X-ray Study of Low-mass Young Stellar Objects in the ρ Ophiuchi ...
X-ray Study of Low-mass Young Stellar Objects in the ρ Ophiuchi ...
X-ray Study of Low-mass Young Stellar Objects in the ρ Ophiuchi ...
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6.3. OTHER T TAURI STARS 77quasi-periodic flares from YLW15A (Tsuboi et al., 2000). We hence make and fit <strong>the</strong> time slicedspectra <strong>of</strong> A-79 as shown <strong>in</strong> Figure 6.14, however no significant sign <strong>of</strong> <strong>in</strong>crease <strong>of</strong> kT is found at<strong>the</strong> second flare but it keeps almost constant <strong>of</strong> 3–4 keV (phases 3–5 <strong>in</strong> Figure 6.14), which is asharp contrast to <strong>the</strong> case <strong>of</strong> YLW15A (Figure 2 <strong>in</strong> Tsuboi et al., 2000).6.3.7 BF-10 – WL22The X-<strong>ray</strong> spectrum <strong>of</strong> a class II BF-10 = WL22 exhibitsclear l<strong>in</strong>e structure at ∼3.2 and ∼3.9 keV (Figure 6.15).The l<strong>in</strong>e energies correspond to He-like Ca and Ar. Wehence relax <strong>the</strong> abundances <strong>of</strong> <strong>the</strong>se elements to be freeand fit it by <strong>the</strong> MEKAL model. The best-fit < kT >and N H are 2.1 keV and 12×10 22 cm −2 , respectively (Table5.2), while <strong>the</strong> abundances <strong>of</strong> Ar and Ca are 2.7 +8.3−2.7and 5.0 +7.9−4.1 solar. Thus Ca is extremely overabundant,although <strong>the</strong> mechanism is an open question.Fig. 6.15.— Spectrum <strong>of</strong> BF10 = WL22. Theupper panel shows data po<strong>in</strong>ts (crosses) and <strong>the</strong>best-fit MEKAL model (solid l<strong>in</strong>e), while <strong>the</strong>lower panel shows residuals from <strong>the</strong> best-fitmodel. The l<strong>in</strong>e structure at ∼3.2 keV and ∼3.9keV is due to He-like Ar and Ca.Fig. 6.14.— (top) Light curve and(middle and bottom) time evolution <strong>of</strong>kT and EM <strong>of</strong> A-79 = GY195.