NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = B.Castel Found 111 matches. Showing 1 to 100. [Next]1999OT02 Phys.Rev. C59, 3429 (1999) S.Ottini-Hustache, N.Alamanos, F.Auger, B.Castel, Y.Blumenfeld, V.Chiste, N.Frascaria, A.Gillibert, C.Jouanne, V.Lapoux, F.Marie, W.Mittig, J.C.Roynette, J.A.Scarpaci Anomalous E1 and E2 Strengths in 40Ca and 48Ca at Low Excitation Energy: A comparative study NUCLEAR REACTIONS 40,48Ca(86Kr, 86Kr'), E=60 MeV/nucleon; measured σ(E, θ). 40,48Ca deduced E1, E2 strength distributions, collective features. 48Ca deduced no low-energy dipole mode.
doi: 10.1103/PhysRevC.59.3429
1997FA24 Phys.Rep. 290, 201 (1997) M.S.Fayache, L.Zamick, B.Castel The Nuclear Tensor Interaction
doi: 10.1016/S0370-1573(97)00013-6
1996AD02 Phys.Rev. C53, 1016 (1996) Neutron Halos and E1 Resonances in 208Pb NUCLEAR STRUCTURE 208Pb; calculated isovector dipole strength; deduced GDR low energy tail associated E1 peaks.
doi: 10.1103/PhysRevC.53.1016
1996WO01 Int.J.Mod.Phys. E5, 227 (1996) C.E.Wolfe, S.Nozawa, M.N.Butler, B.Castel Polarizability Effects in Pion Photoproduction NUCLEAR REACTIONS 1n, 1H(γ, X), E=200 MeV; calculated πN-production σ; deduced polarizability effects related features.
doi: 10.1142/S0218301396000116
1994AD07 Phys.Rev. C50, R1763 (1994) Quasielastic 40Ca(e, e') Reaction in the Transverse Channel: Nuclear structure effects NUCLEAR REACTIONS 40Ca(e, e'), E not given; calculated transverse response function vs energy transfer. Microscopic approach, RPA correlations.
doi: 10.1103/PhysRevC.50.R1763
1994CH41 Phys.Rev. C50, R2671 (1994) J.Chambers, E.Zaremba, J.P.Adams, B.Castel Pygmy Dipole Resonances in the Calcium Isotopes NUCLEAR REACTIONS 42,44,46,48Ca(γ, X), E ≤ 12 MeV; 40,48Ca(γ, X), E ≤ 30 MeV; calculated low energy photoabsorption spectra; deduced dipole resonance characteristics. Microscopic density functional theory.
doi: 10.1103/PhysRevC.50.R2671
1993AD08 Phys.Rev. C48, 1438 (1993) J.P.Adams, P.G.Blunden, B.Castel, Y.Okuhara Role of Nuclear Structure in the Spin-Isopin Nuclear Response Problem NUCLEAR STRUCTURE 40Ca; calculated spin-longitudinal to spin-transverse response functions ratio; deduced structure effects role in discrepancy with data. Hartree-Fock based RPA approach.
doi: 10.1103/PhysRevC.48.1438
1991BA26 Phys.Rev. C44, 93 (1991) F.T.Baker, L.Bimbot, R.W.Fergerson, C.Glashausser, A.Green, O.Hausser, K.Hicks, K.Jones, C.A.Miller, M.Vetterli, R.Abegg, D.Beatty, B.Bonin, B.Castel, X.Y.Chen, V.Cupps, C.Djalali, R.Henderson, K.P.Jackson, R.Jeppesen, K.Nakayama, S.K.Nanda, R.Sawafta, S.Yen Spin Decomposition of the Responses of 44Ca and 48Ca to 300 MeV Protons NUCLEAR REACTIONS 44Ca(polarized p, p'), E=290 MeV; 48Ca(polarized p, p'), E=318 MeV; measured σ(θ, Ep), analyzing power, spin-flip σ(θ). 44,48Ca deduced giant, spin resonance strength distributions.
doi: 10.1103/PhysRevC.44.93
1991CA18 Z.Phys. A339, 261 (1991) B.Castel, E.R.Siciliano, Y.Okuhara Radiative M1 Capture in Light Nuclei NUCLEAR REACTIONS 28Si(n, γ), E not given; analyzed B(M1) data; deduced reaction mechanism. Shell model.
doi: 10.1007/BF01284062
1990BA14 Phys.Lett. 237B, 337 (1990) F.T.Baker, L.Bimbot, B.Castel, R.W.Fergerson, C.Glashausser, A.Green, O.Hausser, K.Hicks, K.Jones, C.A.Miller, S.K.Nanda, R.D.Smith, M.Vetterli, J.Wambach, R.Abegg, D.Beatty, V.Cupps, C.Djalali, R.Henderson, K.P.Jackson, R.Jeppesen, J.Lisantti, M.Morlet, R.Sawafta, W.Unkelbach, A.Willis, S.Yen The Nuclear Spin Response to Intermediate Energy Protons NUCLEAR REACTIONS 12C, 90Zr, 40,44,48Ca, 24Mg, 54Fe(polarized p, p'), E ≈ 300 MeV; 40Ca(polarized p, p'), E=800 MeV; measured spin-flip transition probability; deduced enhanced spin response features. Continuum RPA.
