4.7 Article

Cuspy dark matter density profiles in massive dwarf galaxies

期刊

出版社

OXFORD UNIV PRESS
DOI: 10.1093/mnras/stac588

关键词

galaxies: dwarf; galaxies: ISM; galaxies: kinematics and dynamics; dark matter

资金

  1. National Science Foundation (NSF) through Student Observing Support Program (SOSP) award from the NRAO [7-011]
  2. NSF Astronomy and Astrophysics Postdoctoral Fellowship [AST-2102625]
  3. Graduate Resources Advancing Diversity with Maryland Astronomy and Physics (GRAD-MAP) program - University of Maryland College of Computer, Mathematical, and Natural Sciences
  4. Departments of Astronomy and Physics
  5. NSF [1545949, AST-1615960]
  6. ANID-FULBRIGHT [BIO 2016-56160020]
  7. NRAO through SOSP award [SOSPA7-014]
  8. National Aeronautics and Space Administration [NNX08AR22G]
  9. National Science Foundation [AST-1238877]
  10. [NSF-AST2108140]

向作者/读者索取更多资源

Rotation curves of spiral dwarf galaxies were examined using ALMA, and it was found that these relatively massive dwarfs have steeper dark matter density profiles than predicted by simulations. This suggests the possibility of stronger gas inflows, overestimate of accretion or feedback events in the simulations, or a combination of these effects.
Rotation curves of galaxies probe their total mass distributions, including dark matter. Dwarf galaxies are excellent systems to investigate the dark matter density distribution, as they tend to have larger fractions of dark matter compared to higher mass systems. The core-cusp problem describes the discrepancy found in the slope of the dark matter density profile in the centres of galaxies (beta*) between observations of dwarf galaxies (shallower cores) and dark matter-only simulations (steeper cusps). We investigate beta* in six nearby spiral dwarf galaxies for which high-resolution CO J = 1-0 data were obtained with ALMA (Atacama Large Millimeter/submillimeter Array). We derive rotation curves and decompose the mass profile of the dark matter using our CO rotation curves as a tracer of the total potential and 4.5 mu m photometry to define the stellar mass distribution. We find = 0.6 with a standard deviation of +/- 0.1 among the galaxies in this sample, in agreement with previous measurements in this mass range. The galaxies studied are on the high stellar mass end of dwarf galaxies and have cuspier profiles than lower mass dwarfs, in agreement with other observations. When the same definition of the slope is used, we observe steeper slopes than predicted by the FIRE and NIHAO simulations. This may signal that these relatively massive dwarfs underwent stronger gas inflows towards their centres than predicted by these simulations, that these simulations overpredict the frequency of accretion or feedback events, or that a combination of these or other effects are at work.

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