2002
DOI: 10.1117/12.450405
|View full text |Cite
|
Sign up to set email alerts
|

Compact high-repetition-rate femtosecond laser-driven hard x-ray source

Abstract: A compact, high-repetition rate, ultrashort-pulse laser-driven hard-x-ray source based on the combination of a femtosecond laser system with an x-ray diode is demonstrated. A comparison with available laser-plasma hard-x-ray sources is presented.Hard-x-ray fluxes exceeding 10 10 photons/s (emitted in 4π) are realized at a repetition rate of 250 kHz. Numerical modeling is performed which proves that picosecond and sub-picosecond hard-x-ray pulses can be produced with this source.

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1

Citation Types

0
2
0

Year Published

2011
2011
2018
2018

Publication Types

Select...
2

Relationship

0
2

Authors

Journals

citations
Cited by 2 publications
(2 citation statements)
references
References 12 publications
0
2
0
Order By: Relevance
“…As an additional consideration, the x-ray or electron source needs to be derived from a master laser oscillator to conserve time synchronization between the excitation or perturbation pulse driving the structural change and the structural probe pulse. Quantum efficiencies (QEs) for generating electron pulses based on photoemission range from QE ≈ 10 −4 for simple metals to about 10 −1 for semiconductor photocathodes [13]; whereas the conversion efficiency for the generation of x-ray photons in 'direct' fs-laser driven plasma sources is typically 10 −6 with several approaches to try to improve it [14][15][16][17][18][19][20]. This efficiency is further reduced by a limited solid angle of collection and x-ray optics by a factor of about 10 −2 at the sample's position.…”
Section: Introduction: Quest For Atomically Resolved Dynamicsmentioning
confidence: 99%
“…As an additional consideration, the x-ray or electron source needs to be derived from a master laser oscillator to conserve time synchronization between the excitation or perturbation pulse driving the structural change and the structural probe pulse. Quantum efficiencies (QEs) for generating electron pulses based on photoemission range from QE ≈ 10 −4 for simple metals to about 10 −1 for semiconductor photocathodes [13]; whereas the conversion efficiency for the generation of x-ray photons in 'direct' fs-laser driven plasma sources is typically 10 −6 with several approaches to try to improve it [14][15][16][17][18][19][20]. This efficiency is further reduced by a limited solid angle of collection and x-ray optics by a factor of about 10 −2 at the sample's position.…”
Section: Introduction: Quest For Atomically Resolved Dynamicsmentioning
confidence: 99%
“…First, the cross-section for electron scattering is ~ 6 orders of magnitude larger than that for X-ray scattering [10,67]. Second, the quantum efficiencies for generating electron pulses based on photoemission are on the order of 10 −4 and 10 −1 for metals and semiconductor photocathodes, respectively [68], whereas the conversion efficiency for the generation of X-ray photons is typically 10 −6 [69][70][71]. This efficiency is further reduced due to the limited solid angle of collection and X-ray optics by a factor of ~ 10 −2 at the position of the sample.…”
Section: Introductionmentioning
confidence: 99%