doi: 10.1016/0370-2693(90)91185-E
1990BO03 Phys.Rev. C41, 786 (1990) Quenching of Spin-Dipole Strength in 40Ca NUCLEAR STRUCTURE 40Ca; analyzed isovector spin-dipole transition strength; deduced quenching mechanisms.
doi: 10.1103/PhysRevC.41.786
1990CA31 Nucl.Phys. A514, 682 (1990) Pion Scattering and Nuclear Surface Effects NUCLEAR STRUCTURE 116Sn, 208Pb; analyzed pion scattering giant resonances data; deduced consistency with other reaction data.
doi: 10.1016/0375-9474(90)90016-F
1990CA34 Phys.Rev. C42, R1203 (1990) Isospin Forbidden E1 Transition in 16O and 40Ca and the Applicability of Siegert's Theorem NUCLEAR STRUCTURE 16O, 40Ca; calculated transition charge densities, isoscalar E1 matrix elements. Siegert's theorem test. NUCLEAR REACTIONS 16O(e, e'), E not given; calculated form factors. Siegert's theorem test.
doi: 10.1103/PhysRevC.42.R1203
1989BO15 Z.Phys. A333, 137 (1989) P.M.Boucher, B.Castel, I.P.Johnstone, Y.Okuhara, C.Glashausser Spin Excitations in Light Nuclei: The (p(pol), p(pol)') reaction on 40Ca NUCLEAR REACTIONS 40Ca(polarized p, p'), E=319 MeV; calculated spin-flip σ(θ); deduced interaction parameters. Realistic RPA.
1989BO19 Phys.Rev. C40, 453 (1989) P.M.Boucher, B.Castel, Y.Okuhara Spin Excitations in Light Nuclei: Effect of projectile energy NUCLEAR REACTIONS 40Ca(polarized p, p'), E=319-800 MeV; calculated spin-flip probability vs E.
doi: 10.1103/PhysRevC.40.453
1989BO33 Phys.Rev. C40, 2897 (1989) Can One Observe the Spin Monopole Resonance in 208Pb ( Question ) NUCLEAR REACTIONS 208Pb(n, p), E not given; analyzed spin isovector monopole, quadrupole strength vs excitation; deduced L=0, L=2 resonance excitation differences. Continuum RPA.
doi: 10.1103/PhysRevC.40.2897
1989BO35 Z.Phys. A334, 381 (1989) Isospin Dependence of the Isoscalar Giant Quadrupole Response: Relevance to Pion Scattering in the Ni Isotopes NUCLEAR REACTIONS 56,60,66Ni(π+, π+'), (π-, π-'), E not given; analyzed data; deduced M(n)/M(p) ratio mass dependence. Continuum RPA. NUCLEAR STRUCTURE 56,60,66Ni; calculated transition densities. Hartree-Fock, RPA methods.
1989BO44 Ann.Phys.(New York) 196, 150 (1989) P.M.Boucher, B.Castel, Y.Okuhara, H.Sagawa Many Particle-Many Hole Nuclear Correlations and the Missing Charge Problem NUCLEAR STRUCTURE 12C, 40,48Ca, 56Fe; calculated longitudinal response functions. Many-particle, many-hole correlations.
doi: 10.1016/0003-4916(89)90048-1
1989CA24 J.Phys.(London) G15, L237 (1989) Pion Scattering in 208Pb and Nuclear Surface Effects NUCLEAR STRUCTURE 208Pb; calculated n, p transition densities; analyzed pion scattering data; deduced Mn/Mp near GQR. Continuum RPA.
doi: 10.1088/0954-3899/15/11/003
1989SA04 Phys.Lett. 219B, 10 (1989) H.Sagawa, P.M.Boucher, B.Castel, Y.Okuhara The Missing Charge Problem and Many-Body Correlation Effects NUCLEAR STRUCTURE 40Ca; calculated longitudinal response function.
doi: 10.1016/0370-2693(89)90827-7
1989TO02 Phys.Lett. 219B, 181 (1989) Ikeda's Sum Rule and Charge-Exchange Reactions on 54Fe NUCLEAR STRUCTURE 54Fe; calculated charge exchange reaction transition strengths; deduced Δ isobar role quenching. Ikeda sum rule.
doi: 10.1016/0370-2693(89)90373-0
1989TO12 Z.Phys. A334, 523 (1989) Origin of Quenching of Gamow-Teller Strength in 54Fe NUCLEAR STRUCTURE 54Fe; analyzed (n, p), (p, n) data; deduced Gamow-Teller transition strength quenching mechanisms.
