
Issue of
June 7, 2000
 

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Black holes -- in the
laboratory?
Physicists
hope to simulate 'event horizon'
Einstein's General Theory
of Relativity predicts the existence of black holes --
astrophysical objects so dense that even light cannot
escape from them. The boundary around the black hole
(where the light cannot escape) is called the "event
horizon." In 1974, Stephen Hawking of Cambridge
University theorized that a black hole is not entirely
black, but could actually emit "blackbody," or
"thermal," radiation (the kind of radiation
that also occurs when the stove is red hot). Hawking said
this radiation has a well-defined temperature that is
proportional to the gravitational force at its event
horizon.
Using high-intensity
lasers, scientists hope to simulate a black hole event
horizon in a laboratory within the decade, something that
has never been done before. At the June 6 meeting of the
American Astronomical Society in Rochester, N.Y., Dr.
Pisin Chen from the Department of Energy's Stanford
Linear Accelerator Center (SLAC) at Stanford University
presented a theory that supports the possibility of such
lab experiments. Chen said that an electron under violent
acceleration, such as that driven by an ultra-intense
laser, would quiver under a "heat bath" of
photons that surrounds it and thereby induce a much
stronger Hawking-like radiation (often called Unruh
radiation) that theoretically could be observed in the
lab.
"Hawking's finding
uncovered a deep connection between gravitation, quantum
mechanics and thermodynamics," Chen said, "and
if we can simulate this phenomenon in the lab, it will be
a major step toward understanding the nature of event
horizons." Such an experiment could take place at a
variety of laboratories.
Under normal
circumstances, a vacuum is a space in which there is no
matter. But at the quantum level, the vacuum is full of
particles and antiparticles that constantly appear and
disappear. The Heisenberg uncertainty principle allows
these "virtual" particles and antiparticles to
emerge from the vacuum for a brief moment and disappear
back into the vacuum again without violating the energy
conservation law. According to Hawking, if a
particle/antiparticle pair is created near the event
horizon of a black hole, gravity will pull one of the
particles into the hole permanently, while the other
particle (or antiparticle) can escape, or be
"radiated," from the black hole. "In this
way the black hole could radiate something from
nothing," said Chen.
The typical Hawking
radiation temperature from solar-mass-sized black holes
is as low as 0.0001 degree Kelvin (close to absolute
zero, and radiation becomes fainter as the temperature
decreases). Though of fundamental importance in physics,
Hawking radiation is very hard to observe directly from
space. One curious feature about Hawking radiation is
that the temperature is inversely proportional to the
mass of the black hole. Thus, the only black holes that
might render detectable radiation would be primordial
"mini-holes" that may have formed shortly after
the Big Bang. Such black holes would have a mass of 1015
grams but a size smaller than an atom. The possibility of
detecting such mini-holes, however, is uncertain.
In 1976, Bill Unruh of the
University of British Columbia showed that an accelerated
observer would experience a similar "heat bath"
of photons around him or her, due also to the existence
of an event horizon. The temperature of the heat bath
follows the same Hawking temperature formula, except that
instead of the gravitational force, it is proportional to
the magnitude of the observer's acceleration. Although
the Unruh effect induced by acceleration is not precisely
the Hawking effect from black holes, it nevertheless
shares many common characteristics. It is therefore an
intriguing idea that the Hawking effect could be studied
using violent acceleration in the laboratory setting,
since the temperature associated with the Unruh effect
can be much higher if the observer is intensely
accelerated.
Chen, whose work at SLAC
is supported by the Department of Energy, theorized that
it should be possible to detect the Unruh radiation
emitted by electrons that are accelerated by
ultra-intense lasers. One major challenge with detecting
Unruh radiation is that enormous accelerations are
required to produce sufficient radiation. For example,
one would need to accelerate a particle over 1020 meters
per second squared (m/sec2) to generate a temperature of
1 degree Kelvin. It turns out that state-of-the-art
lasers can deliver pulses of less than a picosecond
(one-trillionth of a second) with petawatts (1015 watts)
of power. These technologies can in principle accelerate
electrons over 1025 times the acceleration due to the
gravity on Earth's surface, or 1028m/sec2, more than two
orders of magnitude higher than previous experimental
proposals.
Since the 1980s several
groups have proposed experiments to detect Unruh
radiation. Unruh himself suggested that sound waves
propagating in a supersonic fluid behave similarly to
quantum fields propagating in the vicinity of a black
hole. The late John Bell of the Geneva-based European
Organization for Nuclear Research (CERN) and Jon Leinaas
of the University of Oslo in Norway suggested that the
known polarization effect of high-energy electrons in
circular accelerators is actually a manifestation of the
Unruh effect. Joseph Rogers of Cornell University
proposed that a magnetically confined electron in a
so-called Penning trap would give the Unruh signal.
Meanwhile Eli Yablonovitch, now at the University of
California-Los Angeles, proposed that Unruh radiation
would be produced when a gas is suddenly ionized to
become a plasma. In addition, Simon Darbinyan of the
Yerevan Physics Institute in Armenia and co-workers
suggested that Unruh radiation could be emitted by a beam
of particles that channel through a crystal lattice.
In all these proposed
experiments, however, the Unruh signal would be buried
under much stronger background signals, a problem that
Chen has managed to circumvent. In the idea proposed by
Chen, electrons are instantly accelerated and decelerated
in every cycle by a standing wave formed by two
counter-propagating, ultra-intense laser pulses. He
proposed to detect the Unruh radiation from a minute
change of the known classical Larmor radiation emitted
when an electron is accelerated. Despite the high
acceleration produced in the petawatt laser, the total
Unruh radiation power is still found to be smaller than
that from the Larmor radiation. However, Chen calculated
the angular distribution of both types of radiation and
found a "blind spot" (along the direction of
acceleration) where the Unruh signal dominates the Larmor
signal.
The proposed Linac (an
abbreviation for Linear Accelerator) Coherent Light
Source (an X-ray free electron laser, or FEL) at SLAC,
and other FEL facilities, would have the capacity for
scientists to conduct such an experiment. Construction of
the Linac Coherent Light Source (LCLS) could start as
early as 2003, with completion in 2006. Petawatt-class
"table-top" lasers currently under development
in various laboratories also might be invoked for such a
test.
It has yet to be seen
whether this new approach proposed by Chen can eventually
provide insights into the Hawking effect. Chen admitted
that his ideas also involve several theoretical and
technical assumptions that need further testing.
"Given the importance of the Hawking effect, I think
that continuing the search for Hawking-like signals in
the laboratory setting is a very worthwhile effort,"
he said. SR
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