NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = D.Huber Found 41 matches. 2017GO06 Nucl.Phys. A961, 1 (2017) M.Gotz, S.Gotz, J.V.Kratz, Ch.E.Dullmann, Ch.Mokry, J.Runke, P.Thorle-Pospiech, N.Wiehl, M.Schadel, J.Ballof, H.Dorrer, J.Grund, D.Huber, E.Jager, O.Keller, J.Krier, J.Khuyagbaatar, L.Lens, B.Lommel, M.Mendel, K.J.Moody, P.Scharrer, B.Schausten, D.Shaughnessy, M.Schmitt, J.Steiner, N.Trautmann, A.Yakushev, V.Yakusheva Radiochemical study of the kinematics of multi-nucleon transfer reactions in 48Ca + 248Cm collisions 10 percent above the Coulomb barrier NUCLEAR REACTIONS 248Cm(48Ca, x), E=262 MeV; measured multinucleon transfer reaction products, Eα, Iα (for identification of the fragments); deduced TKE vs θ, E* vs θ for target-like (trans-target ones, like Fm, Es, Cf, Bk and others) fragments using radiochemical methods.
doi: 10.1016/j.nuclphysa.2017.02.006
2001HU13 Few-Body Systems 30, 95 (2001) D.Huber, J.L.Friar, A.Nogga, H.Witala, U.van Kolck Novel Three-Nucleon-Force Terms in the Three-Nucleon System NUCLEAR REACTIONS 2H(polarized n, n), E=3, 10, 50 MeV; calculated Ay(θ). Three-nucleon force, comparisons with data.
2001KA34 Few-Body Systems 30, 121 (2001) The c-Term of the Tucson-Melbourne Three-Body Force: To be or not to be NUCLEAR STRUCTURE 3H; calculated binding energy; deduced three-nucleon force effects. NUCLEAR REACTIONS 1H(d, d), E=270 MeV; calculated analyzing power; deduced three-nucleon force effects.
doi: 10.1007/s006010170021
2000BI02 Phys.Rev.Lett. 84, 606 (2000) R.Bieber, W.Glockle, J.Golak, M.N.Harakeh, D.Huber, H.Huisman, N.Kalantar-Nayestanaki, H.Kamada, J.G.Messchendorp, A.Nogga, H.Sakai, N.Sakamoto, M.Seip, M.Volkerts, S.Y.van der Werf, H.Witala Three-Nucleon Force and the Ay Puzzle in Inermediate Energy p(pol) + d and d(pol) + p Elastic Scattering NUCLEAR REACTIONS 2H(polarized p, p), E=150, 190 MeV; measured Ay(θ); 1H(polarized d, d), E=270 MeV; analyzed tensor analyzing powers; deduced role of three-nucleon force.
doi: 10.1103/PhysRevLett.84.606
2000FR04 Acta Phys.Pol. B31, 749 (2000) J.L.Friar, D.Huber, H.Witala, G.L.Payne Quartet n-d Scattering Lengths NUCLEAR REACTIONS 2H(n, X), E not given; calculated quartet scattering lengths. Several potentials compared.
1999FR02 Phys.Rev. C59, 53 (1999) J.L.Friar, D.Huber, U.van Kolck Chiral Symmetry and Three-Nucleon Forces
doi: 10.1103/PhysRevC.59.53
1999WI02 Phys.Lett. 447B, 216 (1999) H.Witala, W.Glockle, J.Golak, D.Huber, H.Kamada, A.Nogga Scaling Properties of the Longitudinal and Transversal Asymmetries of the n(pol)d(pol) Total Cross Section NUCLEAR REACTIONS 2H(polarized n, X), E=0.6-65 MeV calculated total σ transversal, longitudinal asymmetries; deduced role of three-nucleon force. Polarized target. Several interactions compared.
doi: 10.1016/S0370-2693(99)00002-7
1999WI05 Phys.Rev. C59, 3035 (1999) H.Witala, H.Kamada, A.Nogga, W.Glockle, Ch.Elster, D.Huber Modern NN Force Predictions for the Total nd Cross Section up to 300 MeV NUCLEAR REACTIONS 2H(n, X), E=10-300 MeV; calculated total σ; deduced rescattering, relativistic, three-nucleon force effects. Fadeev calculations, several potentials compared. Comparison with data.