1988BO07 Phys.Rev. C37, 906 (1988) P.M.Boucher, B.Castel, Y.Okuhara, I.P.Johnstone, J.Wambach, T.Suzuki Spin-Flip Excitations in a Schematic Model NUCLEAR REACTIONS, ICPND 40Ca(p, p'), E ≈ 10-40 MeV; calculated σ(E); deduced spin-flip probability vs E.
doi: 10.1103/PhysRevC.37.906
1988JO04 Phys.Rev. C37, 2239 (1988) Quenching of Magnetic Strength in N = 28 Nuclei NUCLEAR STRUCTURE 52Cr; calculated levels, B(λ). Ground state correlations, renormalized single-particle matrix elements.
doi: 10.1103/PhysRevC.37.2239
1987CA11 Nucl.Phys. A465, 274 (1987) R.F.Carlton, J.A.Harvey, R.L.Macklin, C.H.Johnson, B.Castel Nuclear Structure of 49Ca above 5 MeV Excitation from n + 48Ca and Astrophysics for 30 keV Neutrons NUCLEAR REACTIONS 48Ca(n, n), (n, γ), (n, X), E < 2 MeV; measured total, capture σ(E), transmission. 49Ca deduced levels, J, π, (gΓnGγ/Γ), Γn, Γγ. R-matrix formalism.
doi: 10.1016/0375-9474(87)90435-0
1987OK02 Phys.Lett. 186B, 113 (1987) Y.Okuhara, B.Castel, I.P.Johnstone, H.Toki Nuclear Spin Response to Inelastic Proton Scattering: Finite geometry and absorption effects NUCLEAR STRUCTURE 40Ca; calculated longitudinal to transverse response function ratios. Finite geometry, absorption effects.
doi: 10.1016/0370-2693(87)90264-4
1986CA15 Phys.Rev. C34, 408 (1986) Direct E2 Neutron Capture in Light Nuclei NUCLEAR REACTIONS 20Ne, 25Mg(n, γ), E=thermal; calculated E1, E2 capture σ(E); deduced effective neutron charge multipolarity dependence, particle-core coupling differences role.
doi: 10.1103/PhysRevC.34.408
1986HO19 Phys.Rev. C34, 429 (1986) D.J.Horen, C.H.Johnson, J.L.Fowler, A.D.MacKellar, B.Castel 208Pb + n Reaction and the Mean Nuclear Field near Threshold NUCLEAR REACTIONS 208Pb(n, X), 208Pb(n, n), E=50-1005 keV; measured transmission, σ(E), σ(θ); deduced model parameters. 209Pb deduced resonances, J, π, Γn, neutron reduced width, strength function. Optical model, R-matrix analysis.
doi: 10.1103/PhysRevC.34.429
1986JO03 Phys.Rev. C33, 1086 (1986) Coexistence Models for the 0+1 and 0+2 States in Ge Isotopes NUCLEAR STRUCTURE 70,72,74,76Ge; calculated two-neutron, proton, alpha transfer amplitudes; deduced two-state basis mixing. Coexistence models.
doi: 10.1103/PhysRevC.33.1086
1986OK05 Phys.Rev. C34, 2019 (1986) Y.Okuhara, B.Castel, I.P.Johnstone, H.Toki Surface Effects and the Spin-Isospin Nuclear Response Function NUCLEAR STRUCTURE 40Ca; calculated longitudinal, transverse response function ratio vs spin; deduced surface effects role.
doi: 10.1103/PhysRevC.34.2019
1985AL21 Nucl.Phys. A445, 189 (1985) T.K.Alexander, B.Castel, I.S.Towner Neutron and Proton Polarization Charges from E2 Mirror Transitions NUCLEAR STRUCTURE 17,18O, 17,19F, 18,19,20,22Ne, 22,24,25,26Mg, 25,27Al, 26,27,28,29,30Si, 29P, 30,32,33,34S, 34,36,38Ar, 38Ca; analyzed data; deduced E2 effective charges. Schematic model.
doi: 10.1016/0375-9474(85)90067-3
1985BL03 Phys.Rev. C31, 674 (1985) Anomalous M3 Moment in 39K as a Test of Nuclear Structure NUCLEAR STRUCTURE 43K; calculated quadrupole, M3 moments. Meson exchange, core polarization, isobar excitation.
doi: 10.1103/PhysRevC.31.674
1985BL15 Nucl.Phys. A440, 647 (1985) Quenching of Magnetic Transitions as an Angular Momentum Effect NUCLEAR STRUCTURE A=4-80; analyzed multipole quenching; deduced isobar-hole, nucleon-hole polarizations role multipole dependence.
doi: 10.1016/0375-9474(85)90399-9
1985BL20 Nucl.Phys. A445, 742 (1985) The Magnetic Form Factors of 15N, 17O and 39K NUCLEAR STRUCTURE 15N, 17O, 39K; calculated μ, magnetic form factors.
