PROPAGATION’09
Curved Plasma Channel Generation in Air
Using Ultra-Intense Self-Bending Airy Beams
Pavel Polynkin, Miroslav Kolesik, Jerome Moloney, Georgios Siviloglou
and Demetrios Christodoulides
Ultrafast laser filamentation is a rich, interdisciplinary branch of physics
that addresses propagation of intense
laser pulses in transparent media. 1, 2 Applications range from terahertz generation to lightning control.
When an ultra-intense, ultra-short
laser pulse propagates in air, the defocusing e;ect of the plasma generated via
multi-photon ionization dynamically
balances the self-focusing of the beam
and prevents it from collapsing into a
singularity. ;e hot core of the beam,
composed of the high-intensity laser
field and generated plasma, is referred to
as the filament. Filaments are typically
about 100 µm in diameter and exhibit
self-guided, sub-di;ractive propagation
over long distances.
High optical intensities inside filaments facilitate e;cient nonlinear wavelength conversion, leading to forward
emission of broadband radiation. Analysis of the angularly resolved spectra of
this radiation yields insights into the
pulse propagation dynamics. 3
In early studies of femtosecond laser
filamentation, axially symmetric beam
profiles were used, such as Gaussian,
flat-top and Bessel beams. Accordingly,
filaments were generated along straight
lines. ;e broadband forward emissions
generated at di;erent points along a
straight filament tend to overlap in the
far-field, leading to spectra that are difficult to interpret.
We recently reported generating
optical Airy beams. 4 ;ese non-axially
symmetric beams are approximately
di;raction free, and their main intensity
features freely self-bend (or accelerate)
on propagation in the absence of any
refractive-index gradients.
We also conducted experiments on
the filamentation of ultra-intense Airy
beams in air. 5 We observed an unusual
filamentation regime in which the linear
(a)
Beam displacement [mm]
3
2
1
0
(b) 3 2 1 0
Beam displacement [mm]
Distance from Fourier plane [cm]
– 40 – 20 0 20 40
Distance from Fourier plane [cm]
– 40 – 20 0 20 40
(c)
(d)
(Top row) Numerical simulations for plasma density generated along the beam path at low
pulse energy ( 5 mJ, panel a) and high pulse energy ( 10 mJ, panel b). (Bottom row) Burn
pattern produced by the beam on aluminum foil (c); numerical simulation for the transverse
intensity pro;le of intense Airy beam (d).
self-bending property of the beam pattern competed against nonlinear self-channeling e;ects. ;e plasma channel
generated by the dominant intensity
feature of the beam followed the curved
beam trajectory. In this regime, broad-band forward emission by the curved
filament is angularly resolved in the
far-field, thus enabling detailed study
of this emission along the optical path.
Extended curved filaments generated by
self-bending Airy beams may find applications in remote sensing.
We started with 35-fs pulses with a
Gaussian beam profile and transformed
the beam into a 2-D Airy beam using a
combination of a cubic phase mask and
a focusing lens. ;e pulse energy was
varied between 5 and 15 mJ. Analysis of
forward emission by the curved filament
suggests that the plasma channel was
continuous at low pulse-energy levels but
developed split-o; channels at several locations along the propagation direction
when pulse energy was increased.
At high values of pulse energy, the
transverse beam profile exhibited a
nonlinear reshaping and developed a
whisker-like ghost beam and lagging
satellite lobe. ;ese features, clearly
visible in the burn patterns produced
on aluminum foil, were reproduced in
numerical simulations.
;is work was supported by AFOSR under contracts FA9550-07-1-0010 and FA9550-07-1-
0256. ;e contribution of G.S. and D.C. was
partially supported by Lockheed Martin Corp.
Pavel Polynkin ( ppolynkin@optics.arizona.edu),
Miroslav Kolesik and Jerome Moloney are with the
College of Optical Sciences, University of Arizona,
Tucson, Ariz., U.S.A. Georgios Siviloglou and
Demetrios Christodoulides are with the College of
Optics and Photonics, University of Central Florida
in Orlando, Fla., U.S.A.
References
1. A. Couairon and A. Mysyrowicz. Physics Reports 441,
47-190 (2007).
2. L. Berge et al. 70, 1633-713 (2007).
3. M. Kolesik and J. Moloney. Opt. Express 16, 2971-88
(2008).
4. G. Siviloglou et al. Phys. Rev. Lett. 99, 213901 (2007).
5. P. Polynkin et al. Science 324, 229-32 (2009).