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Sunday, August 5, 2018
Reading List: Losing the Nobel Prize
- Keating, Brian. Losing the Nobel Prize. New York: W. W. Norton, 2018. ISBN 978-1-324-00091-4.
-
Ever since the time of Galileo, the history of astronomy has
been punctuated by a series of “great
debates”—disputes between competing theories of the
organisation of the universe which observation and experiment
using available technology are not yet able to resolve one way
or another. In Galileo's time, the great debate was between the
Ptolemaic model, which placed the Earth at the centre of the
solar system (and universe) and the competing Copernican model
which had the planets all revolving around the Sun. Both models
worked about as well in predicting astronomical phenomena such
as eclipses and the motion of planets, and no observation made
so far had been able to distinguish them.
Then, in 1610, Galileo turned his primitive telescope to
the sky and observed the bright planets Venus and Jupiter.
He found Venus to exhibit phases, just like the Moon, which
changed over time. This would not happen in the Ptolemaic
system, but is precisely what would be expected in the
Copernican model—where Venus circled the Sun in an orbit
inside that of Earth. Turning to Jupiter, he found it to
be surrounded by four bright satellites (now called the
Galilean moons) which orbited the giant planet. This further
falsified Ptolemy's model, in which the Earth was the sole
source of attraction around which all celestial bodies
revolved. Since anybody could build their own telescope
and confirm these observations, this effectively resolved
the first great debate in favour of the Copernican heliocentric
model, although some hold-outs in positions of authority
resisted its dethroning of the Earth as the centre of
the universe.
This dethroning came to be called the “Copernican
principle”, that Earth occupies no special place in the
universe: it is one of a number of planets orbiting an ordinary
star in a universe filled with a multitude of other stars.
Indeed, when Galileo observed the star cluster we call the
Pleiades,
he saw myriad stars too dim to be visible to the
unaided eye. Further, the bright stars were surrounded by
a diffuse bluish glow. Applying the Copernican principle
again, he argued that the glow was due to innumerably more
stars too remote and dim for his telescope to resolve, and
then generalised that the glow of the Milky Way was also
composed of uncountably many stars. Not only had the Earth been
demoted from the centre of the solar system, so had the Sun
been dethroned to being just one of a host of stars possibly
stretching to infinity.
But Galileo's inference from observing the Pleiades was
wrong. The glow that surrounds the bright stars is
due to interstellar dust and gas which reflect light
from the stars toward Earth. No matter how large or powerful
the telescope you point toward such a
reflection
nebula, all you'll ever see is a smooth glow. Driven by
the desire to confirm his Copernican convictions, Galileo had
been fooled by dust. He would not be the last.
William
Herschel was an eminent musician and composer, but his
passion was astronomy. He pioneered the large reflecting
telescope, building more than sixty telescopes. In 1789, funded
by a grant from King George III, Herschel completed a reflector
with a mirror 1.26 metres in diameter, which remained the largest
aperture telescope in existence for the next fifty years. In
Herschel's day, the great debate was about the Sun's position
among the surrounding stars. At the time, there was no way to
determine the distance or absolute brightness of stars, but
Herschel decided that he could compile a map of the galaxy (then
considered to be the entire universe) by surveying the number of
stars in different directions. Only if the Sun was at the
centre of the galaxy would the counts be equal in all
directions.
Aided by his sister Caroline, a talented astronomer herself, he
eventually compiled a map which indicated the galaxy was in
the shape of a disc, with the Sun at the centre. This seemed to
refute the Copernican view that there was nothing special about
the Sun's position. Such was Herschel's reputation that this
finding, however puzzling, remained unchallenged until 1847
when Wilhelm Struve discovered that Herschel's results had been
rendered invalid by his failing to take into account the absorption
and scattering of starlight by interstellar dust. Just as you
can only see the same distance in all directions while within
a patch of fog, regardless of the shape of the patch, Herschel's
survey could only see so far before extinction of light by dust
cut off his view of stars. Later it was discovered that the
Sun is far from the centre of the galaxy. Herschel had been fooled
by dust.
In the 1920s, another great debate consumed astronomy. Was the
Milky Way the entire universe, or were the “spiral
nebulæ” other “island universes”,
galaxies in their own right, peers of the Milky Way? With no
way to measure distance or telescopes able to resolve them into
stars, many astronomers believed spiral neublæ were nearby
objects, perhaps other solar systems in the process of
formation. The discovery of a
Cepheid
variable star in the nearby Andromeda “nebula”
by Edwin Hubble in 1923 allowed settling this debate. Andromeda
was much farther away than the most distant stars found in the
Milky Way. It must, then be a separate galaxy. Once again,
demotion: the Milky Way was not the entire universe, but just
one galaxy among a multitude.
