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NSR database version of May 3, 2024.

Search: Author = W.Schadow

Found 17 matches.

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2004CA27      Nucl.Phys. A737, 200 (2004)

L.Canton, W.Schadow

What can we learn from an explicit treatment of the π in the three-nucleon system?

NUCLEAR REACTIONS 2H(n, n), E=8.5-18 MeV; analyzed σ(θ), analyzing powers, role of pion dynamics.

doi: 10.1016/j.nuclphysa.2004.03.064
Citations: PlumX Metrics

2002CA32      Eur.Phys.J. A 14, 225 (2002)

L.Canton, W.Schadow, J.Haidenbauer

Irreducible Pionic Effects in Nucleon-Deuteron Scattering Below 20 MeV

NUCLEAR REACTIONS 2H(p, p), (n, n), E=3-19 MeV; calculated σ(θ), analyzing powers, spin transfer coefficients, polarization transfer coefficients. Comparison with data and between different potentials.

doi: 10.1140/epja/i2001-10122-3
Citations: PlumX Metrics

2002HO09      Phys.Rev. C65, 065501 (2002)

E.C.Y.Ho, H.W.Fearing, W.Schadow

Radiative Muon Capture by 3He

NUCLEAR REACTIONS 3He(μ-, νγ), E not given; calculated capture rates, γ-spectra. Comparison of elementary particle model and impulse approximation.

doi: 10.1103/PhysRevC.65.065501
Citations: PlumX Metrics

2001CA19      Nucl.Phys. A684, 417c (2001)

L.Canton, G.Pisent, W.Schadow, J.P.Svenne

Spin Observables for Pion Production from pd Collisions

NUCLEAR REACTIONS 2H(polarized p, π0), E ≈ threshold; calculated Ay(θ). Comparison with data.

doi: 10.1016/S0375-9474(01)00442-0
Citations: PlumX Metrics

2001CA44      Phys.Rev. C64, 031001 (2001)

L.Canton, W.Schadow

One-Pion-Exchange Three-Nucleon Force and the Ay Puzzle

NUCLEAR REACTIONS 2H(n, n), E=3-30 MeV; calculated σ(θ), analyzing powers; deduced three-nucleon force effects. Comparisons with data.

doi: 10.1103/PhysRevC.64.031001
Citations: PlumX Metrics

2001SC16      Phys.Rev. C63, 044006 (2001)

W.Schadow, O.Nohadani, W.Sandhas

Photonuclear Reactions of Three-Nucleon Systems

NUCLEAR REACTIONS 3H, 3He(γ, X), E=5-100 MeV; calculated photodisintegration σ, σ(θ), asymmetry. 2H(p, γ), (n, γ), E=5-40 MeV; calculated capture σ, σ(θ). Comparison with data and between various nuclear potentials.

doi: 10.1103/PhysRevC.63.044006
Citations: PlumX Metrics

2000CA23      Phys.Rev. C61, 064009 (2000)

L.Canton, W.Schadow

Isoscalar Off-Shell Effects in Threshold Pion Production from pd Collisions

NUCLEAR REACTIONS 2H(p, π+), E ≈ threshold; calculated σ(θ), tensor analyzing power; deduced off-shell effects. Comparisons with data.

doi: 10.1103/PhysRevC.61.064009
Citations: PlumX Metrics

2000CA39      Phys.Rev. C62, 044005 (2000)

L.Canton, W.Schadow

Why is the Three-Nucleon Force so Odd ?

doi: 10.1103/PhysRevC.62.044005
Citations: PlumX Metrics

2000SC27      Few-Body Systems 28, 241 (2000)

W.Schadow, W.Sandhas, J.Haidenbauer, A.Nogga

Comparison of Triton Bound-State Properties using Different Separable Representations of Realistic Nucleon-Nucleon Potentials

NUCLEAR STRUCTURE 3H; calculated binding energies, wave functions. Separable expansion methods compared.

doi: 10.1007/s006010070023
Citations: PlumX Metrics

1999BE37      Phys.Rev. C60, 034004 (1999)

M.Beyer, W.Schadow, C.Kuhrts, G.Ropke

Three-Body Properties in Nuclear Matter at Thermal Equilibrium

doi: 10.1103/PhysRevC.60.034004
Citations: PlumX Metrics

1999SC03      Phys.Rev. C59, 607 (1999)

W.Schadow, W.Sandhas

Radiative Capture of Protons by Deuterons

NUCLEAR REACTIONS 2H(p, γ), E not given; calculated σ(E), σ(θ). Several potentials compared. Comparison with data.

doi: 10.1103/PhysRevC.59.607
Citations: PlumX Metrics

1998CA09      Phys.Rev. C57, 1588 (1998)

L.Canton, G.Cattapan, G.Pisent, W.Schadow, J.P.Svenne

Spin Observables for the pd ← → π+t Reaction Around the Δ Resonance

NUCLEAR REACTIONS 2H(polarized p, π+), E=350 MeV; calculated σ(θ), A(y0)(θ), T(20)(θ); deduced reaction mechanism, Δ resonance role. Comparison with data.

doi: 10.1103/PhysRevC.57.1588
Citations: PlumX Metrics

1998EL13      Phys.Rev. C58, 3109 (1998)

Ch.Elster, W.Schadow, H.Kamada, W.Glockle

Shadowing and Antishadowing Effects in a Model for the n + d Total Cross Section

NUCLEAR REACTIONS 2H(n, n), E=50-5000 MeV; calculated σ; deduced rescattering effects.

doi: 10.1103/PhysRevC.58.3109
Citations: PlumX Metrics

1998SA14      Nucl.Phys. A631, 210c (1998)

W.Sandhas, W.Schadow, G.Ellerkmann, L.L.Howell, S.A.Sofianos

Photodisintegration of Three- and Four- Nucleon Systems

NUCLEAR REACTIONS 3H(γ, n), E=5-40 MeV; 2H(p, γ), E=12.1 MeV; analyzed σ(θ). 4He(γ, n), E=20-35 MeV; 4He(γ, p), E < 170 MeV; analyzed total σ. Several models compared.

doi: 10.1016/S0375-9474(98)00024-4
Citations: PlumX Metrics

1998SC14      Nucl.Phys. A631, 588c (1998)

W.Schadow, W.Sandhas

Triton Photodisintegration with Realistic Potentials

NUCLEAR REACTIONS 3H(γ, n), E=5-40 MeV; calculated σ(θ); deduced E2 contributions. Ernst-Shakin-Thaler expansion. Comparison with data.

doi: 10.1016/S0375-9474(98)00072-4
Citations: PlumX Metrics

1997CA37      Phys.Rev. C56, 1231 (1997)

L.Canton, W.Schadow

pd → π+t Reaction Around the Δ Resonance

NUCLEAR REACTIONS 2H(p, X), E=300-605 MeV; analyzed π+ production σ vs π momentum, other observables; deduced reaction mechanism related features. Three-body mechanisms.

doi: 10.1103/PhysRevC.56.1231
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1997SC04      Phys.Rev. C55, 1074 (1997)

W.Schadow, W.Sandhas

Photodisintegration of the Triton with Realistic Potentials

NUCLEAR REACTIONS 3H(γ, n), E ≈ 5-40 MeV; analyzed photodisintegration σ(θ) vs E. Three-body integral equations, subsystem amplitudes W-matrix representation in kernel.

doi: 10.1103/PhysRevC.55.1074
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