2019
DOI: 10.1063/1.5093613
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Development of gas jet targets for laser-plasma experiments at near-critical density

Abstract: Computational fluid dynamics simulations are performed to design gas nozzles, associated with a 1000 bars backing pressure system, capable of generating supersonic gas jet targets with densities close to the critical density for 1053 nm laser radiation (1021 cm−3). Such targets should be suitable for laser-driven ion acceleration at a high repetition rate. The simulation results are compared to the density profiles measured by interferometry, and characterization of the gas jet dynamics is performed using stri… Show more

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Cited by 29 publications
(26 citation statements)
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“…This scheme can be implemented at high repetition rate, in a debris free design. Using present high-density gas jets 33 , it allows the creation of a thin (∼ 10 µm) plasma slab of adjustable density up to 2 × 10 22 cm −3 . The typical lifetime of this transient target is ∼ 100 ps, hence the synchronization with the ps-pulse is easy to perform.…”
Section: Thin Over-critical Plasma Productionmentioning
confidence: 99%
See 1 more Smart Citation
“…This scheme can be implemented at high repetition rate, in a debris free design. Using present high-density gas jets 33 , it allows the creation of a thin (∼ 10 µm) plasma slab of adjustable density up to 2 × 10 22 cm −3 . The typical lifetime of this transient target is ∼ 100 ps, hence the synchronization with the ps-pulse is easy to perform.…”
Section: Thin Over-critical Plasma Productionmentioning
confidence: 99%
“…This scheme can be implemented at high repetition rate, in a debris free environment. Using present high-density gas jets 33 , it allows the creation of a thin (∼ 10 µm) plasma slab of adjustable density up to 2 × 10 22 cm −3 . The first part of this paper presents a study, based on hydrodynamic and on ion Fokker-Planck simulations, of this plasma tailoring method.…”
Section: Introductionmentioning
confidence: 99%
“…Over the years different schemes for laser-based electron and ion acceleration were proposed, such as laser-wakefield acceleration (LWFA) [6] , target normal sheath acceleration (TNSA) [7] , radiation pressure acceleration (RPA) [8] , and collisionless shock acceleration [9] . Improving laser-matter coupling in each of these mechanisms requires specific and delicate target design, such as specially designed gas jets, mass-limited and nanostructured solid targets [10][11][12] . A particularly promising ion acceleration scheme is one whereby a high-intensity laser interacts with a structured dynamic plasma target [13] .…”
Section: Introductionmentioning
confidence: 99%
“…Gas targets are naturally easier to refresh. High-energy ion beams resulting from collisionless shockwaves induced in nearly critical gas targets were demonstrated by either using long-wavelength laser pulses [23] or with very high-density gas [12,[24][25][26]. Tailoring the plasma profile around a solid foil target to enhance the emission of TNSA ions was also recently investigated [27].…”
Section: Introductionmentioning
confidence: 99%