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NSR database version of May 2, 2024.

Search: Author = H.Zankel

Found 21 matches.

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1990BE09      Phys.Rev. C41, 1365 (1990)

G.H.Berthold, A.Stadler, H.Zankel

Faddeev Calculations for Low-Energy p-d Scattering

NUCLEAR REACTIONS 2H(polarized p, p), E=2.5-3 MeV; calculated σ(θ), polarization observables; deduced p-d phase shifts, Coulomb corrections.

doi: 10.1103/PhysRevC.41.1365
Citations: PlumX Metrics


1988BE20      Phys.Rev. C38, 444 (1988)

G.H.Berthold, A.Stadler, H.Zankel

Momentum Space Faddeev Calculation of 3He Binding Energy with N-N P and D Waves

NUCLEAR STRUCTURE 3He, 3H; calculated binding energy. Coulomb modified Faddeev equations.

doi: 10.1103/PhysRevC.38.444
Citations: PlumX Metrics


1988BE31      Phys.Rev.Lett. 61, 1077 (1988)

G.H.Berthold, A.Stadler, H.Zankel

Exact Three-Body Calculation of p-d Polarization Observables

NUCLEAR REACTIONS 1H(polarized p, p), (polarized n, n), E=2.5 MeV; calculated σ(θ), nucleon analyzing power vs θ, deuteron tensor analyzing powers. Modified Faddeev-type equations.

doi: 10.1103/PhysRevLett.61.1077
Citations: PlumX Metrics


1986BE25      Nuovo Cim. 93A, 89 (1986)

G.H.Berthold, H.Zankel, L.Mathelitsch, H.Garcilazo

Momentum Space Calculation of 3He Bound-State Energies

NUCLEAR STRUCTURE 3He, 3H; calculated binding energies. 2H; calculated binding energy, quadrupole moment, D-state propability. Momentum space Faddeev equations.

doi: 10.1007/BF02773444
Citations: PlumX Metrics


1986BE29      Phys.Rev. C34, 1203 (1986)

G.H.Berthold, H.Zankel

Momentum Space Faddeev Calculation for N - d Scattering below the Breakup Threshold

NUCLEAR REACTIONS 2H(p, p), E=0.2-2 MeV; calculated σ(θ). Momentum space Coulomb modified Faddeev equations.

doi: 10.1103/PhysRevC.34.1203
Citations: PlumX Metrics


1985BE47      Phys.Lett. 162B, 208 (1985)

G.H.Berthold, H.Zankel

Influence of Coulomb Polarization on pd Low Energy Parameters

NUCLEAR REACTIONS 2H(p, p), E=0.2, 2 MeV; calculated phase shifts, scattering lengths; deduced low energy parameters, Coulomb polarization role.

doi: 10.1016/0370-2693(85)90907-4
Citations: PlumX Metrics


1985GA10      Phys.Rev. C32, 264 (1985)

H.Garcilazo, L.Mathelitsch, H.Zankel

Relativistic Effects in the Neutron-Deuteron Scattering Lengths

NUCLEAR REACTIONS 2H(n, n), E=low; calculated doublet, quartet scattering lengths; deduced relativistic corrections size. Relativistic, nonrelativistic Faddeev equations, local, nonlocal potentials.

doi: 10.1103/PhysRevC.32.264
Citations: PlumX Metrics


1985KO31      Phys.Rev. C32, 1796 (1985)

Y.Koike, W.Plessas, H.Zankel

Nucleon-Deuteron Scattering Based on Meson-Exchange Nucleon-Nucleon Dynamics

NUCLEAR REACTIONS 2H(n, n), E=8, 10, 10.25, 12 MeV; calculated σ(θ). 2H(polarized n, n), E=10 MeV; calculated polarization spin-transfer coefficient. Comparison to 2H(d, d) data, meson exchange effects.

doi: 10.1103/PhysRevC.32.1796
Citations: PlumX Metrics


1984KR23      Phys.Rev. C30, 1810 (1984)

H.Krupp, J.C.Hiebert, H.O.Klages, P.Doll, J.Hansmeyer, P.Plischke, J.Wilczynski, H.Zankel

4He(n(pol), n)4He Analyzing Power in the Energy Range from 15 to 50 MeV

NUCLEAR REACTIONS 4He(polarized n, n), E=15-50 MeV; measured analyzing power vs E, θ; deduced phase shifts, inelasticity parameters.

doi: 10.1103/PhysRevC.30.1810
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset21961.


