4.7 Article

Ultralight scalars as cosmological dark matter

Journal

PHYSICAL REVIEW D
Volume 95, Issue 4, Pages -

Publisher

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevD.95.043541

Keywords

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Funding

  1. National Aeronautics and Space Administration [NNX14AM24G, NXX16AB27G]
  2. National Science Foundation [AST-1406166, PHY-1606531]
  3. Department of Energy [DE-SC0011941]

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Many aspects of the large-scale structure of the Universe can be described successfully using cosmological models in which 27 +/- 1% of the critical mass-energy density consists of cold dark matter (CDM). However, few-if any-of the predictions of CDM models have been successful on scales of similar to 10 kpc or less. This lack of success is usually explained by the difficulty of modeling baryonic physics (star formation, supernova and black-hole feedback, etc.). An intriguing alternative to CDM is that the dark matter is an extremely light (m similar to 10(-22) eV) boson having a de Broglie wavelength lambda similar to 1 kpc, often called fuzzy dark matter (FDM). We describe the arguments from particle physics that motivate FDM, review previous work on its astrophysical signatures, and analyze several unexplored aspects of its behavior. In particular, (i) FDM halos or subhalos smaller than about 10(7) (m/10(-22) eV)(-3/2) M-circle dot do not form, and the abundance of halos smaller than a few times 10(10) (m/10(-22) eV)(-4/3) M-circle dot is substantially smaller in FDM than in CDM. (ii) FDM halos are comprised of a central core that is a stationary, minimum-energy solution of the Schrodinger-Poisson equation, sometimes called a soliton, surrounded by an envelope that resembles a CDM halo. The soliton can produce a distinct signature in the rotation curves of FDM-dominated systems. (iii) The transition between soliton and envelope is determined by a relaxation process analogous to two-body relaxation in gravitating N-body systems, which proceeds as if the halo were composed of particles with mass similar to rho lambda(3) where rho is the halo density. (iv) Relaxation may have substantial effects on the stellar disk and bulge in the inner parts of disk galaxies, but has negligible effect on disk thickening or globular cluster disruption near the solar radius. (v) Relaxation can produce FDM disks but a FDM disk in the solar neighborhood must have a halfthickness of at least similar to 300(m/10(-22) eV)(-2/3) pc and a midplane density less than 0.2(m/10(-22) eV)(2/3) times the baryonic disk density. (vi) Solitonic FDM subhalos evaporate by tunneling through the tidal radius and this limits the minimum subhalo mass inside similar to 30 kpc of the Milky Way to a few times 10(8)(m/10(-22) eV)(-3/2) M-circle dot. (vii) If the dark matter in the Fornax dwarf galaxy is composed of CDM, most of the globular clusters observed in that galaxy should have long ago spiraled to its center, and this problem is resolved if the dark matter is FDM. (viii) FDM delays galaxy formation relative to CDM but its galaxy-formation history is consistent with current observations of high-redshift galaxies and the late reionization observed by Planck. If the dark matter is composed of FDM, most observations favor a particle mass greater than or similar to 10(-22) eV and the most significant observational consequences occur if the mass is in the range 1-10 x 10(-22) eV. There is tension with observations of the Lyman-alpha forest, which favor m greater than or similar to 10-20 x 10(-22) eV and we discuss whether more sophisticated models of reionization may resolve this tension.

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