• 제목/요약/키워드: telescope

검색결과 1,548건 처리시간 0.026초

Faint Quasar Candidates at z~5 in the ELAIS-N1 field

  • Shin, Suhyun;Im, Myungshin;Kim, Yongjung;Hyun, Minhee;Jeon, Yiseul;Kim, Minjin;Kim, Dohyeong;Kim, Jae-Woo;Taak, Yoon Chan;Yoon, Yongmin;Choi, Changsu;Hong, Jueun;Jun, Hyunsung David;Karouzos, Marios;Kim, Duho;Kim, Ji Hoon;Lee, Seong-Kook;Pak, Soojong;Park, Won-Kee
    • 천문학회보
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    • 제42권2호
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    • pp.74.2-74.2
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    • 2017
  • Faint quasars are important to test the possibility that quasars are the main contributor to the cosmic reionization. However, it has been difficult to find faint quasars due to the lack of deep, wide-field imaging data. In this poster, we present our efforts to find faint quasars in the ELAIS-N1 field through the deep data (iAB ~ 25) obtained by the Subaru Hyper Suprime-Cam (HSC) Strategic Program survey. To select reliable quasar candidate, we also use the near-infrared (NIR) data of the Infrared Medium-deep Survey (IMS) and the UKIRT Infrared Deep Sky Survey (UKIDSS) - Deep Extragalactic Survey (DXS). Using multiple-band color cuts, we select high redshift quasar candidates. To confirm them as high redshift quasars, candidates are observed by the SED camera for QUasars in EArly uNiverse (SQUEAN) instrument in several medium band filters that can sample the redshifted Lyman break efficiency. The quasar sample will be used to study the growth of BH and stellar mass, the relation between the quasar activity and the host galaxy, and their contribution to the cosmic re-ionization.

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Filament, the Universal Nersery of Stars: Progress Report on TRAO Survery of Nearby Filamentary Filamentary Molecular Clouds

  • Kim, ShinYoung;Chung, Eun Jung;Lee, Chang Won;Myers, Philip C.;Caselli, Paola;Tafalla, Mario;Kim, Gwanjeong;Kim, Miryang;Soam, Archana;Gophinathan, Maheswar;Liu, Tie;Kim, Kyounghee;Kwon, Woojin;Kim, Jongsoo
    • 천문학회보
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    • 제42권2호
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    • pp.79.2-79.2
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    • 2017
  • To dynamically and chemically understand how filaments, dense cores, and stars form under different environments, we are conducting a systematic mapping survey of nearby molecular clouds using the TRAO 14 m telescope with high ($N_2H^+$ 1-0, $HCO^+$ 1-0, SO 32-21, and $NH_2D$ v=1-0) and low ($^{13}CO$ 1-0, $C^{18}O$ 1-0) density tracers. The goals of this survey are to obtain the velocity distribution of low dense filaments and their dense cores for the study of their origin of the formation, to understand whether the dense cores form from any radial accretion or inward motions toward dense cores from their surrounding filaments, and to study the chemical differentiation of the filaments and the dense cores. Until the 2017A season, the real OTF observation time is ~760 hours. We have almost completed mapping observation with four molecular lines ($^{13}CO$ 1-0, $C^{18}O$ 1-0, $N_2H^+$ 1-0, and $HCO^+$ 1-0) on the six regions of molecular clouds (L1251 of Cepheus, Perseus West, Polaris South, BISTRO region of Serpens, California, and Orion B). The cube data for $^3CO$ and $C^{18}O$ lines were obtained for a total of 6 targets, 57 tiles, 676 maps, and $7.1deg^2$. And $N_2H^+$ and $HCO^+$ data were added for $2.2deg^2$ of dense regions. All OTF data were regridded to a cell size of 44 by 44 arcseconds. The $^{13}CO$ and $C^{18}O$ data show the RMS noise level of about (0.1-0.2) K and $N_2H^+$ and $HCO^+$ data show about (0.07-0.2) K at the velocity resolution of 0.06 km/s. Additional observations will be made on some regions that have not reached the noise level for analysis. To identify filaments, we are using and testing programs (DisPerSE, Dendrogram, FIVE) and visual inspection for 3D image of cube data. A basic analysis of the physical and chemical properties of each filament is underway.

