NSR Query Results
Output year order : Descending NSR database version of May 3, 2024. Search: Author = G.J.Gyapong Found 36 matches. 2000SI36 Phys.Rev. C62, 054609 (2000) S.M.Singer, W.N.Catford, G.J.Gyapong, M.Shawcross, N.M.Clarke, N.Curtis, M.Freer, B.R.Fulton, S.J.Hall, R.A.Le Marechal, M.J.Leddy, J.S.Pople, G.Tungate, R.P.Ward, W.D.M.Rae, P.M.Simmons, S.P.G.Chappell, S.P.Fox, C.D.Jones, P.Lee, D.L.Watson Mechanism of the 12C(24Mg, 12C12C)12C Breakup Reaction: Direct vs compound NUCLEAR REACTIONS 24Mg(12C, 212C), E=85 MeV; measured particle spectra, angular distributions, coincidences, symmetric breakup yield; deduced forward-backward asymmetry, reaction mechanism features. Coupled channels DWBA calculations, comparison with reversed kinematics.
doi: 10.1103/PhysRevC.62.054609
1999FO16 Phys.Rev. C60, 064620 (1999) S.P.Fox, D.L.Watson, C.D.Jones, S.P.Chappell, P.Lee, W.D.M.Rae, M.Freer, S.J.A.Hall, G.Kelly, R.Le Marechal, R.P.Ward, W.N.Catford, G.J.Gyapong, S.Singer Structures in the 12C(16O, 12C(02+) → 3α)16O Reaction in the Region Ec.m. = 15 to 34 MeV NUCLEAR REACTIONS 12C(16O, 12C), E(cm)=15-34 MeV; measured Eα, Iα(θ), αα-coin following carbon breakup; deduced excitation functions. 28Si deduced possible resonance structures energy and angular momenta. Comparisons with model predictions.
doi: 10.1103/PhysRevC.60.064620
1998HO03 J.Phys.(London) G24, 167 (1998) S.J.Hoad, N.M.Clarke, N.Curtis, M.Freer, B.R.Fulton, S.J.Hall, M.J.Leddy, A.St.J.Murphy, J.S.Pople, G.Tungate, R.P.Ward, S.P.G.Chappell, S.P.Fox, C.D.Jones, D.L.Watson, W.D.M.Rae, P.M.Simmons, W.N.Catford, G.J.Gyapong, S.M.Singer Can Break-Up Reactions be Used to Probe High-Lying Inelastic Channels in 12C + 12C Scattering ( Question ) NUCLEAR REACTIONS C(24Mg, 212C), E=170 MeV; measured (12C)(12C(0+2))-coin, total energy.
doi: 10.1088/0954-3899/24/1/020
1998MU16 Phys.Rev. C58, 1569 (1998) J.T.Murgatroyd, J.S.Pople, N.M.Clarke, B.R.Fulton, M.J.Leddy, W.N.Catford, S.P.Fox, G.J.Gyapong, C.D.Jones, D.L.Watson, W.D.M.Rae, Y.Chan, R.G.Stokstad, S.J.Bennett 16O + 8Be Breakup of 24Mg Via the 12C(20Ne, 16O8Be)8Be and 12C(24Mg, 16O8Be)12C Reactions NUCLEAR REACTIONS 12C(20Ne, 8Be16O), E=160 MeV; 12C(24Mg, 8Be16O), E=170 MeV; measured (Be)(O)-coin, angular correlations, excitation energy spectra. 24Mg deduced levels E, J. Comparison with 12C + 12C breakup channel.
