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

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8.2. CORRELATION BETWEEN THE FLARE X-RAY PARAMETERS 1098.2 Correlation between <strong>the</strong> Flare X-<strong>ray</strong> ParametersFigures 8.1 and 8.2 show <strong>the</strong> correlations between <strong>the</strong> derived parameters <strong>of</strong> flares; τ r vs τ d and< kT > vs τ r . In <strong>the</strong>se figures, we exclude those flares that could not determ<strong>in</strong>e errors ma<strong>in</strong>ly dueto <strong>the</strong> limited statistics. Possible positive and negative log-l<strong>in</strong>ear correlations can be seen <strong>in</strong> τ r vsτ d and < kT > vs τ r , respectively. We hence check <strong>the</strong> significances <strong>of</strong> <strong>the</strong>se correlations us<strong>in</strong>g<strong>the</strong> Cox’s proportional hazard model (Isobe et al., 1986) <strong>in</strong> ASURV. This gives <strong>the</strong> significances <strong>of</strong>∼99 % (τ r vs τ d ) and ∼94 % (< kT > vs τ r ). We fur<strong>the</strong>r estimate <strong>the</strong> best-fit log-l<strong>in</strong>ear modelswith ASURV to be( τ ds ) = 102.5±0.4 ( τ rs )0.4±0.1 , (8.2)( τ rs ) = 103.8±0.1 ( < kT >keV )−0.4±0.3 . (8.3)These models are shown by <strong>the</strong> solid l<strong>in</strong>es <strong>in</strong> Figures 8.1 and 8.2.Fig. 8.1.— Relation between <strong>the</strong> rise and decay timescales <strong>of</strong> flares (τ r and τ d ). Symbols are<strong>the</strong> same as Figure 7.6. The solid l<strong>in</strong>e represents <strong>the</strong> best-fit log-l<strong>in</strong>ear correlations derived withASURV (Eq.8.2). The dashed l<strong>in</strong>e is <strong>the</strong> best-fit model <strong>of</strong> Eq.(C.12).

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