Experiments Detail How Powerful Ultrashort Laser Pulses Propagate through Air
Thanks to self-focusing, laser pulses can be launched upward into clouds where they can be used to measure pollutants.
Like many things in physics, refractive index isn't as simple as we
learned in high school. In addition to the familiar constant is a term
that depends on intensity: n = n0 + n2
I.
This intensity dependence, known as the optical Kerr effect, underlies
the phenomenon of self-focusing. If a beam of light is brighter in the
center than at the edges—as most are—the center will encounter a bigger
refractive index and slow down. Wavefronts that start out planar will
therefore collapse about the center. A tighter beam results.
For air, n2 is so tiny that the power must exceed
several gigawatts for self-focusing to kick in. Only strongly focused
or ultrashort-pulse lasers can provide such prodigious power. (For more
on powerful ultrashort lasers, see the article by Gérard Mourou,
Christopher Barty, and Michael Perry, Physics Today, January 1998, page
22.*)
In 1994, soon after ultrashort lasers came on line, Mourou and his group
at the University of Michigan fired 10-GW, 200-fs pulses across their
lab through air. Their goal was to mimic a pulsed microwave radar with
light. Along with the expected self-focusing, they discovered something
else.1 To their surprise, the narrowed pulses,
which they termed filaments, acted as their own waveguides, retaining
their width and propagating across the lab for tens of meters.
In this and other experiments, it became apparent that plasma formation
plays a key role in the filament propagation. Self-focusing increases
the intensity, which leads to greater self-focusing, which further increases
the intensity. What halts this runaway process is ionization.
When self-focusing pushes I above 1014 W cm-2,
multiphoton ionization creates a plasma, whose refractive index, being
less than air's, causes the beam to defocus. Without self-focusing to
boost it, I drops below the ionization threshold. The Kerr effect
switches back on, and self-focusing resumes. The filaments' propagation
depends, therefore, on a quasi-dynamic equilibrium between Kerr focusing
and plasma defocusing.
At high intensities, slight irregularities in the beam profile act as
seeds for the filaments, which travel together in parallel. This phenomenon,
known as modulation instability, causes each stable filament in a 100-fs
beam to draw roughly one millijoule of energy from the initial pulse.
In a sense, the filaments are quantized.
Now, a more detailed view of filament propagation has been obtained,
thanks to experiments at the Ecole Nationale Supérieure de Techniques
Avancées (ENSTA) and the Ecole Polytechnique in Palaiseau, France.
Stelios Tzortzakis, his thesis adviser André Mysyrowicz, and their
colleagues Michel Franco and Bernard Prade have followed the self-focusing
process as it happens. Their experiments reveal that filaments propagate
by carefully husbanding their energy through merging.2
If a beam breaks into two filaments, those two filaments will combine
before the intensity of either drops below the threshold for self-focusing.
The ability of self-focused filaments to propagate without the usual
broadening due to diffraction makes them attractive for applications.
Already, as Figure 1 shows, filaments have been fired through the atmosphere.
A Franco-German team is using the filaments to remotely sense atmospheric
pollutants. And more speculative applications such as lightning channeling
and cloud seeding are under investigation.
Measuring powerful femtosecond light pulses is difficult because of
the high intensities and ultrashort timescales, but it's straightforward
in principle. Figure 2 shows the setup used by the ENSTA investigators.4
The laser, a 1-kHz Ti:sapphire oscillator amplifier system, emits pulses
that last 50 fs and have a wavelength of 810 nm. How the pulses change
shape with time and distance is measured by a charge-coupled device camera,
which records a small fraction of the beam that bounces off a reflective
glass plate. The plasma's conductance—a main ingredient in models—is
measured by a resistive circuit that shorts when the plasma spans the
two electrodes.
Figure 3 encapsulates the main finding of the ENSTA team. There we see
that when the power is high enough to form filaments, those filaments,
after propagating a few meters, fuse to form a single filament, which
continues to propagate.
To model the formation and merging of filaments, the ENSTA team enlisted
the help of Luc Bergé and Arnaud Couairon, two theorists from the
French Atomic Energy Commissariat at Bruyères-le-Châtel.
Bergé and Couairon's numerical model confirmed the basic picture
and predicted the size, shape, and duration of the filaments, as well
as the plasma properties and the criteria for whether filaments merge.
