|
Journey
to the
Center
of the
Galaxy
Introduction
Size Scales
Wavelength
Gas Dynamics
Star Dynamics
The Black Hole
Star Formation

Andromeda Galaxy - M31
|
The Black Hole
As we zoom into the very core of the Galactic Center, our field of view shrinks to
a mere 5 arcseconds (one thousandth of a degree) in size. At radio wavelengths, the most
prominent feature of this tiny region is the point-like radio source called
Sagittarius A* (pronounced "Sag A star"). Studies of the radio properties of Sgr A*
reveal that it is a physically compact object approximately one
Astronomical Unit (1 AU=1.5X10^8 km) in size, many times smaller than our solar system.
However, as seen below, at near-infrared wavelengths, there is no clear sign of a single
prominent source of emission like that seen in the radio. Therefore, the nature of the
source of the radio emission remained a mystery for some time.
|
|
2.2 micron AO image of the central cluster of stars orbiting the supermassive black hole
|
In 1974, Sir Martin Rees proposed the idea that supermassive black holes
could exist within the centers of active galactic nuclei or quasars. In that same year,
Balick & Brown made the connection between their radio detection of Sgr A* and other known active galactic nuclei.
However, only in the past 20 years have we collected enough evidence through
the observed motions of gas and stars to convince ourselves
that something very massive lurks at the center of our galaxy. The first dynamical
evidence came from the motions of the ionized gas streamers of the mini-spiral
orbiting around Sgr A*.
Using the velocities of the gas estimated from the Doppler shift of spectral lines,
they were able to estimate
that a mass of material six million solar masses must lie within 10 arcseconds of
Sgr A*. This did not explicitly
prove the existence of a black hole since that amount of matter could be accounted
for by a high density of stars within
such a large volume.
In the past eight years, recent high resolution near-infrared studies have
observed a compact cluster of stars surrounding the
radio position of Sgr A*. These stars have very large proper motions
considering thier 8 kpc (24 million light years) distance
from the Earth. The two main groups devoted to tracking these stars
include Andrea Ghez and others at UCLA who have been
using the 10-m Keck telescope on Mauna Kea, Hawaii and Genzel & Eckart
who use the 3.5-m NTT telescope in La Silla, Chile.
Both groups take advantage of the high spatial resolution and
sensitivity of these large telescopes
to track the positions of the stars within the cluster using
near-infrared images collected
once or twice a year.
Despite Keck's large diameter, air turbulence in
the Earth's atmosphere blurs the image and therefore greatly
reduces its detail and ability to
distinguish between the stars in the tightly packed cluster.
There are two ways to get around this problem: speckle interferometry and adaptive
optics.
Speckle interferometry involves collecting stacks of images with very short exposure times
which effectively freezes the atmosphere resulting in a pattern of
diffraction limited speckles.
Then, in post processing, the high resolution information is recovered by shifting and adding
onto the brightest speckle within the speckle pattern to produce a PSF
with a diffraction limited
core and seeing halo. Adaptive Optics (AO) uses a deformable mirror
which mimics the shape of the incoming lightwave and corrects for the atmospheric
turbulence before the data is recorded.
In both cases, very accurate stellar positions can be
estimated in order to kept track of the motions of the stars in the
compact central cluster which are
zipping around Sgr A* at speeds up to 1400 km/s (3,000,000 mph)! Using
Kepler's laws of motion, we use the orbital velocities and positions of
the bright stars to estimate
the mass that must be contained within their orbits. The resulting enclosed mass of
2.6X10^6 times the mass of the sun, combined with the minute
size of Sgr A* constraint provided by the radio emission, suggests
that the stars must be swiftly circling around a
supermassive black hole. In fact, the large number of observations of
the stars orbiting the black
hole has allowed us to provide the first even detection of the
accelerations of the stars in the central
cluster.
 |
Now that we believe there is a supermassive black hole at the center of our galaxy, we can
attempt to understand its other mysterious properties including a lack of high
energy emission like
that seen in other active galactic nuclei. The emission properties of Sgr A* have long been
a subject for discussion among many theorists who attempt to use a variety
of different physical
phenomena to model its spectrum from the X-ray to the radio.
Recent observations of a sample of nearby galaxies reveal that such
supermassive black holes are not unique to the Milky Way. The formation of
such a large black hole and how it affects
the evolution of its host galaxy are not well understood, nor is the connection between the
black hole in the Milky Way and those believed to exist in the cores of
AGN's, which emit a huge amount of radiation from their nuclei at many different
wavelengths. However, in the case of Sgr A*, there is a mysterious absence of
the high energy emission
(X-ray and ultra-violet radiation for example) often observed from AGN's.
To further investigate how the brightness of Sgr A* changes with wavelength, Ghez and Morris
are currently trying to measure the luminosity of Sgr A* in the near and mid-infrared.
Their result will have implications for the type of physical processes occurring in
and around the black hole.
|