2017
DOI: 10.1088/2040-8986/aa9b04
|View full text |Cite
|
Sign up to set email alerts
|

Compact 200 kHz HHG source driven by a few-cycle OPCPA

Abstract: -Collection and spectral control of highorder harmonics generated with a 50 W high-repetition rate Ytterbium femtosecond laser system A Cabasse, Ch Hazera, L Quintard et al. AbstractWe present efficient high-order harmonic generation (HHG) based on a high-repetition rate, few-cycle, near infrared (NIR), carrier-envelope phase stable, optical parametric chirped pulse amplifier (OPCPA), emitting 6 fs pulses with 9 μJ pulse energy. In krypton, we reach conversion efficiencies from the NIR to the extreme ultravio… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
5

Citation Types

3
53
0

Year Published

2019
2019
2024
2024

Publication Types

Select...
8
1

Relationship

3
6

Authors

Journals

citations
Cited by 63 publications
(56 citation statements)
references
References 36 publications
3
53
0
Order By: Relevance
“…This article both summarizes and extends the previous work [14,15]. The laser system, located at the Lund High-Power Facility of the Lund Laser Centre, is based on optical parametric chirped pulse amplification (OPCPA), providing sub-6fs long pulses with stabilized carrier-to-envelope phase (CEP) in the nearinfrared (IR) with up to 15 μJ pulse energy at a repetition rate of 200 kHz [14]. The 200-fold increase in repetition rate, compared to standard 1 kHz systems, promotes experiments with high demands on statistics.…”
Section: Introductionsupporting
confidence: 82%
See 1 more Smart Citation
“…This article both summarizes and extends the previous work [14,15]. The laser system, located at the Lund High-Power Facility of the Lund Laser Centre, is based on optical parametric chirped pulse amplification (OPCPA), providing sub-6fs long pulses with stabilized carrier-to-envelope phase (CEP) in the nearinfrared (IR) with up to 15 μJ pulse energy at a repetition rate of 200 kHz [14]. The 200-fold increase in repetition rate, compared to standard 1 kHz systems, promotes experiments with high demands on statistics.…”
Section: Introductionsupporting
confidence: 82%
“…Here, we present a high-repetition rate, flexible attosecond light source, particularly designed for the study of gas phase correlated electron dynamics, as well as timeresolved nanoscale imaging. This article both summarizes and extends the previous work [14,15]. The laser system, located at the Lund High-Power Facility of the Lund Laser Centre, is based on optical parametric chirped pulse amplification (OPCPA), providing sub-6fs long pulses with stabilized carrier-to-envelope phase (CEP) in the nearinfrared (IR) with up to 15 μJ pulse energy at a repetition rate of 200 kHz [14].…”
Section: Introductionmentioning
confidence: 80%
“…1c. Our laser system [33] is based on an ultrabroadband titanium-sapphire oscillator capable of delivering sub-6-fs pulses. The oscillator pulses are amplified in an optical parametric chirped pulse amplifier employing beta barium borate (BBO) crystals.…”
Section: Introductionmentioning
confidence: 99%
“…Historically, the peak intensities necessary for high-flux or high-photon-energy HHG, typically > 10 14 W/cm 2 , have meant that viable laser systems were limited to amplifiers bottle-necked to less than 10 kHz repetition rates. Although other methods such as enhancement cavities [24][25][26] or tight-focusing geometries with lower pulse power [27][28][29][30] have achieved HHG at higher repetition rates, both methods introduce additional experimental challenges that can limit their applicability. The Extreme Light Infrastructure Attosecond Light Pulse Source (ELI-ALPS) facility [31] has been constructed in order to push the frontiers of attosecond science.…”
Section: Introductionmentioning
confidence: 99%