doi: 10.1103/PhysRevC.58.1569
1997CA11 Nucl.Phys. A616, 303c (1997) W.N.Catford, S.Mohammadi, P.H.Regan, C.S.Purry, W.Gelletly, P.M.Walker, G.J.Gyapong, J.Simpson, D.D.Warner, T.Davinson, R.Neal, R.D.Page, A.C.Shotter, I.M.Hibbert, R.Wadsworth, S.A.Forbes, A.M.Bruce, C.Thwaites, P.Thirolf, P.Van Duppen, W.Galster, A.Ninane, J.Vervier, P.Decrock, M.Huyse, J.Szerypo, J.Wauters High Resolution Gamma-Ray Spectroscopy with a Radioactive Beam NUCLEAR REACTIONS Ca(19Ne, X), E=70 MeV; measured Eγ, Iγ, γγ-coin; deduced experimental setup characteristics. High resolution γ-ray spectroscopy.
doi: 10.1016/S0375-9474(97)00101-2
1997GY02 Nucl.Phys. A620, 55 (1997) G.J.Gyapong, N.Curtis, W.N.Catford, S.M.Singer, W.D.M.Rae, M.Freer, S.J.Hall, G.R.Kelly, R.A.Le Marechal, R.P.Ward, S.P.G.Chappell, S.P.Fox, C.D.Jones, P.R.Lee, D.L.Watson Two-Dimensional Alpha Cluster Structures in 28Si NUCLEAR REACTIONS 12C(16O, 212C), E(cm)=28.3-36.8 MeV; measured (12C)(12C)-coin; deduced σ(E). 28Si deduced resonance angular momenta, cluster state characteristics.
doi: 10.1016/S0375-9474(97)00152-8
1996CA48 Nucl.Instrum.Methods Phys.Res. A371, 449 (1996) W.N.Catford, S.Mohammadi, P.H.Regan, C.S.Purry, W.Gelletly, P.M.Walker, G.J.Gyapong, J.Simpson, D.D.Warner, T.Davinson, R.Neal, R.D.Page, A.C.Shotter, I.M.Hibbert, R.Wadsworth, S.A.Forbes, A.M.Bruce, C.Thwaites, P.Thirolf, P.Van Duppen, W.Galster, A.Ninane, J.Vervier, P.Decrock, M.Huyse, J.Szerypo, J.Wauters High Resolution Gamma-Ray Spectroscopy with a Radioactive Beam NUCLEAR REACTIONS 40Ca(19Ne, X), E=70 MeV; measured Eγ, Iγ, γγ-coin. Escape suppressed Ge detectors array, 40Ca(19F, X) reaction also studied.
doi: 10.1016/0168-9002(95)00857-8
1996CU02 Phys.Rev. C53, 1804 (1996) N.Curtis, A.St.J.Murphy, N.M.Clarke, M.Freer, B.R.Fulton, S.J.Hall, M.J.Leddy, J.S.Pople, G.Tungate, R.P.Ward, W.N.Catford, G.J.Gyapong, S.M.Singer, S.P.G.Chappell, S.P.Fox, C.D.Jones, D.L.Watson, W.D.M.Rae, P.M.Simmons, P.H.Regan Evidence for a Highly Deformed Band in 16O + 16O Breakup of 32S NUCLEAR REACTIONS 12C(24Mg, 216O), E=170 MeV; measured (16O)(16O)(θ). 32S deduced levels, possible J, π, rotational parameter, band structure. Compared to DWBA.
doi: 10.1103/PhysRevC.53.1804
1996FR09 J.Phys.(London) G22, 1053 (1996) M.Freer, N.M.Clarke, B.R.Fulton, S.J.Hoad, G.R.Kelly, R.A.Le Marechal, R.P.Ward, C.D.Jones, P.Lee, W.N.Catford, G.J.Gyapong Energy Dependence of the 16O(16O, 12C(*))20Ne, 12C(16O, 12C(*))16O and 7Li(16O, 12C(*))11B Reactions NUCLEAR REACTIONS 12C, 7Li, 16O(16O, 12C), E=51-66 MeV; measured recoil mass, excitation, Q-value spectra, σ(θ) vs E. 32S, 28Si deduced broad structures.
