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NSR database version of April 11, 2024.

Search: Author = D.J.Rowe

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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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2018RO07      J.Phys.(London) G45, 06LT01 (2018)

D.J.Rowe, J.L.Wood

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2009TH02      Eur.Phys.J. A 41, 189 (2009)

G.Thiamova, D.J.Rowe

Large boson number IBM calculations and their relationship to the Bohr model

doi: 10.1140/epja/i2009-10810-x
Citations: PlumX Metrics

2007RO25      Nucl.Phys. A797, 94 (2007)

G.Rosensteel, D.J.Rowe

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2006TH04      Czech.J.Phys. 56, 341 (2006)

G.Thiamova, D.J.Rowe

Persistence of rotational bands in a coupled SU(3) model

doi: 10.1007/s10582-006-0095-5
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2006TH14      Int.J.Mod.Phys. E15, 1741 (2006)

G.Thiamova, D.J.Rowe

Persistence of rotational structure in nuclei and quasi-dynamical symmetry

doi: 10.1142/S0218301306005551
Citations: PlumX Metrics

2005RO09      Nucl.Phys. A753, 94 (2005)

D.J.Rowe, P.S.Turner

The algebraic collective model

doi: 10.1016/j.nuclphysa.2005.01.032
Citations: PlumX Metrics

2005RO24      Nucl.Phys. A759, 92 (2005)

G.Rosensteel, D.J.Rowe

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
Citations: PlumX Metrics

2005RO34      Nucl.Phys. A760, 59 (2005)

D.J.Rowe, G.Thiamova

The many relationships between the IBM and the Bohr model

doi: 10.1016/j.nuclphysa.2005.06.001
Citations: PlumX Metrics

2005TH08      Czech.J.Phys. 55, 957 (2005)

G.Thiamova, D.J.Rowe

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
Citations: PlumX Metrics

2005TU05      Nucl.Phys. A756, 333 (2005)

P.S.Turner, D.J.Rowe

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2004RO17      Nucl.Phys. A735, 372 (2004)


A computationally tractable version of the collective model

doi: 10.1016/j.nuclphysa.2004.02.018
Citations: PlumX Metrics

2004RO31      Phys.Rev.Lett. 93, 122502 (2004)


Quasidynamical Symmetry in an Interacting Boson Model Phase Transition

doi: 10.1103/PhysRevLett.93.122502
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2003RO01      Phys.Rev. C 67, 014303 (2003)

G.Rosensteel, D.J.Rowe

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
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2001RO28      Phys.Rev.Lett. 87, 172501 (2001)

D.J.Rowe, G.Rosensteel

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
Citations: PlumX Metrics

2000BA03      Nucl.Phys. A662, 125 (2000)

C.Bahri, D.J.Rowe

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
Citations: PlumX Metrics

2000RO02      Phys.Lett. 472B, 227 (2000)

D.J.Rowe, S.Bartlett, C.Bahri

Angular-Momentum Projection of Rotational Model Wave Functions

doi: 10.1016/S0370-2693(99)01448-3
Citations: PlumX Metrics

1999RO07      J.Phys.(London) G25, 635 (1999)


Macroscopic and Microscopic Models of Nuclear Rotations

doi: 10.1088/0954-3899/25/4/011
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1998DE28      Nucl.Phys. A636, 47 (1998)

H.de Guise, D.J.Rowe

An Algebraic Representation of the Particle-Plus-Rotor Model

doi: 10.1016/S0375-9474(98)00169-9
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1997CA17      Nucl.Phys. A618, 65 (1997)

M.J.Carvalho, D.J.Rowe

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
Citations: PlumX Metrics

1995CH10      Nucl.Phys. A582, 181 (1995)

H.Chen, T.Song, D.J.Rowe

The Pair-Coupling Model

doi: 10.1016/0375-9474(94)00472-Y
Citations: PlumX Metrics

1995DE19      Nucl.Phys. A589, 58 (1995)

H.de Guise, D.J.Rowe

Rotor Plus SU(3)-Particle with Spin

doi: 10.1016/0375-9474(95)00027-X
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1994RO03      Nucl.Phys. A570, 279c (1994)


The Microscopic Theory of Nuclear Collective Motion

doi: 10.1016/0375-9474(94)90293-3
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1992CA24      Nucl.Phys. A548, 1 (1992)

J.Carvalho, D.J.Rowe

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
Citations: PlumX Metrics

1991JA05      Nucl.Phys. A528, 409 (1991)

M.Jarrio, J.L.Wood, D.J.Rowe

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1987VA12      Nucl.Phys. A466, 227 (1987)

M.G.Vassanji, D.J.Rowe

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1986VA12      Nucl.Phys. A454, 288 (1986)

M.G.Vassanji, D.J.Rowe

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1984VA25      Nucl.Phys. A426, 205 (1984)

M.G.Vassanji, D.J.Rowe

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1983VA13      Phys.Lett. 125B, 103 (1983)

M.G.Vassanji, D.J.Rowe

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
Citations: PlumX Metrics

1983VA16      Phys.Lett. 127B, 1 (1983)

M.G.Vassanji, D.J.Rowe

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1982RO06      Phys.Rev. C25, 3236 (1982)

D.J.Rowe, G.Rosensteel

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
Citations: PlumX Metrics

1982VA15      Phys.Lett. 115B, 77 (1982)

M.Vassanji, D.J.Rowe

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
Citations: PlumX Metrics

1981RO04      Phys.Rev.Lett. 46, 1119 (1981)

G.Rosensteel, D.J.Rowe

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
Citations: PlumX Metrics

1981RO06      Phys.Rev.Lett. 47, 223 (1981)

G.Rosensteel, D.J.Rowe

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1977SU03      Nucl.Phys. A286, 307 (1977)

T.Suzuki, D.J.Rowe

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
Citations: PlumX Metrics

1977SU06      Nucl.Phys. A292, 93 (1977)

T.Suzuki, D.J.Rowe

Comments on Electroexcitation of Deformed Nuclei

NUCLEAR STRUCTURE 152Sm; calculated transition density.

doi: 10.1016/0375-9474(77)90360-8
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1975GU02      Nucl.Phys. A238, 225 (1975)

M.Guidetti, D.J.Rowe, H.Chow

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
Citations: PlumX Metrics

1974AY01      Nucl.Phys. A218, 307 (1974)

A.A.Ayad, D.J.Rowe

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1973GU11      Phys.Rev. C8, 1154 (1973)

K.K.Gupta, N.Ullah, D.J.Rowe

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1971NG02      Phys.Lett. 36B, 553 (1971)

C.Ngo-Trong, D.J.Rowe

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1970RO20      Nucl.Phys. A153, 561 (1970)

D.J.Rowe, S.S.M.Wong

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
Citations: PlumX Metrics

1969RO26      Phys.Letters 30B, 147 (1969)

D.J.Rowe, S.S.M.Wong

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
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1969UL02      Phys.Rev. 188, 1640 (1969)

N.Ullah, D.J.Rowe

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
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1969WO05      Phys.Letters 30B, 150 (1969)

S.S.M.Wong, D.J.Rowe

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
Citations: PlumX Metrics

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
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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
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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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0356.

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
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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
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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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