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1.
Opt Lett ; 40(7): 1414-7, 2015 Apr 01.
Artigo em Inglês | MEDLINE | ID: mdl-25831346

RESUMO

We report on a passively mode-locked erbium-doped fiber laser featuring a large normal dispersion and emitting high-energy dissipative solitons. Mode-locking is stabilized by the combined actions of a high nonlinearity amplitude modulator and a narrow band spectral filter. The laser routinely delivers highly chirped pulses with more than 38 nJ energy that can be compressed down to 700 fs duration using bulk gratings. Numerical simulations confirm the experimental results and reveal the self-similar pulse evolution along the normal dispersion fibers included inside the cavity.

2.
Opt Lett ; 37(15): 3186-8, 2012 Aug 01.
Artigo em Inglês | MEDLINE | ID: mdl-22859127

RESUMO

Direct amplification of output from chirped pulse oscillator (CPO) to 3.3 W of average power (pulse energy of 118 nJ in 20 ps pulse duration before compression) was achieved in a properly designed cladding pumped large mode area Er-doped fiber. Various configurations of CPO cavity with different FWHM of output spectrum and pulse duration were investigated. Fourier limit compression with 480 fs pulse duration and 32 kW peak power has been obtained for pulses with 14.8 nm FWHM spectrum. Subsequent nonlinear compression in a standard SMF-28 fiber yielded pulses as short as 145 fs.

3.
Opt Lett ; 31(12): 1848-50, 2006 Jun 15.
Artigo em Inglês | MEDLINE | ID: mdl-16729091

RESUMO

We apply a novel phase-amplitude characterization method to a one-section quantum dash-based passively mode-locked laser at a 42.2 GHz repetition rate. The method relies on the measurement of the spectral phase of the longitudinal modes by the successive analysis of the correlation signal of a group of three adjacent modes. It provides both the temporal shape of the intensity and the phase of the emitted signal. A pulse of 1.5 ps of width is measured, and a pedestal is exhibited. Extinction ratio limitation is explained by investigating the origin of this pedestal. The accuracy of the method is estimated by comparing the measured autocorrelation signal and the calculated one from the phase analysis.

4.
7.
Phys Rev Lett ; 57(20): 2516-2519, 1986 Nov 17.
Artigo em Inglês | MEDLINE | ID: mdl-10033787
8.
Phys Rev B Condens Matter ; 34(8): 5443-5449, 1986 Oct 15.
Artigo em Inglês | MEDLINE | ID: mdl-9940377
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