NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = M.T.Esat Found 24 matches. 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
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
1985FE05 Aust.J.Phys. 38, 555 (1985) M.P.Fewell, R.H.Spear, G.K.Adam, M.T.Esat Determination of B(E3; 0+1 → 3-1) Values for the Stable Isotopes of Cadmium NUCLEAR REACTIONS 106,116,108,110,112,114Cd(16O, 16O'), E=40-44 MeV; measured σ(E(16O)) following Coulomb excitation. 106,108,110,112,114,116Cd deduced transition B(E3), no shell effects.
doi: 10.1071/PH850555
1984VE03 Phys.Lett. 138B, 365 (1984) W.J.Vermeer, M.T.Esat, M.P.Fewell, R.H.Spear, A.M.Baxter, S.M.Burnett An Experimental Verfication of the Validity of the Reorientation-Effect Technique for the Determination of Nuclear Quadrupole Moments NUCLEAR REACTIONS 208Pb(7Li, 7Li'), E=16-30 MeV; 138Ba(7Li, 7Li'), E=12.5-22 MeV; measured Coulomb excitation reorientation effect. 7Li level deduced B(E2), quadrupole moment.
doi: 10.1016/0370-2693(84)91918-X
1984VE07 Aust.J.Phys. 37, 123 (1984) W.J.Vermeer, M.T.Esat, J.A.Kuehner, R.H.Spear, A.M.Baxter, S.Hinds Coulomb Excitation of the 2.615 MeV (3-) and 4.086 MeV (2+) States of 208Pb NUCLEAR REACTIONS 208Pb(12C, 12C'), E=53-58 MeV; 208Pb(16O, 16O'), E=57-76 MeV; measured Coulomb excitation. 208Pb levels deduced B(λ), quadrupole moment.
doi: 10.1071/PH840123
1984VE08 Aust.J.Phys. 37, 273 (1984) W.J.Vermeer, A.M.Baxter, S.M.Burnett, M.T.Esat, M.P.Fewell, R.H.Spear Coulomb Excitation of 7Li NUCLEAR REACTIONS 208Pb, 138Ba(7Li, 7Li'), E=12.5-30 MeV; measured σ(E(7Li)), Coulomb excitation. 7Li deduced GDR excitation, B(E2), ground state static electric quadrupole moment.
doi: 10.1071/PH840273
1983SP02 Phys.Lett. 128B, 29 (1983) R.H.Spear, W.J.Vermeer, M.T.Esat, J.A.Kuehner, A.M.Baxter, S.Hinds An Improved Determination of the Quadrupole Moment of the First Excited State of 208Pb NUCLEAR REACTIONS 208Pb(12C, 12C'), E=75, 90 MeV; 208Pb(16O, 16O'), E=80-171.6 MeV; analyzed Coulomb excitation data. 208Pb level deduced static quadrupole moment, B(E3).
doi: 10.1016/0370-2693(83)90067-9
1983VE01 Phys.Lett. 122B, 23 (1983) W.J.Vermeer, M.T.Esat, J.A.Kuehner, R.H.Spear, A.M.Baxter, S.Hinds Electric Quadrupole Moment of the First Excited State of 12C NUCLEAR REACTIONS 208Pb(12C, 12C'), E=53, 54, 56, 58 MeV; 208Pb(16O, 16O'), E=72 MeV; measured σ(E(12C)), σ(E(16O)), projectile Coulomb excitation. 12C level deduced quadrupole moment.
doi: 10.1016/0370-2693(83)91160-7
1982KU14 Phys.Lett. 115B, 437 (1982) J.A.Kuehner, R.H.Spear, W.J.Vermeer, M.T.Esat, A.M.Baxter, S.Hinds A Measurement of the Giant-Dipole-Resonance Contribution to the Coulomb Excitation of 17O NUCLEAR REACTIONS 208Pb(17O, 17O'), E=66-88 MeV; measured σ(E(17O)), projectile Coulomb excitation probability. 17O level deduced GDR contribution parameter. Modified hydrodynamic model. 208Pb(17O, 16O), (17O, 18O), E=66-88 MeV; measured σ(E(16O)), σ(E(18O)).
