NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = M.Guidry Found 96 matches. 2022LV08 Phys.Rev.Lett. 129, 042502 (2022) C.-J.Lv, F.-Q.Chen, Y.Sun, M.Guidry ΔI=2 Bifurcation as a Characteristic Feature of Scissors Rotational Bands NUCLEAR STRUCTURE 156Gd; calculated energy levels, B(E2), B(M1), staggering features for the scissors-mode rotational band, moments of inertia. Microscopic many-body. Comparison with available data.
doi: 10.1103/PhysRevLett.129.042502
2018YA24 Eur.Phys.J. A 54, 217 (2018) Y.-C.Yang, Y.-X.Liu, Y.Sun, M.Guidry Superdeformed band in the N = Z + 4 nucleus 40Ar : A projected shell model analysis NUCLEAR STRUCTURE 36,40Ar; calculated rotational band, yrast band levels vs J; compared with published data; deduced kinematical and dynamical moments of inertia vs rotational frequency, g-factor, B(E2) vs spin, neutron and proton pairing gaps using Projected Shell Model (PSM). Compared to data.
doi: 10.1140/epja/i2018-12651-x
2017WU09 Phys.Rev. C 95, 064314 (2017) X.Y.Wu, S.K.Ghorui, L.-J.Wang, Y.Sun, M.Guidry, P.M.Walker Systematic study of multi-quasiparticle K-isomeric bands in tungsten isotopes by the extended projected shell model NUCLEAR STRUCTURE 174,176,178,180,182,184,186W; calculated levels, J, π, K-isomeric bands, bandhead energies, two- and multi-particle Nilsson configurations, moment of inertia plots, B(E2), B(M1), B(M1)/B(E2), g factors. Comparison with experimental data.
doi: 10.1103/PhysRevC.95.064314
2007MA48 Phys.Rev. C 76, 015803 (2007); Erratum Phys.Rev. C 76, 039901 (2007) Z.Ma, D.W.Bardayan, J.C.Blackmon, R.P.Fitzgerald, M.W.Guidry, W.R.Hix, K.L.Jones, R.L.Kozub, R.J.Livesay, M.S.Smith, J.S.Thomas, D.W.Visser Astrophysically important 31S states studied with the 32S(p, d)31S reaction NUCLEAR REACTIONS 32S(p, d), E=32 MeV; measured Ed, σ and angular distributions. 31S deduced level energies and spectroscopic factors.
doi: 10.1103/PhysRevC.76.015803
2006CH30 Phys.Rev. C 74, 012801 (2006) K.Y.Chae, D.W.Bardayan, J.C.Blackmon, D.Gregory, M.W.Guidry, M.S.Johnson, R.L.Kozub, R.J.Livesay, Z.Ma, C.D.Nesaraja, S.D.Pain, S.Paulauskas, M.Porter-Peden, J.F.Shriner, Jr., N.Smith, M.S.Smith, J.S.Thomas First experimental constraints on the interference of (3/2)+ resonances in the 18F(p, α)15O reaction NUCLEAR REACTIONS 1H(18F, α), E(cm) ≈ 663-877 keV; measured particle spectra, excitation functions; deduced resonance interference effects. 19Ne deduced upper limits on resonance widths. R-matrix calculations.
doi: 10.1103/PhysRevC.74.012801
2005NE12 Nucl.Phys. A758, 174c (2005) C.D.Nesaraja, E.L.Lingerfelt, J.P.Scott, M.S.Smith, W.R.Hix, D.W.Bardayan, J.C.Blackmon, K.Chae, M.W.Guidry, R.A.Meyer A New Computational Infrastructure For Nuclear Astrophysics
doi: 10.1016/j.nuclphysa.2005.05.173
2004SM08 Nucl.Phys. A746, 565c (2004) M.S.Smith, W.R.Hix, S.Parete-Koon, L.Dessieux, Z.Ma, S.Starrfield, D.W.Bardayan, M.W.Guidry, D.L.Smith, J.C.Blackmon, A.Mezzacappa Element synthesis calculations for stellar explosions: robust uncertainties, sensitivities, and radioactive ion beam measurements
doi: 10.1016/j.nuclphysa.2004.09.091
2004SM09 Nucl.Phys. A746, 569c (2004) M.S.Smith, R.A.Meyer, D.W.Bardayan, J.C.Blackmon, K.Chae, M.W.Guidry, W.R.Hix, R.L.Kozub, E.J.Lingerfelt, Z.Ma, J.P.Scott Nuclear data on unstable nuclei for astrophysics
doi: 10.1016/j.nuclphysa.2004.09.092
2003BL11 Nucl.Phys. A718, 127c (2003) J.C.Blackmon, D.W.Bardayan, W.Bradfield-Smith, R.Brummitt, A.E.Champagne, A.A.Chen, T.Davinson, L.Dessieux, M.W.Guidry, K.I.Hahn, G.M.Hale, W.R.Hix, R.L.Kozub, Z.Ma, P.D.Parker, G.Rajbaidya, R.C.Runkle, C.M.Rowland, A.C.Shotter, M.S.Smith, L.A.Van Wormer, D.W.Visser, P.J.Woods The 14O(α, p)17F Reaction Rate NUCLEAR REACTIONS 1H(17F, 17F), (17F, 17F'), (17F, 14O), E(cm) ≈ 1-4 MeV; measured particle spectra. 17F(p, p'), E(cm)=2-2.5 MeV; deduced σ. 14O(α, p), E=low; deduced astrophysical reaction rate. R-matrix analysis.