doi: 10.1103/PhysRevC.59.3035
1998AB21 Phys.Rev.Lett. 81, 57 (1998) W.P.Abfalterer, F.B.Bateman, F.S.Dietrich, Ch.Elster, R.W.Finlay, W.Glockle, J.Golak, R.C.Haight, D.Huber, G.L.Morgan, H.W.Witala Inadequacies of the Nonrelativistic 3N Hamiltonian in Describing the n + d Total Cross Section NUCLEAR REACTIONS 1,2H(n, X), E=7-600 MeV; measured σ; deduced possible relativistic effects. Fadeev calculations.
doi: 10.1103/PhysRevLett.81.57
1998HE04 Phys.Rev. C57, 484 (1998) P.Hempen, P.Clotten, K.Hofenbitzer, T.Koble, W.Metschulat, M.Schwindt, W.von Witsch, L.Watzold, J.Weltz, W.Glockle, D.Huber, H.Witala Measurement and Calculation of the Polarization Transfer Parameter K(y)(y') in Neutron-Deuteron Scattering at 15.0, 17.0, 19.0, and 25.8 MeV NUCLEAR REACTIONS 2H(polarized n, n), E=15.0, 17.0, 19.0, 25.8 MeV; measured asymmetries; deduced polarization transfer parameter. Fadeev calculations, four NN potentials compared.
doi: 10.1103/PhysRevC.57.484
1998HU06 Nucl.Phys. A631, 663c (1998) D.Huber, H.Witala, H.Kamada, A.Nogga, W.Glockle Recent Progress in the 3N System Including Three-Nucleon Forces
doi: 10.1016/S0375-9474(98)00087-6
1998HU16 Phys.Rev. C58, 674 (1998) Ay Puzzle and the Nuclear Force
doi: 10.1103/PhysRevC.58.674
1998IS01 Phys.Rev. C57, 39 (1998) S.Ishikawa, J.Golak, H.Witala, H.Kamada, W.Glockle, D.Huber Inclusive Scattering of Polarized Electrons on Polarized 3He: Effects of final state interaction and the magnetic form factor of the neutron NUCLEAR REACTIONS 3He(polarized e, e'X), E not given; analyzed assymetries; deduced final state interaction role, neutron form factor effects. Polarized target.
doi: 10.1103/PhysRevC.57.39
1998KI18 Phys.Rev. C58, 3085 (1998) A.Kievsky, M.Viviani, S.Rosati, D.Huber, W.Glockle, H.Kamada, H.Witala, J.Golak Benchmark Calculations for Polarization Observables in Three-Nucleon Scattering NUCLEAR REACTIONS 2H(polarized n, n), E=3 MeV; calculated σ(θ), Ay(θ), tensor analyzing powers, spin-transfer coefficients. Variational, Fadeev equation methods compared.
doi: 10.1103/PhysRevC.58.3085
1998RO12 Phys.Rev. C57, 2111 (1998) H.Rohdjess, W.Scobel, H.O.Meyer, P.V.Pancella, S.F.Pate, M.A.Pickar, R.E.Pollock, B.von Przewoski, T.Rinckel, F.Sperisen, H.Witala, J.Golak, D.Huber, H.Kamada, W.Glockle Elastic pd Scattering with 200-300 MeV Protons NUCLEAR REACTIONS 2H(p, p), E=200-300 MeV; measured σ(θ); deduced 3N force role. Nonrelativistic Fadeev calculations.
doi: 10.1103/PhysRevC.57.2111
1998SY01 Few-Body Systems 25, 133 (1998) L.Sydow, S.Vohl, S.Lemaitre, H.Patberg, R.Reckenfelderbaumer, H.Paetz gen.Schieck, W.Glockle, D.Huber, H.Witala Polarization-Transfer Coefficients in D(p(pol), p(pol))d and D(p(pol), d(pol))p Reactions at Ep = 19 MeV: Experiment compared to calculations with recent nuclear-interaction models NUCLEAR REACTIONS 2H(polarized p, d), (polarized p, p), E=19.0 MeV; measured analyzing powers, polarization-transfer coefficients. Comparison with three-nucleon Fadeev equation calculations.
doi: 10.1007/s006010050099
1998VO03 Phys.Rev. C57, 2104 (1998) W.von Witsch, P.Hempen, K.Hofenbitzer, V.Huhn, W.Metschulat, M.Schwindt, L.Watzold, Ch.Weber, D.Huber, H.Witala Transverse Polarization Transfer in the 2H(d(pol), n(pol))3He Reaction at θ = 0° NUCLEAR REACTIONS 2H(polarized d, n), E ≈ 13 MeV; measured neutron polarization; deduced polarization transfer coefficient. Vector-polarized beam.
