1. Introduction
In this article, I will briefly review some of the historical development of the subjects of extrasolar planets and the search for extraterrestrial life, starting from their non-scientific beginnings, up to the flood of real data during the last few years. I will try to explain in non-technical terms the various simple but ingenuous methods that have been devised to detect extrasolar planets and to study them, and the intriguing results they have produced. I will then continue to the next logical step, but one that is still at the pre-discovery stage – astrobiology – the search for, and study of, signs of life outside Earth. Again, I will discuss some of the techniques being considered and planned, and some recent developments in Earth-bound biology that guide our ideas of where and how we should look for evidence of extraterrestrial life, and what forms it may assume. Finally, I will argue that a major motivation for the whole pursuit, other than sheer curiosity as to the question of “are we alone?”, is the potential for a much deeper understanding of the emergence of life here on Earth.
Contrary to the popular perception of extraterrestrial life, as envisioned in countless (often highly entertaining) Hollywood films, and in the delusions of UFO aficionados, the scientific reality, as so often happens, will likely turn out to be much stranger and wondrous than imaginable by any screenwriter or crackpot. Finding extraterrestrial life, even though it will almost surely be of a most primitive form, will shed much light on what life is. No less important, a general absence of life on planets that could potentially harbor life would also have profound implications for us and our place in the cosmos.
2. Early HistoryHuman
speculation about the existence of other worlds and other sentient
beings must be as old as humanity itself. For example, in the 6th
century B.C., the Greek philosopher Anaximander discussed the
possibility of a “plurality of worlds”. The Assyrian satirist Lucian of
Samosota composed in the 2nd century
the humorous fantasy “A True Story”, which is considered the first work
of science fiction, replete with life forms and warring civilizations
on the moon, the sun, and the planets. The concept naturally finds
expression also in most, if not all, religions. To bring an example
close to home, in the Babylonian Talmud, Volume “Avoda Zara”, Tractate
3b, there is a discussion of what is God’s daily routine, followed by
the question of what does God then do at night. One possibility, based
on interpretation of a verse in Psalms, is that “he rides on a light
angel of his and sails through eighteen thousand worlds”. As one of the
very few places in Jewish scripture suggesting the existence of other
worlds, this sentence in the Talmud has elicited further debate in the
religious Jewish literature over the centuries. The issue is
particularly critical in the monotheistic religions, where Earth and
Man hold a special position in the Creation. Indeed, in medieval
Christian discussions (e.g., in the condemnations of Aristotelian
doctrines by Bishop Stephanus Tempier of Orleans in 1270), the concept
of human centrality has been used to argue against the existence of
other worlds. The earliest well-known semi-scientific exploration of
the subject was by 16th century Italian philosopher Giordano Bruno, an
early champion of the Copernican world view. In his dialogue “De
L’Infinito Universo et Mondi” (On the Infinite Universe and Worlds,
1584) and in other works, he conjectured that:
- Celestial
bodies are composed of the same elements as the Earth (assumed to be
earth, water, wind, and fire), rather than of a fifth and purer
“quintessence”.
- The stars are immensely distant suns, each orbited by their own planetary systems.
- There is an infinity of other stars and planets, all inhabited.
The
fact that these conjectures, made 25 years before Galileo’s first use
of the telescope, were not based on any scientific evidence, but rather
on a pure but amazingly accurate intuition, make them all the more
striking. It would take until the early twentieth century, with the
development of spectroscopy and atomic physics, to confirm that,
indeed, the stars are made of the same elements found on Earth, and
until only the last few decades to extend this result to the furthest
reaches of the Universe. The understanding that the Sun is a normal
star has again developed over the past century, with the availability
of increasingly accurate astronomical observations and the development
of nuclear physics. The infinity of the Universe, with its implied
infinity of stars (or at least their overwhelmingly large numbers),
have emerged only over the past decade, with the advent of precision
cosmology. Finally, as I will describe in detail below, it is only a
decade and a half ago that the first few extrasolar planets were
discovered, and only within the last few years that it has become clear
that planets are common around other stars. The sole Bruno conjecture
that remains unconfirmed is the one about the ubiquity of life. Based
only on his success so far, it could be argued that surely he must have
gotten that one right as well. As I will explain below, we should know
before too long.
With Galileo and the beginning of modern
astronomy in 1609, it became clear that the moons and the other planets
in the solar system, at least, do qualify as “other worlds”, and the
search for signs of life on them was on. The field got a boost in 1877
when Italian astronomer Schiaparelli, sketching the surface of Mars
based on his visual observations, believed he saw long straight
features which he termed “canali”.

Fig. 1: Sketches of the surface of Mars by Schiaparelli (top) and Lowell (bottom) |

Fig. 2: H. G. Wells: War of the Worlds, 1898 |
This prompted American astronomer Percival Lowell to build and
use an observatory dedicated to Mars observations. Based on his
studies, he promoted between 1895 and 1908 the idea that Mars is
covered by a network of canals built by an advanced but desperate
civilization, in order to channel water from the poles to the arid
equatorial regions. While these ideas were viewed skeptically by
professionals from the start, and the canals were finally demonstrated
to be optical illusions by the spacecraft missions in the 1960s, they
ignited the public imagination with respect to the subject of
extraterrestrial life. Most notable in this sense was H. G. Wells’s
novel “The War of the Worlds” (1898), about an attempt by the desperate
Martians to conquer Earth for the sake of our natural resources (in
line with the colonialist thinking of the period), only to be
vanquished by local bacteria (in line with the then-recent proof of the
germ theory of disease). The planetary probes that have
explored the surface of Mars over the past few decades have found that
Mars is probably inhospitable to life. However, as I write this, Mumma
et al. (2009) have reported telescopic observations in 2003 showing a
transient release of methane into the Northern summer hemisphere of
Mars from plumes, which could, in principle (but not necessarily) be of
subterranean biological origin. Regardless, the possibility remains
that Mars hosted life in the past, when it possessed a denser
atmosphere and liquid water on its surface. Other sites in the
solar system, such as the moons of Jupiter and Saturn, have not been
ruled out yet as sites for some form of life. But, if we are to find
more definitive evidence for extraterrestrial life, or the lack
thereof, we need to expand the search beyond the confines of the solar
system. Particularly relevant are other stars similar to the sun, and
having “terrestrial” planets – rocky planets that are similar to Earth
in terms of their mass (and hence gravity) and their temperatures
(which are set by their distances to their parent stars), and hence
permitting the existence of liquid water. Remarkably, until 1992 there
was not a single known clear example of an extrasolar planet.

