论文标题

强镜头II:椭圆形强力模型的星系质量轮廓

Galaxy mass profiles from strong lensing II: The elliptical power-law model

论文作者

O'Riordan, Conor M., Warren, Stephen J., Mortlock, Daniel J.

论文摘要

当将单数幂律椭圆形模型拟合到对扩展源的典型强透镜观察中时,我们可以在质谱斜率$γ$上进行约束$σ_γ$的系统分析。这些结果扩展了我们先前对圆形系统的分析,论文I。我们从676个模拟观测值中得出了涵盖一系列图像配置的模拟观测值,每个观测值都以固定的信号与噪声比$ $ s = 100 $中的图像中。我们使用理论的组合和简化的模型来分析结果,该模型可以确定对每个镜头图像中单个通量和位置的约束的贡献。主要结果是:1。对于任何镜头椭圆度,两个图像系统的约束$σ_γ$由纸I的结果很好地描述为椭圆形坐标。 2。我们为$σ_γ$的分析表达式提供了与镜头轴对齐的系统的分析表达式; 3。对于两个图像系统和对齐系统,$σ_γ$受通量不确定性的限制; 4。离轴四图像系统的限制比源大小要比两位图像系统高出两到八倍,并且随着镜头椭圆度的增加而改善。我们表明,这些系统中的$γ$的约束从图像的互补位置信息中得出,而无需使用磁通。随着源源从轴的偏移增加,互补性的提高,使得源$σ_γ<0.01 $,对于$ s = 100 $,当源接近苛性碱时就会发生。

We present a systematic analysis of the constraints $σ_γ$ on the mass profile slope $γ$ obtainable when fitting a singular power-law ellipsoid model to a typical strong lensing observation of an extended source. These results extend our previous analysis of circular systems, Paper I. We draw our results from 676 mock observations covering a range of image configurations, each created with a fixed signal to noise ratio $S=100$ in the images. We analyse the results using a combination of theory and a simplified model which identifies the contribution to the constraints of the individual fluxes and positions in each of the lensed images. The main results are: 1. For any lens ellipticity, the constraints $σ_γ$ for two image systems are well described by the results of Paper I, transformed to elliptical coordinates; 2. We derive an analytical expression for $σ_γ$ for systems with the source aligned with the axis of the lens; 3. For both two-image systems and aligned systems, $σ_γ$ is limited by the flux uncertainties; 4. The constraints for off-axis four-image systems are a factor of two to eight better, depending on source size, than for two-image systems, and improve with increasing lens ellipticity. We show that the constraints on $γ$ in these systems derive from the complementary positional information of the images alone, without using flux. The complementarity improves as the offset of the source from the axis increases, such that the best constraints $σ_γ<0.01$, for $S=100$, occur when the source approaches the caustic.

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