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Search: Author = B.J.Cole

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1999CO06      Phys.Rev. C59, 726 (1999)

B.J.Cole

Predicted Proton and Two-Proton Decay Energies for Nuclei in the Upper fp Shell

NUCLEAR STRUCTURE Z=31-42; calculated binding energies, proton and two-proton separation energies for proton-rich isotopes.

doi: 10.1103/PhysRevC.59.726
Citations: PlumX Metrics

1998CO30      Phys.Rev. C58, 2831 (1998)

B.J.Cole

Proton and Two-Proton Drip Lines in the sd Shell

NUCLEAR STRUCTURE ^21,22Al, ^22,23Si, ^23,24,25,26P, ^25,26,27,28S, ^27,28,29,30Cl, ^29,30,31Ar, ^31,32,33,34K, ^32,33,34,35Ca; calculated binding energies, one-, two-proton separation energies; deduced proton, diproton drip lines.

doi: 10.1103/PhysRevC.58.2831
Citations: PlumX Metrics

1998CO42      Mod.Phys.Lett. A 13, 2705 (1998)

B.J.Cole, H.G.Miller, R.M.Quick

Quadrupole Deformation in Nuclei at Finite Temperature

NUCLEAR MOMENTS ²⁰Ne; calculated intrinsic quadrupole moment, deformation vs temperature. Mean-field approach.

doi: 10.1142/S0217732398002874
Citations: PlumX Metrics

1997CO19      Phys.Rev. C56, 1866 (1997)

B.J.Cole

Systematics of Proton and Diproton Separation Energies for Light Nuclei

NUCLEAR STRUCTURE Z=16-22; analyzed generalized Coulomb shift; ^30,31Ar, ^32,33,34K, ^33,34,35Ca, ^37,38Sc, ^38,39,40Ti, ^42,43,44V, ^{41,42,43,44,45}Cr; calculated one-, two-proton separation energies.

doi: 10.1103/PhysRevC.56.1866
Citations: PlumX Metrics

1996CO14      Phys.Rev. C54, 1240 (1996)

B.J.Cole

Stability of Proton-Rich Nuclei in the Upper sd Shell and Lower pf Shell

NUCLEAR STRUCTURE A=37-55; calculated proton-rich nuclei binding energy, single-, diproton-separation energies. A=34-55; calculated β⁺-decay endpoint energies.

doi: 10.1103/PhysRevC.54.1240
Citations: PlumX Metrics

1994CO13      Phys.Rev. C50, 1913 (1994)

B.J.Cole, N.J.Davidson, H.G.Miller

Determination of Nuclear Level Densities from Experimental Information

doi: 10.1103/PhysRevC.50.1913
Citations: PlumX Metrics

1992QU02      Nuovo Cim. 105A, 913 (1992)

R.M.Quick, B.J.Cole, H.G.Miller

Effect of Model Space Size on Finite-Temperature Hartree-Fock Calculations

NUCLEAR STRUCTURE ²⁰Ne, ²⁴Mg; calculated energy, entropy, specific heat; deduced model space effects. Finite temperature Hartree-Fock approximation.

doi: 10.1007/BF02730832
Citations: PlumX Metrics

1991CO11      Phys.Rev. C44, 190 (1991)

B.J.Cole

Empirical Effective Interactions in the Lower fp Shell and Upper sd Shell

NUCLEAR STRUCTURE A=28-64; analyzed data; deduced effective interaction centroids.

doi: 10.1103/PhysRevC.44.190
Citations: PlumX Metrics

1991QU01      Phys.Lett. 254B, 303 (1991)

R.M.Quick, N.J.Davidson, B.J.Cole, H.G.Miller

The Observation of Nuclear Shape Transitions at Fixed Angular Momentum

NUCLEAR STRUCTURE ²⁴Mg; calculated shapes vs spin, temperature; deduced shape transition features. Cranked finite temperature Hartree-Fock.

doi: 10.1016/0370-2693(91)91159-S
Citations: PlumX Metrics

1990CO02      Phys.Rev. C41, 386 (1990)

