Does the galaxy NGC1052–DF2 falsify Milgromian dynamics?
Does the galaxy NGC1052–DF2 falsify Milgromian dynamics?
复制标题
NGC1052-DF2 星系是否伪造了米尔格罗米亚动力学?
DOI:
10.1038/s41586-018-0429-z
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发表时间:
2018
期刊:
影响因子:
64.8
通讯作者:
Jörg Dabringhausen
中科院分区:
文献类型:
--
作者:
Pavel Kroupa;Hosein Haghi;Behnam Javanmardi;Akram Hasani Zonoozi;Oliver Müller;Indranil Banik;Xufen Wu;Hongsheng Zhao;Jörg Dabringhausen
A great challenge in current physics is to understand whether the observed internal dynamics of galaxies is due to dark matter or to a modification of the law of gravity. Recently, van Dokkum et al. 1 reported that the ultra-diffuse dwarf galaxy NGC1052–DF2 lacks dark matter, and they claimed that this would—paradoxically—be problematic for modified gravity theories such as Milgromian dynamics (MOND) 2, 3. However, NGC1052–DF2 is not isolated, so a valid prediction of its internal dynamics in MOND cannot be made without properly accounting for the external gravitational fields from neighbouring galaxies. Including this external field effect, following Haghi et al. 4, shows that NGC1052–DF2 is consistent with MOND. In any viable cosmological model, both primordial and tidal dwarf galaxies, which form in gas-rich tidal debris when galaxies interact, should exist. Within the standard dark-matter-based cosmological model, primordial dwarfs are dark-matter-dominated, whereas tidal dwarf galaxies contain very little (if any) dark matter 5. In MOND—a classical potential theory of gravity, derivable from a Lagrangian with conserved energy, total momentum and angular momentum 2, 6—the two types of dwarf galaxies cannot be distinguished. Until now, all known dwarf galaxies have shown similar dynamic behaviour, possibly implying falsification of the dark-matter models 7. The discovery by van Dokkum et al. 1 of a galaxy lacking dark matter would thus constitute an important verification of the standard dark-matter cosmological model. Given the density distribution of baryonic matter, ρ, the gravitational potential of Milgromian gravitation, φ, is determined by the generalized nonlinear Poisson equation 6∣∣ µ φ φ ρ∇∇∇⋅/= π a G [()] 4