But how far away were the galaxies? Hubble continued his search
and measurements and found that the more distant the galaxy,
the more rapidly it was receding from us. This meant the
universe was expanding. Hubble was then able to
calculate the age of the universe—the time when all of the
galaxies must have been squeezed together into a single point.
From his observations, he computed this age at two billion
years. This was a major embarrassment: astrophysicists and
geologists were confident in dating the Sun and Earth at around
five billion years. It didn't make any sense for them to be
more than twice as old as the universe of which they were a
part. Some years later, it was discovered that Hubble's
distance estimates were far understated because he failed to
account for extinction of light from the stars he measured due
to dust. The universe is now known to be seven times the age
Hubble estimated. Hubble had been fooled by dust.
By the 1950s, the expanding universe was generally accepted and
the great debate was whether it had come into being in some
cataclysmic event in the past (the “Big Bang”) or
was eternal, with new matter spontaneously appearing to form new
galaxies and stars as the existing ones receded from one another
(the “Steady State” theory). Once again, there were
no observational data to falsify either theory. The Steady State
theory was attractive to many astronomers because it was the
more “Copernican”—the universe would appear
overall the same at any time in an infinite past and future, so
our position in time is not privileged in any way, while in the
Big Bang the distant past and future are very different than the
conditions we observe today. (The rate of matter creation required
by the Steady State theory was so low that no plausible laboratory
experiment could detect it.)
The discovery of the
cosmic
background radiation in 1965 definitively settled the debate
in favour of the Big Bang. It was precisely what was expected if
the early universe were much denser and hotter than conditions today,
as predicted by the Big Bang. The Steady State theory made no
such prediction and was, despite rear-guard actions by some
of its defenders (invoking dust to explain the detected radiation!),
was considered falsified by most researchers.
But the Big Bang was not without its own problems. In
particular, in order to end up with anything like the universe
we observe today, the initial conditions at the time of the Big
Bang seemed to have been fantastically fine-tuned (for example,
an infinitesimal change in the balance between the density and
rate of expansion in the early universe would have caused the
universe to quickly collapse into a black hole or disperse into
the void without forming stars and galaxies). There was no
physical reason to explain these fine-tuned values; you had to
assume that's just the way things happened to be, or that a
Creator had set the dial with a precision of dozens of decimal
places.
In 1979, the theory of
inflation
was proposed. Inflation held that in an instant after the Big
Bang the size of the universe blew up exponentially so that all
the observable universe today was, before inflation, the size of
an elementary particle today. Thus, it's no surprise that the
universe we now observe appears so uniform. Inflation so neatly
resolved the tensions between the Big Bang theory and
observation that it (and refinements over the years) became
widely accepted. But could inflation be observed?
That is the ultimate test of a scientific theory.
There have been numerous cases in science where many years elapsed
between a theory being proposed and definitive experimental
evidence for it being found. After Galileo's observations,
the Copernican theory that the Earth orbits the Sun became
widely accepted, but there was no direct evidence for
the Earth's motion with respect to the distant stars until the
discovery of the
aberration
of light in 1727. Einstein's theory of general relativity
predicted gravitational radiation in 1915, but the phenomenon was
not directly detected by experiment until a century later.
Would inflation have to wait as long or longer?
Things didn't look promising. Almost everything we know about the universe comes from observations of electromagnetic radiation: light, radio waves, X-rays, etc., with a little bit more from particles (cosmic rays and neutrinos). But the cosmic background radiation forms an impenetrable curtain behind which we cannot observe anything via the electromagnetic spectrum, and it dates from around 380,000 years after the Big Bang. The era of inflation was believed to have ended 10−32 seconds after the Bang; considerably earlier. The only “messenger” which could possibly have reached us from that era is gravitational radiation. We've just recently become able to detect gravitational radiation from the most violent events in the universe, but no conceivable experiment would be able to detect this signal from the baby universe.
So is it hopeless? Well, not necessarily…. The cosmic background radiation is a snapshot of the universe as it existed 380,000 years after the Big Bang, and only a few years after it was first detected, it was realised that gravitational waves from the very early universe might have left subtle imprints upon the radiation we observe today. In particular, gravitational radiation creates a form of polarisation called B-modes which most other sources cannot create. If it were possible to detect B-mode polarisation in the cosmic background radiation, it would be a direct detection of inflation. While the experiment would be demanding and eventually result in literally going to the end of the Earth, it would be strong evidence for the process which shaped the universe we inhabit and, in all likelihood, a ticket to Stockholm for those who made the discovery. This was the quest on which the author embarked in the year 2000, resulting in the deployment of an instrument called BICEP1 (Background Imaging of Cosmic Extragalactic Polarization) in the Dark Sector Laboratory at the South Pole. Here is my picture of that laboratory in January 2013. The BICEP telescope is located in the foreground inside a conical shield which protects it against thermal radiation from the surrounding ice. In the background is the South Pole Telescope, a millimetre wave antenna which was not involved in this research.