147 research outputs found

    A multi-shot target-wheel assembly for high-repetition-rate, laser-driven proton acceleration

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    A multi-shot target assembly and automatic alignment procedure for laser-plasma proton acceleration at high-repetition-rate are introduced. The assembly is based on a multi-target rotating wheel capable of hosting >>5000 targets, mounted on a three-dimensional motorised stage to allow rapid replenishment and alignment of the target material between laser irradiations. The automatic alignment procedure consists of a detailed mapping of the impact positions at the target surface prior to the irradiation that ensures stable operation of the target, which alongside the purpose-built design of the target wheel, enable the operation at rates up to 10 Hz. Stable and continuous laser-driven proton acceleration is demonstrated, with observed cut-off energy stability about 15%.Comment: 8 pages, 5 figure

    Measurements of the \gamma * p --> \Delta(1232) reaction at low Q2

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    We report new p(e,ep)π(\vec{e},e^\prime p)\pi^\circ measurements in the Δ+(1232)\Delta^{+}(1232) resonance at the low momentum transfer region utilizing the magnetic spectrometers of the A1 Collaboration at MAMI. The mesonic cloud dynamics are predicted to be dominant and appreciably changing in this region while the momentum transfer is sufficiently low to be able to test chiral effective calculations. The results disagree with predictions of constituent quark models and are in reasonable agreement with dynamical calculations with pion cloud effects, chiral effective field theory and lattice calculations. The reported measurements suggest that improvement is required to the theoretical calculations and provide valuable input that will allow their refinements

    Lowest Q^2 Measurement of the gamma*p -> Delta Reaction: Probing the Pionic Contribution

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    To determine nonspherical angular momentum amplitudes in hadrons at long ranges (low Q^2), data were taken for the p(\vec{e},e'p)\pi^0 reaction in the Delta region at Q^2=0.060 (GeV/c)^2 utilizing the magnetic spectrometers of the A1 Collaboration at MAMI. The results for the dominant transition magnetic dipole amplitude and the quadrupole to dipole ratios at W=1232 MeV are: M_{1+}^{3/2} = (40.33 +/- 0.63_{stat+syst} +/- 0.61_{model}) (10^{-3}/m_{\pi^+}),Re(E_{1+}^{3/2}/M_{1+}^{3/2}) = (-2.28 +/- 0.29_{stat+syst} +/- 0.20_{model})%, and Re(S_{1+}^{3/2}/M_{1+}^{3/2}) = (-4.81 +/- 0.27_{stat+syst} +/- 0.26_{model})%. These disagree with predictions of constituent quark models but are in reasonable agreement with lattice calculations with non-linear (chiral) pion mass extrapolations, with chiral effective field theory, and with dynamical models with pion cloud effects. These results confirm the dominance, and general Q^2 variation, of the pionic contribution at large distances.Comment: 6 pages, 3 figures, 1 tabl

    First measurements of the ^16O(e,e'pn)^14N reaction

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    This paper reports on the first measurement of the ^16O(e,e'pn)^14N reaction. Data were measured in kinematics centred on a super-parallel geometry at energy and momentum transfers of 215 MeV and 316 MeV/c. The experimental resolution was sufficient to distinguish groups of states in the residual nucleus but not good enough to separate individual states. The data show a strong dependence on missing momentum and this dependence appears to be different for two groups of states in the residual nucleus. Theoretical calculations of the reaction using the Pavia code do not reproduce the shape or the magnitude of the data.Comment: 10 pages, 11 figures, 2 tables, Accepted for publication in EPJ

    Measurement of the Beam-Recoil Polarization in Low-Energy Virtual Compton Scattering from the Proton

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    Double-polarization observables in the reaction epepγ\vec{e}p \rightarrow e'\vec{p'}\gamma{} have been measured at Q2=0.33(GeV/c)2Q^2=0.33 (GeV/c)^2. The experiment was performed at the spectrometer setup of the A1 Collaboration using the 855 MeV polarized electron beam provided by the Mainz Microtron (MAMI) and a recoil proton polarimeter. From the double-polarization observables the structure function PLTP_{LT}^\perp is extracted for the first time, with the value (15.4±3.3(stat.)2.4+1.5(syst.))GeV2(-15.4 \pm 3.3 (stat.)^{+1.5}_{-2.4} (syst.)) GeV^{-2}, using the low-energy theorem for Virtual Compton Sattering. This structure function provides a hitherto unmeasured linear combination of the generalized polarizabilities of the proton