doi: 10.1016/0375-9474(85)90570-6
1985CA23 Phys.Rev. C32, 323 (1985) B.Castel, I.P.Johnstone, A.G.M.van Hees Magnetic Quadrupole Strength in 12C NUCLEAR STRUCTURE 12C; calculated M2 transition strength fragmentation; deduced 2p-2h correlation, two-body spin-orbit force in quenching. Large basis shell model.
doi: 10.1103/PhysRevC.32.323
1985CA26 Z.Phys. A321, 451 (1985) Can Spin-Flip Quadrupole Resonances be Observed ( Question ) NUCLEAR STRUCTURE 16O; calculated E2 transition strength distribution; deduced GQR spin-flip strength region. Shell model.
doi: 10.1007/BF01411979
1985HA24 Phys.Rev. C32, 1114 (1985) J.A.Harvey, C.H.Johnson, R.F.Carlton, B.Castel Single-Particle 2d5/2 Strength in the 48Ca + n Reaction NUCLEAR REACTIONS 48Ca(n, n), E=0.01-2 MeV; measured σ(E). 49Ca deduced resonances, reduced widths, single particle strength fraction. R-matrix analysis.
doi: 10.1103/PhysRevC.32.1114
1985SA07 Nucl.Phys. A435, 1 (1985) The Giant-Dipole and Spin-Dipole Resonances: A coexistence problem NUCLEAR STRUCTURE 16O; calculated levels, B(E1); deduced GDR, spin-dipole resonances coexistence nonvalidity. Sum rule techniques.
doi: 10.1016/0375-9474(85)90298-2
1984BL03 Phys.Lett. 135B, 367 (1984) The Importance of Meson Exchange Currents, Isobars and Core Polarisation on the Magnetic Form Factor of 17O NUCLEAR REACTIONS 17O(e, e'), E not given; calculated magnetic form factor; deduced meson exchange, isobar, core polarization effects relative magnitude. Perturbation approach.
doi: 10.1016/0370-2693(84)90295-8
1984CA05 Z.Phys. A315, 99 (1984) Effects beyond First-Order Perturbation Theory in the Polarization Charges for E4 Transitions NUCLEAR STRUCTURE 52Fe; calculated intrinsic state E4 moment quadrupole distortion, E4 polarization charge values. 52Cr, 53Fe, 52Mn; calculated E4 polarization charge values; deduced open shell effect role.
doi: 10.1007/BF01436214
1984CA07 Nucl.Phys. A415, 30 (1984) B.Castel, A.G.M.Van Hees, L.Zamick Electric Spin Resonances in Light Nuclei NUCLEAR STRUCTURE 16O, 40Ca; calculated levels, dipole spin-flip strength distribution.
doi: 10.1016/0375-9474(84)90597-9
1984CA11 Phys.Rev. C29, 1912 (1984) B.Castel, A.G.M.Van Hees, H.Toki Origin of M1 Strength in 16O NUCLEAR STRUCTURE 16O; calculated M1 transition strengths; deduced enhancement mechanisms. Shell model, isobar excitation, core polarization, meson exchange.
doi: 10.1103/PhysRevC.29.1912
1984CA14 Phys.Rev. C29, 1980 (1984) R.F.Carlton, W.M.Good, J.A.Harvey, R.L.Macklin, B.Castel Determination of Unbound States in 35S from Neutron Total and Capture Cross-Section Measurements on 34S NUCLEAR STRUCTURE 35S; calculated levels, neutron strength function. Shell model, R-matrix methods. NUCLEAR REACTIONS 34S(n, n), E=90-1500 keV; measured σ(E). 34S(n, γ), E=30-1100 keV; measured capture σ. 35S deduced resonances, average parameters, J, π, (gΓn), (gΓnΓγ/Γ), level spacings, densities, neutron strength function.
doi: 10.1103/PhysRevC.29.1980
1984CA25 Z.Phys. A318, 31 (1984) On the Difference between the Effective Charges Used for Bound States of 29Si and for Low-Energy Neutron Radiative Capture by 28Si NUCLEAR REACTIONS 28Si(n, γ), E=560 keV; calculated p-wave radial function; deduced external capture dominance, neutron E1 effective charge dependence of capture process.
doi: 10.1007/BF02117211
1984LI10 Z.Phys. A317, 149 (1984) A.Lindholm, L.Nilsson, I.Bergqvist, R.Zorro, N.Olsson, B.Castel, A.Likar Fast Neutron Radiative Capture in Silicon NUCLEAR REACTIONS 28Si(n, γ), E=3-14 MeV; measured σ(θ=90°) vs E; deduced reaction mechanism. 29Si deduced GDR, GQR interference channel dependence. Compound nucleus, direct-semidirect, continuum shell model analyses.
doi: 10.1007/BF01421249
1984MA24 Phys.Rev. C29, 1993 (1984) s- and p-Wave Neutrons on 30Si and 34S: Coupled channels optical model NUCLEAR REACTIONS 30Si, 34S(n, n), E not given; analyzed data; deduced optical model parameter target excitation dependence. Coupled-Channels model, collective effects.
