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NSR database version of April 27, 2024.

Search: Author = S.Tesch

Found 13 matches.

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1990AB11      Few-Body Systems 8, 137 (1990)

V.G.Ableev, S.V.Dzhmukhadze, Ch.Dimitrov, A.P.Kobushkin, B.Naumann, L.Naumann, A.A.Nomofilov, L.Penchev, N.M.Piskunov, V.I.Sharov, I.M.Sitnik, E.A.Strokovsky, L.N.Strunov, S.Tesch, S.A.Zaporozhets

Proton and Triton Momentum Distribution from 4He Fragmentation at Relativistic Energies

NUCLEAR REACTIONS 12C(α, p), E at 4.52 GeV/c/per nucleon; 12C(α, t), E at 2.69 GeV/c/nucleon; measured σ(θ=0°). 4He deduced p, t momentum distributions. Model comparison.

doi: 10.1007/BF01081826
Citations: PlumX Metrics

1983MA36      Z.Phys. A312, 259 (1983)

S.G.Mashnik, S.Tesch

On the Mechanism of Inclusive Particle Emission in Proton-Nucleus Collisions at 0.5 GeV

NUCLEAR REACTIONS 58Ni, 181Ta(p, pX), 181Ta, 12C, 27Al, 58Ni(p, nX), (p, πX), E=0.5 GeV; calculated inclusive σ(θp, Ep), σ(θn, En), σ(θ(π), E(π)). Cascade exciton model.

doi: 10.1007/BF01412170
Citations: PlumX Metrics

1980GU11      Nucl.Phys. A342, 239 (1980)

H.Guratzsch, B.Kuhn, H.Kumpf, J.Mosner, W.Neubert, W.Pilz, G.Schmidt, S.Tesch

Neutron-Neutron Effective Range from Quasifree Scattering 2H(n, nn)p At 25 MeV

NUCLEAR REACTIONS 2H(n, 2n), E=25 MeV; measured σ(E(n1), E(n2), θ1, θ2), quasifree neutron-neutron kinematic condition; deduced neutron-neutron effective range. D2O target.

doi: 10.1016/0375-9474(80)90252-3
Citations: PlumX Metrics

1980KO37      Yad.Fiz. 32, 313 (1980); Sov.J.Nucl.Phys. 32, 161 (1980)

V.I.Komarov, G.E.Kosarev, H.Muller, D.Netzband, S.Tesch, T.Stiehler

Two-Particle Differential Cross Sections of Proton Emission in Proton-Nucleus Interactions at 640 MeV

NUCLEAR REACTIONS Be, C, Al, Cu, Pb(p, 2p), E=640 MeV; measured σ(θp1, θp2, Ep1, Ep2); deduced reaction mechanism. Coplanar, noncoplanar geometries. Cascade, phenomenological models.

1980KO40      Yad.Fiz. 32, 1476 (1980)

V.I.Komarov, G.E.Kosarev, H.Muller, D.Netzband, S.Tesch, T.Stiehler

Quasi-Free Knock-Out of Proton Pair from Carbon Nuclei with 640 MeV Protons

NUCLEAR REACTIONS C(p, 3p), E=640 MeV; measured σ(θ1, E1, θ2, E2, θ3, E3). Quasifree knockout kinematic setup. Cluster excitation model.

1979KO21      Nucl.Phys. A326, 297 (1979)

V.I.Komarov, G.E.Kosarev, H.Muller, D.Netzband, V.D.Toneev, T.Stiehler, S.Tesch, K.K.Gudima, S.G.Mashnik

Proton-Nucleus Interactions at 640 MeV Accompanied by Backward Emission of Energetic Protons

NUCLEAR REACTIONS Be, C, Al, Cu, Pb(p, pX), (p, 2pX), E=640 MeV; measured σ(Ep, θp), σ(E1, θ1, E2, θ2), pp-coin; deduced reaction mechanism. Comparison with cascade model predictions, phase space calculations. Natural targets.

