Deep-MOND polytropes

نویسندگان

چکیده

Working within the deep-MOND limit (DML), I describe spherical, self-gravitating systems governed by a polytropic equation of state, $P=\mathcal{K}\rho^\gamma$. As self-consistent structures, such can serve as heuristic models for DML, astronomical systems, dwarf spheroidal galaxies, low-surface-density elliptical galaxies and star clusters, diffuse galaxy groups. They also testing ground various theoretical MOND inferences. In dimensionless form, satisfied radial density profile $\zeta(y)$ is (for $\gamma\not=1$) $[\int_0^y \zeta \bar y^2 d\bar y]^{1/2}=-yd(\zeta^{\gamma-1})/dy$. Or, $\theta^n(y)=y^{-2}[(y\theta')^2]'$, where $\theta=\zeta^{\gamma-1}$, $n\equiv (\gamma-1)^{-1}$. discuss properties solutions, contrasting them with those their Newtonian analogues -- Lane-Emden polytropes. Due to stronger gravity, all DML polytropes have finite mass, $n<\infty$ ($\gamma>1$) radius. (Lane-Emden spheres mass only $n\le 5$.) use study scaling relations. For example, they satisfy universal relation $\mathcal{K}$ $\gamma$) between total $M$, mass-average velocity dispersion $\sigma$: $MGa_0=(9/4)\sigma^4$. However, $M$ other measures dispersion, central, projected one, $\bar\sigma$, does depend on $n$ (but not $\mathcal{K}$), defining `fundamental surface' in $[M,~\bar\sigma,~n]$ space. generalization anisotropic polytropes, which radius $\gamma>1$), above $M-\sigma$ relation. This more extended class exhibits central-surface-densities relation: tight baryonic dynamical central surface densities predicted MOND.

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ژورنال

عنوان ژورنال: Physical review

سال: 2021

ISSN: ['0556-2813', '1538-4497', '1089-490X']

DOI: https://doi.org/10.1103/physrevd.103.044043