¨28 CHAPTER 4. INSTRUMENTATIONsplit threshold (13 ADU; if <strong>the</strong> neighbor<strong>in</strong>g pixel has larger pixel value than <strong>the</strong> split threshold,it is regarded as <strong>the</strong> leak<strong>in</strong>g pixel). Table 4.2 gives <strong>the</strong> relationship <strong>of</strong> <strong>the</strong> ASCA/SIS and ACISgrad<strong>in</strong>g schemes. Usually, we regard <strong>the</strong> grades correspond<strong>in</strong>g to <strong>the</strong> ASCA/SIS grades 0, 2, 3, 4,and 6 as real events.£¢¡¥¤¦¢§¢¡¤ £¢¦Fig. 4.9.— Schematic for determ<strong>in</strong><strong>in</strong>g <strong>the</strong> ACIS grade. For example,an event that caused all pixels to exceed <strong>the</strong>ir threshold is grade 255.A s<strong>in</strong>gle pixel event is grade 0.£ ¡ §Table 4.2: Relation between <strong>the</strong> ASCA/SIS and ACIS gradesASCA/SIS gradeACIS grade0 . . . . . . . . . . . . . . . 01 . . . . . . . . . . . . . . . 1, 4, 5, 32, 33, 36, 37, 128, 129, 132, 133, 160, 161, 164, 1652 . . . . . . . . . . . . . . . 2, 34, 64, 65, 68, 69, 130, 1623/4 . . . . . . . . . . . . 8, 12, 16, 17, 48, 49, 136, 1405 . . . . . . . . . . . . . . . 3, 6, 9, 13, 20, 21, 35, 38, 40, 44, 52, 53, 96, 97, 100, 101, 131, 134,137, 141, 144, 145, 163, 166, 168, 172, 176, 177, 192, 193, 196, 1976 . . . . . . . . . . . . . . . 10, 11, 18, 22, 50, 54, 72, 76, 80, 81, 104, 108, 138, 139, 208, 2097 . . . . . . . . . . . . . . . All o<strong>the</strong>r gradesOperat<strong>in</strong>g modeTwo operat<strong>in</strong>g modes are available for ACIS. In this <strong>the</strong>sis, we only use <strong>the</strong> data <strong>of</strong> Timed Exposuremode with full frames and <strong>the</strong> frame time <strong>of</strong> 3.2 s.• Timed Exposure (TE) modeThe 1024 × 1024 active region <strong>of</strong> <strong>the</strong> CCD is exposed for a selected time <strong>in</strong>terval (frametime), <strong>the</strong>n <strong>the</strong> collected charge quickly (∼41 ms) transfers to <strong>the</strong> framestore region. For <strong>the</strong>entire CCD (full frames), <strong>the</strong> frame time is 3.2 s, which is <strong>the</strong> nom<strong>in</strong>al tim<strong>in</strong>g resolution <strong>of</strong>ACIS. In order to obta<strong>in</strong> better tim<strong>in</strong>g resolution or to avoid <strong>the</strong> pileup effect (see below),we can select subar<strong>ray</strong> mode; <strong>the</strong> active region is limited to 1/2, 1/4, or 1/8 subar<strong>ray</strong>, whichshortens <strong>the</strong> frame time to 0.4 s at <strong>the</strong> m<strong>in</strong>imum.
4.3. ACIS – ADVANCED CCD IMAGING SPECTROMETER 29• Cont<strong>in</strong>uous Clock<strong>in</strong>g (CC) modeCC mode achieves high tim<strong>in</strong>g resolution (3 ms) but has only one dimension <strong>of</strong> spatial resolution.Data are cont<strong>in</strong>uously clocked through <strong>the</strong> CCD and framestore to m<strong>in</strong>imize <strong>the</strong>readout time, with one-dimensional (1 × 1024 pixels) images.Telemetry formatThree telemetry formats are available as follows. Table 4.3 lists <strong>the</strong> operat<strong>in</strong>g modes, associatedformats, and approximate event rates at <strong>the</strong> telemetry saturation. The fa<strong>in</strong>t and very fa<strong>in</strong>t formatswere used for obs-BF and obs-A, respectively (§5.1).• GradedThis provides event positions <strong>in</strong> detector coord<strong>in</strong>ates, event amplitudes, arrival times, andevent grades.• Fa<strong>in</strong>tThis provides <strong>the</strong> same <strong>in</strong>formation as <strong>the</strong> Graded format o<strong>the</strong>r than <strong>the</strong> event grades. Alternatively,this supplies all <strong>in</strong>formation about 3 × 3 pixels around <strong>the</strong> event pixel. The biasmap (zero level <strong>of</strong> each pixel) is telemetered separately.• Very Fa<strong>in</strong>tThis is basically <strong>the</strong> same as <strong>the</strong> Fa<strong>in</strong>t format, but provides all <strong>in</strong>formation about 5 × 5 pixelsaround <strong>the</strong> event pixel. This format is used for <strong>the</strong> TE mode only and <strong>of</strong>fers <strong>the</strong> advantagefor m<strong>in</strong>imiz<strong>in</strong>g <strong>the</strong> background after ground process<strong>in</strong>g, but is limited for low-count sources(Table 4.3).Event pileupFor bright sources, two or more X-<strong>ray</strong> photons are <strong>of</strong>ten registered <strong>in</strong> a s<strong>in</strong>gle ACIS pixel with<strong>in</strong> onereadout cycle, which is called pileup. It causes an artificial spectral harden<strong>in</strong>g and underestimate<strong>of</strong> <strong>the</strong> X-<strong>ray</strong> counts. In fact, <strong>the</strong> brightest two sources <strong>in</strong> <strong>the</strong> <strong>ρ</strong> <strong>Ophiuchi</strong> cloud (A-2 and BF-64,see chapter 5) suffered <strong>the</strong> pileup effect. It can be reduced by select<strong>in</strong>g a proper observ<strong>in</strong>g mode(e.g., shorten <strong>the</strong> exposure time).
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Chapter 8Systematic Study of YSO Fl
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8.2. CORRELATION BETWEEN THE FLARE
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8.3. MAGNETIC RECONNECTION MODEL 11
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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