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首页> 外文期刊>The Astrophysical journal >GRAVITATIONAL LENSING BY A CLUSTER OF GALAXIES AND THE CENTRAL cD GALAXY: MEASURING THE MASS PROFILE
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GRAVITATIONAL LENSING BY A CLUSTER OF GALAXIES AND THE CENTRAL cD GALAXY: MEASURING THE MASS PROFILE

机译:星系群和中央cd银河系的引力透镜:测量质量轮廓

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We study the constraints on the density profile of the mass in a cluster of galaxies that can be obtained when a radial arc produced by gravitational lensing is observed. We apply this to the cluster MS 2137 — 23, which contains a radial arc, a tangential arc, and three other arclets. As shown by Mellier and coworkers, the positions and elongations of all these five images are well reproduced as arising from two different background galaxies, if the mass distribution in the cluster is elliptical, is exactly centered on the brightest cluster galaxy, and has the same ellipticity and position angle as this galaxy. The galaxy is therefore identified as the center of the cluster potential well. We show that the ratio θ_r/θ_i of the distance from the radial arc to the center of the cluster to the distance from the other image of the same source to the center gives a powerful constraint on the form of the dark matter density profile. Models that are favored have well-defined core radii of ~30 h~(-1) kpc, with the slope changing rapidly from almost flat to roughly isothermal around this radius. Density profiles that remain steeper than r~(-1) all the way to the center are probably ruled out, since they predict θ_r/θ_i to be smaller than observed. We also show that θ_r/θ_i is significantly affected by the mass in stars in the central galaxy. The stellar mass tends to move the radial arc closer to the center, since its profile is very steep. This implies an upper limit to the mass-to-light ratio of the stars, similar to the dynamical measurements of the mass-to-light ratio of elliptical galaxies. The constraints on the profile will be improved once the position of the radial arc is measured more accurately and the arc redshifts are determined. All the models for the density profile that are consistent with the observed position of the radial arc predict a velocity dispersion for the cluster galaxies of ~1200 km s~(-1) and a central velocity dispersion for the stars of ~350 km s~(-1), consistent with the observed velocity dispersions in other cD galaxies. The models also predict that the velocity dispersion of the cD halo should rise rapidly with radius and that the two sources producing the five arcs should be at similar redshifts. This can be tested by future observations.
机译:我们研究了星团簇中质量密度分布的约束条件,当观察到引力透镜产生的径向弧时可以获得这些约束。我们将其应用于群集MS 2137-23,该群集包含一个径向弧,一个切向弧和其他三个小弧。如梅利尔(Mellier)和他的同事所显示的,如果群集中的质量分布为椭圆形,正好位于最亮的群集星系上并且具有相同的质量,则这五个图像的位置和伸长率都可以很好地复制,这是由于两个不同的背景星系引起的椭圆度和位置角就是这个星系。因此,银河系被确定为团簇势阱的中心。我们表明,从径向弧到星团中心的距离与从同一源的另一个图像到中心的距离的比值θ_r/θ_i对暗物质密度分布图的形式给出了强有力的约束。首选的模型具有约30 h〜(-1)kpc的明确定义的核心半径,并且在该半径附近,坡度从几乎平坦变为大致等温。可以排除一直到中心比r〜(-1)陡峭的密度分布,因为它们预测θ_r/θ_i小于观测值。我们还表明,θ_r/θ_i受到中心星系中恒星质量的显着影响。由于其轮廓非常陡峭,恒星质量倾向于使径向弧更靠近中心。这意味着恒星的质光比有一个上限,类似于对椭圆星系质光比的动态测量。一旦更精确地测量了径向电弧的位置并确定了电弧的红移,轮廓上的约束条件将得到改善。所有与径向弧观测位置一致的密度分布模型都预测了〜1200 km s〜(-1)的星团星系的速度色散和〜350 km s〜的恒星的中心速度色散(-1),与在其他cD星系中观察到的速度色散一致。该模型还预测,cD光晕的速度色散应随半径迅速增加,并且产生五个弧的两个源应处于相似的红移。这可以通过将来的观察进行检验。

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