We present the first measurement of the attosecond emission
generated from underdense plasma produced on a solid target. We generate
high-order harmonics of a femtosecond Ti:sapphire laser focused in a
weakly ionized underdense chromium plasma. Using the .Reconstruc-
tion of Attosecond Beating by Interference of Two-photon Transitions.
(RABITT) technique, we show that the 11thto the 19thharmonic orders
form in the time domain an attosecond pulse train with each pulse having
300 as duration, which is only 1.05 times the theoretical Fourier transform
limit. Measurements reveal a very low positive group delay dispersion of
4200 as2. Beside its fundamental interest, high-order harmonic generation
in plasma plumes could thus provide an intense source of attosecond pulses
for applications.
http://www.opticsinfobase.org/oe/abstract.cfm?uri=oe-19-4-3677
material...
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Tuesday, 21 June 2011
Monday, 16 May 2011
DM: Tsuneto: Development of CEP-stabilized high power CPA/OPA lasers and direct generation of highly phase-matched isolated attosecond pulses
One of the most crucial issues for the present attophysics is to
increase the pulse energy of isolated attosecond pulses (IAP.s). For
this purpose, there are two crucial experimental challenges to
demonstrate; one is to develop multi-mJ few cycle lasers with a
stabilized carrier-envelope phase (CEP) and the other is to achieve the
phase-matching highly between the few cycle pulses and high harmonics of
them.
In this talk, I will present our research activities on both challenges.
First, I will present our recent results of RIKEN based on our
TW-class 2-cycle laser system (5 fs, 780 nm, 5 mJ, 1 kHz). Recently, we
have stabilized CEP of this system with two feedback loops and by
blocking mechanical vibrations on the laser system thoroughly. Through
the phase matching process, we could select the supercontinuum component
of the harmonics without any use of bandpass filters such as Mo/Si
mirrors. By using a heterodyne interferometry using mixed gases, we
verified that we could select IAP directly. Second, I will briefly
introduce our recent results at Imperial College London on constructing a
CEP-stabilized high power OPA (optical parametric amplification) laser.
CEP-stabilized seed pulses were generated using type II DFG of
different frequency components of the supercontinuum generated with a
hollow fiber compression technique, and the seed pulses were amplified
by two-stage OPA.s. Final output pulses had a pulse energy of 500 μJ,
pulse duration of 40fs, and tunable wavelength from 1300-1800 nm. As
the first demonstration of this handmade laser, we could generate high
harmonics up to 47th using a tube target filled with Xe gas.
material...
material...
Tuesday, 5 April 2011
JC: Stefan: Study of high Mach number laser driven blast waves in gases
A series of experiments were performed examining the evolution of blast waves produced by laser
irradiation of a target immersed in gas. Blast waves were produced by illumination of wires by 1 kJ,
1 ns laser pulses from the Z-Beamlet laser at Sandia National Laboratories. The blast waves were
imaged by probe laser pulses at various times to examine the trajectory, radiative precursor, and
induced perturbations on the blast wave front. Well de.ned perturbations were induced on the blast
wave front with arrays of wires placed in the gas and the results of the experiments are compared
to the theoretical predictions for the Vishniac overstability. It is found that the experimental results
are in general agreement with these theoretical predictions on thin blast wave shells and are in
quantitative agreement in the simplest case.
http://scitation.aip.org/getpdf/servlet/GetPDFServlet?filetype=pdf&id=PHPAEN000017000011112104000001&idtype=cvips&prog=normal
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http://scitation.aip.org/getpdf/servlet/GetPDFServlet?filetype=pdf&id=PHPAEN000017000011112104000001&idtype=cvips&prog=normal
material...
Tuesday, 29 March 2011
DM: Damien: OPA/OPCPA in crystals and fibres
I will do a general discussion/presentation about OPA/OPCPA in non
linear crystal and in fiber. I will show some experimental results
related to what I did in the PETAL Petawatt project.
material...
material...
Tuesday, 22 March 2011
DM: Jon: Programme Grant overview & introduction
we plan to extend attosecond science to larger molecules and condensed
phase systems building upon our present activity in HHG spectroscopy and
attosecond pulse generation. I hope to give a short briefing on the
scientific plans
material...
material...
Tuesday, 8 March 2011
JC: Misha: Radiation Generated by the Ultrafast Migration of a Positive Charge Following the Ionization of a Molecular System
Electronic many-body effects alone can be the driving force for an
ultrafast migration of a positive charge created upon ionization of
molecular systems. Here we show that this purely electronic phenomenon
generates a characteristic IR radiation. The situation when the initial
ionic wave packet is produced by a sudden removal of an electron is also
studied. It is shown that in this case a much stronger UV emission is
generated. This emission appears as an ultrafast response of the
remaining electrons to the perturbation caused by the sudden ionization
and as such is a universal phenomenon to be expected in every
multielectron system.
http://prl.aps.org/abstract/PRL/v106/i5/e053001
What I want everyone to think about is:
- What is the role of the detached electron that they have completely neglected?
- Can this radiation be observed, and if yes, will it be coherent?
PPT slides to follow...#
http://prl.aps.org/abstract/PRL/v106/i5/e053001
What I want everyone to think about is:
- What is the role of the detached electron that they have completely neglected?
- Can this radiation be observed, and if yes, will it be coherent?
PPT slides to follow...#
Tuesday, 22 February 2011
DM: Luis: how to grow micro and nanostructures, with both, nanosecond and femtosecond laser pulses
(i) Laser irradiation of materials with laser pulses whose energy density
is around the ablation limit, no matter whether they are femtosecond or
nanosecond pulses, do produce microconical structures despite of the, most
likely, different mechanisms involved. These structucture do have several
interesting applications.
(ii) We will show how a metalic thin film of nanoparticles can be rearranged just by shining few laser pulses with a well defined intensity structure.
PPT slides to follow...
(ii) We will show how a metalic thin film of nanoparticles can be rearranged just by shining few laser pulses with a well defined intensity structure.
PPT slides to follow...
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