NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = D.J.Rowe Found 88 matches. 2020DY01 Phys.Rev.Lett. 124, 042501 (2020) T.Dytrych, K.D.Launey, J.P.Draayer, D.J.Rowe, J.L.Wood, G.Rosensteel, C.Bahri, D.Langr, R.B.Baker Physics of Nuclei: Key Role of an Emergent Symmetry NUCLEAR STRUCTURE 6Li, 8He, 20Ne; calculated excitation energies of the ground-state rotational band using first-principles of nuclear structure that the special nature of the strong nuclear force determines highly regular patterns unrecognized in nuclei that can be tied to an emergent approximate sy mmetry.
doi: 10.1103/PhysRevLett.124.042501
2020RO05 Phys.Rev. C 101, 054301 (2020) Nuclear shape coexistence from the perspective of an algebraic many-nucleon version of the Bohr-Mottelson unified model NUCLEAR STRUCTURE 12C, 16O, 166Er; calculated energies for irrotational flow, rigid-body rotation, and kinetic energy for shape coexistent intrinsic state in 166Er, positive parity symplectic-model irreducible representations using fully quantal algebraic version of the Bohr-Mottelson unified model. Comparison with experimental data for 166Er taken from NuDat 2.7 database.
doi: 10.1103/PhysRevC.101.054301
2018RO07 J.Phys.(London) G45, 06LT01 (2018) A relationship between isobaric analog states and shape coexistence in nuclei NUCLEAR STRUCTURE 40Ca, 44Sc, 44Ti, 44V, 44Cr; analyzed available data; deduced direct a relationship between the persistence of isospin as a good quantum number.
doi: 10.1088/1361-6471/aabc1b
2016RO05 J.Phys.(London) G43, 024011 (2016) The emergence of deformation and rotational states in the many-nucleon quantum theory of nuclei NUCLEAR STRUCTURE 12C, 16O, 168Er; analyzed available data; calculated energies. Shell structure in the Mayer-Jensen model.
doi: 10.1088/0954-3899/43/2/024011
2012TH11 Nucl.Phys. A895, 20 (2012) G.Thiamova, D.J.Rowe, M.A.Caprio The relationship between the interacting boson model and the algebraic version of Bohr's collective model in its triaxial limit
doi: 10.1016/j.nuclphysa.2012.09.002
2009RO05 Phys.Rev. C 79, 054304 (2009) D.J.Rowe, T.A.Welsh, M.A.Caprio Bohr model as an algebraic collective model
doi: 10.1103/PhysRevC.79.054304
2009TH02 Eur.Phys.J. A 41, 189 (2009) Large boson number IBM calculations and their relationship to the Bohr model
doi: 10.1140/epja/i2009-10810-x
2007RO25 Nucl.Phys. A797, 94 (2007) The competition between SU(3) and pair coupling in the many-fermion sd shell and interacting boson models NUCLEAR STRUCTURE 20Ne; calculated level energies, J, E2 transition probabilities using a nuclear shell model. Comparison with data.
doi: 10.1016/j.nuclphysa.2007.10.004
2006RO43 Phys.Rev.Lett. 97, 202501 (2006) D.J.Rowe, G.Thiamova, J.L.Wood Implications of Deformation and Shape Coexistence for the Nuclear Shell Model NUCLEAR STRUCTURE 16O; calculated excited states J, π, rotational band features.
doi: 10.1103/PhysRevLett.97.202501
2006TH04 Czech.J.Phys. 56, 341 (2006) Persistence of rotational bands in a coupled SU(3) model
doi: 10.1007/s10582-006-0095-5
2006TH10 Nucl.Phys. A780, 112 (2006) G.Thiamova, D.J.Rowe, J.L.Wood Coupled-SU(3) models of rotational states in nuclei
doi: 10.1016/j.nuclphysa.2006.09.020
2006TH14 Int.J.Mod.Phys. E15, 1741 (2006) Persistence of rotational structure in nuclei and quasi-dynamical symmetry
doi: 10.1142/S0218301306005551
2005RO09 Nucl.Phys. A753, 94 (2005) The algebraic collective model
doi: 10.1016/j.nuclphysa.2005.01.032
2005RO24 Nucl.Phys. A759, 92 (2005) Phase transitions and quasi-dynamical symmetry in nuclear collective models, III: The U(5) to SU(3) phase transition in the IBM
doi: 10.1016/j.nuclphysa.2005.05.144
2005RO34 Nucl.Phys. A760, 59 (2005) The many relationships between the IBM and the Bohr model
doi: 10.1016/j.nuclphysa.2005.06.001
2005TH08 Czech.J.Phys. 55, 957 (2005) The O(6) description of the nuclear rotation NUCLEAR STRUCTURE 162Dy, 168Er; calculated levels, J, rotational bands, B(E2). Interacting boson model.
