The nature of dark matter
Dark matter is one of the major unresolved questions in
modern physics. It cannot be observed directly through ordinary electromagnetic
radiation, yet its gravitational influence is evident in the motion of stars
and galaxies, gravitational lensing, galaxy clusters, and the large-scale
structure of the Universe.
Among these observations, galactic rotation provides one of
the simplest ways to understand the problem. The argument requires only basic
Newtonian gravity: if the motion of an object is known, that motion can be used
to infer the mass responsible for the gravitational field.
Consider a star orbiting a galaxy at a distance r from its centre. For an approximately circular orbit, its orbital velocity is given by:
where G is the gravitational constant and M is the mass
enclosed within the star's orbit. Rearranging,
This relationship provides a direct connection between the observed motion of stars and the gravitational mass of a galaxy. The same gravitational reasoning can also be expressed through escape velocity,
In both cases, the important point is the same:
gravitational motion provides information about mass, including mass that
cannot be seen directly.
The problem with galactic rotation
If the visible matter of a galaxy contained essentially all
of its mass, the orbital velocity of stars should generally decrease with
increasing distance from the galactic centre. Once the enclosed mass becomes
approximately constant,
Thus, the outer regions of a galaxy should exhibit
progressively lower orbital velocities.
Observations of spiral galaxies, however, show a different
behaviour. Their rotation curves often remain approximately flat over
substantial radial distances. Stars and gas in the outer regions continue to
orbit at velocities that are higher than expected from the distribution of
visible matter alone.
The conventional interpretation is that galaxies contain an
additional, non-luminous component known as dark matter.
Figure 1. Galactic rotation curve of the Andromeda Galaxy (M31) comparing predicted velocities based on visible matter with observed velocities (Rubin & Ford, 1970).
The Milky Way as a case study
The Milky Way provides an especially useful example because
its stellar motions can be studied in considerable detail. The European Space
Agency's Gaia mission has provided extensive astrometric data that allow the
kinematics of our Galaxy to be investigated with much greater precision.
Cautun et al. (2020) used the Galactic rotation curve from
Gaia DR2, together with other observational constraints, to construct a
physically motivated model of the Milky Way's mass distribution. Their
preferred model includes the stellar and gaseous components of the Galaxy
embedded within a dark-matter halo.
Their best-fitting model gives a dark-matter halo mass of:
and a total halo mass of:
The corresponding stellar mass is:
with the quoted uncertainty corresponding to approximately:
This number should be interpreted carefully. It is not a
direct measurement or weighing of dark-matter particles. Rather, it is the
dark-matter mass inferred from a gravitational model that reproduces the
observed dynamics of the Milky Way. The quantity M_200 represents the mass
within a conventional halo boundary defined by an average density of 200 times
the critical density of the Universe.
The mass distribution tells an even clearer story
The significance of the result becomes more apparent when
the mass distribution is considered as a function of distance from the Galactic
centre.
Cautun et al. provide an enclosed mass profile for the Milky
Way, separating the contributions from stars, baryonic matter, dark matter, and
total mass. Their model shows that the inferred dark-matter contribution
becomes increasingly important with increasing Galactic radius.
Figure 2. Enclosed mass profiles of the Milky Way as a function of distance from the Galactic centre. The solid black line shows the enclosed baryonic mass; the coloured lines show the enclosed dark-matter mass for haloes of different masses and concentrations, before (dotted) and after (solid) baryonic contraction. Based on Cautun et al. (2020), Figure 5.
At relatively small radii, the stellar component makes a
substantial contribution to the enclosed mass. At larger radii, the dark-matter
contribution becomes progressively more significant. This provides the physical
basis for describing the Milky Way as a visible stellar disc embedded within a
much more extended dark-matter halo.
The model also gives a local dark-matter density at the
Solar position of:
or equivalently:
The local density and the total halo mass describe different
aspects of the same inferred component: one characterizes the dark-matter
density near the Solar neighbourhood, while the other represents the integrated
mass of the Galactic halo within the adopted halo boundary.
What does this actually demonstrate?
It is important not to overstate what the rotation curve
establishes.
The motion of stars does not constitute a direct detection
of a dark-matter particle. Instead, it demonstrates that the observed
gravitational field cannot be adequately accounted for by the visible matter
alone under the standard gravitational interpretation.
Dark matter is the conventional explanation for this
additional gravitating mass. However, alternative explanations based on
modified theories of gravity have also been investigated. Consequently, the
most precise statement is that galactic dynamics provide strong evidence for an
additional unseen gravitating component, conventionally identified with dark
matter.
The significance of dark matter does not rest on galactic
rotation alone. Independent evidence comes from gravitational lensing, the
dynamics of galaxy clusters, the cosmic microwave background, and the observed
formation and distribution of large-scale cosmic structures. The convergence of
these different observations is what makes the dark-matter interpretation
particularly important in modern cosmology.
References
Rubin, V. C., & Ford, W. K., Jr. (1970). Rotation of the
Andromeda Nebula from a spectroscopic survey of emission regions. The
Astrophysical Journal, 159, 379–403. https://doi.org/10.1086/150317
Cautun, M., BenÃtez-Llambay, A., Deason, A. J., Frenk, C. S., Fattahi, A., Gómez, F. A., Grand, R. J. J., Oman, K. A., Navarro, J. F., & Simpson, C. M. (2020). The Milky Way total mass profile as inferred from Gaia DR2. Monthly Notices of the Royal Astronomical Society, 494(3), 4291–4313. https://doi.org/10.1093/mnras/staa1017.
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