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首页> 外文期刊>The Astrophysical journal >MEASURING THE REDSHIFT DEPENDENCE OF THE COSMIC MICROWAVE BACKGROUND MONOPOLE TEMPERATURE WITH PLANCK DATA
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MEASURING THE REDSHIFT DEPENDENCE OF THE COSMIC MICROWAVE BACKGROUND MONOPOLE TEMPERATURE WITH PLANCK DATA

机译:用普朗克数据测量宇宙微波背景单极温度的降低依赖性。

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We study the capability of Planck data to constrain deviations of the cosmic microwave background (CMB) blackbody temperature from adiabatic evolution using the thermal Sunyaev-Zeldovich anisotropy induced by clusters of galaxies. We consider two types of data sets depending on how the cosmological signal is removed: using a CMB template or using the 217?GHz map. We apply two different statistical estimators, based on the ratio of temperature anisotropies at two different frequencies and on a fit to the spectral variation of the cluster signal with frequency. The ratio method is biased if CMB residuals with amplitude ~1 μK or larger are present in the data, while residuals are not so critical for the fit method. To test for systematics, we construct a template from clusters drawn from a hydro-simulation included in the pre-launch Planck Sky Model. We demonstrate that, using a proprietary catalog of X-ray-selected clusters with measured redshifts, electron densities, and X-ray temperatures, we can constrain deviations of adiabatic evolution, measured by the parameter α in the redshift scaling T(z) = T 0(1 + z)1 – α, with an accuracy of σα = 0.011 in the most optimal case and with σα = 0.018 for a less optimal case. These results represent a factor of 2-3 improvement over similar measurements carried out using quasar spectral lines and a factor 6-20 with respect to earlier results using smaller cluster samples.
机译:我们使用星系团引起的热Sunyaev-Zeldovich各向异性研究了普朗克数据约束绝热演化产生的宇宙微波背景(CMB)黑体温度偏差的能力。根据如何删除宇宙信号,我们考虑两种类型的数据集:使用CMB模板或使用217?GHz映射。我们基于两个不同频率上的温度各向异性之比,并根据群集信号随频率变化的频谱变化,应用两个不同的统计估计量。如果数据中存在振幅〜1μK或更大的CMB残差,则比率方法会有偏差,而残差对于拟合方法不是那么关键。为了测试系统性,我们从预启动的普朗克天空模型中包含的水力模拟中提取的簇构建了模板。我们证明,使用专有的X射线选择簇的目录,该簇具有测得的红移,电子密度和X射线温度,我们可以限制绝热演变的偏差,该偏差由红移缩放比例T(z)=中的参数α测得T 0(1 + z)1 –α,在最佳情况下,精度为σα= 0.011,在次佳情况下,精度为σα= 0.018。这些结果表示,与使用类星体光谱线进行的类似测量相比,提高了2-3倍,而与使用较小簇样本的早期结果相比,则提高了6-20倍。

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