doi: 10.1007/s10582-005-0096-9
2005TU05 Nucl.Phys. A756, 333 (2005) Phase transitions and quasidynamical symmetry in nuclear collective models. II. The spherical vibrator to gamma-soft rotor transition in an SO(5)-invariant Bohr model
doi: 10.1016/j.nuclphysa.2005.04.003
2004BA32 Comput.Phys.Commun. 159, 121 (2004) C.Bahri, D.J.Rowe, J.P.Draayer Programs for generating Clebsch-Gordan coefficients of SU(3) in SU(2) and SO(3) bases
doi: 10.1016/j.cpc.2004.01.005
2004RO17 Nucl.Phys. A735, 372 (2004) A computationally tractable version of the collective model
doi: 10.1016/j.nuclphysa.2004.02.018
2004RO31 Phys.Rev.Lett. 93, 122502 (2004) Quasidynamical Symmetry in an Interacting Boson Model Phase Transition
doi: 10.1103/PhysRevLett.93.122502
2004RO38 Nucl.Phys. A745, 47 (2004) Phase transitions and quasidynamical symmetry in nuclear collective models: I. The U(5) to O(6) phase transition in the IBM
doi: 10.1016/j.nuclphysa.2004.09.007
2004RO41 Phys.Rev.Lett. 93, 232502 (2004) D.J.Rowe, P.S.Turner, G.Rosensteel Scaling Properties and Asymptotic Spectra of Finite Models of Phase Transitions as They Approach Macroscopic Limits
doi: 10.1103/PhysRevLett.93.232502
2003RO01 Phys.Rev. C 67, 014303 (2003) Seniority-conserving forces and USp(2j+1) partial dynamical symmetry NUCLEAR STRUCTURE 92Mo, 94Ru, 96Pd, 210Po, 212Rn, 214Ra; calculated levels, J, seniority. Seniority-conserving forces, partial dynamical symmetry, comparison with data.
doi: 10.1103/PhysRevC.67.014303
2002CA21 Nucl.Phys. A703, 167 (2002) M.J.Carvalho, D.J.Rowe, S.Karram, C.Bahri Optimal Basis States for a Microscopic Calculation of Intrinsic Vibrational Wave Functions of Deformed Rotational Nuclei
doi: 10.1016/S0375-9474(01)01458-0
2001RO25 Nucl.Phys. A691, 691 (2001) Restoration of Particle Number as a Good Quantum Number in BCS Theory
doi: 10.1016/S0375-9474(01)00588-7
2001RO28 Phys.Rev.Lett. 87, 172501 (2001) Partially Solvable Pair-Coupling Models with Seniority-Conserving Interactions NUCLEAR STRUCTURE 92Mo, 94Ru, 96Pd; calculated levels, J, π, configurations. Seniority-conserving interactions, comparison with data.
doi: 10.1103/PhysRevLett.87.172501
2000BA03 Nucl.Phys. A662, 125 (2000) SU(3) Quasi-Dynamical Symmetry as an Organizational Mechanism for Generating Nuclear Rotational Motions NUCLEAR STRUCTURE 166Er; calculated rotational band levels, J, B(E2), giant resonance features. SU(3) quasi-dynamical symmetry, phenomenological symplectic model.
