NSR Query Results
Output year order : Descending NSR database version of May 2, 2024. Search: Author = M.Mayer Found 14 matches. 2024HE04 Nucl.Instrum.Methods Phys.Res. B547, 165141 (2024) L.Hess, M.Mayer, T.Schwarz-Selinger Cross-section data for the reactions 12C(3He, p0)14N to 12C(3He, p6)14N at energies up to 6 MeV NUCLEAR REACTIONS 12C(3He, p), E=1.5-6 MeV; measured reaction products; deduced σ(θ). The RKS experiment chamber at the 3 MV Tandem Accelerator at IPP Garching, Germany.
doi: 10.1016/j.nimb.2023.165141
2023FO01 Nucl.Instrum.Methods Phys.Res. B542, 158 (2023) V.Foteinou, F.Maragkos, H.-W.Becker, L.Hess, K.Ivankovic, M.Kokkoris, M.Mayer, G.Provatas, D.Rogalla Differential cross-section measurements for the 9Be(3He, 3He0)9Be elastic scattering and the 9Be(3He, px)11B reactions NUCLEAR REACTIONS 9Be(3He, 3He), (3He, p), E=1.6-6 MeV; measured reaction products; deduced σ(θ) for IBANDL project. The Tandem Accelerator Facility of the Ruder Boskovic Institute (RBI) in Zagreb, Croatia.
doi: 10.1016/j.nimb.2023.06.016
2022MO13 Phys.Rev. C 105, 034906 (2022) J.Mohs, M.Ege, H.Elfner, M.Mayer Collective flow at SIS energies within a hadronic transport approach: Influence of light nuclei formation and equation of state
doi: 10.1103/PhysRevC.105.034906
2021GU06 Nucl.Instrum.Methods Phys.Res. B493, 28 (2021) R.d.S.Guimaraes, T.F.Silva, C.L.Rodrigues, M.H.Tabacniks, S.Bach, V.V.Burwitz, P.Hiret, M.Mayer Processing of massive Rutherford Back-scattering Spectrometry data by artificial neural networks
doi: 10.1016/j.nimb.2021.02.010
2019PE02 Nucl.Phys. A982, 399c (2019) H.Petersen, D.Oliinychenko, M.Mayer, J.Staudenmaier, S.Ryu SMASH - A new hadronic transport approach
doi: 10.1016/j.nuclphysa.2018.08.008
2017MA05 Phys.Rev. C 95, 024005 (2017) M.Mayer, for the CLAS Collaboration Beam-target double-spin asymmetry in quasielastic electron scattering off the deuteron with CLAS NUCLEAR REACTIONS 2H(polarized e, e'), E=1.6-1.7, 2.5, 4.2, 5.6-5.8 GeV; measured scattered electron spectra, beam-target double-spin asymmetry for longitudinally polarized electrons scattered quasielastically, and bin averages of the kinematic variables using polarized deuterons and the CEBAF Large Acceptance Spectrometer (CLAS) at JLab facility; deduced that final-state interactions (FSI) have a lesser role for polarization observables in deuteron two-body electro-disintegration than for absolute cross sections. Comparison with a model which includes final-state interactions (FSI), and with a simplified model using the plane wave impulse approximation (PWIA).
doi: 10.1103/PhysRevC.95.024005
2016WI02 Nucl.Instrum.Methods Phys.Res. B371, 41 (2016) B.Wielunska, M.Mayer, T.Schwarz-Selinger, U.von Toussaint, J.Bauer Cross section data for the D(3He, p)4He nuclear reaction from 0.25 to 6 MeV NUCLEAR REACTIONS 2H(3He, p), E=0.25-5.6 MeV; measured reaction products, Ep, Ip; deduced σ(θ). Comparison with he total cross section parameterizations from Bosch and Hale.
doi: 10.1016/j.nimb.2015.09.049
2015KR06 Nucl.Instrum.Methods Phys.Res. B358, 72 (2015) The 9Be(p, p0)9Be, 9Be(p, dO)8Be, and 9Be(p, αO)6Li cross-sections for analytical purposes NUCLEAR REACTIONS 9Be(p, d), (p, p), E=0.4-4.15 MeV; 9Be(p, α), E=1.1-4.1 MeV; measured reaction products, Eα, Iα, Ep, Ip; deduced ground state partial σ, σ(θ). Comparison with available data.
doi: 10.1016/j.nimb.2015.05.004
2012MA26 Nucl.Instrum.Methods Phys.Res. B25, 116 (2012) Statistical analysis of cross-section data for 12C(4He, 4He)12C backscattering NUCLEAR REACTIONS 12C(α, α), E=1.6-8.2 MeV; analyzed available data; deduced average σ deviations. SigmaCalc 1.6 data, IBANDL, CODATA.
doi: 10.1016/j.nimb.2012.05.011
2011GU27 J.Korean Phys.Soc. 59, 2010s (2011) A.F.Gurbich, D.Abriola, N.P.Barradas, A.R.Ramos, I.Bogdanovic Radovic, M.Chiari, C.Jeynes, M.Kokkoris, M.Mayer, L.Shi, I.Vickridge Measurements and Evaluation of Differential Cross-sections for In Beam Analysis COMPILATION 16O(p, p0), E=0.5-4.9 MeV; calculated, analyzed σ(E, θ); deduced effect of single-particle resonance. Analyzed about 30 reactions, results presented only for one of them.
doi: 10.3938/jkps.59.2010
2005AL27 Nucl.Instrum.Methods Phys.Res. B234, 169 (2005) Differential cross-section of the D(3He, p)4He nuclear reaction and depth profiling of deuterium up to large depths NUCLEAR REACTIONS 2H(3He, p), E=0.5-6 MeV; measured Ep, σ(E, θ=135°). Application to depth profiling discussed.
doi: 10.1016/j.nimb.2005.01.009
2003MA23 Nucl.Instrum.Methods Phys.Res. B207, 263 (2003) M.Mayer, B.Diaz-Herrera, M.Schneider Backscattering of 6Li and 7Li Ions from oxygen below 6 MeV NUCLEAR REACTIONS O(6Li, 6Li), E=1585-4992 keV; O(7Li, 7Li), E=2475-5987 keV; measured σ(θ=165°). Comparison with previous results, model predictions.
doi: 10.1016/S0168-583X(03)00464-6
2001MB08 Nucl.Instrum.Methods Phys.Res. B 183, 221 (2001) Scattering cross sections for6Li and 7Li ions from carbon below 5. 5 MeV NUCLEAR REACTIONS 6Li(12C, 12C), 7Li(12C, 12C), E=1.7-5.4 MeV; measured products, 6Li, 7Li; deduced σ(θ). Data were imported from EXFOR entry O0909.
doi: 10.1016/S0168-583X(01)00768-6
1998MA54 Nucl.Instrum.Methods Phys.Res. B143, 244 (1998) M.Mayer, A.Annen, W.Jacob, S.Grigull The 11B(p, α0)8Be Nuclear Reaction and 11B(p, p)11B Backscattering Cross Sections for Analytical Purposes NUCLEAR REACTIONS 11B(p, α), (p, p), E=1700-2700 keV; measured σ(θ=165°). B, C, 27Al, 197Au(p, p'), E=2600 keV; measured σ(Ep, θ=165°). B, C, 27Al, 197Au(α, α'), E=1350 keV; measured σ(Eα, θ=165°).
doi: 10.1016/S0168-583X(98)00383-8
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