doi: 10.1016/S0375-9474(03)00689-4
2003PA54 Astrophys.J. 598, 1239 (2003) S.Parete-Koon, W.R.Hix, M.S.Smith, S.Starrfield, D.W.Bardayan, M.W.Guidry, A.Mezzacappa A new 17F(p, γ)18Ne reaction rate and its implications for nova nucleosynthesis NUCLEAR REACTIONS 17F(p, γ), E=low; analyzed data; deduced reaction rates, implications for nucleosynthesis in novae.
doi: 10.1086/378979
2002LE09 Phys.Rev. C65, 041301 (2002) C.-T.Lee, Y.Sun, J.-Y.Zhang, M.Guidry, C.-L.Wu Microscopic Description of Band Structure at Very Extended Shapes in the A ∼ 110 Mass Region NUCLEAR STRUCTURE 108Cd; calculated rotational bands energy vs spin, transition quadrupole moments, g factors. Projected shell model, comparison with data.
doi: 10.1103/PhysRevC.65.041301
2002SU06 Nucl.Phys. A703, 130 (2002) Y.Sun, C.-L.Wu, K.Bhatt, M.Guidry SU(3) Symmetry and Scissors Mode Vibrations in Nuclei NUCLEAR STRUCTURE 168Er; calculated rotational bands energy vs spin, transitions B(E2); deduced SU(3) symmetry, scissors mode vibrations. Extended projected shell model.
doi: 10.1016/S0375-9474(01)01457-9
2001SU05 Phys.Rev. C63, 047306 (2001) g Factors and the Interplay of Collective and Single-Particle Degrees of Freedom in Superdeformed Mass-190 Nuclei NUCLEAR STRUCTURE 188,190,192,194,196Hg, 190,192,194,196,198Pb; calculated superdeformed bands g factors vs spin. Projected shell model.
doi: 10.1103/PhysRevC.63.047306
2000SU13 Phys.Rev. C61, 064323 (2000) Y.Sun, K.Hara, J.A.Sheikh, J.G.Hirsch, V.Velazquez, M.Guidry Multiphonon γ-Vibrational Bands and the Triaxial Projected Shell Model NUCLEAR STRUCTURE 156,158,160,162,164,166,168,170Er; calculated ground, γ-vibrational bands energy and spin, multiphonon bands properties. Triaxial projected shell model, unified treatment.
doi: 10.1103/PhysRevC.61.064323
2000SU15 Phys.Rev. C62, 021601 (2000) Y.Sun, J.-Y.Zhang, M.Guidry, J.Meng, S.Im Single-Particle and Collective Motion for Proton-Rich Nuclei in the Upper pf Shell NUCLEAR STRUCTURE 60,62Zn, 64,66Ge; calculated transition energies, B(E2). New Nilsson parameters.
doi: 10.1103/PhysRevC.62.021601
1999SU10 Phys.Rev.Lett. 83, 686 (1999) Y.Sun, J.-Y.Zhang, M.Guidry, C.-L.Wu Theoretical Constraints for Observation of Superdeformed Bands in the Mass-60 Region NUCLEAR STRUCTURE 60,62,64,66Zn; calculated superdeformed bands transition energies, moments of inertia; deduced role of pair alignment. Projected shell model.
