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Search: Author = D.A.Bromley

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1992SH19      Phys.Rev. C46, 1946 (1992)

B.Shivakumar, D.J.Blumenthal, S.V.Greene, J.T.Mitchell, D.A.Bromley, D.Shapira, J.Gomez del Campo, A.Ray, M.M.Hindi

Evolution Towards Equilibration in Orbiting Interactions

NUCLEAR REACTIONS 16O(24Mg, 16O), E=75-115 MeV; measured backward angle yields of 16O, 12C nuclei; deduced yields energy dependence. Orbiting, transition state models.

doi: 10.1103/PhysRevC.46.1946
Citations: PlumX Metrics

1991GA08      Phys.Rev. C43, 2127 (1991)

M.Gai, M.Ruscev, D.A.Bromley, J.W.Olness

Spectroscopy of 18O: 14C(7Li, tγ)18O reaction; observation of selective enhanced E1 deexcitations of cluster states

NUCLEAR REACTIONS 14C(7Li, tγ), E=15 MeV; measured γt-coin. 14C(7Li, αγ), E=15 MeV; measured not given. 17N, 18O levels deduced γ-branching ratios.

doi: 10.1103/PhysRevC.43.2127
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1989GA01      Phys.Rev.Lett. 62, 874 (1989)

M.Gai, S.L.Rugari, R.H.France III, B.J.Lund, Z.Zhao, D.A.Bromley, B.A.Lincoln, W.W.Smith, M.J.Zarcone, Q.C.Kessel

Collective Band Structure and Origin of Enhanced E1 Decays in 18O

NUCLEAR REACTIONS 14C(α, γ), E=1.14 MeV; measured γ-spectra. 18O deduced transition, branching ratio, B(E2).

doi: 10.1103/PhysRevLett.62.874
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1988GA33      Phys.Lett. B 215, 242 (1988)

M.Gai, J.F.Ennis, D.A.Bromley, H.Emling, F.Azgui, E.Grosse, H.J.Wollersheim, C.Mittag, F.Riess

Enhanced E1 deexcitations in 218Ra and the evolution of reflection asymmetry at moderate spins

NUCLEAR REACTIONS 13C(208Pb, 3n), E=5.31 MeV/nucleon; measured Doppler-shifted Eγ, Iγ. 218Ra levels deduced T1/2, B(E1), B(E2). Recoil distance technique.

doi: 10.1016/0370-2693(88)91427-X
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1988SH03      Phys.Rev. C37, 652 (1988)

B.Shivakumar, D.Shapira, P.H.Stelson, S.Ayik, B.A.Harmon, K.Teh, D.A.Bromley

28Si + 14N Orbiting Interaction

NUCLEAR REACTIONS 14N(28Si, 14N), E=100 MeV; 14N(28Si, 16O), E=140 MeV; 14N(28Si, 12C), E=100-170 MeV; measured ejectile yields. 28Si(14N, X), E=100-170 MeV; measured orbiting σ(E) for X=10,11B, 11,12,13C, 13,14,15N, 15,16,17O, 17,18,19F, 19,20,21Ne; deduced critical angular momentum.

doi: 10.1103/PhysRevC.37.652
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1987CO10      Phys.Rev. C35, 1891 (1987)

P.D.Cottle, D.A.Bromley

Simple Parametrization for Octupole States in Spherical and Weakly Deformed Heavy Nuclei

NUCLEAR STRUCTURE Z=28-38; Z=32-38; Z=40-50; Z=50-64; Z=82-90; calculated single particle levels. Ra, Th deduced isotopes negative parity state characteristics. Simple parametrization of octupole phonon frequencies.

doi: 10.1103/PhysRevC.35.1891
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1987CO11      Phys.Rev. C35, 1939 (1987)

P.D.Cottle, M.Gai, J.F.Ennis, J.F.Shriner, Jr., S.M.Sterbenz, D.A.Bromley, C.W.Beausang, L.Hildingsson, W.F.Piel, Jr., D.B.Fossan, J.W.Olness, E.K.Warburton

Yrast States of 216Rn and the Extent of a Region of Possible Static Intrinsic Reflection Asymmetry

NUCLEAR REACTIONS 208Pb(14C, 2nα), E=67-68 MeV; measured Eγ, Iγ, γ(θ), γγ-, γ(X-ray)-coin. 216Rn deduced levels, J, π, yrast scheme. Hyperpure Ge, Ge(Li) detectors.

doi: 10.1103/PhysRevC.35.1939
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1987CO36      Phys.Rev. C36, 2286 (1987)

P.D.Cottle, M.Gai, J.F.Ennis, J.F.Shriner, Jr., D.A.Bromley, C.W.Beausang, L.Hildingsson, W.F.Piel, Jr., D.B.Fossan, J.W.Olness, E.K.Warburton

Level Spectrum of 219Ra and Weak Coupling in the Light Actinide Region

NUCLEAR REACTIONS, ICPND 208Pb(14C, 3n), E=60-78 MeV; measured Eγ, Iγ, γ(θ), I(ce), thick target yield, σ(E). 219Ra deduced levels, J, π, ICC, B(λ) ratios, γ-multipolarity. Weak coupling model.

doi: 10.1103/PhysRevC.36.2286
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1987GA15      Phys.Rev. C36, 1256 (1987)

M.Gai, R.Keddy, D.A.Bromley, J.W.Olness, E.K.Warburton

Spectroscopy of 18O: Radiative capture, 14C(α, γ)18O

NUCLEAR REACTIONS, ICPND 14C(α, γ), E=1.7-2.7 MeV; measured γ yield vs E. 18O deduced resonances, B(λ), γ-multipolarity, γ-branching, Γγ, Γ, Γα/Γ, α-reduced widths.

doi: 10.1103/PhysRevC.36.1256
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1986CO05      Phys.Rev. C33, 1855 (1986)

P.D.Cottle, M.Gai, J.F.Ennis, J.F.Shriner, Jr., D.A.Bromley, C.W.Beausang, L.Hildingsson, W.F.Piel, Jr., D.B.Fossan, J.W.Olness, E.K.Warburton

Intermediate and Weak Coupling in 219Ra

NUCLEAR REACTIONS 208Pb(14C, 3n), E=60-78 MeV; measured Eγ, Iγ, γ(θ). 219Ra deduced levels, γ-branching, J, π, rotational band. Weak coupling model.