doi: 10.1016/0375-9474(79)90396-8
Citations: PlumX Metrics

1979KO36      J.Phys.(London) G5, 1717 (1979)

V.I.Komarov, G.E.Kosarev, H.Muller, D.Netzband, T.Stiehler, S.Tesch

Quasifree Knock-Out of Proton Pairs in the Reaction C(p, 3p) at 640 Mev

NUCLEAR REACTIONS C(p, 3p), E=640 MeV; measured σ(E1, θ1, E2, θ2, E3), ppp-coin. Phenomenoligical models, natural target.

doi: 10.1088/0305-4616/5/12/010
Citations: PlumX Metrics

1978KO30      Phys.Lett. 80B, 30 (1978)

V.I.Komarov, G.E.Kosarev, H.Muller, D.Netzband, T.Stiehler, S.Tesch

Observation of Correlation between Two Fast Protons in Proton-Nucleus Interactions at 640 MeV

NUCLEAR REACTIONS 12C(p, 2p), E=640 MeV; measured σ(θ) for backward emission of fast protons. Comparison with theoretical models.

doi: 10.1016/0370-2693(78)90298-8
Citations: PlumX Metrics

1977GU13      Nucl.Phys. A293, 109 (1977)

H.Guratzsch, B.Kuhn, H.Kumpf, J.Mosner, W.Neubert, W.Pilz, G.Schmidt, S.Tesch

The Neutron-Proton Final-State Interaction in Proton-Induced Deuteron Break-up at 8.5 MeV

NUCLEAR REACTIONS 2H(p, 2p), E=8.5 MeV; measured σ(Ep1, Ep2, θ1, θ2, φ); deduced final-state interaction angular distribution; compared with Faddeev theory for exponential, Yamaguchi form factors.

doi: 10.1016/0375-9474(77)90479-1
Citations: PlumX Metrics

1976KO03      Nucl.Phys. A256, 362 (1976)

V.I.Komarov, G.E.Kosarev, E.S.Kuzmin, A.G.Molokanov, G.P.Reshetnikov, O.V.Savchenko, S.Tesch

Production of Fast Fragments by Bombarding Light Nuclei with Intermediate-Energy Protons

NUCLEAR REACTIONS Li, Be, C(p, X), (p, πd), E=380-665 MeV; measured σ(E, Ed). 6Li, Be, C(p, X), (p, πt), (p, π3He), (p, πα), E=665 MeV; measured σ. Natural, enriched targets.

doi: 10.1016/0375-9474(76)90378-X
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1972KU08      Nucl.Phys. A183, 640 (1972)

B.Kuhn, H.Kumpf, S.Parzhitsky, S.Tesch

Determination of the Neutron-Neutron Scattering Length from a Kinematically Complete Experiment with the Reaction 3H(t, n4He)n

NUCLEAR REACTIONS 3H(t, nα), E=1.39 MeV; 3He(3He, pα), E=3.35 MeV; 3He(t, pα), E=1.39 MeV; measured σ(En, Eα), σ(Ep, Eα); deduced n-n, p-p, n-p singlet scattering lengths. 3H, 3He gas targets.

doi: 10.1016/0375-9474(72)90361-2
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1970KL04      Nucl.Phys. A152, 232 (1970)

R.Klabes, F.Baldeweg, V.Bredel, H.Guratzsch, G.Stiller, S.Tesch

The (d, α) Reaction on 13C

NUCLEAR REACTIONS 13C(d, α), E=12.1-14.1 MeV; measured σ(E;Eα, θ). Enriched target. DWBA calculations.

doi: 10.1016/0375-9474(70)90825-0
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1771.

1968TE04      Nucl.Phys. A117, 66(1968)

S.Tesch, F.Baldeweg, V.Bredel, H.Guratzsch, R.Klabes, G.Stiller

The (d, t) Reaction on 13C

NUCLEAR REACTIONS 13C(d, t), E=12.1-14.0 MeV; measured σ(E; Et, θ). 12C deduced S. Enriched target.

doi: 10.1016/0375-9474(68)90861-0
Citations: PlumX Metrics

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