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428 result(s) for "Denig, A"
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Measurement of the 12C(e,e′) Cross Sections at Q2=0.8GeV2/c2
We present the findings of a study based on a new inelastic electron-scattering experiment on the 12C nucleus focusing on the kinematic region of Q2=0.8GeV2/c2. The measured cross section is sensitive to the transverse response function and provides a stringent test of theoretical models, as well as of the theoretical assumptions made in Monte-Carlo event-generator codes developed for the interpretation of neutrino-nucleus experiments, such as DUNE and HyperK. We find that modern generators such as GENIE and GiBUU reproduce our new experimental data within 10%.
The MAGIX focal plane time projection chamber
The MAGIX experiment is a versatile system optimized for low-energy nuclear and particle physics measurements. The setup is currently under development and will be installed at the MESA electron accelerator, at the Institute for Nuclear Physics of the University of Mainz. The main detectors of that experiment are a couple of high-precision magnetic spectrometers, each of them equipped with a GEM-based TPC at the focal plane to achieve a momentum resolution and angular resolution at the scattering vertex respectively of ≈δPP<10−4and≈1 1 mrad on scattered electron momenta between 1 MeV/c and 105 MeV/c. The limiting factor to achieve those results is the amount and uniformity of the material before the focal plane and even the presence of the TPC field cage can be relevant. Therefore we developed, and hereby introduce, an open field-cage TPC to fulfil those challenging requirements.
Offline Software for the PANDA Luminosity Detector
In 2018 data taking for hadronphysics facility PANDA is planned to commence. It will be build at the antiproton accelerator HESR, which itself is a part of the FAIR complex (GSI, Darmstadt, Germany). The luminosity at PANDA will be measured by a dedicated sub-detector, which will register scattered antiproton tracks from pp elastic scattering. From a software point of view, the Luminosity Detector is a tracking system. Therefore the most of its offline software parts are typical for a track reconstruction. The basic concept and Monte Carlo based performance studies of each reconstruction step is presented in this paper.
Quest for precision in hadronic cross sections at low energy: Monte Carlo tools vs. experimental data
We present the achievements of the last years of the experimental and theoretical groups working on hadronic cross section measurements at the low-energy e + e − colliders in Beijing, Frascati, Ithaca, Novosibirsk, Stanford and Tsukuba and on τ decays. We sketch the prospects in these fields for the years to come. We emphasise the status and the precision of the Monte Carlo generators used to analyse the hadronic cross section measurements obtained as well with energy scans as with radiative return, to determine luminosities and τ decays. The radiative corrections fully or approximately implemented in the various codes and the contribution of the vacuum polarisation are discussed.
Non-forward radiative corrections to electron-carbon scattering
Radiative corrections to elastic scattering represent an important part of the interpretation of electron-induced nuclear reactions at small energy transfers, where they represent a dominant part of the background. Here we present and validate a new event generator for simulating QED radiative processes in electron-carbon scattering that exactly calculates the coherent sum of the Bethe-Heitler amplitudes for the leading diagrams. We demonstrate that the generator describes the shape of the radiative tail of an elastic peak with a precision better than 10 % over the whole energy range of the scattered electrons and can thus be reliably employed in the analyses of electron scattering experiments for more precise extraction of inelastic cross-sections.
Precise measurement of Γ(K→e ν(γ))/Γ(K→μ ν(γ)) and study of K→e ν γ
We present a precise measurement of the ratio RK=Γ(K→eν(γ))/Γ(K→μν(γ)) and a study of the radiative process K→eνγ, performed with the KLOE detector. The results are based on data collected at the Frascati e+e− collider DAΦNE for an integrated luminosity of 2.2 fb−1. We find RK=(2.493±0.025stat±0.019syst)×10−5, in agreement with the Standard Model expectation. This result is used to improve constraints on parameters of the Minimal Supersymmetric Standard Model with lepton flavor violation. We also measured the differential decay rate dΓ(K→eνγ)/dEγ for photon energies 10
Offine Software for the PANDA Luminosity Detector
In 2018 data taking for hadronphysics facility PANDA is planned to commence. It will be build at the antiproton accelerator HESR, which itself is a part of the FAIR complex (GSI, Darmstadt, Germany). The luminosity at PANDA will be measured by a dedicated sub-detector, which will register scattered antiproton tracks from pp elastic scattering. From a software point of view, the Luminosity Detector is a tracking system. Therefore the most of its offline software parts are typical for a track reconstruction. The basic concept and Monte Carlo based performance studies of each reconstruction step is presented in this paper.
Improved measurement of the absolute branching fraction ofD⁺→ K̄⁰ μ ⁺ν _(μ)
Here, by analyzing 2.93 fb-1 of data collected at √s = 3.773 GeV with the BESIII detector, we measure the absolute branching fraction B(D+ → K¯0μ+νμ) = (8.72 ± 0.07stat. ± 0.18sys.)%, which is consistent with previous measurements within uncertainties but with significantly improved precision. Combining the Particle Data Group values of B(D0 → K-μ+νμ), B(D+ → K¯0e+νe), and the lifetimes of the D0 and D+ mesons with the value of B(D+ → K¯0μ+νμ) measured in this work, we determine the following ratios of partial widths: Γ(D0 → K-μ+νμ)/Γ(D+ → K¯0μ+νμ) = 0.963 ± 0.044 and Γ(D+ → K¯0μ+νμ)/Γ(D+ → K¯0e+νe) = 0.988 ± 0.033.
Improved measurement of the absolute branching fraction of D+→K¯0μ+νμ
By analyzing 2.93 fb - 1 of data collected at s = 3.773 GeV with the BESIII detector, we measure the absolute branching fraction B ( D + → K ¯ 0 μ + ν μ ) = ( 8.72 ± 0 . 07 stat . ± 0 . 18 sys . ) % , which is consistent with previous measurements within uncertainties but with significantly improved precision. Combining the Particle Data Group values of B ( D 0 → K - μ + ν μ ) , B ( D + → K ¯ 0 e + ν e ) , and the lifetimes of the D 0 and D + mesons with the value of B ( D + → K ¯ 0 μ + ν μ ) measured in this work, we determine the following ratios of partial widths: Γ ( D 0 → K - μ + ν μ ) / Γ ( D + → K ¯ 0 μ + ν μ ) = 0.963 ± 0.044 and Γ ( D + → K ¯ 0 μ + ν μ ) / Γ ( D + → K ¯ 0 e + ν e ) = 0.988 ± 0.033 .