doi: 10.1103/PhysRevC.33.1855
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1986CO16      Phys.Lett. 182B, 129 (1986)

P.D.Cottle, D.A.Bromley

Possible Unified Interpretation of Low-Lying Negative Parity States inn Lanthanide and Actinide Regions

NUCLEAR STRUCTURE Z=56-94; analyzed level systematics in Z=56-94; deduced negative parity states origin.

doi: 10.1016/0370-2693(86)91562-5
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1986SH25      Phys.Rev.Lett. 57, 1211 (1986)

B.Shivakumar, D.Shapira, P.H.Stelson, M.Beckerman, B.A.Harmon, K.Teh, D.A.Bromley

Equilibration in Orbiting Reactions

NUCLEAR REACTIONS 14N(28Si, 14N), E=100-170 MeV; measured ejectile yield at θ=15°, absolute orbiting σ(E). 14N(28Si, 12C), (28Si, 16O), E=100-170 MeV; measured absolute orbiting σ(E); deduced charge, mass equilibration.

doi: 10.1103/PhysRevLett.57.1211
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1985GA05      Phys.Rev. C31, 1255 (1985)

M.Gai, S.K.Korotky, J.M.Manoyan, E.C.Schloemer, B.Shivakumar, S.M.Sterbenz, S.J.Willett, D.A.Bromley, H.Voit

Interplay of Resonant and l-Window Background Amplitude in 16O + 16O

NUCLEAR REACTIONS, ICPND 16O(16O, α), (16O, 16O), E(cm)=15.5-16.5 MeV; measured σ(θ), σ(E), Eγ, Iγ, γ yield vs E. 32S resonances deduced J, π, Γ, Γα, α-reduced width.

doi: 10.1103/PhysRevC.31.1255
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1985SH25      Phys.Rev. C32, 1888 (1985)

J.F.Shriner, Jr., P.D.Cottle, J.F.Ennis, M.Gai, D.A.Bromley, J.W.Olness, E.K.Warburton, L.Hildingsson, M.A.Quader, D.B.Fossan

Level Structure of 220Ra

NUCLEAR REACTIONS 208Pb(14C, 2n), E=60-78 MeV; measured Eγ, Iγ, γ(θ), γγ-coin, σ(Eγ). 220Ra deduced levels, J, π, B(E1)/B(E2) ratios. Stable octupole deformation, α-clustering.

doi: 10.1103/PhysRevC.32.1888
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1985UM01      Phys.Rev. C32, 172 (1985)

A.S.Umar, M.R.Strayer, R.Y.Cusson, P.-G.Reinhard, D.A.Bromley

Time-Dependent Hartree-Fock Calculations of 4He + 14C, 12C + 12C(0+), and 4He + 20Ne Molecular Formations

NUCLEAR REACTIONS 14C, 20Ne(α, α), 12C(12C, 12C), E ≈ Coulomb barrier; calculated composite system density contours, isoscalar quadrupole, octupole, isovector dipole moment frequency dependence; deduced dynamical degrees of freedom, associated classical frequencies. TDHF.

doi: 10.1103/PhysRevC.32.172
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1984CO22      Phys.Rev. C30, 1768 (1984)

P.D.Cottle, J.F.Shriner, Jr., F.Dellagiacoma, J.F.Ennis, M.Gai, D.A.Bromley, J.W.Olness, E.K.Warburton, L.Hildingsson, M.A.Quader, D.B.Fossan

Level Structure and Deexcitations in 220Ra and Their Systematic Behavior as a Function of Neutron Number

NUCLEAR REACTIONS 208Pb(14C, 2n), E=60-68 MeV; measured Eγ, Iγ, γγ-coin, σ(Eγ, E), γ(θ). 220Ra deduced levels, J, π, γ-branching, B(λ) ratios.

doi: 10.1103/PhysRevC.30.1768
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1984ME12      Nucl.Phys. A429, 351 (1984)

M.C.Mermaz, M.Ruscev, M.Gai, J.F.Ennis, K.N.Gamadia, J.F.Shriner, Jr., N.Tsoupas, S.M.Sterbenz, D.A.Bromley

Phenomenological Analysis of the 24Mg(12C, α)32S Resonant Reaction Studied at Low Incident Energy

NUCLEAR REACTIONS 24Mg(12C, α), E=20.305, 21.307, 21.81 MeV; measured σ(θ). 36Ar resonance deduced J. Regge pole, phase shift analyses.

doi: 10.1016/0375-9474(84)90212-4
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1984ST02      Phys.Lett. 135B, 261 (1984)

M.R.Strayer, R.Y.Cusson, A.S.Umar, P.-G.Reinhard, D.A.Bromley, W.Greiner

Time-Dependent Hartree-Fock Picture of Nuclear Molecular Resonances

NUCLEAR STRUCTURE 18O; calculated isovector dipole, isocalar quadrupole, octupole molecular resonances. TDHF method.

doi: 10.1016/0370-2693(84)90387-3
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1983BR31      Nucl.Phys. A400, 3c (1983)


Heavy Ion Science: Gateway to the unknown

doi: 10.1016/0375-9474(83)90425-6
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1983GA02      Phys.Rev.Lett. 50, 239 (1983)

M.Gai, M.Ruscev, A.C.Hayes, J.F.Ennis, R.Keddy, E.C.Schloemer, S.M.Sterbenz, D.A.Bromley

Coexistence of Single-Particle, Collective-Quadrupole, and α + 14C Molecular-Dipole Degrees of Freedom in 18O

NUCLEAR REACTIONS 14C(7Li, t), E=15 MeV; 14C(α, γ), E=resonance; measured tγ-coin, resonance capture γ-spectra. 18O deduced γ-transition multipolarity, β(λ), single particle, collective quadrupole, molecular dipole degrees of freedom coexistence.

doi: 10.1103/PhysRevLett.50.239
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1983GA11      Phys.Rev.Lett. 51, 646 (1983)

M.Gai, J.F.Ennis, M.Ruscev, E.C.Schloemer, B.Shivakumar, S.M.Sterbenz, N.Tsoupas, D.A.Bromley

Molecular Alpha-Particle Clustering in 218Ra; Dipole collectivity in the vicinity of nuclear shell closures

NUCLEAR REACTIONS 208Pb(13C, 3n), E=59, 59.5, 67 MeV; measured σ(Eγ), γγ-coin, γ(θ), αγ(t), σ(Eα), recoil. 218Ra deduced levels, J, π, B(λ), B(E1)/B(E2), α-clustering.