doi: 10.1088/0954-3899/22/7/011
1996MA25 Phys.Lett. 381B, 407 (1996) F.M.Marques, E.Liegard, N.A.Orr, J.C.Angelique, L.Axelsson, G.Bizard, W.N.Catford, N.M.Clarke, G.Costa, M.Freer, S.Grevy, D.Guillemaud-Mueller, G.J.Gyapong, F.Hanappe, P.G.Hansen, B.Heusch, B.Jonson, C.Le Brun, F.R.Lecolley, F.Lefebvres, M.Lewitowicz, G.Martinez, A.C.Mueller, T.Nilsson, A.Ninane, G.Nyman, B.Petersen, F.Pougheon, K.Riisager, M.G.Saint-Laurent, Y.Schutz, M.Smedberg, O.Sorlin, L.Stuttge, D.D.Warner Neutrons from the Breakup of 19C NUCLEAR REACTIONS Ta(19C, xn), E=30 MeV/nucleon; measured σ(θn). 19C deduced neutron halo. Core breakup reaction model.
doi: 10.1016/0370-2693(96)00617-X
1996MU03 Phys.Rev. C53, 1963 (1996) A.St.J.Murphy, R.A.Le Marechal, S.J.Bennett, N.M.Clarke, N.Curtis, M.Freer, B.R.Fulton, S.J.Hall, M.J.Leddy, J.T.Murgatroyd, J.S.Pople, G.Tungate, R.P.Ward, W.D.M.Rae, P.M.Simmons, W.N.Catford, G.J.Gyapong, S.M.Singer, S.P.G.Chappell, S.P.Fox, C.D.Jones, P.Lee, D.L.Watson Search for 16O + 16O + 16O Structure in 48Cr NUCLEAR REACTIONS 12C, 24Mg(24Mg, 216O), E=150, 170 MeV; measured Eγ, Iγ, σ(θ1, θ2).
doi: 10.1103/PhysRevC.53.1963
1995CH07 Phys.Rev. C51, 695 (1995) S.P.G.Chappell, D.L.Watson, S.P.Fox, C.D.Jones, W.D.M.Rae, P.M.Simmons, M.Freer, B.R.Fulton, N.M.Clarke, N.Curtis, M.J.Leddy, J.S.Pople, S.J.Hall, R.P.Ward, G.Tungate, W.N.Catford, G.J.Gyapong, S.M.Singer, P.H.Regan 12C + 12C ' 6α-Chain State ' Resonance NUCLEAR REACTIONS 12C(12C, 12C'), E(cm)=25-40 MeV; measured spectra, σ(θ). 24Mg deduced resonance features.
doi: 10.1103/PhysRevC.51.695
1995CU01 Phys.Rev. C51, 1554 (1995) N.Curtis, N.M.Clarke, B.R.Fulton, S.J.Hall, M.J.Leddy, A.St.J.Murphy, J.S.Pople, R.P.Ward, W.N.Catford, G.J.Gyapong, S.M.Singer, S.P.G.Chappell, S.P.Fox, C.D.Jones, D.L.Watson, W.D.M.Rae, P.M.Simmons, and the Charissa Collaboration Association of the 12C + 12C Breakup States in 24Mg with the Quasimolecular Resonances NUCLEAR REACTIONS 12C(24Mg, 212C), E=170 MeV; measured (12C)(12C)-coin spectra. 24Mg deduced resonances, J, π, Γ upper limit.
doi: 10.1103/PhysRevC.51.1554
1995FR05 Phys.Rev. C51, 1682 (1995) M.Freer, N.M.Clarke, N.Curtis, B.R.Fulton, S.J.Hall, M.J.Leddy, J.S.Pople, G.Tungate, R.P.Ward, P.M.Simmons, W.D.M.Rae, S.P.G.Chappell, S.P.Fox, C.D.Jones, D.L.Watson, G.J.Gyapong, S.M.Singer, W.N.Catford, P.H.Regan 8Be and α Decay of 16O NUCLEAR REACTIONS 12C(16O, 4α), E=99 MeV; measured Q-value spectra, 16O excitation spectra leading to breakup, (12C)(α)(θ). 16O deduced resonances, decay channels, partial Γ, J.