Fig. 3 Methane release on Mars (Mumma et al., 2009) |
As we will see, at the large distances of even the
nearest stars, detecting a planet is extremely challenging. Following
an initiative by Tel-Aviv University astronomer Tsevi Mazeh, his group
(Latham et al. 1989) announced the discovery of a 10-Jupiter-mass
companion in a close orbit around another star. Although at the time it
was not widely recognized as a planet, many such planets are known
today, and in retrospect this was likely the first extrasolar planet
found. The first unambiguous discovery of extrasolar planets was made
in 1992 by Wolszczan and Frail, who found, by means of radio timing
observations, two planets around a pulsar – the extremely dense remnant
of an exploded massive star. The first detection of a Jupiter-mass
planet around a normal star came only three years later, by Mayor and
Queloz (1995). This opened the floodgates on extrasolar planet
discoveries, with over 300 found to date, and the number rapidly
growing. Let us review the various techniques that have made it
possible, after more than 400 years, to confirm Bruno’s planetary
conjecture.
3. How to find extrasolar planets
3.1 The radial-velocity method
The large majority of known extrasolar planets have been discovered by
measuring the “wobble” that they induce on their parent stars. A basic
result of Newtonian mechanics is that two masses under the influence of
their mutual gravitational attraction will move in elliptical orbits
around an imaginary point between them called the center of mass. The
ratio of the distances of the two masses to this point equals the
inverse of the ratio of the masses, and thus the center of mass is
always closer to the more massive object. In the context of stars and
their planets, consider, for example, the Sun and the planet Jupiter.
With Jupiter’s mass being 1/1000 that of the Sun, and the Sun-Jupiter
separation being about 5 “astronomical units” (i.e., 5 times the
Earth-Sun separation, or 5 x 150,000, 000 km), the center of mass is at
distance from the center of the sun of 5 x 150, 000,000 km/1000=750,000
km. This happens to be just over the solar radius. Thus, while Jupiter
goes through a full, more-or-less circular, 12-year orbit, the sun
moves is a corresponding little circle around a point just outside its
limb. It is then easy to calculate the velocity at which the sun does
this little dance. The circumference of the circle the sun traces is
2π x 750, 000 km, or about 5 million km, so the velocity is (5 million
km)/12 years, or 400,000 km/yr. There are 365 x 24 = 8760 hours in a
year, so this is equivalent to about 50 km/hr, a typical driving speed.
Now, each of the planets in the solar system makes the sun go through
its own dance around a point that is always between the sun and the
planet, and the actual motion of the sun will be the combination of all
those motions. But in practice, Jupiter, because of its large mass and
relatively short distance to the sun, is by far the dominant body
behind the sun’s driving-speed wobble.

Fig. 4: Doppler shift of the light from a wobbling star caused by an unseen planet |
Astronomers are very adept at measuring velocities of celestial bodies
using the Doppler effect that velocity induces on the light waves
emitted by those bodies. Just as the pitch of the sound from an
approaching train whistle is higher than that from a receding one,
light from an approaching star gets shifted to blue wavelengths, and
from a receding star to red wavelengths. The relative shift in
wavelength equals just the ratio of the star’s velocity to the velocity
of light. The 50 km/hr velocity of the sun thus corresponds to a 50
parts-per-billion Doppler shift in the wavelength of the emitted light.
While this sounds challenging, police radar guns that are used to catch
speeding vehicles, and which operate on the same principle, reach more
or less these accuracies. The idea is then simple: monitor over time
the velocity of a star, as deduced from the Doppler shifts of its
emitted light. If that star has, e.g., a planet orbiting it just like
Jupiter orbits the sun, and the orbital plane happens to be inclined
“edge-on” to our line of sight, then, over 12-year periods, we will
detect its wobble in the form of a periodic variation in the observed
velocity. Half the time the star will be approaching us, reaching a
maximum of 50 km/s in its observed velocity when its planet is abreast
to one side, and 6 years later reaching this velocity in the opposite,
receding, direction. When the planet passes exactly before or behind
the star, the star is also at the point in its little orbit where it is
moving perpendicular to our line of sight, i.e., neither approaching
nor receding, and hence its velocity is zero. So, if we monitor the
Doppler line-of-sight velocity of a nearby star and see this kind of
periodic wobbling we can deduce the presence of a planet around it.
From the period (12 years in the above example) and the amplitude of
the variation (50 km/hr in the above example) we can deduce the orbital
separation and the mass (5 astronomical units and 1 Jupiter mass in the
above example. In reality, this is true only if we assume the edge-on
inclination; if, as is often the case, we do not know the inclination
of the unseen planet, we can only find a lower limit to the planet
mass.) If the planet is more massive and/or it is in a closer orbit
around it’s star, its stronger gravitational tug will cause a stronger
and faster wobble, and hence the period will shorten and the amplitude
will rise. Such planets will therefore be easier to detect (larger
Doppler effect), and will require a shorter monitoring period.

