Photoelectron holography of atomic targets

We study the spatial interference effects appearing during the ionization of atoms (H, He, Ne, and Ar) by few-cycle laser pulses using single-electron ab initio calculations. The spatial interference is the result of the coherent superposition of the electronic wave packets created during one half c...

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Autores principales: Borbély, S., Tóth, A., Arbó, D.G., Tokési, K., Nagy, L.
Formato: JOUR
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Acceso en línea:http://hdl.handle.net/20.500.12110/paper_24699926_v99_n1_p_Borbely
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spelling todo:paper_24699926_v99_n1_p_Borbely2023-10-03T16:41:41Z Photoelectron holography of atomic targets Borbély, S. Tóth, A. Arbó, D.G. Tokési, K. Nagy, L. Argon lasers Atom lasers Atoms Calculations Wave functions Wave packets Ab initio calculations Coherent superpositions Electronic wave packets Few-cycle laser pulse Interference patterns Photoelectron holographies Spatial interference Spatial interference patterns Holograms We study the spatial interference effects appearing during the ionization of atoms (H, He, Ne, and Ar) by few-cycle laser pulses using single-electron ab initio calculations. The spatial interference is the result of the coherent superposition of the electronic wave packets created during one half cycle of the driving field following different spatial paths. This spatial interference pattern may be interpreted as the hologram of the target atom. With the help of a wave-function analysis (splitting) technique and approximate (strong-field and Coulomb-Volkov) calculations, we directly show that the hologram is the result of the electronic-wave-packet scattering on the parent ion. On the He target we demonstrate the usefulness of the wave-function splitting technique in the disentanglement of different interference patterns. Further, by performing calculations for the different targets, we show that the pattern of the hologram does not depend on the angular symmetry of the initial state and it is strongly influenced by the atomic species of the target: A deeper bounding potential leads to a denser pattern. © 2019 American Physical Society. JOUR info:eu-repo/semantics/openAccess http://creativecommons.org/licenses/by/2.5/ar http://hdl.handle.net/20.500.12110/paper_24699926_v99_n1_p_Borbely
institution Universidad de Buenos Aires
institution_str I-28
repository_str R-134
collection Biblioteca Digital - Facultad de Ciencias Exactas y Naturales (UBA)
topic Argon lasers
Atom lasers
Atoms
Calculations
Wave functions
Wave packets
Ab initio calculations
Coherent superpositions
Electronic wave packets
Few-cycle laser pulse
Interference patterns
Photoelectron holographies
Spatial interference
Spatial interference patterns
Holograms
spellingShingle Argon lasers
Atom lasers
Atoms
Calculations
Wave functions
Wave packets
Ab initio calculations
Coherent superpositions
Electronic wave packets
Few-cycle laser pulse
Interference patterns
Photoelectron holographies
Spatial interference
Spatial interference patterns
Holograms
Borbély, S.
Tóth, A.
Arbó, D.G.
Tokési, K.
Nagy, L.
Photoelectron holography of atomic targets
topic_facet Argon lasers
Atom lasers
Atoms
Calculations
Wave functions
Wave packets
Ab initio calculations
Coherent superpositions
Electronic wave packets
Few-cycle laser pulse
Interference patterns
Photoelectron holographies
Spatial interference
Spatial interference patterns
Holograms
description We study the spatial interference effects appearing during the ionization of atoms (H, He, Ne, and Ar) by few-cycle laser pulses using single-electron ab initio calculations. The spatial interference is the result of the coherent superposition of the electronic wave packets created during one half cycle of the driving field following different spatial paths. This spatial interference pattern may be interpreted as the hologram of the target atom. With the help of a wave-function analysis (splitting) technique and approximate (strong-field and Coulomb-Volkov) calculations, we directly show that the hologram is the result of the electronic-wave-packet scattering on the parent ion. On the He target we demonstrate the usefulness of the wave-function splitting technique in the disentanglement of different interference patterns. Further, by performing calculations for the different targets, we show that the pattern of the hologram does not depend on the angular symmetry of the initial state and it is strongly influenced by the atomic species of the target: A deeper bounding potential leads to a denser pattern. © 2019 American Physical Society.
format JOUR
author Borbély, S.
Tóth, A.
Arbó, D.G.
Tokési, K.
Nagy, L.
author_facet Borbély, S.
Tóth, A.
Arbó, D.G.
Tokési, K.
Nagy, L.
author_sort Borbély, S.
title Photoelectron holography of atomic targets
title_short Photoelectron holography of atomic targets
title_full Photoelectron holography of atomic targets
title_fullStr Photoelectron holography of atomic targets
title_full_unstemmed Photoelectron holography of atomic targets
title_sort photoelectron holography of atomic targets
url http://hdl.handle.net/20.500.12110/paper_24699926_v99_n1_p_Borbely
work_keys_str_mv AT borbelys photoelectronholographyofatomictargets
AT totha photoelectronholographyofatomictargets
AT arbodg photoelectronholographyofatomictargets
AT tokesik photoelectronholographyofatomictargets
AT nagyl photoelectronholographyofatomictargets
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