2020
DOI: 10.1038/s41598-019-57125-z
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Quantum control and characterization of ultrafast ionization with orthogonal two-color laser pulses

Abstract: We study ultrafast ionization dynamics using orthogonally polarized two-color (OTC) laser pulses involving the resonant "first plus second" (ω + 2ω) scheme. The scheme is illustrated by numerical simulations of the time-dependent Schrödinger equation and recording the photoelectron momentum distribution. On the basis of the simulations of this resonant ionization, we identify signatures of the dynamic Autler-Townes effect and dynamic interference, in which their characterization is not possible in spectral dom… Show more

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Cited by 7 publications
(3 citation statements)
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“…The equation is solved using a Split-operator method combined with a fast Fourier transform algorithm. Details about the method and numerical convergence have been discussed in our previous works 36 , 37 .…”
Section: Methodsmentioning
confidence: 99%
“…The equation is solved using a Split-operator method combined with a fast Fourier transform algorithm. Details about the method and numerical convergence have been discussed in our previous works 36 , 37 .…”
Section: Methodsmentioning
confidence: 99%
“…The equation is solved using a Split-operator method combined with a fast Fourier transform algorithm. Details about the method and numerical convergence have been discussed in our previous works 36,37 . In all the calculations performed in the present work, we use the dipole approximation to describe the interaction between the laser fields and the target.…”
Section: Methodsmentioning
confidence: 99%
“…Having established a comprehensive picture of the role of an IR single-cycle pulse in inducing high-energy plateaus, we now discuss how this phenomenon can be controlled. Taking advantage of the properties of the optical phase in controlling the continuum wavepacket, as it has been discussed in the context of a single-color few-cycle pulse [60] and within a two-color scheme involving two multi-cycle laser pulses [58,61], we aim here at implementing this control procedure. The basic physics involved in this control scheme is that the ionized electrons are presumed to follow the instantaneous oscillating field, as shown in Figure 3d.…”
Section: Irmentioning
confidence: 99%