论文标题
伽马射线爆发的光度选择
Luminosity Selection for Gamma Ray Bursts
论文作者
论文摘要
存在伽马射线爆发(GRB)的内在光度中不可避免的散射。如果源中有相对论的光束,则视角变化必定会引入内在光度函数(ILF)的变化。散射在ILF中会导致选择偏差,其中检测到的远处的源具有比附近检测到的偏差更大的亮度。 众所周知,中位亮度将任何给定的人群分为相等的一半。当分布的功能形式尚不清楚时,它可能比使用试验功能形式的任何诊断更强大。在这项工作中,我们采用了基于中位光度的统计测试,并将其应用于测试GRB的一类模型。我们假设GRB射流具有有限的开头,并且GRB射流的方向是随机的,相对于观察者。我们以恒定的lorentz因子$γ$和开头$θ_0$参数化射流。 我们根据经验上的每个红移垃圾箱($ dz = 0.01 $)的平均为17个GRB,计算$ l_ {中值} $,从理论上讲并使用Fermi GBM数据,并指出Swift数据是有问题的,因为它是偏见的,特别是在高红移。我们发现$ l_ {中值} $接近$ l_ {max} $,用于足够扩展的GRB喷气机,并且不符合数据。当$γ$在$ 100 $和200美元之间,$θ_0\ leq 0.1 $之间,我们发现与数据的可接受拟合,前提是沿着视线沿线到ON Axis Observer的喷气材料在光学上是光学厚的,因此,屏蔽的最大亮度远低于裸$ l_ {max} $。如果我们将轴心观察者与经典投影的单调减少余辉相关联,我们发现它们的ILF与我们与平坦相位余潮相关联的离喷射观察者的ILF类似。
There exists an inevitable scatter in intrinsic luminosity of Gamma Ray Bursts(GRBs). If there is relativistic beaming in the source, viewing angle variation necessarily introduces variation in the intrinsic luminosity function(ILF). Scatter in the ILF can cause a selection bias where distant sources that are detected have a larger median luminosity than those detected close by. Median luminosity, as we know, divides any given population into equal halves. When the functional form of a distribution is unknown, it can be a more robust diagnostic than any that use trial functional forms. In this work we employ a statistical test based on median luminosity and apply it to test a class of models for GRBs. We assume that the GRB jet has a finite opening angle and that the orientation of the GRB jet is random relative to the observer. We parameterize the jet with constant Lorentz factor $Γ$ and opening angle $θ_0$. We calculate $L_{median}$ as a function of redshift with an average of 17 grbs in each redshift bin($dz=0.01$) empirically, theoretically and use Fermi GBM data, noting that SWIFT data is problematic as it is biased, specially at high redshifts. We find that $L_{median}$ is close to $L_{max}$ for sufficiently extended GRB jet and does not fit the data. We find an acceptable fit with the data when $Γ$ is between $100$ and $200$, $θ_0\leq 0.1$, provided that the jet material along the line of sight to the on axis observer is optically thick, such that the shielded maximum luminosity is well below the bare $L_{max}$. If we associate an on-axis observer with a classically projected monotonically decreasing afterglow, we find that their ILF is similar to those of off-jet observer which we associate with flat phase afterglows.