NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = M.Schneider Found 40 matches. 2016HU14 Nat.Phys. 12, 800 (2016) O.A.Hurricane, D.A.Callahan, D.T.Casey, E.L.Dewald, T.R.Dittrich, T.Doppner, S.Haan, D.E.Hinkel, L.F.Berzak Hopkins, O.Jones, A.L.Kritcher, S.Le Pape, T.Ma, A.G.MacPhee, J.L.Milovich, J.Moody, A.Pak, H.-S.Park, P.K.Patel, J.E.Ralph, H.F.Robey, J.S.Ross, J.D.Salmonson, B.K.Spears, P.T.Springer, R.Tommasini, F.Albert, L.R.Benedetti, R.Bionta, E.Bond, D.K.Bradley, J.Caggiano, P.M.Celliers, C.Cerjan, J.A.Church, R.Dylla-Spears, D.Edgell, M.J.Edwards, D.Fittinghoff, M.A.Barrios Garcia, A.Hamza, R.Hatarik, H.Herrmann, M.Hohenberger, D.Hoover, J.L.Kline, G.Kyrala, B.Kozioziemski, G.Grim, J.E.Field, J.Frenje, N.Izumi, M.Gatu-Johnson, S.F.Khan, J.Knauer, T.Kohut, O.Landen, F.Merrill, P.Michel, A.Moore, S.R.Nagel, A.Nikroo, T.Parham, R.R.Rygg, D.Sayre, M.Schneider, D.Shaughnessy, D.Strozzi, R.P.J.Town, D.Turnbull, P.Volegov, A.Wan, K.Widmann, C.Wilde, C.Yeamans Inertially confined fusion plasmas dominated by alpha-particle self-heating
doi: 10.1038/nphys3720
2006KO27 Appl.Radiat.Isot. 64, 1031 (2006) K.Kossert, H.Janssen, R.Klein, M.K.H.Schneider, H.Schrader Activity standardization and nuclear decay data of 109Cd RADIOACTIVITY 109Cd(EC); measured conversion electron spectra; deduced photon emission probability. 109Ag transition deduced ICC.
doi: 10.1016/j.apradiso.2006.04.008
2006KO31 Appl.Radiat.Isot. 64, 1420 (2006) K.Kossert, H.Janssen, R.Klein, M.Schneider, H.Schrader Standardization and nuclear decay data of 65Zn RADIOACTIVITY 65Zn(EC), (β+); measured Eγ, Iγ, βγ-coin, T1/2; deduced photon emission probabilities.
doi: 10.1016/j.apradiso.2006.02.054
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
1997HU08 Nucl.Phys. A620, 385 (1997) A.Hunger, J.Peise, A.Robbiano, J.Ahrens, I.Anthony, H.-J.Arends, R.Beck, G.P.Capitani, B.Dolbilkin, H.Falkenberg, G.Galler, S.J.Hall, J.D.Kellie, R.Kondratev, R.Kordsmeier, V.Lisin, A.I.L'vov, G.J.Miller, C.Molinari, P.Ottonello, A.R.Reolon, M.Sanzone, M.Schmitz, M.Schneider, M.Schumacher, O.Selke, Th.Walcher, F.Wissmann, S.Wolf, A.Zucchiatti Compton Scattering by the Proton Through θ(cms) = 75° and 90° in the Δ-Resonance Region NUCLEAR REACTIONS 1H(γ, γ), E=200-500 MeV; measured Compton scattering σ(θ); deduced multipole distribution. Dispersion relations. Δ-resonance.
doi: 10.1016/S0375-9474(97)00184-X
1996HU12 Nucl.Instrum.Methods Phys.Res. A372, 135 (1996) A.Hunger, R.Kordsmeier, M.Schumacher, O.Selke, J.Ahrens, J.Peise, M.Schmitz, M.Schneider, F.Wissmann, B.Dolbilkin, R.Kondratev, V.Lisin, A.Polonsky A High Angular-Resolution and Time-of-Flight Detector System for Recoil Protons from the Reactions p(γ, γ)p and p(γ, π0)p NUCLEAR REACTIONS 1H(γ, γ), (γ, π0), E ≤ 350 MeV; measured proton trajectories, π0 photoproduction scatter plots; deduced Compton scattering, π0 background separation related features. High angular resolution recoil proton tof detector.
