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| Query : 2001MNRAS.326..164O |
2001MNRAS.326..164O - Mon. Not. R. Astron. Soc., 326, 164-180 (2001/September-1)
Luminous and dark matter in the Milky Way.
OLLING R.P. and MERRIFIELD M.R.
Abstract (from CDS):
Thus, if R0 is larger than ∼7kpc, or θ0≳170km.s–1, we can rule out two dark matter candidates that require a highly flattened dark matter halo: (1) decaying massive neutrinos, and (2) a disc of cold molecular hydrogen.
It is possible to construct a self-consistent axisymmetric model of the Galaxy based on the IAU-recommended values for the Galactic constants (R0=8.5kpc, θ0=220km.s–1) only in the unlikely case that the effective gaseous velocity dispersion is ∼19 per cent larger than observed, and if the local stellar column density is less than about 18M☉pc–2. If we assume that the halo is oblate and a value of Σ∗ of 35±5M☉pc–2, we can rule out Galactic models with R0≳8.0kpc and θ0≳200km.s–1.
Combining the best kinematical and star-count estimates of Σ∗, we conclude that Σ∗ probably lies between 25 and 45M☉pc–2. We find that Kuijken & Gilmore's determination of the column density of matter within 1.1kpc of the plane is robust and valid over a wide range of Galactic constants.
Our mass models show that, largely owing to the uncertainty in the Galactic light distribution, the dark matter density in the Galactic Centre is uncertain by up to three orders of magnitude. In the solar neighbourhood this uncertainty is much reduced: our models imply a dark matter density of some 0.42GeV/c2 per cubic centimetre, or (11±5)mM☉pc–3 - roughly 15 per cent of the total mass density.
Abstract Copyright: The Royal Astronomical Society
Journal keyword(s): Galaxy: fundamental parameters - Galaxy: kinematics and dynamics - solar neighbourhood - Galaxy: stellar content - Galaxy: structure
Simbad objects: 2
| Number of rows : 2 |
| N | Identifier | Otype |
ICRS (J2000) RA |
ICRS (J2000) DEC |
Mag U | Mag B | Mag V | Mag R | Mag I | Sp type |
#ref
1850 - 2026 |
#notes |
|---|---|---|---|---|---|---|---|---|---|---|---|---|
| 1 | NGC 891 | H2G | 02 22 32.907 | +42 20 53.95 | 11.08 | 10.81 | 9.93 | 7.86 | ~ | 1741 | 2 | |
| 2 | NGC 4565 | Sy2 | 12 36 20.804 | +25 59 14.61 | 13.61 | 12.43 | ~ | 991 | 0 |
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