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NSR database version of April 11, 2024.

Search: Author = O.Scholten

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2014AB06      Nucl.Phys. A927, 91 (2014)

S.Abu Musleh, H.M.Abu Zeid, O.Scholten

A description of odd mass Xe and Te isotopes in the Interacting Boson-Fermion Model

NUCLEAR STRUCTURE 123,125,127,129,131Te, 125,127,129,131Xe; calculated levels, J, π, γ transitions, spectroscopic factors, B(M1), B(E2) using IBFA (interacting Boson-Fermion approximation) model; deduced IBFM parameters.

doi: 10.1016/j.nuclphysa.2014.04.009
Citations: PlumX Metrics


2013SH32      Phys.Rev. C 88, 025209 (2013)

R.Shyam, O.Scholten, A.W.Thomas

Production of the H dibaryon via the (K-, K+) reaction on a 12C target

doi: 10.1103/PhysRevC.88.025209
Citations: PlumX Metrics


2012AB03      Nucl.Phys. A878, 37 (2012)

S.Abu Musleh, O.Scholten

A description of odd mass W-isotopes in the Interacting Boson-Fermion model

NUCLEAR STRUCTURE 183,185,187W; calculated levels, J, π, B(E2), occupation probabilities of single-particle states, spectroscopic factors using IBFA (Interacting Boson-Fermion Approx). Compared to data and other calculation.

doi: 10.1016/j.nuclphysa.2012.01.011
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2012KA20      Eur.Phys.J. A 48, 56 (2012)

H.Kaneko, A.Hosaka, O.Scholten

A hidden local symmetry approach to rho-meson photoproduction

doi: 10.1140/epja/i2012-12056-y
Citations: PlumX Metrics


2011SH29      Phys.Rev. C 84, 042201 (2011)

R.Shyam, O.Scholten, A.W.Thomas

Production of a cascade hyperon in the K--proton interaction

doi: 10.1103/PhysRevC.84.042201
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2010OZ03      Nucl.Phys. A835, 321c (2010)

S.Ozaki, H.Nagahiro, A.Hosaka, O.Scholten

Φ Photoproduction in a Coupled-Channel Approach

doi: 10.1016/j.nuclphysa.2010.01.209
Citations: PlumX Metrics


2010SH04      Phys.Rev. C 81, 015204 (2010)

R.Shyam, O.Scholten, H.Lenske

Associated photoproduction of K+ mesons off protons within a coupled-channels K-matrix approach

doi: 10.1103/PhysRevC.81.015204
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2009MA59      Eur.Phys.J. A 41, 25 (2009)

M.Mahjour-Shafiei, H.R.Amir-Ahmadi, J.C.S.Bacelar, R.Castelijns, K.Ermisch, E.D.van Garderen, I.Gasparic, M.N.Harakeh, N.Kalantar-Nayestanaki, M.Kis, H.Lohner, O.Scholten

Proton-proton bremsstrahlung cross-sections including the kinematical singularity

NUCLEAR REACTIONS 1H(polarized p, p'), E=190 MeV; measured bremsstrahlung σ, σ(θ) and relative energy of the two protons. Comparison with two soft-photon models.

doi: 10.1140/epja/i2009-10786-5
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2009OZ01      Phys.Rev. C 80, 035201 (2009), Erratum Phys.Rev. C 81, 059901 (2010)

S.Ozaki, A.Hosaka, H.Nagahiro, O.Scholten

Coupled-channel analysis for φ photoproduction with Λ(1520)

doi: 10.1103/PhysRevC.80.035201
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2008SH25      Phys.Rev. C 78, 065201 (2008)

R.Shyam, O.Scholten

Photoproduction of η mesons within a coupled-channels K-matrix approach

doi: 10.1103/PhysRevC.78.065201
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2007BU23      Phys.Rev.Lett. 99, 092503 (2007)

O.Burda, N.Botha, J.Carter, R.W.Fearick, S.V.Fortsch, C.Fransen, H.Fujita, J.D.Holt, M.Kuhar, A.Lenhardt, P.von Neumann-Cosel, R.Neveling, N.Pietralla, V.Yu.Ponomarev, A.Richter, O.Scholten, E.Sideras-Haddad, F.D.Smit, J.Wambach

High-Energy-Resolution Inelastic Electron and Proton Scattering and the multiphonon Nature of Mixed-Symmetry 2+ States in 94Mo

NUCLEAR REACTIONS 94Mo(e, e'), E=70 MeV; 94Mo(p, p'), E=200 MeV; measured σ and excitation strengths. Compared results to model calculations.

doi: 10.1103/PhysRevLett.99.092503
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Data from this article have been entered in the XUNDL database. For more information, click here.


2007CO03      Phys.Rev. C 75, 014006 (2007)

M.D.Cozma, O.Scholten, R.G.E.Timmermans, J.A.Tjon

Two-pion exchange contributions to the relativistic NN kernel: Peripheral scattering

doi: 10.1103/PhysRevC.75.014006
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2007FU12      Nucl.Phys. A788, 94c (2007)

H.Fujita, N.T.Botha, O.Burda, J.Carter, R.W.Fearick, S.V.Fortsch, C.Fransen, M.Kuhar, A.Lenhardt, P.von Neumann-Cosel, R.Neveling, N.Pietralla, V.Yu.Ponomarev, A.Richter, O.Scholten, E.Sideras-Haddad, F.D.Smit, J.Wambach

One- and two-phonon mixed-symmetry states in 94Mo in high-resolution electron and proton scattering

NUCLEAR REACTIONS 94Mo(e, e'), E=70 MeV; 94Mo(p, p')E=200 MeV; measured excitation energy spectra; deduced mixed-symmetry state features. Comparison with shell model, quasiparticle phonon model and interacting boson model.

doi: 10.1016/j.nuclphysa.2007.01.053
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2007SC23      Phys.Rev. C 75, 055203 (2007)

O.Scholten, S.Tamenaga, H.Toki

Loop corrections and the K-matrix formalism

doi: 10.1103/PhysRevC.75.055203
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2006MA03      Phys.Lett. B 632, 480 (2006)

