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Chandra Observations of Galaxy Cluster A2218

机译:钱德拉对星系团A2218的观察

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We present results from two observations (combined exposure of ~17 ks) of galaxy cluster A2218 using the Advanced CCD Imaging Spectrometer on board the Chandra X-Ray Observatory that were taken on 1999 October 19. Using a Raymond-Smith single-temperature plasma model corrected for galactic absorption, we find a mean cluster temperature of kT = 6.9 ± 0.5 keV, metallicity of 0.20 ± 0.13 (errors are 90% CL), and a rest-frame luminosity in the 2-10 keV energy band of 6.2 × 1044 ergs s-1 within a 51 aperture in a Λ cold dark matter cosmology (ΛCDM) with H0 = 65 km s-1 Mpc-1. The brightness distribution within 42 of the cluster center is well fitted by a simple spherical beta model with core radius of 664 and β = 0.705. High-resolution Chandra data of the inner 2' of the cluster show the X-ray brightness centroid displaced ~22'' from the dominant cD galaxy and the presence of azimuthally asymmetric temperature variations along the direction of the cluster mass elongation. X-ray and weak lensing mass estimates are in good agreement for the outer parts (r 200 h-1) of the cluster; however, in the core the observed temperature distribution cannot reconcile the X-ray and strong lensing mass estimates in any model in which the intracluster gas is in thermal hydrostatic equilibrium. Our X-ray data are consistent with a scenario in which A2218 is not in hydrostatic equilibrium because of recent merger activity that has produced significant nonthermal pressure in the core and substructure along the line of sight; each of these phenomena probably contributes to the difference between lensing and X-ray core mass estimates.
机译:我们介绍了1999年10月19日使用钱德拉X射线天文台上的先进CCD成像光谱仪对星系团A2218进行的两次观测(约17 ks的联合曝光)的结果。校正银河吸收后,我们发现平均团簇温度为kT = 6.9±0.5 keV,金属度为0.20±0.13(误差为90%CL),在2-10 keV能带中的静止帧亮度为6.2×1044 erg s-1在H0 = 65 km s-1 Mpc-1的Λ冷暗物质宇宙学(ΛCDM)的51孔径内。一个简单的球贝塔模型可以很好地拟合聚类中心42内的亮度分布,球心半径为664,β= 0.705。团簇内部2'的高分辨率Chandra数据显示,X射线亮度重心偏离了优势cD星系〜22'',并且沿团簇质量延伸的方向存在方位角不对称的温度变化。对于星团的外部​​(r> 200 h-1),X射线和微弱的透镜质量估计值非常吻合;但是,在任何簇内气体处于热流体静力平衡的模型中,在岩心中观察到的温度分布都无法使X射线和强大的透镜质量估计值协调一致。我们的X射线数据与A2218处于静水平衡状态的情况是一致的,因为最近的合并活动沿视线在核心和子结构中产生了很大的非热压力。这些现象中的每一个都可能导致透镜和X射线核心质量估计之间的差异。

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