The special feature in this issue is a response to
recent breakthroughs in the technology of sources of ultra-short
electromagnetic pulses; such pulses can now be delivered at the
limits of coherence over a wide frequency range. Studies of
ultra-short electromagnetic pulses and their interaction with
matter are attracting increasing interest in many areas of
science and technology because of the inherent potential of such
pulses to reveal transient features of physical phenomena and
probe peculiar electromagnetic and physical properties of all
kinds of matter. The laser is widely involved in generating or
detecting ultra-short electromagnetic pulses. These developments
have consequences for the instrumentation of measurements,
as scientists endeavour to implement new methods and
analytical approaches in the difficult challenge of
modelling the dynamics of ultra-fast physical phenomena.
The aim of this feature is to provide the reader with a
comprehensive overview of the current state of research and to
stimulate interest in implementing new ultra-short pulse
generators and device technologies in order to study more deeply
the rich field of ultra-short wideband electromagnetic pulse
technology. This issue includes articles exploring a `new
frontier in physics' and contributed articles on broadband
aspects of the field.
Thus, we report new developments and trends in the
following areas:
ultra-wideband short pulse electromagnetic waves in the
microwave range of frequency, developed in Section I;
ultra-short laser pulse technology and coherent
beam interaction with matter, developed in Section II;
ultra-short high-intensity laser and plasma interactions
and transient x-ray laser pulses, developed in Section III;
ultra-short laser pulses inducing the emission of
coherent soft x-ray beams as a result of high order harmonic
generation or high contrast energy modulation, developed
in Section IV;
the temporal aspect in synchrotron radiation sources and
applications, developed in Section V;
methods of time-resolved spectroscopy applied to
measurements of ultra-short electromagnetic pulses and
diagnostics of dynamical phenomena, developed in Section VI.
The techniques for generating, manipulating and detecting
picosecond and sub-picosecond electromagnetic pulses have been
documented extensively in the literature [1-6]. To measure
an ultra-short electromagnetic pulse in the picosecond
(or sub-picosecond) time-scale, an
electromagnetic source with a high repetition rate
is required (such as a laser source or eventually a synchrotron
radiation source). When this condition is fulfilled, a pump-probe
optoelectronic sampling
measurement method can be applied. The relatively fast
detectors used for infrared and visible ultra-short pulses of
radiation generally have a weak sensitivity for x-ray
detection. This is because of the fast response of the photocarrier
generation and the weak x-ray absorption of semiconductors.
In the VUV and x-ray domain, the main system fordetecting picosecond to femtosecond signals is generally a streak
camera [7, 8] photoswitched by a synchronized
femtosecond laser pulse (see Section VI).
These researches and experiments on pulsed electromagnetic
radiation interacting with matter open new domains to
theoretical research and technological development [9],
promising previously unsuspected knowledge about the
universe. The generation, detection and measurement of
transient electromagnetic waves, i.e. short pulses, are of
considerable interest to experimental studies of interaction with
various media and modern information and communications
technologies. Numerous applications are found in the field of
wideband radar echoes, measurements of
electromagnetic properties of materials and time-resolved spectroscopy (e.g.
x-ray diffraction, reflection and absorption, etc). New
measuring techniques and data processing methods have been
and are being developed and are, in fact, indispensable for
analysing the detailed features of the real-time results delivered
by high power lasers, wideband impulse radar and x-ray beamlines.
The propagation of a transient wave packet through plasmas, for
instance the ionosphere, condensed matter (obtained by inertial
compression) and biological aerosol streams, is now
of widespread interest.
References
[1] Eloy J-F 2001 Progress in Ultra-Short
Electromagnetic Pulses Technology. A New Frontier in
Physics (London: Hermes-Penton)
[2] Elton R C (ed) 1989 X-Ray Laser (New York: Academic)
[3] Kim K-J, Chattopadhyay S and Shank C V 1994
Generation of femtosecond X-rays by 90° Thomson scatteringNucl. Instrum. Methods Phys. Res. A 341 351-4
[4] Klisnick A et al 2000 Generation of a transient short pulse
X-ray laser using a travelling-wave sub-ps pump pulse 7th
Int. Conf. on X-ray Lasers, St Malo, France, 18-23 June
[5] Lappas D and L'Huillier A 1998 Generation of
attosecond XUV pulses in strong laser-atom interactions
Phys. Rev. A 58 4140-6
[6] Smith P R, Auston D H and Nuss M C 1988
Subpicosecond photoconducting dipole antennas IEEE J.
Quantum Electron.QE-24 255-60
[7] Knox W, Nordlund T M and Mourou G 1982 Jitter-free streak
camera system Picosecond Phenomena III, Proc. 3rd. Int.
Conf. on Picosecond Phenomena ed K B Eisenthal \etal (Berlin:
Springer) pp 98-100
[8] Watanabe M, Koishi M, Kan H, Kaufmann K J and Tsuchiya Y
1990 Picosecond fluorescence microscopy Picosecond and
Femtosecond Spectroscopy from Laboratory to Real World ed K A
Nelson Proc. SPIE'90, Los Angeles, 16-17 July vol. 1209,
pp 157-64
[9] Svanberg S 1998 High-power lasers and their
applications Adv. Quantum Chem.30 209-33