Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Journal of Physics Conference Series

Time delays in above-threshold ionization

Stefan Nagele, S. D. López, D. G. Arbó, Joachim Burgdörfer

Published Sep 7, 2015• 0 citations
Publisher

Abstract

We theoretically analyze time-resolved above-threshold ionization as probed by an interferometric measurement technique. We investigate the time delays in the ATI process as a function of the number of involved photons and the intensity of the ionizing UV field and identify IR-probe field induced contributions to the time shifts.
DOI
10.1088/1742-6596/635/9/092129

Related papers

Two photon above threshold ionization in a relativistic framework : Attosecond delays in high Z elements

Jimmy Vinbladh

Recent advances in experimental physics opens up for improved time resolution on measurements of ionizing processes in atoms caused by an EM-field. There exist non-relativistic models that describe ...

•Jan 1, 2018•1 citation

Time-resolved photoemission using attosecond streaking

S Nagele, R Pazourek, M Wais +2 more

We theoretically study time-resolved photoemission in atoms as probed by attosecond streaking. We review recent advances in the study of the photoelectric efect in the time domain and show that the experimentally accessible time shifts can be decomposed into distinct contributions that stem from the feld-free photoionization process itself and from probe-field induced corrections. We perform accurate quantum-mechanical as well as classical simulations of attosecond streaking for efective one-electron systems and determine all relevant contributions to the time delay with attosecond precision. In particular, we investigate the properties and limitations of attosecond streaking for the transition from short-ranged potentials (photodetachment) to long-ranged Coulomb potentials (photoionization). As an example for a more complex system, we study time-resolved photoionization for endohedral fullerenes A @C 60 and discuss how streaking time shifts are modifed due to the interaction of the C 60 cage with the probing infrared streaking field.

arXiv:1401.6328•Journal of Physics Conference Series•Apr 10, 2014•17 citations

Research progress of the control and measurement of the atomic and molecular ultrafast electron dynamics using two-color field

Liu Can-Dong, Jia Zheng-Mao, Zheng Ying-Hui +3 more

The advent of the ultrafast laser pulse provides the powerful and efficient tool for probing the ultrafast electron dynamics in atoms and molecules. The various nonlinear process induced by the laser-matter interaction allows one to obtain the electron motion information on the sub-femtosecond time scale. A series of the ultrafast spectroscopic technique, such as attosecond streak camera, attosecond transient absorption spectrum, and etc., have been successfully applied to the probe of electron dynamics in atoms, molecules, and solids. Using two-color field is one of the significant methods to achieve the coherent control and exploring of the electron motion. This paper summarizes recent research activities in the field of the atomic and molecular ultrafast process investigated in State Key Laboratory of High Field Laser Physics, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, including the detection of the electron dynamics of the multi-bound states, measurement of the carrier envelope phase (CEP) and the phase of the attosecond pulse, and the ultrafast electron control with the THz/UV and MIR/IR field. To measure the dynamics of the multi-bound states, a broadband attosecond pulse can be used to ionize the electrons after it is excited by the pump laser. By changing the delay between the pump laser and the attosecond pulse, the measured electrons ionized by the broadband xuv attosecond pulse can present the multi-bound states dynamics simultaneously. The XUV/IR scheme is popularly used in attosecond dynamics measurement. But usually, the IR field is not very strong. We find that, if the IR field is strong enough to induce the above threshold ionization (ATI), the interference between the ATI electron and the electron from XUV pulse can be used to measure the CEP of the attosecond XUV pulse. Besides, if the electron ionized by attosecond pulse can be pushed back to the nuclei, the emission from the recombination can be used to determine the spectral phase of the attosecond pulse, which is an all-optical measurement. We also investigate the two color scheme of THz/UV and MIR/IR fields. With THz/UV two color scheme, very high electron localization can be achieved duration molecular dissociation when we use the UV pulse to excite the electron and the THz pulse to control the following electron movement. When we use the MIR/IR field to control the electron motion during the high harmonic generation, the recollision can be greatly decreased and the single attosecond pulse can be produced with multi-cycle MIR laser field.

Acta Physica Sinica•Jan 1, 2016•1 citation

Experimental studies of laser-induced continuum structure in the atomic ionization continuum

Stefano Cavalieri, R. Eramo, Lorenzo Fini +1 more

In this contribution we present an experimental investigation of LICS (Laser‐Induced Continium Structure) in the single‐photon ionization spectrum of cesium and sodium. We report observations of the ionization spectrum of these atoms induced embedding a discrete state (5s for sodium and 8s for cesium) in the continuum by means of an IR laser. The structures, probed by single‐photon ionization from the ground state by an UV tunable laser show a marked asymmetry, typical of the process. We have performed the experiments observing the charge produced in the photoionization or the birefrincence and dichroism induced in the atomic medium. The two techniques allow the study of LICS for different intensity of the embedding laser (from 108 to 1011 W/cm2) giving complementary information on the physical process. The measured line‐shapes are compared with quantitative predictions of theoretical models.

AIP conference proceedings•Jan 1, 1995•0 citations

A Systematic Study of Interference Effects in Non-Sequential Double Ionisation

Andrew Maxwell, Carla Figueira de Morisson Faria

We perform a detailed study of interference in time-delayed NSDI showing significant effects on the momentum dependent transition amplitude. We also provide analytical arguments to back up our findings.

