The gas cloud G2

 

We have detected the gas cloud G2, a dusty, ionized gas cloud on a highly eccentric orbit around Sgr A*, which passed pericenter in spring 2014. We have discovered G2 in 2011 both from its dust and recombination line emission (Gillessen et al. 2012). We were able to predict the soon-to-come pericenter passage as well as the tidal disruption. We identified G2 in the data sets ranging back to 2002 (NACO) and 2004 (SINFONI).

 

Time series of NACO L-band images, showing how G2 (arrow) approached the position of Sgr A* (asterisk) during the past decade.

 

Most spectacular is the SINFONI data, from which we extract position-velocity diagrams along the orbital path. A compilation of such diagrams shows in beautiful detail how the gravitational force of the MBH has tidally disrupted G2 - the first time that one can follow and study this process observationally.

 

Time series of SINFONI position-velocity diagrams of G2. The initially compact object gets faster and more and more tidally elongated as it approaches Sgr A*. From 2013 to 2015, the gas swings around the black hole onto the blue-shifted, post-peri side.

 

 

Since 2013 we have been able to see how the gas has swirled around the black hole (Gillessen et al. 2013, Pfuhl et al. 2015), with more and more gas moving from the red-shifted side of the orbit that is approaching Sgr A* over to the blue-shifted side. The data are to first order well described by a simple model consisting only of a cloud of non-interacting test particles - the evolution is thus dominated by the tidal interaction.

 

 

The measured radial velocity of G2 in the last years (2016, 2017, 2018) is slower than what the purely Keplerian orbit model predicts. G2 has been slowed down during pericenter passage. This is because G2 was flying through SgrA*'s atmosphere, the accretion flow from which the black hole is fed. Unlike a star, a gaseous object like G2 is notably affected by the ambient gas density and loses energy – very much like satellites that can feel the upper part of Earth's atmosphere. The amount of energy loss can be measured from G2's orbital motion, and allows estimating the density of the gas through which it was flying. This yields an estimate of the gas density at around 1000 Schwarzschild radii, a regime which previously was inaccessible. The accretion flow density was measured previously at around 10 Schwarzschild radii from radio polarisation data, and at around 10^5 Schwarzschild radii from its X-ray emission. Our novel estimate nicely fills the gap in-between.

The origin of G2 is debated. The two basic model types are purely gaseous clouds, and models that assume a central star with some circumstellar material. Our preferred model is that G2 is a dense knot in a much longer gas streamer, perhaps a stretched clump of a stellar wind, or the debris from a partial tidal disruption of a giant star that came a bit too close to Sgr A*, since there is more, lower surface density gas along the orbital trace.

 

For more information, see also the press releases A Black Hole's Dinner is Fast Approaching and Ripped Apart by a Black Hole.

 

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