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首页> 外文期刊>The Astrophysical journal >CHANDRA AND ASCA OBSERVATIONS OF THE X-RAY-BRIGHTEST T TAURI STARS IN THE ρ OPHIUCHI CLOUD
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CHANDRA AND ASCA OBSERVATIONS OF THE X-RAY-BRIGHTEST T TAURI STARS IN THE ρ OPHIUCHI CLOUD

机译:费城云中X射线最亮的T陶里星的CHANDRA和ASCA观测

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We present the Chandra Advanced CCD Imaging Spectrometer and ASCA Gas Imaging Spectrometer results for a series of four long-term observations on DoAr 21, ROXs 21, and ROXs 31, the X-ray-brightest T Tauri stars in the ρ Ophiuchi cloud. In the four observations with a net exposure of ~600 ks, we found six, three, and two flares from DoAr 21, ROXs 21, and ROXs 31, respectively; hence, the flare rate is fairly high. The spectra of DoAr 21 are well fitted with a single-temperature plasma model, while those of ROXs 21 and ROXs 31 need an additional soft plasma component. Since DoAr 21 is younger (~10~5 yr) than ROXs 21 and ROXs 31 (~10~6, yr), these results may indicate that the soft component gradually increases as T Tauri stars age. The abundances are generally subsolar and vary from element to element. Both high first ionization potential (FIP) and low-FIP elements show enhancement over the mean abundances. An unusual giant flare is detected from ROXs 31. The peak luminosity and temperature are ~10~(33) ergs s~(-1) and ~10 keV, respectively. The temperature reaches its peak value before the flux maximum and is nearly constant (4-5 keV) during the decay phase, indicating successive energy release during the flare. The abundances and absorption show dramatic variability from the quiescent to flare phase.
机译:我们介绍了Chandra Advanced CCD成像光谱仪和ASCA气体成像光谱仪的结果,该结果对ρ蛇夫座云中DoAr 21,ROX 21和ROX 31(X射线最亮的T Tauri星)进行了四次长期观测。在四个净暴露量约为600 ks的观测中,我们分别从DoAr 21,ROX 21和ROX 31中发现了六个,三个和两个火炬。因此,耀斑率很高。 DoAr 21的光谱非常适合单温度等离子体模型,而ROX 21和ROX 31的光谱则需要额外的软等离子体成分。由于DoAr 21比ROX 21和ROX 31(〜10〜6,yr)年轻(〜10〜5年),因此这些结果可能表明,随着T Tauri星体年龄的增加,软组分逐渐增加。丰度通常是太阳下的,并且随元素的不同而变化。高第一电离势(FIP)和低FIP元素均显示出超过平均丰度的增强。从ROXs 31处检测到一个不寻常的巨大耀斑。峰值发光度和温度分别为〜10〜(33)ergs s〜(-1)和〜10 keV。温度在通量最大值之前达到峰值,并且在衰减阶段几乎保持恒定(4-5 keV),这表明在爆发期间能量不断释放。从静止阶段到耀斑阶段,丰度和吸收率显示出巨大的变化。

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