2021
DOI: 10.1016/j.physrep.2020.12.002
|View full text |Cite
|
Sign up to set email alerts
|

Atomic, molecular and optical physics applications of longitudinally coherent and narrow bandwidth Free-Electron Lasers

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
4

Citation Types

0
13
0

Year Published

2021
2021
2023
2023

Publication Types

Select...
8
1

Relationship

3
6

Authors

Journals

citations
Cited by 34 publications
(16 citation statements)
references
References 417 publications
0
13
0
Order By: Relevance
“…The advent of high-intensity x-ray free-electron lasers (XFELs) has opened frontiers to study nonlinear ionization processes, such as the two-photon ionization (TPI) [1][2][3]. The TPI is one of the most fundamental nonlinear phenomena in the light-matter interaction process, in which an atom absorbs two photons and emits a photoelectron.…”
Section: Introductionmentioning
confidence: 99%
“…The advent of high-intensity x-ray free-electron lasers (XFELs) has opened frontiers to study nonlinear ionization processes, such as the two-photon ionization (TPI) [1][2][3]. The TPI is one of the most fundamental nonlinear phenomena in the light-matter interaction process, in which an atom absorbs two photons and emits a photoelectron.…”
Section: Introductionmentioning
confidence: 99%
“…The generation of ultra-bright electron sources is currently demanded in many fields of applications, ranging from high-resolution spectroscopy [ 1 ] to electron diffraction [ 2 ] and electron microscopy [ 3 ]. Laser-driven photocathode radio-frequency injectors are currently employed in particle accelerators to pursue enhanced beam brightness, which in turn grants unprecedented opportunities for material characterization following the dynamics of charge carriers in their natural space and time scales [ 4 ].…”
Section: Introductionmentioning
confidence: 99%
“…Changing the relative phase and the strength of harmonics provides a way to control the PADs as it was realized in the ω + 2ω process 30 years ago in the optical domain [16][17][18]. Recently, with the advent of longitudinally coherent free-electron lasers, experimental studies of the coherent control in the ω + 2ω process in the XUV wavelength range became possible and the first such measurements have been done [19][20][21].…”
Section: Introductionmentioning
confidence: 99%
“…20.03 0.89|2p 5 3d 3 P − 0.43|2p 5 3d 1 P − 0.12|2p 5 3d 3 D 2p 5 ( 2 P 3/2 )3d[3/2] 20.04 0.27|2p 5 3d 3 P + 0.72|2p 5 3d 1 P − 0.64|2p 5 3d 3 D 2p 5 ( 2 P 1/2 )3d[3/2]20.14 −0.36|2p 5 3d 3 P − 0.54|2p 5 3d 1 P − 0.76|2p 5 3d 3 D 2p 5( 2 P 3/2 )5s[3/2]20.57 −0.62|2p 5 5s 3 P − 0.78|2p 5 5s 1 P 2p 5( 2 P 1/2 )5s[1/2]20.66 −0.76|2p 5 5s 3 P + 0.60|2p 5 5s 1 P2p 5 ( 2 P 3/2 )4d[1/2]20.70 0.87|2p 5 4d 3 P − 0.39|2p 5 4d 1 P − 0.16|2p 5 4d 3 D − −0.20|2p 5 5s 3 P + 0.17|2p 5 5s 1 P 2p 5 ( 2 P 3/2 )4d[3/2] 20.71 0.18|2p 5 4d 3 P + 0.73|2p 5 4d 1 P − 0.66|2p 5 4d 3 D − −0.05|2p 5 5s 3 P + 0.05|2p 5 5s 1 P 2p 5 ( 2 P 1/2 )4d[3/2] 20.81 0.39|2p 5 4d 3 P + 0.57|2p 5 4d 1 P + 0.73|2p 5 4d 3 D 2p 5 ( 2 P 3/2 )6s[3/2] 20.95 0.60|2p 5 6s 3 P + 0.80|2p 5 6s 1 P 2p 5 ( 2 P 3/2 )5d[1/2] 21.01 0.90|2p 5 5d 3 P − 0.40|2p 5 5d 1 P − 0.18|2p 5 5d 3 D 2p 5 ( 2 P 3/2 )5d[3/2] 21.02 0.18|2p 5 5d 3 P + 0.72|2p 5 5d 1 P − 0.67|2p 5 5d 3 D 2p 5 ( 2 P 1/2 )6s[1/2] 21.04 −0.80|2p 5 6s 3 P + 0.60|2p 5 6s 1 P 2p 5 ( 2 P 1/2 )5d[3/2] 21.11 0.40|2p 5 5d 3 P + 0.57|2p 5 5d 1 P + 0.72|2p 5 5d 3 D…”
mentioning
confidence: 99%