Chandra & HST类星体成像PKS B0106 +013 & 3C 345：逆康普顿X射线和磁化喷流
Chandra & HST Imaging of the Quasars PKS B0106+013 & 3C345: Inverse Compton X-rays and Magnetized Jets
摘要：
我们介绍了来自深（70 ks）钱德拉ACIS观测和哈勃空间望远镜ACS F475 W观测的两个高光学偏振类星体的结果，它们属于MOJAVE blazar样本，即，PKS B 0106 +013和1641+399（3C 345）。这些观测结果揭示了两个来源中射流的X射线和光学发射。在0106+013射电喷流的整个长度上都探测到了X射线辐射，它显示出明显的弯曲或摆动--X射线辐射在第一个显著的kpc喷流弯曲处最亮。一个螺旋状的kpc喷流的图片与第一个kpc尺度的弯曲代表一个喷流段移动接近（r）我们的视线，并得到多普勒增强在无线电和X射线频率，是与这些观察一致的。然而，来自喷流末端的X射线发射在射电热点上游约0.4”（~3.4 kpc）处达到峰值。在X射线喷流终止峰和射电热点处都检测到光发射。X射线喷流终止峰位于射电热点上游约0.2”（~1.3 kpc）的3C 345短喷流中。HST光发射被认为是在一个弧形结构符合明亮的无线电热点，我们建议是一个尖锐的（明显的）喷流弯曲，而不是一个终点，穿过我们的视线，因此具有较高的多普勒波束因子。在明亮的射电热点下游不到1英寸的地方确实观察到了一个弱的射电热点，但没有光学或X射线对应物。通过利用pc尺度的射电和kpc尺度的射电/X射线数据，我们推导出对喷流洛伦兹因子（Gamma_jet）和倾角（θ）的约束：对于从pc尺度到kpc尺度的恒定喷流速度，我们得到0106+013的Gamma_jet约为70，3C 345的Gamma_jet约为40。在放松这一假设，我们得出一个伽玛喷约2.5的两个源。两个类星体的θ的上限为~13度。（简略）
英文摘要：
We present results from deep (70 ks) Chandra ACIS observations and Hubble Space Telescope ACS F475W observations of two highly optically polarized quasars belonging to the MOJAVE blazar sample, viz., PKS B0106+013 and 1641+399 (3C345). These observations reveal X-ray and optical emission from the jets in both sources. X-ray emission is detected from the entire length of the 0106+013 radio jet, which shows clear bends or wiggles - the X-ray emission is brightest at the first prominent kpc jet bend. A picture of a helical kpc jet with the first kpc-scale bend representing a jet segment moving close(r) to our line of sight, and getting Doppler boosted at both radio and X-ray frequencies, is consistent with these observations. The X-ray emission from the jet end however peaks at about 0.4" (~3.4 kpc) upstream of the radio hot spot. Optical emission is detected both at the X-ray jet termination peak and at the radio hot spot. The X-ray jet termination peak is found upstream of the radio hot spot by around 0.2" (~1.3 kpc) in the short projected jet of 3C345. HST optical emission is seen in an arc-like structure coincident with the bright radio hot spot, which we propose is a sharp (apparent) jet bend instead of a terminal point, that crosses our line of sight and consequently has a higher Doppler beaming factor. A weak radio hot spot is indeed observed less than 1" downstream of the bright radio hot spot, but has no optical or X-ray counterpart. By making use of the pc-scale radio and the kpc-scale radio/X-ray data, we derive constraints on the jet Lorentz factors (Gamma_jet) and inclination angles (theta): for a constant jet speed from pc- to kpc-scales, we obtain a Gamma_jet of ~70 for 0106+013, and ~40 for 3C345. On relaxing this assumption, we derive a Gamma_jet of ~2.5 for both the sources. Upper limits on theta of ~13 degrees are obtained for the two quasars. (ABRIDGED)
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