B.J.Cole

Information on Effective Interactions from Experimental Single-Particle Energies

NUCLEAR STRUCTURE A=28-56; analyzed single particle energies; deduced effective interaction features.

doi: 10.1103/PhysRevC.41.386
Citations: PlumX Metrics

1990CO04      Phys.Rev. C41, 789 (1990)

B.J.Cole, H.G.Miller, R.M.Quick

Effect of the Continuum on Thermally Induced Phase Transitions in Nuclei

NUCLEAR STRUCTURE ²⁰Ne, ¹⁶O, ²⁴Mg; calculated specific heat vs temperature. Continuum effects, thermally induced phase transitions.

doi: 10.1103/PhysRevC.41.789
Citations: PlumX Metrics

1990CO18      Phys.Rev. C42, 625 (1990)

B.J.Cole

Centroids of Effective Interactions from Measured Single-Particle Energies: An application

NUCLEAR STRUCTURE A=28-64; analyzed single particle energies; deduced effective interaction centroids.

doi: 10.1103/PhysRevC.42.625
Citations: PlumX Metrics

1989CO10      Phys.Rev. C40, 456 (1989)

B.J.Cole, R.M.Quick, H.G.Miller

Shape of ²⁴Mg at Zero and Finite Temperature

NUCLEAR STRUCTURE ²⁴Mg; calculated ground state deformation. Hartree-Fock-Rothaan calculations.

doi: 10.1103/PhysRevC.40.456
Citations: PlumX Metrics

1989MI05      Phys.Rev. C39, 1599 (1989)

H.G.Miller, R.M.Quick, B.J.Cole

Nuclear Shape Transitions at Finite Temperature

NUCLEAR STRUCTURE ²⁴Mg; calculated shapes, quadrupole moment, specific heat vs temperature. Finite temperature mean field approach.

doi: 10.1103/PhysRevC.39.1599
Citations: PlumX Metrics

1989MI18      Phys.Rev.Lett. 63, 1922 (1989)

H.G.Miller, B.J.Cole, R.M.Quick

Evidence for Phase Transitions in Finite Systems

NUCLEAR STRUCTURE ²⁰Ne; calculated specific heat vs temperature; deduced phase transition evidence.

doi: 10.1103/PhysRevLett.63.1922
Citations: PlumX Metrics

1989QU01      Phys.Rev. C40, 993 (1989)

R.M.Quick, H.G.Miller, B.J.Cole

Reliability of the Finite Temperature Hartree-Fock Approximation

NUCLEAR STRUCTURE ²⁰Ne; calculated internal energy average ensemble. Finite temperature Hartree-Fock approximation.

doi: 10.1103/PhysRevC.40.993
Citations: PlumX Metrics

1988CO01      J.Phys.(London) G14, 37 (1988)

B.J.Cole

Coulomb Energies for Multi-Orbital Shell-Model Calculations

NUCLEAR STRUCTURE A=37-47; calculated ground state binding energies. ^34,35,36Cl, ^36,38Ar, ^42,43Ca, ⁴³Sc, ^45,47Ca; calculated excited state Coulomb energies differences. ³³S, ^35,36,33Cl, ^35,36,37Ar, ^37,39K, ^39,41Ca, ^41,43Sc, ^43,45Ti, ^45,47V, ⁴⁷Cr, ⁵⁵Co, ⁵⁵Ni; calculated parent, analog state energies. Multi-orbital shell model.

doi: 10.1088/0305-4616/14/1/008
Citations: PlumX Metrics

1985CO02      Phys.Lett. 150B, 21 (1985)

B.J.Cole

Constraints on Matrix Elements of the Effective Nucleon-Nucleon Interaction for Nuclei Around Mass 40

NUCLEAR STRUCTURE ⁴⁰Ca, ^40,46K; calculated effective nucleon-nucleon interaction matrix elements; deduced constraints.

doi: 10.1016/0370-2693(85)90129-7
Citations: PlumX Metrics

1985CO04      J.Phys.(London) G11, 351 (1985)

