NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = A.E.Dieperink Found 72 matches. 2013KO02 Phys.Rev. C 87, 014616 (2013) Nuclear Drell-Yan effect in a covariant model
doi: 10.1103/PhysRevC.87.014616
2012WA24 Phys.Rev. C 86, 015503 (2012) L.W.Wansbeek, S.Schlesser, B.K.Sahoo, A.E.L.Dieperink, C.J.G.Onderwater, R.G.E.Timmermans Charge radii of radium isotopes NUCLEAR MOMENTS 208,209,210,211,212,213,220,221,222,223,224,225,226,227,228,229,230,232Ra; analyzed optical isotope shifts from experiments at ISOLDE, CERN and at KVI; deduced King plots, charge radii. Relevance to atomic parity violation in a chain of Ra isotopes.Comparison with theoretical atomic structure calculations.
doi: 10.1103/PhysRevC.86.015503
2009DI11 Eur.Phys.J. A 42, 269 (2009) A.E.L.Dieperink, P.Van Isacker Shell corrections to a liquid-drop description of nuclear masses and radii NUCLEAR STRUCTURE Z=8-100; analyzed two-neutron and two-proton separation energies, radii, related features using extended liquid drop model with shell corrections. Comparison with quantities derived from 2003 mass evaluation.
doi: 10.1140/epja/i2009-10869-3
2007DI15 Eur.Phys.J. A 32, 11 (2007) A.E.L.Dieperink, P.Van Isacker The symmetry energy in nuclei and in nuclear matter
doi: 10.1140/epja/i2007-10360-3
2007LI54 Phys.Rev. C 76, 035503 (2007) C.-P.Liu, M.J.Ramsey-Musolf, W.C.Haxton, R.G.E.Timmermans, A.E.L.Dieperink Atomic electric dipole moments: The Schiff theorem and its corrections
doi: 10.1103/PhysRevC.76.035503
2006VA18 Int.J.Mod.Phys. E15, 1371 (2006) P.van Isacker, A.E.L.Dieperink The symmetry energy in nuclei and in nuclear matter
doi: 10.1142/S0218301306005034
2004KO41 Phys.Rev. C 70, 015207 (2004) Covariant propagator of the Rarita-Schwinger field in the nuclear medium
doi: 10.1103/PhysRevC.70.015207
2004VA05 Phys.Rev. C 69, 025802 (2004) E.N.E.van Dalen, A.E.L.Dieperink Bulk viscosity in neutron stars from hyperons
doi: 10.1103/PhysRevC.69.025802
2003DI12 Phys.Rev. C 68, 064307 (2003) A.E.L.Dieperink, Y.Dewulf, D.Van Neck, M.Waroquier, V.Rodin Nuclear symmetry energy and the neutron skin in neutron-rich nuclei
doi: 10.1103/PhysRevC.68.064307
2003VA06 Phys.Rev. C 67, 065807 (2003) E.N.E.van Dalen, A.E.L.Dieperink, J.A.Tjon Neutrino emission in neutron stars
doi: 10.1103/PhysRevC.67.065807
2002KO01 Phys.Rev. C65, 015208 (2002) C.L.Korpa, A.E.L.Dieperink, R.G.E.Timmermans Hyperon-Nucleon Scattering and Hyperon Masses in the Nuclear Medium
doi: 10.1103/PhysRevC.65.015208
2002RO27 Phys.Lett. 541B, 71 (2002) Electromagnetic Transitions between Giant Resonances within a Continuum-RPA Approach NUCLEAR STRUCTURE 90Nb, 208Bi; calculated radiative widths and branching ratios for E1 transitions between resonance states. Continuum-RPA approach.
doi: 10.1016/S0370-2693(02)02187-1
2002TI04 Phys.Rev. C65, 064007 (2002) R.G.E.Timmermans, A.Yu.Korchin, E.N.E.van Dalen, A.E.L.Dieperink Soft Electroweak Bremsstrahlung: Theorems and astrophysical relevance NUCLEAR REACTIONS 1n, 1H(n, nX), (n, pX), E not given; calculated electroweak bremsstrahlung amplitudes, matrix elements, axial-vector currents. 1n(n, nνν-bar), E at 50-300 MeV/c; calculated σ. Astrophysical implications discussed.