M.Mahjour-Shafiei, H.R.Amir-Ahmadi, J.C.S.Bacelar, R.Castelijns, K.Ermisch, E.D.van Garderen, I.Gasparic, M.N.Harakeh, N.Kalantar-Nayestanaki, M.Kis, H.Lohner, O.Scholten

Proton-proton bremsstrahlung towards the elastic limit at 190 MeV incident beam energy

NUCLEAR REACTIONS 1H(polarized p, p'), E=190 MeV; measured bremsstrahlung σ(θ), vector analyzing power.

doi: 10.1016/j.physletb.2005.10.088
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2006US02      Phys.Rev. C 74, 015205 (2006)

A.Usov, O.Scholten

Channel coupling effects in ρ-meson photoproduction

NUCLEAR REACTIONS 1n, 1H(γ, X), E ≈ 1-3.5 GeV; analyzed π-meson production σ(θ), related data; deduced channel coupling effects.

doi: 10.1103/PhysRevC.74.015205
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2005SC03      Phys.Rev. C 71, 034005 (2005)

O.Scholten, J.G.O.Ojwang, S.Tamenaga

Dibaryon resonance and two-photon bremsstrahlung in pp scattering

NUCLEAR REACTIONS 1H(p, 2γX), E=216 MeV; calculated two-photon bremsstrahlung σ(E, θ), dibaryon state contribution.

doi: 10.1103/PhysRevC.71.034005
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2005US02      Phys.Rev. C 72, 025205 (2005)

A.Usov, O.Scholten

KΛ and KΣ photoproduction in a coupled-channels framework

NUCLEAR REACTIONS 1H(γ, K+X), (γ, K0X), E=high; analyzed hyperon production associated σ, polarization observables; deduced parameters, channel coupling effects. K-matrix approach.

doi: 10.1103/PhysRevC.72.025205
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2004KO25      Nucl.Phys. A736, 339 (2004)

S.Kondratyuk, K.Kubodera, F.Myhrer, O.Scholten

The Adler-Weisberger and Goldberger-Miyazawa-Oehme sum rules as probes of constraints from analyticity and chiral symmetry in dynamical models for pion-nucleon scattering

doi: 10.1016/j.nuclphysa.2004.03.003
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2004MA71      Phys.Rev. C 70, 024004 (2004)

M.Mahjour-Shafiei, J.C.S.Bacelar, M.D.Cozma, M.J.van Goethem, M.N.Harakeh, M.Hoefman, H.Huisman, N.Kalantar-Nayestanaki, H.Lohner, J.G.Messchendorp, R.W.Ostendorf, S.Schadmand, O.Scholten, M.Volkerts, H.W.Wilschut

High-precision proton-proton bremsstrahlung measurements at 190 MeV

NUCLEAR REACTIONS 1H(polarized p, p), (polarized p, p'γ), E=190 MeV; measured σ(θ), Ay(θ). Comparison with model predictions.

doi: 10.1103/PhysRevC.70.024004
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1226.


2004VO07      Phys.Rev.Lett. 92, 202301 (2004)

M.Volkerts, J.C.S.Bacelar, M.J.van Goethem, M.N.Harakeh, M.Hoefman, H.Huisman, N.Kalantar-Nayestanaki, S.Kopecky, H.Lohner, J.G.Messchendorp, K.Nakayama, R.W.Ostendorf, S.Schadmand, O.Scholten, H.W.Wilschut

Exclusive Measurement of Quasifree Proton-Neutron Bremsstrahlung

NUCLEAR REACTIONS 2H(p, np), E=190 MeV; measured En, Ep, bremsstrahlung Eγ, σ(E, θ); deduced proton-neutron bremsstrahlung features.

doi: 10.1103/PhysRevLett.92.202301
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2004ZH37      Phys.Rev. C 70, 054322 (2004)

Y.M.Zhao, A.Arima, N.Shimizu, K.Ogawa, N.Yoshinaga, O.Scholten

Patterns of the ground states in the presence of random interactions: Nucleon systems

doi: 10.1103/PhysRevC.70.054322
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2003CO18      Phys.Rev. C 68, 044003 (2003)

M.D.Cozma, O.Scholten, R.G.E.Timmermans, J.A.Tjon

Sensitivity of pp bremsstrahlung on low-energy NN interaction

NUCLEAR REACTIONS 1H(p, p'γ), E=0-250 MeV; analyzed bremsstrahlung σ, σ(θ), analyzing powers, partial wave contributions; deduced sensitivity to low-energy interaction model. Relativistic covariant model.

doi: 10.1103/PhysRevC.68.044003
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2003KO57      Phys.Rev. C 68, 045206 (2003)

A.Yu.Korchin, O.Scholten

Comparing phenomenological recipes with a microscopic model for the electric amplitude in strangeness photoproduction

NUCLEAR REACTIONS 1H(γ, K+X), E=0.8, 1.8 GeV; calculated hyperon production associated vertex corrections, internal contributions, form factors. Semirealistic microscopic model.

doi: 10.1103/PhysRevC.68.045206
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2003VO04      Phys.Rev.Lett. 90, 062301 (2003)

M.Volkerts, J.C.S.Bacelar, M.J.van Goethem, M.N.Harakeh, M.Hoefman, H.Huisman, N.Kalantar-Nayestanaki, H.Lohner, J.G.Messchendorp, R.W.Ostendorf, S.Schadmand, O.Scholten, H.W.Wilschut, R.S.Simon, V.Wagner

Exclusive Measurement of Coherent Proton-Deuteron Bremsstrahlung

NUCLEAR REACTIONS 2H(polarized p, p'γ), E=190 MeV; measured Ep, Ed, bremsstrahlung Eγ, Iγ, σ(θ), Ay(θ). Comparison with model predictions.

doi: 10.1103/PhysRevLett.90.062301
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2002CO02      Phys.Rev. C65, 024001 (2002)

M.D.Cozma, G.H.Martinus, O.Scholten, R.G.E.Timmermans, J.A.Tjon

Covariant Model for Proton-Proton Bremsstrahlung: Comparison with high-precision data

