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arXiv 2402.07159astro-ph.GAgr-qchep-ph
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一般MOND理论中的中心面密度关联

Central-surface-densities correlation in general MOND theories

Mordehai Milgrom

AI总结:

本文证明MOND基础公理可预言重子面密度与动力学面密度之间的强关联,并在更广泛的MOND理论中考察中心面密度的更紧密关系,提出用加速度积分作为中心动力学面密度的代理量。

摘要:

本文表明,仅凭MOND的基础公理即可预言孤立天体(如星系)的重子面密度体度量$Σ_B$与相应的动力学面密度$Σ_D$之间存在强关联。该关联由其高$Σ_B$和低$Σ_B$行为所概括。当$Σ_B\ggΣ_M\equiv a_0/2πG$($Σ_M$为临界MOND面密度)时,有$Σ_D\approxΣ_B$。二者之差——通常会被解释为暗物质的贡献——为$Σ_P=Σ_D-Σ_B\simΣ_M\llΣ_B$。在深MOND极限$Σ_B\llΣ_M$下,有$Σ_D\sim (Σ_MΣ_B)^{1/2}$。这是MOND的一个基本预言,所有体现其基本宗旨的理论都共享这一预言。在具体的MOND理论中,对于特定类别的质量分布——例如纯盘或球对称系统——以及对面密度的特定定义,可以预言更清晰的关联,甚至是严格的代数关系$Σ_D(Σ_B)$。接着,我讨论了轴对称星系系统中心面密度$Σ^0_B$和$Σ^0_D$的这种更紧密关联。过去的工作已在AQUAL和QUMOND理论中证明了纯盘的此类关系。本文中,我在更广泛的MOND理论类别中考察这些关系。对于大多数观测系统,目前无法直接确定$Σ^0_D$,但在许多情况下,加速度积分$\mathcal{G}\equiv\int_0^\infty g_r d\ln~r$是它的一个良好代理量,其中$g_r$是沿系统反射对称平面(如盘星系)的径向加速度。$\mathcal{G}$可以直接由旋转曲线确定。我讨论了$\mathcal{G}$在多大程度上是$Σ^0_D$的良好代理量,以及二者之间的关系如何依赖于系统几何,从纯盘、盘加核球系统,到准球对称系统。

英文摘要:

It is shown that the foundational axioms of MOND alone predict a strong correlation between a bulk measure of the baryonic surface density, $Σ_B$, and the corresponding dynamical one, $Σ_D$, of an isolated object, such as a galaxy. The correlation is encapsulated by its high- and low-$Σ_B$ behaviors. For $Σ_B\ggΣ_M\equiv a_0/2πG$ ($Σ_M$ is the critical MOND surface density) one has $Σ_D\approxΣ_B$. Their difference -- which would be interpreted as the contribution of dark matter -- is $Σ_P=Σ_D-Σ_B\simΣ_M\llΣ_B$. In the deep-MOND limit, $Σ_B\llΣ_M$, one has $Σ_D\sim (Σ_MΣ_B)^{1/2}$. This is a primary prediction of MOND, shared by all theories that embody its basic tenets. Sharper correlations, even strict algebraic relations, $Σ_D(Σ_B)$, are predicted in specific MOND theories, for specific classes of mass distribution -- e.g., pure discs, or spherical systems -- and for specific definitions of the surface densities. I proceed to discuss such tighter correlations for the central surface densities of axisymmetric galactic systems, $Σ^0_B$ and $Σ^0_D$. Past work has demonstrated such relations for pure discs in the AQUAL and QUMOND theories. Here I consider them in broader classes of MOND theories. For most observed systems, $Σ^0_D$ can not be determined directly at present, but, in many cases, a good proxy for it is the acceleration integral $\mathcal{G}\equiv\int_0^\infty g_r d\ln~r$, where $g_r$ is the radial acceleration along a reflection-symmetry plane of a system, such as a disc galaxy. $\mathcal{G}$ can be determined directly from the rotation curve. I discuss the extent to which $\mathcal{G}$ is a good proxy for $Σ^0_D$, and how the relation between them depends on system geometry, from pure discs, through disc-plus-bulge ones, to quasi-spherical systems.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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