doi: 10.1103/PhysRevC.29.1993
1983BL06 Z.Phys. A312, 247 (1983) Quenched Magnetic Transitions from High Spin States in Light Nuclei NUCLEAR STRUCTURE 28Si, 24Mg; calculated isoscalar, isovector M6 transition strength quenching factors; deduced isoscalar, isovector transition density structure difference role. Shell model, Landau-Migdal, boson exchange interactions.
doi: 10.1007/BF01412167
1983BR16 Phys.Lett. 127B, 151 (1983) B.A.Brown, D.J.Horen, B.Castel, H.Toki Core Excitations and M1 Strengths in the Ca Isotopes NUCLEAR STRUCTURE 40Ca; calculated positive parity T=0, 1 states, isovector B(M1). 16,18,20,22O; calculated B(M1) vs excitation energy. Shell model. 42,44Ca; calculated M1 transition strength reduction, fragmentation. Weak-coupling extension.
doi: 10.1016/0370-2693(83)90864-X
1983CA15 Nucl.Phys. A403, 93 (1983) B.Castel, G.R.Satchler, L.Zamick, I.P.Johnstone Core-Polarization and Open-Shell Effects in E6 Transitions NUCLEAR STRUCTURE 50,52Cr, 52Fe; analyzed E6 decay negative proton polarization charge; deduced quadrupole deformation role. Collective model core polarization, open shell approaches.
doi: 10.1016/0375-9474(83)90190-2
1983CA24 Phys.Rev. C28, 2571 (1983) Distribution of E1 Spin Flip Strength in 12C NUCLEAR STRUCTURE 12C; calculated spin-flip E1 transition strength distribution. Shell model.
doi: 10.1103/PhysRevC.28.2571
1983HA12 Phys.Rev. C28, 24 (1983) J.A.Harvey, W.M.Good, R.F.Carlton, B.Castel, J.B.McGrory, S.F.Mughabghab Neutron Spectroscopy as a High-Resolution Probe: Identification of the missing (1/2)+ states in 31Si NUCLEAR STRUCTURE 31Si; calculated levels, spectroscopic strengths. Shell model. NUCLEAR REACTIONS 30Si(n, X), E=0.2-1400 keV; measured transmission, σ(E). 31Si deduced resonances, J, π, Γn, level densities, s-, p-, d-wave strength functions.
doi: 10.1103/PhysRevC.28.24
1983JO03 Phys.Rev. C27, 846 (1983) I.P.Johnstone, N.Kumar, B.Castel Isospin Mixing in the Lowest T = 2 State of 8Be NUCLEAR STRUCTURE 8Be; calculated level Γ, partial decay widths. Shell model, charge dependent forces.
doi: 10.1103/PhysRevC.27.846
1983MA30 Phys.Rev. C28, 441 (1983) l Dependence of the Optical Potential: Application to the 32S + n reaction using coupled channels NUCLEAR REACTIONS 32S(n, n), E=0.5 MeV; calculated s-, p-wave, σ(shape elastic). 32S(n, n), E=0.1-0.8 MeV; calculated s-wave σ(shape elastic); deduced optical potential parameters. Dynamical deformation, coupled-channels calculation.
doi: 10.1103/PhysRevC.28.441
1982CA06 Phys.Rev. C25, 2148 (1982) Role of Isobar-Hole Excitations in the Quenching of the 40K(β-)40Ca Transition RADIOACTIVITY 40K; calculated β-decay rate; deduced nuclear, isobar excitation quenching effects. Shell model, isobar-hole excitations.
doi: 10.1103/PhysRevC.25.2148
1981CU04 Phys.Rev. C23, 1279 (1981) Isopin Mixing in 16O by use of Pion and Deuteron Probes NUCLEAR REACTIONS 16O(π+, π+'), E=164 MeV; calculated σ. 16O(d, t), E not given; calculated C2S. 16O levels deduced isopin matrix element. Euler angle representation.
doi: 10.1103/PhysRevC.23.1279
1980CA06 Phys.Lett. 91B, 185 (1980) B.Castel, G.R.Satchler, K.Goeke Core Polarization Effects and Giant Quadrupole Resonances in the A = 90 Region NUCLEAR STRUCTURE A ≈ 90; calculated proton, neutron effective charges. Linearized Hartree-Fock, macroscopic GQR excitation models.
doi: 10.1016/0370-2693(80)90426-8
1980CA09 Phys.Rev. C21, 1538 (1980) Isomeric States and Spin Polarization in A ≈ 90 Nuclei NUCLEAR STRUCTURE 88,87Sr, 89Y; calculated B(λ), inhibition factor, spin polarization for isomeric M4 transition. RPA, collective renormalizations.
doi: 10.1103/PhysRevC.21.1538
1980CA15 Nucl.Phys. A341, 93 (1980) B.Castel, R.Y.Cusson, L.Zamick Isospin Mixing in 16O: A Three-Level Model NUCLEAR STRUCTURE 16O; calculated isospin mixing effects for 2- states. Three-level model.