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STSAT-3 Main Payload, MIRIS Flight Model Developments

  • 한원용;이대희;박영식;정웅섭;이창희;문봉근;박성준;차상목;남욱원;박장현;이덕행;가능현;선광일;양순철;박종오;이승우;이형목
    • 천문학회보
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    • 제35권1호
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    • pp.40.1-40.1
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    • 2010
  • The Main payload of the STSAT-3 (Korea Science & Technology Satellite-3), MIRIS (Multipurpose Infra-Red Imaging System) has been developed for last 3 years by KASI, and its Flight Model (FM) is now being developed as the final stage. All optical lenses and the opto-mechanical components of the FM have been completely fabricated with slight modifications that have been made to some components based on the Engineering Qualification Model (EQM) performances. The components of the telescope have been assembled and the test results show its optical performances are acceptable for required specifications in visual wavelength (@633 nm) at room temperature. The ensuing focal plane integration and focus test will be made soon using the vacuum chamber. The MIRIS mechanical structure of the EQM has been modified to develop FM according to the performance and environment test results. The filter-wheel module in the cryostat was newly designed with Finite Element Analysis (FEM) in order to compensate for the vibration stress in the launching conditions. Surface finishing of all components were also modified to implement the thermal model for the passive cooling technique. The FM electronics design has been completed for final fabrication process. Some minor modifications of the electronics boards were made based on EQM test performances. The ground calibration tests of MIRIS FM will be made with the science grade Teledyne PICNIC IR-array.

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IRAS 15099-5856: Remarkable Mid-Infrared Source with Prominent Crystalline Silicate Emission

  • 구본철;;서경원;문대식;;;;;김현정;정웅섭;;임명신;이호규;이재준
    • 천문학회보
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    • 제35권1호
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    • pp.57-57
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    • 2010
  • We report the discovery of a bright mid-infrared (MIR) source with prominent crystalline silicate emission using the space telescope AKARI and Spitzer. This source, IRAS 15099-5856, has a spectacular morphology with a bright central compact source (CCS) surrounded by knots, spurs, and several extended (~4') arc-like filaments. The source is seen only in infrared at ${\geq}10{\mu}m$. The Spitzer MIR spectrum of the CCS shows prominent emission features from Mg-rich crystalline silicates and strong [Ne II] 12.88 ${\mu}m$ and several other faint ionic lines. We model the MIR spectrum as thermal emission from several independent dust components and compare their properties to those of the Herbig Be star HD 100546 which shows very similar MIR spectrum. Our molecular line observations reveal two molecular clouds around the source, but no associated dense molecular cores. We discuss two possible origins for IRAS 15099-5856; a deeply embedded massive young stellar object on the other side of the Galaxy and a disrupted, protoplanetary disk being photoevaporated by the UV radiation from the nearby O star Muzzio 10.

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TRAO Multi-beam Legacy Survey of Nearby Filamentary Molecular Clouds : Progress Report