doi: 10.1103/PhysRevC.65.064007
1999DI09 Phys.Lett. 456B, 9 (1999) Photodisintegration of the Deuteron in the Few GeV Region using Asymptotic Amplitudes NUCLEAR REACTIONS 2H(γ, n), E=1-4 GeV; calculated σ(θ); deduced scaling behaviour. Covariant and gauge invariant approach. Comparison with data.
doi: 10.1016/S0370-2693(99)00430-X
1999KO02 Phys.Lett. 446B, 15 (1999) Pions in Isospin Asymmetric Matter and Nuclear Drell-Yan Scattering
doi: 10.1016/S0370-2693(98)01521-4
1999NA33 Eur.Phys.J. A 5, 417 (1999) Gauge Constraints and Electromagnetic Properties of Off-Shell Particles
doi: 10.1007/s100500050305
1998DI04 Nucl.Phys. A629, 290c (1998) Tagged Structure Functions in Semi-Inclusive Deep-Inelastic Scattering on Nuclear Targets
doi: 10.1016/S0375-9474(97)00702-1
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
1998VA07 Phys.Rev. C57, 2308 (1998) D.Van Neck, M.Waroquier, A.E.L.Dieperink, S.C.Pieper, V.R.Pandharipande Center-of-Mass Effects on the Quasihole Spectroscopic Factors in the 16O(e, e'p) Reaction NUCLEAR REACTIONS 16O(e, e'p), E not given; calculated spectroscopic factors; deduced center-of-mass effect. Variational Monte Carlo calculation.
doi: 10.1103/PhysRevC.57.2308
1997DI02 Phys.Rev. C55, 2665 (1997) Pions in the Nuclear Medium and Drell-Yan Scattering
doi: 10.1103/PhysRevC.55.2665
1997DI04 Phys.Lett. 397B, 20 (1997) Electromagnetic Form Factors of the Proton in the ' Unphysical ' Region from the γp → pe+e- Reaction NUCLEAR REACTIONS 1H(γ, X), E not given; calculated e+e--asymmetry vs E; deduced 1H form factor F1(q2, W2) in time-like region deduction possibility.
doi: 10.1016/S0370-2693(97)00153-6
1996VA04 Phys.Rev. C53, 2231 (1996) D.Van Neck, A.E.L.Dieperink, M.Waroquier Natural Orbitals, Overlap Functions, and Mean-Field Orbitals in an Exactly Solvable A-Body System NUCLEAR STRUCTURE A=3; A=10; A=100; calculated one-body density, natural orbitals characteristics. Nontrivial many-body system.
doi: 10.1103/PhysRevC.53.2231
1996VA11 Z.Phys. A355, 107 (1996) D.Van Neck, A.E.L.Dieperink, M.Waroquier Single-Particle Properties in an Exactly Solvable A-Body System NUCLEAR STRUCTURE A=10; calculated bound, continuum single particle overlap functions contribution to density, momentum distributions.
doi: 10.1007/s002180050085
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
1995SZ05 Nucl.Phys. A595, 307 (1995) A.Szczurek, G.D.Bosveld, A.E.L.Dieperink Slow Proton Production in Semi-Inclusive Deep Inelastic Scattering and the Pion Cloud in the Nucleon NUCLEAR REACTIONS 1H(ν, X), (ν-bar, X), E not given; calculated proton momentum distributions, semi-inclusive deep inelastic scattering.
doi: 10.1016/0375-9474(95)00390-3
1995VA03 Phys.Rev. C51, 1800 (1995) D.Van Neck, A.E.L.Dieperink, E.Moya de Guerra Spectral Function for Finite Nuclei in the Local-Density Approximation NUCLEAR STRUCTURE 16O, 208Pb, 40,48Ca, 90Zr; calculated momentum density, overlap, spectral functions, per particle kinetic, mean removal energies. Local density approximation.
doi: 10.1103/PhysRevC.51.1800
1994BO13 Phys.Rev. C49, 2379 (1994) G.D.Bosveld, A.E.L.Dieperink, A.G.Tenner Slow Proton Production in Deep-Inelastic Neutrino Scattering on Deuterium NUCLEAR REACTIONS 2H(ν, μ-X), (ν-bar, μ-X), E not given; calculated spectator, direct process, inclusive σ ratio for slow proton production vs Bjorken parameter x.
