2019
DOI: 10.1103/physrevlett.122.204802
|View full text |Cite
|
Sign up to set email alerts
|

Optimizing Laser Pulses for Narrow-Band Inverse Compton Sources in the High-Intensity Regime

Abstract: Scattering of ultraintense short laser pulses off relativistic electrons allows one to generate a large number of X-or gamma-ray photons with the expense of the spectral width-temporal pulsing of the laser inevitable leads to considerable spectral broadening. In this Letter, we describe a simple method to generate optimized laser pulses that compensate the nonlinear spectrum broadening, and can be thought of as a superposition of two oppositely linearly chirped pulses delayed with respect to each other. We dev… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1

Citation Types

0
20
0

Year Published

2021
2021
2023
2023

Publication Types

Select...
7
2

Relationship

0
9

Authors

Journals

citations
Cited by 33 publications
(20 citation statements)
references
References 40 publications
0
20
0
Order By: Relevance
“…Quantifying the emittance contribution thus requires further detailed designs considerations and investigations. An alternative path for generating mono-energetic ICS photons could be seen in using the higher harmonics from a non-linear Compton scattering source with optimised chirped laser pulses [122].…”
Section: Inverse Compton Sourcementioning
confidence: 99%
“…Quantifying the emittance contribution thus requires further detailed designs considerations and investigations. An alternative path for generating mono-energetic ICS photons could be seen in using the higher harmonics from a non-linear Compton scattering source with optimised chirped laser pulses [122].…”
Section: Inverse Compton Sourcementioning
confidence: 99%
“…As such, the on-axis emission is broadband unless the intensity is rather low. In order to overcome this, and obtain a narrowband source of Compton 𝛾 rays even when 𝑎 0 is not small, it has been proposed to chirp the pulse in a particular way [69][70][71][72][73]. If the instantaneous frequency of the pulse varies as 𝜔(𝜙) = 𝜔 0 [1 + 𝑎 2 rms (𝜙)], then 𝑠 = 2𝜂 0 /(1 + 2𝜂 0 ) for all 𝜙 and the nonlinear redshift is perfectly compensated.…”
Section: B Chirped Pulsesmentioning
confidence: 99%
“…Further motivation for improving the accuracy of modelling strong-field QED processes at the LUXE experiment, is provided by the search for new physics. The 'LUXE New Physics search with Optical Dump' LUXE-NPOD [76] is based on a secondary production mechanism that utilises the high-energy inverse Compton-scattered photons [77] produced in the electron beam-laser collision, to produce axionlike particles (ALPs) in a beam dump further downstream of the experiment. Such a setup will be sensitive to ALPs with masses O(MeV)-O(GeV), which is a range that has attracted much attention in recent years [78][79][80][81][82][83][84][85][86].…”
Section: Introductionmentioning
confidence: 99%