doi: 10.1103/PhysRevLett.83.686
1999VE06 Nucl.Phys. A653, 355 (1999) V.Velazquez, J.G.Hirsch, Y.Sun, M.W.Guidry Backbending in Dy Isotopes within the Projected Shell Model NUCLEAR STRUCTURE 154,156,158,160,162,164Dy; calculated rotational bands quadrupole moments, B(E2), g-factors; deduced deformation. Projected shell model, comparisons with data.
doi: 10.1016/S0375-9474(99)00238-9
1999ZH12 J.Phys.(London) G25, 819 (1999) J.-Y.Zhang, Y.Sun, L.L.Riedinger, M.Guidry Does an Independent Quasiparticle Picture Hold in Mass-190 Superformed Nuclei ? NUCLEAR STRUCTURE 190,191Hg, 191,192Tl; analyzed superdeformed bands relative spins; deduced deviations from additivity. Projected shell model, independent quasiparticle picture.
doi: 10.1088/0954-3899/25/4/045
1998SU02 Phys.Rev.Lett. 80, 672 (1998) Y.Sun, C.-L.Wu, K.Bhatt, M.Guidry, D.H.Feng Scissors-Mode Vibrations and the Emergence of SU(3) Symmetry from the Projected Deformed Mean Field NUCLEAR STRUCTURE 168Er; calculated levels, J, π; deduced 1+ band collective scissors mode characterization. Nilsson+BCS, exact angular momentum projection.
doi: 10.1103/PhysRevLett.80.672
1998ZH24 Phys.Rev. C58, 868 (1998) J.-Y.Zhang, Y.Sun, L.L.Riedinger, M.Guidry Lack of Additivity in Mass-190 Superdeformed Bands NUCLEAR STRUCTURE 190,191,192Hg, 191,192Tl; analyzed superdeformed bands relative spins; deduced residual interactions. Projected shell model calculations.
doi: 10.1103/PhysRevC.58.868
1998ZH37 Phys.Rev. C58, R2663 (1998) J.-Y.Zhang, Y.Sun, M.Guidry, L.L.Riedinger, G.A.Lalazissis Single Particle and Collective Structure for Nuclei Near 132Sn NUCLEAR STRUCTURE 136Te, 142Xe; calculated rotational bands transition energies. 131,133Sn, 131In, 133Sb; calculated single-particle levels. Cd, Te, Xe; calculated ground-state deformations for N=62-102. Nilsson model, new parameter set. Comparisons with data.
doi: 10.1103/PhysRevC.58.R2663
1997SU07 Phys.Rev.Lett. 78, 2321 (1997) Systematic Description of Yrast Superdeformed Bands in Even-Even Nuclei of the Mass-190 Region NUCLEAR STRUCTURE 188,190,192,194,196Hg, 190,192,194,196,198Pb; analyzed yrast superdeformed bands Eγ, dynamical moment of inertia. 194Hg; analyzed transition quadrupole moments, g-factors. Projected shell model.
doi: 10.1103/PhysRevLett.78.2321
1996GU10 J.Phys.(London) G22, 425 (1996) M.W.Guidry, D.H.Feng, X.-W.Pan, C.-L.Wu Solution of the Nuclear Shell Model by Symmetry-Dictated Truncation
doi: 10.1088/0954-3899/22/4/004
1996PA03 Phys.Rev. C53, 715 (1996) X.-W.Pan, J.-L.Ping, D.H.Feng, J.-Q.Chen, C.-L.Wu, M.W.Guidry Fermion Dynamical Symmetry Model for the Even-Even and Even-Odd Nuclei in the Xe-Ba Region NUCLEAR STRUCTURE 120,122,124,127,129,131,133,126,128,130,132Xe, 131,133,135,137Ba; calculated levels, B(λ), relative B(λ) in some cases. Fermion dynamical symmetry.
doi: 10.1103/PhysRevC.53.715
1996SU03 Phys.Rev. C53, 2227 (1996) Y.Sun, C.-L.Wu, D.H.Feng, J.L.Egido, M.Guidry Identical Bands at Normal Deformation: Necessity of going beyond the mean-field approach NUCLEAR STRUCTURE 170Yb, 171Lu; analyzed identical band data; deduced need to go beyond mean field approach. Projected shell model.
doi: 10.1103/PhysRevC.53.2227
1996SU14 Phys.Rev. C54, 2967 (1996) Properties of ΔI = 4 Bifurcation from the Projected Shell Model NUCLEAR STRUCTURE 162,166Tm, 167Er, 165Ho, 170Yb; analyzed levels data. 136Pm; analyzed superdeformed bands; deduced ΔI=4 bifurcation sensitivity to quasiparticle distribution near Fermi surface. Projected shell model.
