2020
DOI: 10.1103/physreva.101.023407
|View full text |Cite
|
Sign up to set email alerts
|

Optimization of high-order harmonic generation by optimal control theory: Ascending a functional landscape in extreme conditions

Abstract: The ω sampling is the same as the DCT sampling (Cf. Eq. (C5)). The functional has to be expressed by the terms of the discrete optimization space:where J d is a discretized variant of J. Theǭ(ω) dependence in J is reformulated by discrete means;J energy is replaced by

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1

Citation Types

0
2
0

Year Published

2020
2020
2021
2021

Publication Types

Select...
4

Relationship

0
4

Authors

Journals

citations
Cited by 4 publications
(2 citation statements)
references
References 68 publications
(136 reference statements)
0
2
0
Order By: Relevance
“…To reduce the sensitivity to the noises, the high-frequency components in h is reduced by penalizing the energy of high-order derivatives [30], which is given by…”
Section: Related Workmentioning
confidence: 99%
“…To reduce the sensitivity to the noises, the high-frequency components in h is reduced by penalizing the energy of high-order derivatives [30], which is given by…”
Section: Related Workmentioning
confidence: 99%
“…[30][31][32][33][34][35][36][37][38] While there is an extensive amount of work on controlling laser-matter interactions via selected field parameters such as carrier envelope phase or polarization, so far the application of full control theory to strong-field science and to double ionization in particular has been limited. Some selected applications to date include control of single ionization, 34,[39][40][41] and experimental pulse optimization for double ionization with IR pulses. 37 The objective of this article is twofold.…”
Section: Introductionmentioning
confidence: 99%