NUCLEAR REACTIONS 1H(p, p'γ), E=190 MeV; calculated bremsstrahlung σ(θ), Ay(θ). Relativistic covariant model, comparison with data.

doi: 10.1103/PhysRevC.65.024001
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2002KO12      Phys.Rev. C65, 038201 (2002)

S.Kondratyuk, O.Scholten

Low-Energy Compton Scattering on the Nucleon and Sum Rules

NUCLEAR REACTIONS 1H(γ, γ'), E=low; calculated polarizabilities. Gerasimov-Drell-Hearn and Baldin-Lapidus sum rules.

doi: 10.1103/PhysRevC.65.038201
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2002SC15      Acta Phys.Pol. B33, 847 (2002)

O.Scholten, S.Kondratyuk, L.Van Daele, D.Van Neck, M.Waroquier, A.Yu.Korchin

Compton Scattering on the Proton and Light Nuclei in the Δ-Resonance Region

NUCLEAR REACTIONS 1H, 4He, 12C(γ, γ), E ≈ 150-500 MeV; calculated Compton scattering σ(θ); deduced medium modification, Δ resonance effects. Comparison with data.


2002SC17      Phys.Rev. C65, 054004 (2002)

O.Scholten, A.Yu.Korchin

Virtual-Pion and Two-Photon Production in pp Scattering

NUCLEAR REACTIONS 1H(p, p'γ), E=280 MeV; calculated two-photon production σ(E, θ), bremsstrahlung and virtual pion contributions.

doi: 10.1103/PhysRevC.65.054004
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2002VA01      Phys.Rev. C65, 014613 (2002)

L.Van Daele, A.Yu.Korchin, D.Van Neck, O.Scholten, M.Waroquier

Coherent Compton Scattering on Light Nuclei in the Δ-Resonance Region

NUCLEAR REACTIONS 1H, 4He, 12C(γ, γ), E=150-500 MeV; calculated Compton scattering σ(θ); deduced role of Δ resonance, medium effects. Impulse approximation, comparisons with data.

doi: 10.1103/PhysRevC.65.014613
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2001KO06      Nucl.Phys. A680, 175c (2001)

S.Kondratyuk, O.Scholten

Nucleon Dressing from Dispersion Relations

doi: 10.1016/S0375-9474(00)00412-7
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2001KO22      Nucl.Phys. A684, 426c (2001)

A.Yu.Korchin, O.Scholten

Photoproduction of Electron-Positron Pairs on the Proton in the Resonance Region

NUCLEAR REACTIONS 1H(γ, e+e-), E=0-600 MeV; calculated response functions, charge asymmetry.

doi: 10.1016/S0375-9474(01)00447-X
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2001KO46      Phys.Rev. C64, 024005 (2001)

S.Kondratyuk, O.Scholten

Compton Scattering on the Nucleon at Intermediate Energies and Polarizabilities in a Microscopic Model

NUCLEAR REACTIONS 1H(γ, π), E=150-800 MeV; calculated partial wave amplitudes. 1H(γ, γ), E < 600 MeV; calculated σ(θ), nucleon polarizabilities. Dressed K-matrix model.

doi: 10.1103/PhysRevC.64.024005
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2000HU03      Phys.Lett. 476B, 9 (2000)

H.Huisman, J.C.S.Bacelar, M.J.Van Goethem, M.N.Harakeh, M.Hoefman, N.Kalantar-Nayestanaki, H.Lohner, J.G.Messchendorp, R.W.Ostendorf, S.Schadmand, O.Scholten, R.S.Simon, R.G.E.Timmermans, M.Volkerts, H.W.Wilschut

Dynamical Effects in Proton-Proton Bremsstrahlung for Non-Coplanar Geometries

NUCLEAR REACTIONS 1H(polarized p, pγ), E=190 MeV; measured σ(θ), analyzing power. Two-arm photon spectrometer, comparisons with model predictions.

doi: 10.1016/S0370-2693(00)00130-1
Citations: PlumX Metrics


2000KO31      Phys.Rev. C62, 015205 (2000)

A.Yu.Korchin, O.Scholten

Photoproduction of Electron-Positron Pairs on the Proton in the Resonance Region

NUCLEAR REACTIONS 1H(γ, e+e-), E=320, 700 MeV; calculated σ(θ), response functions, Bethe-Heitler contribution, resonance effects. Comparisons with data.

doi: 10.1103/PhysRevC.62.015205
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2000KO34      Phys.Rev. C62, 025203 (2000)

S.Kondratyuk, O.Scholten

Dressing the Nucleon in a Dispersion Approach

doi: 10.1103/PhysRevC.62.025203
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2000KO40      Nucl.Phys. A677, 396 (2000)

S.Kondratyuk, O.Scholten

Compton Scattering in a Unitary Approach with Causality Constraints

NUCLEAR REACTIONS 1n, 1H(γ, γ'), E=0-400 MeV; calculated Compton scattering form factors, partial wave amplitudes, pion-loop corrections. K-matrix formalism.

doi: 10.1016/S0375-9474(00)00307-9
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2000ME14      Phys.Lett. 481B, 171 (2000)

J.G.Messchendorp, J.C.S.Bacelar, M.J.van Goethem, M.N.Harakeh, M.Hoefman, H.Huisman, N.Kalantar-Nayestanaki, A.Yu.Korchin, H.Lohner, R.W.Ostendorf, S.Schadmand, O.Scholten, M.Volkerts, H.W.Wilschut, R.S.Simon

Cross Sections and Electromagnetic Response Functions for Radiative Proton Capture in pd → 3He + e+e-

NUCLEAR REACTIONS 2H(p, ee+), (p, γ), E=190 MeV; measured σ(θ); deduced electromagnetic response functions, possible role of Δ resonance. Comparison with model predictions.

doi: 10.1016/S0370-2693(00)00441-X
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1999HU15      Phys.Rev.Lett. 83, 4017 (1999)

H.Huisman, J.C.S.Bacelar, M.J.van Goethem, M.N.Harakeh, M.Hoefman, N.Kalantar-Nayestanaki, H.Lohner, J.G.Messchendorp, R.W.Ostendorf, S.Schadmand, O.Scholten, R.G.E.Timmermans, R.Turrisi, M.Volkerts, H.W.Wilschut, R.S.Simon, A.Kugler, V.Wagner