doi: 10.1103/PhysRevC.54.2967
1996WU09 Phys.Lett. 387B, 449 (1996) Z = 110-111 Elements and the Stability of Heavy and Superheavy Elements NUCLEAR STRUCTURE 256Rf, 258Db, 260Sg, 262Bh, 264Hs, 266Mt, 269Ds, 272Rg; calculated mass excess. ATOMIC MASSES 256Rf, 258Db, 260Sg, 262Bh, 264Hs, 266Mt, 269Ds, 272Rg; calculated mass excess.
doi: 10.1016/0370-2693(96)01072-6
1995GU25 Ann.Phys.(New York) 242, 135 (1995) The Dynamical Pauli Effect NUCLEAR STRUCTURE 162Dy; calculated 2n-transfer probability to 160Dy ground state. N=84-108; calculated single particle energy. Fermi dynamical symmetry model, dynamical Pauli effect.
doi: 10.1006/aphy.1995.1077
1995SM07 Phys.Rev.Lett. 75, 3086 (1995) B.H.Smith, X.-W.Pan, D.H.Feng, M.Guidry Universality of Symmetry and Mixed-Symmetry Collective Nuclear States NUCLEAR STRUCTURE 168Er, 160,162,164Dy, 154,156,158,160Gd, 144,148,150,152,154Sm, 142,146,148,150Nd; analyzed B(λ), level energy ratio; deduced symmetry universality evidence. Fermion dynamical symmetry model.
doi: 10.1103/PhysRevLett.75.3086
1995SU19 Phys.Rev.Lett. 75, 3398 (1995) ΔI = 4 Bifurcation Without Explicit Fourfold Symmetry NUCLEAR STRUCTURE 166Tm; calculated ΔI=4 bifurcation in yrast band; deduced staggering related features. Projected shell model.
doi: 10.1103/PhysRevLett.75.3398
1995SU21 Phys.Rev. C52, R2844 (1995) Quantitative Description of Superdeformed Bands with the Projected Shell Model NUCLEAR STRUCTURE 132Ce; calculated superdeformed band dynamical moment of inertia, Eγ. Projected shell model.
doi: 10.1103/PhysRevC.52.R2844
1995WU03 Phys.Rev. C51, R1086 (1995) C.-L.Wu, D.H.Feng, M.W.Guidry, H.-T.Chen, X.-W.Pan Single-Particle Nondegeneracy and SU(3) Fermion Dynamical Symmetry
doi: 10.1103/PhysRevC.51.R1086
1995ZH30 Phys.Rev. C52, R2330 (1995) J.-Y.Zhang, Y.Sun, M.Guidry, D.H.Feng Statistical Distribution of Inertial Parameters in Normally Deformed Nuclei NUCLEAR STRUCTURE 164Er, 186W; calculated yrast band kinematic, dynamical moment of inertia vs spin, Eγ. Projected shell, cranking models comparison, other nuclei included.
doi: 10.1103/PhysRevC.52.R2330
1994GU02 Nucl.Phys. A570, 109c (1994) Dynamical Symmetry and Truncation of the Spherical Shell Model NUCLEAR STRUCTURE 152,154,156,158Gd, 154,156,158,160,162,164Dy, 156,158,160,164,168,166Er; calculated, reviewed level spectra, B(λ) predictions. 196Pt; calculated, reviewed level spectra; deduced model advantages. Fermion dynamical symmetry model.
doi: 10.1016/0375-9474(94)90274-7
1994GU11 Nucl.Phys. A579, 163 (1994) Comments on the Origin of Gaps in Deformed Single-Particle Spectra
doi: 10.1016/0375-9474(94)90799-4
1994LI67 Int.J.Mod.Phys. E3, 1119 (1994) Z.-P.Li, M.W.Guidry, C.-L.Wu, D.H.Feng New Microscopic View of Nuclear Deformation NUCLEAR STRUCTURE N=60-150; analyzed B(E2) systematics, calculations; N=82-126; calculated energy surface primary, secondary minima deformation vs particle number in Sm isotopes, superdeformation discussed. Fermi dynamical symmetry model.
doi: 10.1142/S0218301394000334
1994PA08 Nucl.Phys. A570, 273c (1994) X.-W.Pan, D.H.Feng, J.-Q.Chen, M.W.Guidry The Mottelson-Valatin Effect in the SO(5) Scheme NUCLEAR STRUCTURE 128Xe, 132Ba; calculated SO(5) level spectra; deduced τ-bunching, SO(6) symmetry properties violation in γ-soft nuclei.
