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

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86 CHAPTER 6. INDIVIDUAL SOURCESthat A-31 is surely associated with KSHK-A. The chance probability to detect a background AGN<strong>in</strong> <strong>the</strong> KSHK-A region is only ∼0.2 %. Fur<strong>the</strong>rmore, A-31 exhibits variable X-<strong>ray</strong>s typical <strong>of</strong>low-<strong>mass</strong> YSOs. The column density <strong>of</strong> KSHK-A is ∼10 24 cm −2 (Kamazaki et al., 2001), whichis about twice <strong>of</strong> <strong>the</strong> X-<strong>ray</strong> determ<strong>in</strong>ed N H <strong>of</strong> A-31 (∼ 5×10 23 cm −2 ). Thus A-31 would be aYSO embedded near <strong>the</strong> center <strong>of</strong> <strong>the</strong> compact core KSHK-A. KSHK-A is spatially co<strong>in</strong>cidentwith a 6 cm cont<strong>in</strong>uum source LFAM6 (Leous et al., 1991), which may be produced by a shock<strong>of</strong> outflow from a putative protostar (e.g., Rodriguez et al.1989, and references <strong>the</strong>ir<strong>in</strong>). No NIRcounterpart with K < 15 mag, its close location at <strong>the</strong> compact core center KSHK-A, <strong>the</strong> largeabsorption (∼5×10 23 cm −2 ), and <strong>the</strong> presence <strong>of</strong> <strong>the</strong> 6 cm enhancement <strong>in</strong>dicate that A-31 is astrong candidate <strong>of</strong> X-<strong>ray</strong> emitt<strong>in</strong>g class 0.A northwest part <strong>of</strong> <strong>the</strong> CO molecular outflow from <strong>the</strong> class 0 VLA1623 (designated as E–H<strong>in</strong> Yu, & Chern<strong>in</strong> 1997) is not aligned to <strong>the</strong> central part (B–D) but is slightly shifted to <strong>the</strong> northdirection po<strong>in</strong>t<strong>in</strong>g to A-29 and A-31 (Figure 6.21). We speculate that <strong>the</strong> orig<strong>in</strong> <strong>of</strong> <strong>the</strong> outflowE–H is A-29 or A-31 (not from VLA1623), although <strong>the</strong>re is no CO emission at <strong>the</strong>ir closer vic<strong>in</strong>ity(Kamazaki et al., 2001).Fig. 6.21.— 12 CO (J=1–0) map aroundVLA1623 (Yu, & Chern<strong>in</strong>, 1997). Filledsquares represent <strong>the</strong> positions <strong>of</strong> A-29 andA-31.BF-36BF-36 is located <strong>in</strong> <strong>the</strong> 850 µm clump SMM J16272−2430 with about 30 ′′ separation from its center.It lies <strong>in</strong> an elongated 1.3 mm core cha<strong>in</strong> with local peaks <strong>of</strong> B1-MM2, 3, and 4 (Motte et al., 1998).The source is about 30 ′′ south <strong>of</strong> <strong>the</strong> peak <strong>of</strong> B1-MM4 (Figure 6.18). The chance probability <strong>of</strong>background AGN to be associated with<strong>in</strong> 30 ′′ radius from <strong>the</strong> core center is ∼20 %. However,BF-36 is among <strong>the</strong> brightest unidentified sources and is very unique which exhibits a clear flare.We <strong>the</strong>refore suggest that BF-36 is also a cloud member embedded near <strong>the</strong> dense core B1-MM4.S<strong>in</strong>ce millimeter/sub-millimeter peak fluxes <strong>of</strong> B1-MM4/SMM J16272−2430 are about ten timesfa<strong>in</strong>ter than those harbor A-29 and A-31, although <strong>the</strong> clump size is comparable (6200 AU), <strong>the</strong>2–6 times smaller N H <strong>of</strong> BF-36 (9×10 22 cm −2 ) than those <strong>of</strong> A-29 and A-31 is consistent with <strong>the</strong>

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