The structure of the nuclear stellar cluster of the Milky Way

Abstract

We present high-resolution seeing limited and AO NIR imaging observations of the stellar cluster within about one parsec of Sgr A*, the massive black hole at the centre of the Milky Way. Stellar number counts and the diffuse background light density were extracted from these observations in order to examine the structure of the nuclear stellar cluster.Our findings are as follows: (a) A broken-power law provides an excellent fit to the overall structure of the GC nuclear cluster. The power-law slope of the cusp is $\Gamma =0.19\pm 0.05$, the break radius is $R_{\mathrm{break}}=6.0^{\prime \prime }\pm 1.0^{\prime \prime }$ or $0.22\pm 0.04$ pc, and the cluster density decreases with a power-law index of $\Gamma =0.75\pm 0.1$ outside of $R_{\mathrm{break}}$. (b) Using the best velocity dispersion measurements from the literature, we derive higher mass estimates for the central parsec than assumed until now. The inferred density of the cluster at the break radius is $2.8\pm 1.3\times 10^6{\mathrm{M}}_{\odot }\mathrm{p}{\mathrm{c}}^{-3}$. This high density agrees well with the small extent and flat slope of the cusp. Possibly, the mass of the stars makes up only about 50% of the total cluster mass. (c) Possible indications of mass segregation in the cusp are found (d) The cluster appears not entirely homogeneous. Several density clumps are detected that are concentrated at projected distances of $R=3^{\prime \prime }$ and $R=7^{\prime \prime }$ from Sgr A*.(e) There appears to exist an under-density of horizontal branch/red clump stars near $R=5^{\prime \prime }$, or an over-density of stars of similar brightness at $R=3^{\prime \prime }$ and $R=7^{\prime \prime }$. (f) The extinction map in combination with cometary-like features in an L'-band image may provide support for the assumption of an outflow from Sgr A*.

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