B.J.Cole

Coulomb Contribution to Shell-Model Binding Energies

NUCLEAR STRUCTURE A=33-39, 42-54; calculated Coulomb displacement energies, Coulomb corrected binding energies.

doi: 10.1088/0305-4616/11/3/013
Citations: PlumX Metrics

1985CO12      J.Phys.(London) G11, 953 (1985)

B.J.Cole

The Structure of Low-Lying Negative-Parity States of ⁴⁵Sc

NUCLEAR STRUCTURE ⁴⁵Sc; measured levels, B(λ), ground state μ, quadrupole moment. Shell model.

doi: 10.1088/0305-4616/11/8/011
Citations: PlumX Metrics

1985CO13      J.Phys.(London) G11, 961 (1985)

B.J.Cole

Shell-Model Calculations for Negative-Parity States of ⁴⁵Ca

NUCLEAR STRUCTURE ⁴⁵Ca; calculated levels, T_1/2, δ, γ-branching ratio, ground state μ, quadrupole moment. Shell model.

doi: 10.1088/0305-4616/11/8/012
Citations: PlumX Metrics

1985MI02      Phys.Lett. 150B, 15 (1985)

H.G.Miller, B.J.Cole

Calculation of Interband Level Spacings in the Constrained Hartree-Fock Approach

NUCLEAR STRUCTURE ²⁴Mg; calculated T=0, 8⁺ levels, interband level spacings. Constrained Hartree-Fock.

doi: 10.1016/0370-2693(85)90127-3
Citations: PlumX Metrics

1981CO01      J.Phys.(London) G7, 25 (1981)

B.J.Cole

Shell-Model Studies of Mass-45 Nuclei and Calcium Isotopes A=46-50: energy spectra and electromagnetic moments

NUCLEAR STRUCTURE ⁴⁵Ti, ⁴⁵Sc, ^{45,46,47,48,49,50}Ca; calculated levels, binding energies, wave functions, quadrupole moment, μ. Shell model, modified Kuo-Brown interaction.

doi: 10.1088/0305-4616/7/1/007
Citations: PlumX Metrics

1981CO09      J.Phys.(London) G7, 173 (1981)

B.J.Cole

Shell-Model Spectroscopic Factors for Reactions Involving A=45 Nuclei and Calcium Isotopes A=44-49

NUCLEAR STRUCTURE ^44,45,47,49Ca, ^44,45Sc; calculated levels, J, π, S. Shell-model, modified Kuo-Brown interactions, fp-shell configuration space.

doi: 10.1088/0305-4616/7/2/009
Citations: PlumX Metrics

1979CO06      Nucl.Phys. A318, 507 (1979)

B.J.Cole, C.Toepffer

Intermediate Structure in Heavy-Ion Reactions

NUCLEAR REACTIONS ¹²C(¹²C, ¹²C), (¹²C, γ), (¹²C, n), (¹²C, p), (¹²C, d), (¹²C, α), E(cm)=19.5 MeV; calculated σ; discussed reaction mechanism, continuum shell model.

doi: 10.1016/0375-9474(79)90663-8
Citations: PlumX Metrics

1977CO11      Phys.Rev.Lett. 39, 3 (1977)

B.J.Cole, C.Toepffer, K.Dietrich

Schematic Model for Continuum Resonances in Heavy-Ion Reactions

NUCLEAR REACTIONS ¹²C(¹²C, p), E(cm)=19.3 MeV; analyzed reaction mechanism. ²⁴Mg resonances deduced explanation of small widths.

doi: 10.1103/PhysRevLett.39.3
Citations: PlumX Metrics

1977CO16      J.Phys.(London) G3, 919 (1977)

B.J.Cole, D.Kelvin, A.Watt, R.R.Whitehead

Shell-Model Calculations in the sd Shell: VIII. High-Spin States in ²³Na

NUCLEAR STRUCTURE ²³Na; calculated levels, B(E2), B(M1), branching, δ, T_1/2. Shell model, preedom-wildenthal interaction.

