697 research outputs found

    Laser-wakefield accelerators as hard x-ray sources for 3D medical imaging of human bone

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    A bright μm-sized source of hard synchrotron x-rays (critical energy Ecrit > 30 keV) based on the betatron oscillations of laser wakefield accelerated electrons has been developed. The potential of this source for medical imaging was demonstrated by performing micro-computed tomography of a human femoral trabecular bone sample, allowing full 3D reconstruction to a resolution below 50 μm. The use of a 1 cm long wakefield accelerator means that the length of the beamline (excluding the laser) is dominated by the x-ray imaging distances rather than the electron acceleration distances. The source possesses high peak brightness, which allows each image to be recorded with a single exposure and reduces the time required for a full tomographic scan. These properties make this an interesting laboratory source for many tomographic imaging applications

    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

    Control of Strong-Laser-Field Coupling to Electrons in Solid Targets with Wavelength-Scale Spheres

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    Irradiation of a planar solid by an intense laser pulse leads to fast electron acceleration and hard x-ray production. We have investigated whether this high field production of fast electrons can be controlled by introducing dielectric spheres of well-defined size on the target surface. We find that the presence of spheres with a diameter slightly larger than half the laser wavelength leads to Mie enhancements of the laser field which, accompanied by multipass stochastic heating of the electrons, leads to significantly enhanced hard x-ray yield and temperature

    Ultra-high brilliance multi-MeV γ\gamma-ray beam from non-linear Thomson scattering

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    We report on the generation of a narrow divergence (θ≈2.5\theta\approx 2.5 mrad), multi-MeV (EMAX=18E_\text{MAX} = 18 MeV) and ultra-high brilliance (≈2×1019\approx 2\times10^{19} photons s−1^{-1} mm−2^{-2} mrad −2^{-2} 0.1\% BW) γ\gamma-ray beam from the scattering of an ultra-relativistic laser-wakefield accelerated electron beam in the field of a relativistically intense laser (dimensionless amplitude a0≈2a_0\approx2). The spectrum of the generated γ\gamma-ray beam is measured, with MeV resolution, seamlessly from 6 MeV to 18 MeV, giving clear evidence of the onset of non-linear Thomson scattering. The photon source has the highest brilliance in the multi-MeV regime ever reported in the literature

    Inverse problem for wave equation with sources and observations on disjoint sets

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    We consider an inverse problem for a hyperbolic partial differential equation on a compact Riemannian manifold. Assuming that Γ1\Gamma_1 and Γ2\Gamma_2 are two disjoint open subsets of the boundary of the manifold we define the restricted Dirichlet-to-Neumann operator ΛΓ1,Γ2\Lambda_{\Gamma_1,\Gamma_2}. This operator corresponds the boundary measurements when we have smooth sources supported on Γ1\Gamma_1 and the fields produced by these sources are observed on Γ2\Gamma_2. We show that when Γ1\Gamma_1 and Γ2\Gamma_2 are disjoint but their closures intersect at least at one point, then the restricted Dirichlet-to-Neumann operator ΛΓ1,Γ2\Lambda_{\Gamma_1,\Gamma_2} determines the Riemannian manifold and the metric on it up to an isometry. In the Euclidian space, the result yields that an anisotropic wave speed inside a compact body is determined, up to a natural coordinate transformations, by measurements on the boundary of the body even when wave sources are kept away from receivers. Moreover, we show that if we have three arbitrary non-empty open subsets Γ1,Γ2\Gamma_1,\Gamma_2, and Γ3\Gamma_3 of the boundary, then the restricted Dirichlet-to-Neumann operators ΛΓj,Γk\Lambda_{\Gamma_j,\Gamma_k} for 1≤j<k≤31\leq j<k\leq 3 determine the Riemannian manifold to an isometry. Similar result is proven also for the finite-time boundary measurements when the hyperbolic equation satisfies an exact controllability condition
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