doi: 10.1103/PhysRevC.51.1682
1995JA06 Phys.Rev. C51, 2606 (1995) N.S.Jarvis, D.L.Watson, G.J.Gyapong, C.D.Jones, S.J.Bennett, M.Freer, B.R.Fulton, O.Karban, J.T.Murgatroyd, G.Tungate, W.D.M.Rae, A.E.Smith Breakup Studies with 23Na NUCLEAR REACTIONS 12C(23Na, 11B12C), E=176 MeV; 12C(23Na, 212C), E=156 MeV; measured fragment E(total), spectra. 23Na, 24Mg deduced breakup state energies, width upper limits, fragmentation characteristics.
doi: 10.1103/PhysRevC.51.2606
1995LE22 Nucl.Phys. A589, 363 (1995) M.J.Leddy, S.J.Bennett, N.M.Clarke, M.Freer, B.R.Fulton, J.T.Murgatroyd, G.J.Gyapong, C.D.Jones, D.L.Watson, W.D.M.Rae, A.E.Smith, W.N.Catford Comparison of Resonances Observed in the 12C(24Mg, 12C12C)12C and 12C(20Ne, 12C12C)8Be Reactions NUCLEAR REACTIONS 12C(24Mg, 212C), E=170 MeV; measured (fragment)(fragment)-coin. 24Mg deduced excitation energies, J.
doi: 10.1016/0375-9474(95)00053-4
1995MU04 Nucl.Phys. A587, 367 (1995) J.T.Murgatroyd, S.J.Bennett, N.M.Clarke, B.R.Fulton, G.J.Gyapong, C.D.Jones, D.L.Watson, T.M.Cormier, H.Dejbakhsh, A.Szanto de Toledo, N.Carlin Termination of the 12C-12C Cluster States Revealed in the 12C)(20Ne, 12C12C)8Be Breakup Reaction NUCLEAR REACTIONS 12C(20Ne, 212C), E=300 MeV; measued (12C)(12C)-coin. 24Mg deduced energies of breakup states.
doi: 10.1016/0375-9474(95)00003-J
1995SI13 Phys.Rev. C51, 3500 (1995) P.M.Simmons, W.D.M.Rae, S.P.G.Chappell, S.P.Fox, C.D.Jones, D.L.Watson, M.Freer, B.R.Fulton, N.M.Clarke, N.Curtis, M.J.Leddy, J.S.Pople, S.J.Hall, R.P.Ward, G.Tungate, W.N.Catford, G.J.Gyapong, S.M.Singer, P.H.Regan Search for a 7-α Chain State NUCLEAR REACTIONS 12C(16O, X), E(cm)=37.7-51.4 MeV; measured σ(E) for (12C)(12C)(α), (12C)(8Be)(8Be) production. 28Si deduced no 7α-chain state.
doi: 10.1103/PhysRevC.51.3500
1994CU05 Nucl.Instrum.Methods Phys.Res. A351, 359 (1994) N.Curtis, A.St.J.Murphy, M.J.Leddy, J.S.Pople, N.M.Clarke, M.Freer, B.R.Fulton, S.J.Hall, G.Tungate, R.P.Ward, S.M.Singer, W.N.Catford, G.J.Gyapong, R.A.Cunningham, J.S.Lilley, S.P.Chappell, S.P.Fox, C.D.Jones, D.L.Watson, P.M.Simmons, R.A.Hunt, A.C.Merchant, A.E.Smith, W.D.M.Rae, J.Zhang, and the Charissa Collaboration The Construction and Operation of a Hybrid Gas-Silicon Detector for Studies of Cluster Breakup Reactions NUCLEAR REACTIONS 12C(24Mg, 212C), E=170 MeV; measured (12C)(12C)-coin spectra following projectile breakup. 197Au(12C, 12C), E=84 MeV; 197Au(24Mg, 24Mg), E=170 MeV; measured spectra. Hybrid gas-silicon detector.