Journal of Physics Conference Series•Sep 7, 2015•0 citations

Ac Stark shifts induced by a YAG laser in the nP and nF Rydberg series in xenon

Didier Normand, Louis A. Lompre, Anne L’Huillier +5 more

Nonresonant ac Stark shifts of Rydberg states in Xe have been investigated by probing an atomic transition with a weak UV light in the presence of an intense YAG-laser pulse. Rydberg atoms produced through two-photon excitation, 5p → np (n = 15–48) and 5p → nf (n = 12–49), are subsequently ionized. IR-laser-induced shifts of the resonant ionization profiles are then measured. The measured shift, 3.9 ± 0.3 cm−1 at 1010 W cm−2, is more than a factor of 2 smaller than that expected from the basis of ponderomotive term, 8.5 cm−1 at 1010 W cm−2. In addition, the shift varies linearly as a function of the IR-laser intensity and does not depend on the principal quantum number of the np and nf series investigated here.

Journal of the Optical Society of America B•Aug 1, 1989•39 citations
We theoretically study time-resolved photoemission in atoms as probed by attosecond streaking. We review recent advances in the study of the photoelectric efect in the time domain and show that the experimentally accessible time shifts can be decomposed into distinct contributions that stem from the feld-free photoionization process itself and from probe-field induced corrections. We perform accurate quantum-mechanical as well as classical simulations of attosecond streaking for efective one-electron systems and determine all relevant contributions to the time delay with attosecond precision. In particular, we investigate the properties and limitations of attosecond streaking for the transition from short-ranged potentials (photodetachment) to long-ranged Coulomb potentials (photoionization). As an example for a more complex system, we study time-resolved photoionization for endohedral fullerenes A @C 60 and discuss how streaking time shifts are modifed due to the interaction of the C 60 cage with the probing infrared streaking field.
The advent of the ultrafast laser pulse provides the powerful and efficient tool for probing the ultrafast electron dynamics in atoms and molecules. The various nonlinear process induced by the laser-matter interaction allows one to obtain the electron motion information on the sub-femtosecond time scale. A series of the ultrafast spectroscopic technique, such as attosecond streak camera, attosecond transient absorption spectrum, and etc., have been successfully applied to the probe of electron dynamics in atoms, molecules, and solids. Using two-color field is one of the significant methods to achieve the coherent control and exploring of the electron motion. This paper summarizes recent research activities in the field of the atomic and molecular ultrafast process investigated in State Key Laboratory of High Field Laser Physics, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, including the detection of the electron dynamics of the multi-bound states, measurement of the carrier envelope phase (CEP) and the phase of the attosecond pulse, and the ultrafast electron control with the THz/UV and MIR/IR field. To measure the dynamics of the multi-bound states, a broadband attosecond pulse can be used to ionize the electrons after it is excited by the pump laser. By changing the delay between the pump laser and the attosecond pulse, the measured electrons ionized by the broadband xuv attosecond pulse can present the multi-bound states dynamics simultaneously. The XUV/IR scheme is popularly used in attosecond dynamics measurement. But usually, the IR field is not very strong. We find that, if the IR field is strong enough to induce the above threshold ionization (ATI), the interference between the ATI electron and the electron from XUV pulse can be used to measure the CEP of the attosecond XUV pulse. Besides, if the electron ionized by attosecond pulse can be pushed back to the nuclei, the emission from the recombination can be used to determine the spectral phase of the attosecond pulse, which is an all-optical measurement. We also investigate the two color scheme of THz/UV and MIR/IR fields. With THz/UV two color scheme, very high electron localization can be achieved duration molecular dissociation when we use the UV pulse to excite the electron and the THz pulse to control the following electron movement. When we use the MIR/IR field to control the electron motion during the high harmonic generation, the recollision can be greatly decreased and the single attosecond pulse can be produced with multi-cycle MIR laser field.
In this contribution we present an experimental investigation of LICS (Laser‐Induced Continium Structure) in the single‐photon ionization spectrum of cesium and sodium. We report observations of the ionization spectrum of these atoms induced embedding a discrete state (5s for sodium and 8s for cesium) in the continuum by means of an IR laser. The structures, probed by single‐photon ionization from the ground state by an UV tunable laser show a marked asymmetry, typical of the process. We have performed the experiments observing the charge produced in the photoionization or the birefrincence and dichroism induced in the atomic medium. The two techniques allow the study of LICS for different intensity of the embedding laser (from 108 to 1011 W/cm2) giving complementary information on the physical process. The measured line‐shapes are compared with quantitative predictions of theoretical models.
Nonresonant ac Stark shifts of Rydberg states in Xe have been investigated by probing an atomic transition with a weak UV light in the presence of an intense YAG-laser pulse. Rydberg atoms produced through two-photon excitation, 5p → np (n = 15–48) and 5p → nf (n = 12–49), are subsequently ionized. IR-laser-induced shifts of the resonant ionization profiles are then measured. The measured shift, 3.9 ± 0.3 cm−1 at 1010 W cm−2, is more than a factor of 2 smaller than that expected from the basis of ponderomotive term, 8.5 cm−1 at 1010 W cm−2. In addition, the shift varies linearly as a function of the IR-laser intensity and does not depend on the principal quantum number of the np and nf series investigated here.