Fig. 5: Radial velocity curve of 51 Pegasi, the first Jupiter-mass extrasolar planet found (Mayor and Queloz, 1995). |
In the early 1990s, astronomers refined the stability and accuracy of optical spectrographs
on telescopes so that precisions of order 50 km/hr could be obtained
when monitoring the light from the nearest (and hence brightest) stars.
Planet discoveries around some of these stars soon began to flow in,
with two main groups of researchers contributing, the Geneva group led
by Mayor and the California group led by Marcy and Butler. The first
planets discovered were, naturally, those that are easiest to find –
massive objects like Jupiter. However, the big surprise was that these
planets were orbiting their stars at tiny separations, smaller than
Mercury’s orbit in the solar system, and hence with orbital periods of
only a few days. At these small separations, the temperatures of these
planets due to the irradiation by their host stars must be quite high,
and hence they have been dubbed “hot Jupiters”. Their discovery was
completely unexpected based on the only planetary system known
previously, the solar system, where giant planets exist only in the
outer regions – Jupiter and beyond. It was also unexpected
theoretically. It was, and still is, thought that giant planets can
only form at large distances, beyond the “snow line” where water can
exist as a solid (more on this later). Although debate about the nature
of hot Jupiters continues, it is generally believed that these planets
indeed initially form far from their stars, but then “migrate” to their
present close orbits.
As the radial-velocity surveys
continued and accumulated data, they were able to discover also planets
of somewhat lower masses (of order Neptune), and on longer orbits,
approaching that of Jupiter in the solar system. However, the very
nature of the technique is biased toward finding hot Jupiters, which
therefore constitute the large majority of the extrasolar planets
discovered so far. In no way does this imply that such planets are
typical. To find other types of planets, which are more similar to
ours, and in particular planets that could sustain life, we must turn
to additional techniques.
3.2 The transit method
The orbital planes of extrasolar planetary systems are inclined at
random angles to our line of sight. Some fraction of them will be seen
nearly edge on. A planet in such a system will transit the face of its
parent star once per orbit. This “mini-eclipse” will cause a small
reduction in the amount of light arriving from the star, in proportion
to the ratio of the areas of the disks of the planet and the star.
Jupiter, for example, has 1/10 the radius of the sun. Transiting across
the face of the sun as viewed from outside the solar system, it would
cause an approximately 1/100 shadowing of the sun’s output during the
transit. Obviously, detecting this requires high photometric (i.e.,
light measuring) accuracies, of better the 1%, in order to discover
"Jupiters", and even higher in order to discover smaller planets. As in
the radial-velocity method, this requirement limits the search to
nearby (and hence bright) stars, although the demands are not as
stringent as in the radial-velocity case. The first extrasolar planet
transit was detected in 2000, (independently by Charbonneau et al. and
by Henry et al.) by monitoring the light from a sample of stars that
were already known to have orbiting hot Jupiters (but with unknown
orbital plane inclinations). The transit occurred exactly when expected
based on the radial velocity data, i.e., when the radial velocity is
zero, and between the phase when the planet is approaching us and when
it is receding from us.

Fig.6: Planet transit of HD 209458 (Charbonneau et al. 2000) |
Transit-detected planets have a rich variety of possibilities for
interesting follow-up studies. First, the fact, that they transit means
that their orbital inclination to our line of sight is basically
determined (edge-on), and therefore their masses are known accurately.
The depth of the eclipses reveal their radii, and hence their mean
densities can be calculated. From the densities one can learn about
their internal compositions. Perhaps more dramatically, during the
transit, light from the star will be partially absorbed by the
semitransparent atmosphere of the planet. By comparing the spectrum of
the system in and out of transit one can then find spectral signatures
of atoms and molecules in the planet atmosphere, from which one can
learn about its chemical composition, temperature, and more. Similarly,
one can compare the spectrum of the system when the planet is out of
transit to when it is hidden behind the star, and thus to isolate the
reflected light of the planet. Again, spectral analysis can then reveal
a wealth of detail about the planet surface and atmosphere. Such
analyses will figure prominently in future searches for “biomarkers” –
molecular spectral signatures of biological processes on other planets
(but more on that later).

Fig. 7: Extraction of a planet’s reflected spectrum |
After the first transit discovery (which was quickly followed by the
additional observations that are possible, outlined above), many
surveys to search for transiting planets among nearby stars were
initiated. The number of planets discovered in this way are currently
in the tens, and growing rapidly. Again, large planets on close orbits
are the most likely to be found, and are indeed those found: the larger
the planet, the larger its “silhouette”; the smaller the orbit, the
greater the range of inclinations around exactly edge-on that will
yield a transit; and the smaller the orbit, the shorter the period, and
hence the less time required to observe many transits and thus to
obtain a significant detection. A particularly sensitive survey is
being carried out now by the French-led CoRoT satellite. Thanks to the
photometric stability possible above our constantly changing
atmosphere, CoRoT can detect transit amplitudes of a few parts in
10,000, and already has several planet candidates of this sort. This is
already approaching the Earth-size domain; An earth transiting a sun
will cause a reduction of 1/10,000 in the observed light (Earth has
1/100 the radius of the sun). The Kepler space mission, slated for
launch in 2009, is planned to discover such “terrestrial” planets, and
not only in very close orbits. The length of the mission is such that
of order 100 terrestrial planets may be discovered (assuming, of
course, that they are really out there in sufficiently large numbers),
including some on Earth-like orbits.

Fig. 8: The Kepler Mission – Spring 2009: Will be sensitive to eclipses of Earth-like planets (about 100 expected). |
3.3 The direct imaging method
Paradoxically, the method of detecting extrasolar planets that is
conceptually the simplest, getting a picture of a star and looking for
little planets near it, is also the most challenging technologically,
with the first handful of successes being announced as I write. The
challenge lies in the huge contrast, at small angular separation,
between the brightness of a star and the very faint planet seen mainly
or entirely by the star’s reflected light. For example, the sun and
Jupiter, as viewed in visible light from one of the stars nearest to
us, would have a a brightness contrast of about 1 billion, but at an
angular separation of about 5 arcseconds (1 arcsecond is 1/3600 of a
degree). For the sun and Earth, the contrast is about 10 billion, with
a separation of only 1 arcsecond. The contrast ratio can be lowered by
a few orders of magnitude by observing in the infrared, taking
advantage of the fact that planets are much cooler than stars, and
therefore emit more of their light at those wavelengths.
Nevertheless, direct imaging remains very difficult because, even given
perfect telescope optics (which is an unachievable idealization), the
wave nature of light dictates that light from a source, no matter how
compact, when imaged through an aperture, is spread out over an
extended region in the focal plane in a “diffraction pattern”. The
angular size of the diffraction pattern is set by the wavelength. and
the size D of the entrance aperture of the instrument (e.g. the
diameter of the telescope) roughly as α = λ/D. For the largest
telescopes, with D = 10 m, imaging in near-infrared light, e.g., λ = 2
microns, we get (after converting to suitable units) α = 0.04
arcseconds, i.e., about half of the light from a nearby star in
concentrated in a spot having a radius 1/100 of the projected
separation between that star and a Jupiter-like planet. Sounds good.
Unfortunately, there is the other half of the light, which is spread
further out in the diffraction pattern. With a factor of 1 billion in
contrast in the total light between the star and the planet, the outer
parts of the star’s diffraction pattern still constitute a huge
background that drowns out the planet’s light, even at a separation of
5 arcseconds. To make things worse, any slight imperfections in any of
the optics will further enlarge and complicate the shape of the
diffraction pattern.
Despite these challenges, projects are
underway to successfully image extrasolar planets. One approach
involves specially designed “apodizing aperture masks”. When placed on
the aperture of a telescope, they will produce an azimuthally
asymmetric diffraction pattern, in which light is concentrated more
along one axis than along the perpendicular axis. One can then search
for the faint planets along the darker axis with its lower background.
Another approach is infrared interferometry, where light is combined
from several widely spaced telescopes. The telescope separation B,
which can be of order hundreds of meters, now replaces D in the
diffraction limit equation above, and the diffraction pattern can be
correspondingly more concentrated. Furthermore, using a variant of this
technique called nulling interferometry, one can search for the planet
in the regions where the combined light of the star from the various
telescopes interferes destructively, producing a relatively dark
background. By changing the separations among the telescopes, one can
null and scan for planets in different regions around the star. The
most ambitious planned mission of this type for the next decade is
Darwin, a flotilla of space telescopes flying in formation. Darwin aims
to not only obtain images of terrestrial extrasolar planets, but to
follow up with spectroscopy in search of biomarkers.