doi: 10.1016/0168-9002(95)01280-X
1996PE19 Phys.Lett. 384B, 37 (1996) J.Peise, A.Hunger, J.Ahrens, I.Anthony, H.-J.Arends, R.Beck, G.P.Capitani, B.Dolbilkin, H.Falkenberg, S.J.Hall, P.Jennewein, J.D.Kellie, R.Kondratev, R.Kordsmeier, V.Lisin, A.I.Lvov, G.J.Miller, C.Molinari, A.R.Reolon, A.Robbiano, M.Sanzone, M.Schmitz, M.Schneider, M.Schumacher, O.Selke, Th.Walcher, F.Wissmann Compton Scattering by the Proton Through θ(cms) = 75° in the Δ-Resonance Region NUCLEAR REACTIONS 1H(γ, γ), E=200-410 MeV; measured Compton scattering σ(θ); deduced Δ-photo excitation reduced M1 strength.
doi: 10.1016/0370-2693(96)00709-5
1996SE02 Phys.Lett. 369B, 207 (1996) O.Selke, A.Hunger, A.Kraus, M.Schumacher, R.Wichmann, J.Ahrens, H.J.Arends, R.Beck, J.Peise, M.Schneider, F.Wissmann Compton Scattering from 4He in the Δ(1232) Resonance Region NUCLEAR REACTIONS 4He(γ, γ), E=120-510 MeV; measured Compton scattering σ(θ). Schematic model analysis.
doi: 10.1016/0370-2693(95)01580-9
1996WI10 Z.Phys. A355, 169 (1996) R.Wichmann, J.Ahrens, H.J.Arends, R.Beck, G.Galler, A.Hunger, A.Kraus, I.J.D.MacGregor, J.Peise, B.Seitz, M.Schmitz, M.Schneider, O.Selke, M.Schumacher, F.Wissmann Photoemission of Protons from 4He in the Δ-Resonance Region NUCLEAR REACTIONS 4He(γ, p), E=130-525 MeV; measured proton spectra; deduced three separate reaction channels.
doi: 10.1007/s002180050095
1994LO19 Nucl.Instrum.Methods Phys.Res. A343, 494 (1994) D.Lohmann, J.Peise, J.Ahrens, I.Anthony, H.-J.Arends, R.Beck, R.Crawford, A.Hunger, K.H.Kaiser, J.D.Kellie, Ch.Klumper, P.Krahn, A.Kraus, U.Ludwig, M.Schumacher, O.Selke, M.Schmitz, M.Schneider, F.Wissmann, S.Wolf Linearly Polarized Photons at MAMI (Mainz)
doi: 10.1016/0168-9002(94)90230-5
1994WI13 Phys.Lett. 335B, 119 (1994) F.Wissmann, J.Peise, M.Schmitz, M.Schneider, J.Ahrens, I.Anthony, R.Beck, B.Dolbilkin, S.J.Hall, F.Harter, S.Herdade, J.Herrmann, A.Hunger, P.Jennewein, J.D.Kellie, R.Kondratev, H.-P.Krahn, K.-H.Krause, V.Kusnetzov, V.Lisin, G.J.Miller, A.Polonsky, M.Schumacher, J.Sobolewski, Th.Walcher, A.Zabrodin Elastic and Inelastic Photon Scattering from 12C NUCLEAR REACTIONS 12C(γ, γ), (γ, γ'), E=200-500 MeV; measured σ(θ) vs Eγ. Simple static ansatz, Δ-hole models comparison.
doi: 10.1016/0370-2693(94)91401-X
1992SO01 Phys.Rev. C45, 326 (1992) J.P.Soderstrum, C.R.Gould, D.G.Haase, N.R.Roberson, M.B.Schneider, L.W.Seagondollar Transverse and Longitudinal Polarized-Neutron, Polarized-93Nb Scattering, and the Tensor Spin-Spin Potential NUCLEAR REACTIONS 93Nb(polarized n, n), E=7.5 MeV; measured spin-spin σ; deduced spin-spin potential parameters. Other data included. Cryogenically polarized target.
doi: 10.1103/PhysRevC.45.326
1991SC05 Z.Phys. A338, 217 (1991) M.Schneider, R.Bacher, P.Blum, D.Gotta, K.Heitlinger, W.Kunold, D.Rohmann, J.Egger, L.M.Simons, K.Elsener X-Rays from Antiprotonic 3He and 4He NUCLEAR REACTIONS 3,4He(p-bar, X), E at 309, 202 MeV/c; measured X-ray spectra, yields; deduced strong interaction shifts, widths. ATOMIC PHYSICS 3,4He(p-bar, X), E at 309, 202 MeV/c; measured X-ray spectra, yields; deduced strong interaction shifts, widths.
doi: 10.1007/BF01284797
1989BA46 Z.PHYS. A334, 93 (1989) R.Bacher, P.Blum, D.Gotta, K.Heitlinger, D.Rohmann, M.Schneider, J.Egger, L.M.Simons, K.Elsener Measurement of Balmer and Lyman X-Rays in Antiprotonic Hydrogen Isotopes at Pressures below 300 hPa ATOMIC PHYSICS 2,1H(p-bar, X), E at 202 MeV/c; measured X-ray spectra; deduced strong interaction level parameters.