doi: 10.1103/PhysRevLett.51.646
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1983KO15      Phys.Rev. C28, 168 (1983)

S.K.Korotky, K.A.Erb, R.L.Phillips, S.J.Willett, D.A.Bromley

Evidence for Nuclear Molecular Orbital Effects in the 13C + 13C → 12C + 14C Transfer Reaction

NUCLEAR REACTIONS 13C(13C, 12C), (13C, 14C), E=16-50 MeV; measured σ(θ, E); deduced evidence for effective Q-value reduction in surface region, collision delay time increase. DWBA analysis, two-pole model. 13C(13C, 13C), E=14.5-71 MeV; measured σ(θ, E); deduced geometrical effect oscillations. Optical model analysis, single pole model.

doi: 10.1103/PhysRevC.28.168
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1983SC29      Phys.Rev.Lett. 51, 881 (1983)

E.C.Schloemer, M.Gai, J.F.Ennis, M.Ruscev, B.Shivakumar, S.M.Sterbenz, N.Tsoupas, D.A.Bromley

Nature of Molecular Resonances and Background in the 16O + 12C System

NUCLEAR REACTIONS, ICPND 12C(16O, α), 12C(16O, 16O), E(cm)=7-15 MeV; measured σ(θα), total reaction σ(E). 28Si deduced resonances, J, π, Γ, Γ(12C), dinuclear molecular configuration characterising parameter.

doi: 10.1103/PhysRevLett.51.881
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1983WI11      Phys.Rev. C28, 1986 (1983)

S.J.Willett, S.K.Korotky, R.L.Phillips, D.A.Bromley, K.A.Erb

Spin Alignment and Phase Angles in 12C + 12C Inelastic Scattering

NUCLEAR REACTIONS, ICPND 12C(12C, 12C'), E=30-65 MeV; measured 12Cγ(θ); deduced σ(E). 12C level deduced magnetic substate alignments, phase angles. Band crossing, diffraction, DWBA, barrier top models.

doi: 10.1103/PhysRevC.28.1986
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1981ER02      Phys.Rev. C23, 2781 (1981)

K.A.Erb, D.A.Bromley

Rotational and Vibrational Excitations in Nuclear Molecular Spectra

NUCLEAR REACTIONS 12C(12C, 12C), (12C, X), E(cm) < 13 MeV; analyzed all data. Molecular symmetry model.

doi: 10.1103/PhysRevC.23.2781
Citations: PlumX Metrics

1981GA33      Phys.Rev.Lett. 47, 1878 (1981)

M.Gai, E.C.Schloemer, J.E.Freedman, A.C.Hayes, S.K.Korotky, J.M.Manoyan, B.Shivakumar, S.M.Sterbenz, H.Voit, S.J.Willett, D.A.Bromley

Resonances in 16O + 16O

NUCLEAR REACTIONS 16O(16O, 16O), 16O(16O, α), E(cm)=15.5-17 MeV; measured σ(θ) vs E; deduced resonant, background S-matrix elements. 32S deduced resonances, J, π.

doi: 10.1103/PhysRevLett.47.1878
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1980ER06      Phys.Rev. C22, 507 (1980)

K.A.Erb, R.R.Betts, S.K.Korotky, M.M.Hindi, P.P.Tung, M.W.Sachs, S.J.Willett, D.A.Bromley

Resonant and Average Behavior of the 12C+12C Total Reaction Cross Section: 5.6≤E(cm)≤10.0 MeV

NUCLEAR REACTIONS 12C(12C, γ), E=11.8-20 MeV; measured σ(E); deduced total reaction σ. 24Mg deduced resonances, J, π, Γ(12C), Γ. Optical model analysis, incoming-wave boundary condition model.

doi: 10.1103/PhysRevC.22.507
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1980KO21      Prog.Theor.Phys.(Kyoto) 63, 722 (1980)

Y.Kondo, D.A.Bromley, Y.Abe

Evidence for Molecular Resonances in the 16O+16O System

NUCLEAR REACTIONS 16O(16O, 16O), (16O, X), E=15-35 MeV; 16O(16O, 16O'), E=12-40 MeV; calculated σ(E), fusion σ(E); deduced molecular resonances. Band crossing model.

doi: 10.1143/PTP.63.722
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1980KO24      Phys.Rev. C22, 1068 (1980)

Y.Kondo, D.A.Bromley, Y.Abe

Application of a Band-Crossing Model for Resonances in 16O+16O Scattering

NUCLEAR REACTIONS 16O(16O, 16O), (16O, 16O'), E(cm)=10-41 MeV; calculated σ(E), fusion σ(E). Resonance mechanism, band crossing model.

doi: 10.1103/PhysRevC.22.1068
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1979KO19      Phys.Rev. C20, 1014 (1979)

S.K.Korotky, K.A.Erb, S.J.Willett, D.A.Bromley

12C + 12C Coulomb Barrier Resonances: Direct Determination of Resonance Parameters from Elastic Scattering Measurements

NUCLEAR REACTIONS 12C(12C, 12C), E=13.0-14.1 MeV; measured σ(E;θ); deduced phase shift parameters. 24Mg resonances deduced J, Γ(12C). Breit-Wigner analysis.

doi: 10.1103/PhysRevC.20.1014
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1979PH01      Phys.Rev.Lett. 42, 566 (1979)

R.L.Phillips, K.A.Erb, D.A.Bromley, J.Weneser

Origin of Gross Structure in 12C + 12C and 16O + 16O Inelastic Scattering

NUCLEAR REACTIONS 12C(12C, 12C'), E(cm)=10-40 MeV; 16O(16O, 16O'), E(cm)=15-45 MeV; calculated σ(E). Nonresonant diffraction model.

doi: 10.1103/PhysRevLett.42.566
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1978CH29      Nuovo Cim. 47A, 430 (1978)

L.T.Chua, A.Gobbi, M.W.Sachs, D.Shapira, R.Wieland, D.A.Bromley

The 12C + 13C Elastic-Transfer Interaction at Intermediate Energies

NUCLEAR REACTIONS 13C(12C, 12C), (12C, 12C'), E=20-35.5 MeV; measured σ(θ(12C)), energy-angle σ surfaces. 12C levels deduced reaction mechanism. Enriched target.

doi: 10.1007/BF02896234
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1978CH30      Nuovo Cim. 47A, 443 (1978)