doi: 10.1103/PhysRevC.49.2379
1994DI02 Z.Phys. A348, 117 (1994) Semi-Inclusive Deep Inelastic Lepton Scattering in a Pion Cloud Model NUCLEAR STRUCTURE 3He; calculated semi-inclusive σ for deep-inelastic lepton scattering vs Bjorken parameter x, target recoil momentum. Pion cloud model. NUCLEAR REACTIONS 3He(ν-bar, μ-X), (ν-bar, μ+X), E not given; calculated σ ratio. Pion cloud model.
doi: 10.1007/BF01289599
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
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
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
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
1988DI10 Nucl.Phys. A489, 627 (1988) Quark Exchange in Quasi-Elastic Electron-Nucleus Scattering NUCLEAR STRUCTURE 2H, 4He; calculated longitudinal, transverse structure function. Quark exchange. NUCLEAR REACTIONS 4He(e, e'p), E not given; calculated spectroscopic function. Quark exchange.
doi: 10.1016/0375-9474(88)90113-3
1988MU11 Nucl.Phys. A483, 461 (1988) Quark Exchange Effects in Nuclei NUCLEAR STRUCTURE 2,3H, 3,4He; calculated nuclear, electromagnetic form factors.
doi: 10.1016/0375-9474(88)90079-6
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
1987DI04 Phys.Lett. 189B, 267 (1987) A.E.L.Dieperink, E.Moya de Guerra On Magnetic Dipole Form Factors in Deformed Nuclei NUCLEAR STRUCTURE 156Gd; calculated M1 form factor. Projected Hartree-Fock approximation, interacting boson model.
doi: 10.1016/0370-2693(87)91429-8
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
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
1986DE26 Phys.Lett. 179B, 322 (1986) L.C.De Winter, N.R.Walet, P.J.Brussaard, K.Allaart, A.E.L.Dieperink Collective Pair Structure of K = 0 and K = 1 Bands in Deformed Nuclei NUCLEAR STRUCTURE 156Gd; calculated level structure; deduced collective pair structure. Fermion pair description.
doi: 10.1016/0370-2693(86)90485-5
1986WE12 Nucl.Phys. A459, 631 (1986) G.Wenes, J.N.Ginocchio, A.E.L.Dieperink, B.van der Cammen Algebraic Treatment of Multistep Exciation Processes in Collective Nuclei. (III). Medium Energy Proton Scattering NUCLEAR REACTIONS 154Sm(p, p'), E=800 MeV; calculated σ(θ). Glauber theory, collective state excitation, channel coupling.
doi: 10.1016/0375-9474(86)90165-X
1985CI06 Phys.Lett. 164B, 236 (1985) Onset of Static Quadrupole Deformation in the Light Actinides NUCLEAR STRUCTURE A ≈ 220; analyzed E2 systematics; deduced spherical to deformed shape transition.
doi: 10.1016/0370-2693(85)90316-8
1985WA27 Phys.Lett. 163B, 1 (1985) N.R.Walet, P.J.Brussaard, A.E.L.Dieperink Semiclassical Treatment of the M1-Mode in IBA-2 NUCLEAR STRUCTURE 156Gd; calculated M1 level excitation. Interacting boson model, semi-classical approximation.
doi: 10.1016/0370-2693(85)90180-7
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
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
1984SC42 Phys.Lett. 149B, 279 (1984) O.Scholten, A.E.L.Dieperink, K.Heyde, P.Van Isacker M3 Transitions in the Interacting Boson Model NUCLEAR STRUCTURE 154Sm; calculated levels, B(λ), form factors. Neutron-proton interacting boson model.
doi: 10.1016/0370-2693(84)90406-4
1983DI12 Nuovo Cim. 76A, 377 (1983) Electron Scattering in the Interacting-Boson Model NUCLEAR STRUCTURE 144,148,150,152,154Sm; calculated 2+ state transition charge densities. Electron scattering data input, interacting boson model.
doi: 10.1007/BF02833734
1982BI02 Nucl.Phys. A379, 221 (1982) Description of Odd-A Nuclei in the Pt Region in the Interacting Boson-Fermion Model NUCLEAR STRUCTURE 185,187,189,191Ir, 185,187,189,191,193Pt, 185,187,189,191,193,195Au; calculated levels. Interacting boson fermion model.
