2017
DOI: 10.1063/1.4978953
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Enhanced laser radiation pressure acceleration of protons with a gold cone-capillary

Abstract: A scheme with gold cone-capillary is proposed to improve the protons acceleration and involved problems are investigated by using the two-dimensional particle-in-cell simulations. It is demonstrated that the cone-capillary can efficiently guide and collimate the protons to a longer distance and lead to a better beam quality with a dense density ≥ 10n c , monoenergetic peak energy E k ∼ 1.51 GeV, spatial emittance ∼ 0.0088 mm mrad with divergence angle θ ∼ 1.0 • and diameter ∼ 0.5µm. The enhancement is mainly a… Show more

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Cited by 3 publications
(2 citation statements)
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“…Among them, laser wakefield acceleration [37] and laser ponderomotive acceleration [38,39] are generally used to enhance electron acceleration and constraint. Recently, the radiation pressure acceleration (RPA) of ultra-thin foils is also applied to γ-ray emission and dense e + e − pairs production [40], as it is capable of obtaining high energy electrons and quasi-monoenergetic ion beams [41][42][43][44].…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…Among them, laser wakefield acceleration [37] and laser ponderomotive acceleration [38,39] are generally used to enhance electron acceleration and constraint. Recently, the radiation pressure acceleration (RPA) of ultra-thin foils is also applied to γ-ray emission and dense e + e − pairs production [40], as it is capable of obtaining high energy electrons and quasi-monoenergetic ion beams [41][42][43][44].…”
Section: Introductionmentioning
confidence: 99%
“…Among them, laser wakefield acceleration [43] and laser ponderomotive acceleration [44,45] are generally used to realize electron acceleration and constraint. Recently, the radiation pressure acceleration (RPA) of ultra-thin foils has also been applied to γ-ray emission and dense e e +pair production [46], as it is capable of obtaining high energy electrons and quasi-monoenergetic ion beams [47][48][49][50]. However, in this mechanism, the laser intensity of 5× 10 23 W cm −2 is too high to obtain experimentally and, on the other hand, the plane target cannot prevent the electrons from transverse escaping, while the radiative trapping [51] and pair plasma compression induced by standing wave fields can also be used to confine high-energy charged particles [6].…”
Section: Introductionmentioning
confidence: 99%