L.T.Chua, D.A.Bromley

An Analysis of Neutron Transfer between Identical Cores with Applications to the 12C + 13 C System

NUCLEAR REACTIONS 13C(12C, 12C), E=15-35 MeV; calculated σ(θ). Coupled-channel analysis of HI transfer reactions. Source term methods of Ascuitto, Glendenning.

doi: 10.1007/BF02896235
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1978SH22      Phys.Rev. C18, 2574 (1978)

G.B.Sherwood, K.A.Erb, D.L.Hanson, R.J.Ascuitto, D.A.Bromley, J.J.Kolata

Interference Effects in the Reaction 48Ti(16O, 15N)49V

NUCLEAR REACTIONS 48Ti(16O, 15N), E=50 MeV; measured σ(θ). 48Ti, 49V levels deduced B(E2), (2j+1)C2S. CCBA analysis of inelastic multistep contributions. Particle-core model. Enriched targets.

doi: 10.1103/PhysRevC.18.2574
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1978TU06      Phys.Rev. C18, 1663 (1978)

P.P.Tung, K.A.Erb, M.W.Sachs, G.B.Sherwood, R.J.Ascuitto, D.A.Bromley

Sequential Amplitudes in Heavy-Ion Induced Two-Proton Transfer Reactions

NUCLEAR REACTIONS 90Zr, 88Sr(16O, 16O), (16O, 14C), E=80 MeV; 88Sr, 90Zr(12C, 12C), (12C, 10Be), E=60 MeV; measured σ(θ). Finite range DWBA, CCBA analyses. Enriched targets.

doi: 10.1103/PhysRevC.18.1663
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1977HA28      Phys.Rev. C16, 902 (1977)

D.L.Hanson, K.A.Erb, J.S.Vaagen, R.J.Ascuitto, D.A.Bromley, J.J.Kolata

Quadrupole Transfer Strength Studied Through Heavy-Ion Induced Two-Neutron Transfer between the Shape Transitional Nuclei 190,192Os

NUCLEAR REACTIONS 192Os(12C, 12C), (12C, 14C), E=70 MeV; measured σ(θ); deduced effect of shape transitions on quadrupole transfer strength. CCBA analysis.

doi: 10.1103/PhysRevC.16.902
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1976ER03      Phys.Rev.Lett. 37, 670 (1976)

K.A.Erb, R.R.Betts, D.L.Hanson, M.W.Sachs, R.L.White, P.P.Tung, D.A.Bromley

New Resonances in the Low-Energy 12C-12C Spectrum

NUCLEAR REACTIONS 12C(12C, α), E(cm)=6.5-11 MeV; measured σ(E, Eα, θ). 20Ne deduced levels. 24Mg deduced resonances, Γα.

doi: 10.1103/PhysRevLett.37.670
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1976HA46      Nucl.Phys. A269, 520 (1976)

D.L.Hanson, R.J.Ascuitto, J.S.Vaagen, K.A.Erb, D.A.Bromley, J.J.Kolata, D.J.Pisano

Quadrupole Transfer Strength for Deformed Rare-Earth Nuclei as Studied With Heavy-Ion Induced Two-Nucleon Transfer Reactions

NUCLEAR REACTIONS 154Sm(12C, 14C), E=65 MeV; 182W(12C, 14C), E=70 MeV; measured σ(E(14C), θ); deduced σ(θ) dependence on quadrupole transfer strength in presence of multistep processes. Enriched targets.

doi: 10.1016/0375-9474(76)90697-7
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1975AS01      Phys.Lett. 55B, 289 (1975)

R.J.Ascuitto, J.S.Vaagen, K.A.Erb, D.L.Hanson, D.A.Bromley, J.J.Kolata

Inelastic Nuclear-Coulomb Interference and Direct-Two-Step Interference in Heavy-Ion Induced Two-Nucleon Transfer Reactions on Rare-Earth Nuclei

NUCLEAR REACTIONS 186W(12C, 10Be), E=70 MeV; measured σ(E(10Be), θ).

doi: 10.1016/0370-2693(75)90602-4
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1975PO10      Nuovo Cim. 28A, 215 (1975)

J.E.Poth, M.W.Sachs, D.A.Bromley

Transfer of Neutron-Proton Pairs in Heavy-Ion Interactions

NUCLEAR REACTIONS 12,13C, 14,15N, 16O, 20Ne(11B, 9Be), E=116 MeV; measured σ(E(9Be)).

doi: 10.1007/BF02820881
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1975SH24      Phys.Rev. C12, 1907 (1975)

D.Shapira, R.G.Stokstad, M.W.Sachs, A.Gobbi, D.A.Bromley

Experimental Studies of the Resonance at E(c.m.) = 19.7 MeV in the 12C + 16O System

NUCLEAR REACTIONS 12C(16O, 16O'), (16O, 12C), (16O, α), (16O, p), E=45.96 MeV; measured σ(E). 16O, 24Mg, 27Al, 28Si deduced resonance structure.

doi: 10.1103/PhysRevC.12.1907
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1974CL07      Nucl.Phys. A232, 311 (1974)

T.P.Cleary, N.Stein, W.D.Callender, D.A.Bromley, J.P.Coffin, A.Gallmann

The Structure of 209Bi (II). Macroscopic Structure from Direct Scattering

NUCLEAR REACTIONS 209Bi, 208Pb(p, p'), E=16.10 MeV; measured σ(Ep', θ). 209Bi deduced levels, L, J, β. 209Bi(p, p'), E=14.95 MeV; measured σ(Ep', θ). 209Bi deduced levels. Enriched, natural targets.

doi: 10.1016/0375-9474(74)90624-1
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1974HA11      Phys.Rev. C9, 929 (1974)

D.L.Hanson, R.G.Stokstad, K.A.Erb, C.Olmer, D.A.Bromley

Compound Nature of the Reaction 12C(14N, 6Li)20Ne

NUCLEAR REACTIONS 12C(14N, 6Li), E(cm)=24, 36, 55 MeV; calculated σ(E(6Li), θ). 12C(14N, 2p), (14N, α), (14N, 7Be), E=12-60 MeV; calculated σ.

doi: 10.1103/PhysRevC.9.929
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1974HA25      Phys.Rev. C9, 1760 (1974)

D.L.Hanson, R.G.Stokstad, K.A.Erb, C.Olmer, M.W.Sachs, D.A.Bromley

Systematics of 'Quasimolecular' Resonances: A Search for Sub-Coulomb Resonant Structure in the Reactions 14N + 14N and 9Be + 12C