doi: 10.1016/0375-9474(82)90391-8
1982DI02 Phys.Lett. 109B, 1 (1982) Impact of Magnetic Electron Scattering on Spectroscopic Factors NUCLEAR STRUCTURE 51V, 87Sr; calculated valence orbit radius, neutron hole, particle number, nucleon pickup spectroscopic factor renormalization. Magnetic electron scattering data input.
doi: 10.1016/0370-2693(82)90448-8
1982DI12 Phys.Lett. 116B, 77 (1982) On Triaxial Features in the Neutron-Proton IBA NUCLEAR STRUCTURE 104Ru; calculated levels, B(E2), quadrupole moment vs spin. Interacting boson approximation, dynamical symmetry.
doi: 10.1016/0370-2693(82)90979-0
1982MO14 Nucl.Phys. A383, 264 (1982) M.A.Moinester, J.Alster, G.Azuelos, A.E.L.Dieperink Charge and Transition Densities of Samarium Isotopes in the Interacting Boson Model NUCLEAR STRUCTURE 144,148,150,152,154Sm; calculated transition charge densities, B(E2). Interacting boson model.
doi: 10.1016/0375-9474(82)90452-3
1981HA14 Phys.Rev. C23, 2329 (1981) Isoscalar Dipole Resonance: Form factor and energy weighted sum rule NUCLEAR REACTIONS 16O(α, α'), E=104 MeV; 208Pb(α, α'), E=172 MeV; analyzed σ(θ). DWBA analysis, hadron excitation of giant resonances, collective form factors.
doi: 10.1103/PhysRevC.23.2329
1981SA38 Phys.Lett. 107B, 249 (1981) G-Factors in the Neutron-Proton Interacting Boson Approximation NUCLEAR STRUCTURE Ru, Pd, Cd, Ba, Xe, Te; calculated 2+ state g vs neutron number. Proton-neutron interacting boson approximation.
doi: 10.1016/0370-2693(81)90822-4
1980BI06 Nucl.Phys. A344, 207 (1980) R.Bijker, A.E.L.Dieperink, O.Scholten, R.Spanhoff Description of the Pt and Os Isotopes in the Interacting Boson Model NUCLEAR STRUCTURE 196,194,192,190,188,186Pt, 194,192,190,188,186,184Os; calculated levels, B(E2), quadrupole moments, isomer shifts. Interacting boson model.
doi: 10.1016/0375-9474(80)90673-9
1980DI08 Phys.Rev.Lett. 44, 1747 (1980) A.E.L.Dieperink, O.Scholten, F.Iachello Classical Limit of the Interacting-Boson Model NUCLEAR STRUCTURE Nd, Sm, Gd, Os, Pt; calculated two-neutron separation energies, equilibrium shapes; deduced nature of shape transitions. Interacting boson model.
doi: 10.1103/PhysRevLett.44.1747
1980DI17 Nucl.Phys. A346, 125 (1980) On Shapes and Shape Phase Transitions in the Interacting Boson Model NUCLEAR STRUCTURE Gd, Sm, Pt, Os; calculated two-neutron separation energies; deduced interacting boson model limiting case, shape phase transition correspondence. SU(6) Hamiltonian, Gilmore, Feng algorithm technique.
doi: 10.1016/0375-9474(80)90492-3
1980VA09 Nucl.Phys. A342, 1 (1980) J.van Driel, R.Kamermans, R.J.de Meijer, A.E.L.Dieperink Investigation of the (3He, 2He) Reaction; Reaction Mechanism and Application to the Reaction on 28Si NUCLEAR REACTIONS 28Si(3He, 2p), E=52 MeV; measured σ(Ep1, Ep2, θ). 29Si deduced levels, J, π, L, S. DWBA analysis, normalization constant, optical model. Natural target.
doi: 10.1016/0375-9474(80)90503-5
1979FO05 Phys.Rev. C19, 1112 (1979) E0 Matrix Elements in 40,42,44Ca NUCLEAR STRUCTURE 40,42,44Ca; calculated E0 matrix elements. Wave functions from Gerace-Green calculation, (d, p) data.
