Bahcall–Wolf cusp

Bahcall–Wolf cusp refers to a particular distribution of stars around a massive black hole at the center of a galaxy or globular cluster. If the nucleus containing the black hole is sufficiently old, exchange of orbital energy between stars drives their distribution toward a characteristic form, such that the density of stars, ρ, varies with distance from the black hole, r, as

${\displaystyle \rho (r)\propto r^{-7/4}.}$

Growth of a Bahcall–Wolf cusp. The unit of length is the black hole influence radius. The elapsed time is roughly one relaxation time. The dashed line shows the steady-state density profile.

So far, no clear example of a Bahcall–Wolf cusp has been found in any galaxy or star cluster.[1] This may be due in part to the difficulty of resolving such a feature.

Distribution of stars around a supermassive black hole

Supermassive black holes reside in galactic nuclei. The total mass of the stars in a nucleus is roughly equal to the mass of the supermassive black hole. In the case of the Milky Way, the mass of the supermassive black hole is about 4 million Solar masses, and the number of stars in the nucleus is about ten million.[2]

The stars move around the supermassive black hole in elliptical orbits, similar to the orbits that planets follow around the Sun. The orbital energy of a star is

${\displaystyle E={\boldsymbol {v}}^{2}/2-GM/r}$

where v is the star's velocity, r is its distance from the supermassive black hole, and M is the supermassive black hole's mass. A star's energy remains nearly constant for many orbital periods. But after roughly one relaxation time, most of the stars in the nucleus will have exchanged energy with other stars, causing their orbits to change. Bahcall and Wolf[3] showed that once this has taken place, the distribution of orbital energies has the form

${\displaystyle N(E)\,dE=N_{0}|E|^{-9/4}dE,}$

which corresponds to the density ρ=ρ₀ r ^−7/4. The figure shows how the density of stars evolves toward the Bahcall–Wolf form. The fully formed cusp[4] extends outward to a distance of roughly one-fifth the supermassive black hole's influence radius. It is believed that relaxation times in the nuclei of small, dense galaxies are short enough for Bahcall–Wolf cusps to form.[5]

The Galactic Center

The influence radius of the supermassive black hole at the Galactic Center is about 2–3 parsecs (pc), and a Bahcall–Wolf cusp if present would extend outward to a distance of about 0.5 pc from the supermassive black hole. A region of this size is easily resolved from Earth. However, no cusp is observed; instead, the density of the oldest stars is flat or even declining toward the Galactic Center.[6][7] This observation does not necessarily rule out the existence of a Bahcall–Wolf cusp in some still unobserved component. However, current observations imply a relaxation time at the Galactic Center of roughly 10 billion years, comparable with the age of the Milky Way. It is therefore likely that not enough time has elapsed for a Bahcall–Wolf cusp to form.[8] Alternatively, some process may have destroyed the bright stars near the supermassive black hole.

Multi-mass cusps

The Bahcall–Wolf solution applies to a nucleus consisting of stars of a single mass. If there is a range of masses, each component will have a different density profile. There are two limiting cases. If the more massive stars dominate the total density, their density will follow the Bahcall–Wolf form, whereas the less-massive objects will have ρ ${\displaystyle \propto }$ r^−3/2.[9] If the less massive stars dominate the total density, their density will follow the Bahcall–Wolf form, whereas the more-massive stars will follow ρ ${\displaystyle \propto }$ r⁻².[10]

In an old stellar population, most of the mass is either in the form of main-sequence stars, with masses ${\displaystyle \lesssim }$ 1–2 Solar masses, or in black hole remnants, with masses ~ 10–20 Solar masses. It is likely that the main-sequence stars dominate the total density; so their density should follow the Bahcall–Wolf form whereas the black holes should have the steeper, ρ ~ r⁻² profile. On the other hand, it has been suggested that the distribution of stellar masses at the Galactic Center is "top-heavy", with a much larger fraction of black holes.[11] If this is the case, the observed stars would be expected to attain the shallower density profile, ρ ~ r^−3/2. However, even this shallower profile is probably inconsistent with what is observed at the Galactic Center, implying that a Bahcall–Wolf cusp never formed. The number and distribution of black hole remnants at the Galactic Center is very poorly constrained.

See also

• Stellar dynamics

References

1. Merritt, David (2013). Dynamics and Evolution of Galactic Nuclei. Princeton, NJ: Princeton University Press.
2. Figer, D. F. (2004). "Young Massive Clusters in the Galactic Center". In Lamers, H. J.; Smith, L. J.; Nota, A. (eds.). The Formation and Evolution of Massive Young Star Clusters, Astronomical Society of the Pacific Conference Series, vol. 322. The Formation and Evolution of Massive Young Star Clusters. 322. San Francisco: Astronomical Society of the Pacific. p. 49. arXiv:astro-ph/0403088. Bibcode:2004ASPC..322...49F. ISBN 1-58381-184-2.
3. Bahcall, J. N.; Wolf, R. A. (1976), "Star distribution around a massive black hole in a globular cluster", The Astrophysical Journal, 209: 214–232, Bibcode:1976ApJ...209..214B, doi:10.1086/154711
4. The term "cusp" refers to the fact that a graph of density vs. radius has a cuspy appearance if plotted on linear axes, rather than the logarithmic axes used in the figure.
5. Merritt, David (2009), "Evolution of Nuclear Star Clusters", The Astrophysical Journal, 694 (2): 959–970, arXiv:0802.3186, Bibcode:2009ApJ...694..959M, doi:10.1088/0004-637X/694/2/959
6. Buchholz, R. M.; Schoedel, R.; Eckart, A. (2009), "Composition of the galactic center star cluster. Population analysis from adaptive optics narrow band spectral energy distributions", Astronomy and Astrophysics, 499 (2): 483–501, arXiv:0903.2135, Bibcode:2009A&A...499..483B, doi:10.1051/0004-6361/200811497
7. Do, T.; et al. (2009), "High Angular Resolution Integral-Field Spectroscopy of the Galaxy's Nuclear Cluster: A Missing Stellar Cusp?", Astrophysical Journal, 703 (2): 1323–1337, arXiv:0908.0311, Bibcode:2009ApJ...703.1323D, doi:10.1088/0004-637x/703/2/1323
8. Merritt, David (2010), "The Distribution of Stars and Stellar Remnants at the Galactic Center", The Astrophysical Journal, 718 (2): 739–761, arXiv:0909.1318, Bibcode:2010ApJ...718..739M, doi:10.1088/0004-637X/718/2/739
9. Bahcall, J. N.; Wolf, R. A. (1977), "Star distribution around a massive black hole in a globular cluster. II Unequal star masses", The Astrophysical Journal, 216: 883–907, Bibcode:1977ApJ...216..883B, doi:10.1086/155534
10. Alexander, T.; Hopman, C. (2009), "Strong Mass Segregation Around a Massive Black Hole", The Astrophysical Journal, 697 (2): 1861–1869, arXiv:0808.3150, Bibcode:2009ApJ...697.1861A, doi:10.1088/0004-637X/697/2/1861
11. Bartko, H.; et, al. (2010), "An Extremely Top-Heavy Initial Mass Function in the Galactic Center Stellar Disks", The Astrophysical Journal, 708 (1): 834–840, arXiv:0908.2177, Bibcode:2010ApJ...708..834B, doi:10.1088/0004-637X/708/1/834