NUCLEAR REACTIONS 9Be(12C, α), (12C, p), E(cm)=2.4-6.34 MeV; measured σ(E, Eα, Ep); 14N(14N, α), (14N, p), (14N, d), E(cm)=7-10 MeV; measured σ(E, Eα, Ep, Ed); deduced no resonances.

doi: 10.1103/PhysRevC.9.1760
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1974OL06      Phys.Rev. C10, 1722 (1974)

C.Olmer, R.G.Stokstad, D.L.Hanson, K.A.Erb, M.W.Sachs, D.A.Bromley

Light Particle and Gamma-Ray Production in 12C + 14N Interactions

NUCLEAR REACTIONS 12C(14N, d), (14N, p), (14N, α), E=20, 25 MeV; measured σ(Ed, θ), σ(Ep, θ), σ(Eα, θ); 14N(12C, γ), E=14-33 MeV; measured σ(E, Eγ). 24,25Mg deduced levels, J, π.

doi: 10.1103/PhysRevC.10.1722
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1974PE13      Nucl.Phys. A232, 269 (1974)

R.E.Peschel, J.M.Long, H.D.Shay, D.A.Bromley

The Radiative Capture Reactions 40Ca(α, γ)44Ti and 48Ca(α, γ)52Ti in The Region of the Giant Dipole Resonance

NUCLEAR REACTIONS 40Ca(α, γ), E=6.5-17.5 MeV; measured σ(E;Eγ, θ); 48Ca(α, γ), E=6.0-14.0 MeV; measured σ(E;Eγ). 44Ti deduced levels, J, π. Natural 40Ca target. Enriched 48Ca target.

doi: 10.1016/0375-9474(74)90622-8
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetT0259.

1974SH01      Phys.Rev. C9, 76 (1974)

H.D.Shay, R.E.Peschel, J.M.Long, D.A.Bromley

Radiative 3He Capture in 12C and 16O

NUCLEAR REACTIONS 9Be(3He, γ), E=3-26 MeV; 13C(3He, γ), E=3-16 MeV; measured σ(E;Eγ, θ). 12C, 16O deduced levels, J, π, resonance parameters. Natural 9Be target. Enriched 13C target.

doi: 10.1103/PhysRevC.9.76
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1201.

1974SH16      Phys.Rev. C10, 1063 (1974)

D.Shapira, R.G.Stokstad, D.A.Bromley

Statistical Analysis of the Energy Dependence of 12C + 12C Cross Sections

NUCLEAR REACTIONS 12C(12C, 12C), E=13.5-37.5 MeV; calculated σ. 12C(12C, α), E=16-21 MeV; measured σ(E, Eα). 24Mg resonances deduced level-width.

doi: 10.1103/PhysRevC.10.1063
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1974WI05      Phys.Rev. C9, 1474 (1974)

R.Wieland, R.Stokstad, A.Gobbi, D.Shapira, L.Chua, M.W.Sachs, D.A.Bromley

Three-Body Final States in 16O + 12C-Induced Reactions: The Structure Of 24Mg at High Excitation

NUCLEAR REACTIONS 12C(16O, 2α), (16O, α12C), E=58.3 MeV; measured αα-coin, α12C-coin, deduced reaction mechanism. 20Ne deduced levels; 16O, 24Mg deduced resonances.

doi: 10.1103/PhysRevC.9.1474
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1973GO01      Phys.Rev. C7, 30 (1973)

A.Gobbi, R.Wieland, L.Chua, D.Shapira, D.A.Bromley

Entrance Channel Phenomena in Complex Nuclear Scattering

NUCLEAR REACTIONS 6Li(6Li, 6Li), 12C(12C, 12C), 14N(14N, 14N), 16O(16O, 16O), 18O(18O, 18O), E < 35 MeV cms; analyzed σ(E;θ).

doi: 10.1103/PhysRevC.7.30
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1973RE12      Nuovo Cim. 13A, 913 (1973)

W.Reilly, R.Wieland, A.Gobbi, M.W.Sachs, J.Maher, R.H.Siemssen, D.Mingay, D.A.Bromley

Elastic-Scattering Excitation Functions for the 12C + 12C System

NUCLEAR REACTIONS 12C(12C, 12C), E=10-75 MeV; measured σ(E;θ).

doi: 10.1007/BF02804158
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1973RE13      Nuovo Cim. 13A, 897 (1973)

W.Reilly, R.Wieland, A.Gobbi, M.W.Sachs, D.A.Bromley

A Comparative Study of the Elastic Scattering in the 12C, 14N and 16O Identical-Particle Systems

NUCLEAR REACTIONS 14N(14N, 14N), E(cm)=17-30 MeV; measured σ(E;θ); deduced optical model parameters.

doi: 10.1007/BF02804157
Citations: PlumX Metrics

1973WI09      Phys.Rev. C8, 37 (1973)

R.Wieland, A.Gobbi, L.Chua, M.W.Sachs, D.Shapira, R.Stokstad, D.A.Bromley

Inelastic Scattering of 12C on 12C

NUCLEAR REACTIONS 12C(12C, 12C), (12C, 12C'), E=40-60 MeV; measured σ(E(12C), θ). Deduced single, mutual excitation of first excited state.

doi: 10.1103/PhysRevC.8.37
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1972AY01      Phys.Rev.Lett. 29, 182 (1972)

E.E.Ayoub, R.J.Ascuitto, D.A.Bromley

Compound Particle-Core Coupled States and Direct Nuclear Processes

NUCLEAR REACTIONS 206Pb(p, p'), E=14.2-17.3 MeV; measured σ(E;θ); deduced resonance-resonance, direct-resonance interference.

doi: 10.1103/PhysRevLett.29.182
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1972BR26      Phys.Rev. C6, 53 (1972)

C.Brassard, H.D.Shay, J.P.Coffin, W.Scholz, D.A.Bromley

Giant Resonances in C12

NUCLEAR REACTIONS 11B(p, γ), E=14-22 MeV; measured σ(E;Eγ, θ(γ)). 12C deduced giant resonance structure, isospin mixing.

doi: 10.1103/PhysRevC.6.53
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0355.

