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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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56 CHAPTER 5. CHANDRA OBSERVATIONS OF THE <strong>ρ</strong> OPHIUCHI CLOUDTable 5.4 (Cont<strong>in</strong>ued)No. t p τ r τ d Q Comment(ks) (ks) (ks) (Cts ks −1 )BF-36 30 4.4(1.7–9.4) ... ‡ 0.8(0.6–0.9)BF-92 20 0.5 * 2.6(1.1–4.4) 1.9 ** We can not determ<strong>in</strong>e errors because <strong>of</strong> <strong>the</strong> limited statistics and/or strong coupl<strong>in</strong>g <strong>of</strong> <strong>the</strong> o<strong>the</strong>rparameters.† Fitt<strong>in</strong>g is obta<strong>in</strong>ed for light curves <strong>in</strong> 2. ′′ 5–12. ′′ 5 (A-2) and 2. ′′ 5–7. ′′ 5 (BF-64) radius circles <strong>in</strong> orderto avoid <strong>the</strong> pileup effect.‡ No fitt<strong>in</strong>g is possible because <strong>of</strong> <strong>the</strong> limited statistics and/or <strong>the</strong> boundary <strong>of</strong> <strong>the</strong> observations.§ We relax <strong>the</strong> flare peak time (t p ) to be free <strong>in</strong> order to obta<strong>in</strong> as good results as possible.‖ This should be <strong>the</strong> upper limit because <strong>the</strong> fitt<strong>in</strong>g does not <strong>in</strong>clude <strong>the</strong> time b<strong>in</strong> with zero counts.

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