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arXiv 1111.0989astro-ph.CO
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星系群的弱透镜质量估计和视线污染

Weak lensing mass estimates of galaxy groups and the line-of-sight contamination

P. F. Spinelli, S. Seitz, M. Lerchster, F. Brimioulle, A. Finoguenov

摘要:

弱透镜效应是确定星系团质量的重要方法。然而,背景星系形状上的扭曲印记受到视线上所有质量含量的影响。使用COSMOS剪切模拟数据,我们研究了165组的剪切剖面,并调查了相邻组可以增强或抑制来自主晕的剪切信号的水平。我们的模拟数据是基于CFHT和斯巴鲁观测和信息的星系群是从宇宙X射线目录的扩展源。这些群体的预期重力剪切场的计算假设的晕遵循NFW密度分布。我们的结论是,平均而言,检测主晕的信噪比受~15%x \sqrt{ngal/30}的影响,相对于相同晕在天空中孤立时的信噪比。具有投影距离接近(<1 ')的相邻组受影响最大,但是位于较大角距离处的晕也引起可测量的剪切信号,其可以被解释为不相关的大尺度结构。由外部晕引入的单个组的质量过量估计的平均偏差为零,均方根为~6- 72%,取决于所使用的孔径大小。由大尺度结构引入的剪切信号充当外部噪声源。当孔径尺寸为5“时,引入的平均不确定度为σ_{γ_t}^{LSS}~0.006,相当于单分量本征椭圆度值的1.8%。这种大尺度结构噪声误差变得等于固有的椭圆率噪声,如果在一定的孔径内有约3000个星系的测量,一个数字,已经实现了目前的深调查,如COSMOS,因此,不应该被忽略。

英文摘要:

Weak lensing is an important technique to determine the masses of galaxy groups. However, the distortion imprint on the shape of the background galaxies is affected by all the mass content along the line-of-sight. Using COSMOS shear mock data we study the shear profile of 165 groups and investigate the level at which the neighbouring groups can enhance or suppress the shear signal from the main halo. Our mock data are based on CFHT and Subaru observations and the information on the galaxy groups is taken from the COSMOS X-ray catalogue of extended sources. The expected gravitational shear field of these groups is calculated assuming that the haloes follow NFW density profiles. We conclude that, on average, the signal-to-noise for a detection of the main halo is affected by ~15%x\sqrt{ngal/30} with respect to the signal-to-noise the same halo would have if it was isolated in the sky. Groups with neighbours that are close in projected distance (<1') are the most affected, but haloes located at larger angular distances also cause a measurable shear signal, which can be interpreted as uncorrelated large-scale structure. The average bias in the mass excess estimate of individual groups that is introduced by the external haloes is zero with an rms of ~6-72%, depending on the aperture size used. The shear signal introduced by large-scale structure acts as an external source of noise. The averaged uncertainty introduced is σ_{γ_t}^{LSS}~0.006 per component for an aperture size of ~5', which corresponds to 1.8% of the one-component intrinsic ellipticity value. This large-scale structure noise error becomes equal to intrinsic ellipticity noise if there are measurements for ~3000 galaxies within a certain aperture, a number that is already achieved by current deep surveys such as COSMOS and, therefore, should not be ignored.

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