Fig. 9: The Darwin mission – 2015. An infrared spectrograph will search for biological signatures (03 , H20, CO2 ) |
3.4 The gravitational microlensing method
All of the methods outlined above can be applied only to the nearest
stars, at distances of tens of light years. In the first two methods,
we need large quantities of light in order to obtain high accuracies,
whether spectroscopic or photometric. In the direct imaging method, the
same applies, and we also need to maximize the angular separation of
the planet from its parent star and its glare. There is one
planet-hunting method, however, that is particularly suited for finding
planets around stars at distances of 10 to 30 thousand light-years,
typical distance scales across the Milky Way galaxy. That method is
gravitational lensing. Before addressing its application to planets, let us understand the basics of this effect.
Gravitational lensing refers to the phenomenon whereby the
gravitational field in the region around a mass concentration causes
light rays propagating through the region to be deflected. “Lensing”
(for short), was the first prediction of Einstein’s 1915 general theory
of relativity to be verified experimentally, during the 1919 total
eclipse of the sun. In the theory, Einstein predicted that stars that
happened to be projected near the limb of the sun would appear
displaced away from the solar limb by 1.8 arcseconds. A total eclipse,
during which the moon hides the glare of the sun and permits seeing
stars during daylight, would be an opportunity to measure the effect.
Two separate expeditions traveled to two locations in the path of
totality, in South America and Africa. The effect to be measured is
small, and had be observed in field conditions, in remote locations,
during the brief (few minute) duration of the event, and with the
limited technology of the time. In view of this, it is not surprising
that the results were ambiguous, with one experiment reporting
agreement with Einstein’s prediction, and the other not. Nevertheless,
Arthur Eddington, the prominent physicist of the time and a champion of
Einstein’s work, after analyzing the results declared that the theory
had been vindicated. Although Einstein, by then, was well known among
physicists, he was not a public figure. However, the eclipse story
reached the headlines of several major newspapers who turned Einstein,
literally overnight, into the cult figure he remains today. Thus,
lensing is actually what made Einstein famous.

Fig. 10: ….Lensing is actually what made Einstein famous |
The light rays from any source of light will be deflected (i.e.
“lensed”) by any intervening mass lying close to the line of sight of
an observer to that source. In particular, the mass of a star can serve
as a lens that deflects the light of another star that happens to lie
behind it, if they are at suitable distances from each other and from
an observer. When the source star is exactly behind the lens star, the
light of the source star, as viewed by the observer, will be distorted
into a perfect ring shape – an “Einstein ring” – around the lens star.
If the lens star is distant enough, and hence subtends a small enough
angle to the observer to avoid hiding the ring, the ring will, in
principle, be observable. Suppose the following: the lens star has the
mass of the sun (which is is a common type of star, as Bruno guessed);
the source star is at a distance of 30,000 light years (the distance to
the center of our galaxy); and the lens star is halfway in between.
Then, the angular radius of the Einstein ring turns out to be about one
milli-arcsecond. If the alignment between source, lens, and observer is
not quite perfect, the symmetry of the problem is broken, and the ring
breaks up into two distinct arcs straddling the lens. As the alignment
is further worsened, both arcs become progressively shorter, with one
becoming very faint and eventually disappearing, with the other
approaching the size and location of the actual source. (You can see
all of this by looking at a light source through the base of a wine
glass, which has optics similar to that of a gravitational lens.)

Fig. 11: Illustration of light bending by a gravitational lens. Left: side view of the light-ray trajectories from the source (red) and its two apparent lensed images (blue). Right: Appearance on the sky of the lensed arcs (blue), relative to the true position of the source (red), which is no longer seen. |
The
regime of lensing of stars by other stars is coined “microlensing”. At
any given moment, from our vantage point in our Milky Way galaxy, such
stellar alignments that are good enough to produce perfect or
near-perfect Einstein rings are very rare, with about one in a million
stars lensing another star at a given moment. However, due to the
orbits of the stars (including the sun) around the Milky Way’s center,
it is a different rare star every time that crosses close enough to the
line of sight to another star for the effect to occur. If we had
visual-band telescopes with milli-arcsecond resolution (which we do
not, yet), and we monitored such a source star, we would see its image
gradually getting tangentially stretched around the point where the
lens mass is (we need not necessarily see the lens star). At the same
time, a counter-image would appear and gradually grow on the opposite
side of the lens. If, at the moment of closest projected approach,
there were near perfect alignment, then the two arcs would merge into a
full, or nearly full Einstein ring. Then, as the source and lens
continued on their relative trajectories on the sky, the lens would
split again into two images, and the whole movie would play itself in
reverse as the source gets further and further away on the sky from the
lens.