High-Precision Proton-Proton Bremsstrahlung Measurements below the Pion-Production Threshold

NUCLEAR REACTIONS 1H(polarized p, pγ), E=190 MeV; measured σ(θ), analyzing powers in coplanar kinematics. Comparison with calculations.

doi: 10.1103/PhysRevLett.83.4017
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1999KO05      Phys.Rev. C59, 1070 (1999)

S.Kondratyuk, O.Scholten

Consistent Off-Shell πNN Vertex and Nucleon Self-Energy

doi: 10.1103/PhysRevC.59.1070
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1999KO12      Phys.Rev. C59, 1890 (1999); Comment Phys.Rev. C63, 019801 (2001)

A.Yu.Korchin, D.Van Neck, O.Scholten, M.Waroquier

Radiative Proton-Deuteron Capture in a Gauge Invariant Relativistic Model

NUCLEAR REACTIONS 2H(polarized p, γ), E=100-500 MeV; calculated σ(θ), Ay(θ), tensor analyzing powers. 3He(e, e'p), (e, e'd), E=390, 560 MeV; calculated σ(E, θ). Gauge invariant relativistic model. Comparison with data.

doi: 10.1103/PhysRevC.59.1890
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1999MA78      Few-Body Systems 26, 197 (1999)

G.H.Martinus, O.Scholten, J.Tjon

Proton-Proton Virtual Bremsstrahlung in a Relativistic Convariant Model

NUCLEAR REACTIONS 1H(p, p'ee+), E=190, 400 MeV; calculated structure functions; deduced role of negative energy states, two-body currents. Relativistic covariant model.

doi: 10.1007/s006010050114
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1999ME22      Phys.Rev.Lett. 83, 2530 (1999)

J.G.Messchendorp, J.C.S.Bacelar, M.J.van Goethem, M.N.Harakeh, M.Hoefman, H.Huisman, N.Kalantar-Nayestanaki, H.Lohner, R.W.Ostendorf, S.Schadmand, O.Scholten, M.Volkerts, H.W.Wilschut, R.S.Simon

First Determination of the Nucleon-Nucleon Response Functions in the Timelike Region

NUCLEAR REACTIONS 1H(polarized p, p'ee+), E=190 MeV; measured σ(θ); deduced average transverse, longitudinal response functions. Comparison with model predictions.

doi: 10.1103/PhysRevLett.83.2530
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1999SC34      Eur.Phys.J. A 6, 211 (1999)

O.Scholten, A.Yu.Korchin

Q2-Dependence of the Drell-Hearn-Gerasimov Integral

NUCLEAR REACTIONS 1n, 1H(γ, X), E=200-800 MeV; calculated photoabsorption σ; deduced resonance contributions. Effective-Lagrangian model.

doi: 10.1007/s100500050336
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1998KO04      Phys.Lett. 418B, 20 (1998)

S.Kondratyuk, G.Martinus, O.Scholten

Electromagnetic Off-Shell Effects in Proton-Proton Bremsstrahlung

NUCLEAR REACTIONS 1H(polarized p, pγ), E=280 MeV; analyzed bremsstrahlung σ(θ1, θ2, θ(γ)), A(y)(θ(γ)); deduced off-shell electromagnetic form factor effects.

doi: 10.1016/S0370-2693(97)01471-8
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1998KO31      Phys.Rev. C58, 1098 (1998)

A.Yu.Korchin, O.Scholten

Nucleon Polarizabilities in Virtual Compton Scattering

doi: 10.1103/PhysRevC.58.1098
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1998KO53      Phys.Lett. 438B, 1 (1998)

A.Yu.Korchin, O.Scholten, R.G.E.Timmermans

Pion and Photon Couplings of N* Resonances from Scattering on the Proton

NUCLEAR REACTIONS 1H(π, π), (γ, π), E < 800 MeV; 1H(γ, γ), E=200-500 MeV; analyzed phase shifts, σ(θ); deduced resonance coupling features.

doi: 10.1016/S0370-2693(98)01041-7
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1998KO60      Phys.Lett. 441B, 17 (1998)

A.Yu.Korchin, D.Van Neck, M.Waroquier, O.Scholten, A.E.L.Dieperink

Production of e+e- Pairs in Proton-Deuteron Capture to 3He

NUCLEAR REACTIONS 2H(p, γ), (p, ee+), E=190, 350 MeV; calculated response functions, σ(θ); deduced time-like form factors influence. 3He(γ, p), E < 400 MeV; calculated σ(E, θ).

doi: 10.1016/S0370-2693(98)01197-6
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1998MA44      Phys.Rev. C58, 686 (1998)

G.H.Martinus, O.Scholten, J.A.Tjon

Meson Exchange and Δ Isobar Currents in Proton-Proton Bremsstrahlung

NUCLEAR REACTIONS 1H(p, pγ), E=100-400 MeV; calculated σ(θ), A(y)(θ); deduced meson exchange, Δ isobar excitation contributions.

doi: 10.1103/PhysRevC.58.686
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1997KO18      Phys.Lett. 402B, 1 (1997)

A.Yu.Korchin, O.Scholten, F.de Jong

Lepton-Pair Production in Virtual Compton Scattering Off the Proton

doi: 10.1016/S0370-2693(97)00389-4
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1997MA30      Phys.Lett. 402B, 7 (1997)

G.H.Martinus, O.Scholten, J.A.Tjon

Relativistic Description of Proton-Proton Bremsstrahlung

NUCLEAR REACTIONS 1H(p, γ), (polarized p, γ), E=280 MeV; analyzed σ(θ1, θ2, θγ), analyzing power vs θ.

doi: 10.1016/S0370-2693(97)00466-8
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1997MA66      Phys.Rev. C56, 2945 (1997)

G.H.Martinus, O.Scholten, J.A.Tjon

Effects of Relativity in Proton-Proton Bremsstrahlung

NUCLEAR REACTIONS 1H(polarized p, pγ), E=190, 280 MeV; analyzed σ(θ(γ)), A(y)(θ(γ)); deduced bremsstrahlung negative-energy states role, retardation effects.

