NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = O.Scholten Found 129 matches. Showing 1 to 100. [Next]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
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
2012AB03 Nucl.Phys. A878, 37 (2012) 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
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
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
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
2010SH04 Phys.Rev. C 81, 015204 (2010) Associated photoproduction of K+ mesons off protons within a coupled-channels K-matrix approach
doi: 10.1103/PhysRevC.81.015204
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
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
2008SH25 Phys.Rev. C 78, 065201 (2008) Photoproduction of η mesons within a coupled-channels K-matrix approach
doi: 10.1103/PhysRevC.78.065201
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
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
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
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
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
2006US02 Phys.Rev. C 74, 015205 (2006) 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
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
2005US02 Phys.Rev. C 72, 025205 (2005) 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
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
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
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
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
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
2003KO57 Phys.Rev. C 68, 045206 (2003) 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
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
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
2002KO12 Phys.Rev. C65, 038201 (2002) 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
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) 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
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
2001KO06 Nucl.Phys. A680, 175c (2001) Nucleon Dressing from Dispersion Relations
doi: 10.1016/S0375-9474(00)00412-7
2001KO22 Nucl.Phys. A684, 426c (2001) 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
2001KO46 Phys.Rev. C64, 024005 (2001) 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
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
2000KO31 Phys.Rev. C62, 015205 (2000) 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
2000KO34 Phys.Rev. C62, 025203 (2000) Dressing the Nucleon in a Dispersion Approach
doi: 10.1103/PhysRevC.62.025203
2000KO40 Nucl.Phys. A677, 396 (2000) 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
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
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
1999KO05 Phys.Rev. C59, 1070 (1999) Consistent Off-Shell πNN Vertex and Nucleon Self-Energy
doi: 10.1103/PhysRevC.59.1070
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
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
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
1999SC34 Eur.Phys.J. A 6, 211 (1999) 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
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
1998KO31 Phys.Rev. C58, 1098 (1998) Nucleon Polarizabilities in Virtual Compton Scattering
doi: 10.1103/PhysRevC.58.1098
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
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
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
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
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
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
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
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
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
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
1995KO02 Nucl.Phys. A581, 493 (1995) Dilepton Production in Nucleon-Nucleon Collisions and the Low-Energy Theorem
doi: 10.1016/0375-9474(94)00457-X
1995PA31 Nucl.Phys. A591, 658 (1995) On the Structure of the γNΔ Vertex: Compton scattering in the Δ(1232) region and below
doi: 10.1016/0375-9474(95)00301-G
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
1987SA51 Nucl.Phys. A474, 155 (1987) 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
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
1986SC20 Phys.Rev. C34, 601 (1986) (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
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
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
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
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
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
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
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
1985SC21 Phys.Lett. 161B, 13 (1985) 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
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
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
1984JA11 Phys.Lett. 141B, 281 (1984) 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
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
1984SC22 Nucl.Phys. A424, 221 (1984) 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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