NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = W.H.Dickhoff Found 73 matches. 2023HE08 J.Phys.(London) G50, 060501 (2023) C.Hebborn, F.M.Nunes, G.Potel, W.H.Dickhoff, J.W.Holt, M.C.Atkinson, R.B.Baker, C.Barbieri, G.Blanchon, M.Burrows, R.Capote, P.Danielewicz, M.Dupuis, C.Elster, J.E.Escher, L.Hlophe, A.Idini, H.Jayatissa, B.P.Kay, K.Kravvaris, J.J.Manfredi, A.Mercenne, B.Morillon, G.Perdikakis, C.D.Pruitt, G.H.Sargsyan, I.J.Thompson, M.Vorabbi, T.R.Whitehead Optical potentials for the rare-isotope beam era
doi: 10.1088/1361-6471/acc348
2022YO02 Phys.Rev. C 105, 014622 (2022) K.Yoshida, M.C.Atkinson, K.Ogata, W.H.Dickhoff First application of the dispersive optical model to (p, 2p) reaction analysis within the distorted-wave impulse approximation framework NUCLEAR REACTIONS 40Ca(p, 2p), (e, e'p)39K, E=200 MeV; analyzed experimental data for differential cross sections; deduced spectroscopic factors using dispersive optical model (DOM) applied to the nonrelativistic distorted-wave impulse approximation (DWIA) framework, using several types of input for the p-p effective interactions: the Franey-Love interaction, the Melbourne g-matrix interaction with zero and mean density.
doi: 10.1103/PhysRevC.105.014622
2021AT02 Phys.Rev. C 104, 059802 (2021) M.C.Atkinson, W.H.Dickhoff, M.Piarulli, A.Rios, R.B.Wiringa Reply to "Comment on 'Reexamining the relation between the binding energy of finite nuclei and the equation of state of infinite nuclear matter'"
doi: 10.1103/PhysRevC.104.059802
2021AU02 Prog.Part.Nucl.Phys. 118, 103847 (2021) T.Aumann, C.Barbieri, D.Bazin, C.A.Bertulani, A.Bonaccorso, W.H.Dickhoff, A.Gade, M.Gomez-Ramos, B.P.Kay, A.M.Moro, T.Nakamura, A.Obertelli, K.Ogata, S.Paschalis, T.Uesaka Quenching of single-particle strength from direct reactions with stable and rare-isotope beams
doi: 10.1016/j.ppnp.2021.103847
2020AT01 Phys.Rev. C 101, 044303 (2020) M.C.Atkinson, M.H.Mahzoon, M.A.Keim, B.A.Bordelon, C.D.Pruitt, R.J.Charity, W.H.Dickhoff Dispersive optical model analysis of 208Pb generating a neutron-skin prediction beyond the mean field NUCLEAR REACTIONS 208Pb(p, X), (n, X), (p, p), (n, n), E=10-200 MeV; 208Pb(e, e), E=502 MeV; calculated reaction σ(E), differential σ(E, θ), analyzing powers Ay(θ) using dispersive optical model (DOM). Comparison with experimental data. NUCLEAR STRUCTURE 208Pb; calculated neutron and proton single-particle energy levels, charge density, orbital occupation and depletion numbers, spectroscopic factors, binding energies, momentum distributions of protons and neutrons. 40,48Ca, 208Pb; calculated proton and neutron point distributions, and neutron skins. Hartree-Fock and dispersive optical model (DOM) calculations. Comparison with experimental data. Relevance to nuclear equation of state.
doi: 10.1103/PhysRevC.101.044303
2020AT02 Phys.Rev. C 102, 044333 (2020) M.C.Atkinson, W.H.Dickhoff, M.Piarulli, A.Rios, R.B.Wiringa Reexamining the relation between the binding energy of finite nuclei and the equation of state of infinite nuclear matter NUCLEAR STRUCTURE 12C, 40,48Ca, 208Pb; calculated binding energies, binding energy as a function of radius in 12C, energy densities using a dispersive optical model. Comparison with ab initio self-consistent Green's-function calculations, and with experimental data. 8Be; calculated total binding-energy density, the kinetic-energy density, the two-body potential-energy density, and the three-body potential-energy density using Green's-function Monte Carlo method, with the Argonne-Urbana two- and three-body interactions. 12C; calculated three-body potential-energy densities for different chiral interactions and the Urbana-X. NUCLEAR REACTIONS 12C(p, p), (n, n), (polarized p, p), (polarized n, n), (p, X), (n, X), E<200 MeV; calculated differential σ(θ, E) and analyzing powers Ay(θ, E) for elastic scattering, proton and neutron total reaction σ(E) generated from the dispersive optical model (DOM). Comparison with experimental data.
