9 research outputs found

    Bright X-ray radiation from plasma bubbles in an evolving laser wakefield accelerator

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    We show that the properties of the electron beam and bright x-rays produced by a laser wakefield accelerator can be predicted if the distance over which the laser self-focuses and compresses prior to self-injection is taken into account. A model based on oscillations of the beam inside a plasma bubble shows that performance is optimised when the plasma length is matched to the laser depletion length. With a 200~TW laser pulse this results in an x-ray beam with median photon energy of \unit[20]{keV}, >6×108> 6\times 10^{8} photons above \unit[1]{keV} per shot and a peak brightness of \unit[3 \times 10^{22}]{photons~s^{-1}mrad^{-2}mm^{-2} (0.1\% BW)^{-1}}.Comment: 5 pages, 4 figure

    Observation of laser power amplification in a self-injecting laser wakefield accelerator

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    We report on the depletion and power amplification of the driving laser pulse in a strongly-driven laser wakefield accelerator. Simultaneous measurement of the transmitted pulse energy and temporal shape indicate an increase in peak power from 187±11187 \pm 11TW to a maximum of 318±12318 \pm 12 TW after 13 mm of propagation in plasma density of 0.9×10180.9 \times 10^{18} cm−3^{-3}. The power amplification is correlated with the injection and acceleration of electrons in the non-linear wakefield. This process is modeled by including localized redshifting and subsequent group delay dispersion at the laser pulse front

    Bright X-ray radiation from plasma bubbles in an evolving laser wakefield accelerator

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    We show that the properties of the electron beam and bright X-rays produced by a laser wakefield accelerator can be predicted if the distance over which the laser self-focuses and compresses prior to self-injection is taken into account. A model based on oscillations of the beam inside a plasma bubble shows that performance is optimised when the plasma length is matched to the laser depletion length. With a 200~TW laser pulse this results in an X-ray beam with median photon energy of 20 keV, >109> 10^{9} photons per shot and a peak brightness of 4×10234 \times 10^{23} photons s−1^{-1} mrad−2^{-2} mm−2^{-2} (0.1 % BW)−1^{-1}

    Producing bright X-rays for imaging applications using a laser wakefield accelerator

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    We report on the generation of bright multi-keV betatron X-ray radiation using a GeV laser wakefield accelerator and investigate the use of these X-rays for various imaging applications. © 2014 Optical Society of America

    Producing bright X-rays for imaging applications using a laser wakefield accelerator

    No full text
    We report on the generation of bright multi-keV betatron X-ray radiation using a GeV laser wakefield accelerator and investigate the use of these X-rays for various imaging applications. © 2014 Optical Society of America
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