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

The Japan Society of Applied Physics

Coherent control of photoelectron angular distribution of He and Ne atoms by bichromatic extreme ultraviolet laser

Oyunbileg Tugs, Yuki Orimo, Daehyun You, Kiyoshi Ueda, Takeshi Sato, Kenichi Ishikiwa

Published Jul 10, 2018• 0 citations
OpenAlex

Related papers

Two-pathway coherent control of photoelectron angular distributions in molecular NO

Yi-Yian Yin, Daniel S. Elliott, Rana Shehadeh +1 more

Chemical Physics Letters•Aug 1, 1995•59 citations

Control of ion-photoelectron entanglement and coherence via Rabi oscillations

Kenichi L. Ishikawa, Kevin Charles Prince, Kiyoshi Ueda

We theoretically show that photoelectron-ion entanglement created by bichromatic extreme-ultraviolet pulses can be converted into coherence through Rabi coupling between the two ionic states. Then, the photoelectron angular distribution can be coherently controlled.

High-Brightness Sources and Light-Driven Interactions•Jan 1, 2024•0 citations

Photoelectron angular distributions from strong-field coherent electronic excitation

M. Wollenhaupt, Marc Krug, Jens Köhler +3 more

Applied Physics B•Feb 26, 2009•68 citations

Photoelectron angular distribution in two-color atomic ionization

Alexei N. Grum-Grzhimailo, Грызлова Елена Владимировна, Ekaterina I. Staroselskaya +4 more

•Jan 1, 2015•0 citations

Coherent Control of Ion-Photoelectron Dynamics through Rabi Oscillations: An ab initio study

Shen, Bo-Ren, Yi-Jia Mao, Zhaohan Zhang +4 more

We present first-principles numerical simulations of photoionization in neon induced by bichromatic extreme ultraviolet pulses with frequencies $ω$ and $2ω$, specially chosen to make $ω$ equal to the energy difference between the $2s$ and $2p$ subshells. This allows for the production of photoelectrons from the $2s$ shell by $2ω$ pulse and from the $2p$ shell by $ω$ pulse with the same energy. Using the multi-configurational time-dependent Hartree-Fock method, we explore how Rabi coupling between subshells generates coherence between the corresponding photoelectron wave packets. Our \textit{ab initio} calculations confirm the analytical results derived from the essential-states approach in [K. L. Ishikawa, K. C. Prince, and K. Ueda, J. Phys. Chem. A 127, 10638 (2023)], validating the theoretical predictions. Although we focus on the Ne $2p$ and $2s$ subshells, our approach is applicable to a broad range of systems exhibiting photoionization from multiple subshells. The laser parameters employed in our simulations are available in modern Free Electron Lasers (FELs), and we anticipate that this work could stimulate experimental investigations using FELs to study ion-photoelectron coherence and entanglement.

arXiv:2505.19681•May 26, 2025•0 citations

Quantum coherent control of the photoelectron angular distribution in bichromatic-field ionization of atomic neon

Грызлова Елена Владимировна, Alexei N. Grum-Grzhimailo, Ekaterina I. Staroselskaya +2 more

We investigate the coherent control of the photoelectron angular distribution in bichromatic atomic ionization. Neon is selected as target since it is one of the most popular systems in current gas-phase experiments with free-electron lasers (FELSs). In particular, we tackle practical questions, such as the role of the fine-structure splitting, the pulse length, and the intensity. Time-dependent and stationary perturbation theory are employed, and we also solve the time-dependent Schr\"odinger equation in a single-active electron model. We consider neon ionized by a FEL pulse whose fundamental frequency is in resonance with either $2p\text{\ensuremath{-}}3s$ or $2p\text{\ensuremath{-}}4s$ excitation. The contribution of the nonresonant two-photon process and its potential constructive or destructive role for quantum coherent control is investigated.

arXiv:1712.00842•Physical Review A•Jan 26, 2018•29 citations
We present first-principles numerical simulations of photoionization in neon induced by bichromatic extreme ultraviolet pulses with frequencies ωωω and 2ω2ω2ω, specially chosen to make ωωω equal to the energy difference between the 2s2s2s and 2p2p2p subshells. This allows for the production of photoelectrons from the 2s2s2s shell by 2ω2ω2ω pulse and from the 2p2p2p shell by ωωω pulse with the same energy. Using the multi-configurational time-dependent Hartree-Fock method, we explore how Rabi coupling between subshells generates coherence between the corresponding photoelectron wave packets. Our \textit{ab initio} calculations confirm the analytical results derived from the essential-states approach in [K. L. Ishikawa, K. C. Prince, and K. Ueda, J. Phys. Chem. A 127, 10638 (2023)], validating the theoretical predictions. Although we focus on the Ne 2p2p2p and 2s2s2s subshells, our approach is applicable to a broad range of systems exhibiting photoionization from multiple subshells. The laser parameters employed in our simulations are available in modern Free Electron Lasers (FELs), and we anticipate that this work could stimulate experimental investigations using FELs to study ion-photoelectron coherence and entanglement.
We investigate the coherent control of the photoelectron angular distribution in bichromatic atomic ionization. Neon is selected as target since it is one of the most popular systems in current gas-phase experiments with free-electron lasers (FELSs). In particular, we tackle practical questions, such as the role of the fine-structure splitting, the pulse length, and the intensity. Time-dependent and stationary perturbation theory are employed, and we also solve the time-dependent Schr\"odinger equation in a single-active electron model. We consider neon ionized by a FEL pulse whose fundamental frequency is in resonance with either $2p\text{\ensuremath{-}}3s$ or $2p\text{\ensuremath{-}}4s$ excitation. The contribution of the nonresonant two-photon process and its potential constructive or destructive role for quantum coherent control is investigated.