Fig. 11a: Left: Schematic diagram of the trajectory, projected on the sky, of a source star behind a lens. Right: Three possibilities for the brightening and fading behavior as a function of time of the source star, as it passes behind the lens. |
While the splitting and Einstein rings of
microlensing are currently un-observable, a secondary effect actually
is. What the lens is effectively doing to the source is magnifying it,
albeit, in a rather peculiar way. This means that light that was
intended for someone else is reaching you. As a result, even if you do
not see the ring and the image splitting, but just monitor the total
amount of light from your source, you will see it brighten, reach a
maximum corresponding to the time of best alignment, and then return
symmetrically to its normal brightness. The shape of the rise and fall
as a function of time is very particular, and can be used to
distinguish such a “microlensing event” from other variable
astronomical phenomena. The timescale for such an event depends on the
several parameters in the problem, but is typically of order weeks.
Thus, a microlensing event can be identified by monitoring the light
from many stars (of order several million need to be followed in
order
to have a fair chance of observing the phenomenon), and looking for the
specific brightening and fading behavior described above.

Fig. 12 and 13: Einstein's notes from 1912 (top) and 1936 (bottom) with his calculation of the geometrical optics of star-star lensing |
Einstein was aware of all of this from the start. His notes from 1912,
3 years before he published general relativity, show the sketches and
the basic equations for the lensing of a star by another star. However,
for over two decades these results remained unpublished. In 1936, when
already living in Princeton, Einstein was approached by an engineer and
amateur physicist, Rudy Mandl who, reading about Einstein’s theories,
had conceived independently of the possibility of microlensing.
Einstein confirmed to Mandl that, in principle, such an event could
occur, but that in practice it was unobservable, and hence there was no
point in publication. Apparently, Mandl persisted in pushing Einstein
to publish a paper on the effect, until Einstein reluctantly agreed. In
the paper, Einstein emphasized that “There is little chance of
observing this phenomenon.” And in a private note to the editor of the
journal, he condescendingly wrote, “Let me thank you again for your
help with the small publication that Mister Mandl has squeezed out of
me. It is of little value, but it makes the poor fellow happy.” It
would take over four more decades until lensing became an active
observational field, but Einstein’s “Mandl-driven” 1936 paper launched
a considerable body of theoretical work on the many possibile
manifestations that lensing could take, and the astrophysical and
cosmological information that could be revealed by observing it.

Fig. 14: Hubble Space Telescope image of a foreground galaxy (yellow) lensing a background galaxy (blue) that is directly behind it into a near-perfect Einstein ring. |
Lensing by the sun,
mentioned at the start, has by now has been confirmed by many
experiments to obey general relativity’s prediction to great precision.
The first additional astronomical gravitational lensing phenomena were
discovered starting in 1979, with hundreds of more examples turning up
in the subsequent decades. These cases involved galaxies, or their
sometimes active central regions, called quasars, serving as light
sources and being lensed by the masses of entire intervening galaxies
or clusters of galaxies. For the masses and distances involved in such
cases (1010 to 1012 solar masses, and billions of light years,
respectively) Einstein rings and related phenomena occur on angular
scales of one to a few tens of arcseconds, resolvable by telescopes on
Earth, and even better by telescopes (such as Hubble) above the Earth’s
distorting atmosphere. The first microlensing (i.e., of stars by stars)
events were announced in 1993. By now, thousands of microlensing events
have been detected and measured based on the particular symmetric
brightening and fading behavior of a source star.
Where, then,
did Einstein go wrong in his assessment of the observability of
gravitational lensing? In 1936, it was indeed impossible to monitor
many millions of stars for periods of years, in order to find the
handful undergoing transient microlensing magnification. Einstein could
hardly have foreseen the development of large digital imaging arrays
combined with modern computing power, which permit searching
automatically for these rare events. In fact, even when the idea of
microlensing surveys was first proposed by Paczynski in 1982, it was
considered unfeasible, but Moore’s Law of exponentially increasing
computing power turned it into a reality within less than a decade.
Returning to the issue of planets, imagine now that a star is lensing
the light of another star that is behind it into a complete, or nearly
complete, Einstein ring. If the lens star has a planet near it, and the
light rays producing the ring image happen to pass near that planet,
the planet’s gravitational field will cause an additional deflection of
the rays. When we monitor the light from the source star as it passes
behind the lens, we will see deviations from the simple symmetric
brightening and fading produced by a single, isolated star. This
perturbation in the brightness as a function of time, caused by the
planet, can assume a rich variety of forms, depending exactly on the
mass ratio of the lens star and its planet, and on the location of the
planet relative to the path of the source star in the background. But
in general, these perturbations signaling the presence of a planet or
planets will be brief compared to the entire lensing event, often
lasting only a few hours. Thus they will be “caught” only if the event
is monitored around the clock, with few gaps. “Large magnification
events”, in which the main lens attains near perfect alignment with the
source, will be particularly sensitive to planets, because the Einstein
ring encompasses a large region around the lens star, and hence planets
lying over a large region will cause a conspicuous perturbation to the
ring. Even Earth-mass and lighter planets, if they lie close enough to
the Einstein ring, will cause a significant perturbation and can be
detected.