doi: 10.1016/S0375-9474(99)00394-2
2000RO02 Phys.Lett. 472B, 227 (2000) Angular-Momentum Projection of Rotational Model Wave Functions
doi: 10.1016/S0370-2693(99)01448-3
1999RO07 J.Phys.(London) G25, 635 (1999) Macroscopic and Microscopic Models of Nuclear Rotations
doi: 10.1088/0954-3899/25/4/011
1998BA62 Phys.Rev. C58, 1539 (1998) C.Bahri, D.J.Rowe, W.Wijesundera Phase Transition in the Pairing-Plus-Quadrupole Model
doi: 10.1103/PhysRevC.58.1539
1998DE28 Nucl.Phys. A636, 47 (1998) An Algebraic Representation of the Particle-Plus-Rotor Model
doi: 10.1016/S0375-9474(98)00169-9
1998RO16 Phys.Rev.Lett. 80, 4394 (1998) D.J.Rowe, C.Bahri, W.Wijesundera Exactly Solvable Model of a Superconducting to Rotational Phase Transition
doi: 10.1103/PhysRevLett.80.4394
1997CA17 Nucl.Phys. A618, 65 (1997) Transverse Form Factors in the Collective and Symplectic Models NUCLEAR REACTIONS 16O, 24Mg, 40Ca(e, e'), E not given; calculated transverse form factors. Collective, symplectic models.
doi: 10.1016/S0375-9474(97)00064-X
1995CH10 Nucl.Phys. A582, 181 (1995) The Pair-Coupling Model
doi: 10.1016/0375-9474(94)00472-Y
1995DE19 Nucl.Phys. A589, 58 (1995) Rotor Plus SU(3)-Particle with Spin
doi: 10.1016/0375-9474(95)00027-X
1994DE16 Nucl.Phys. A575, 46 (1994) H.de Guise, D.J.Rowe, R.Okamoto The Role of Spin in the Strong Coupling of a Rotor and Single Particle
doi: 10.1016/0375-9474(94)90136-8
1994RO03 Nucl.Phys. A570, 279c (1994) The Microscopic Theory of Nuclear Collective Motion
doi: 10.1016/0375-9474(94)90293-3
1994RO05 Nucl.Phys. A574, 253c (1994) Algebraic Models of Nuclear Collective Motion NUCLEAR STRUCTURE 126Ba, 154Sm, 164Yb, 166Er; compiled, reviewed data, analyses. Algebraic models, collective motion.
doi: 10.1016/0375-9474(94)90049-3
1993CA33 Phys.Lett. 318B, 273 (1993) M.J.Carvalho, M.G.Vassanji, D.J.Rowe A Symplectic Model Calculation of Transverse Electron Scattering Form Factors for 24Mg NUCLEAR REACTIONS 24Mg(e, e), E not given; calculated transverse form factor. Symplectic model.
doi: 10.1016/0370-2693(93)90127-4
1992CA24 Nucl.Phys. A548, 1 (1992) The Shell-Model Distribution of Nuclear Shapes NUCLEAR STRUCTURE 168Er; calculated n(h-bar x omega) configurations, E/(h-bar x omega) vs n. Irreducible sp(2, R) representation, shell model space.
doi: 10.1016/0375-9474(92)90073-S
1991JA05 Nucl.Phys. A528, 409 (1991) The SU(3) Structure of Rotational States in Heavy Deformed Nuclei NUCLEAR STRUCTURE 160,162,164,168,170Er, 182,184,186W; analyzed B(λ), level data; deduced SU(3) representation labels distribution.
doi: 10.1016/0375-9474(91)90096-O
1990AR04 Nucl.Phys. A511, 49 (1990) F.Arickx, J.Broeckhove, M.G.Vassanji, D.J.Rowe Application of the Symplectic Model to the Giant Resonance States in 16O and 40Ca NUCLEAR STRUCTURE 40Ca, 16O; calculated levels. Symplectic model, generator coordinate formalism. NUCLEAR REACTIONS 40Ca, 16O(e, e'), E not given; calculated form factors. Symplectic model, generator coordinate formalism.
