Highly efficient fourth harmonic generation ofbroadband laser pulses retaining 3D pulse shape

2021 ◽  
Author(s):  
Igor Kuzmin ◽  
Sergey Mironov ◽  
Mikhail Martyanov ◽  
Anatoly Poteomkin ◽  
Efim Khazanov
1995 ◽  
Vol 20 (4) ◽  
pp. 353 ◽  
Author(s):  
C. Y. Chien ◽  
R. S. Craxton ◽  
G. Korn ◽  
J. S. Coe ◽  
J. Squier ◽  
...  

Author(s):  
I.V. Kuzmin ◽  
S. Yu. Mironov ◽  
E.I. Gacheva ◽  
A.K. Potemkin ◽  
E.A. Khazanov

2006 ◽  
Vol 14 (5) ◽  
pp. 1905 ◽  
Author(s):  
Konstantinos Moutzouris ◽  
Florian Sotier ◽  
Florian Adler ◽  
Alfred Leitenstorfer

1996 ◽  
Vol 69 (25) ◽  
pp. 3812-3814 ◽  
Author(s):  
Lalit B. Sharma ◽  
H. Daido ◽  
Y. Kato ◽  
S. Nakai ◽  
T. Zhang ◽  
...  

1996 ◽  
Author(s):  
Vitaly N. Krylov ◽  
Alexander G. Kalintsev ◽  
Aleksander Rebane ◽  
Daniel Erni ◽  
Urs P. Wild

Materials ◽  
2021 ◽  
Vol 14 (12) ◽  
pp. 3194
Author(s):  
Adrian Petris ◽  
Petronela Gheorghe ◽  
Tudor Braniste ◽  
Ion Tiginyanu

The ultrafast third-order optical nonlinearity of c-plane GaN crystal, excited by ultrashort (fs) high-repetition-rate laser pulses at 1550 nm, wavelength important for optical communications, is investigated for the first time by optical third-harmonic generation in non-phase-matching conditions. As the thermo-optic effect that can arise in the sample by cumulative thermal effects induced by high-repetition-rate laser pulses cannot be responsible for the third-harmonic generation, the ultrafast nonlinear optical effect of solely electronic origin is the only one involved in this process. The third-order nonlinear optical susceptibility of GaN crystal responsible for the third-harmonic generation process, an important indicative parameter for the potential use of this material in ultrafast photonic functionalities, is determined.


1994 ◽  
Vol 72 (3) ◽  
pp. 673-677 ◽  
Author(s):  
Eric E. Aubanel ◽  
André D. Bandrauk

We examine two consequences of the unique behaviour of molecules in strong fields. First, by time gating of laser-induced avoided crossings with femtosecond laser pulses, one can obtain efficient vibrational inversion into a narrow distribution of vibrational levels of a molecular ion. We demonstrate this by numerical solution of the time-dependent Schrödinger equation for [Formula: see text] Second, we show results of numerical calculation with vibrationally excited [Formula: see text] of harmonic generation up to the 11th order of an intense 1064- nm laser. We predict that competition of photodissociation can be minimized by trapping the molecule in high-field-induced potential wells, thus enhancing the high-order harmonic generation process. Furthermore, the harmonic spectrum can serve as a measure of the structure of these laser-induced potentials.


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