Principal frequency of an ultrashort laser pulse

被引:8
|
作者
Neyra, Enrique G. [1 ]
Vaveliuk, Pablo [1 ]
Pisanty, Emilio [2 ,3 ]
Maxwell, Andrew S. [2 ,4 ]
Lewenstein, Maciej [2 ,5 ]
Ciappina, Marcelo F. [2 ,6 ,7 ]
机构
[1] UNLP, CICBA, CONICET, CIOp Ctr Invest Opt, Camino Centenario & 506, RA-1897 Pcia Bs As, Argentina
[2] Barcelona Inst Sci & Technol, ICFO Inst Ciencies Foton, Barcelona 08860, Spain
[3] Max Born Inst Nonlinear Opt & Short Pulse Spect, Max Born Str 2A, D-12489 Berlin, Germany
[4] UCL, Dept Phys & Astron, Gower St, London WC1E 6BT, England
[5] ICREA, Passeig Lluis Companys 23, Barcelona 08010, Spain
[6] Guangdong Technion Israel Inst Technol, Phys Program, Shantou 515063, Guangdong, Peoples R China
[7] Technion Israel Inst Technol, IL-32000 Haifa, Israel
基金
欧盟地平线“2020”;
关键词
HIGH-HARMONIC-GENERATION; CYCLE; REGIME;
D O I
10.1103/PhysRevA.103.053124
中图分类号
O43 [光学];
学科分类号
070207 ; 0803 ;
摘要
We introduce an alternative definition of the main frequency of an ultrashort laser pulse-the principal frequency omega(P). This parameter is complementary to the most accepted and widely used carrier frequency omega(0). Given the fact that these ultrashort pulses, also known as transients, have a temporal width comprising only a few cycles of the carrier wave, corresponding to a spectral bandwidth Delta omega covering several octaves, omega(P) describes, in a more precise way, the dynamics driven by these sources. We present examples where, for instance, omega(P) is able to correctly predict the high-order harmonic cutoff independent of the carrier envelope phase. This is confirmed by solving the time-dependent Schrodinger equation in reduced dimensions, supplemented with the time-analysis of the quantum spectra, where it is possible to observe how the subcycle electron dynamics is better described using omega(P). The concept of omega(P), however, can be applied to a large variety of scenarios, not only within the strong-field physics domain.
引用
收藏
页数:11
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