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首页> 外文期刊>The Astrophysical journal >BLAST: CORRELATIONS IN THE COSMIC FAR-INFRARED BACKGROUND AT 250, 350, AND 500 μm REVEAL CLUSTERING OF STAR-FORMING GALAXIES
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BLAST: CORRELATIONS IN THE COSMIC FAR-INFRARED BACKGROUND AT 250, 350, AND 500 μm REVEAL CLUSTERING OF STAR-FORMING GALAXIES

机译:爆炸:星系星系在250、350和500μm的宇宙远红外背景下的相关性

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We detect correlations in the cosmic far-infrared background due to the clustering of star-forming galaxies in observations made with the Balloon-borne Large Aperture Submillimeter Telescope, at 250, 350, and 500 μm. We perform jackknife and other tests to confirm the reality of the signal. The measured correlations are well fitted by a power law over scales of 5'-25', with ΔI/I = 15.1% ± 1.7%. We adopt a specific model for submillimeter sources in which the contribution to clustering comes from sources in the redshift ranges 1.3 ≤ z ≤ 2.2, 1.5 ≤ z ≤ 2.7, and 1.7 ≤ z ≤ 3.2, at 250, 350, and 500 μm, respectively. With these distributions, our measurement of the power spectrum, P(k θ), corresponds to linear bias parameters, b = 3.8 ± 0.6, 3.9 ± 0.6, and 4.4 ± 0.7, respectively. We further interpret the results in terms of the halo model, and find that at the smaller scales, the simplest halo model fails to fit our results. One way to improve the fit is to increase the radius at which dark matter halos are artificially truncated in the model, which is equivalent to having some star-forming galaxies at z ≥ 1 located in the outskirts of groups and clusters. In the context of this model, we find a minimum halo mass required to host a galaxy is log(M min/M ☉) = 11.5+0.4 –0.1, and we derive effective biases b eff = 2.2 ± 0.2, 2.4 ± 0.2, and 2.6 ± 0.2, and effective masses , 12.8 ± 0.2, and 12.7 ± 0.2, at 250, 350 and 500 μm, corresponding to spatial correlation lengths of r 0 = 4.9, 5.0, and , respectively. Finally, we discuss implications for clustering measurement strategies with Herschel and Planck.
机译:在250、350和500μm的气球载大孔径亚毫米望远镜进行的观测中,我们检测到由于形成恒星的星系团簇而在宇宙远红外背景下的相关性。我们执行折刀和其他测试以确认信号的真实性。幂律在5'-25'的尺度上很好地拟合了测得的相关性,ΔI/ I = 15.1%±1.7%。对于亚毫米波源,我们采用一种特定的模型,其中对聚类的贡献分别来自于250,350和500μm的红移范围1.3≤z≤2.2、1.5≤z≤2.7和1.7≤z≤3.2。 。利用这些分布,我们对功率谱的测量值P(kθ)分别对应于线性偏置参数b = 3.8±0.6、3.9±0.6和4.4±0.7。我们进一步根据光环模型来解释结果,并发现在较小的规模上,最简单的光环模型无法满足我们的结果。改善拟合度的一种方法是增加模型中暗物质晕圈被人为截断的半径,这等效于在群和星团的郊区有z≥1的一些恒星形成星系。在此模型的背景下,我们发现容纳一个星系所需的最小晕质量为log(M min / M☉)= 11.5 + 0.4 –0.1,并且得出有效偏差b eff = 2.2±0.2、2.4±0.2,分别为250、350和500μm时的2.6±0.2和有效质量12.8±0.2和12.7±0.2,分别对应于r 0 = 4.9、5.0和的空间相关长度。最后,我们与Herschel和Planck讨论了对度量策略进行聚类的含义。
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