Abstract

We report the generation of sub-80fs pulses with energy in the 100nJ range at 1050nm and a repetition rate up to 164kHz based on a nonlinear fiber amplification system combined with an active control of the spectral phase. This control is performed by an acousto-optic programmable dispersive filter operated at a multiple of its acoustic repetition rate. This result opens up its possible use in highly nonlinear fiber chirped-pulse amplification setups.

© 2008 Optical Society of America

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2008 (1)

2007 (4)

2006 (2)

2005 (1)

2002 (1)

2000 (2)

M. E. Fermann, V. I. Kruglov, B. C. Thomsen, J. M. Dudley, and J. D. Harvey, Phys. Rev. Lett. 84, 6010 (2000).
[CrossRef] [PubMed]

F. Verluise, V. Laude, Z. Cheng, C. Spielmann, and P. Tournois, Opt. Lett. 25, 575 (2000).
[CrossRef]

Aguergaray, C.

Boullet, J.

Cheng, Z.

Cho, G.

Chong, A.

Clausnitzer, T.

Cormier, E.

Druon, F.

Dudley, J. M.

M. E. Fermann, V. I. Kruglov, B. C. Thomsen, J. M. Dudley, and J. D. Harvey, Phys. Rev. Lett. 84, 6010 (2000).
[CrossRef] [PubMed]

Fermann, M.

Fermann, M. E.

M. E. Fermann, V. I. Kruglov, B. C. Thomsen, J. M. Dudley, and J. D. Harvey, Phys. Rev. Lett. 84, 6010 (2000).
[CrossRef] [PubMed]

Finot, C.

Fuchs, H.-J.

Georges, P.

Hanna, M.

Hartl, I.

Harvey, J. D.

M. E. Fermann, V. I. Kruglov, B. C. Thomsen, J. M. Dudley, and J. D. Harvey, Phys. Rev. Lett. 84, 6010 (2000).
[CrossRef] [PubMed]

Huang, L.

Imeshev, G.

Kley, E.-B.

Kruglov, V. I.

M. E. Fermann, V. I. Kruglov, B. C. Thomsen, J. M. Dudley, and J. D. Harvey, Phys. Rev. Lett. 84, 6010 (2000).
[CrossRef] [PubMed]

Kuznetsova, L.

Laude, V.

Limpert, J.

Liu, Z.

Mottay, E.

Müller, D.

Papadopoulos, D. N.

Parmigiani, F.

Petropoulos, P.

Richardson, D.

Röser, F.

Schimpf, D.

Schreiber, T.

Shah, L.

Spielmann, C.

Thomsen, B. C.

M. E. Fermann, V. I. Kruglov, B. C. Thomsen, J. M. Dudley, and J. D. Harvey, Phys. Rev. Lett. 84, 6010 (2000).
[CrossRef] [PubMed]

Tournois, P.

Tünnermann, A.

van Howe, J.

Verluise, F.

Wise, F. W.

Xu, C.

Zaouter, Y.

Zellner, H.

Zhu, G.

Zöllner, K.

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Figures (3)

Fig. 1
Fig. 1

Experimental setup.

Fig. 2
Fig. 2

Retrieved temporal intensity profile of the compressed pulses (a) with a grating pair and (b) a Dazzler at 6 W (upper part) and 5 W (lower part) of pump power (FROG traces and retrieved spectra are shown as insets).

Fig. 3
Fig. 3

FROG traces of the Dazzler+grating compressed pulse at 41 164 kHz (upper part) and corresponding retrieved temporal intensity profiles (retrieved spectra are shown as insets).

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