  • Kim, ShinYoung;Chung, Eun Jung;Lee, Chang Won;Myers, Philip C.;Caselli, Paola;Tafalla, Mario;Kim, Gwanjeong;Kim, Miryang;Soam, Archana;Gophinathan, Maheswar;Liu, Tie;Kim, Kyounghee;Kwon, Woojin;Kim, Jongsoo
    • 천문학회보
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    • 제42권1호
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    • pp.32.1-32.1
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    • 2017
  • To dynamically and chemically understand how filaments, dense cores, and stars form under different environments, we are conducting a systematic mapping survey of nearby molecular clouds using the TRAO 14 m telescope with high ($N_2H^+$ 1-0, $HCO^+$ 1-0, SO 32-21, and $NH_2D$ v=1-0) and low ($^{13}CO$ 1-0, $C^{18}O$ 1-0) density tracers. The goals of this survey are to obtain the velocity distribution of low dense filaments and their dense cores for the study of their origin of the formation, to understand whether the dense cores form from any radial accretion or inward motions toward dense cores from their surrounding filaments, and to study the chemical differentiation of the filaments and the dense cores. Until Feb. 2017, the real OTF observation time is 460 hours. We have almost completed mapping observation with four molecular lines ($^{13}CO$ 1-0, $C^{18}O$ 1-0, $N_2H^+$ 1-0, and $HCO^+$ 1-0) on the five regions of molecular clouds (L1251 of Cepheus, Perseus west, Polaris south, BISTRO region of Serpense, California, and Orion B). The maps of a total area of $7.38deg^2$ for both $^{13}CO$ and $C^{18}O$ lines and $2.19deg^2$ for both $N_2H^+$ and $HCO^+$ lines were obtained. All OTF data were regridded to a cell size of 22 by 22 arcseconds. The $^{13}CO$ and $C^{18}O$ data show the RMS noise level of about 0.22 K and $N_2H^+$ and $HCO^+$ data show about 0.14 K at the velocity resolution of 0.06 km/s. Additional observations will be made on some regions that have not reached the noise level for analysis. We are refining the process for a massive amount of data and the data reduction and analysis are underway. This presentation introduces the overall progress from observations to data processing and the initial analysis results to date.

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SEARCH FOR EXOPLANETS AROUND NORTHERN CIRCUMPOLAR STARS III. LONG-PERIOD RADIAL VELOCITY VARIATIONS IN HD 18438 AND HD 158996

  • Bang, Tae-Yang;Lee, Byeong-Cheol;Jeong, Gwang-Hui;Han, Inwoo;Park, Myeong-Gu
    • 천문학회지
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    • 제51권1호
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    • pp.17-25
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    • 2018
  • Detecting exoplanets around giant stars sheds light on the later-stage evolution of planetary systems. We observed the M giant HD 18438 and the K giant HD 158996 as part of a Search for Exoplanets around Northern circumpolar Stars (SENS) and obtained 38 and 24 spectra from 2010 to 2017 using the high-resolution Bohyunsan Observatory Echelle Spectrograph (BOES) at the 1.8m telescope of Bohyunsan Optical Astronomy Observatory in Korea. We obtained precise RV measurements from the spectra and found long-period radial velocity (RV) variations with period 719.0 days for HD 18438 and 820.2 days for HD 158996. We checked the chromospheric activities using Ca $\text\tiny{II}$ H and $H{\alpha}$ lines, HIPPARCOS photometry and line bisectors to identify the origin of the observed RV variations. In the case of HD 18438, we conclude that the observed RV variations with period 719.0 days are likely to be caused by the pulsations because the periods of HIPPARCOS photometric and $H{\alpha}$ EW variations for HD 18438 are similar to that of RV variations in Lomb-Scargle periodogram, and there are no correlations between bisectors and RV measurements. In the case of HD 158996, on the other hand, we did not find any similarity in the respective periodograms nor any correlation between RV variations and line bisector variations. In addition, the probability that the real rotational period can be as longer than the RV period for HD 158996 is only about 4.3%. Thus we conclude that observed RV variations with a period of 820.2 days of HD 158996 are caused by a planetary companion, which has the minimum mass of 14.0 $M_{Jup}$, the semi-major axis of 2.1 AU, and eccentricity of 0.13 assuming the stellar mass of $1.8 M_{\odot}$. HD 158996 is so far one of the brightest and largest stars to harbor an exoplanet candidate.