    Final State Interaction Effects in pol 3He(pol e,e'p)

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    Asymmetries in quasi-elastic pol 3He(pol e,e'p) have been measured at a momentum transfer of 0.67 (GeV/c)^2 and are compared to a calculation which takes into account relativistic kinematics in the final state and a relativistic one-body current operator. With an exact solution of the Faddeev equation for the 3He-ground state and an approximate treatment of final state interactions in the continuum good agreement is found with the experimental data.Comment: 11 pages, 6 figures, submitted to Phys. Lett. B, revised version, sensitivity study to relativity and NN-potential adde

    Spectral characterization of laser-accelerated protons with CR-39 nuclear track detector

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    CR-39 nuclear track material is frequently used for the detection of protons accelerated in laser-plasma interactions. The measurement of track densities allows for determination of particle angular distributions, and information on the kinetic energy can be obtained by the use of passive absorbers. We present a precise method of measuring spectral distributions of laser-accelerated protons in a single etching and analysis process. We make use of a one-to-one relation between proton energy and track size and present a precise calibration based on monoenergetic particle beams. While this relation is limited to proton energies below 1 MeV, we show that the range of spectral measurements can be significantly extended by simultaneous use of absorbers of suitable thicknesses. Examples from laser-plasma interactions are presented, and quantitative results on proton energies and particle numbers are compared to those obtained from a time-of-flight detector. The spectrum end points of continuous energy distributions have been determined with both detector types and coincide within 50-100 keV

    A new measurement of the structure functions PLLPTT/epsilonP_{LL}-P_{TT}/epsilon and PLTP_{LT} in virtual Compton scattering at Q2=Q^2= 0.33 (GeV/c)2^2

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    The cross section of the epepγep \to e' p' \gamma reaction has been measured at Q2=0.33Q^2 = 0.33 (GeV/c)2^2. The experiment was performed using the electron beam of the MAMI accelerator and the standard detector setup of the A1 Collaboration. The cross section is analyzed using the low-energy theorem for virtual Compton scattering, yielding a new determination of the two structure functions P_LL}-P_{TT}/epsilon and PLTP_{LT} which are linear combinations of the generalized polarizabilities of the proton. We find somewhat larger values than in the previous investigation at the same Q2Q^2. This difference, however, is purely due to our more refined analysis of the data. The results tend to confirm the non-trivial Q2Q^2-evolution of the generalized polarizabilities and call for more measurements in the low-Q2Q^2 region (\le 1 (GeV/c)2^2).Comment: 9 pages, 10 figures. EPJA version. slight revisions in the text and figure

    Self energies of the pion and the delta isobar from the ^3He(e,e'pi^+)^3H reaction

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    In a kinematically complete experiment at the Mainz microtron MAMI, pion angular distributions of the 3^3He(e,e'π+)3\pi^+)^3H reaction have been measured in the excitation region of the Δ\Delta resonance to determine the longitudinal (LL), transverse (TT), and the LTLT interference part of the differential cross section. The data are described only after introducing self-energy modifications of the pion and Δ\Delta-isobar propagators. Using Chiral Perturbation Theory (ChPT) to extrapolate the pion self energy as inferred from the measurement on the mass shell, we deduce a reduction of the π+\pi^+ mass of Δmπ+=(1.72.1+1.7)\Delta m_{\pi^+} = (-1.7^{+ 1.7}_{- 2.1}) MeV/c2^2 in the neutron-rich nuclear medium at a density of ρ=(0.0570.057+0.085)\rho = (0.057^{+ 0.085}_{- 0.057}) fm3^{-3}. Our data are consistent with the Δ\Delta self energy determined from measurements of π0\pi^0 photoproduction from 4^4He and heavier nuclei.Comment: Elsart, 12 pages and 4 figures, Correspondent: Professor Dr. Dr. h.c. mult. Achim Richter, [email protected], submitted to Phys. Rev. Let
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