Fig. 15 and 16: Top (arrowed): the microlensing event OGLE-2005-BLG-390; Bottom: the event's brightness versus time, showing (inset) the deviation caused by a Jupiter-mass companion to the main lens star. |
Over the past years, two projects, with the acronyms OGLE (Optical
Gravitational Lens Experiment) and MOA (Microlensing Observations in
Astrophysics), have been monitoring the brightnesses of tens of
millions of stars in the direction of the center of the Milky Way, in
search of microlensing events. Because of the large density of stars in
this direction, there is the highest probability on the sky of close
line-of-sight alignment between two passing stars, and indeed almost
all of the thousands of events that have been discovered have been
found in this direction in the sky. Considering the facts above,
several years ago a collaboration of astronomers with the acronym
MicroFUN (Microlensing FollowUp Network, of which I am a member) set
out to find planets by means of microlensing using the following
strategy. Wait for OGLE or MOA to alert that a particular lensing event
may have a large magnification (and thus may be highly sensitive to the
presence of planets). Track the brightness changes of that event over
its peak, using a network of telescopes around the globe, in order to
get the most complete time coverage, with the fewest possible gaps (in
which the signature of a planet might get lost). That strategy has
proved to be very effective. Over the past 5 years, 9 extrasolar
planets have been found through microlensing, with 8 involving
observations by MicroFUN.
Contrary to the “strange” planets
found by other techniques, the planets turning up by the microlensing
searches so far seem to be quite “normal” planets – mostly Neptune-mass
to Jupiter-mass planets on Jupiter-like orbits. More specifically, the
planets being discovered by microlensing are generally in the region of
the “snowline” of their parent stars. The snowline is the distance from
a star beyond which the temperature is low enough for water vapor to
condense into ice (this depends also on the pressure of the water
vapor). According to the most popular scenario for planet formation,
the availability of water ice in large quantities just outside the
snowline allows the formation of relatively large agglomerations of
"planetessimals" composed of rock and ice. These, in turn, serve as
cores that are massive enough to accrete, and hold on to, a large mass
of gas, leading to the formation of gas giants. As one goes to large
distances, less raw material is available, and progressively smaller
gas giants are formed. This explains the mass sequence seen in the
solar system, with the first and most massive gas giant, Jupiter, just
outside the snowline, and progressively smaller gas giants at larger
distances from the sun – Saturn, Uranus, and Neptune. Inside the
snowline one finds only the small rocky planets: Mercury, Venus, Earth,
and Mars.
Stars that are less massive than the sun are cooler
and less luminous, and hence have snowlines at smaller radii than the
sun, and vice versa for more massive stars. The fact that
microlensing-dicovered planets have been found largely near the
snowlines of their planet stars is the result of a fortunate
coincidence: The Einstein-ring radius of a solar-mass star serving as a
lens at a typical distance in the Milky Way happens to be similar to
the radius of the snowline of a solar-mass star. Since the
Einstein-ring radius is proportional to mass (to its square root,
actually), lower-mass stars will have both smaller Einstein rings and
smaller snowline radii. And since microlensing is most sensitive to
planets in the region of the Einstein ring, it is no surprise then that
most of the microlensing-discovered planets are turning up near the
interesting region of their parent stars’ snowlines.
But do
these “normal” extrasolar planetary systems resemble our own in other
respects as well? Microlensing has recently provided a first,
tentative, “yes” to this question. In April 2006, the MicroFUN
collaboration monitored a microlensing event (with the uninteresting
name OGLE-2006-BLG-109; this was the 109th event discovered in 2006 by
the OGLE network in the direction of the “bulge” of the Milky Way), an
event that promised to rise to large magnification and therefore to be
sensitive to planets around the lens star. Early on, indeed,
perturbations in its brightening pattern indicated the presence of a
Saturn-mass planet. However, once all the data were collected and
analyzed, it became clear that they could not be explained solely with
that single planet. The collaboration’s Science journal article by
Gaudi et al. (2008) showed that another, Jupiter-mass planet on a
closer orbit was required by the data. The signature of the “Jupiter”
in this first discovery via microlensing of a planetary system (i.e., a
system with more than one planet) was visible only for a few hours, at
a time when all but one of the 12 telescopes in the network were in
daylight, and hence could not observe. The information on this second
planet came solely from the Wise Observatory 1-meter telescope in
Israel. The event was overall observed well enough that it permitted
determination of the systems’ parameters better that any previous
microlensing planet discovery. The system’s masses, separations, and
distance to Earth, can all be measured to an accuracy of about 10%.

Fig. 17: Brightness versus time (in days) of the microlensing event OGLE-2006-BLG-109, the first planetary system discovered via microlensing. Inset shows the feature due to the "Jupiter" in the system. Red points are measurements from Wise Observatory. |

Fig. 17a: Wise Observatory, near Mitzpe Ramon, Israel. |

Fig. 18: The planetary system, OGLE-BLG-109, is very reminiscent of the solar system |
The picture that emerges (Fig. 18) is of a planetary system very
reminiscent of the solar system. The mass ratio (0.37) of the “Saturn”
and the “Jupiter” in the system is like the mass ratio (0.30) of Saturn
and Jupiter in the solar system. The distance ratio of the two planets
from their star (0.50) is similar to that of Saturn and Jupiter (0.55).
But in terms of absolute values, everything is roughly scaled down by
one half: the star has one-half the mass of the sun; the planetary
distances are close to one half the distances of Jupiter and Saturn to
the sun; and the masses of the planets are smaller than Jupiter and
Saturn. So, effectively, this is a scaled-down solar system. This is
exactly what one would expect from the standard theory of planetary
formation described above: a lower-mass star would result in a
closer-in snowline, and therefore the same descending sequence of gas
giants, but closer in. With just one example so far, it is much too
soon to jump to conclusions. But finding (as soon as we had available a
technique than could find) a system that resembles the solar system so
nicely, with the expected scaling, hints that the Copernican principle
– we are not in a privileged or special position (which in the end, was
all that Giordano Bruno was invoking) – has been successful yet again:
yes, it seems quite possible that many or most stars have planetary
systems very similar to that of the sun.
We cannot say
whether or not the OGLE-2006-BLG-109 system includes additional
planets, and specifically an “Earth”, perhaps also scaled down in mass
and orbit. This specific event did not have the sensitivity to discover
such an inner planet. However, earth-mass planets, if they exist, will
be discovered in the near future, whether by microlensing or by one of
the other methods. The progress of the past few years and the near-term
future exoplanet projects tell us that a full picture of the frequency
of occurrence, the characteristics, and the variety of types, of
planetary systems is just around the corner.
4. The Next Step: Astrobiology
Assuming we find extrasolar terrestrial planets that seem to be, in
principle, capable of sustaining life, the next obvious step will be to
actually search for signs of life. The fairly new science of studying
life outside the Earth is called Astrobiology. How will we go about it?
Beyond the bodies in the solar system, for which life-searching
experiments can be done by robots and space probes, searches for life
on extrasolar planets will always involve remote sensing. The simplest
was to find evidence of life may be by life’s indirect effect on the
environment. On Earth, the oxygen in the atmosphere is of biological
origin, having been first released by cyanobacteria 2-3 billion years
ago, and later boosted by blue-green algae and plants. Without life,
oxygen in the atmosphere would decrease to very low levels within a few
million years, similar to the situation in Mars today. Thus the first
biomarkers that will be searched for are oxygen, both as diatomic (O 2)
and ozone (O 3) molecules. Finding such molecules in an exoplanet’s
atmosphere together with water vapor and CO 2, in proportions similar to
Earth, would be strong evidence for the presence of life. The spectral
signatures of these atoms in an atmosphere can be detected either in
the transmitted light or the reflected light of a transiting planet
(see above). Such measurements should be possible within a few years
with the James Webb Space Telescope, NASA’s replacement for Hubble. The
same spectral biomarkers can be found by analyzing the light of planets
isolated from the glare of their parent stars by means of
interferometric imaging.