Current status and future plans of KMTNet microlensing experiments

  • Chung, Sun-Ju;Gould, Andrew;Jung, Youn Kil;Hwang, Kyu-Ha;Ryu, Yoon-Hyun;Shin, In-Gu;Yee, Jennifer C.;Zhu, Wei;Han, Cheongho;Cha, Sang-Mok;Kim, Dong-Jin;Kim, Hyun-Woo;Kim, Seung-Lee;Lee, Chung-Uk;Lee, Yongseok
    • 천문학회보
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    • 제43권1호
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    • pp.41.1-41.1
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    • 2018
  • We introduce a current status and future plans of Korea Microlensing Telescope Network (KMTNet) microlensing experiments, which include an observational strategy, pipeline, event-finder, and collaborations with Spitzer. The KMTNet experiments were initiated in 2015. From 2016, KMTNet observes 27 fields including 6 main fields and 21 subfields. In 2017, we have finished the DIA photometry for all 2016 and 2017 data. Thus, it is possible to do a real-time DIA photometry from 2018. The DIA photometric data is used for finding events from the KMTNet event-finder. The KMTNet event-finder has been improved relative to the previous version, which already found 857 events in 4 main fields of 2015. We have applied the improved version to all 2016 data. As a result, we find that 2597 events are found, and out of them, 265 are found in KMTNet-K2C9 overlapping fields. For increasing the detection efficiency of event-finder, we are working on filtering false events out by machine-learning method. In 2018, we plan to measure event detection efficiency of KMTNet by injecting fake events into the pipeline near the image level. Thanks to high-cadence observations, KMTNet found fruitful interesting events including exoplanets and brown dwarfs, which were not found by other groups. Masses of such exoplanets and brown dwarfs are measured from collaborations with Spitzer and other groups. Especially, KMTNet has been closely cooperating with Spitzer from 2015. Thus, KMTNet observes Spitzer fields. As a result, we could measure the microlens parallaxes for many events. Also, the automated KMTNet PySIS pipeline was developed before the 2017 Spitzer season and it played a very important role in selecting the Spitzer target. For the 2018 Spitzer season, we will improve the PySIS pipeline to obtain better photometric results.

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Survey of Faint Quasar candidates at 4.7 ≤ z ≤ 5.2

  • Shin, Suhyun;Im, Myungshin;Kim, Yongjung;Hyun, Minhee;Park, Woojin;Ji, Tae-geun;Jeon, Yiseul;Kim, Minjin;Kim, Dohyeong;Kim, Jae-Woo;Taak, Yoon Chan;Yoon, Yongmin;Choi, Changsu;Hong, Jueun;Jun, Hyunsung David;Karouzos, Marios;Kim, Duho;Kim, Ji Hoon;Lee, Seong-Kook;Pak, Soojong;Park, Won-Kee
    • 천문학회보
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    • 제43권1호
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    • pp.59.4-60
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    • 2018
  • To investigate the impact of the high-redshift quasars on cosmic reionization, the faint end slope of the quasars luminosity function has to be determined precisely. More quasars with low luminosity are needed to constrain the contribution to reionization in the early universe. However, finding these quasars has been regarded as tough process owing to the improper shallow depth of imaging data. In recent days, the release data of Subaru Hyper Suprime-Cam (HSC) Strategic Program survey which provide the deep images reaching ~ 25 mag facilitates searching the faint quasars candidates. To find faint quasar candidates in ELAIS-N1 field, along with the HSC data, two near-infrared (NIR) data sets also be used : The Infrared Medium-deep Survey (IMS) and The UKIRT Infrared Deep Sky Survey (UKIDSS) - Deep Extragalactic Survey (DXS). Quasar candidates selected from the multi-band color cut were observed by the SED camera for QUasars in EArly uNiverse (SQUEAN) instrument. To trace the redshifted Lyman break efficiently, appropriate medium bands comparable to targeted redshift range are chosen. The most reliable quasar candidates are finally determined through SED fitting. Using this less luminous quasars candidates, we can speculate the relation between the quasar growth and the host galaxy unbiasedly and estimate the contribution to the cosmic reionization.