doi: 10.1016/0370-2693(82)90387-2
1982SP05 Nucl.Phys. A378, 559 (1982) R.H.Spear, T.H.Zabel, M.T.Esat, A.M.Baxter, S.Hinds The Quadrupole Moments of 26Mg as a Test of Shell-Model Interactions NUCLEAR REACTIONS 208Pb(26Mg, 26Mg'), E=80-120 MeV; measured Coulomb excitation. 26Mg level deduced quadrupole moment, B(E2). Enriched target.
doi: 10.1016/0375-9474(82)90466-3
1982VE09 Nucl.Phys. A389, 185 (1982) W.J.Vermeer, M.T.Esat, R.H.Spear Quadrupole Moment of the First Excited State of 32S NUCLEAR REACTIONS 208Pb(32S, 32S'), E=122-160 MeV; measured Coulomb excitation probabilities. 32S level deduced quadrupole moment, B(E2). Enriched target.
doi: 10.1016/0375-9474(82)90297-4
1982VE11 Aust.J.Phys. 35, 283 (1982) W.J.Vermeer, T.H.Zabel, M.T.Esat, J.A.Kuehner, R.H.Spear, A.M.Baxter The Giant Dipole Resonance Effect in Coulomb Excitation of 10B NUCLEAR REACTIONS 208Pb(10B, 10B'), (10B, 9B), (10B, 11B), E=32-38 MeV; measured σ(E(10B)), σ(E(9B)), σ(E(11B)), projectile Coulomb excitation. 10B deduced virtual GDR excitation.
doi: 10.1071/PH820283
1981ES02 Phys.Rev. C23, 1822 (1981) M.T.Esat, R.H.Spear, J.L.Zyskind, M.H.Shapiro, W.A.Fowler, J.M.Davidson Test of Global Hauser-Feshbach Calculations for Proton-Induced Reactions on 68Zn NUCLEAR REACTIONS 68Zn(p, γ), E=1.67-4.97 MeV; 68Zn(p, α), E=3.36-5.48 MeV; 68Zn(p, n), E=3.77-5.03 MeV; measured σ(E). Hauser-Feshbach calculations. Enriched targets.
doi: 10.1103/PhysRevC.23.1822
1981ES03 Nucl.Phys. A362, 227 (1981) M.T.Esat, M.P.Fewell, R.H.Spear, T.H.Zabel, A.M.Baxter, S.Hinds The Electric Quadrupole Moment of the First Excited State of 204Hg NUCLEAR REACTIONS 204Hg(α, α'), E=13.5-16.5 MeV; 204Hg(12C, 12C'), E=45-56 MeV; 204Hg(16O, 16O'), E=63, 65 MeV; measured Coulomb excitation. 204Hg deduced B(E2), quadrupole moment. 204Hg(p, p'), E=18 MeV; measured σ(Ep). 204Hg deduced levels. Enriched targets.
doi: 10.1016/0375-9474(81)90678-3
1980SP05 Nucl.Phys. A345, 252 (1980) R.H.Spear, M.T.Esat, M.P.Fewell, D.C.Kean, T.H.Zabel, A.M.Baxter, S.Hinds Static Quadrupole Moments of the First Excited States of 200Hg and 202Hg NUCLEAR REACTIONS 200,202Hg(α, α'), E=13.5-16.5 MeV; 200,202Hg(12C, 12C'), E=40-60 MeV; 202,200Hg(16O, 16O'), E=59-65 MeV; measured Coulomb excitation probabilities. 200,202Hg level deduced B(E2), quadrupole moment. Enriched targets.
doi: 10.1016/0375-9474(80)90423-6
1979ZY01 Nucl.Phys. A315, 430 (1979) J.L.Zyskind, J.M.Davidson, M.T.Esat, R.H.Spear, M.H.Shapiro, W.A.Fowler, C.A.Barnes Cross Section Measurements and Thermonuclear Reaction Rates for 48Ca(p, γ)49Sc and 48Ca(p, n)48Sc NUCLEAR REACTIONS 48Ca(p, γ), 48Ca(p, n), E=0.58-2.67 MeV; measured σ(E); deduced thermonuclear reaction rates as function of temperature. Hauser-Feshbach calculations. Enriched target. Ge(Li), BF3 long counter.