1988EA01 Can.J.Phys. 66, 534 (1988) E.D.Earle, A.B.McDonald, S.H.Kidner, E.T.H.Clifford, J.J.Hill, G.H.Keech, T.E.Chupp, M.B.Schneider Measurement of Parity Violation in the Photodisintegration of Deuterium and in the Production of Bremsstrahlung on Tantalum NUCLEAR REACTIONS 2H(polarized γ, np), E=4.1 MeV bremsstrahlung; measured CP dependent photodisintegration σ component; deduced parity dependent observables.
doi: 10.1139/p88-089
1988HA40 Hyperfine Interactions 43, 133 (1988) D.G.Haase, C.R.Gould, J.E.Koster, N.R.Roberson, L.W.Seagondollar, J.P.Soderstrum, M.B.Schneider, X.Zhu Studies of Parity and Time Reversal Symmetries in Neutron Scattering from 165Ho NUCLEAR REACTIONS 165Ho(polarized n, X), E=7.1, 11 MeV; measured transmission differences; deduced parity, time violating analyzing powers.
doi: 10.1007/BF02398293
1988SO10 Phys.Rev. C38, 2424 (1988) J.P.Soderstrum, C.R.Gould, D.G.Haase, L.W.Seagondollar, M.B.Schneider, N.R.Roberson Limits on P- and P, T-Violating Absorption of MeV Neutrons in 165Ho NUCLEAR REACTIONS 165Ho(polarized n, X), E=7.1, 11 MeV; measured P-violating analyzing power; deduced limits on P-, P-T violating absorption. Polarized neutron transmission through polarized, unpolarized targets.
doi: 10.1103/PhysRevC.38.2424
1986GO20 Phys.Rev.Lett. 57, 2371 (1986) C.R.Gould, D.G.Haase, L.W.Seagondollar, J.P.Soderstrum, K.E.Nash, M.B.Schneider, N.R.Roberson Spin-Spin Potentials in 27Al(pol) + n(pol) and the Nuclear Ramsauer Effect NUCLEAR REACTIONS 27Al(polarized n, n), E=5-17 MeV; measured spin-spin σ. Tof. Optical model.
doi: 10.1103/PhysRevLett.57.2371
1984HA01 Phys.Rev.Lett. 52, 337 (1984); Erratum Phys.Rev.Lett 52, 1054 (1984) A.L.Hallin, F.P.Calaprice, D.W.MacArthur, L.E.Piilonen, M.B.Schneider, D.F.Schreiber Test of Time-Reversal Symmetry in the β Decay of 19Ne RADIOACTIVITY 19Ne(β+), (EC); measured β+(recoil ion)-coin; deduced asymmetry parameter, time reversal symmetry validity. Atomic beam polarized source.
doi: 10.1103/PhysRevLett.52.337
1983KU11 Z.Phys. A313, 11 (1983) W.Kunold, M.Schneider, L.M.Simons, J.Wuest, R.Abela Isotope Shift Measurements of Muonic X-Rays in 134,136,138 Barium NUCLEAR MOMENTS 134,136,138Ba; measured muonic X-ray isotope shifts; deduced optical isotope shift calibration. 134,136Ba deduced rms radii. ATOMIC PHYSICS, Mesic-Atoms 134,136,138Ba; measured muonic X-ray isotope shifts.
doi: 10.1007/BF02115838
1983SC32 Phys.Rev.Lett. 51, 1239 (1983); Erratrum Phys.Rev.Lett. 52, 695 (1984) M.B.Schneider, F.P.Calaprice, A.L.Hallin, D.W.MacArthur, D.F.Schreiber Limit on Im(C(S)C(A)*) from a Test of T Invariance in 19Ne Beta Decay RADIOACTIVITY 19Ne(β+), (EC) [from 19F(p, n), E=12 MeV]; measured β polarization, asymmetry, time reversal odd angular correlation magnitude R; deduced time reversal invariance, scalar, axial vector coupling imaginary interference limit. Polarized source.
