpc. Outer spiral structure is clearly seen, though the features appear due to differential rotation, therefore transient in nature. A good correlation is seen between the supershells previously identified in Halpha (e.g. Meaburn 1980) and HI structures.

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HI 21 CM EMISSION LINE STUDY OF SOUTHERN GALACTIC SUPERNOVA REMNANTS

  • KOO BON-CHUL;KANG JI-HYUN;MCCLURE-GRIFFITHS N. M.
    • Journal of The Korean Astronomical Society
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    • v.37 no.2
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    • pp.61-77
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    • 2004
  • We have searched for HI 21 cm line emission from shocked atomic gas associated with southern supernova remnants (SNRs) using data from the Southern Galactic Plane Survey. Among the 97 sources studied, we have detected 10 SNRs with high-velocity HI emission confined to the SNR. The large velocity and the spatial confinement suggest that the emission is likely from the gas accelerated by the SN blast wave. We also detected 22 SNRs which show HI emission significantly brighter than the surrounding regions over a wide ($>10 km\;s^{-1}$) velocity interval. The association with these SNRs is less certain. We present the parameters and maps of the excess emission in these SNRs. We discuss in some detail the ten individual SNRs with associated high-velocity HI emission.

Optical Emission Spectra of Oxygen Plasma Produced by Radio-Frequency Plasma (RF 플라즈마에 의해 생성된 산소 플라즈마의 발광 스펙트럼)

  • Kim, Do-Yeob;Kim, Min-Su;Kim, Tae-Hoon;Kim, Ghun-Sik;Choi, Hyun-Young;Cho, Min-Young;Jeon, Su-Min;Park, Sung-Dong;Kim, Jin-Ha;Kim, Eun-Do;Hwang, Do-Weon;Lee, Jae-Young
    • Journal of the Korean Vacuum Society
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    • v.18 no.2
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    • pp.102-107
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    • 2009
  • We investigated optical emission of oxygen plasma discharged by 13.56 MHz radio frequency (rf) by using optical emission spectroscopy (OES). Experimental measurement is done at a range of oxygen flow rate of 1$\sim$20 seem, rf power of 25$\sim$250 W, and orifice 3 and 5 mm in diameter. When oxygen plasma was generated, typical emission spectra for oxygen plasma were observed regardless of diameter of orifice. Strong atomic emission lines are observe at 776.8 an 843.9 nm, corresponding to the $3p^{5}P-3s^{5}S^{0}$ and $3p^{3}P-3s^{3}S^{0}$ transitions, respectively. The emission intensity of line at 776.8 and 843.9 nm increased with increasing the oxygen flow rate and rf power. The increasing rate of emission intensity of 776.8 nm line was larger than that of 843.9 nm line. When the diameter of orifice was 3 mm, the oxygen plasma was more stably generated than orifice 5 mm in diameter.