Fig. 19: Simulation of the transit spectrum of an Earth-like planet. |
In terms of more direct signs of life, optical imaging of the Earth’s
surface from artificial satellites easily reveals vegetation by means
of a spectral signature called the “red edge”, due to chlorophyl, at
700 nm. This feature is strong enough that it could be detected on
Earth-like planets among those that the Darwin mission finds. In
principle, one could do much more. Remote sensing of the Earth is a
mature science, and Earth-imaging satellites can routinely identify and
measure the density of specific plant species based on their spectral
signatures. Doing the same for an extrasolar planet at a huge distance
is simply a question of having a sufficiently strong signal. In
practice, going to such levels of detail in analyzing life on other
planets is unfeasible with currently conceivable technology. The
telescope sizes (and costs) required to gather enough of the feeble
light are impractical. We should, however, remember the lessons of the
past; what is impractical today may become fairly easy with the advent
of new, yet unimagined, technology.
A possibly more serious
problem is the non-Copernican, anthropocentric aspect of the strategies
outlined above for searching for signs of life. Of course, it would be
amazing if we do find the signature of chlorophyl in a distant planet.
But should we expect it? And if we do not see it, will that exclude the
presence of life there? Probably not. This is a lesson that has been
learned in recent years, actually by studying life here on Earth. A
huge variety of previously unknown organisms, mostly microbial, is
being discovered, not only in normal environments such as the oceans,
but also in the most unexpected of places – near undersea oceanic
vents, in deep underground aquifers, within rocks, in ice, and in hot
acidic lakes. Each of these “extremophile” life forms has adapted to
exploit a different energy source that is available in its particular
niche.

Fig. 20: Top: Mponeng gold mine in South Africa; Bottom: microscope image of an extremophile bacterium found in the mine (Chivian et al., 2008). |
For example, Chivian et al. (2008) have discovered a self-sustaining
community of bacteria in the Mponeng gold mine in South African at a
depth of 3 km. These organisms, which have been isolated from the
Earth’s surface for millions of years, derive their metabolic energy
indirectly from the natural radioactivity of the surrounding rock. The
radioactive radiation dissociates molecules of ground water to hydrogen
and oxygen. The hydrogen combines with sulfur to form compounds that
the bacteria feed on. It seems that wherever there is liquid water (at
least some of the time), a source of energy, and some common chemical
compounds, an organism has developed to exploit it. On the one hand,
this bodes well for finding life in remote environments that are
different from those we traditionally consider as hospitable to life.
On the other hand, it raises the problem of how to recognize remotely
the signs of activity by such life forms, which can be so different
from those we know on Earth.
5. Why Finding Life (or not) Matters
The popular concept of extraterrestrial life has not changed much since
Lucian’s second-century fantasies. It almost always consists of a
Universe densely populated by sentient beings, more or less
technologically sophisticated, but remarkably similar to humans in
terms of body plan and all aspects of behavior. This concept is
constantly reinforced by a huge entertainment industry, but also by
governments (mainly the US), who are aggressively promoting and
pursuing the idea that humanity’s “destiny” is to colonize space. The
largest and most expensive space project of recent years is the
International Space Station. Although the word “science” is often heard
in the context of the space station, there is actually little science
that is carried out there, and the main work of the astronauts is home
maintenance. The express purpose of the project is to prepare for the
colonization of the moon and Mars. Such colonization, again, has little
to do with science. Scientific exploration of the solar system can be
done much more effectively, safely, and inexpensively with robotic
probes than with astronauts. But NASA's great reputation and the mix of
science with manned space flight certainly end up promoting in the
public perception the plausibility of Star Wars imagery.

Figs. 21-24: Some popular conceptions of extraterrestrial life. |
In reality, extraterrestrial life, if it exists and we find it, will
certainly not be of the “Mars Attacks” film sort. We can look at the
evolution of life on Earth for guidance. Life on Earth emerged perhaps
as soon as the young planet cooled enough, after a billion years or so,
and hence Earth has been inhabited for most of its 4.5 billion year
history. However, land plants and insects have been here for only the
last 10% of the time. Reptiles have existed for only 7% of the time,
and mammals for only 4%. Humans have been around for only of order
100,000 years. Civilizations have existed for less than 10,000 years,
of order one millionth the age of the Earth. And the capacity for radio
communication and space travel have been here only 50–100 years, of
order one part in one-hundred-million of Earth’s history.
We
do not know, of course, for how much longer there will be humans on
Earth, doing the things we do today. The possibilities for human
extinction through war, artificial, or natural global catastrophes
(climate change, disease, asteroid impacts) are numerous. Looking at
the history of other species and at the extinction record, it is hard
to imagine that humans in their present form will still exist on
geological timescales into the future. If so, this would mean that, to
find extra terrestrial creatures of the sort we see in the movies
(i.e., very similar to us), we would have to search among one-hundred
million earths. Even if earths are abundant around stars, and evolution
always proceeds as it did on Earth (which is contrary to the whole
principle of randomness behind evolution itself, and therefore is
highly unlikely), there are only about one-million stars within 300
light years of the sun. It is only within such a distance that there
is any hope, in the foreseeable future, of remotely sensing any
evidence for life, using the various techniques outlined above. So,
just from these simple considerations, it is almost certain that
extraterrestrial life, should we find it, will be microbial, or not
much more complex than that.
If human extinction of the
“back-to-square-one” kind is avoided and evolution continues at the
pace it has, then our descendants, and those of similar species on
other planets are likely to be so highly advanced compared to us that
we face a new problem: next to them, we would be like microbes.
Considering mutual visits and communication between galactic
civilizations, it is unlikely that a species as advanced as we might be
a billion years hence would have any interest in communicating with
“microbes” like us.
Despite these sobering facts, the search
for extraterrestrial life is among the most exciting human endeavors
ever, and I believe it must be pursued. The reason has to do with the
very existence of life on Earth. The emergence of the first life forms
on Earth is a complete mystery. Although some ideas are emerging,
creating the first structure that could be called a living organism,
one that then reproduces, multiplies, and evolves, still seems like an
insurmountable challenge. Was “abiogenesis” a wildly improbable
accident that occurred only once, here on Earth? Or is the appearance
of life unavoidable whenever the appropriate, but altogether common,
conditions exist? There are hints pointing in both directions.