doi: 10.1103/PhysRevC.57.2104
1998WE03 Phys.Rev. C57, 1378 (1998) S.P.Weppner, Ch.Elster, D.Huber Off-Shell Structures of Nucleon-Nucleon t Matrices and Their Influence on Nucleon-Nucleus Elastic Scattering Observables NUCLEAR REACTIONS 16O(polarized p, p), E=135, 200 MeV; 40Ca(polarized p, p), E=160, 200 MeV; 208Pb(polarized p, p), E=200 MeV; analyzed σ(θ), A(y)(θ), spin rotation function; deduced sensitivity to off-shell structures.
doi: 10.1103/PhysRevC.57.1378
1998WI22 Phys.Rev.Lett. 81, 1183 (1998) H.Witala, W.Glockle, D.Huber, J.Golak, H.Kamada Cross Section Minima in Elastic Nd Scattering: Possible evidence for three-nucleon force effects NUCLEAR REACTIONS 2H(n, n), E=12, 65, 140, 200 MeV; calculated σ(θ); deduced three-nucleon force effects. Comparison with (p, p), (n, n) data.
doi: 10.1103/PhysRevLett.81.1183
1997HU10 Acta Phys.Pol. B28, 1677 (1997) D.Huber, H.Kamada, H.Witala, W.Glockle How to Include a Three-Nucleon Force into Faddeev Equations for the 3N Continuum: A new form NUCLEAR REACTIONS 2H(polarized n, n), E=10.3 MeV; calculated spin transfer, correlation coefficients; 2H(polarized n, np), E=10.3 MeV; calculated σ(θ1, θ2) vs arc length, A(y). Three-nucleon force.
1997HU17 Few-Body Systems 22, 107 (1997) D.Huber, H.Witala, A.Nogga, W.Glockle, H.Kamada A New Look Into the Partial-Wave Decomposition of Three-Nucleon Forces
1997KU16 Phys.Rev. C56, 654 (1997) J.Kuros, H.Witala, W.Glockle, J.Golak, D.Huber, H.Kamada Optical Nucleon-Deuteron Potential NUCLEAR REACTIONS 2H(n, n), (polarized n, n), E=10-300 MeV; calculated σ(θ), analyzing power, polarization transfer, spin correlation vs θ, other observables. Optical potential, polarized target. Integral equation approach.
doi: 10.1103/PhysRevC.56.654
1997NO10 Phys.Lett. 409B, 19 (1997) A.Nogga, D.Huber, H.Kamada, W.Glockle Triton Binding Energies for Modern NN Forces and the π-π Exchange Three-Nucleon Force NUCLEAR STRUCTURE 3H; calculated binding energy, two-body correlation functions; deduced π-π exchange three-nucleon force role. Several potentials compared.
doi: 10.1016/S0370-2693(97)00841-1
1997ZE01 Phys.Rev. C55, 42 (1997) J.Zejma, M.Allet, K.Bodek, J.Lang, R.Muller, S.Navert, O.Naviliat-Cuncic, J.Sromicki, E.Stephan, L.Jarczyk, St.Kistryn, J.Smyrski, A.Strzalkowski, W.Glockle, J.Golak, D.Huber, H.Witala, P.A.Schmelzbach Cross Sections and Analyzing Powers A(y) in the Breakup Reaction 2H(p(pol), pp)n at 65 MeV: Star configurations NUCLEAR REACTIONS 2H(polarized p, 2p), E=65 MeV; measured σ(θ1, θ2) vs arc length, analyzing power for three star configurations; deduced effects of 3-body force.
doi: 10.1103/PhysRevC.55.42
1996AL10 Phys.Lett. 376B, 255 (1996) M.Allet, K.Bodek, J.Golak, W.Glockle, W.Hajdas, D.Huber, L.Jarczyk, H.Kamada, St.Kistryn, J.Lang, R.Muller, O.Naviliat-Cuncic, J.Smyrski, J.Sromicki, A.Strzalkowski, H.Witala, J.Zejma Effects of the Tucson-Melbourne Three-Nucleon Force in the Proton-Deuteron Breakup Process at E(p) = 65 MeV NUCLEAR REACTIONS 2H(polarized p, np), E=65 MeV; analyzed σ(θ1, θ2) vs arc length, analyzing power vs (θ1, θ2). Quasi-free breakup, Tucson-Melbourne three-nucleon force.
