Nuclear Science References (NSR)

NUCLEAR REACTIONS ¹H(p, π⁺), E=295-810 MeV; ²H(p, π⁰), E=340-500 MeV; ³He(³He, π⁺), E=300-600 MeV; calculated σ(θ). Microscopic reaction model, nucleon resonance excitation role in channel coupling, other high energy data analysis included.

doi: 10.1007/BF01290328
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1990HU03 Z.Phys. C46, S37 (1990)

M.G.Huber, B.Ch.Metsch

KAON and COSY - Common Aspects in Hadron Physics

NUCLEAR REACTIONS ¹²C(π, π), E=260 MeV; calculated σ(θ), scattering amplitude.

1987ME16 Nucl.Phys. A473, 160 (1987)

W.Mettner, A.Richter, W.Stock, B.C.Metsch, A.G.M.van Hees

Electroexcitation of ⁵⁸Ni: A study of the fragmentation of the magnetic dipole strength

NUCLEAR REACTIONS ⁵⁸Ni(e, e'), E=39-57 MeV; measured σ(E(e')), σ(θ). ⁵⁸Ni deduced B(λ). Comparison with shell model calculation.

doi: 10.1016/0375-9474(87)90159-X
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1986KN05 Nucl.Phys. A457, 292 (1986)

W.Knupfer, W.Muller, B.C.Metsch, A.Richter

Consistent Empirical Description of Magnetic Moments and M1 Transitions - Quenching of the Diagonal and Off-Diagonal Spin Matrix Elements -

NUCLEAR STRUCTURE A < 100; ²⁰⁸Pb; calculated B(M1); deduced spin matrix element quenching. Shell model.

doi: 10.1016/0375-9474(86)90379-9
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1985SO05 Phys.Rev. C31, 2054 (1985)

D.I.Sober, B.C.Metsch, W.Knupfer, G.Eulenberg, G.Kuchler, A.Richter, E.Spamer, W.Steffen

Magnetic Dipole Excitations in the N = 28 Isotones ⁵⁰Ti, ⁵²Cr, and ⁵⁴Fe

NUCLEAR REACTIONS ⁵⁰Ti, ⁵²Cr, ⁵⁴Fe(e, e'), E=30-57 MeV; measured σ(θ), σ(E(e')). ⁵⁰Ti, ⁵²Cr, ⁵⁴Fe levels deduced B(λ), transition radius, M1 total strength, fragmentation. Shell model calculations.

doi: 10.1103/PhysRevC.31.2054
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1984KN03 J.Phys.(Paris), Colloq.C4, 513 (1984); See 1984Kn04

W.Knupfer, B.C.Metsch

Many-Particle Many-Hole Excitations and the Retardation of Magnetic Dipole and GT Transition-Strengths

1984KN04 J.Phys.(Paris), Colloq.C-4, 513 (1984)

W.Knupfer, B.C.Metsch

Many-Particle Many-Hole Excitations and the Retardation of Magnetic Dipole and GT Transition-Strengths

NUCLEAR STRUCTURE ⁹⁰Zr; calculated level density, Gamow-Teller transition strength distributions. A ≤ 210; calculated B(M1), μ; deduced spin, tensor corrections.

1984MU25 Nucl.Phys. A430, 61 (1984)

W.Muller, B.C.Metsch, W.Knupfer, A.Richter

Calculation of the β⁺ Decay of Proton-Rich sd-Shell Nuclei into a Gamow-Teller Resonance

RADIOACTIVITY ^32,33Ar, ³⁶Ca(β⁺); calculated β⁺ strength function; deduced Gamow-Teller resonance, J, π. Shell Model.

doi: 10.1016/0375-9474(84)90192-1
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1983BE11 Nucl.Phys. A398, 408 (1983)

D.Bender, G.Eulenberg, A.Richter, E.Spamer, B.C.Metsch, W.Knupfer

Search for M1 Strength in ⁵¹V and the Difference in ⁵¹V(e, e') and ⁵¹V(p, p') Spectra

NUCLEAR REACTIONS ⁵¹V(e, e'), E=38-57 MeV; measured σ(E, θ). ⁵¹V deduced B(M1).

doi: 10.1016/0375-9474(83)90292-0
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1983KN05 Phys.Rev. C27, 2487 (1983)

W.Knupfer, B.C.Metsch

Importance of the Orbital Magnetization for Isovector M1 Transitions of Nuclei in the sd Shell

NUCLEAR STRUCTURE ²⁰Ne, ²⁸Si, ³²S; calculated B(M1) strength distribution. Isovector transitions, shell model.

NUCLEAR REACTIONS ²⁰Ne(e, e'), E not given; ²⁰Ne(π^-, γ), E at rest; ²⁰Ne(p, n), E=135 MeV; calculated B(M1) transition strength distribution, radiative pion capture, σ(p, n); deduced orbital magnetization effect. Shell model.

doi: 10.1103/PhysRevC.27.2487
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1983KN08 Phys.Lett. 129B, 375 (1983)

W.Knupfer, B.C.Metsch, A.Richter

Proton Correlations and the Missing M1 Strength in ⁴⁸Ca: A two-state model

NUCLEAR STRUCTURE ⁴⁸Ca; calculated B(M1); deduced proton correlation. Two-state shell model.

doi: 10.1016/0370-2693(83)90122-3
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1983MU03 Phys.Lett. 120B, 305 (1983)

S.Muller, A.Richter, E.Spamer, W.Knupfer, B.C.Metsch

Experimental Study of Proton and Neutron Spin-Flip Contributions to the Electroexcitation of the J(π) = 1⁺ State at E(x) = 5.846 MeV in ²⁰⁸Pb

