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X-ray Study of Low-mass Young Stellar Objects in the ρ Ophiuchi ...

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92 CHAPTER 6. INDIVIDUAL SOURCESFig. 6.26.— ACIS image around A-48 <strong>in</strong> 0.5–9.0 keVsmoo<strong>the</strong>d with a Gaussian <strong>of</strong> σ = 6 pixels. Large andsmall circles represent <strong>the</strong> position <strong>of</strong> A-48 and a BD cGY84, respectively.6.6.3 A-75/BF-11 – LFAM21A-75 = BF-11 has no NIR counterpart but is spatially identified with <strong>the</strong> radio-bright sourceLFAM21, a candidate <strong>of</strong> a compact extragalactic AGN (St<strong>in</strong>e et al., 1988). Both X-<strong>ray</strong> spectra <strong>of</strong>LFAM21 seem to be non-<strong>the</strong>rmal typical <strong>of</strong> AGNs and show l<strong>in</strong>e-like structure at ∼5 keV (Figure6.27). We hence fit <strong>the</strong>m by a (power-law + gaussian) model assum<strong>in</strong>g <strong>the</strong> same absorption. Thebest-fit models and parameters are shown <strong>in</strong> Figure 6.27 and Table 6.8. The best-fit photon <strong>in</strong>dex<strong>of</strong> 1.2–1.4 and N H <strong>of</strong> ∼6×10 22 cm −2 are reasonable to consider that <strong>the</strong> typical AGN spectrum isabsorbed at <strong>the</strong> <strong>ρ</strong> Oph cloud (Tachihara et al., 2000). The l<strong>in</strong>e center energy is 4.8–5.0 keV. If thisis a redshifted neutral iron (6.4 keV) frequently seen <strong>in</strong> <strong>the</strong> AGN spectra (Awaki et al., 1991), aredshift (z) <strong>of</strong> LFAM21 is estimated to be ∼ 0.3.Fig. 6.27.— X-<strong>ray</strong> spectra <strong>of</strong> LFAM21 <strong>in</strong> obs-A (A-75, left) and obs-BF (BF-11, right). The upperpanel shows data po<strong>in</strong>ts (crosses) and <strong>the</strong> best-fit (power-law + gaussian) model (solid and dashedl<strong>in</strong>es), while <strong>the</strong> lower panel shows residuals from <strong>the</strong> best-fit model.

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