doi: 10.1016/0370-2693(96)00259-6
1996AL34 Few-Body Systems 20, 27 (1996) M.Allet, K.Bodek, W.Hajdas, J.Lang, R.Muller, S.Navert, O.Naviliat-Cuncic, J.Sromicki, J.Zejma, L.Jarczyk, St.Kistryn, J.Smyrski, A.Strzalkowski, H.Witala, W.Glockle, J.Golak, D.Huber, H.Kamada Proton-Induced Deuteron Breakup at E(p)(lab) = 65 MeV in Quasi-Free Scattering Configurations NUCLEAR REACTIONS 2H(polarized p, 2p), E=65 MeV; measured σ(θ1, θ2), analyzing power vs arc length. Kinematically complete configurations, quasi-free scattering geometry. Faddeev calculations comparison, realistic interactions.
doi: 10.1007/s006010050029
1996GE05 Phys.Rev. C54, 1523 (1996) E.A.George, J.Frandy, M.K.Smith, Y.Zhou, L.D.Knutson, J.Golak, H.Witala, W.Glockle, D.Huber Measurement of the Longitudinal Analyzing Power for Noncoplanar p-d Breakup NUCLEAR REACTIONS 2H(polarized p, X), E=9 MeV; measured noncoplanar breakup associated longitudinal analyzing power. Faddeev calculations comparison.
doi: 10.1103/PhysRevC.54.1523
1996GL05 Phys.Rep. 274, 107 (1996) W.Glockle, H.Witala, D.Huber, H.Kamada, J.Golak The Three-Nucleon Continuum: Achievements, challenges and applications
doi: 10.1016/0370-1573(95)00085-2
1996GR10 Nucl.Phys. A603, 161 (1996) R.Grossmann, G.Nitzsche, H.Patberg, L.Sydow, S.Vohl, H.Paetz gen.Schieck, J.Golak, H.Witala, W.Glockle, D.Huber Low Energy Proton-Deuteron Versus Neutron-Deuteron Breakup in Four Configurations: Implications for Coulomb-Force Effects NUCLEAR REACTIONS 2H(p, 2p), E=10.5 MeV; measured σ(E1, E2, θ1, θ2); deduced Coulomb effects. Faddeev calculations, nucleon-nucleon potentials, three-nucleon force, comparison with other data.
doi: 10.1016/0375-9474(96)00108-X
1996PA09 Phys.Rev. C53, 1497 (1996) H.Patberg, R.Grossmann, G.Nitzsche, L.Sydow, S.Vohl, H.Paetz gen.Schieck, J.Golak, H.Witala, W.Glockle, D.Huber Deuteron Breakup Reaction 2H(p(pol), pp)n Induced by Polarized Protons at E(p) = 19.0 MeV NUCLEAR REACTIONS 2H(polarized p, 2p), E=19 MeV; measured σ(θ3, θ4, φ3, φ4), vector analyzing power vs arc length. Comparison with Faddeev calculations using different realistic NN-potentials.
doi: 10.1103/PhysRevC.53.1497
1996WI22 Few-Body Systems 20, 81 (1996) H.Witala, D.Huber, W.Glockle, W.Tornow, D.E.Gonzalez Trotter Extraction of the Neutron-Neutron Scattering Length a(nn) from Kinematically Complete Neutron-Deuteron Breakup Experiments NUCLEAR REACTIONS 2H(n, 2n), E=13 MeV; analyzed σ(θ1, θ2) vs arc length; deduced nn-scattering length, associated uncertainities. Faddeev equations, realistic nucleon-nucleon interactions.
doi: 10.1007/s006010050033
1995FR11 Phys.Rev. C51, 2356 (1995) J.L.Friar, G.L.Payne, W.Glockle, D.Huber, H.Witala Benchmark Solutions for n-d Breakup Amplitudes NUCLEAR REACTIONS 2H(n, X), E=14.1, 42 MeV; calculated breakup σ(θ1, θ2) vs arc length. 2H(n, n), E=14.1, 42 MeV; calculated phase shifts. S-wave potential model.
doi: 10.1103/PhysRevC.51.2356
1995GO23 Phys.Rev. C52, 1216 (1995) J.Golak, H.Witala, H.Kamada, D.Huber, S.Ishikawa, W.Glockle Inclusive Electron Scattering on 3H and 3He with Full Inclusion of Final State Interactions NUCLEAR REACTIONS 3He, 3H(e, e'X), E not given; calculated longitudinal, transverse response functions. Final state interactions.