doi: 10.1103/PhysRevC.102.044333
2020PR09 Phys.Rev.Lett. 125, 102501 (2020) C.D.Pruitt, R.J.Charity, L.G.Sobotka, M.C.Atkinson, W.H.Dickhoff Systematic Matter and Binding-Energy Distributions from a Dispersive Optical Model Analysis NUCLEAR STRUCTURE 16,18O, 40,48Ca, 58,64Ni, 112,124Sn, 208Pb; analyzed available bound-state anscattering data; deduced neutronn skins, the interplay of asymmetry, Coulomb, and shell effects on the skin thickness.
doi: 10.1103/PhysRevLett.125.102501
2020PR10 Phys.Rev. C 102, 034601 (2020) C.D.Pruitt, R.J.Charity, L.G.Sobotka, J.M.Elson, D.E.M.Hoff, K.W.Brown, M.C.Atkinson, W.H.Dickhoff, H.Y.Lee, M.Devlin, N.Fotiades, S.Mosby Isotopically resolved neutron total cross sections at intermediate energies NUCLEAR REACTIONS 16,18O, 58,64Ni, 103Rh, 112,124Sn(n, X), E=3-450 MeV; measured E(n), I(n), σ(E) by time-of-flight using wave-form-digitizer technology and BC-400 fast plastic scintillators at the WNR facility of the Los Alamos Neutron Science Center; deduced spectroscopic factors for valence proton and neutron levels through a dispersive optical model (DOM) analyses of σ(θ) data. 16,18O, 58,64Ni, 103Rh, 112,124Sn(p, p), (polarized p, p), (n, n), E=10-200 MeV; analyzed experimental σ(E), σ(θ, E), Ay(θ, E) data in literature; deduced dispersive optical model (DOM) parameters, charge radii and binding energies. Comparison with previous experimental measurements of σ(E) using analog methods.
doi: 10.1103/PhysRevC.102.034601
2019AT01 Phys.Lett. B 798, 135027 (2019) Investigating the link between proton reaction cross sections and the quenching of proton spectroscopic factors in 48Ca NUCLEAR REACTIONS 48Ca(E, X)47K, E not given; 40,48Ca(p, X), E<200 MeV; analyzed available data; deduced σ, spectral strength as a function of excitation energy using a nonlocal dispersive optical model (DOM).
doi: 10.1016/j.physletb.2019.135027
2018AT02 Phys.Rev. C 98, 044627 (2018) M.C.Atkinson, H.P.Blok, L.Lapikas, R.J.Charity, W.H.Dickhoff Validity of the distorted-wave impulse-approximation description of 40Ca(e, e'p)39K data using only ingredients from a nonlocal dispersive optical model NUCLEAR REACTIONS 40Ca(e, e'p)39K, E=299-532 MeV; measured Ep, Ip, electron spectra, spectral strengths as function of excitation energy, and spectral functions in parallel kinematics using high-resolution magnetic spectrometers for charged particle detection at the Medium Energy Accelerator at Nikhef, Amsterdam. Comparison with calculations using dispersive optical model (DOM) for distorted wave impulse-approximation (DWIA). 39K; deduced levels, J, π, spectroscopic factors. 40Ca(p, p), (n, n), E=10-100 MeV; analyzed σ(θ, E) and analyzing powers Ay(θ, E) by nonlocal DOM description. 40Ca(p, X), E<200 MeV; analyzed σ(E) by nonlocal DOM description. 40Ca; analyzed charge density using the DOM propagator, and compared with experimental data.
doi: 10.1103/PhysRevC.98.044627
2017DI03 J.Phys.(London) G44, 033001 (2017) W.H.Dickhoff, R.J.Charity, M.H.Mahzoon Novel applications of the dispersive optical model
doi: 10.1088/1361-6471/44/3/033001
2017MA76 Phys.Rev.Lett. 119, 222503 (2017) M.H.Mahzoon, M.C.Atkinson, R.J.Charity, W.H.Dickhoff Neutron Skin Thickness of 48Ca from a Nonlocal Dispersive Optical-Model Analysis NUCLEAR REACTIONS 48Ca(n, n), E not given; analyzed available data; deduced σ, σ(θ), neutron and proton numbers, and the charge distributions.
doi: 10.1103/PhysRevLett.119.222503
2017PO13 Eur.Phys.J. A 53, 178 (2017) G.Potel, G.Perdikakis, B.V.Carlson, M.C.Atkinson, W.H.Dickhoff, J.E.Escher, M.S.Hussein, J.Lei, W.Li, A.O.Macchiavelli, A.M.Moro, F.M.Nunes, S.D.Pain, J.Rotureau Toward a complete theory for predicting inclusive deuteron breakup away from stability NUCLEAR REACTIONS 93Nb(d, pn), E=10, 25.5 MeV; calculated σ(ln), σ(θn) assuming both elastic and nonelastic breakup. Compared with published calculations. 40,48,60Ca(d, pn), E=20, 40 MeV; calculated σ(Ep) vs En and vs ln using both elastic and nonelastic breakup and using Hussein-McVoy theory.
