NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = J.Copnell Found 19 matches. 2017PE01 Nucl.Phys. A957, 240 (2017) P.Petkov, A.Dewald, O.Moller, I.Deloncle, R.Chapman, S.Pascu, D.Bucurescu, D.Tonev, M.Reese, C.Fransen, S.Y.Araddad, G.Asova, J.Copnell, N.Goutev, M.Hackstein, J.Jolie, J.C.Lisle, J.N.Mo, Th.Pissulla, W.Rother, A.G.Smith, C.Tenereiro, D.M.Thompson, K.O.Zell On the quadrupole collectivity in the yrast band of 168Yb NUCLEAR REACTIONS 154Sm(18O, 4n), E=80 MeV;124Sn(48Ca, 4n), E=189 MeV; measured Eγ, Iγ, γγ-coin, RDDS (Recoil distance Doppler-shift) spectra using five large volume Ge (Sm target) and 21 escape-suppressed HPGe (Sn target). 168Yb deduced T1/2, B(E2) of levels using lifetime analysis with differential decay curve method (one B(E2) deduced using published T1/2), yrast band quadrupole moments; calculated B(E2) vs spin. Yrast band moments of inertia and B(E2) compared with published values for 164,166,168,170Yb; deduced indication for reduced collectivity at low spin unexplained by available calculations.
doi: 10.1016/j.nuclphysa.2016.09.006
1998WH04 Nucl.Phys. A644, 277 (1998) G.N.White, N.J.Stone, J.Rikovska, S.Ohya, J.Copnell, T.J.Giles, Y.Koh, I.S.Towner, B.A.Brown, B.Fogelberg, L.Jacobsson, P.Rahkila, M.Hjorth-Jensen Magnetic Dipole Moments Near 132Sn: New measurement on 135I by NMR/ON RADIOACTIVITY 135I(β-) [from 233U(n, F), E=thermal]; measured Iγ(θ, H, T), NMR on oriented nuclei. 135I deduced ground state g, μ. Shell model, core polarization, mesonic exchange currents. NUCLEAR STRUCTURE 125,127,129,131,133Sb, 133,135I, 137Cs, 139La; calculated μ. Shell model.
doi: 10.1016/S0375-9474(98)00597-1
1998WH05 Nucl.Phys. A640, 322 (1998) G.White, J.Rikovska, N.J.Stone, J.Copnell, I.S.Towner, A.M.Oros, K.Heyde, B.Fogelberg, L.Jacobsson, F.Gustavsson Magnetic Dipole Moments Near 132Sn: Measurement on isomeric 11/2- states in odd-A 131Te and 133Te by NMR/ON RADIOACTIVITY 131,133Te(β-) [from 233U(n, F)]; measured Eγ, Iγ(θ, T, H), NMR on oriented nuclei. 131,133Te deduced isomeric states g, μ. Shell model, core polarization, mesonic exchange currents, particle-core coupling model.
doi: 10.1016/S0375-9474(98)00461-8
1997JE07 Z.Phys. A359, 127 (1997) H.J.Jensen, R.A.Bark, R.Bengtsson, G.B.Hagemann, P.O.Tjom, S.Y.Araddad, C.W.Beausang, R.Chapman, J.Copnell, A.Fitzpatrick, S.J.Freeman, S.Leoni, J.C.Lisle, J.Simpson, A.G.Smith, D.M.Thompson, S.J.Warburton, J.Wrzesinski Loss of Alignment Gain in the πh9/2[541 (1/2)-)] (x) (νi13/2)2 Band in 167Tm and Neighbouring Odd-Z N = 98 Nuclei NUCLEAR REACTIONS 124Sn(48Ca, 4np), E=210 MeV; measured Eγ, Iγ, γγ-coin. 167Tm deduced high-spin levels, J, π, band structure. Cranked shell model calculations, data from other nuclei compared.
doi: 10.1007/s002180050377
1996SM05 J.Phys.(London) G22, 1411 (1996) D.H.Smalley, A.G.Smith, S.Y.Araddad, C.W.Beausang, R.Chapman, J.Copnell, A.Fitzpatrick, S.J.Freeman, S.Leoni, F.Linden, J.C.Lisle, J.F.Sharpey-Schafer, J.Simpson, J.P.Sweeney, D.M.Thompson, W.Urban, S.J.Warburton, J.Wrzesinski Evidence for a Rotational Alignment in a High-K Band in 167Yb NUCLEAR REACTIONS 124Sn(48Ca, 5n), E=210 MeV; measured γγ-coin. 167Yb deduced high-spin levels, J, π, K, Iγ, band structure, alignment, configuration.
