62 CHAPTER 6. INDIVIDUAL SOURCES6.2 X-<strong>ray</strong> Brightest T Tauri Stars (DoAr21, ROXs21, and ROXs31)Imanishi et al. (2002a) showed <strong>the</strong> Chandra/ACIS and ASCA/GIS results for a series <strong>of</strong> four longtermobservations <strong>of</strong> DoAr21 (A-2), ROXs21 (BF-46) and ROXs31 (BF-96), <strong>the</strong> X-<strong>ray</strong> brightestTTSs <strong>in</strong> <strong>the</strong> <strong>ρ</strong> <strong>Ophiuchi</strong> cloud, <strong>the</strong>n studied <strong>the</strong>ir long-term time variability and detailed structure<strong>of</strong> X-<strong>ray</strong> spectra. Here we show details.6.2.1 Previous knowledgeThe E<strong>in</strong>ste<strong>in</strong> satellite first recognized <strong>the</strong>se sources as bright X-<strong>ray</strong> sources (Montmerle et al.,1983). Subsequent optical observations revealed that <strong>the</strong>y are K–M type stars hav<strong>in</strong>g weak Hαemission (Bouvier & Appenzeller, 1992), which are classified as WTTSs (class III). Simon et al.(1995) observed <strong>the</strong>m by us<strong>in</strong>g <strong>the</strong> lunar occultation <strong>in</strong> <strong>the</strong> <strong>in</strong>frared wavelengths and found thatROXs21 and ROXs31 are b<strong>in</strong>ary systems with separation angles <strong>of</strong> 0. ′′ 3 and 0. ′′ 48, respectively.Shevchenko & Herbst (1998) reported <strong>the</strong> rotation period <strong>of</strong> ROXs21 to be 1.39 days. S<strong>in</strong>ce <strong>the</strong>yshow no cont<strong>in</strong>uum emission at 1.3 mm (André & Montmerle, 1994), <strong>the</strong> circumstellar envelopewould have already disappeared, while DoAr21 may still have an accretion disk as suggested by<strong>the</strong> detection <strong>of</strong> NIR polarized emission (Ageorges et al., 1997). Us<strong>in</strong>g <strong>the</strong> <strong>the</strong>oretical evolutionarytracks <strong>in</strong> <strong>the</strong> H-R diagram, <strong>the</strong> age <strong>of</strong> DoAr21 is estimated to be ∼10 5 yr, which is younger thanthat <strong>of</strong> ROXs21 and ROXs31 (∼10 6 yr: Nürnberger et al., 1998). F<strong>in</strong>ally, DoAr21 and ROXs31show variable centimeter emission, which is probably due to gyro-synchrotron mechanism <strong>in</strong>ducedby surface magnetic field (St<strong>in</strong>e et al., 1988).6.2.2 Long-term observations with Chandra and ASCAWe use <strong>the</strong> data <strong>of</strong> obs-BF for ROXs21 and ROXs31. Although DoAr21 suffers <strong>the</strong> pileup effect <strong>in</strong>obs-A, obs-BF detected X-<strong>ray</strong>s from DoAr21 at <strong>the</strong> ACIS-S2 chip, which mitigates photon pileupbecause <strong>of</strong> <strong>the</strong> large <strong>of</strong>f-axis angle (= large PSF size). We hence use <strong>the</strong> ACIS-S2 data for <strong>the</strong>follow<strong>in</strong>g analysis. The background region for DoAr21 is taken from a source-free 19 arcm<strong>in</strong> 2 regionon ACIS-S2, while that for ROXs21 and ROXs31 is <strong>the</strong> same as used <strong>in</strong> <strong>the</strong> previous analyses.In order to exam<strong>in</strong>e long-term variability and spectral evolution <strong>of</strong> <strong>the</strong>se sources, we additionallyuse <strong>the</strong> previous ASCA observations. Three observations (obs-A1, A2, and A3) were carriedout with <strong>the</strong> two Gas Imag<strong>in</strong>g Spectrometers (GISs: Ohashi et al., 1996) and <strong>the</strong> two Solid-stateImag<strong>in</strong>g Spectrometers (SISs: Burke et al., 1991) onboard ASCA, which are at <strong>the</strong> foci <strong>of</strong> <strong>the</strong> X-<strong>ray</strong>telescopes (XRTs: Serlemitsos et al., 1995) sensitive to photons <strong>in</strong> 0.4–10 keV. However, <strong>the</strong>y wereoutside <strong>of</strong> or at <strong>the</strong> edge <strong>of</strong> <strong>the</strong> SIS’s field <strong>of</strong> view <strong>in</strong> <strong>the</strong> majority <strong>of</strong> <strong>the</strong> observations, hence we use