doi: 10.1140/epja/i2017-12371-9
2016DI12 Phys.Rev. C 94, 025802 (2016); Pub.Note Phys.Rev. C 94, 029901 (2016) D.Ding, A.Rios, H.Dussan, W.H.Dickhoff, S.J.Witte, A.Carbone, A.Polls Pairing in high-density neutron matter including short- and long-range correlations
doi: 10.1103/PhysRevC.94.025802
2015RO17 Phys.Rev. C 92, 044607 (2015) A.Ross, L.J.Titus, F.M.Nunes, M.H.Mahzoon, W.H.Dickhoff, R.J.Charity Effects of nonlocal potentials on (p, d) transfer reactions NUCLEAR REACTIONS 40Ca(p, d)39Ca, E=20, 35, 50 MeV; 40Ca(p, p), E=50 MeV; calculated σ(θ) distributions using nonlocal potential obtained from non-local dispersive optical model (DOM) and DOM-phase equivalent (PE), combined with DWBA. Comparison with Perey-Buck (PB) optical potential predictions, and with experimental data.
doi: 10.1103/PhysRevC.92.044607
2014CH08 Eur.Phys.J. A 50, 23 (2014), Erratum Eur.Phys.J. A 50, 64 (2014) R.J.Charity, W.H.Dickhoff, L.G.Sobotka, S.J.Waldecker Isospin dependence of nucleon correlations in ground-state nuclei NUCLEAR STRUCTURE 102,106,112,124,130,132Sn; calculated proton orbit strength function, spectroscopic factor. 154Sn; calculated proton hole spectroscopic factor. 132Sn, 208Pb; calculated neutron states above the core, spectroscopic factor. Dispersive optical model.
doi: 10.1140/epja/i2014-14023-0
2014DU15 Phys.Rev. C 90, 061603 (2014) H.Dussan, M.H.Mahzoon, R.J.Charity, W.H.Dickhoff, A.Polls Elastic nucleon-nucleus scattering as a direct probe of correlations beyond the independent-particle model NUCLEAR REACTIONS 40Ca(p, p), (n, n), E<200 MeV; analyzed scattering and structure data using the full nonlocal treatment of the dispersive optical model (DOM). Discussed application for inverse kinematics reactions.
doi: 10.1103/PhysRevC.90.061603
2014MA18 Phys.Rev.Lett. 112, 162503 (2014) M.H.Mahzoon, R.J.Charity, W.H.Dickhoff, H.Dussan, S.J.Waldecker Forging the Link between Nuclear Reactions and Nuclear Structure NUCLEAR REACTIONS 40Ca(n, n), (p, p), E<200 MeV; calculated σ, σ(θ), spectral strength. Comparison with experimental data.
doi: 10.1103/PhysRevLett.112.162503
2014RI02 Phys.Rev. C 89, 044303 (2014) Density and isospin-asymmetry dependence of high-momentum components NUCLEAR STRUCTURE 2H; calculated momentum distribution for neutrons and protons in asymmetric nuclear matter, ratio of the neutron, proton and nucleon momentum distributions to corresponding deuteron distribution at high momenta, density and isospin dependence, integrated single-particle strengths and kinetic energies for neutrons and protons. High-momentum components dominated by tensor correlations. Self-consistent Green's function (SCGF) ladder calculations and dilute Fermi gas (DFG) model.
doi: 10.1103/PhysRevC.89.044303
2011DU21 Phys.Rev. C 84, 044319 (2011) H.Dussan, S.J.Waldecker, W.H.Dickhoff, H.Muther, A.Polls Microscopic self-energy of 40Ca from the charge-dependent Bonn potential NUCLEAR STRUCTURE 40Ca; calculated spectral functions, single-particle levels, spectroscopic factors, natural orbits; comparison of microscopic CD Bonn Self-Energy and Dispersive Optical Model fit. 40Ca(n, n), E=0-100 MeV; calculated total and differential cross sections. Comparison with experimental data; analyzed non-locality of the imaginary part of the CD Bonn Self-energy.
