2019
DOI: 10.1088/1367-2630/ab1047
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Interaction of relativistically intense laser pulses with long-scale near critical plasmas for optimization of laser based sources of MeV electrons and gamma-rays

Abstract: Experiments were performed to study electron acceleration by intense sub-picosecond laser pulses propagating in sub-mm long plasmas of near critical electron density (NCD). Low density foam layers of 300-500 μm thickness were used as targets. In foams, the NCD-plasma was produced by a mechanism of super-sonic ionization when a well-defined separate ns-pulse was sent onto the foamtarget forerunning the relativistic main pulse. The application of sub-mm thick low density foam layers provided a substantial increa… Show more

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Cited by 75 publications
(76 citation statements)
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“…The effective temperature of the DLA accelerated electrons exceeds more than one order of magnitude the ponderomotive potential and their energies extend up to 100 MeV, already at moderate relativistic laser intensities 55 , 56 . The reason for this behavior is a long acceleration path in a NCD plasma ensured by pre-ionized sub-mm thick foams and a relatively long sub-ps laser pulse duration.…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…The effective temperature of the DLA accelerated electrons exceeds more than one order of magnitude the ponderomotive potential and their energies extend up to 100 MeV, already at moderate relativistic laser intensities 55 , 56 . The reason for this behavior is a long acceleration path in a NCD plasma ensured by pre-ionized sub-mm thick foams and a relatively long sub-ps laser pulse duration.…”
Section: Resultsmentioning
confidence: 99%
“…These different intensity regimes were achieved by different focusing systems 56 . Polymer aerogel-foams with a mean density of 2 mg/cm 3 and sub-millimeter thickness 65 were used for the production of a NCD-plasma via the mechanism of super-sonic ionization 55 , 66 by sending a well-controlled nanosecond-pulse before the main relativistic pulse. A fully ionized plasma corresponds to 0.64 × 10 21 cm −3 electron density or 0.64 n cr ( n cr = 10 21 cm −3 ).…”
Section: Resultsmentioning
confidence: 99%
“…The TPS has an acceptance angle of 2 µSr and is capable of detecting protons with energy from 30 keV up to several MeV in a single shot. We also used a calibrated electron spectrometer [25] based on magnetic deflection with image plates to measure the temperature of the electrons along the target normal direction. This spectrometer has an acceptance angle of 0.3 mSr and can measure up to several of tens of MeV.…”
Section: Methodsmentioning
confidence: 99%
“…It was shown in Refs. [6][7][8] that the application of foam nanostructure targets resulted in a significant increase of X-ray emission from a laser plasma [9] . Unfortunately for most of the cases, the production of these targets is a complicated many-step process, which makes such target application rather expensive for wide use.…”
Section: Introductionmentioning
confidence: 98%