Cuspy halo problem

The cuspy halo problem (also known as the core-cusp problem) is a discrepancy between the inferred dark matter density profiles of low-mass galaxies and the density profiles predicted by cosmological N-body simulations. Nearly all simulations form dark matter halos which have "cuspy" dark matter distributions, with density increasing steeply at small radii, while the rotation curves of most observed dwarf galaxies suggest that they have flat central dark matter density profiles ("cores").[1][2]

Several possible solutions to the core-cusp problem have been proposed. Many recent studies have shown that including baryonic feedback (particularly feedback from supernovae and active galactic nuclei) can "flatten out" the core of a galaxy's dark matter profile, since feedback-driven gas outflows produce a time-varying gravitational potential that transfers energy to the orbits of the collisionless dark matter particles.[3][4] Other works have shown that the core-cusp problem can be solved outside of the most widely accepted Cold Dark Matter (CDM) paradigm: simulations with warm or self-interacting dark matter also produce dark matter cores in low-mass galaxies.[5][6] It is also possible that the distribution of dark matter that minimizes the system energy has a flat central dark matter density profile.[7]

  1. ^ Moore, Ben; et al. (August 1994). "Evidence against dissipation-less dark matter from observations of galaxy haloes". Nature. 370 (6491): 629–631. Bibcode:1994Natur.370..629M. doi:10.1038/370629a0. S2CID 4325561.
  2. ^ Oh, Se-Heon; et al. (May 2015). "High-resolution Mass Models of Dwarf Galaxies from LITTLE THINGS". The Astronomical Journal. 149 (6): 180. arXiv:1502.01281. Bibcode:2015AJ....149..180O. doi:10.1088/0004-6256/149/6/180. S2CID 1389457.
  3. ^ Navarro, Julio; et al. (December 1996). "The cores of dwarf galaxy haloes". MNRAS. 283 (3): L72 – L78. arXiv:astro-ph/9610187. Bibcode:1996MNRAS.283L..72N. doi:10.1093/mnras/283.3.l72.
  4. ^ Pontzen, Andrew; et al. (2012). "How supernova feedback turns dark matter cusps into cores". Nature. 421 (4): 3464–3471. arXiv:1106.0499. Bibcode:2012MNRAS.421.3464P. doi:10.1111/j.1365-2966.2012.20571.x. S2CID 26992856.
  5. ^ Lovell, Mark; et al. (March 2012). "The haloes of bright satellite galaxies in a warm dark matter universe". MNRAS. 420 (3): 2318–2324. arXiv:1104.2929. Bibcode:2012MNRAS.420.2318L. doi:10.1111/j.1365-2966.2011.20200.x. S2CID 53698295.
  6. ^ Elbert, Oliver; et al. (October 2015). "Core formation in dwarf haloes with self-interacting dark matter: no fine-tuning necessary". MNRAS. 453 (1): 29–37. arXiv:1412.1477. Bibcode:2015MNRAS.453...29E. doi:10.1093/mnras/stv1470.
  7. ^ Runstedtler, Allan (November 2018). "A model for the mass and distribution of particles in dark matter halos". Canadian Journal of Physics. 96 (11): 1178–1182. Bibcode:2018CaJPh..96.1178R. doi:10.1139/cjp-2017-0804. ISSN 0008-4204. S2CID 125555275.

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