1984ZA06      Z.Phys. A317, 45 (1984)

H.Zankel, W.Plessas

Off-Shell Effects in Nucleon-Deuteron Polarization Observables

NUCLEAR REACTIONS 1H(polarized d, d), E=10 MeV; calculated spin correlation parameter. Vector polarized beam. 2H(polarized p, p), E=10 MeV; calculated spin transfer coefficients, polarized outgoing proton; deduced intermediate range repulsion, off-shell effect roles. Separable representation, S-wave Paris potential.

doi: 10.1007/BF01420447
Citations: PlumX Metrics


1983SC02      Phys.Lett. 120B, 297 (1983)

R.Schmelzer, H.Kuiper, M.Schoberl, S.Berber, H.Hilmert, R.Koppel, R.Pferdmenges, H.Zankel

Polarized Deuteron Elastic Scattering from a Polarized Proton Target

NUCLEAR REACTIONS 1H(polarized d, d), E=10 MeV; measured spin correlation parameter vs θ. Polarized target. Faddeev calculation, local potentials, Coulomb distortion.

doi: 10.1016/0370-2693(83)90448-3
Citations: PlumX Metrics


1983ZA01      Phys.Rev. C27, 419 (1983)

H.Zankel, G.M.Hale

Difference of Neutron and Proton Analyzing Powers in Elastic N - d Scattering between 5 and 14 MeV

NUCLEAR REACTIONS 2H(polarized p, p), (polarized n, n), E=5-14 MeV; analyzed A(θ) data; deduced Coulomb distortion role. Faddeev amplitudes.

doi: 10.1103/PhysRevC.27.419
Citations: PlumX Metrics


1983ZA06      Phys.Lett. 132B, 27 (1983)

H.Zankel, L.Mathelitsch

Nucleon-Deuteron Low Energy Parameters

NUCLEAR REACTIONS 2H(p, p), (n, n), E=low; calculated scattering lengths, effective range parameters. Momentum space Faddeev equations.

doi: 10.1016/0370-2693(83)90215-0
Citations: PlumX Metrics


1982FR11      Nucl.Phys. A384, 97 (1982)

J.Frohlich, H.Kriesche, L.Streit, H.Zankel

Prediction of n - 4He Phase Shifts from p - 4He Data between 20 and 55 MeV

NUCLEAR REACTIONS 4He(n, n), E < 20 MeV; calculated phase shifts. R-matrix, proton scattering data input.

doi: 10.1016/0375-9474(82)90307-4
Citations: PlumX Metrics


1981HA30      Phys.Rev. C24, 1322 (1981)

M.I.Haftel, H.Zankel

Approximate Coulomb Effects in the Three-Body Scattering Problem

NUCLEAR REACTIONS 2H(p, p), E=2, 10 MeV; calculated σ(θ). Faddeev equations, Coulomb, nuclear interference.

doi: 10.1103/PhysRevC.24.1322
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1981ZA06      Phys.Rev. C24, 1384 (1981)

H.Zankel, G.M.Hale

Approximate Coulomb Correction to Elastic N - d Scattering

NUCLEAR REACTIONS 2H(polarized n, n), (polarized p, p), E=5 MeV; calculated σ(θ), A(θ); 1n, 1H(polarized d, d), E=10 MeV; calculated iT11(θ), T21(θ), T20(θ), T22(θ). T-matrix, Coulomb correction.

doi: 10.1103/PhysRevC.24.1384
Citations: PlumX Metrics


1980FR07      Phys.Lett. 92B, 8 (1980)

J.Frohlich, L.Streit, H.Zankel

Coulomb Corrections in N-N Coupled States

NUCLEAR REACTIONS 1H(p, p), E=50-400 MeV; calculated angular momentum mixing parameters, phase shifts. Coulomb nuclear interference effects, on-shell approximation.

doi: 10.1016/0370-2693(80)90290-7
Citations: PlumX Metrics


1980KR13      J.Phys.(London) G6, 853 (1980)

H.Kriesche, H.Zankel

Coulomb Corrections in Non-Relativistic π+-p Scattering

NUCLEAR REACTIONS 1H(π+, π+), E=20-500 MeV; calculated Coulomb corrections to phase shifts. Separable potentials.

doi: 10.1088/0305-4616/6/7/008
Citations: PlumX Metrics


1976AL13      Phys.Rev.Lett. 37, 1537 (1976)

E.O.Alt, W.Sandhas, H.Zankel, H.Ziegelmann

Coulomb Corrections in Proton-Deuteron Scattering

NUCLEAR REACTIONS 2H(p, p), E=2, 10 MeV; calculated σ(θ).

doi: 10.1103/PhysRevLett.37.1537
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1976ZA04      Acta Phys.Austr. 44, 245 (1976)

H.Zankel, H.Zingl

An Application of the Quasiparticle Method to Three-Nucleon Bound States

NUCLEAR STRUCTURE 3H, 3He; calculated potentials.


1975ZA03      Lett.Nuovo Cim. 12, 221 (1975)

H.Zankel, C.Fayard, G.H.Lamot

Coulomb Energy of 3He

NUCLEAR STRUCTURE 3H, 3He; calculated Coulomb energies.

doi: 10.1007/BF02784801
Citations: PlumX Metrics


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