Prologue
Key Concepts:
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Recent CMB experiments have revealed sound waves
in the fine angular scale structure of the temperature anisotropies.
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Sound waves can be used to probe the infant universe
as a kind of cosmic ultrasound
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The era of precision cosmology has begun
According to the theory of the Big Bang, the
universe started hot and dense and then expanded and cooled. In the hot,
dense conditions of the early universe, photons were
tightly glued to matter. When the universe was about 300,000 years
old the temperature dropped below 3,000K allowing
atomic hydrogen to form and releasing the photons. These photons,
which travelled freely through the universe as it expanded and cooled,
make up the cosmic microwave background (CMB)
we see today. Ten to twenty billion years after the Big Bang, the CMB is
a cold sea of photons with an average temperature of 2.7K (-270 C). These
photons are all around us, causing about 1% of the noise on our television
sets. (For a more thorough introduction to the CMB please see the sister
pages: An
Introduction to the Cosmic Microwave Background.)
When it was discovered in the 1960s, the CMB was found to be remarkably
uniform across the sky. It was not until 1992 that the Cosmic Background
Explorer (COBE) satellite discovered temperature
variations (or ripples) at the level of 1 part in 100,000. Temperature
maps of the CMB form a snapshot image of the universe when it was extremely
young. So these ripples reflect tiny density fluctuations in the primordial
soup of particles. These same density fluctuations are thought to grow
by gravitational attraction into the familiar
structures we see today (stars, galaxies, and clusters of galaxies). This
is the gravitational instability model of structure formation.
COBE told us what the large-scale fluctuations
in the background look like, but cosmologists today are more interested
in the small-scale fluctuations. Astronomers divide up the sky into angular
degrees, so that 90 degrees is the distance from the horizon to a point
directly overhead. COBE measured temperature ripples from the 10 degree
to 90 degree scale. This scale is so large that there has not been enough
time for structures to evolve. Hence COBE sees the so-called
initial conditions of the universe. At the degree
scale, on the other hand, the process of structure formation imprints
information in the ripples about conditions in the early universe.
Since the COBE discovery, many ground and balloon-based experiments have
shown the ripples peak at the degree scale.
What CMB experimentalists do is take a power spectrum
of the temperature maps, much as you would if you wanted to measure background
noise. The angular wavenumber, called a multipole
l, of the power spectrum is related to the inverse of the angular scale
(l=100 is approximately 1 degree). Recent experiments, noteably
the Boomerang and Maxima experiments, have show that the power spectrum
exhibits a sharp peak of exactly the right form to be the ringing or acoustic
phenomena long awaited by cosmologists:
Soundscape: COBE measured
the temperature fluctuations DT on the largest
angular scales which correspond to multipoles as roughly l=100/angle
(degrees) ~ 2-20. The current generation of experiments are measuring
multipoles l>100 where the acoustic peaks are expected to dominate
the scene (yellow curve). The physical landscape described in these
pages begins with sound waves and proceeds through baryon loading, radiation
driving, and dissipation by diffusion damping. In the background,
are the measurements as of January 2001.
Such acoustic phenomena probe the conditions of the infant universe as
a kind of cosmic ultrasound. These pages are
devoted to exploring the implications of current and upcoming measurements
of sound waves in the CMB.
With the discovery of sound waves in the CMB, we have entered a new era
of precision cosmology in which we can begin
to talk with certainty about the origin of structure
and the content of matter and energy in the
universe.
Introduction based on News &
Views in Nature 404, 939 (2000). Pages based on Warner
Prize lecture presented at the January 2001, AAS meeting