doi: 10.1016/0375-9474(79)90620-1
1979ZY04 Nucl.Phys. A331, 180 (1979) J.L.Zyskind, J.M.Davidson, M.T.Esat, M.H.Shapiro, R.H.Spear Competition Cusps in (α, γ) Reactions NUCLEAR REACTIONS 37Cl(α, γ), E=2.9-5.23 MeV; 62Ni(α, γ), E=5.07-8.64 MeV; 62Ni(α, n), E=6.95-8.76 MeV; 64Ni(α, γ), E=4.5-7.45 MeV; 64Ni(α, n), E=5.3-7.45 MeV; measured σ(E). Hauser-Feshbach calculations. Enriched target, Ge(Li) detector, BF3 long counter.
doi: 10.1016/0375-9474(79)90308-7
1978ZY03 Nucl.Phys. A301, 179 (1978) J.L.Zyskind, J.M.Davidson, M.T.Esat, M.H.Shapiro, R.H.Spear A cusp in the 54Cr(p, γ)55Mn reaction NUCLEAR REACTIONS 54Cr(p, γ), 54Cr(p, n), E=796 keV-3.7 MeV; measured products, 55Mn, Eγ, Iγ; deduced σ, σ(E). Data were imported from EXFOR entry C0671.
doi: 10.1016/0375-9474(78)90136-7
1977ES02 Phys.Lett. 72B, 49 (1977) M.T.Esat, D.C.Kean, R.H.Spear, M.P.Fewell, A.M.Baxter The Static Quadrupole Moment of the First Excited State of 198Hg NUCLEAR REACTIONS 198Hg(α, α'γ), E=14.1-18 MeV; 198Hg(12C, 12C'γ), E=43-54 MeV; 198Hg(16O, 16O'γ), E=60-80 MeV; measured Coulomb excitation reorientation effect. 198Hg level deduced quadrupole moment, B(E2).
doi: 10.1016/0370-2693(77)90060-0
1977SP05 Aust.J.Phys. 30, 133 (1977) R.H.Spear, J.P.Warner, A.M.Baxter, M.T.Esat, M.P.Fewell, S.Hinds, A.M.R.Joye, D.C.Kean Vibrational Excitations in the Even-Mass Cadmium Isotopes NUCLEAR REACTIONS 106,108,110,112,114,116Cd(α, α), (α, α'), E=17.5 MeV; measured σ(Eα'). 106,108,110,112,114,116Cd deduced levels.
doi: 10.1071/PH770133
1976ES01 Phys.Lett. 61B, 242 (1976) M.T.Esat, D.C.Kean, R.H.Spear, R.A.I.Bell Quadrupole Moments in the Cadmium Isotopes NUCLEAR REACTIONS 106,110,112,114,116Cd(α, α'γ), E=8.5 MeV; 106,110,112,114,116Cd(16O, 16O'γ), E=44 MeV; measured Coulomb excitation. 106,110,112,114,116Cd levels deduced B(E2).
doi: 10.1016/0370-2693(76)90139-8
1976ES02 Nucl.Phys. A274, 237 (1976) M.T.Esat, D.C.Kean, R.H.Spear, A.M.Baxter Mass Dependence of the Static Quadrupole Moments of the First 2+ States in the Cadmium Isotopes NUCLEAR REACTIONS 106,108,110,112,114,116Cd(α, α'), E=8-17 MeV; 106,108,110,112,114,116Cd(16O, 16O'), E=40-44 MeV; measured Coulomb excitation probabilities of first 2+ states. 106,108,110,112,114,116Cd deduced B(E2), quadrupole moment. Enriched targets.
doi: 10.1016/0375-9474(76)90239-6
1975SP02 Phys.Rev. C11, 742 (1975) R.H.Spear, R.A.I.Bell, M.T.Esat, P.R.Gardner, D.C.Kean, A.M.Baxter Electromagnetic Transitions in 22Na NUCLEAR REACTIONS 23Na(3He, αγ), E=8.46 MeV; measured αγ-coin. 19F(α, nγ), E=4.7-6.1, 11.2 MeV; measured σ(E, Eγ, θ), nγ(θ). 22Na levels deduced J, π, γ-mixing, Q0, g K-gR.
doi: 10.1103/PhysRevC.11.742
1974ES01 Nucl.Phys. A232, 139 (1974) M.T.Esat, J.R.Leslie, W.McLatchie Resonances in the Reaction 56Fe(p, γ)57Co NUCLEAR REACTIONS 56Fe(p, γ), E=1.2-1.5 MeV; measured σ(E;Eγ, θ). 57Co deduced levels, analog resonances, J, T, γ-mixing, resonance strengths. Natural target.
doi: 10.1016/0375-9474(74)90649-6
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