doi: 10.1016/0375-9474(80)90363-2
1980GO05 Nucl.Phys. A339, 377 (1980) K.Goeke, B.Castel, P.-G.Reinhard Isovector Giant Monopole Resonances: A Sum-Rule Approach NUCLEAR STRUCTURE 16O, 40Ca, 56Ni, 90Zr, 208Pb; calculated T=1, giant monopole resonance sum rules. Adiabatic time-dependent Hartree-Fock, Skyrme interacion.
doi: 10.1016/0375-9474(80)90022-6
1980HA01 J.Phys.(London) G6, 59 (1980) D.Halderson, B.Castel, G.Aizer Non-Statistical Effects in Neutron Reactions on 32S NUCLEAR REACTIONS 32S(n, γ), E ≈ 0-1.2 MeV; calculated cumulative Γn(E), Γγ, reduced n-width. Shell model in continuum.
doi: 10.1088/0305-4616/6/1/013
1980YA01 Phys.Lett. 89B, 307 (1980) H.L.Yadav, A.Faessler, H.Toki, B.Castel Electromagnetic Transitions in the Pt Nuclei NUCLEAR STRUCTURE 190,192,194Pt; calculated B(E2). Asymmetric rotor model, quasiparticle collective excitation coupling.
doi: 10.1016/0370-2693(80)90130-6
1980YA06 Phys.Rev. C22, 2644 (1980) E2 Interference Terms in the Coulomb Excitations of the Os and Pt Nuclei NUCLEAR STRUCTURE 192,194Pt, 192Os;calculated B(E2), δ vs collective parameter; deduced quasiparticle excitation role in E2 interference term size anomaly. Extended Davydov-Fillipov model.
doi: 10.1103/PhysRevC.22.2644
1979CA05 Phys.Lett. 82B, 160 (1979) Calculation of Nuclear RMS Radii Using a Skyrme Interaction with a State Dependent Effective Mass NUCLEAR STRUCTURE 40,48Ca; calculated properties of valence orbits. Modified Skyrme interaction, local enhancement of effective mass at Fermi surface.
doi: 10.1016/0370-2693(79)90724-X
1979GO01 Phys.Rev. C19, 201 (1979) Calculation of Giant Monopole Resonances in the Adiabatic Time-Dependent Hartree-Fock Theory NUCLEAR STRUCTURE 16O, 40Ca, 90Zr, 208Pb; calculated GMR. time-dependent Hartree-Fock with Skyrme interactions.
doi: 10.1103/PhysRevC.19.201
1978CA23 Phys.Lett. 80B, 13 (1978) Giant E0 Resonances and their Effects on the Lifetime of Excited 0+ States NUCLEAR STRUCTURE 40Ca, 90Zr, 208Pb; calculated renormalization effects on low energy E0 transitions due to excitation of giant E0 resonances using a state dependent monopole effective charge.
doi: 10.1016/0370-2693(78)90293-9
1978HA32 Phys.Rev. C18, 1542 (1978) Neutron and Gamma Width Correlations in Neutron Capture Reactions: A Comparative Study NUCLEAR REACTIONS 28Si(n, γ); calculated Γγ.
doi: 10.1103/PhysRevC.18.1542
1978MI14 Ann.Phys.(New York) 114, 452 (1978) Doorway Structures in the Radiative Capture of Neutrons by 28Si and 32S NUCLEAR REACTIONS 28Si, 32S(n, γ); calculated σ. K-matrix formalism, microscopic treatment including single-particle resonances.
doi: 10.1016/0003-4916(78)90277-4
1977CA25 Phys.Rev. C16, 2092 (1977) Effective Charges and Isoscalar Shifts in the Linearized Hartree-Fock Model NUCLEAR STRUCTURE 207,208Pb, 209Bi, 89Y, 90Zr; calculated change in rms radii. Skyrme interaction.
doi: 10.1103/PhysRevC.16.2092
1977HA22 Ann.Phys.(New York) 103, 133 (1977) D.Halderson, B.Castel, M.Divadeenam, H.W.Newson s- and p-Wave Neutron Spectroscopy. Xf(ii). Intermediate Structure in the 28Si+n Reaction: Doorway State Calculation NUCLEAR STRUCTURE 29Si; calculated low-lying structure. Doorway state calculation.
doi: 10.1016/0003-4916(77)90265-2
1977MI05 Z.Phys. A282, 117 (1977) Higher Order Processes in the Radiative Capture of Fast Neutrons NUCLEAR REACTIONS 40Ca(n, γ); calculated σ; predicted single particle resonances superimposed on broad giant resonance.
doi: 10.1007/BF01881013
1976CA07 Phys.Rev. C13, 1765 (1976) Prolate-Oblate Energy Difference and Shape Variation in the f-p Shell NUCLEAR STRUCTURE 48Ti, 50,52Cr, 54,56Fe, 64Zn, 72Ge; calculated prolate-oblate energy differences. Generator-coordinate method.