doi: 10.1103/PhysRevLett.51.1239
1982EF01 Z.Phys. A309, 77 (1982) B.Effenberger, W.Kunold, W.Oesterle, M.Schneider, L.M.Simons, R.Abela, J.Wuest Determination of the Spectroscopic Quadrupole Moments of 7533As and 6329Cu NUCLEAR MOMENTS 75As, 63Cu; measured muonic X-rays, hfs splitting; deduced nuclear charge distribution parameters. 75As, 63Cu deduced spectroscopic quadrupole moments. ATOMIC PHYSICS, Mesic-Atoms 75As, 63Cu; measured muonic X-rays, hfs splitting; deduced nuclear charge distributions, Barrett moments. Model independent analysis.
doi: 10.1007/BF01420154
1982MA39 Phys.Rev. C26, 1753 (1982) D.W.MacArthur, F.P.Calaprice, A.L.Hallin, M.B.Schneider, D.F.Schreiber Nuclear Magnetic Moment of 19Ne with Possible Applications to Other Radioactive Gas Isotopes RADIOACTIVITY 19Ne [from 19F(p, n), E=12 MeV]; measured NMR; deduced μ. Polarized source.
doi: 10.1103/PhysRevC.26.1753
1980AB14 Helv.Phys.Acta 53, 300 (1980) R.Abela, W.Kunold, M.Schneider, L.M.Simons, P.Zsoldos Suche Nach Einer E0-Anregung im 68Zn und Bestimmung des Quadrupolmomentes im 97Mo Mittels Messung von 2s-2p Ubergangen in μ-Atomen NUCLEAR MOMENTS 97Mo; measured muonic atom transitions; deduced quadrupole moment. ATOMIC PHYSICS, Mesic-Atoms 68Zn; measured muonic atom transitions. 68Zn deduced E0 transition probability.
1980BA24 Phys.Lett. B94, 331 (1980) R.Abela, W.Kunold, L.M.Simons, M.Schneider Search for a Dynamical E0 Excitation in the Muonic 68Zn Atom ATOMIC PHYSICS, Mesic-Atoms 68Zn; measured muonic X-rays; deduced no dynamical E0 excitation.
doi: 10.1016/0370-2693(80)90890-4
1978BU07 Nucl.Phys. A299, 117 (1978) J.D.Burch, M.J.Schneider, J.J.Kraushaar Two-Step Processes and Finite-Range Effects in the 60,62Ni(p, t) Reaction NUCLEAR REACTIONS 60,62Ni(p, t), E=26.8 MeV; measured absolute σ(Et, θ). DWBA, coupled-channels, exact finite-range analysis. Enriched 60,62Ni targets.
doi: 10.1016/0375-9474(78)90212-9
1978ZI01 Nucl.Phys. A297, 263 (1978) W.R.Zimmerman, J.J.Kraushaar, M.J.Schneider, H.Rudolph A Study of the (3He, t) Reaction on 60Ni NUCLEAR REACTIONS 60Ni(3He, t), (3He, α), E=38 MeV; measured σ(θ). 60Cu, 59Ni deduced levels, J, π, S. Enriched targets, coupled-reaction-channels calculations.
doi: 10.1016/0375-9474(78)90276-2
1977ZI02 Phys.Rev. C16, 2432 (1977) W.R.Zimmerman, J.J.Kraushaar, M.J.Schneider, H.Rudolph 56Fe(3He, t)56Co Reaction NUCLEAR REACTIONS 56Fe(3He, t), E=38.2 MeV; measured σ(Et, θ). 56Co deduced levels, J, π, L. DWBA analysis.
doi: 10.1103/PhysRevC.16.2432
1976SC06 Phys.Rev. C13, 1392 (1976) 24Mg(d, α) Reaction as a Test of 22Na Wave Functions NUCLEAR REACTIONS 24Mg(d, α), E=17-26 MeV; measured σ(E, Eα, θ). 22Na deduced wave functions. Shell model. Enriched targets.
doi: 10.1103/PhysRevC.13.1392
1976SC21 Phys.Lett. 63B, 129 (1976) M.J.Schneider, J.D.Burch, P.D.Kunz Competition of Two-Step Processes in the Reactions 60,62Ni(p, t) Leading to Unnatural Parity States NUCLEAR REACTIONS 60,62Ni(p, t), E=26.8 MeV; measured σ(Et, θ); deduced reaction mechanism. DWBA analysis.
