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Search: Author = D.Huber

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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
Citations: PlumX Metrics

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)

H.Kamada, D.Huber, A.Nogga

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
Citations: PlumX Metrics

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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0481.

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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13889.

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
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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
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1998HU16      Phys.Rev. C58, 674 (1998)

D.Huber, J.L.Friar

Ay Puzzle and the Nuclear Force

doi: 10.1103/PhysRevC.58.674
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0648.

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
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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
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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
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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
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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
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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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
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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
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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
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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
Citations: PlumX Metrics

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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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)

H.Witala, D.Huber, W.Glockle

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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