2019
DOI: 10.1063/1.5081509
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Characterization of supersonic and subsonic gas targets for laser wakefield electron acceleration experiments

Abstract: The choice of the correct density profile is crucial in laser wakefield acceleration. In this work, both subsonic and supersonic gas targets are characterized by means of fluid-dynamic simulations and experimental interferometric measurements. The gas targets are studied in different configurations, and the density profiles most suitable for laser wakefield acceleration are discussed.

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Cited by 34 publications
(24 citation statements)
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“…The system of partial differential equations consisting of Navier–Stokes equations for compressible flow, equation of conservation of energy and Shear Stress Transport turbulence model is solved by Finite Volume Method. More details of the simulation method are addressed in 23 . As seen in Fig.…”
Section: Resultsmentioning
confidence: 99%
“…The system of partial differential equations consisting of Navier–Stokes equations for compressible flow, equation of conservation of energy and Shear Stress Transport turbulence model is solved by Finite Volume Method. More details of the simulation method are addressed in 23 . As seen in Fig.…”
Section: Resultsmentioning
confidence: 99%
“…but also an innovative subsonic gas jet with a 100-µm long micro-capillary coupled to a blade and a fast gas-valve [11] and a cryogenic hydrogen ribbon delivery system [12]. A continuous effort is put on the development of reliable solutions for rapid target delivery, data acquisition and real-time data analysis, suitable for proton acceleration schemes at high repetition rates that were preliminary tested at TERESA up to 3.3 Hz [13,14].…”
Section: Discussionmentioning
confidence: 99%
“…Two target systems are available at TERESA by default: a target matrix with up to 900 solid targets (usually plastic or metallic foils) [6], operating at repetition rates up to 1 Hz and a gas jet, operating with various gas types and pressures [7], as typically employed in laser wake-field electron acceleration, with special care taken over the total amount of gas released into the chamber to allow the target operation at 10 Hz. The list of targets that have been tested at TERESA includes not only conventional thin foils and gas targets, but also an innovative subsonic gas jet with a 100-µm long micro-capillary coupled to a blade and a fast gas-valve [11] and a cryogenic hydrogen ribbon delivery system [12]. A continuous effort is put on the development of reliable solutions for rapid target delivery, data acquisition and real-time data analysis, suitable for proton acceleration schemes at high repetition rates that were preliminary tested at TERESA up to 3.3 Hz [13,14].…”
Section: Available Diagnostics and Target Systemsmentioning
confidence: 99%
“…The valve backing pressure was varied in the range of 20-64 bar, corresponding to a gas density in the range 2-6 × 10 19 atoms/cm 3 (1 mm above the nozzle). The gas density profile was measured experimentally and simulated using the FLUENT code (details are available in [21]). The gas density profile was uniform along the 1.26-mm side (or z-axis) for the Ar case, while for the N case two peaks were present at the boundaries with density increase of 1.15 times the density at the center.…”
Section: Methodsmentioning
confidence: 99%