47th Annual Meeting of the APS Division of Atomic, Molecular and Optical Physics
Volume 61, Number 8
Monday–Friday, May 23–27, 2016;
Providence, Rhode Island
Session U9: Invited Session: Ultrafast Techniques and Light Sources
10:30 AM–12:30 PM,
Friday, May 27, 2016
Room: 556AB
Chair: Kenneth Knappenberger, Florida State University
Abstract ID: BAPS.2016.DAMOP.U9.3
Abstract: U9.00003 : Frequency domain nonlinear optics.
11:30 AM–12:00 PM
Preview Abstract
Abstract
Author:
Francois Legare
(INRS-EMT)
The universal dilemma of gain narrowing occurring in fs amplifiers prevents
ultra-high power lasers from delivering few-cycle pulses. This problem is
overcome by a new amplification concept: Frequency domain Optical Parametric
Amplification -- FOPA [1]. It enables simultaneous up-scaling of peak power
and amplified spectral bandwidth and can be performed at any wavelength
range of conventional amplification schemes, however, with the capability to
amplify single cycles of light. The key idea for amplification of
octave-spanning spectra without loss of spectral bandwidth is to amplify the
broad spectrum "slice by slice" in the frequency domain, i.e. in the Fourier
plane of a \textit{4f}-setup.
The striking advantages of this scheme, are its capability to amplify (more
than) one octave of bandwidth without shorting the corresponding pulse
duration. This is because ultrabroadband phase matching is not defined by
the properties of the nonlinear crystal employed but the number of crystals
employed. In the same manner, to increase the output energy one simply has
to increase the spectral extension in the Fourier plane and to add one more
crystal. Thus, increasing pulse energy and shortening its duration accompany
each other.
A proof of principle experiment was carried out at ALLS on the sub-two cycle
IR beam line and yielded record breaking performance in the field of
few-cycle IR lasers. 100$\mu $J two-cycle pulses from a hollow core fibre
compression setup were amplified to 1.43mJ without distorting spatial or
temporal properties. Pulse duration at the input of FOPA and after FOPA
remains the same. Recently, we have started upgrading this system to be
pumped by 250 mJ to reach 40 mJ two-cycle IR few-cycle pulses and latest
results will be presented at the conference. Furthermore, the extension of
the concept of FOPA to other nonlinear optical processes will be discussed.
[1] B. E. Schmidt et al. \textit{Nature Commun.} \textbf{5}, 3643 (2014).
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2016.DAMOP.U9.3