Mid-infrared frequency domain optical parametric amplifier

被引:6
|
作者
Dalla-Barb, Gilles [1 ,2 ]
Jargot, Gaetan [1 ]
Lassonde, Philippe [1 ]
Toth, Szabolcs [3 ]
Haddad, Elissa [1 ]
Boschini, Fabio
Delagnes, Jean-Christophe [4 ]
Leblanc, Adrien [5 ]
Ibrahim, Heide [1 ]
Cormier, Eric [2 ,6 ]
Legare, Francois [1 ]
机构
[1] Adv Laser Light Source ALLS, Inst Natl Rech Sci, Ctr Energie Mat & Telecommun, 1650 Blvd Lionel Boulet, Varennes, PQ J3X 1S2, Canada
[2] CNRS IOGS Univ Bordeaux, Lab Photon Numer & Nanosci LP2N, UMR 5298, F-33400 Talence, France
[3] ELI ALPS Res Inst, Dugonics ter 13, H-6720 Szeged, Hungary
[4] Ctr Natl Rech Sci, Ctr Lasers Intenses & Applicat, 351,Cours de la Liberat, Talence, France
[5] Univ Paris Saclay, Ecole Polytech, Lab Opt Appliquee, ENSTA,CNRS, Palaiseau, France
[6] Inst Univ France IUF, 1 rue Descartes, F-75231 Paris, France
基金
加拿大创新基金会; 加拿大自然科学与工程研究理事会;
关键词
HIGH-HARMONIC-GENERATION; 5; MU-M; LASER-PULSES; ULTRAFAST; DRIVEN; SPECTROSCOPY; BRIGHT; LEVEL; POWER;
D O I
10.1364/OE.487813
中图分类号
O43 [光学];
学科分类号
070207 ; 0803 ;
摘要
We report on an optical architecture delivering sub-120 femtosecond laser pulses of 20 pJ tunable from 5.5 pm to 13 pm in the mid-infrared range (mid-IR). The system is based on a dual-band frequency domain optical parametric amplifier (FOPA) optically pumped by a Ti:Sapphire laser and amplifying 2 synchronized femtosecond pulses each with a widely tunable wavelength around 1.6 and 1.9 pm respectively. These amplified pulses are then combined in a GaSe crystal to produce the mid-IR few-cycle pulses by means of difference frequency generation (DFG). The architecture provides a passively stabilized carrier-envelope phase (CEP) whose fluctuations has been characterized to 370 mrad RMS.
引用
收藏
页码:14954 / 14964
页数:11
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