Plasma-guided Compton source

We investigated numerically the emission properties of an x-ray source based on direct laser acceleration of electrons interacting with an intense counterpropagating laser pulse. The source was realized by irradiating from both sides a high atomic number plasma-plume target. The resulting x-ray beam was analyzed through three-dimensional particle-in-cell simulations for its spectral content, source size, angular divergence, and temporal structure. For simulated experiments in which the total laser-pulse energy was 1.5 J, we obtained a peak brightness of approximately ${10}^{22}\phantom{\rule{0.2em}{0ex}}(\mathrm{s}\phantom{\rule{0.2em}{0ex}}{\mathrm{mrad}}^{2}\phantom{\rule{0.2em}{0ex}}{\mathrm{mm}}^{2}\phantom{\rule{0.2em}{0ex}}0.1\mathrm{%}\mathrm{BW}{)}^{\ensuremath{-}1}$ of x-ray photons peaking at an energy of 25 keV. The results and their competitiveness in applications are discussed and compared with other laser-based x-ray generation methods.

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Publication Details

Journal
Physical Review Applied
Published
2024-10-02
DOI
https://doi.org/10.1103/physrevapplied.22.044004
Citations
1
Primary Topic
Laser-Plasma Interactions and Diagnostics
Type
article
Field-Weighted Citation Impact
0.66

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article

Plasma-guided Compton source

M. Fraenkel, Talia Meir, Itamar Cohen, Ishay Pomerantz et al.
1 citations
Physical Review Applied
Laser-Plasma Interactions and Diagnostics
0.66
article

Plasma-guided Compton source

M. Fraenkel, Talia Meir, Itamar Cohen, Ishay Pomerantz, Alexey Arefiev, Kavin Tangtartharakul, Tamir Cohen
article en
1 citations

Abstract

We investigated numerically the emission properties of an x-ray source based on direct laser acceleration of electrons interacting with an intense counterpropagating laser pulse. The source was realized by irradiating from both sides a high atomic number plasma-plume target. The resulting x-ray beam was analyzed through three-dimensional particle-in-cell simulations for its spectral content, source size, angular divergence, and temporal structure. For simulated experiments in which the total laser-pulse energy was 1.5 J, we obtained a peak brightness of approximately ${10}^{22}\phantom{\rule{0.2em}{0ex}}(\mathrm{s}\phantom{\rule{0.2em}{0ex}}{\mathrm{mrad}}^{2}\phantom{\rule{0.2em}{0ex}}{\mathrm{mm}}^{2}\phantom{\rule{0.2em}{0ex}}0.1\mathrm{%}\mathrm{BW}{)}^{\ensuremath{-}1}$ of x-ray photons peaking at an energy of 25 keV. The results and their competitiveness in applications are discussed and compared with other laser-based x-ray generation methods.

Physical Review AppliedVol. 22(4)
Tel Aviv University (IL), University of California San Diego (US)
National Science Foundation, United States-Israel Binational Science Foundation, Ministry of Science and Technology, Israel, Engineering and Physical Sciences Research Council
Openalex Percentile: Top 14%
Laser-Plasma Interactions and Diagnostics
0.66
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