论文标题

一种新的方法,用于高角度分辨率下的干涉重力透镜观测值的可见空空间建模

A novel approach to visibility-space modelling of interferometric gravitational lens observations at high angular resolution

论文作者

Powell, Devon, Vegetti, Simona, McKean, John P., Spingola, Cristiana, Rizzo, Francesca, Stacey, Hannah R.

论文摘要

我们提出了一种新的重力透镜建模技术,旨在建模具有大量可见性的高分辨率干涉观测值,而无需在时间或频率上预先启动数据。我们使用模拟观测值的验证测试证明了该方法的准确性。使用$ \ sim 10^3 $可见性的小型数据集,我们首先将方法与更传统的直接傅立叶变换(DFT)实现和直接线性求解器进行比较。我们的测试表明,我们的源反转与DFT没有区别。我们的方法还将晶状体参数置于地面真相和DFT的1%至2%以内,鉴于足够高的信噪比(SNR)。当SNR低至5时,这两种方法都会导致镜头参数中数百分之几的错误和严重破坏的源结构,这表明这与SNR和先验的选择有关,而不是建模技术本身。然后,我们分析了一个具有$ \ sim 10^8 $可见性的大数据集,以及与重力镜头系统MG J0751+2716的真实全局非常长的基线干涉测量值相匹配的SNR。数据的大小使其无法通过传统实现进行建模。使用我们的新技术,我们发现我们可以分别推断镜头参数和源亮度分布,相对于地面真相,RMS误差为0.25和0.97%。

We present a new gravitational lens modelling technique designed to model high-resolution interferometric observations with large numbers of visibilities without the need to pre-average the data in time or frequency. We demonstrate the accuracy of the method using validation tests on mock observations. Using small data sets with $\sim 10^3$ visibilities, we first compare our approach with the more traditional direct Fourier transform (DFT) implementation and direct linear solver. Our tests indicate that our source inversion is indistinguishable from that of the DFT. Our method also infers lens parameters to within 1 to 2 per cent of both the ground truth and DFT, given sufficiently high signal-to-noise ratio (SNR). When the SNR is as low as 5, both approaches lead to errors of several tens of per cent in the lens parameters and a severely disrupted source structure, indicating that this is related to the SNR and choice of priors rather than the modelling technique itself. We then analyze a large data set with $\sim 10^8$ visibilities and a SNR matching real global Very Long Baseline Interferometry observations of the gravitational lens system MG J0751+2716. The size of the data is such that it cannot be modelled with traditional implementations. Using our novel technique, we find that we can infer the lens parameters and the source brightness distribution, respectively, with an RMS error of 0.25 and 0.97 per cent relative to the ground truth.

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