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arXiv 1111.0290astro-ph.COgr-qchep-phhep-th
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暖暗物质涨落的宇宙学演化I:基于Volterra积分方程的有效计算框架

Cosmological evolution of warm dark matter fluctuations I: Efficient computational framework with Volterra integral equations

H. J. de Vega, N. G. Sanchez

摘要:

本文研究了在辐射占优时期,即keV尺度暖暗物质(WDM)的情况下,超相对论性解耦的暗物质(DM)密度涨落的完整宇宙学演化。这里提出的新框架可以应用于其他类型的DM,特别是我们将其扩展到冷DM(CDM)。在各向异性应力作用下,详细研究了光子存在下WDM和中微子的无碰撞线性化Boltzmann-Vlasov方程(B-V)与线性化Einstein方程的耦合,其中牛顿势一般不同于空间曲率扰动.我们重铸DM和中微子的B-V方程的完整系统耦合Volterra积分方程的系统。这些Volterra型方程在辐射主导(RD)和物质主导(MD)时代都是有效的,在此期间WDM粒子是超相对论的,然后是非相对论的。这推广了所谓的吉尔伯特积分方程,该方程仅适用于MD时代的非相对论粒子。我们成功地减少到只有两个耦合的Volterra方程组的DM和中微子的密度和各向异性应力起伏的四个Volterra积分方程的系统。这些方程中的核和非齐次性是显式给定的函数。结合Boltzmann-Vlasov方程和线性化的Einstein方程,对分布函数和引力势的初始条件进行了约束。在没有中微子的情况下,各向异性应力消失,Volterra型方程减少到一个单一的积分方程。这些Volterra积分方程提供了一个有用的和精确的框架来计算原始WDM波动在很宽的尺度范围内,包括小尺度到k ~ 1/5 kpc。

英文摘要:

We study the complete cosmological evolution of dark matter (DM) density fluctuations for DM particles that decoupled being ultrarelativistic during the radiation dominated era which is the case of keV scale warm DM (WDM). The new framework presented here can be applied to other types of DM and in particular we extend it to cold DM (CDM). The collisionless and linearized Boltzmann-Vlasov equations (B-V) for WDM and neutrinos in the presence of photons and coupled to the linearized Einstein equations are studied in detail in the presence of anisotropic stress with the Newtonian potential generically different from the spatial curvature perturbations. We recast this full system of B-V equations for DM and neutrinos into a system of coupled Volterra integral equations. These Volterra-type equations are valid both in the radiation dominated (RD) and matter dominated (MD) eras during which the WDM particles are ultrarelativistic and then nonrelativistic. This generalizes the so-called Gilbert integral equation only valid for nonrelativistic particles in the MD era. We succeed to reduce the system of four Volterra integral equations for the density and anisotropic stress fluctuations of DM and neutrinos into a system of only two coupled Volterra equations. The kernels and inhomogeneities in these equations are explicitly given functions. Combining the Boltzmann-Vlasov equations and the linearized Einstein equations constrain the initial conditions on the distribution functions and gravitational potentials. In the absence of neutrinos the anisotropic stress vanishes and the Volterra-type equations reduce to a single integral equation. These Volterra integral equations provide a useful and precise framework to compute the primordial WDM fluctuations over a wide range of scales including small scales up to k ~ 1/5 kpc.

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