NUCLEAR REACTIONS ²⁰⁸Pb(e, e'), E=23.3, 36.4, 49.8, 61.2 MeV; measured σ(E(e')), σ(θ) vs E; deduced tensor correlation, neutron, proton contribution interference. ²⁰⁸Pb deduced M1 transition isovector character. RPA calculations.

doi: 10.1016/0370-2693(83)90450-1
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1983PU02 Nucl.Phys. A401, 269 (1983)

N.G.Puttaswamy, W.Oelert, A.Djaloeis, C.Mayer-Boricke, P.Turek, P.W.M.Glaudemans, B.C.Metsch, K.Heyde, M.Waroquier, P.Van Isacker, G.Wenes, V.Lopac, V.Paar

Structure of the Energy Levels of ^{53, 55, 57}Mn from the (d, ³He) Reaction on Iron Isotopes at 80 MeV

NUCLEAR REACTIONS ^54,56,58Fe(d, ³He), E=80 MeV; measured σ(E(³He)), σ(θ). ^53,55,57Mn deduced levels, L, S. DWBA analysis, shell model, quasiparticle-core coupling, cluster vibration model calculations.

doi: 10.1016/0375-9474(83)90530-4
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1982EU01 Phys.Lett. 116B, 113 (1982)

G.Eulenberg, D.I.Sober, W.Steffen, H.-D.Graf, G.Kuchler, A.Richter, E.Spamer, B.C.Metsch, W.Knupfer

Inelastic Electron Scattering on the N = 28 Isotones ⁴⁸Ca, ⁵⁰Ti, ⁵²Cr and ⁵⁴Fe and the Shape and Magnitude of the M1 Strength Distributions

NUCLEAR REACTIONS ⁴⁸Ca, ⁵⁰Ti, ⁵²Cr, ⁵⁴Fe(e, e'), E=30-58 MeV; measured σ(E(e')), σ(θ). ⁵⁰Ti, ⁵²Cr, ⁵⁴Fe deduced B(M1) strength distribution. ⁴⁸Ca deduced total B(M1). Shell model.

doi: 10.1016/0370-2693(82)90987-X
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1982ME07 Z.Phys. A306, 105 (1982)

B.C.Metsch, G.A.Timmer, R.van der Heyden, P.W.M.Glaudemans

Effects of Central and Noncentral Components of the Preedom-Wildenthal Interaction

NUCLEAR STRUCTURE A=20-22; calculated levels, quadrupole moments, μ, B(M1), γ-branching, binding energies. Phenomenological interactions.

doi: 10.1007/BF01415479
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1982ME09 Z.Phys. A307, 251 (1982)

B.C.Metsch, P.W.M.Glaudemans

Model-Space Dependence of Nuclear Observables

NUCLEAR STRUCTURE ^24,25,26Mg, ²⁵Na, ²⁶Al; calculated binding energies, levels, quadrupole moment, B(λ), μ, spectroscopic factors; deduced model space dependence. Shell model, effective interactions.

doi: 10.1007/BF01438646
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1982VA02 Nucl.Phys. A373, 81 (1982)

C.J.Van Der Poel, G.A.P.Engelbertink, H.J.M.Aarts, D.E.C.Scherpenzeel, H.F.R.Arciszewski, B.C.Metsch

High-Spin States in ³⁴Cl

NUCLEAR REACTIONS ³¹P(α, nγ), E=11.7, 16.3 MeV; measured σ(Eγ, E), Doppler pattern, T_1/2. ²⁴Mg(¹²C, npγ), E=32-35 MeV; measured σ(Eγ, θ), σ(Eγ, E), γγ-coin, Eγ, γγ(θ). ³⁴Cl deduced levels, T_1/2, γ-branching, J, π, δ. Enriched target, hyperpure Ge, large-angle Compton suppression spectrometer.

doi: 10.1016/0375-9474(82)90182-8
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1981ME01 Nucl.Phys. A352, 60 (1981)

B.C.Metsch, P.W.M.Glaudemans

Spectroscopic Properties and Collective Structure from a Shell-Model Description of A=53 Nuclei

NUCLEAR STRUCTURE ⁵³Ni, ⁵³Co, ⁵³Fe, ⁵³Mn; calculated negative-parity levels, S, B(λ), log ft, quadrupole moments, g, band structure, high-spin states. Shell model, modified Kuo-Brown force, surface delta interactions.

doi: 10.1016/0375-9474(81)90559-5
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1979TI01 Phys.Lett. 82B, 305 (1979)

G.A.Timmer, R.van der Heyden, B.C.Metsch, K.Klingenbeck

Central and Noncentral Components of the Preedom-Wildenthal Interaction

NUCLEAR STRUCTURE ²¹Ne; calculated level properties. Shell model with Preedom-Wildenthal interaction. Influence of central, tensor, spin-orbit, antisymmetric spin-orbit examined.

doi: 10.1016/0370-2693(79)90228-4
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1979VA19 Z.Phys. A293, 327 (1979)

A.G.M.van Hees, P.W.M.Glaudemans, B.C.Metsch

The Influence of f₇/₂ Hole Configurations on Properties of ^57-59Ni

NUCLEAR STRUCTURE ^57,58,59Ni; calculated energy levels, B(λ), S, μ, quadrupole moment. Shell model, surface delta interactions.

1978GL06 Fizika, Suppl. 10, 57 (1978)

P.W.M.Glaudemans, R.J.G.Goossens, A.G.M.van Hees, B.C.Metsch, R.Vennink

Effects of ⁵⁶Ni Core Excitations

NUCLEAR STRUCTURE ⁵⁷Ni; calculated electromagnetic properties. Shell model, effective interactions.

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