1972CL02      Phys.Rev.Lett. 28, 699 (1972)

T.P.Cleary, W.D.Callender, N.Stein, C.H.King, D.A.Bromley, J.P.Coffin, A.Gallmann

Alternate Models of Particle-Core Coupling in 209Bi

NUCLEAR REACTIONS 209Bi(p, p'), E=16.10, 14.95 MeV; measured σ(Ep', θ). 209Bi deduced levels.

doi: 10.1103/PhysRevLett.28.699
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1972CO05      Nucl.Phys. A181, 337 (1972)

J.P.Coffin, N.Stein, T.P.Cleary, C.H.King, D.A.Bromley

Structure of 209Bi and 210Bi from Isobaric Analogue Resonances in the 209Bi(p, p') Reaction

NUCLEAR REACTIONS 209Bi(p, p'), E=14-21 MeV; measured σ(E;Ep, θ). 210Po deduced isobaric analog resonances. 210Bi, 209Bi deduced level structure. Natural target.

doi: 10.1016/0375-9474(72)90489-7
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1972HO06      Priv.Comm., (1972); to be published in Nucl.Phys.

G.E.Holland, C.A.Whitten, Jr., D.A.Bromley

1972HO52      Nuovo Cim. 11A, 575 (1972)

A.J.Howard, R.G.Hirko, D.A.Bromley, K.Bethge, J.W.Olness

A Study of 22Ne via the 20Ne(t, pγ)22Ne Reaction

NUCLEAR REACTIONS 20Ne(t, pγ), E=3 MeV; measured σ(Ep, Eγ, θ(pγ)). 22Ne deduced levels, J, π.

doi: 10.1007/BF02729464
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1972LI02      Nucl.Phys. A180, 1 (1972)

R.A.Lindgren, R.G.Hirko, J.G.Pronko, A.J.Howard, M.W.Sachs, D.A.Bromley

A Study of 23Na

NUCLEAR REACTIONS 23Na(α, α'γ), 26Mg(p, αγ), Eα=16.85 MeV, Ep=14.25 MeV; measured αγ(θ), pγ(θ), Iγ. 23Na levels deduced J, branching, multipole mixing ratios. Enriched 26Mg target.

doi: 10.1016/0375-9474(72)90152-2
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1972RE04      Nucl.Phys. A179, 51 (1972)

I.Rezanka, F.M.Bernthal, J.O.Rasmussen, R.Stokstad, I.Fraser, J.Greenberg, D.A.Bromley

High-Spin States in 153Gd and 154Gd from (α, xnγ) Studies

NUCLEAR REACTIONS 152Sm(α, 3nγ), (α, 2nγ), E=27-32 MeV; measured Eγ, Iγ(θ), γγcoin. 153Gd, 154Gd deduced levels, J, π. Enriched target.

doi: 10.1016/0375-9474(72)90104-2
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1972ST09      Phys.Rev.Lett. 28, 1523 (1972)

R.Stokstad, D.Shapira, L.Chua, P.Parker, M.W.Sachs, R.Wieland, D.A.Bromley

Possible Nuclear Molecule at 36.5 MeV in Si28

NUCLEAR REACTIONS 12C(16O, X), E approx 19.7 MeV cms; analyzed σ(E). 28Si resonance deduced molecular-type structure.

doi: 10.1103/PhysRevLett.28.1523
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1971GO03      Phys.Rev.Lett. 26, 396 (1971)

A.Gobbi, P.R.Maurenzig, L.Chua, R.Hadsell, P.D.Parker, M.W.Sachs, D.Shapira, R.Stokstad, R.Wieland, D.A.Bromley

Spins and Parities of Highly Excited States in Mg24

NUCLEAR REACTIONS 12C(16O, α1); E=48, 48.8, 58.3 MeV; measured σ(Eα1, Eα2, θ((α1)(α2))). 24Mg levels deduced J, π, branching ratios.

doi: 10.1103/PhysRevLett.26.396
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1971HI05      Particles and Nuclei 1, 372 (1971)

R.G.Hirko, R.A.Lindgren, A.J.Howard, J.G.Pronko, M.W.Sachs, D.A.Bromley

Nuclear Structure Studies on 29Al

NUCLEAR REACTIONS 27Al(t, p), E=3.34 MeV; measured σ(Ep, θ). 26Mg(α, pγ), E=13.82, 14 MeV; measured σ(Ep, Eγ, θ(γ), θ(pγ)). 29Al deduced levels, J, π, γ-mixing, γ-branching.

1971ME12      Phys.Rev. C4, 1778 (1971)

M.C.Mermaz, C.A.Whitten, Jr., J.W.Champlin, A.J.Howard, D.A.Bromley

Study of the (d, p) Reaction on 28Si, 32S, and 36Ar at E = 18.00 MeV

NUCLEAR REACTIONS 28Si, 32S, 36Ar(d, p), E=18 MeV; measured σ(Ep, θ). 29Si, 33S, 37Ar deduced levels, J, π, L(n), S.

doi: 10.1103/PhysRevC.4.1778
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1971ST20      Phys.Rev.Lett. 27, 748 (1971)

R.G.Stokstad, J.S.Greenberg, I.A.Fraser, S.H.Sie, D.A.Bromley

Rotation-Vibration Interaction in Sm152

NUCLEAR STRUCTURE 152Sm; calculated levels, moments of inertia, E2 matrix elements. VMI model;rotation-vibration interaction.

doi: 10.1103/PhysRevLett.27.748
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1970AP03      Nucl.Phys. A159, 367 (1970)

A.A.Aponick, Jr., C.M.Chesterfield, D.A.Bromley, N.K.Glendenning

Quadrupole and Hexadecapole Deformations in Rare Earth Nuclei

NUCLEAR REACTIONS 154Sm, 166Er, 176Yb(α, α'), E=27.5, 30.0, 32.5 MeV; measured σ(Eα', θ). 148Sm(α, α), E=27.5, 30.0, 32.5 MeV; measured σ(θ); deduced optical model parameters. 154Sm, 166Er, 176Yb levels deduced deformation parameters β(L).

doi: 10.1016/0375-9474(70)90713-X
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1970HO17      Phys.Rev. C1, 1446 (1970)

A.J.Howard, R.G.Hirko, D.A.Bromley, K.Bethge, J.W.Olness

Studies of the Low-Lying Levels of Ne24

NUCLEAR REACTIONS 22Ne(t, pγ), E=3.3 MeV; measured σ(Ep, Eγ, θ(pγ)). 24Ne levels deduced L, J, π.

doi: 10.1103/PhysRevC.1.1446
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1970LI08      Phys.Lett. 32B, 103 (1970)