doi: 10.1103/PhysRevC.56.2945
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1996KO19      Nucl.Phys. A602, 423 (1996)

A.Yu.Korchin, O.Scholten, D.Van Neck

Low-Energy Theorems for Virtual Nucleon-Nucleon Bremsstrahlung; Formalism and results

NUCLEAR REACTIONS 1H, 1n(p, γ), E=280 MeV; calculated virtual bremsstrahlung σ, response function, anisotropy coefficient vs photon invariant mass.

doi: 10.1016/0375-9474(96)00095-4
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1996SC30      Phys.Lett. 384B, 13 (1996)

O.Scholten, A.Yu.Korchin, V.Pascalutsa, D.Van Neck

Pion and Photon Induced Reactions on the Nucleon in a Unitary Model

doi: 10.1016/0370-2693(96)00825-8
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1996WU06      Phys.Rev. C54, 1208 (1996)

H.C.Wu, J.N.Ginocchio, A.E.L.Dieperink, O.Scholten

Double Charge Exchange on Te Isotopes in the Generalized Seniority Scheme

NUCLEAR STRUCTURE 128,130Te; calculated double IAS, ground state double charge exchange transition σ leading to 128,130Xe. Generalized seniority scheme, pion double charge exchange reactions.

doi: 10.1103/PhysRevC.54.1208
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1995HE03      Nucl.Phys. A582, 568 (1995)

V.Herrmann, K.Nakayama, O.Scholten, H.Arellano

Proton-Proton Bremsstrahlung and the Off-Shell Behavior of the NN Interaction

NUCLEAR REACTIONS 1H(polarized p, γ), E=280 MeV; calculated bremsstrahlung σ(θ), polarization observables, σ(θ1, θ2); deduced NN-interaction off-shell behavior features.

doi: 10.1016/0375-9474(94)00474-2
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1995KO02      Nucl.Phys. A581, 493 (1995)

A.Yu.Korchin, O.Scholten

Dilepton Production in Nucleon-Nucleon Collisions and the Low-Energy Theorem

doi: 10.1016/0375-9474(94)00457-X
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1995PA31      Nucl.Phys. A591, 658 (1995)

V.Pascalutsa, O.Scholten

On the Structure of the γNΔ Vertex: Compton scattering in the Δ(1232) region and below

doi: 10.1016/0375-9474(95)00301-G
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1994DE35      Phys.Lett. 333B, 1 (1994)

F.de Jong, K.Nakayama, V.Herrmann, O.Scholten

The Δ-Isobar and Proton-Proton Bremsstrahlung

NUCLEAR REACTIONS 1H(p, γ), E=280 MeV; calculated σ(θ1, θ2, θγ), analyzing power vs θγ bremsstrahlung; deduced Δ-isobar role.

doi: 10.1016/0370-2693(94)90998-9
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1994VA17      Nucl.Phys. A574, 643 (1994)

D.Van Neck, A.E.L.Dieperink, O.Scholten

Dilepton Production from Virtual Bremsstrahlung Induced by Proton Capture

NUCLEAR REACTIONS 1n(p, e+e-), E=200 MeV; calculated four structure functions. 11B(p, e+e-), E=98 MeV; calculated longitudinal, transverse conversion factor. Dilepton production, impulse approximation.

doi: 10.1016/0375-9474(94)90952-0
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1993WO06      Phys.Lett. 312B, 372 (1993)

A.Wolf, O.Scholten, R.F.Casten

F-Spin Purity of 2+1 States in Even-Even Nuclei

NUCLEAR STRUCTURE 110Pd, 152Sm, 154Gd, 168Er, 184W, 130,132Ba, 186,192Os, 146,148Ce, 150Nd, 192,194,196Pt, 170Yb, 180Hf; analyzed g factor data; deduced F-spin purity upper limits.

doi: 10.1016/0370-2693(93)90969-O
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1992BO13      Phys.Rev. C45, 2616 (1992)

G.D.Bosveld, A.E.L.Dieperink, O.Scholten

Slow Proton Production in Semi-Inclusive Deep-Inelastic Neutrino Scattering on Hydrogen and Deuterium

NUCLEAR REACTIONS 1,2H(ν, pX), (ν-bar, pX), E not given; calculated slow proton production σ. Spectator diquark fragmentation, nuclear spectators emission.

doi: 10.1103/PhysRevC.45.2616
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1992DO07      Phys.Rev. C45, 2795 (1992)

J.Dobes, P.Navratil, O.Scholten

Comparison of Two Approaches to Microscopy of the Interacting Boson Model

NUCLEAR STRUCTURE Z=50-82; calculated d, g, d' boson energies, pair structure coefficients, quadrupole, hexadecupole operator parameters. Interacting boson model, two microscopic approaches comparison.

doi: 10.1103/PhysRevC.45.2795
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1992PA02      Phys.Rev. C45, 284 (1992)

V.Paar, D.Vretenar, C.De Coster, K.Heyde, O.Scholten

Microscopic Approach to the U(6/4x4) Sub-Set Spin(BFF)(6) Hamiltonian of the Interacting Boson-Fermion-Fermion Model

NUCLEAR STRUCTURE 206Hg, 206Tl, 206Pb; calculated levels. Interacting boson-fermion-fermion model.

doi: 10.1103/PhysRevC.45.284
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1991BO37      Phys.Lett. 264B, 11 (1991)

G.D.Bosveld, A.E.L.Dieperink, O.Scholten

Semi-Inclusive Cross Sections for Deep-Inelastic Neutrino Scattering on Hydrogen and Deuterium

NUCLEAR REACTIONS 2,1H(ν, X), (ν-bar, X), E not given; calculated low energy proton production in deep-inelastic neutrino scattering.

doi: 10.1016/0370-2693(91)90694-L
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1991BO39      Phys.Lett. 269B, 1 (1991)

H.F.Boersma, R.Malfliet, O.Scholten

Compressibility of Nuclei in Relativistic Mean Field Theory

NUCLEAR STRUCTURE 16O, 48,40Ca, 90Zr, 114Sn, 208Pb; calculated compressibilities, anharmonicity coefficients, mass parameters, isoscalar giant monopole resonance frequencies. Relativistic mean field theory.