doi: 10.1103/PhysRevC.52.1216
1995HU03 Phys.Rev. C51, 1100 (1995) D.Huber, W.Glockle, J.Golak, H.Witala, H.Kamada, A.Kievsky, S.Rosati, M.Viviani Realistic Phase Shift and Mixing Parameters for Elastic Neutron-Deuteron Scattering: Comparison of momentum space and configuration space methods NUCLEAR REACTIONS 2H(n, n), E=1-3 MeV; calculated eigenphase shift, mixing parameters. Momentum, configuration space methods comparison, AV14 NN potential.
doi: 10.1103/PhysRevC.51.1100
1995HU18 Few-Body Systems 19, 175 (1995) D.Huber, J.Golak, H.Witala, W.Glockle, H.Kamada Phase Shifts and Mixing Parameters for Elastic Neutron-Deuteron Scattering Above Breakup Threshold NUCLEAR REACTIONS 2H(n, n), E ≤ 20 MeV; calculated phase shifts, mixing parameters. Faddeev approach.
1995QI02 Nucl.Phys. A587, 252 (1995) L.M.Qin, W.Boeglin, D.Fritschi, J.Gotz, J.Jourdan, G.Masson, S.Robinson, I.Sick, P.Trueb, M.Tuccillo, B.Zihlmann, H.Witala, J.Golak, W.Glockle, D.Huber Tensor and Vector Analyzing Power of the 1H(d(pol), pp)n Reaction NUCLEAR REACTIONS 1H(polarized d, 2p), E=52.1 MeV; measured tensor, vector analyzing power. Symmetric collinear, coplanar kinematic configurations. Three-nucleon continuum calculations, realistic nucleon-nucleon potentials.
doi: 10.1016/0375-9474(95)00010-X
1995WI08 Phys.Rev. C51, 1095 (1995) H.Witala, J.Golak, W.Tornow, W.Glockle, D.Huber Effects of the Tucson-Melbourne Three-Nucleon Force on Proton Spectra from Kinematically Incomplete Neutron-Deuteron Breakup Experiments NUCLEAR REACTIONS 2H(n, p), E=11-62.8 MeV; analyzed σ(θ, Ep) following breakup; deduced Tucson-Melbourne three-nucleon force related features. Kinematically incomplete reaction.
doi: 10.1103/PhysRevC.51.1095
1995WI21 Phys.Rev. C52, 1254 (1995) H.Witala, D.Huber, W.Glockle, J.Golak, A.Stadler, J.Adam, Jr. Effects of the Three-Nucleon Forces Due to π and ρ Meson Exchanges in the Three-Nucleon Continuum NUCLEAR REACTIONS 2H(polarized n, n), E=3, 14.1 MeV; calculated σ(θ), polarization transfer coefficient, analyzing power, tensor, vector analyzing power vs θ. Three-nucleon continuum, π--, ρ-meson exchange.
doi: 10.1103/PhysRevC.52.1254
1995WI27 Phys.Rev. C52, 2906 (1995) H.Witala, J.Golak, W.Glockle, D.Huber, H.Kamada, W.Tornow, E.J.Stephenson, D.A.Low Tensor Analyzing Power A(yy) for dp Breakup in the Symmetric Constant Relative Energy Configuration NUCLEAR REACTIONS 1H(polarized d, 2p), E=94.5-99.2 MeV; analyzed analyzing power data. Breakup, Faddeev approach, different realistic interactions.
doi: 10.1103/PhysRevC.52.2906
1994HU20 Few-Body Systems 16, 165 (1994) D.Huber, H.Kamada, H.Witala, W.Glockle Algorithm for Solving the Faddeev Equations in the Three-Body Continuum Under Avoidance of Moving Logarithmic Singularities NUCLEAR REACTIONS 2H(n, X), E=13 MeV; calculated breakup σ(θ1, θ2) vs arc length, kinematically complete configurations. Three-body continuum, Faddeev equations.
1994WI01 Phys.Rev. C49, R14 (1994) Analyzing Power Puzzle in Low Energy Elastic Nd Scattering NUCLEAR REACTIONS 2H(polarized n, n), E=3 MeV; analyzed analyzing power data. Three-nucleon Faddeev calculations.
doi: 10.1103/PhysRevC.49.R14
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