doi: 10.1016/0168-9002(94)91364-1
1994GY01 Nucl.Phys. A579, 207 (1994) G.J.Gyapong, D.L.Watson, W.N.Catford, N.M.Clarke, S.J.Bennett, M.Freer, B.R.Fulton, C.D.Jones, M.Leddy, J.T.Murgatroyd, W.D.M.Rae, P.Simmons Reaction Mechanism for the Symmetric Breakup of 24Mg following an Interaction with 12C NUCLEAR REACTIONS 12C(24Mg, 212C), E(cm)=43.3-60 MeV; measured symmetric breakup yield; deduced reaction mechanism. 24Mg deduced cluster states characteristics.
doi: 10.1016/0375-9474(94)90802-8
1994PO19 Z.Phys. A349, 349 (1994) J.S.Pople, N.M.Clarke, B.R.Fulton, M.J.Leddy, J.T.Murgatroyd, Y.Chan, R.G.Stokstad, W.D.M.Rae, W.N.Catford, S.P.Fox, G.J.Gyapong, D.L.Watson, S.J.Bennett, and the Charissa Collaboration The Breakup of 24Mg into 16O and 8Be NUCLEAR REACTIONS 12C(24Mg, 8Be16O), E=170 MeV; 12C(20Ne, 8Be16O), E=160 MeV; measured breakup spectra; deduced reaction mechanism. 24Mg deduced breakup level configuration, shape features.
1993BE56 Nucl.Instrum.Methods Phys.Res. A332, 476 (1993) S.J.Bennett, N.M.Clarke, M.Freer, B.R.Fulton, S.J.Hall, O.Karban, J.T.Murgatroyd, G.Tungate, G.J.Gyapong, N.S.Jarvis, D.L.Watson, W.D.M.Rae, A.E.Smith, J.S.Lilley, P.J.Woods, R.D.Page, and the Charissa Collaboration Application of Inverse Kinematics to 1H + 23Na → 12C + 12C using a Thick Target NUCLEAR REACTIONS 1H(23Na, 12C), E=180 MeV; measured 12C-spectra, σ(θ) vs 24Mg excitation. Kinematically complete experiment.
doi: 10.1016/0168-9002(93)90303-Y
1992LI14 Nucl.Phys. A548, 308 (1992) C.S.Lim, R.H.Spear, M.P.Fewell, G.J.Gyapong Measurements of Static Electric Quadrupole Moments of the 2+1, 2+2, 4+1 and 6+1 States of 196Pt NUCLEAR REACTIONS 196Pt(α, α), E=14.2-15.8 MeV; 196Pt(7Li, 7Li), E=22, 22.5 MeV; 196Pt(12C, 12C), E=42-46 MeV; 196Pt(58Ni, 58Ni), E=214-226 MeV; measured (particle)γ-coin, Eγ, Iγ, γγ(θ), Coulomb excitation probabilities. 196Pt levels deduced B(E2), B(E4), static quadrupole moments.
doi: 10.1016/0375-9474(92)90013-A
1991FU09 Phys.Lett. 267B, 325 (1991) B.R.Fulton, S.J.Bennett, M.Freer, J.T.Murgatroyd, G.J.Gyapong, N.S.Jarvis, C.D.Jones, D.L.Watson, J.D.Brown, W.D.M.Rae, A.E.Smith, J.S.Lilley Spin Measurement for Symmetric Fission States of 24Mg. A New Angle on the 12C + 12C Interaction NUCLEAR REACTIONS 12C(24Mg, 212C), E=170 MeV; measured (12C)(12C)(θ). 24Mg deduced symmetric fission decay states J, deformation features. Cranked cluster model, Nilsson-Strutinsky calculations.