doi: 10.1103/PhysRevC.19.1112
1978DI07 Phys.Lett. 76B, 135 (1978) A.E.L.Dieperink, F.Iachello, A.Rinat, C.Creswell Electron Scattering in the Interacting Boson Model NUCLEAR STRUCTURE 150Nd, 150,152,154Sm; calculated B(E2). Interacting boson model.
doi: 10.1016/0370-2693(78)90259-9
1978MO17 Phys.Rev. C18, 1596 (1978) E.Moya de Guerra, A.E.L.Dieperink Electromagnetic Form Factors of Odd-A Axially Symmetric Deformed Nuclei NUCLEAR STRUCTURE 25Mg, 181Ta; calculated magnetic form factors.
doi: 10.1103/PhysRevC.18.1596
1976DI09 Phys.Lett. 63B, 261 (1976) A.E.L.Dieperink, T.De Forest, Jr., I.Sick, R.A.Brandenburg Quasi-Elastic Electron Scattering on 3He NUCLEAR REACTIONS 3He(e, X); calculated quasi-elastic scattering. Impulse approximation.
doi: 10.1016/0370-2693(76)90258-6
1973LA11 Nucl.Phys. A203, 609 (1973) L.Lapikas, A.E.L.Dieperink, G.Box Elastic Electron Scattering from the Magnetization Distribution of 27Al NUCLEAR REACTIONS Mg, Al, Si(e, e'), E=35-95 MeV; measured σ(E; θ=180°). 27Al deduced parameters of nuclear magnetization distribution, ±.
doi: 10.1016/0375-9474(73)90367-9
1971DI01 Nucl.Phys. A160, 171 (1971) Second-Order Calculation of the Isotope Effect in the Ca Isotopes NUCLEAR STRUCTURE 40,42Ca; calculated isotope effect.
doi: 10.1016/0375-9474(70)90181-8
1971GL10 Ann.Phys.(N.Y.) 63, 134 (1971) P.W.M.Glaudemans, P.M.Endt, A.E.L.Dieperink Many-Particle Shell Model Calculation of Electromagnetic Transition Rates and Multipole Moments in A = 30-34 Nuclei NUCLEAR STRUCTURE 30P, 30Si, 31P, 31Si, 32S, 32P, 32Si, 33S, 33P, 34Cl, 34S; calculated transition strengths, μ, quadrupole moment, log ft, γ-mixing ratios. Many-particle shell model.
doi: 10.1016/0003-4916(71)90299-5
1971WR01 Phys.Rev. C4, 355 (1971) Microscopic Calculation of the Charge Form Factor of 4He NUCLEAR STRUCTURE 4He; calculated charge form factor. Nonlocal n-n interaction.
doi: 10.1103/PhysRevC.4.355
1970DI15 Lett.Nuovo Cim. 4, 395 (1970) Microscopic Description of the Charge Form Factor of 4He NUCLEAR REACTIONS 4He(e, e), E not given; calculated form factors.
doi: 10.1007/BF02824304
1969DI03 Phys.Letters 28B, 531(1969) A.E.L.Dieperink, P.W.M.Glaudemans Shell Model Description of States in 38K NUCLEAR STRUCTURE 38K calculated levels, T1/2, γ-branching.
doi: 10.1016/0370-2693(69)90045-8
1969GL02 Phys.Letters 28B, 645 (1969) P.M.W.Glaudemans, A.E.L.Dieperink, R.J.Keddy, P.M.Endt Shell-Model Calculation of Transition Probabilities Between A = 31 Even-Parity States RADIOACTIVITY 31S, 31Si; calculated log ft. NUCLEAR STRUCTURE 31P, 31S, 31Si; calculated levels, B(E2), B(M1). NUCLEAR MOMENTS 31P; calculated μ.
doi: 10.1016/0370-2693(69)90209-3
1968DI01 Nucl.Phys. A106, 177 (1968) A.E.L.Dieperink, P.J.Brussaard Shell-Model Calculations on 1f7/2(n) and 1f7/2(n+1)+1d3/2(-1) Configurations
doi: 10.1016/0375-9474(67)90836-6
1968DI08 Nucl.Phys. A116, 556 (1968) A.E.L.Dieperink, H.P.Leenhouts, P.J.Brussaard An Investigation of the Odd-Parity States of 40Ca with the Tabakin Interaction and the MSDI NUCLEAR STRUCTURE 40Ca; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0375-9474(68)90391-6
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