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Distribution function of dark matter with constant anisotropy

机译:具有恒定各向异性的暗物质的分布函数

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摘要

N-body simulations of dark matter halos show that the density is cusped near the center of the halo. The density pro. le behaves as r(-gamma). in the inner parts, where gamma similar or equal to 1 for the NFW model and gamma similar or equal to 1.5 for the Moore model, but in the outer parts the two models agree with each other in the asymptotic behavior of the density profile. The simulations also show information about the anisotropy parameter beta(r) of the velocity distribution: beta approximate to 0 in the inner part and beta approximate to 0.5 (radially anisotropic) in the outer part of the halo. We provide some distribution functions F(E, L) with the constant anisotropy parameter beta for the two spherical models of dark matter halos: a new generalized NFW model and a generalized Moore model. There are two parameters alpha and epsilon for those two generalized models to determine the asymptotic behavior of the density pro. le. In this paper, we concentrate on the situation of beta(r) = 1/2 from the viewpoint of the simulation.
机译:暗物质晕的N体模拟显示密度在晕中心附近被限制。密度pro。 le表现为r(-gamma)。在内部,其中NFW模型的gamma值等于或等于1,而对于Moore模型的gamma值等于或等于1.5,但是在外部,两个模型在密度分布的渐近行为上彼此一致。模拟还显示了有关速度分布的各向异性参数beta(r)的信息:β的内部晕圈近似为0,β的外部晕圈近似为0.5(径向各向异性)。我们为暗物质晕的两个球形模型:新的广义NFW模型和广义的Moore模型提供了具有恒定各向异性参数β的分布函数F(E,L)。对于这两个广义模型,有两个参数alpha和epsilon可以确定密度pro的渐近行为。乐在本文中,我们从仿真的角度着眼于beta(r)= 1/2的情况。

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