doi: 10.1016/0370-2693(91)90940-R
1991GY01 Phys.Rev. C44, 520 (1991) G.J.Gyapong, N.S.Jarvis, D.L.Watson, S.J.Bennett, M.Freer, B.R.Fulton, J.T.Murgatroyd, R.Hunt, W.D.M.Rae, A.E.Smith Near-Symmetric Breakup of 25Mg NUCLEAR REACTIONS 12C(25Mg, X), E=180 MeV; measured (fragment)(fragment)-coin, X=12C, 13C following projectile breakup. 24,25Mg deduced symmetric fissioning states energy.
doi: 10.1103/PhysRevC.44.520
1991RE03 Nucl.Phys. A533, 476 (1991) P.H.Regan, R.Wadsworth, J.R.Hughes, G.J.Gyapong, W.Gelletly, M.J.Godfrey, I.Jenkins, Y.-J.He, S.M.Mullins, P.J.Nolan, J.Simpson, B.J.Varley, D.L.Watson Spectroscopy of the Light Rare-Earth Nuclei 133Pm and 133Sm: Configuration-dependent pairing and evidence for strong residual proton-neutron interactions in neighbouring odd-N and odd-Z nuclei NUCLEAR REACTIONS 96Ru(40Ca, 2np), (40Ca, 3p), E=180 MeV; measured Iγ, Eγ. 133Sm, 133Pm levels deduced J, π, configurations.
doi: 10.1016/0375-9474(91)90529-F
1989BU07 Nucl.Phys. A494, 102 (1989) S.M.Burnett, A.M.Baxter, G.J.Gyapong, M.P.Fewell, R.H.Spear Electric Quadrupole Moments of the First Excited States of 130,134,138Ba NUCLEAR REACTIONS 130,134,138Ba(α, α'), E=10.8-11.8 MeV; 130,134Ba(12C, 12C'), E=32-38 MeV; 130,134,138Ba(16O, 16O'), E=43-49 MeV; measured Coulomb excitation probabilities of first 2+ states. 130,134,138Ba levels deduced B(E2), static electric quadrupole moment. Enriched targets.
doi: 10.1016/0375-9474(89)90200-5
1989SP07 Aust.J.Phys. 42, 345 (1989) R.H.Spear, W.J.Vermeer, S.M.Burnett, G.J.Gyapong, C.S.Lim Coulomb Excitation of 142Ce and 144Nd NUCLEAR REACTIONS 142Ce(α, α'), E=10, 12, 11.8 MeV; 142Ce, 144Nd(12C, 12C'), E=35 MeV; 142Ce(16O, 16O'), E=46 MeV; 144Nd(16O, 16O'), E=48 MeV; measured particle spectra following Coulomb excitation. 142Ce, 144Nd levels deduced B(λ), static quadrupole moments.
doi: 10.1071/PH890345
1989WA20 Z.Phys. A333, 409 (1989) R.Wadsworth, P.Regan, S.M.Mullins, G.J.Gyapong, D.L.Watson, P.J.Nolan, M.J.Godfrey, I.Jenkins, Y.J.He, B.J.Varley, W.Gelletly, J.Simpson Evidence for an i13/2 Neutron Band in 133Sm NUCLEAR REACTIONS 96Ru(40Ca, n2p), E=195 MeV; measured γγ-, nγ-, nnγ-coin. 133Sm deduced levels, J, π, band structure.
1989WA21 Z.Phys. A333, 411 (1989) R.Wadsworth, P.Regan, S.M.Mullins, G.J.Gyapong, D.L.Watson, P.J.Nolan, M.J.Godfrey, I.Jenkins, Y.J.He, B.J.Varley, J.Simpson, W.Gelletly Yrast Band Spectroscopy of 132Sm and 130Nd NUCLEAR REACTIONS 96Ru(40Ca, 2n2p), 96Ru(40Ca, 2pα), E=195 MeV; measured γγ-, nγ-, nnγ-coin. 130Nd, 132Sm deduced levels, J, π, band structure.