doi: 10.1103/PhysRevC.84.044319
2011MU10 Phys.Rev. C 83, 064605 (2011) J.M.Mueller, R.J.Charity, R.Shane, L.G.Sobotka, S.J.Waldecker, W.H.Dickhoff, A.S.Crowell, J.H.Esterline, B.Fallin, C.R.Howell, C.Westerfeldt, M.Youngs, B.J.Crowe, III, R.S.Pedroni Asymmetry dependence of nucleon correlations in spherical nuclei extracted from a dispersive-optical-model analysis NUCLEAR REACTIONS 40,48Ca(n, n), E=11.9, 16.9 MeV; measured E(n), I(n), σ, σ(E, θ), time-of-flight spectra. 40Ca(n, n), E=9.9-85.0; 48Ca(n, n), E=7.97-16.9 MeV; 54Ca(n, n), E=5.5-26.0 MeV; 58,60Ni(n, n), E=4.5-24.0 MeV; 92Mo(n, n), E=7.0-30.4 MeV; 116,118Sn(n, n), E=9.95-24.0 MeV; 120Sn(n, n), E=9.94-16.91 MeV; 124Sn(n, n), E=11.0-24.0 MeV; 208Pb(n, n), E=4.0-185.0 MeV; 50Ti(p, p), E=6.0-65.0 MeV; 52Cr(p, p), E=10.77-39.9 MeV; 54Fe, 64Ni(p, p), E=9.69-65.0 MeV; 58Ni(p, p), E=7.0-192.0 MeV; 60Ni(p, p), E=7.0-178.0 MeV; 62Ni(p, p), E=8.02-156.0 MeV; 90Zr(p, p), E=5.57-185.0 MeV; 92Mo(p, p), E=12.5-49.45 MeV; 114Sn(p, p), E=30.4 MeV; 116Sn(p, p), E=16.0-61.4 MeV; 118,122,124Sn(p, p), E=16.0-49.35 MeV; 120Sn(p, p), E=9.8-156.0 MeV; 208Pb(p, p), E=9.0-200.0 MeV; analyzed total cross sections, σ(E, θ), single-particle levels, spectroscopic factors, occupation probabilities, mass dependence on cross section. Dispersal optical model (DOM) analysis.
doi: 10.1103/PhysRevC.83.064605
2011NG04 Phys.Rev. C 84, 044611 (2011) N.B.Nguyen, S.J.Waldecker, F.M.Nunes, R.J.Charity, W.H.Dickhoff Transfer reactions and the dispersive optical model NUCLEAR REACTIONS 40Ca(d, p), E=20, 56 MeV; 48Ca(d, p), E=2, 13, 19.3, 56 MeV; 132Sn(d, p), E=9.46 MeV; 208Pb(d, p), E=8, 20 MeV; analyzed optical potentials, σ(θ, E), spectroscopic factors. Test of dispersive optical potentials. Comparison with experimental data and with predictions of a standard global optical potential. Finite-range adiabatic (FR-ADWA) calculations in the range of closed-shell nuclei.
doi: 10.1103/PhysRevC.84.044611
2011WA24 Phys.Rev. C 84, 034616 (2011) S.J.Waldecker, C.Barbieri, W.H.Dickhoff Microscopic self-energy calculations and dispersive optical-model potentials NUCLEAR STRUCTURE 40,48,60Ca; calculated nucleon self energies, volume integrals, angular momentum dependence for the volume integrals, asymmetry dependence of the absorption for neutrons and protons. Dispersive optical model (DOM), and Faddeev-random-phase approximation (FRPA) method.
doi: 10.1103/PhysRevC.84.034616
2010BA36 Nucl.Phys. A834, 788c (2010) C.Barbieri, R.J.Charity, W.H.Dickhoff, L.G.Sobotka Toward a Global Dispersive Optical Model for the Driplines NUCLEAR REACTIONS 40Ca(n, n), E=9-185 MeV; 40Ca(p, p), E=17.6-200 MeV; 42,44Ca(p, p), E=21-65 MeV; 48Ca(p, p), E=8-200 MeV; calculated σ(θ), analyzing power. 40,48Ca calculated levels, J, widths, radii, spectroscopic factors; deduced dispersive optical model parameters. 58,60,62,64Ni(p, p), E not given; calculated σ(θ). Comparison with data.
doi: 10.1016/j.nuclphysa.2010.01.147
2010DI12 Phys.Rev. C 82, 054306 (2010) W.H.Dickhoff, D.Van Neck, S.J.Waldecker, R.J.Charity, L.G.Sobotka Nonlocal extension of the dispersive optical model to describe data below the Fermi energy NUCLEAR REACTIONS 40Ca(e, e'p), (p, 2p), E<150 MeV; calculated spectral functions, quasihole energies, spectroscopic factors, radii and charge density for proton orbits in 40Ca using dispersive-optical-model (DOM) analysis. Comparison with experimental data.
doi: 10.1103/PhysRevC.82.054306
2009RI06 Phys.Rev. C 79, 064308 (2009) Depletion of the nuclear Fermi sea
doi: 10.1103/PhysRevC.79.064308
2007CH72 Phys.Rev. C 76, 044314 (2007) R.J.Charity, J.M.Mueller, L.G.Sobotka, W.H.Dickhoff Dispersive-optical-model analysis of the asymmetry dependence of correlations in Ca isotopes NUCLEAR REACTIONS 40Ca(p, p), E=17.57-200.0 MeV; 42,44Ca(p, p), E=21.0-65.0 MeV; 48Ca(p, p), E=8.0-200.0 MeV; 40Ca(n, n), E=9.9-185.0 MeV; analyzed differential cross sections, angular distributions, polarization asymmetry, widths, rms radii and spectroscopic factors. Deduced optical-model parameters. 60Ca, 70Ca deduced prediction for particle stability.