doi: 10.1016/0375-9474(90)90026-I
1988VA22 Phys.Lett. 210B, 20 (1988) M.G.Vassanji, J.Carvalho, D.J.Rowe A Symplectic Model Calculation of the Inelastic Electron Scattering Form Factor for the 02+ Excitation of 4He NUCLEAR REACTIONS 4He(e, e'), E not given; calculated form factor. Symplectic shell model.
doi: 10.1016/0370-2693(88)90340-1
1987CA10 Nucl.Phys. A465, 265 (1987) J.Carvalho, M.Vassanji, D.J.Rowe Application of the Symplectic Shell Model to the L = 0+ States of 4He NUCLEAR STRUCTURE 4He; calculated levels; deduced monopole state collectivity. Symplectic shell model.
doi: 10.1016/0375-9474(87)90434-9
1987RO06 Nucl.Phys. A464, 39 (1987) D.J.Rowe, P.Rochford, R.Le Blanc The Coupling of Valence Shell and Particle-Hole Degrees of Freedom in a Partial Random Phase Approximation NUCLEAR STRUCTURE 166Er; calculated levels, J, π, B(E2). Partial RPA.
doi: 10.1016/0375-9474(87)90421-0
1987VA12 Nucl.Phys. A466, 227 (1987) An Application of Boson Second Quantization Techniques to the Calculation of Electron Scattering Form Factors NUCLEAR REACTIONS 20Ne(e, e), (e, e'), E not given; calculated longitudinal scattering form factor. Boson second quantization technique.
doi: 10.1016/0375-9474(87)90440-4
1986CA03 Nucl.Phys. A452, 240 (1986) J.Carvalho, R.Le Blanc, M.Vassanji, D.J.Rowe, J.B.McGrory The Symplectic Shell-Model Theory of Collective States NUCLEAR STRUCTURE 24Mg; calculated levels, B(λ). Symplectic shell model.
doi: 10.1016/0375-9474(86)90308-8
1986VA12 Nucl.Phys. A454, 288 (1986) Electron Scattering in the Microscopic Sp(3, R) Model NUCLEAR REACTIONS 20Ne(e, e), (e, e'), E not given; calculated longitudinal, transverse form factors. Microscopic Sp(3, R) models.
doi: 10.1016/0375-9474(86)90270-8
1984PA04 Nucl.Phys. A414, 93 (1984) P.Park, J.Carvalho, M.Vassanji, D.J.Rowe, G.Rosensteel The Shell-Model Theory of Nuclear Rotational States NUCLEAR STRUCTURE 126Ba, 154Sm, 166Er, 164Yb; calculated levels, deformation parameters, moments of inertia, B(E2). 166Er, 20Ne, 126Ba; calculated deformed intrinsic state spectral decomposition. Symplectic model.
doi: 10.1016/0375-9474(84)90499-8
1984VA25 Nucl.Phys. A426, 205 (1984) The Geometric SO(3) x D Model: A practical microscopic theory of quadrupole collective motion NUCLEAR STRUCTURE 24Mg; calculated binding energy, B(E2), quadrupole moment, rms radius. Geometric SO(3)xD model.
doi: 10.1016/0375-9474(84)90105-2
1983RO17 Prog.Theor.Phys.(Kyoto), Suppl. 74/75, 306 (1983) The Hydrodynamic Limit of the Microscopic Collective Model - The U(3)-Boson Model - NUCLEAR STRUCTURE 20Ne, 16O, 40Ca; calculated levels; deduced microscopic collective model hydrodynamic limit.
doi: 10.1143/PTPS.74.306
1983VA13 Phys.Lett. 125B, 103 (1983) Application of the Microscopic sp(3, R) Model to the Giant Monopole and Quadrupole Resonances in 16O NUCLEAR STRUCTURE 16O; calculated binding energy, levels, quadrupole moment, B(E2), B(E0), rms radii; deduced giant resonances. Microscopic sp(3, R) model.
doi: 10.1016/0370-2693(83)91244-3
1983VA16 Phys.Lett. 127B, 1 (1983) Application of the SO(3) x D Model to the Ground-State Rotational Band of 20Ne NUCLEAR STRUCTURE 20Ne; calculated binding energy, quadrupole moment, B(E2), ground state rotational band. Microscopic model, SO(3)xD six dimensional space.