1988FE08 Aust.J.Phys. 41, 37 (1988) M.P.Fewell, G.J.Gyapong, R.H.Spear Coulomb Excitation of the 41+ States of 194,196,198Pt NUCLEAR REACTIONS 194,196Pt(α, α'), E=14.199-15.599; 198Pt(α, α'), E=15.599 MeV; 194,198Pt(12C, 12C'), E=40.998-49.998 MeV; 196Pt(12C, 12C'), E=40.985-55.996 MeV; 194Pt(16O, 16O'), E=54.998-62.998 MeV; 196Pt(16O, 16O'), E=54.993-60.994 MeV; 198Pt(16O, 16O'), E=56.997-62.998 MeV; measured Coulomb excitation probability. 194,196,198Pt levels deduced E2, E4 transition matrix elements, deformation parameters.
doi: 10.1071/PH880037
1988LI22 Nucl.Phys. A485, 399 (1988) C.S.Lim, R.H.Spear, W.J.Vermeer, M.P.Fewell, G.J.Gyapong Electric Quadrupole Moments of the First Excited State of 192Os NUCLEAR REACTIONS 192Os(α, α'), E=14.2-16.5 MeV; 192Os(12C, 12C'), E=40-55 MeV; 192Os(12C, 12C'), E=44-47 MeV; measured Coulomb excitation probabilities. 192Os levels deduced B(E2), static quadrupole moment. Enriched targets.
doi: 10.1016/0375-9474(88)90110-8
1987GY01 Nucl.Phys. A470, 415 (1987) G.J.Gyapong, R.H.Spear, M.P.Fewell, A.M.Baxter, S.M.Burnett Experimental Determination of the Electric Quadrupole Moment of the First Excited State of 192Pt NUCLEAR REACTIONS 192Pt(α, α'), E=14.4-15.2 MeV; 192Pt(12C, 12C'), E=41-48 MeV; 192Pt(16O, 16O'), E=55-60 MeV; measured Coulomb excitation probabilities of the first 2+ state. 192Pt levels deduced B(E2), quadrupole moment. Enriched targets.
doi: 10.1016/0375-9474(87)90011-X
1986GY04 Nucl.Phys. A458, 165 (1986) G.J.Gyapong, R.H.Spear, M.T.Esat, M.P.Fewell, A.M.Baxter, S.M.Burnett Electric Quadrupole Moments of the First Excited States of 194Pt, 196Pt and 198Pt NUCLEAR REACTIONS 194,196,198Pt(α, α'), E=14-15.6 MeV; 196Pt(α, α'), E=16.8-18.6 MeV; 194,196,198Pt(12C, 12C'), E=41-45 MeV; 194,196,198Pt(16O, 16O'), E=55-63 MeV; measured Coulomb excitation probabilities. 194,196,198Pt levels deduced B(E2), quadrupole moments. Enriched targets.
doi: 10.1016/0375-9474(86)90289-7
1986RO15 Phys.Rev. C34, 732 (1986) P.J.Rothschild, A.M.Baxter, S.M.Burnett, M.P.Fewell, G.J.Gyapong, R.H.Spear Quadrupole Moment of the First Excited State of 136Ba NUCLEAR REACTIONS 136Ba(α, α'), E=11-11.8 MeV; 136Ba(7Li, 7Li'), E=15, 16 MeV; 136Ba(16O, 16O'), E=45-49 MeV; measured Coulomb excitation probabilities. 136Ba level deduced quadrupole moment, B(E2). Enriched targets.
doi: 10.1103/PhysRevC.34.732
1985FE03 Phys.Lett. 157B, 353 (1985) M.P.Fewell, G.J.Gyapong, R.H.Spear, M.T.Esat, A.M.Baxter, S.M.Burnett The Quadrupole Moment of 196Pt - A Crucial Test of Nuclear Models NUCLEAR REACTIONS 196Pt(16O, 16O'), E=55-61 MeV; 196Pt(12C, 12C'), E=41-56 MeV; measured Coulomb excitation, particle spectra. 196Pt level deduced B(E2), quadrupole moment. Bohr-Mottelson, O(6) interacting boson model limits.
doi: 10.1016/0370-2693(85)90379-X
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