doi: 10.1088/0954-3899/22/10/006
1996TE02 Phys.Rev. C53, 2870 (1996) C.Tenreiro, J.C.Acquadro, P.A.B.Freitas, R.Liguori Neto, G.Ramirez, N.Cuevas, P.R.S.Gomes, R.Cabezas, R.M.Anjos, J.Copnell Elastic amd Inelastic Scattering of 16O + 64Zn at Near-Barrier Energies NUCLEAR REACTIONS 64Zn(16O, 16O), (16O, 16O'), E(cm)=41.6-51.2 MeV; measured σ(θ); deduced model parameters. Optical, coupled-channels models.
doi: 10.1103/PhysRevC.53.2870
1995CO31 Phys.Rev. A51, R879 (1995) J.Copnell, W.R.Phillips, A.R.Barnett, K.E.Rehm, I.Ahmad, J.Gehring, B.G.Glagola, W.Kutschera Internal Conversion in Highly Stripped 83Kr Ions RADIOACTIVITY 83mKr(IT) [from 197Au(83Kr, 83Kr'), E=650 MeV]; measured total decay probabilities per unit time. 83Kr deduced transition ICC.
doi: 10.1103/PhysRevA.51.R879
1995FI01 Nucl.Phys. A582, 335 (1995) A.Fitzpatrick, S.Y.Araddad, R.Chapman, J.Copnell, F.Liden, J.C.Lisle, A.G.Smith, J.P.Sweeney, D.M.Thompson, W.Urban, S.J.Warburton, J.Simpson, C.W.Beausang, J.F.Sharpey-Schafer, S.J.Freeman, S.Leoni, J.Wrzesinski Proton Alignments at High Rotational Frequency in 167,168Yb NUCLEAR REACTIONS 124Sn(48Ca, 5n), (48Ca, 4n), E=210 MeV; measured Eγ, Iγ, γγγ-coin. 167,168Yb deduced high-spin levels, J, π, rotational bands, aligned angular momentum. Cranking, Nilsson, Woods-Saxon models.
doi: 10.1016/0375-9474(94)00459-Z
1995GA13 J.Phys.(London) G21, 193 (1995) S.J.Gale, J.Simpson, M.A.Riley, J.F.Sharpey-Schafer, E.S.Paul, M.A.Bentley, A.M.Bruce, R.Chapman, R.M.Clark, S.Clarke, J.Copnell, D.M.Cullen, P.Fallon, A.Fitzpatrick, P.D.Forsyth, S.J.Freeman, P.M.Jones, M.J.Joyce, F.Liden, J.C.Lisle, A.O.Macchiavelli, A.G.Smith, J.F.Smith, J.Sweeney, D.M.Thompson, S.Warburton, J.N.Wilson, I.Ragnarsson Band Termination Spectroscopy in 157Er NUCLEAR REACTIONS 114Cd(48Ca, 5n), E=210 MeV; measured γγγ-, γγγγ-coin, Eγ, Iγ, γγ(θ). 157Er deduced high-spin levels, transition energies, Iγ, J, π. Enriched targets, EUROGAM array of escape suppressed spectrometers (Ge and BGO detectors). Cranked-shell model, cranked Nilsson-Strutinsky calculations, band terminating states.
1995SM02 Nucl.Phys. A587, 150 (1995) A.G.Smith, R.Chapman, D.C.Clark, J.Copnell, S.J.Freeman, F.Khazaie, G.S.Li, J.C.Lisle, J.N.Mo, C.Tenreiro, D.M.Thompson, G.J.Yuan, J.Espino, G.B.Hagemann Electromagnetic Properties of 161Tm at High Spin NUCLEAR REACTIONS 128Te(37Cl, 4n), E=170 MeV; measured Eγ, γγ-coin, Iγ, DSA. 161Tm deduced high-spin levels, T1/2, B(M1), B(E2). Enriched targets, array of Compton-suppressed Ge detectors.
doi: 10.1016/0375-9474(94)00810-A
1995WA21 Nucl.Phys. A591, 323 (1995) S.J.Warburton, R.Chapman, J.Copnell, F.Liden, A.G.Smith, J.P.Sweeney, D.M.Thompson, S.J.Freeman, G.B.Hagemann, M.Piiparinen Configuration-Dependent Transition Rates in 161Tm NUCLEAR REACTIONS 128Te(37Cl, 4n), E=167 MeV; measured γγ-coin, RDM. 161Tm deduced high-spin levels, J, π, quasiparticle alignments, routhians, T1/2, δ, B(λ), ratios. Enriched targets, array of Compton-suppressed Ge detectors, inner ball of barium fluoride detectors, recoil distance methods.