doi: 10.1016/0370-2693(83)91617-9
1982CA18 Phys.Lett. 119B, 249 (1982) J.Carvalho, P.Park, D.J.Rowe, G.Rosensteel Rotational Bands in the Stretched sp(3, R) Approximation NUCLEAR STRUCTURE 126Ba, 154Sm, 164Yb, 166Er; calculated levels, rotational bands, deformation, B(E2), moments of inertia. Stretched sp(3, R) approximation.
doi: 10.1016/0370-2693(82)90663-3
1982RO06 Phys.Rev. C25, 3236 (1982) Rotational Bands in the u(3)-Boson Model NUCLEAR STRUCTURE 20Ne; calculated levels, B(E2). Collective theory, boson models.
doi: 10.1103/PhysRevC.25.3236
1982VA15 Phys.Lett. 115B, 77 (1982) The Geometric SO(3) X D Model NUCLEAR STRUCTURE 4He, 8Be, 16O, 20Ne; calculated energy vs deformation parameter. Hartree-Fock calculation, submodel of Sp(3, R).
doi: 10.1016/0370-2693(82)90799-7
1981RO04 Phys.Rev.Lett. 46, 1119 (1981) Collective Rotational States in the Symplectic Shell Model NUCLEAR STRUCTURE 156Gd; calculated rotational bands. Microscopic, algebraic models, irrotational, rigid limits.
doi: 10.1103/PhysRevLett.46.1119
1981RO06 Phys.Rev.Lett. 47, 223 (1981) u(3)-Boson Model of Nuclear Collective Motion NUCLEAR STRUCTURE 16O, 40Ca; calculated levels. Collective motion, u(3) boson model.
doi: 10.1103/PhysRevLett.47.223
1979NG01 Nucl.Phys. A313, 15 (1979) C.Ngo-Trong, T.Suzuki, D.J.Rowe The Tensor Open-Shell Random Phase Approximation with Application to the Even Nickel Isotopes NUCLEAR STRUCTURE 58,60,62,64Ni; calculated energy levels, isoscalar, electromagnetic transition rates in tensor open-shell RPA.
doi: 10.1016/0375-9474(79)90566-9
1978RO07 Nucl.Phys. A298, 31 (1978) D.J.Rowe, S.S.M.Wong, H.Chow, J.B.McGrory Isovector M6 Excitations in the Open-Shell Random Phase Approximation NUCLEAR STRUCTURE 20Ne, 24Mg, 28Si, 32S, 36Ar, 40Ca; calculated isovector m6 excitations.
doi: 10.1016/0375-9474(78)90005-2
1977SU03 Nucl.Phys. A286, 307 (1977) Sum Rule for the Current Density and Nuclear Hydrodynamic Models NUCLEAR STRUCTURE 12C, 16O, 40Ca; calculated transition current densities.
doi: 10.1016/0375-9474(77)90410-9
1977SU06 Nucl.Phys. A292, 93 (1977) Comments on Electroexcitation of Deformed Nuclei NUCLEAR STRUCTURE 152Sm; calculated transition density.
doi: 10.1016/0375-9474(77)90360-8
1977ZA02 Phys.Rev.Lett. 38, 750 (1977) H.Zarek, B.O.Pich, T.E.Drake, D.J.Rowe, W.Bertozzi, C.Creswell, A.Hirsch, M.V.Hynes, S.Kowalski, B.Norum, F.N.Rad, C.P.Sargent, C.F.Williamson, R.A.Lindgren Discovery of a 6-, T = 1 Resonance in 24Mg via High-Resolution Inelastic Electron Scattering NUCLEAR REACTIONS 24Mg(e, e'), E=108-260 MeV; measured spectra. 24Mg deduced resonance, J, π, t.
doi: 10.1103/PhysRevLett.38.750
1975GU02 Nucl.Phys. A238, 225 (1975) Upper and Lower Bounds for the Quadrupole Moment and Octupole Strength Of the First Excited 3- State in 208Pb NUCLEAR STRUCTURE 208Pb; calculated quadrupole moment.
