NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = D.A.Bromley Found 157 matches. Showing 1 to 100. [Next]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
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
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
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
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
1987CO10 Phys.Rev. C35, 1891 (1987) 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
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
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
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
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
1986CO16 Phys.Lett. 182B, 129 (1986) 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
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
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
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
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
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
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
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
1983BR31 Nucl.Phys. A400, 3c (1983) Heavy Ion Science: Gateway to the unknown
doi: 10.1016/0375-9474(83)90425-6
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
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
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
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
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
1981ER02 Phys.Rev. C23, 2781 (1981) 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
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
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
1980KO21 Prog.Theor.Phys.(Kyoto) 63, 722 (1980) 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
1980KO24 Phys.Rev. C22, 1068 (1980) 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
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
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
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
1978CH30 Nuovo Cim. 47A, 443 (1978) 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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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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