doi: 10.1016/0370-2693(76)90631-6
1975RI05 Phys.Lett. 60B, 19 (1975) L.D.Rickertsen, M.J.Schneider, J.J.Kraushaar, W.R.Zimmerman, H.Rudolph Two-Step Processes in the (3He, t) Reaction to Analog and Anti-Analog States in 56Co NUCLEAR REACTIONS 56Fe(3He, t), E=38.2 MeV; measured σ(Et, θ). 56Fe(3He, α), E=38.2 MeV; measured σ(Eα, θ). 55Fe levels deduced S.
doi: 10.1016/0370-2693(75)90516-X
1975SC19 Nucl.Phys. A246, 156 (1975) M.J.Schneider, R.E.Anderson, P.G.Brabeck Proton Spectroscopy of 86,88Sr via (3He, d) NUCLEAR REACTIONS 85,87Rb(3He, d), E=33 MeV; measured σ(θ). 86,88Sr deduced levels, L, S, J, π. Natural, enriched targets, magnetic spectrometer.
doi: 10.1016/0375-9474(75)90569-2
1975SC27 Phys.Rev. C12, 335 (1975) M.J.Schneider, B.W.Ridley, M.E.Rickey, J.J.Kraushaar, W.R.Zimmerman Study of Unbound Levels in 10C via 10B(3He, t) NUCLEAR REACTIONS 10B(3He, t), E=38.2 MeV; measured σ(Et, θ). 10C deduced levels, Γ.
doi: 10.1103/PhysRevC.12.335
1974BI04 Phys.Rev. C9, 2154 (1974) P.K.Bindal, K.Nagatani, M.J.Schneider, P.D.Bond Elastic and Inelastic Scattering of 6Li on 12C NUCLEAR REACTIONS 12C(6Li, 6Li), (6Li, 6Li'), E=36.4, 40.0 MeV; measured σ(θ), deduced energy-dependent optical-model parameters for E=20-63 MeV; DWBA analysis. 12C level deduced deformation parameters β(L).
doi: 10.1103/PhysRevC.9.2154
1973AU02 Phys.Rev.Lett. 30, 1078 (1973) E.H.Auerbach, A.J.Baltz, P.D.Bond, C.Chasman, J.D.Garrett, K.W.Jones, S.Kahana, M.J.LeVine, M.Schneider, A.Z.Schwarzschild, C.E.Thorn Anomalous and Normal Angular Distributions in Ni(18O, 16O) Reactions NUCLEAR REACTIONS 58,60,62,64Ni(18O, 16O), E=50, 57, 65 MeV; measured σ(E, E(16O), θ); deduced optical model parameters.
doi: 10.1103/PhysRevLett.30.1078
1973CH31 Phys.Rev.Lett. 31, 1074 (1973) C.Chasman, S.Kahana, M.J.Schneider Observation and Interpretation of Angular Oscillations in 48Ca(14N, 13C)49Sc NUCLEAR REACTIONS 48Ca(14N, 13C), E=50 MeV; measured σ(θ).
doi: 10.1103/PhysRevLett.31.1074
1973SC16 Phys.Rev.Letters 31, 320 (1973) M.J.Schneider, C.Chasman, E.H.Auerbach, A.J.Baltz, S.Kahana Possible L-Dependent Angular Distributions in the Reaction 48Ca(14N, 13C)49Sc NUCLEAR REACTIONS 48Ca(14N, 13C), E=50 MeV; measured σ(E(13C), θ). 49Sc levels deduced L, S. 48Ca(14N, 14N), (13C, 13C) measured σ(θ), deduced optical model parameters.
doi: 10.1103/PhysRevLett.31.320
1972SC13 Phys.Rev. C5, 1330 (1972) High-Resolution Study of Co58 by (d, α) and (He3, d) Reactions NUCLEAR REACTIONS 60Ni(d, α), E=17 MeV; 57Fe(3He, d), E=18 MeV; 59Co(3He, α), E=18 MeV; measured σ(Eα, θ), σ(Ed, θ), σ(Eα, θ). 58Co deduced levels, J, π, S.
doi: 10.1103/PhysRevC.5.1330
1971SC18 Phys.Rev. C4, 1649 (1971) High-Resolution Study of Co56 by (d, α) and (He3, p) Reactions NUCLEAR REACTIONS 58Ni(d, α), E=17 MeV;54Fe(3He, p), E=18 MeV; measured σ(θ). 56Co deduced levels, J, π, L.
doi: 10.1103/PhysRevC.4.1649
Back to query form Note: The following list of authors and aliases matches the search parameter M.Schneider: , M.B.SCHNEIDER, M.H.SCHNEIDER, M.J.SCHNEIDER, M.K.SCHNEIDER |