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Constraints on the Collimated X-ray Emission of SS 433 from the Reflection on Molecular Clouds

机译:来自分子云反射的SS 433的准直X射线发射的约束

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We calculate the X-ray signal that should arise due to reflection of the putative collimated X-ray emission of the Galactic supercritical accretor SS 433 on the molecular clouds in its vicinity. The molecular gas distribution in the region of interest has been constructed based on the data of the Boston University-Five College Radio Astronomy Observatory Galactic Ring Survey in (CO)-C-13 J= 1 0 emission line, while the collimated emission was assumed to be aligned with the direction of the relativistic jets, which are continuously launched by the system. We consider all the available Chandraobservations covering the regions possibly containing the reflection signal and put constraints on the apparent face-on luminosity of SS 433 above 4 keV. No signatures of the predicted signal have been found in the analysed regions down to a 4-8 keV surface brightness level of approximate to 10(-11) erg/s/cm(2)/deg(2). This translates into the limit on the apparent face-on 2-10 keV luminosity of SS 433 LX2-10 less than or similar to 8 x10(38) erg/s, provided that the considered clouds do fall inside the illumination cone of the collimated emission. This, however, might not be the case due to persisting uncertainty in the line-of-sight distances to SS 433 d(SS433) (4.5-5.5 kpc) and to the considered molecular clouds. For the half-opening angle of the collimation cone larger than or comparable to the amplitude of the jets' precession (approximate to 21 degrees), the stringent upper limit quoted above is most relevant if d(SS433) < 5 kpc, provided that the kinematic distances to the considered molecular clouds are sufficiently accurate (within approximate to 1000 pc of the adopted values). Dropping the last assumption, a more conservative constraint is LX2-10 less than or similar to 10(40) erg/s for d(SS433) = 4.65-4.85 kpc, and yet worse for d(SS433) outside this range. We conclude that SS 433 is not likely to belong to the brightest ultraluminous X-ray sources if it could be obser
机译:我们计算出由于在其附近的分子云上的半乳液超临界血管缩放器SS 433的推定准直的X射线发射而产生的X射线信号。利息区域的分子气体分布是基于(CO)-C-13J = 1 0排放线(CO)-C-13J = 1 0排放线的波士顿大学 - 五大学射频天文学天文台勘测的数据而构建。假设准直排放与由系统连续发射的相对论喷射器的方向对齐。我们考虑所有可用的Chandraobservations,覆盖可能包含反射信号的区域,并在4 keV以上的SS 433的表观面对明显的亮度上放置约束。在分析的区域中没有发现预测信号的签名降至4-8keV表面亮度水平近似为10(-11)erg / s / cm(2)/ deg(2)。这转化为SS 433 LX2-10的表观面对2-10keV光度的极限,小于或类似于8 x10(38)ERG / s,只要被认为的云确实落入准直的照明锥内排放。然而,这可能不是由于持续存在于SS 433d(SS433)(4.5-5.5 kPc)和所考虑的分子云的不确定性而不确定性的情况。对于大于或与喷射器的幅度大的准直锥体的半开口角度(近似为21度),上面引用的严格上限是最相关的,如果d(ss433)<5 kpc提供了对所考虑的分子云的运动距离足够精确(在近似1000 pc的所采用值内)。丢弃最后的假设,更保守的约束是LX2-10小于或类似于D(SS433)= 4.65-4.85 kPc的10(40)个ERG / s,但在该范围之外的D(SS433)更差。我们得出结论,如果可能是观察者,SS 433不太可能属于最亮的超亮X射线源

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