doi: 10.1088/0305-4616/3/7/006
Citations: PlumX Metrics

1976CO19      J.Phys.(London) G2, 501 (1976)

B.J.Cole, A.Watt, R.R.Whitehead

Shell-Model Calculations in the sd Shell: VII. Spectroscopic Factors for A = 23-31 Nuclei

NUCLEAR STRUCTURE ^23,24,25Na, ²³Ne, ^24,25,26,27Mg, ^26,27,28,29Al, ^28,29,30,31Si, ^30,31P; calculated S. Shell-model method. Preedom-Wildenthal interaction.

doi: 10.1088/0305-4616/2/7/010
Citations: PlumX Metrics

1976CO22      J.Phys.(London) G2, 541 (1976)

B.J.Cole

Large-Basis Shell-Model Calculations for ²⁵Mg

NUCLEAR STRUCTURE ²⁵Mg; calculated levels, B(E4), B(E2), B(M1), T_1/2, δ, branching. Shell-model method. Preedom-Wildenthal interaction.

doi: 10.1088/0305-4616/2/8/006
Citations: PlumX Metrics

1975CO01      J.Phys.(London) G1, 17 (1975)

B.J.Cole, A.Watt, R.R.Whitehead

Shell-Model Calculations in the sd Shell III. The Structure of Mass 25 Nuclei

NUCLEAR STRUCTURE ²⁵Na, ²⁵Al, ²⁵Mg; calculated levels, B(λ).

doi: 10.1088/0305-4616/1/1/005
Citations: PlumX Metrics

1975CO02      J.Phys.(London) G1, 213 (1975)

B.J.Cole, A.Watt, R.R.Whitehead

Shell-Model Calculations in the sd Shell. IV. Energy Spectra for A = 26-31 Nuclei

NUCLEAR STRUCTURE ^26,28,29Al, ^26,27,28Mg, ^28,30,31Si, ^30,31P; calculated levels, shell-model method; Kuo, Preedom-Wildenthal interactions.

doi: 10.1088/0305-4616/1/2/008
Citations: PlumX Metrics

1975CO03      Phys.Lett. 55B, 11 (1975)

B.J.Cole, A.Watt, R.R.Whitehead

How Pure Are Shell-Model Wavefunctions (Question)

NUCLEAR STRUCTURE ²³Na; calculated level properties.

doi: 10.1016/0370-2693(75)90173-2
Citations: PlumX Metrics

1975CO07      J.Phys.(London) G1, 303 (1975)

B.J.Cole, A.Watt, R.R.Whitehead

Shell-Model Calculations in the sd Shell V. The Structure of Mass-23 Nuclei

NUCLEAR STRUCTURE ²³Na, ²³Mg, ²³Ne; calculated levels, B(E2), B(M1), quadrupole moment, μ. Shell-model method. Kuo, Preedom-Wildenthal interactions.

doi: 10.1088/0305-4616/1/3/006
Citations: PlumX Metrics

1975CO17      J.Phys.(London) G1, 935 (1975)

B.J.Cole, A.Watt, R.R.Whitehead

Shell-Model Calculations of the sd Shell: VI. The Structure of Mass 27 and 29 Nuclei

NUCLEAR STRUCTURE ²⁷Mg, ^27,29Al, ^27,29Si, ²⁹P; calculated levels, B(E2), B(M1), quadrupole moment, μ, T_1/2, δ, branching. Shell-model method. Preedom-Wildenthal, Kuo interactions.

doi: 10.1088/0305-4616/1/9/005
Citations: PlumX Metrics

1975MO10      Nucl.Phys. A243, 365 (1975)

K.Mohring, R.Lipperheide, B.J.Cole

Neutron Transfer into Resonant States

NUCLEAR REACTIONS ¹⁵N, ³²S, ²⁴Mg(n, X), ¹⁵N, ³²S, ²⁴Mg(d, p), E=12 MeV; calculated σ.

doi: 10.1016/0375-9474(75)90284-5
Citations: PlumX Metrics

1974CO15      Phys.Lett. 49B, 133 (1974)