R.A.Lindgren, J.G.Pronko, A.J.Howard, D.A.Bromley

The Identification of Mirror State Structure in 21Na and 21Ne

NUCLEAR REACTIONS 24Mg(p, α); E=17.5 MeV; measured σ(Eα, Ep), αp(θ). 21Na levels deduced J.

doi: 10.1016/0370-2693(70)90598-8
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1970PR01      Nucl.Phys. A140, 465 (1970)

J.G.Pronko, R.A.Lindgren, D.A.Bromley

Structure of 21Na from the 24Mg(p, α)21Na Reaction

NUCLEAR REACTIONS 24Mg(p, α), E=17.5 MeV; measured αγ(θ), Iγ, σ(Eα, θ(α)). 21Na levels deduced J, γ-branching, γ-mixing . Enriched target.

doi: 10.1016/0375-9474(70)90337-4
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1970ST18      Nucl.Phys. A156, 145 (1970)

R.G.Stokstad, I.A.Fraser, J.S.Greenberg, S.H.Sie, D.A.Bromley

Doppler Shift Attenuation Studies in Heavy Nuclei

NUCLEAR REACTIONS 152Sm(16O, 16O'γ), E=60 MeV; 150Nd, 152Sm(32S, 32S'γ), E=94-110 MeV; measured σ(E;Eγ), Doppler shift attenuation. 150Nd, 152Sm levels deduced T1/2.

doi: 10.1016/0375-9474(70)91122-X
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1970WH04      Phys.Rev. C1, 1455 (1970)

C.A.Whitten, Jr., M.C.Mermaz, D.A.Bromley

Study of the (d, t) Reaction on Si28, S32, and Ar36

NUCLEAR REACTIONS 28Si, 32S, 36Ar(d, t), E=22, 21 MeV; measured σ(Et, θ). 27Si, 31S, 35Ar levels deduced L(n), S.

doi: 10.1103/PhysRevC.1.1455
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1969CA19      Phys.Rev. 187, 1532 (1969)

R.F.Casten, J.S.Greenberg, S.H.Sie, G.A.Burginyon, D.A.Bromley

Transition Matrix Elements in the Even-Even Osmium Isotopes: A Comparison with Pairing-Plus-Quadrupole Model Calculations

NUCLEAR REACTIONS 186,188,190,192Os(16O, 16O'γ), E=42-80 MeV; measured σ(E(16O'), Eγ, θ(γ), θ(16O'γ)), γγ-coin. 186,188,190,192Os deduced levels, B(E2), branching ratios, quadrupole moment, J, π.

doi: 10.1103/PhysRev.187.1532
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1969FR10      Phys.Rev.Letters 23, 1047 (1969); Erratum Phys.Rev.Letters 23, 1270 (1969)

I.A.Fraser, J.S.Greenberg, S.H.Sie, R.G.Stokstad, G.A.Burginyon, D.A.Bromley

Investigation of Band-Mixing Anomalies in Sm152

NUCLEAR REACTIONS 152Sm(16O, 16O'γ), E = 48-60 MeV; measured σ(E;Eγ, θ). 152Sm transitions deduced B(E2), γ-mixing ratios, band mixing parameters.

doi: 10.1103/PhysRevLett.23.1047
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1969FR11      Phys.Rev.Letters 23, 1051 (1969)

I.S.Fraser, J.S.Greenberg, S.H.Sie, R.G.Stokstad, D.A.Bromley

E2 Matrix Elements Between High-Spin States in the Ground-State Bands of Sm152 and Sm154

NUCLEAR REACTIONS 152,154Sm(16O, 16O'γ), E = 48-60 MeV; 152,154Sm(32S, 32S'γ), E = 87-110 MeV; measured σ(E;E(16O'), Eγ), σ(E;E(32S'), Eγ). 152,154Sm transitions deduced E2 matrix elements, band mixing parameters, isomer shifts.

doi: 10.1103/PhysRevLett.23.1051
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1969HA49      Phys.Rev. 188, 1625 (1969)

F.Haas, B.Heusch, A.Gallmann, D.A.Bromley

Experimental Investigations of the C12(h, p)N14 Reaction Mechanism

NUCLEAR REACTIONS 12C(3He, pγ), E=4.6-11 MeV; measured σ(E;θ(p), θ(pγ)); deduced heavy-particle direct stripping. 15O deduced resonances. 14N deduced level population.

doi: 10.1103/PhysRev.188.1625
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1969MA40      Phys.Rev. 188, 1665 (1969)

J.V.Maher, M.W.Sachs, R.H.Siemssen, A.Weidinger, D.A.Bromley

Nuclear Interaction of Oxygen with Oxygen

NUCLEAR REACTIONS 16O(16O, 16O), E=20-80 MeV; measured σ(E;θ); deduced optical model parameters.

doi: 10.1103/PhysRev.188.1665
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1969ME20      Phys.Rev. 187, 1466 (1969)

M.C.Mermaz, C.A.Whitten, Jr., D.A.Bromley

Studies on the Shapes of Si28, S32, and Ar36 via Deuteron Scattering

NUCLEAR REACTIONS 28Si, 32S, 36Ar(d, d), (d, d'), E=18 MeV; measured σ(Ed', θ); deduced optical model parameters. 28Si, 32S, 36Ar levels deduced β(L).

doi: 10.1103/PhysRev.187.1466
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1969OV01      Nucl.Instr.Methods 68, 61 (1969)

J.C.Overley, P.D.Parker, D.A.Bromley

The Energy Calibration of Tandem Accelerators

NUCLEAR REACTIONS 12C, 24Mg, 28Si, 32S, 40Ca, 19F, 27Al, 58,60Ni, 54Fe(p, n), E=2-20 MeV; measured σ(E); deduced thresholds.

doi: 10.1016/0029-554X(69)90689-2
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1969WH06      Phys.Rev. 188, 1941 (1969)

C.A.Whitten, Jr., N.Stein, G.E.Holland, D.A.Bromley

Single-Hole Structure of Pb207

NUCLEAR REACTIONS 208Pb(p, d), E=20, 22 MeV; measured σ(Ed, θ). 207Pb levels deduced L(n), S.

doi: 10.1103/PhysRev.188.1941
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1968GA10      Nucl.Phys. A118, 515(1968)