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광해에 따른 밤하늘의 밝기 변화를 중심으로 본 천문 관측 환경 (Astronomical Observation Environment Study focusing on Night Sky Brightness Variation under Light Pollution)

  • 이진희;최승언;정재훈;우홍균
    • 한국지구과학회지
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    • 제30권3호
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    • pp.344-353
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    • 2009
  • 광해의 정도를 알아보기 위해 서울대 사범대학 주변 밤하늘의 밝기를 측정하였다. 표준성을 이용하여 고도에 따른 소광 계수 및 영점 상수를 구한 결과, 2009년 1월 28일에는 소광계수가 $k_B$=0.359, 영점상수는 $C_B$=4.397이 었고, 2009년 3월 27일에는 소광계수가 $k_B$=0.896, $k_V$=0.725, 영점상수는 $C_B$=6.235, $C_V$=6.027이었다. 밤하늘의 밝기는 동, 서, 남, 북 네 방위에 대해 고도 $20^{\circ}$, $40^{\circ}$, $60^{\circ}$, $75^{\circ}$, $90^{\circ}$에서 측정하였다. IRAF를 사용하여 전처리하고 측광한 결과, 1월 28일의 시상은 평균 5.1"였고 3월 27일은 5.7"이었다. 밤하늘의 등급은 방위 및 고도에 따라 $16{\leq}m_V$, $m_B{\leq}18$이었다. 도심 방향의 밤하늘 밝기는 어두운 지역에 비해 2-4정도 밝게 나타났다. 이러한 관측 조건에서 구경 40cm인 망원경을 통해 육안으로 관측할 수 있는 한계 등급은 밤하늘의 밝기 정도에 따라 대략 11-13등급이다. 1월과 3월의 밤하늘 밝기를 비교해 본 결과, B필터에서 1월이 3월에 비해 1등급 정도 어두운 것으로 나타났다.

헤일-밥 혜성(Comet Hale-Bopp, C/1995 O1)에 대한 근일점 근처에서의 분광측광 I : $C_2$, $C_3$, CN 분자 방출선의 측광학적 특성 (NARROW-BAND SPECTROPHOTOMETRY OF COMET HALE-BOPP (C/1995 O1) NEAR PERIHELION I : PHOTOMETRIC BEHAVIOR OF $C_2$, $C_3$, CN MOLECULAR BANDS)

  • 성언창;김호일;윤재혁
    • Journal of Astronomy and Space Sciences
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    • 제17권2호
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    • pp.199-210
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    • 2000
  • 이 연구는 1997년 2월 21일부터 5월 l일까지 소백산천문대 61 cm망원경과 CCD카메라, 그리고 5개의 협대역 필터를 이용하여 근일점 근방을 지나는 헤일-밥 혜성 (Comet Hale-Bopp, C/1995 01) 코어 4’ 내의 CN, $C_2$, $C_3$ 방출선에 대한 분광측광 관측 결과이다. 이 연구에서는 협대역 필터를 이용한 분자 방출선 영상의 형태학적인 특징과 근일점 근처에서의 시간에 따른 분자 방출 선의 변화 추이에 대하여 논의하였다. 헤일-밥 혜성은 형태학적인 면에서 중심에서 반경 4' 내에 있는 혜성 코어의 CN의 분자 방출선은$C_2$$C_3$에 비하여 구형의 대청척인 형태를 보인 반면, $C_2$$C_3$ 분자의 방출선은 비대청적인 분포를 보였다. 그리고 이들 분자의 방출선 영상에서 광대역 필터의 영상에 나타난 나선팔과 같은 형태학적 특성이 나타났다. 한편 측광학적인 특정으로 $C_2$, $C_3$ 분자 방출선의 광도 분포는 CN 보다 중심 집중도가 높게 나타났으며, 태양으로부터 거리에 따른 CN의 표면광도 변화는 $C_2$, $C_3$ 표면광도 변화와 약간 다른 경향을 나타내었다. 그 러나 근일점 근처에서 이들 분자의 방출선의 광도의 따른 변화는 이천 연구에서 제기되었던 7일 주기로 나타나는 극대 광도를 보여 주고 있다.

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