6.2. X-RAY BRIGHTEST T TAURI STARS (DOAR21, ROXS21, AND ROXS31) 63<strong>the</strong> GIS data only. We retrieve <strong>the</strong> ASCA unscreened data from <strong>the</strong> HEASARC onl<strong>in</strong>e service 1 ,<strong>the</strong>n filtered out <strong>the</strong> data taken at a geomagnetic cut<strong>of</strong>f rigidity lower than 4 GV, at an elevationangle less than 5 ◦ from <strong>the</strong> Earth, and dur<strong>in</strong>g passage through <strong>the</strong> South Atlantic Anomaly.Particle events were also removed us<strong>in</strong>g <strong>the</strong> rise-time discrim<strong>in</strong>ation method. The total availableexposure times were ≈38 ks (obs-A1), 93 ks (A2), and 75 ks (A3) (Table 6.2).Table 6.2: ASCA/GIS observation logObs.ID Sequence ID Observation Date (UT) ExposureStart End (ks)A1 . . . 20015010 1993 Aug 20 02:20 Aug 20 22:46 37.7A2 . . . 25020000 1997 Mar 2 07:32 Mar 4 21:21 93.1A3 . . . 96003000 1998 Aug 13 06:35 Aug 15 21:16 74.76.2.3 Time variabilityFigures 6.3 and 6.4 show <strong>the</strong> X-<strong>ray</strong> light curves (no background subtraction) <strong>of</strong> (a) DoAr21, (b)ROXs21, and (c) ROXs31 obta<strong>in</strong>ed with Chandra/ACIS (obs-BF) and ASCA/GIS (obs-A1, A2,and A3), respectively. The vertical axis is photon counts normalized by <strong>the</strong> effective area at 1 keVfor comparison with <strong>the</strong> different <strong>in</strong>struments and observation epochs. The time <strong>in</strong>tervals <strong>of</strong> eachdata po<strong>in</strong>t are 10 3 s and 10 4 s for ACIS (Figure 6.3) and GIS (Figure 6.4), respectively.energy bands <strong>of</strong> <strong>the</strong> ACIS and GIS data for DoAr21 are 0.5–9.0 keV, while <strong>the</strong> GIS light curves forROXs21 and ROXs31 are limited <strong>in</strong> <strong>the</strong> s<strong>of</strong>t energy band <strong>of</strong> 0.5–1.5 keV <strong>in</strong> order to avoid possiblecontam<strong>in</strong>ation from a nearby variable hard X-<strong>ray</strong> source YLW15A = BF-61 (Tsuboi, 1999; Tsuboiet al., 2000). To verify whe<strong>the</strong>r or not <strong>the</strong> contam<strong>in</strong>ation from YLW15A is significant <strong>in</strong>
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Contents1 Introduction 12 Review of
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List of Figures2.1 The H-R diagram
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LIST OF FIGURESix6.17 Light curves
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List of Tables3.1 Multiwavelength s
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Chapter 1IntroductionStar formation
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Chapter 2Review of Low-mass Young S
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2.1. EVOLUTION OF LOW-MASS STARS 5w
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2.2. MOLECULAR CLOUDS 72.2 Molecula
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2.3. X-RAY OBSERVATIONS OF LOW-MASS
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8.5. EFFECT OF THE QUIESCENT X-RAYS
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8.6. EVOLUTION OF YSOS AND THEIR FL
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Chapter 9ConclusionWe summarize the
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Appendix AFlare Light CurvesFig. A.
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Fig.A.2 (Continued)121
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Fig. A.4.— Same as Figure A.1, bu
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126 APPENDIX B. PHYSICAL PARAMETERS
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128 APPENDIX B. PHYSICAL PARAMETERS
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Appendix CModeling of the FlareIn t
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C.2. PREDICTED CORRELATIONS BETWEEN
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BibliographyAgeorges, N., Eckart, A
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BIBLIOGRAPHY 137Feigelson, E. D., &
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BIBLIOGRAPHY 139Johnstone, D., Wils
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BIBLIOGRAPHY 141Rutledge, R. E., Ba
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BIBLIOGRAPHY 143Yokoyama, T. & Shib