2009
DOI: 10.1063/1.3067825
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Effect of plasma density scale length on the properties of bremsstrahlung x-ray sources created by picosecond laser pulses

Abstract: Results of an experimental study of multi-MeV bremsstrahlung x-ray sources created by picosecond laser pulses are presented. The x-ray source is created by focusing the short pulse in an expanding plasma obtained by heating a solid target with a time-delayed nanosecond laser beam. The high-energy part of the x-ray spectrum and emission lobe are inferred from photonuclear activation techniques. The x-ray dose is measured with silicon diodes. Two-dimensional images of the source are reconstructed from a penumbra… Show more

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Cited by 67 publications
(49 citation statements)
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“…Laser-driven accelerators offer a cheaper and smaller alternative, and they are now capable of generating bursts of γ -rays10. γ -ray generation has been demonstrated in a number of experiments on laser interactions with solid and gas targets, where the main mechanism is the Bremsstrahlung radiation of fast electrons interacting with high-Z material targets11121314151617. However, due to the small bremsstrahlung cross-section, the conversion efficiency of this scheme is rather low.…”
mentioning
confidence: 99%
“…Laser-driven accelerators offer a cheaper and smaller alternative, and they are now capable of generating bursts of γ -rays10. γ -ray generation has been demonstrated in a number of experiments on laser interactions with solid and gas targets, where the main mechanism is the Bremsstrahlung radiation of fast electrons interacting with high-Z material targets11121314151617. However, due to the small bremsstrahlung cross-section, the conversion efficiency of this scheme is rather low.…”
mentioning
confidence: 99%
“…If a high-Z solid target is set behind the interaction zone, the relativistic electrons thus produced generate in turn an intense Bremsstrahlung emission upon slowing down and colliding in this radiator. [15][16][17][18] Such multi-MeV x-ray sources are used in various applications such as radiography of dense objects, 16,[19][20][21][22] photonuclear fission and activation, 15,[23][24][25] positron emission, [26][27][28] and also pose radiological constraints to the facilities. 29 The temporal and spatial characteristics of these sources are, respectively, in the few picosecond and few hundred micron ranges, significantly better than for the sources produced by electron induction accelerators, diodes, or rod pinches usually used for flash radiography.…”
Section: Introductionmentioning
confidence: 99%
“…Previously, prior researches have mainly been focused on the radiation from electrons generated by laser-driven * Authors to whom correspondence should be addressed. Electronic mail: yi@uni-duesseldorf.de wakefield accelerators (LWFAs) [14][15][16] as well as hot electrons produced in interactions of high power laser and foils [17][18][19][20][21] or near-critical-density (NCD) plasmas [22][23][24]. However, although the x-ray source based on LWFA is more mature, the electron number produced by the LWFA is limited by the underdense plasma required for wakefield excitation, which further results in a relativelysmall photon yield.…”
Section: Introductionmentioning
confidence: 99%