doi: 10.1103/PhysRevC.13.1765
1976CA27 Phys.Lett. 65B, 27 (1976) Giant Spin Resonances and Effective Mλg-Factors NUCLEAR STRUCTURE 207,208Pb, 40Ca, 39K, 32,33S, 207Tl; calculated giant resonance parameters, B(λ).
doi: 10.1016/0370-2693(76)90526-8
1976HA05 Phys.Rev.Lett. 36, 760 (1976) D.Halderson, B.Castel, I.P.Johnstone, M.Divadeenam Neutron and Gamma Widths of a J = 3/2- Doorway State in 29Si NUCLEAR STRUCTURE 29Si; calculated doorway resonances, widths.
doi: 10.1103/PhysRevLett.36.760
1975CA25 Z.Phys. A274, 275 (1975) B.Castel, D.Halderson, M.Micklinghoff, M.Divadeenam Structure of Doorway States in the 40Ca + n Reaction NUCLEAR STRUCTURE 41Ca; calculated S.
doi: 10.1007/BF01437740
1975MI10 Nucl.Phys. A251, 181 (1975) M.Micklinghoff, B.Castel, I.P.Johnstone Ground State Correlations in the Core-Particle Model: Application to 37Ar NUCLEAR STRUCTURE 37Ar; calculated levels, B(λ), S.
doi: 10.1016/0375-9474(75)90709-5
1975RO28 Can.J.Phys. 53, 2631 (1975) B.C.Robertson, M.Micklinghoff, B.Castel The 7/2- Doublet in 55Fe NUCLEAR REACTIONS 52Cr(α, nγ), E=6.75 MeV; 55Mn(p, nγ), E=3.6 MeV; measured DSA, Iγ. 55Fe levels deduced T1/2, γ-branching, μ.
doi: 10.1139/p75-322
1974JO12 Can.J.Phys. 52, 1998 (1974) Electric Dipole Transition Strengths in 19F NUCLEAR STRUCTURE 19F; calculated levels, B(E1).
doi: 10.1139/p74-263
1974MI17 Phys.Lett. 52B, 166 (1974) Spectroscopic Factors and E3 Transition Rates in 39K NUCLEAR STRUCTURE 39K; calculated levels, S, B(E3).
doi: 10.1016/0370-2693(74)90079-3
1974NG03 Phys.Rev. C10, 2643 (1974) Lipkin-Nogami Approximation of Pairing Interaction NUCLEAR STRUCTURE 58,60,62,64,66Ni; calculated levels.
doi: 10.1103/PhysRevC.10.2643
1974PW01 Phys.Rev. C9, 1650 (1974) Dynamic Treatment of the Mass Distribution in Fission NUCLEAR STRUCTURE, Fission 238U, 240Pu, 242,244Cm, 252Cf, 256Fm; calculated yield curves.
doi: 10.1103/PhysRevC.9.1650
1973BE58 Nucl.Phys. A217, 189 (1973); Erratum Nucl.Phys. A223, 627 (1974) H.G.Benson, I.P.Johnstone, B.Castel Five-Particle-One-Hole States in 44Sc NUCLEAR STRUCTURE 44Sc; calculated levels, B(E2).
doi: 10.1016/0375-9474(73)90632-5
1973CA34 Can.J.Phys. 51, 2403 (1973) B.Castel, M.Micklinghoff, I.P.Johnstone Shell Model and Collective Excitations in 72Ge NUCLEAR STRUCTURE 72Ge; calculated levels, J, E2 transition rates.
doi: 10.1139/p73-314
1973JO04 Can.J.Phys. 51, 988 (1973) Effect of Core Excitations on 29Si and on the Giant Dipole Resonance in 28Si NUCLEAR STRUCTURE 29Si calculated levels, B(E2), S.
doi: 10.1139/p73-128
1973JO16 Nucl.Phys. A213, 341 (1973) Retardation of E1 Transitions and the Neutron Effective Charge in 29Si NUCLEAR STRUCTURE 29Si; calculated levels, B(E1).
doi: 10.1016/0375-9474(73)90155-3
1973PW01 Lett.Nuovo Cim. 8, 945 (1973) Mass Asymmetry in Fission and Nuclear Viscosity NUCLEAR STRUCTURE 236U; calculated fission product mass distribution.
doi: 10.1007/BF02727805
1972CA20 Can.J.Phys. 50, 1630 (1972) B.Castel, I.P.Johnstone, B.P.Singh, K.W.C.Stewart Low-Lying Structure and Inelastic Scattering of Cu Isotopes in a Unified Model NUCLEAR STRUCTURE 59,61,63,65Cu; calculated levels, μ, quadrupole moment, B(E2), B(M1), γ-mixing, γ-branching, S. Quasiparticle coupling to anharmonic vibrations.
doi: 10.1139/p72-220
1972SI13 Phys.Rev. C5, 1613 (1972) B.P.Singh, B.Castel, I.P.Johnstone, K.W.C.Stewart Nuclear Structure of 30P and 34Cl in a Unified Model NUCLEAR STRUCTURE 30P, 34Cl; calculated levels, B(E2), B(M1). Vibrational unified model.
doi: 10.1103/PhysRevC.5.1613
1972SI53 Izv.Akad.Nauk SSSR, Ser.Fiz. 36, 2526 (1972); Bull.Acad.Sci.USSR, Phys.Ser. 36, 2195 (1973) D.Sinclair, B.Castel, I.P.Johnstone, J.T.Yuang Structure of the Excited Levels of Odd Iodine Isotopes NUCLEAR STRUCTURE 127I calculated levels, B(E2), S for single proton transfer. 121,123,125,129,131I calculated levels.