doi: 10.1016/0375-9474(75)90350-4
1974AY01 Nucl.Phys. A218, 307 (1974) Application of Infinite Oscillator Shell Model Calculations to the Description of Nuclear Reactions NUCLEAR REACTIONS 15N(n, n); measured nothing, calculated σ, phase shifts.
doi: 10.1016/0375-9474(74)90006-2
1974LO04 Nucl.Phys. A219, 171 (1974) N.Lo Iudice, D.J.Rowe, S.S.M.Wong 'Exact' Shell Model Calculations in A = 17 and A = 18 Nuclei and Effective Operators in the (2s, 1d) Shell NUCLEAR STRUCTURE A=17-18; calculated E2 effective charge, B(E2).
doi: 10.1016/0375-9474(74)90090-6
1974NA01 Nucl.Phys. A218, 495 (1974) O.Nalcioglu, D.J.Rowe, C.Ngo-Trong Excitation of the T > Components of the Giant Dipole States in N > Z Nuclei by Muon Capture NUCLEAR REACTIONS 58,60,62,64Ni(μ-, ν); measured nothing, calculated σ.
doi: 10.1016/0375-9474(74)90037-2
1974WO02 Phys.Lett. 48B, 403 (1974) S.S.M.Wong, D.J.Rowe, J.C.Parikh Calculations of the Giant Dipole Resonance for sd-Shell Nuclei in the Open-Shell Random Phase Approximation NUCLEAR STRUCTURE 16O, 20Ne, 24Mg, 28Si, 32S, 36Ar, 40Ca; calculated giant dipole resonance.
doi: 10.1016/0370-2693(74)90364-5
1973GU11 Phys.Rev. C8, 1154 (1973) Effect of Vibrational Correlations on the Moment of Inertia in a Generalized Skyrme-Levinson Model NUCLEAR STRUCTURE 28Si; calculated moment of inertia, binding energy for prolate, oblate shapes.
doi: 10.1103/PhysRevC.8.1154
1973RO12 Phys.Lett. 44B, 155 (1973) Is Hartree-Fock Self-Consistency Important in Particle-Hole Calculations(Question) NUCLEAR STRUCTURE 16O calculated particle-hole excitations. Hartree-Fock.
doi: 10.1016/0370-2693(73)90508-X
1971LO23 Phys.Lett. 37B, 44 (1971) N.Lo Iudice, D.J.Rowe, S.S.M.Wong A Shell-Model Calculation of the Mass 18 Nuclei and the Effective Interaction in the sh-Shell NUCLEAR STRUCTURE 18O, 18F; calculated levels. Shell model Kuo-Brown G-matrix elements.
doi: 10.1016/0370-2693(71)90565-X
1971NG02 Phys.Lett. 36B, 553 (1971) Isospin Structure of the Giant Dipole Resonance of the Even Isotopes of Nickel; a Microscopic Calculation Based on the Equations-of-Motion Formalism NUCLEAR STRUCTURE 58,60,62,64Ni; calculated isospin structure of giant dipole resonance. p-H approximation, equations-of-motion formalism.
doi: 10.1016/0370-2693(71)90087-6
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
1970RO01 Nucl.Phys. A140, 74 (1970) The Nature of the Hartree-Fock Energy Gap in Finite Nuclei NUCLEAR STRUCTURE 28Si; calculated levels, Hartree-Fock energy gap.
doi: 10.1016/0375-9474(70)90885-7
1970RO18 Nucl.Phys. A152, 273 (1970) How Do Deformed Nuclei Rotate (Question) NUCLEAR STRUCTURE 156Gd, 160Dy; calculated ground-state rotational band.
doi: 10.1016/0375-9474(70)90830-4
1970RO20 Nucl.Phys. A153, 561 (1970) The Open-Shell Random-Phase Approximation and the Negative Parity Excitations of 12C NUCLEAR STRUCTURE 12C; calculated negative-parity levels. Open-shell RPA.
doi: 10.1016/0375-9474(70)90792-X
1969RO26 Phys.Letters 30B, 147 (1969) Open-Shell RPA Calculations for the Giant-Dipole Excitations of 12C NUCLEAR STRUCTURE 12C; calculated giant dipole excitations. Open-shell random phase approximation.