doi: 10.1103/PhysRevC.76.044314
2006CH46 Phys.Rev.Lett. 97, 162503 (2006) R.J.Charity, L.G.Sobotka, W.H.Dickhoff Asymmetry Dependence of Proton Correlations NUCLEAR REACTIONS 40,48Ca(p, X), E=5-50 MeV; analyzed reaction σ. 40Ca(p, p), E=18-135 MeV; 48Ca(p, p), E=8-65 MeV; analyzed σ(θ), analyzing powers. 40,48Ca deduced proton states energies, widths, occupation probabilities, asymmetry dependence of proton correlations. Dispersive optical model. NUCLEAR STRUCTURE 40,48,60Ca; calculated proton single-particle level energies.
doi: 10.1103/PhysRevLett.97.162503
2005BA66 J.Phys.(London) G31, S1301 (2005) Self-consistent Green's function calculations of 16O at small missing energies NUCLEAR STRUCTURE 16O; calculated one-hole spectral function, level energies and configurations. Self-consistent Green's function approach.
doi: 10.1088/0954-3899/31/8/008
2005MU29 Phys.Rev. C 72, 054313 (2005) Pairing properties of nucleonic matter employing dressed nucleons
doi: 10.1103/PhysRevC.72.054313
2005RO28 Phys.Rev. C 72, 024320 (2005) Correlation effects on the nonmesonic weak decay of the Λ hyperon in nuclear matter
doi: 10.1103/PhysRevC.72.024320
2004BA61 Phys.Rev. C 70, 014606 (2004) C.Barbieri, C.Giusti, F.D.Pacati, W.H.Dickhoff Effects of nuclear correlations on the 16O(e, e'pN) reactions to discrete final states NUCLEAR REACTIONS 16O(e, e'np), (e, e'2p), E=855 MeV; calculated σ(E, θ); deduced sensitivity to short-range and long-range correlations.
doi: 10.1103/PhysRevC.70.014606
2004DI08 Prog.Part.Nucl.Phys. 52, 377 (2004) Self-consistent Greens's function method for nuclei and nuclear matter
doi: 10.1016/j.ppnp.2004.02.038
2004RO36 Phys.Rev. C 70, 044301 (2004) Correlation effects on Λ propagation in nuclear matter
doi: 10.1103/PhysRevC.70.044301
2003BA56 Phys.Rev. C 68, 014311 (2003) Extension of the random phase approximation including the self-consistent coupling to two-phonon contributions NUCLEAR STRUCTURE 16O; calculated levels, J, π, configurations. Extended RPA, coupling to two particle-hole phonons.
doi: 10.1103/PhysRevC.68.014311
2003DE10 Phys.Rev.Lett. 90, 152501 (2003) Y.Dewulf, W.H.Dickhoff, D.Van Neck, E.R.Stoddard, M.Waroquier Saturation of Nuclear Matter and Short-Range Correlations
doi: 10.1103/PhysRevLett.90.152501
2003RA16 Eur.Phys.J. A 17, 65 (2003) M.Radici, A.Meucci, W.H.Dickhoff Spectroscopic information from different theoretical descriptions of (un)polarized (e, e'p) reactions NUCLEAR REACTIONS 16O(e, e'p), (polarized e, e'p), E=high; analyzed σ(E, θ), polarization observables; deduced spectroscopic parameters. Two theoretical approaches considered.
doi: 10.1140/epja/i2002-10137-2
2002BA59 Phys.Rev. C65, 064313 (2002) Faddeev Treatment of Long-Range Correlations and the One-Hole Spectral Function of 16O NUCLEAR STRUCTURE 16O; calculated spectroscopic factors, one-hole spectral function, role of particle-particle and particle-hole phonons. Fadeev equations, iterative procedure.
doi: 10.1103/PhysRevC.65.064313
2002DI03 Acta Phys.Pol. B33, 65 (2002) Nuclear Equation of State and Spectral Functions
2002RA35 Phys.Rev. C66, 014613 (2002) M.Radici, W.H.Dickhoff, E.Roth Stoddard Consistency of Spectroscopic Factors from (e, e'p) Reactions at Different Momentum Transfers NUCLEAR REACTIONS 16O(e, e'p), E=90 MeV; analyzed σ(E, θ), asymmetry, structure functions; deduced spectroscopic factors.
doi: 10.1103/PhysRevC.66.014613
2001BA15 Phys.Rev. C63, 034313 (2001) Faddeev Description of Two-Hole-One-Particle Motion and the Single-Particle Spectral Function
doi: 10.1103/PhysRevC.63.034313
2000ST02 Phys.Lett. 474B, 33 (2000) R.Starink, M.F.van Batenburg, E.Cisbani, W.H.Dickhoff, S.Frullani, F.Garibaldi, C.Giusti, D.L.Groep, P.Heimberg, W.H.A.Hesselink, M.Iodice, E.Jans, L.Lapikas, R.De Leo, C.J.G.Onderwater, F.D.Pacati, R.Perrino, J.Ryckebusch, M.F.M.Steenbakkers, J.A.Templon, G.-M.Urciuoli, L.B.Weinstein Evidence for Short-Range Correlations in 16O NUCLEAR REACTIONS 16O(e, e'2p), E=580-585 MeV; measured σ(E), missing momentum spectra. 16O deduced short-range correlations.