Fig. 25: Amino-acids in living organisms are usually “left-handed”, while sugars are “right-handed” |
Amino acids are the components of proteins, which, in turn, are the
building blocks of living organisms. When synthesized in the lab, amino
acid molecules are created in similar numbers in two mirror forms that
are chemically equivalent, called right-handed and left-handed.
Left-handed amino acids can combine only with other left-handed amino
acids to build proteins, and the same is true for right-handed ones. A
creature composed of right-handed amino acids would be able to eat only
organisms that are right-hand based, and to use their amino acids in
order to grow and reproduce. (In fact, opposite-handed organisms would
likely be poisonous to it). If life emerged quickly and spontaneously
in the young Earth, wherever conditions were suitable, we would expect
to see both right-hand-amino-acid and left-handed amino-acid life
forms. All of the above applies also to sugars. However, all known
organisms on Earth are based on left-handed amino acids and
right-handed sugars. This suggests that all organisms on Earth are
descended from one single “mother” cell, which happened to have this
handedness of amino acids and sugars. It would seem, then, that the
emergence of such a viable cell is something exceedingly rare and
improbable, that occurred just one single time in Earth’s history.

Fig. 26: ATP (adenosine triphosphate) is the "molecular unit of currency" of intracellular energy transfer in all living organisms on planet Earth. |
Another hint in this direction comes from the fact that all living
organisms, without exception, use the adenosine triphosphate (ATP)
molecule as an energy “currency” for managing and transferring energy
in the cell. One could imagine many different molecular mechanisms for
energy manipulation that would have developed in organisms that had had
an independent start. The universality of ATP again hints at a single
ancestor. On the other hand, the speed with which life appeared on
Earth argues for the “inevitable life” option. Perhaps the specific
handedness of amino acids and sugars was somehow enhanced in the
“primordial soup” out of which the first organisms formed. And, perhaps
ATP gave our microbial ancestors some evolutionary advantage over other
species using different energy currencies, and those species all became
extinct.
The search for extraterrestrial life offers a way
to address this mystery, which is at the heart of understanding life
itself. If, over the next years, we discover a Universe teeming with
life, albeit primitive, it will be a clear verdict that nature forms
life “easily” under suitable conditions, even if we do not understand
the process at present. Alternatively, a complete absence of what we
could call life on other planets, after excluding also the possibility
of exotic and difficult-to-identify life forms, different from those
most familiar from Earth, would also have profound implications. It
would tell us that, at least in our local neighborhood of stars, we are
truly alone, and that we are the result of a highly improbable chain of
events, a “miracle”.
6. Some Final Thoughts
We
have seen that Giordano Bruno, with an Olympian intuition, foresaw in
the late 16th century many of the facts that have been established only
in the last few decades and years. However, during his times, Bruno’s
ideas, coupled with a tendency to get into trouble, led him to the life
of a fugitive, drifting across the capitals of Europe and constantly
making new enemies. The Inquisition eventually caught up with him,
imprisoned him for 8 years, convicted him of heresy, and burned him at
the stake in Rome in 1600. There is debate among historians about the
weight of Bruno’s astronomical ideas in sealing his fate, compared to
that of his heretical opinions on other matters of Church dogma. But we
can probably be confident that his astronomical ideas did not help him.
Returning
to “De L’Infinito Universo et Mondi”, we find in the treatise, along
with the dialogue exposing the ideas that have been discussed above,
three “sonnets” by the author, as sometimes found in Renaissance
essays. Written in 1584 in London, the third sonnet evokes an eerie
feeling that, among all that Bruno foresaw, he foresaw also his own
final fate. One cannot help imagining Bruno reciting the poem 16 years
later in his dungeon cell in Rome, as he awaits his execution. In
beautiful verse, he expresses the humanistic Renaissance idea of the
power of thought, observation, and reasoning to transcend all physical
obstacles and distances, an idea that I feel is still at the heart of
basic science, and of astronomy in particular. With no humility
whatsoever, Bruno concludes by notifying his contemporaries that he has
seen much further than they ever will. Indeed!
I reproduce below the Italian text, followed by my attempt at an English translation.
E chi mi impenna, e chi mi scalda il core? Chi non mi fa temer fortuna o morte? Chi le catene ruppe e quelle porte, Onde rari son sciolti ed escon fore? L’etadi, gli anni, i mesi, i giorni e l’ore, Figlie ed armi del tempo, e quella corte A cui ne ferro, ne diamante son forte, Assicurato m’han dal suo furore. Quindi l’ali sicure a l’aria porgo; Ne temo intoppo di cristallo o vetro, Ma fendo i cieli e a l’infinito m’ergo. E mentre dal mio globo a gli altri sorgo, E per l’eterio campo oltre penetro: Quel ch’altri lungi vede, lascio al tergo.
And who delights me, and who warms my heart? Who makes me fear neither fortune nor death? Who breaks the chains and those doors, through which few are released and exit? The seasons, the years, the months, the days, and the hours, Daughters and weapons of time, and that court Against which neither iron nor diamond is strong, They have safeguarded me from the fury. Therefore, confident wings to the air I spread, I fear not obstacles of crystal or glass, But cleave the heavens and toward the infinite I rise. And while from my sphere to the others I surge, And through the ethereal field I further penetrate, That which others see far away, I leave behind me.
I thank Giorgio Dieci for pointing out Giordano Bruno’s beautiful sonnet, and Omer Bromberg for Lucian’s “True Story”.
For further reading
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