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Quasars as standard candles - I. The physical relation between disc and coronal emission

机译:类星体作为标准蜡烛-I.椎间盘与日冕发射之间的物理关系

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Context. A tight non-linear relation exists between the X-ray and UV emission in quasars (i.e. L X ∝ L _(UV)~(γ)), L X ∝ L UV γ with a dispersion of ~ 0.2 dex over approximately three orders of magnitude in luminosity. Such observational evidence has two relevant consequences: (1) an ubiquitous physical mechanism must regulate the energy transfer from the accretion disc to the X-ray emitting corona ; and (2) the non-linearity of the relation provides a new, powerful way to estimate the absolute luminosity, turning quasars into a new class of standard candles . Aims. Here we propose a modified version of this relation, which involves the emission line full-width half maximum, L _(X) ∝ L _(UV)~( γ? ) υ ~( β? )_(fwhm). L X ∝ L UV γ? υ fwhm β? Methods. We interpret this new relation through a simple, ad hoc model of accretion disc corona, derived from previous works in the literature where it is assumed that reconnection and magnetic loops above the accretion disc can account for the production of the primary X-ray radiation. Results. We find that the monochromatic optical-UV (2500 ?) and X-ray (2 keV) luminosities depend on the black hole mass and accretion rate as L _(UV) ∝ M _(BH)~(4/3)( M? / M? _(Edd))~(2/3) L UV ∝ M BH 4 / 3 ( M? / M? ) 2 / 3 Edd and L _(X) ∝ M _(BH)~(19/21)( M? / M? _(Edd))~(5/21), L X ∝ M BH 19 / 21 ( M? / M? ) 5 / 21 Edd respectively. Assuming a broad line region size function of the disc luminosity R _(blr) ∝ L _(disc)~(0.5) R blr ∝ L disc 0.5 we finally have that L _(X) ∝ L _(UV)~(4/7) υ ~(4/7)_(fwhm). L X ∝ L UV 4 / 7 υ fwhm 4 / 7 Such relation is remarkably consistent with the slopes and the normalisation obtained from a fit of a sample of 545 optically selected quasars from SDSS DR7 cross matched with the latest XMM-Newton catalogue 3XMM-DR6. Conclusions. The homogeneous sample used here has a dispersion of 0.21 dex, which is much lower than previous works in the literature and suggests a tight physical relation between the accretion disc and the X-ray emitting corona. We also obtained a possible physical interpretation of the L _(X)? L _(UV) relation (considering also the effect of υ _(fwhm) ), which puts the determination of distances based on this relation on a sounder physical grounds. The proposed new relation does not evolve with time, and thus it can be employed as a cosmological indicator to robustly estimate cosmological parameters.
机译:上下文。类星体的X射线和UV发射之间存在紧密的非线性关系(即LX L L_(UV)〜(γ)),LX L L UVγ,在大约三个数量级上的色散为〜0.2 dex在发光度上。这种观察证据有两个相关的后果:(1)普遍存在的物理机制必须调节从吸积盘到X射线发射日冕的能量转移; (2)关系的非线性为估算绝对光度提供了一种新的强大方法,将类星体转变为一类新的标准蜡烛。目的在这里,我们提出对此关系的修改版本,其中涉及发射线全角半最大值L_(X)∝L_(UV)〜(γ?)υ〜(β?)_(fwhm)。 L X ∝ L UVγ? ββ?方法。我们通过简单,临时的吸积盘电晕模型来解释这种新关系,该模型源自文献中以前的工作,其中假设吸积盘上方的重新连接和磁环可以解释初级X射线辐射的产生。结果。我们发现单色光学UV(2500?)和X射线(2 keV)的光度取决于黑洞质量和吸积率,如L _(UV)∝ M _(BH)〜(4/3)(M / / M?_(Edd))〜(2/3)L UV ∝ M BH 4/3(M?/ M?)2/3 Edd和L _(X)∝ M _(BH)〜(19 / 21)(M·/ M·_(Edd))〜(5/21),LX M BH 19/21(M·/ M·)5/21 Edd。假设圆盘亮度R _(blr)∝ L _(disc)〜(0.5)R blr ∝ L盘0.5的宽线区域大小函数,我们最终得到L _(X)∝ L _(UV)〜(4 / 7)υ〜(4/7)_(fwhm)。 LX ∝ L UV 4/7υfhm 4/7这种关系与斜率和归一化非常一致,该归一化是通过对来自SDSS DR7的545个光学选择类星体的样本进行拟合获得的,该样本与最新的XMM-Newton目录3XMM-DR6交叉匹配。结论。此处使用的均质样品的色散为0.21 dex,比文献中的先前工作低得多,并且表明吸积盘和X射线发射电晕之间存在紧密的物理关系。我们还获得了L _(X)的可能物理解释。 L _(UV)关系(还考虑υ_(fwhm)的影响),这使基于该关系的距离确定基于更合理的物理基础。提出的新关系不会随时间发展,因此可以用作宇宙学指标来稳健地估计宇宙学参数。

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