doi: 10.1016/S0370-2693(99)01510-5
1999DI19 Phys.Rev. C60, 064319 (1999) W.H.Dickhoff, C.C.Gearhart, E.P.Roth, A.Polls, A.Ramos Phase Shifts and In-Medium Cross Sections for Dressed Nucleons in Nuclear Matter
doi: 10.1103/PhysRevC.60.064319
1998DI10 Phys.Rev. C58, 2807 (1998) Scattering of Dressed Nucleons in Nuclear Matter
doi: 10.1103/PhysRevC.58.2807
1998GI05 Phys.Rev. C57, 1691 (1998) C.Giusti, F.D.Pacati, K.Allaart, W.J.W.Geurts, W.H.Dickhoff, H.Muther Selectivity of the 16O(e, e'pp) Reaction to Discrete Final States NUCLEAR REACTIONS 16O(e, e'2p), E=475, 584, 855 MeV; calculated σ(E, θ); deduced final state selectivity.
doi: 10.1103/PhysRevC.57.1691
1998ON02 Phys.Rev.Lett. 81, 2213 (1998) C.J.G.Onderwater, K.Allaart, E.C.Aschenauer, Th.S.Bauer, D.J.Boersma, E.Cisbani, W.H.Dickhoff, S.Frullani, F.Garibaldi, W.J.W.Geurts, C.Giusti, D.L.Groep, W.H.A.Hesselink, M.Iodice, E.Jans, N.Kalantar-Nayestanaki, W.-J.Kasdorp, C.Kormanyos, L.Lapikas, J.J.van Leeuwe, R.De Leo, A.Misiejuk, H.Muther, F.D.Pacati, A.R.Pellegrino, R.Perrino, R.Starink, M.Steenbakkers, G.van der Steenhoven, J.J.M.Steijger, M.A.van Uden, G.M.Urciuoli, L.B.Weinstein, H.W.Willering Signatures for Short-Range Correlations in 16O Observed in the Reaction 16O(e, e'pp)14C NUCLEAR REACTIONS 16O(e, e'2p), E=584 MeV; measured σ(Ee, θ(e), Ep, θ(p)), missing momentum; deduced short-range correlations role.
doi: 10.1103/PhysRevLett.81.2213
1997PO01 Phys.Rev. C55, 810 (1997) A.Polls, M.Radici, S.Boffi, W.H.Dickhoff, H.Muther High-Momentum Proton Removal from 16O and the (e, e'p) Cross Section NUCLEAR REACTIONS 16O(e, e'p), E not given; calculated reduced σ vs missing momentum. Single-hole spectral function evaluated with short-range, tensor correlations.
doi: 10.1103/PhysRevC.55.810
1996GE01 Phys.Rev. C53, 2207 (1996) W.J.W.Geurts, K.Allaart, W.H.Dickhoff, H.Muther Spectroscopic Factors for Nucleon Knock-Out from 16O at Small Missing Energy NUCLEAR STRUCTURE 16O; calculated one-nucleon knock-out spectroscopic factors. Green's function formalism.
doi: 10.1103/PhysRevC.53.2207
1996GE03 Phys.Rev. C54, 1144 (1996) W.J.W.Geurts, K.Allaart, W.H.Dickhoff, H.Muther Two-Nucleon Spectral Function of 16O at High Momenta NUCLEAR STRUCTURE 16O; calculated two-nucleon spectral functions. NUCLEAR REACTIONS 16O(e, e'X), E=700 MeV; calculated longitudinal differential σ for 2p knockout. Plane wave approximation.
doi: 10.1103/PhysRevC.54.1144
1996GE09 Int.J.Mod.Phys. E5, 461 (1996) C.C.Gearhart, W.H.Dickhoff, A.Polls, A.Ramos Some Consequences of Dressing Nucleons
doi: 10.1142/S0218301396000220
1996RI01 Phys.Rev. C53, 201 (1996) G.A.Rijsdijk, W.J.W.Geurts, K.Allaart, W.H.Dickhoff Hole Spectral Function and Two-Particle-One-Hole Response Propagator NUCLEAR STRUCTURE 48Ca, 90Zr; calculated hole-state spectral functions. 47K, 89Y; calculated quasihole states spectroscopic factors.
doi: 10.1103/PhysRevC.53.201
1995MU09 Phys.Rev. C51, 3040 (1995) H.Muther, A.Polls, W.H.Dickhoff Momentum and Energy Distributions of Nucleons in Finite Nuclei Due to Short-Range Correlations NUCLEAR STRUCTURE 16O; calculated nucleon momentum, energy distributions. Short range correlations, realistic meson-exchange potential.