doi: 10.1016/0375-9474(95)00179-5
1994SI10 Phys.Lett. 327B, 187 (1994) J.Simpson, M.A.Riley, S.J.Gale, J.F.Sharpey-Schafer, M.A.Bentley, A.M.Bruce, R.Chapman, R.M.Clark, S.Clarke, J.Copnell, D.M.Cullen, P.Fallon, A.Fitzpatrick, P.D.Forsyth, S.J.Freeman, P.M.Jones, M.J.Joyce, F.Linden, J.C.Lisle, A.O.Macchiavelli, A.G.Smith, J.F.Smith, J.Sweeney, D.M.Thompson, S.Warburton, J.N.Wilson, T.Bengtsson, I.Ragnarsson Single Particle Excitations and Properties of Multiple Band Terminations Near Spin 50(h-bar) in 158Er NUCLEAR REACTIONS 114Cd(48Ca, 4n), E=210 MeV; measured γγ-coin. 158Er deduced levels, J, π, band structure, configuration. Cranked Nilsson-Strutinsky calculations.
doi: 10.1016/0370-2693(94)90716-1
1993CI01 Phys.Rev. C47, 1294 (1993) J.A.Cizewski, M.A.C.Hotchkis, J.L.Durell, J.Copnell, A.S.Mowbray, J.Fitzgerald, W.R.Phillips, I.Ahmad, M.P.Carpenter, R.V.F.Janssens, T.L.Khoo, E.F.Moore, L.R.Morss, Ph.Benet, D.Ye New N = 84 Isotone: 136Te RADIOACTIVITY 248Cm(SF); measured γγ-coin. 252Cf(SF); measured Eγ, Iγ. 136Te deduced levels, J, π, transitions.
doi: 10.1103/PhysRevC.47.1294
1992CO21 Phys.Rev. C46, 1301 (1992) J.Copnell, S.J.Robinson, J.Jolie, K.Heyde Structure of the N = 84 Isotones 138Xe-146Sm NUCLEAR STRUCTURE 138Xe, 140Ba, 142Ce, 143,144Nd, 148Sm; calculated levels, B(λ). Interacting boson model, particle-core model.
doi: 10.1103/PhysRevC.46.1301
1992CO25 J.Phys.(London) G18, 1943 (1992) J.Copnell, K.Kumar, S.J.Robinson, C.Tenreiro An Application of the Dynamic Deformation Model to the N = 84 Isotones 138Xe-146Sm NUCLEAR STRUCTURE 138Xe, 146Sm, 140Ba, 142Ce, 144Nd; calculated levels, B(λ), δ. Dynamic deformation model.
doi: 10.1088/0954-3899/18/12/010
1992CO26 Z.Phys. A344, 35 (1992) J.Copnell, S.J.Robinson, W.Lippert, V.Rabbel Levels of 138Xe Populated in the β-Decay of 138I RADIOACTIVITY 138I(β-) [from 235U(n, F), E=thermal]; measured Eγ, Iγ, βγ-coin, γγ-coin. 138Xe deduced levels, J, π.
doi: 10.1007/BF01291017
1991PE12 Nucl.Phys. A533, 49 (1991) P.Petkov, W.Andrejtscheff, J.Copnell, S.J.Robinson E1 and M1 Transition Strengths from Two-Quasiparticle Structures in 168Er NUCLEAR REACTIONS 167Er(n, γ), E=thermal; measured Eγ, Iγ, γγ(t). 168Er levels deduced T1/2, B(λ). Natural target, Ge detectors, generalized centroid-shift analysis, E1 systematics.
doi: 10.1016/0375-9474(91)90819-R
1990VE10 Phys.Rev. C42, 588 (1990) M.Veskovic, I.Bikit, I.Anicin, W.D.Hamilton, J.Copnell, M.Krmar, J.Slivka Some Aspects of the 111Cd Level Scheme NUCLEAR REACTIONS 110Cd(n, γ), E=thermal; measured γ- spectra, γγ-coin; deduced σ(n, γ). 111Cd deduced level, isomer population mode.
doi: 10.1103/PhysRevC.42.588
1989CO06 Phys.Lett. 222B, 1 (1989) J.Copnell, S.Robinson, J.Jolie, K.Heyde Test of the Interacting Boson Approximation in the N = 84 Isotones Using Particle-Core Coupling NUCLEAR STRUCTURE 144Nd; calculated levels, B(λ), δ, μ, quadrupole moment. Interacting boson approximation.
doi: 10.1016/0370-2693(89)90713-2
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