B.J.Cole, A.Watt, R.R.Whitehead

Rotational Band Shifts in ²⁵Mg and ²⁶Al

NUCLEAR STRUCTURE ^24,25Mg, ²⁶Al; calculated levels.

doi: 10.1016/0370-2693(74)90490-0
Citations: PlumX Metrics

1974CO39      J.Phys.(London) A7, 1374 (1974)

B.J.Cole, A.Watt, R.R.Whitehead

Shell-Model Calculations in the sd Shell I. Energy Spectra

NUCLEAR STRUCTURE ^19,20,21F, ¹⁹O, ^20,21,22,23Ne, ^{20,22,23,24,25}Na, ^24,26Mg, ^30,32P, ^30,31Si; calculated levels.

doi: 10.1088/0305-4470/7/12/003
Citations: PlumX Metrics

1974CO40      J.Phys.(London) A7, 1399 (1974)

B.J.Cole, A.Watt, R.R.Whitehead

Shell-Model Calculations in the sd Shell II. Mass Excesses and Energy Spectra of Exotic Nuclei

NUCLEAR STRUCTURE ^20,21,22,23O, ^22,23,24,25F, ^24,25,26,27Ne, ^{26,27,28,29,30}Na, ^28,29,30,31Mg, ^30,31Al, ^32,33Si; calculated levels, J, mass excess.

doi: 10.1088/0305-4470/7/12/004
Citations: PlumX Metrics

1974WA17      Phys.Lett. 51B, 435 (1974)

A.Watt, B.J.Cole, R.R.Whitehead

Towards an Improved Effective Interaction

NUCLEAR STRUCTURE ^17,18O, ¹⁸F; calculated levels. ¹⁶O calculated binding energies.

doi: 10.1016/0370-2693(74)90302-5
Citations: PlumX Metrics

1973CO20      Phys.Lett. 45B, 429 (1973)

B.J.Cole, A.Watt, R.R.Whitehead

The Kuo Interaction and Band Shifts in the sd-Shell

NUCLEAR STRUCTURE ^23,24Na, ²⁶Al, ³³P; calculated levels, J, π.

doi: 10.1016/0370-2693(73)90635-7
Citations: PlumX Metrics

1973CO23      Phys.Lett. 46B, 55 (1973)

B.J.Cole, R.Huby

The Model-Independent Analysis of Stripping to Unbound Levels

NUCLEAR REACTIONS ¹²C(d, p), (n, n); calculated σ(E(cm)).

doi: 10.1016/0370-2693(73)90474-7
Citations: PlumX Metrics

1973CO27      J.Phys.(London) A6, 1224 (1973)

B.J.Cole, R.Huby, Q.K.K.Liu

The Application of the Real Weinberg State Method to Unbound Levels in ¹³C Formed by Neutron Scattering and (d, p) on ¹²C

NUCLEAR REACTIONS ¹²C(n, n), (d, p); calculated σ(E). ^12,13C calculated levels.

doi: 10.1088/0305-4470/6/8/017
Citations: PlumX Metrics

1971CO04      Phys.Rev.Lett. 26, 264 (1971)

B.J.Cole, R.Huby, J.R.Mines

Explanation of Some Stripping Transitions to Unbound Isobaric Analog States

NUCLEAR REACTIONS ^92,94,96Mo, ^90,92,96Zr(³He, d), ^92,94,96Mo(d, n), E not given; calculated σ. DWBA.

doi: 10.1103/PhysRevLett.26.264
Citations: PlumX Metrics

1970CO30      Phys.Lett. 33B, 320 (1970)

B.J.Cole, R.Huby, J.R.Mines

Method of Pseudo-Bound States for Stripping to Unbound Levels

NUCLEAR REACTIONS ¹⁵N(³He, d), E not given; ²⁰Ne, ⁴²Ca(d, n), E not given; measured nothing; analyzed σ(θ). ¹⁶O levels deduced S.

doi: 10.1016/0370-2693(70)90241-8
Citations: PlumX Metrics