doi: 10.1103/PhysRevC.51.3040
1994CZ01 J.Phys.(London) G20, 425 (1994) P.Czerski, H.Muther, W.H.Dickhoff Effective Local Interactions and the Equation of State for Nuclear Matter and Finite Nuclei NUCLEAR STRUCTURE 16O; calculated binding energy per nucleon, two-nucleon density. Equation of state, effective nuclear interactions.
doi: 10.1088/0954-3899/20/3/004
1994GE04 Phys.Rev. C50, 514 (1994) W.J.W.Geurts, K.Allaart, W.H.Dickhoff Gamow-Teller (p, n) and (n, p) Strength in a Dressed Extended Random Phase Approximation NUCLEAR STRUCTURE 48Ca; calculated (p, n) Gamow-Teller transition strength. Dressed, extended RPA.
doi: 10.1103/PhysRevC.50.514
1994MU01 Phys.Rev. C49, R17 (1994) Single-Particle Spectral Function of 16O NUCLEAR STRUCTURE 16O; calculated single particle spectral function; deduced short range correlations role.
doi: 10.1103/PhysRevC.49.R17
1994PO07 Phys.Rev. C49, 3050 (1994) A.Polls, A.Ramos, J.Ventura, S.Amari, W.H.Dickhoff Energy Weighted Sum Rules for Spectral Functions in Nuclear Matter
doi: 10.1103/PhysRevC.49.3050
1993RI08 Phys.Rev. C48, 1752 (1993) G.A.Rijsdijk, W.J.W.Geurts, M.G.E.Brand, K.Allaart, W.H.Dickhoff Spin-Isospin Strength and Spectral Functions NUCLEAR REACTIONS 90Zr, 48Ca(p, n), (n, p), E not given; calculated Gamow-Teller, spin-dipole response functions. Dressed independent particle, RPA approaches.
doi: 10.1103/PhysRevC.48.1752
1992RI08 Nucl.Phys. A550, 159 (1992) G.A.Rijsdijk, K.Allaart, W.H.Dickhoff Hole Spectral Functions and Collective Excitations NUCLEAR STRUCTURE 48Ca, 90Zr; calculated spectral strength distributions, occupation probabilities. Large configuration space, realistic G-matrix interaction.
doi: 10.1016/0375-9474(92)91137-E
1991BR22 Nucl.Phys. A531, 253 (1991) M.G.E.Brand, G.A.Rijsdijk, F.A.Muller, K.Allaart, W.H.Dickhoff Fragmentation of Single-Particle Strength and the Validity of the Shell Model NUCLEAR REACTIONS 90Zr, 48Ca(e, e'p), E not given; calculated spectral functions, several l-values; deduced shell model validity features. Green function Dyson equation.
doi: 10.1016/0375-9474(91)90612-A
1990BR03 Nucl.Phys. A509, 1 (1990) M.G.E.Brand, K.Allaart, W.H.Dickhoff Nuclear Response Beyond Mean Field Theory NUCLEAR STRUCTURE 48Ca; calculated levels, transition densities, currents, B(λ), electric quadrupole, dipole resonance strength functions. 48Sc; calculated levels, Gamow-Teller resonance strength functions. Extended RPA. NUCLEAR REACTIONS 48Ca(e, e'), E not given; calculated form factor. Extended RPA.
doi: 10.1016/0375-9474(90)90374-U
1988BR33 Phys.Lett. 214B, 483 (1988) M.G.E.Brand, K.Allaart, W.H.Dickhoff Conserving RPA and the Response of 48Ca NUCLEAR STRUCTURE 48Ca; calculated electric quadrupole, dipole resonance strength functions. 48Sc; calculated Gamow-Teller resonance strength functions.
doi: 10.1016/0370-2693(88)90104-9
1987CZ01 Nucl.Phys. A465, 189 (1987) P.Czerski, H.Muther, P.K.Rath, A.Faessler, W.H.Dickhoff Effective Operator for the Transition Density NUCLEAR STRUCTURE 58Ni; calculated level energy, electric transition density.
doi: 10.1016/0375-9474(87)90430-1
1987TE02 J.Phys.(London) G13, 463 (1987) A.Tereno, H.Muther, W.H.Dickhoff High-Momentum Phonon Exchange and the Effective Shell-Model Interaction NUCLEAR STRUCTURE A=18; calculated levels, isospin. Effective shell model interaction.
doi: 10.1088/0305-4616/13/4/009
1986CZ01 Phys.Rev. C33, 1753 (1986) P.Czerski, W.H.Dickhoff, A.Faessler, H.Muther Δ Isobars in Finite Nuclei and Nuclear Matter NUCLEAR STRUCTURE 16O; calculated levels, B(λ). 12C; calculated M1 form factor. RPA, isobar effects.
