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TIME-VARIABLE COMPLEX METAL ABSORPTION LINES IN THE QUASAR HS 1603+3820

机译:QUASAR HS 1603 + 3820中随时间变化的复杂金属吸收线

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We present a new spectrum of the quasar HS 1603+3820 taken 1.28 yr (0.36 yr in the quasar rest frame) after a previous observation with Subaru+HDS. The new spectrum enables us to search for time variability as an identifier of intrinsic narrow absorption lines (NALs). This quasar shows a rich complex of C IV NALs within 60,000 km s~(-1) of the emission redshift. On the basis of covering factor analysis, Misawa et al. found that the C IV NAL system at Z_(abs) = 2.42-2.45 (system A, at a shift velocity of v_(sh) = 8300-10,600 km s~(-1) relative to the quasar) was intrinsic to the quasar. With our new spectrum, we perform time variability analysis, as well as covering factor analysis, to separate intrinsic NALs from intervening NALs for eight C IV systems. Only system A, which was identified as an intrinsic system in the earlier paper by Misawa et al., shows a strong variation in line strength (W_(obs) ≈ 10.4 → 19.1 A). We speculate that a broad absorption line (BAL) could be forming in this quasar (i.e., many narrower lines will blend together to make a BAL profile). We illustrate the plausibility of this suggestion with the help of a simulation in which we vary the column densities and covering factors of the NAL complex. Under the assumption that a change of ionization state causes the variability, a lower limit can be placed on the electron density (n_e approx > 3 x 10~4 cm~(-3)) and an upper limit on the distance from the continuum source (r ≤ 6 kpc). On the other hand, if the motion of clumpy gas causes the variability (a more likely scenario), the crossing velocity and the distance from the continuum source are estimated to be v_(cross) > 8000 km s~(-1) and r < 3 pc. In this case, the absorber does not intercept any flux from the broad emission line region, but only flux from the UV continuum source. If we adopt the dynamical model of Murray et al., we can obtain a much more strict constraint on the distance of the gas parcel from the continuum source, r < 0.2 pc.
机译:在先前使用Subaru + HDS观测之后,我们提出了1.28年(类星体静止框架中为0.36年)的类星体HS 1603 + 3820的新光谱。新频谱使我们能够搜索时间变化作为固有窄吸收线(NAL)的标识符。该类星体在发射红移的60,000 km s〜(-1)范围内显示出丰富的C IV NALs复合体。根据覆盖因子分析,Misawa等。发现在Z_(abs)= 2.42-2.45时的C IV NAL系统(系统A,相对于类星体的v_(sh)= 8300-10,600 km s〜(-1)的移动速度)是类星体固有的。利用我们的新频谱,我们执行时间变异性分析以及覆盖因子分析,以将内在NAL与来自中间NAL的八个C IV系统分开。只有系统A(在Misawa等人的较早论文中被确定为内在系统)显示出线强度的强烈变化(W_(obs)≈10.4→19.1 A)。我们推测此类星体中可能会形成一条宽吸收线(BAL)(即,许多较窄的吸收线将融合在一起以形成BAL轮廓)。我们通过模拟来说明该建议的合理性,在模拟中我们改变了NAL复合物的色谱柱密度和覆盖因子。假设电离状态的变化会引起可变性,则可以对电子密度设置下限(n_e大约> 3 x 10〜4 cm〜(-3)),而对距连续源的距离设置上限(r≤6 kpc)。另一方面,如果块状气体的运动引起变化(更可能的情况),则估计交叉速度和距连续源的距离为v_(cross)> 8000 km s〜(-1)和r <3个在这种情况下,吸收剂不会拦截来自宽发射线区域的任何通量,而只会拦截来自UV连续体源的通量。如果我们采用Murray等人的动力学模型,我们可以获得对气包到连续源的距离的更严格的约束,r <0.2 pc。

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