doi: 10.1016/0370-2693(91)91441-W
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1991WO01      Phys.Rev. C43, 2279 (1991)

A.Wolf, O.Scholten, R.F.Casten

Analytic Formula for B(E2) Values in Even-Even Nuclei with A > 60

NUCLEAR STRUCTURE A>60; calculated B(E2), even-even nuclei. Analytic formula.

doi: 10.1103/PhysRevC.43.2279
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1990CH29      Phys.Rev. C42, 221 (1990)

W.-T.Chou, W.A.Olivier, Wm.C.McHarris, O.Scholten

Odd-Odd Interacting-Boson-Approximation Calculations: Experimental agreement for doubly decoupled and highly distorted bands in 176-180Re

NUCLEAR STRUCTURE 177,179Os, 176,179,180,175,177Re; calculated levels. Interacting boson-fermion-fermion approximation.

doi: 10.1103/PhysRevC.42.221
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1990ME06      Phys.Rev. C41, 2386 (1990)

R.A.Meyer, O.Scholten, S.Brant, V.Paar

Mixed-Symmetry States in 144Nd: Semimicroscopic accounting within the cluster vibration model and its mapping into the interacting boson model

NUCLEAR STRUCTURE 144Nd; calculated levels, J, π, electric quadrupole, magnetic dipole moments, B(E2), B(M1). Cluster-vibration, interacting boson models.

doi: 10.1103/PhysRevC.41.2386
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1990ZA11      Z.Phys. A337, 293 (1990)

N.V.Zamfir, O.Scholten, P.von Brentano

E1 Calculations in the sdf-Interacting Boson Model

NUCLEAR STRUCTURE 152,154Sm, 158Gd; calculated B(λ), ratios. Interacting sdf-boson model, one-body, two-body terms.


1989BA01      Z.Phys. A332, 29 (1989)

A.F.Barfield, P.von Brentano, A.Dewald, K.O.Zell, N.V.Zamfir, D.Bucurescu, M.Ivascu, O.Scholten

Evidence for the Two-Body Nature of the E1 Transition Operator in the sdf-Interacting Boson Model

NUCLEAR REACTIONS 144Sm(α, α'), E=14 MeV; measured γ-spectra following Coulomb excitation. 144Sm levels deduced B(λ). sdf-interacting boson model.


1989DI03      Phys.Lett. 220B, 351 (1989)

K.-G.Dietrich, F.Humbert, A.Richter, B.A.Brown, A.A.Kuliev, O.Scholten

Magnetic Dipole Strength Distribution at High Excitation Energies in Deformed Nuclei

NUCLEAR REACTIONS 156Gd, 168Er(e, e'), E=25-40 MeV; measured electron spectra. 156Gd, 168Er deduced B(λ), M1 strength distribution. Quasiparticle RPA.

doi: 10.1016/0370-2693(89)90886-1
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1989SC01      Z.Phys. A332, 1 (1989)

O.Scholten, H.C.Wu, A.E.L.Dieperink

The Even Mass N = 83 Isotones in the Generalized Seniority Scheme

NUCLEAR STRUCTURE 134Te, 136Xe, 138Ba, 140Ce, 142Nd, 144Sm, 146Gd, 140La, 142Pr, 144Pm, 146Eu; calculated levels. Interacting boson model, generalized seniority scheme.


1989UC01      Nucl.Phys. A503, 723 (1989)

T.Uchiyama, A.E.L.Dieperink, O.Scholten

Quark Exchange Effect on the Coulomb Energies of Three-Body Nuclei

NUCLEAR STRUCTURE 3H, 3He; calculated Coulomb energy, difference. 3He; calculated charge form factor; deduced quark exchange effects role. Quark cluster model.

doi: 10.1016/0375-9474(89)90437-5
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1989UC02      Phys.Lett. 233B, 31 (1989)

T.Uchiyama, A.E.L.Dieperink, O.Scholten

Final State Interactions and y-Scaling in Inclusive Electron Scattering

NUCLEAR STRUCTURE 4He; calculated scaling function. Inclusive electron scattering, final state interactions.

doi: 10.1016/0370-2693(89)90610-2
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1988AH01      Phys.Rev. C37, 1836 (1988)

A.Ahmad, G.Bomar, H.Crowell, J.H.Hamilton, H.Kawakami, C.F.Maguire, W.G.Nettles, R.B.Piercey, A.V.Ramayya, R.Soundranayagam, R.M.Ronningen, O.Scholten, P.H.Stelson

Coulomb Excitation of 144, 146, 148, 150Nd

NUCLEAR REACTIONS 144,146,148,150Nd(α, α'), E=10.5, 11 MeV; measured σ(Eα) following Coulomb excitation. 144,146,148,150Nd deduced B(E2), B(E3), hexadecapole transition matrix element. Enriched targets.

doi: 10.1103/PhysRevC.37.1836
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1988BA17      Ann.Phys.(New York) 182, 344 (1988)

A.F.Barfield, B.R.Barrett, J.L.Wood, O.Scholten

An Interacting Boson Model Description of Octupole States in Nuclei

NUCLEAR STRUCTURE 154Sm, 156,158Gd, 158,162Dy, 168Er, 172Yb, 178Hf, 182W; calculated levels, B(λ). Interacting boson model.

doi: 10.1016/0003-4916(88)90016-4
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1988CH20      Phys.Rev. C37, 2834 (1988)

W.-T.Chou, Wm.C.McHarris, O.Scholten

Deformed Odd-Odd 180,182,184Re Isotopes in the Interacting-Boson Model

NUCLEAR STRUCTURE 181,183,185Re, 181,183,185Os; calculated levels, μ, quadrupole moments, B(λ). Interacting boson fermion fermion approximation.

doi: 10.1103/PhysRevC.37.2834
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1988VA10      Phys.Rev. C37, 1624 (1988)

B.I.M.van der Cammen, A.E.L.Dieperink, O.Scholten, G.Wenes

Nonperipheral Effects in Medium Energy Proton Scattering on Collective Nuclear States

NUCLEAR REACTIONS 154Gd(p, p'), E not given; analyzed σ(θ). Glauber approximation plus interacting boson model.

doi: 10.1103/PhysRevC.37.1624
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1988WU01      Phys.Rev. C38, 1638 (1988)

H.C.Wu, A.E.L.Dieperink, O.Scholten, M.N.Harakeh, R.De Leo, M.Pignanelli, I.Morrison

E4 Properties in Deformed Nuclei and the sdg Interacting Boson Model

NUCLEAR REACTIONS 150Nd(p, p'), E=30.3 MeV; measured σ(Ep), σ(θ). 150Nd deduced B(E4) distribution. Interacting boson model.