A.Gallmann, F.Jundt, E.Aslanides, D.A.Bromley

Etude de la Region de 3 MeV d'Excitation de 27Al

NUCLEAR REACTIONS 27Al(p, p'); E=4.32-4.43; 4.81-4.90; 5.70-5.80 MeV; measured σ(E;Ep'), γγ-coin. 27Al levels deduced γ-branching ratios, J. Natural target.

doi: 10.1016/0375-9474(68)90436-3
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1968ST01      Phys.Rev.Letters 20, 113 (1968)

N.Stein, C.A.Whitten, Jr., D.A.Bromley

Particle-Core Coupling in the Lead Nuclei

NUCLEAR STRUCTURE 209Bi, 207Bi; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRevLett.20.113
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1968ST21      Phys.Rev.Letters 21, 1456 (1968)

N.Stein, J.P.Coffin, C.A.Whitten, Jr., D.A.Bromley

Isobaric Analog Resonances in Stripping and Pickup Reactions

NUCLEAR STRUCTURE 207Pb, 208Pb; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRevLett.21.1456
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1967AL02      Phys.Rev. 154, 1058 (1967)

J.P.Allen, A.J.Howard, D.A.Bromley, J.W.Olness, E.K.Warburton

Studies of Ar41 from the Ar40(d, pγ)Ar41 Reaction

NUCLEAR STRUCTURE 41Ar; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.154.1058
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1967BI06      Phys.Rev. 157, 787 (1967)

J.Birnbaum, J.C.Overley, D.A.Bromley

Mechanism of Nucleon Transfer Reactions Induced by 148-MeV N14 Ions

NUCLEAR STRUCTURE 13C, 11B, 11C, 12C, 10B; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.157.787
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1967BU04      Bull.Am.Phys.Soc. 12, No.1, 36, BG4 (1967)

G.A.Burginyon, J.S.Greenberg, D.A.Bromley, R.K.Kasten

Coulomb Excitation of Low-Lying Levels in the Even Neodymium Isotopes

1967CA08      Phys.Rev.Lett. 18, 912 (1967)

R.F.Casten, J.S.Greenberg, G.A.Burginyon, D.A.Bromley

Experimental Tests of Recent Pairing-Plus-Quadrupole Model Calculations in the Osmium Nuclei

NUCLEAR STRUCTURE 186Os, 188Os, 190Os, 192Os; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRevLett.18.912
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1967HO08      Phys.Rev. 154, 1067 (1967)

A.J.Howard, J.P.Allen, D.A.Bromley, J.W.Olness, E.K.Warburton

Studies on the Ne22(d, pγ)Ne23 Reaction

NUCLEAR STRUCTURE 23Ne; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.154.1067
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1967HO10      Phys.Rev. 157, 1022(1967)

A.J.Howard, J.P.Allen, D.A.Bromley, J.W.Olness, E.K.Warburton

Studies of Some Low-Lying Levels of Ne21

NUCLEAR REACTIONS 20Ne(d, pγ), E= < 4 MeV; measured σ(Ep, Eγ, θ(p), θ(pγ)). 21Ne deduced levels, J, π, branching ratios, γ-multipolarity.

doi: 10.1103/PhysRev.157.1022
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1967PO13      Phys.Rev. 164, 1295 (1967)

J.E.Poth, J.C.Overley, D.A.Bromley

B11-Induced Single-Nucleon Transfer Reactions

NUCLEAR STRUCTURE 20Ne, 16O, 13C, 15N, 14N, 12C; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.164.1295
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1967SI18      Phys.Rev.Lett. 19, 369 (1967)

R.H.Siemssen, J.V.Maher, A.Weidinger, D.A.Bromley

Excitation-function structure in 16O + 16O scattering

NUCLEAR REACTIONS 16O(16O, 16O), E=16.4-39.5 MeV; measured products, 16O; deduced σ(θ). Data were imported from EXFOR entry F0393.

doi: 10.1103/PhysRevLett.19.369
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0393.

1966BR17      Phys.Rev.Letters 17, 705 (1966)

D.A.Bromley, J.C.Overley, P.D.Parker

Masses of N12, Al24, P28, Cl32, and Sc40

NUCLEAR STRUCTURE 24Al, 12C, 12N, 40Sc, 28P, 32Cl; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRevLett.17.705
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1966LI04      Phys.Rev. 141, 1089 (1966)

A.C.Li, I.L.Preiss, P.M.Strudler, D.A.Bromley

Low Levels of Ba128 from La128 Decay

NUCLEAR STRUCTURE 128La; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.141.1089
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1966LI05      Phys.Rev. 141, 1097 (1966)

A.C.Li, I.L.Preiss, P.M.Strudler, D.A.Bromley

Isomerism in Ba129

NUCLEAR STRUCTURE 129Ba; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.141.1097
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1966SE06      Phys.Rev. 149, 925 (1966)

G.G.Seaman, J.S.Greenberg, D.A.Bromley, F.K.McGowan

Collective Nuclear Structure in the Even-Even Samarium Isotopes

NUCLEAR STRUCTURE 150Sm, 154Sm, 152Sm, 148Sm; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.149.925
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1965AL13      Nucl.Phys. 68, 426 (1965)

J.P.Allen, A.J.Howard, D.A.Bromley, J.W.Olness

The Low Levels of O19

NUCLEAR REACTIONS 18O(d, pγ)19O, E = 2.2, 2.5 MeV; measured γ, pγ-coin, γγ(θ). 19O deduced levels, J, π.

doi: 10.1016/0029-5582(65)90659-0
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1965AL20      Phys.Rev. 140, B1245 (1965)

J.P.Allen, A.J.Howard, D.A.Bromley, J.W.Olness

Studies on F19 in the O18(p, γ)F19 Reaction

NUCLEAR STRUCTURE 18O, 19F; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.140.B1245
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1965HO03      Phys.Rev. 137, B32 (1965)

A.J.Howard, D.A.Bromley, E.K.Warburton

Studies on the Ne20(d, pγ)Ne21 Reaction

NUCLEAR STRUCTURE 21Ne; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.137.B32
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1965NA04      Phys.Rev. 140, B824 (1965)

K.Nagatani, T.A.Tombrello, D.A.Bromley

Alpha-Particle-Induced Breakup of the Deuteron

NUCLEAR STRUCTURE 2H, 4He; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.140.B824
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1965SA07      Phys.Rev. 139, B92 (1965)

M.W.Sachs, C.Chasman, D.A.Bromley

Nuclear Spectroscopic Studies with High-Energy Boron Ions

NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.139.B92
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