doi: 10.1016/0370-2693(69)90351-7
1969UL02 Phys.Rev. 188, 1640 (1969) Investigation of Octupole Correlations in O16 NUCLEAR STRUCTURE 16O; calculated levels, ground-state correlation energy. Shell-model Hamiltonian, octupole-octupole interaction.
doi: 10.1103/PhysRev.188.1640
1969WO05 Phys.Letters 30B, 150 (1969) The Giant Dipole Excitations of 12C in the Open Shell Tamm-Dancoff Approximation and in the Intermediate-Coupling Shell Model NUCLEAR STRUCTURE 12C; calculated giant dipole excitations. Tamm-Dancoff approximation, intermediate-coupling shell-model.
doi: 10.1016/0370-2693(69)90352-9
1965RO03 Nucl.Phys. 61, 1 (1965) A Calculation of Some ΔK = ± 2 Band-Mixing Effects in the Odd-Mass Nucleus W183 NUCLEAR STRUCTURE 183W; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(65)90929-6
1964NE06 Nucl.Phys. 53, 433 (1964) D.Newton, A.B.Clegg, G.L.Salmon, D.J.Rowe The 11B(p, p') Reaction at 150 MeV and the Unified Model of 11B NUCLEAR STRUCTURE 11B; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(64)90623-6
1964RO23 Nucl.Phys. 54, 193 (1964) D.J.Rowe, G.L.Salmon, A.B.Clegg, D.Newton Distorted Wave Effects and the Impulse Approximation In the Inelastic Scattering of 147 MeV Protons from C12 NUCLEAR REACTIONS 12C(p, p'), E=147 MeV; measured products, 12C; deduced σ(θ). Data were imported from EXFOR entry O0356.
doi: 10.1016/0029-5582(64)90405-5
1963RO30 Proc.Phys.Soc.(London) 81, 332 (1963) D.J.Rowe, A.B.Clegg, G.L.Salmon, D.Newton The 40Ca(p, p') Reaction at 150 MeV NUCLEAR STRUCTURE 40Ca; measured not abstracted; deduced nuclear properties.
doi: 10.1088/0370-1328/81/2/315
1962RO25 Proc.Phys.Soc.(London) 80, 1205 (1962) D.J.Rowe, A.B.Clegg, G.L.Salmon, P.S.Fisher The 16O(p, p') Reaction at 150 MeV NUCLEAR REACTIONS 16O(p, p'), E=150 MeV; measured reaction products, Eγ, Iγ; deduced σ(θ), σ(θ, E), levels, J, π, angular correlations between the gamma rays and the protons. The Atomic Energy Research Establishment cyc lotron.
doi: 10.1088/0370-1328/80/6/301
1962SA05 Proc.Phys.Soc.(London) 79, 14 (1962) G.L.Salmon, A.B.Clegg, K.J.Foley, P.S.Fisher, D.J.Rowe NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
1961AU04 Proc.Rutherford Jubilee Intern.Conf., Manchester, England, J.B.Birks, Ed., Academic Press, New York, p.139 (1961) S.M.Austin, G.L.Salmon, D.J.Rowe, A.B.Clegg, D.Newton, K.J.Foley The 12C(n, np)11B, 12C(p, pn)11C and 12C(p, 2p)11B Reactions Induced by Nucleons of 120-150 MeV NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset21459. 1961RO27 Proc.Rutherford Jubilee Intern.Conf., Manchester, England, J.B.Birks, Ed., Academic Press Inc., New York, p.145 (1961) D.J.Rowe, G.L.Salmon, A.B.Clegg, D.Newton Gamma-Rays from Inelastic Scattering of High Energy Protons from Carbon NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
1961RO28 Proc.Rutherford Jubilee Intern.Conf., Manchester, England, J.B.Birks, Ed., Academic Press Inc., New York, p.271 (1961) D.J.Rowe, A.B.Clegg, G.L.Salmon, D.Newton Inelastic Scattering of 150 MeV Protons from 40Ca NUCLEAR STRUCTURE 40Ca; measured not abstracted; deduced nuclear properties.
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