NUCLEAR STRUCTURE 156Gd, 150Nd; calculated levels, B(λ). Interacting boson model.

doi: 10.1103/PhysRevC.38.1638
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1987AR02      Phys.Lett. 185B, 259 (1987)

A.Arima, A.Gelberg, O.Scholten

Coriolis Coupling in the Interacting Boson Fermion Model

NUCLEAR STRUCTURE 73As; calculated levels, J, π. Interacting boson fermion model.

doi: 10.1016/0370-2693(87)90996-8
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1987DI05      Nucl.Phys. A469, 173 (1987)

A.E.L.Dieperink, O.Scholten, D.D.Warner

Magnetic Dipole Transitions in Deformed Even-Even Nuclei

NUCLEAR STRUCTURE 152Sm, 154,156Gd, 160,162Dy, 166,168Er, 184W; calculated M1 matrix elements. Neutron-proton IBA model.

doi: 10.1016/0375-9474(87)90090-X
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1987OT01      Phys.Rev. C35, 328 (1987)

T.Otsuka, N.Yoshida, P.Van Isacker, A.Arima, O.Scholten

Shell-Model Evidence for the Exchange Term in the Interacting-Boson-Fermion Hamiltonian

NUCLEAR STRUCTURE 92Mo, 93Tc; calculated levels. Quadrupole pairing interaction, interacting boson-fermion Hamiltonian.

doi: 10.1103/PhysRevC.35.328
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1987SA03      Nucl.Phys. A462, 1 (1987)

H.Sawaga, O.Scholten, B.A.Brown, B.H.Wildenthal

Core Polarization Effects on Transition Densities in Medium-Heavy Nuclei

NUCLEAR STRUCTURE 134Te, 136Xe, 138Ba, 140Ce, 142Nd, 144Sm; calculated levels; 144Sm, 122Sn; calculated core polarization charges; 110Pd, 116,122Sn, 134Te, 136Xe, 138Ba, 140Ce, 142Nd, 144Sm, 146Gd, 148Dy, 150Er; calculated transition densities, B(E2); 110Pd, 116Sn, 134Te, 138Ba, 142Nd, 146Gd; calculated Coulomb form factors. Hartree-Fock-RPA method.

doi: 10.1016/0375-9474(87)90376-9
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1987SA51      Nucl.Phys. A474, 155 (1987)

H.Sagawa, A.Arima, O.Scholten

Nuclear Compression Modulus and Isotope Shifts of Pb Nuclei

NUCLEAR STRUCTURE 196,197,198,199,200,201,202,203,204,205,206,207,209,210,211,212,213,214,215Pb; calculated isotope shifts, B(E2) sum values. Perturbative method, giant resonance effects.

doi: 10.1016/0375-9474(87)90198-9
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1987WU02      Phys.Lett. 187B, 205 (1987)

H.C.Wu, A.E.L.Dieperink, O.Scholten

Magnetic Dipole Properties in the SU(3) Limit of IBA-2 with L=0, 2 and 4 Bosons

NUCLEAR STRUCTURE 156Gd; calculated g-factors. IBA model.

doi: 10.1016/0370-2693(87)91081-1
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1986SC20      Phys.Rev. C34, 601 (1986)

O.Scholten, H.Toki

(p, π-) Continuum Spectra at Intermediate Energy in the Local Fermi Gas Model

NUCLEAR REACTIONS 42,48Ca, 90Zr(p, π-), E=200, 400 MeV; calculated σ. Local Fermi gas model.

doi: 10.1103/PhysRevC.34.601
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1986SC30      Phys.Rev. C34, 1962 (1986)

O.Scholten, R.M.Ronningen, A.Y.Ahmed, G.O.Bomar, H.L.Crowell, J.H.Hamilton, H.Kawakami, C.F.Maguire, W.G.Nettles, R.B.Piercey, A.V.Ramayya, R.Soundranayagam, P.H.Stelson

Mass Dependence of Effective Charges in the Interacting-Boson Model

NUCLEAR REACTIONS 144,146,148,150Nd(α, α'), E not given; measured Coulomb excitation. 144,146,148,150Nd levels deduced B(E2). Magnetic spectrometer. Interacting boson model.

NUCLEAR STRUCTURE 142,144,146,148,150Nd; calculated B(E2), effective charges. Interacting boson model.

doi: 10.1103/PhysRevC.34.1962
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1985CA03      Phys.Rev.Lett. 54, 881 (1985): Erratum Phys.Rev.Lett. 54, 1736 (1985)

J.A.Carr, F.Petrovich, R.J.Philpott, M.J.Threapleton, O.Scholten, H.McManus

Inelastic Proton Scattering as a Test of the New Collective - ' Current ' M1 Mode in Deformed Nuclei

NUCLEAR REACTIONS 156Gd(p, p'), E=200 MeV; 156Gd(e, e'), E=40 MeV; calculated σ(θ), transition densities, t-interaction components, transverse magnetic form factors vs θ, momentum transfer. 156Gd deduced M1 transitions character. Born approximation.

doi: 10.1103/PhysRevLett.54.881
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1985JO01      Nucl.Phys. A438, 15 (1985)

J.Jolie, P.Van Isacker, K.Heyde, J.Moreau, G.Van Landeghem, M.Waroquier, O.Scholten

Multilevel Description of the Rh Isotopes in the Interacting Boson-Fermion Model

NUCLEAR STRUCTURE 101,103,105,107,109Rh; calculated levels, B(λ), C2S. Interacting boson-fermion model.