1971CA02 Phys.Rev. C3, 964 (1971) Projected Hartree-Fock and Core-Particle Coupling for A = 29 and 30 NUCLEAR STRUCTURE 29,30Si, 29P; calculated levels, B(E2), B(M1). Projected Hartree-Fock, core-quasiparticle coupling model.
doi: 10.1103/PhysRevC.3.964
1971CA04 Nucl.Phys. A162, 273 (1971) B.Castel, K.W.C.Stewart, M.Harvey Coupling of Quasiparticles and Anharmonic Vibrations: A = 33 and 34 NUCLEAR STRUCTURE 33,34S, 33Cl; calculated levels. Intermediate coupling vibrational model.
doi: 10.1016/0375-9474(71)90984-5
1971CA20 Can.J.Phys. 49, 1641 (1971) Two Particle - One Hole Contributions to Magnetic Moments and M1 Transitions NUCLEAR STRUCTURE 29Si, 31P, 35Cl; calculated μ, B(M1); deduced 2p-1h contributions.
doi: 10.1139/p71-192
1971CA24 Can.J.Phys. 49, 2028 (1971) Compressibility under Deformation of the Hartree-Fock Field NUCLEAR STRUCTURE 44Ca, 50Cr, 56,58Ni; calculated rms radius, compressibility under deformation. Deformed Hartree-Fock model.
doi: 10.1139/p71-245
1971CA31 Phys.Rev. C4, 1966 (1971) B.Castel, K.W.C.Stewart, M.Harvey Coupling of Particle-Hole and Surface Excitations in Closed-Shell Nuclei NUCLEAR STRUCTURE 32S; calculated levels, B(E2).particle-hole, surface excitation coupling.
doi: 10.1103/PhysRevC.4.1966
1971JO01 Phys.Lett. 34B, 34 (1971) I.P.Johnstone, B.Castel, P.Sostegno Proton Hole States in 20F NUCLEAR STRUCTURE 20F; calculated levels, transition rates. Projected Hartree-Fock theory.
doi: 10.1016/0370-2693(71)90498-9
1971JO21 Phys.Lett. 37B, 329 (1971) On the 19/2- (3.12 MeV) State in 43Sc and the 6+ (3.19 MeV) State in 42Ca RADIOACTIVITY 42Sc; calculated log ft. NUCLEAR MOMENTS 43Sc, 42Ca; calculated g.
doi: 10.1016/0370-2693(71)90192-4
1971PA39 Phys.Lett. 37B, 7 (1971) Pairing Effects in the Projected Hartree-Fock Model NUCLEAR STRUCTURE 58,60,62,64Ni; calculated ground-state energies. Projected Hartree-Fock model, pairing correlations.
doi: 10.1016/0370-2693(71)90554-5
1971RO03 Phys.Rev. C3, 73 (1971) D.J.Rowe, N.Ullah, S.S.M.Wong, J.C.Parikh, B.Castel Investigation of the One-Particle-Hole and Projected Hartree-Fock Approximations in C12 and O16 NUCLEAR STRUCTURE 12C, 16O; calculated levels, quadrupole moment. Particle-hole, projected Hartree-Fock approximations.
doi: 10.1103/PhysRevC.3.73
1971ST32 Phys.Rev. C4, 2131 (1971) K.W.C.Stewart, B.Castel, B.P.Singh Odd Co Isotopes in a Unified Vibrational Model NUCLEAR STRUCTURE 57,59,61,63Co; calculated levels, B(λ). Unified vibrational model.
doi: 10.1103/PhysRevC.4.2131
1970CA10 Can.J.Phys. 48, 1490 (1970) B.Castel, K.W.C.Stewart, M.Harvey Intermediate-Coupling Structure of Odd-A Nuclei in the 2s-1d Shell NUCLEAR STRUCTURE 29Si, 31P, 35Cl; calculated positive-parity levels. Intermediate coupling model.
doi: 10.1139/p70-188
1970CA18 Lett.Nuovo Cimento 3, 23 (1970) B.Castel, K.W.C.Stewart, J.C.Parikh Quadrupole Moments of Excited States in Light Nuclei NUCLEAR STRUCTURE 24Mg, 28Si; calculated quadrupole moment ratio for levels in rotational bands. SU3, projected Hartree-Fock formalisms.
doi: 10.1007/BF02755772
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