Bergé and Couairon's model followed an approach devised two years
ago by the University of Arizona's Michal Mlejnek, Miroslav Kolesik, Jerry
Moloney, and Ewan Wright.3 (Mlejnek now
works for Corning Inc.) As their starting point, the Arizona group used
the nonlinear Schrödinger (NLS) equation. "The NLS is a natural,"
explains Moloney. "It describes weakly nonlinear dispersive behavior in
any physical system—optical propagation, water waves, or plasma instabilities
in Langmuir turbulence."
Like the self-focusing itself, solutions to the NLS evolve toward a
singularity unless something steps in to avert that fate. In the Arizona
model, multiphoton ionization, as embodied in a plasma model, plays the
role of moderator.
Averting the singularity is more than a matter of mathematical neatness.
Multiphoton ionization costs less energy than the processes that would
occur if self-focusing proceeded further. Filaments are able to propagate
because multiphoton ionization causes diffraction that temporarily spreads
the filaments' energy but doesn't absorb much of it.
Foreshadowing Tzortzakis's experiments, the Arizona model produced filaments
that propagated, merged, and then continued to propagate. Unlike the ENSTA
experiments, the Arizona model wasn't constrained by the output power
of real lasers and could produce up to 30 filaments. The laser that Tzortzakis
used could produce two.
But in a new set of experiments with a more powerful laser, Tzortzakis
hopes to test a key prediction of the Arizona model: that a beam of, say,
10 filaments would merge, then, having lost some energy because of ionization,
would break up again into a smaller number of filaments, say, 8, that
would merge and break up yet again.
Photon torpedoes
Although the self-guided filaments are intense, they contain just a
few millijoules of energy—far too low for use as Star Trek phasers, let
alone photon torpedoes. But they are potentially useful even so.
Under the extreme conditions of filament formation, nonlinear effects
convert the initially monochromatic light to a continuum that stretches
from 300 nm in the ultraviolet to 4.5 µm in
the infrared. Couple this property with the filaments' ability to travel
undispersed over long distances, and one has the potential to do remote
spectroscopy of atmospheric pollutants.
Laser pulses are already used to map pollutants in the atmosphere. The
technique, known as lidar, involves launching two laser beams into the
atmosphere. One beam is tuned to an absorption band of the pollutant of
interest; the other acts as a reference. The two beams—one diminished
by absorption, the other not—scatter off nitrogen and oxygen molecules
or dust particles in the atmosphere. A detector on the ground measures
the backscattered fraction of each beam.
This, the traditional form of lidar, suffers from three drawbacks that
don't beset self-focused filaments.
Traditional lidar can measure only one pollutant at a time. That's
not a problem for the filaments, whose broad continuum encompasses multiple
absorption bands.
Most interesting species have absorption bands in the infrared, but
the backscattered signal is weak in that waveband. The filaments don't
rely on backscattered light at all. Rather, they generate their own
infrared emission, which, thanks to a back-reflection process induced
by the plasma, is preferentially directed backward to the ground.
Monochromatic sources are insensitive to the form the species takes:
they can't, for instance, measure the size of aerosols. The filaments,
being broadband sources, lack this limitation because the spectrum of
scattered light depends on the size of the scattering particles.
In addition to these advantages, self-focused filaments share one of
traditional lidar's useful properties: the ability to exploit the delay
time of reflected pulses to yield distance information.
Exploiting self-focused filaments for detecting pollutants is one of
the aims of Teramobile, a mobile terawatt laser.5
The nine-ton facility, which fits in a standard cargo container, is a
joint project of two French and two German research groups: Mysyrowicz's
at ENSTA, Jean-Pierre Wolf's at Claude Bernard University in Lyons, Roland
Sauerbrey's at Friedrich Schiller University in Jena, and Ludger Wöste's
at Berlin's Free University.
In its four-month life, Teramobile has already detected water and methane
in the atmosphere. "Now we want to attack the real pollutants," says Wöste.
Those experiments begin this month in Jena.
Charles Day
References
1. A. Braun et al., Opt. Lett. 20, 73 (1995).
2. S. Tzortzakis et al., Phys. Rev. Lett. 86, 5470 (2001).
3. M. Mlejnek et al., Phys. Rev. Lett. 83, 2938 (1999).
4. S. Tzortzakis et al., Phys. Rev. E 60, R3505 (1999).
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