doi: 10.1016/0375-9474(85)90116-2
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1985SA29      Phys.Lett. 159B, 228 (1985)

H.Sagawa, B.A.Brown, O.Scholten

Shell-Model Calculations with a Skyrme-Type Effective Interaction

NUCLEAR STRUCTURE 18O, 38,36Ar, 112,116,120Sn; calculated levels. Shell model, Skyrme type effective interaction.

doi: 10.1016/0370-2693(85)90240-0
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1985SC07      Nucl.Phys. A438, 41 (1985)

O.Scholten, K.Heyde, P.Van Isacker, J.Jolie, J.Moreau, M.Waroquier, J.Sau

Mixed-Symmetry States in the Neutron-Proton Interacting Boson Model

NUCLEAR STRUCTURE 98,100,102,104,106,108,110,112,114,116,118,120,122,124,126Pd, 186,188,190,192,196,198Pt; calculated levels, F-spin vector reduced matrix elements. 148,150,152,154,156Sm; calculated levels, B(λ), F-spin vector reduced matrix elements. 156,158Gd, 168Er; calculated levels. Interacting boson model, different dynamical symmetries.

doi: 10.1016/0375-9474(85)90118-6
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1985SC11      Phys.Rev. C32, 653 (1985)

O.Scholten, H.Toki, J.Aichelin, A.Bonasera, R.Kaps, H.Sarafian

Microscopic Description of the (p, π-) Continuum at Intermediate Proton Energy

NUCLEAR REACTIONS 42Ca(p, π-), E ≈ 200 MeV; calculated σ(E(π), θ(π)). Standard pion production model.

doi: 10.1103/PhysRevC.32.653
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1985SC18      Phys.Rev.Lett. 55, 1866 (1985)

O.Scholten, K.Heyde, P.Van Isacker

Distribution of Collective Magnetic Multipole Strength as a Measure of Neutron-Proton Symmetry Breaking

NUCLEAR STRUCTURE 156Gd; calculated levels, B(M1), B(M3). Interacting boson model, SU(3) limit.

doi: 10.1103/PhysRevLett.55.1866
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1985SC21      Phys.Lett. 161B, 13 (1985)

O.Scholten, Z.R.Yu

Double Beta Decay in the Interacting Boson Approximation

RADIOACTIVITY 128,130Te(2β); calculated Gamow-Teller matrix elements; deduced hindrance, nuclear deformation connection. Interacting boson approximation.

doi: 10.1016/0370-2693(85)90598-2
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1985SC24      Phys.Rev. C32, 1729 (1985)

O.Scholten, K.Heyde, P.Van Isacker, T.Otsuka

Mixed-Symmetry Interpretation of some Low-Lying Bands in Deformed Nuclei

NUCLEAR STRUCTURE 156Gd; calculated band head energies, B(λ). Mixed symmetry interpretation.

doi: 10.1103/PhysRevC.32.1729
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1984BO09      Phys.Lett. 137B, 27 (1984)

D.Bohle, A.Richter, W.Steffen, A.E.L.Dieperink, N.Lo Iudice, F.Palumbo, O.Scholten

New Magnetic Dipole Excitation Mode Studied in the Heavy Deformed Nucleus 156Gd by Inelastic Electron Scattering

NUCLEAR REACTIONS 156Gd(e, e'), E=25-56 MeV; measured σ(E(e')), σ(θ), M1 transition form factor. 158Gd(e, e'), E=25 MeV; measured σ(E(e')). 156Gd deduced collective magnetic dipole excitation mode, B(λ). 158Gd deduced evidence for collective magnetic dipole excitation mode.

doi: 10.1016/0370-2693(84)91099-2
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1984JA11      Phys.Lett. 141B, 281 (1984)

J.Janecke, O.Scholten

Isotope and Isomer Shifts of Samarium Isotopes in the Interacting Boson Model

NUCLEAR STRUCTURE 144,146,148,150,152Sm; calculated isotope, isomer shifts. Interacting boson model.

doi: 10.1016/0370-2693(84)90245-4
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1984SA16      Nucl.Phys. A423, 333 (1984)

M.Sambataro, O.Scholten, A.E.L.Dieperink, G.Piccitto

On Magnetic Dipole Properties in the Neutron-Proton IBA Model

NUCLEAR STRUCTURE 144,146,148,150,152,154,156,158,160,162,164,166,168,170,172,174,176Ba, 146,148,150,152,154,156,158,160,162,164,166,168,170,172,174,176,178Ce, 148,150,152,154,156,160,162,164,166,168,170,172,174,176,178,180Nd, 150,152,154,156,158,160,162,164,166,168,170,172,174,176,178,180,182Sm, 152,154,156,158,160,162,164,166,168,170,172,174,176,178,180,182,184Gd, 154,156,158,160,162,164,166,168,170,172,174,176,178,180,182,184,186Dy, 156,158,160,162,164,166,168,170,172,174,176,178,180,182,184,186,188Er, 158,160,162,164,166,168,170,172,174,176,178,180,182,184,186,188,190Yb, 160,162,164,166,168,170,172,174,176,178,180,182,184,186,188,190,192Hf, 162,164,166,168,170,172,174,176,178,180,182,184,186,188,190,192,194W, 164,166,168,170,172,174,176,178,180,182,184,186,188,190,192,194,196Os, 166,168,170,172,178,180,182,184,186,188,190,192,194W, 164,166,168,170,172,174,176,178,180,182,184,186,188,190,192,194,196,198Pt; calculated 2+ state g. 152Sm; calculated δ(E2/M1). Neutron-proton interacting boson model.

doi: 10.1016/0375-9474(84)90593-1
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1984SC22      Nucl.Phys. A424, 221 (1984)

O.Scholten, T.Ozzello

The Promethium Isotopes in the Interacting Boson-Fermion Model

NUCLEAR STRUCTURE 147,149,151,153Pm; calculated levels, B(λ), nucleon transfer spectroscopic factors C2S, μ. Interacting boson-fermion model.

doi: 10.1016/0375-9474(84)90183-0
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