doi: 10.1103/PhysRevC.33.1753
1986HE07 Nucl.Phys. A451, 269 (1986) W.Hengeveld, W.H.Dickhoff, K.Allaart Self-Consistent Medium Polarization in RPA NUCLEAR REACTIONS 56Ni(e, e'), E not given; calculated form factors. RPA, self-consistent medium polarization. NUCLEAR STRUCTURE 56Ni; calculated levels, B(M1), transition density. 56Co; calculated levels. RPA, self-consistent medium polarization.
doi: 10.1016/0375-9474(86)90415-X
1985HE04 Nucl.Phys. A435, 381 (1985) W.Hengeveld, K.Allaart, W.H.Dickhoff Application of Realistic Meson-Exchange Forces in the Broken-Pair Model NUCLEAR REACTIONS 88Sr(e, e'), E not given; calculated form factor. DWBA, broken pair model functions, meson exchange. NUCLEAR STRUCTURE 58Ni, 88Sr; calculated levels, transition charge density. Broken pair model, meson exchange.
doi: 10.1016/0375-9474(85)90470-1
1985IS01 J.Phys.(London) G11, 763 (1985) M.Ismail, A.Faessler, M.Trefz, W.H.Dickhoff The Volume and Surface Contributions to the Ion-Ion Optical Potential NUCLEAR REACTIONS 12C, 40,48Ca, 16O(12C, 12C), 16O, 40,48Ca(16O, 16O), 40,48Ca(40Ca, 40Ca), 48Ca(48Ca, 48Ca), E=5.18-82.94 MeV/nucleon; calculated ion-ion potential volume, surface contributions, parameter energy dependence, reaction σ(E). Bethe-Goldstone equation, Reid soft core potential.
doi: 10.1088/0305-4616/11/6/013
1985TR04 Nucl.Phys. A443, 499 (1985) M.Trefz, A.Faessler, W.H.Dickhoff Microscopic Description of Heavy-Ion Scattering in the Nuclear Matter Picture NUCLEAR REACTIONS 60Ni, 120Sn, 208Pb(40Ar, X), E=1760 MeV; calculated reaction σ; deduced potential parametes, nucleon-nucleon collision dominance. Microscopic description, nuclear matter approach.
doi: 10.1016/0375-9474(85)90415-4
1984CZ01 Phys.Lett. 146B, 1 (1984) P.Czerski, W.H.Dickhoff, A.Faessler, H.Muther Spin-Isospin Excitations in Finite Nuclei and Nuclear Matter NUCLEAR STRUCTURE 16O; calculated spin-isospin excitations, B(λ). Brueckner G-matrix, realistic meson exchange potential.
doi: 10.1016/0370-2693(84)90630-0
1984CZ02 Nucl.Phys. A427, 224 (1984) P.Czerski, W.H.Dickhoff, A.Faessler, H.Muther Local Forces and the 16O Reaction Matrix NUCLEAR STRUCTURE 16O; calculated levels. RPA, local forces, reaction matrix.
doi: 10.1016/0375-9474(84)90083-6
1984FA12 Nucl.Phys. A428, 271c (1984) A.Faessler, W.H.Dickhoff, M.Trefz, M.Rhoades-Brown Microscopic Approach to Real and Imaginary Part of the Heavy Ion Potential NUCLEAR REACTIONS 12C(12C, 12C), (12C, 12C'), E=1016 MeV; 12C(12C, 12C), E=360 MeV; calculated σ(θ), potential parameters. Microscopic model.
doi: 10.1016/0375-9474(84)90256-2
1984TR14 Phys.Lett. 149B, 459 (1984) M.Trefz, A.Faessler, W.H.Dickhoff, M.Rhoades-Brown The Reaction Mechanism of Heavy Ion Scattering at Intermediate Energies NUCLEAR REACTIONS 12C(12C, 12C), E=1016 MeV; calculated σ(θ). 12C(12C, X), E=0.16-2.25 GeV; calculated reaction σ(E); deduced reaction mechanism. Microscopic parameter free calculation.
doi: 10.1016/0370-2693(84)90366-6
1982VA07 Nucl.Phys. A379, 35 (1982) P.Van Nes, W.H.A.Hesselink, W.H.Dickhoff, J.J.Van Ruyven, M.J.A.DeVoigt, H.Verheul A Neutron Decoupled from a Rotating Odd Core in 114Sb and 116Sb NUCLEAR REACTIONS 113,115In(α, 3nγ), E=36-48 MeV; 117Sn(p, 2nγ), E=15-25 MeV; measured Eγ, Iγ, γγ-coin, Iγ(θ, t), I(ce). 114,116Sb deduced levels, J, π, γ-branching, δ, T1/2, ICC. Enriched targets, Ge(Li), Si-Li detectors, mini-orange electron spectrometer.
doi: 10.1016/0375-9474(82)90555-3
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