doi: 10.1016/0375-9474(94)90292-5
1994PA09 Phys.Rev. C49, 2493 (1994) X.-W.Pan, D.H.Feng, J.-Q.Chen, M.W.Guidry τ Compression in the SO(5) Scheme NUCLEAR STRUCTURE 132Ba; calculated levels. 128Xe; calculated levels, B(λ); deduced τ-compression features, origin. SO(6)+ pairing model.
doi: 10.1103/PhysRevC.49.2493
1994WE13 Nucl.Phys. A578, 1 (1994) T.R.Werner, J.Dobaczewski, M.W.Guidry, W.Nazarewicz, J.A.Sheikh Microscopic Aspects of Nuclear Deformation NUCLEAR STRUCTURE N ≤ 110; calculated equilibrium deformations for Kr, Sr, Zr, Mo, Gd, Er, Hf isotopes. 92,106Mo; calculated potential energy curves, ground state, deformation energies. Skyrme Hartree-Fock + BCS model based self-consistent approach.
doi: 10.1016/0375-9474(94)90966-0
1993FE07 Phys.Rev. C48, R1488 (1993) D.H.Feng, M.W.Guidry, X.-W.Pan, C.-L.Wu, I.Zlatev Effective Fermion SO(6) Dynamical Symmetry in the Platinum Nuclei NUCLEAR STRUCTURE 196Pt; calculated levels; deduced fermion SO(6) dynamical symmetry evidence.
doi: 10.1103/PhysRevC.48.R1488
1993GU08 Phys.Rev. C48, 1739 (1993) M.W.Guidry, M.R.Strayer, C.-L.Wu, D.H.Feng Some General Constraints on Identical Band Symmetries NUCLEAR STRUCTURE 192,194,196Hg, 234,236,238U, 238,240,242,244Pu, 246,248Cm, 248,250Cf; analyzed band structure; deduced normal, superdeformed identical bands related features.
doi: 10.1103/PhysRevC.48.1739
1993HE14 Phys.Rev. C48, 1879 (1993) K.G.Helmer, C.Y.Wu, D.Cline, A.E.Kavka, W.J.Kernan, E.G.Vogt, M.W.Guidry, X.L.Han, R.W.Kincaid, X.T.Liu, H.Schecter, J.O.Rasmussen, A.Shihab-Eldin, M.A.Stoyer, M.L.Halbert Search for Diabolical Pair Transfer in Two-Neutron Transfer Reactions NUCLEAR REACTIONS 206Pb(156Gd, 154Gd), (156Gd, 158Gd), E=888 MeV; measured Eγ, Iγ, γ-ray multiplicity; deduced diabolical pair transfer related features.
doi: 10.1103/PhysRevC.48.1879
1993KI03 Phys.Rev. C47, 277 (1993) R.W.Kincaid, H.Schechter, M.W.Guidry, S.Landowne, R.Donangelo, G.Leander Semiclassical Particle-Rotor Model of One-Neutron Transfer Reactions NUCLEAR REACTIONS 161Dy(58Ni, 59Ni), E=270 MeV; 161Dy(116Sn, 117Sn), E=637 MeV; analyzed nucleon transfer probabilities data; deduced transfer to ground, excited states bands. Semi-classical particle-rotor model.
doi: 10.1103/PhysRevC.47.277
1993WU05 Nucl.Phys. A565, 455 (1993) L.-A.Wu, C.-L.Wu, M.W.Guidry, D.H.Feng The Polarization Effect of SO(6) in the Fermion Dynamical Symmetry Model NUCLEAR STRUCTURE 133La; calculated levels; deduced band structure. Fermion dynamical symmetry model, SO(6) polarization effect.
doi: 10.1016/0375-9474(93)90221-I
1993WU06 Ann.Phys.(New York) 222, 187 (1993) Nuclear Superdeformation and the Supershell Fermion Dynamical Symmetry Model NUCLEAR STRUCTURE Z=60-110; N=60-150; calculated regions favorable for superdeformation. Other aspects related to superdeformation discussed. Supershell fermion dynamical symmetry model.
doi: 10.1006/aphy.1993.1021
1992HA06 Phys.Rev. C45, 1127 (1992) X.-L.Han, C.-L.Wu, D.H.Feng, M.W.Guidry Nuclear Masses in the Fermion Dynamical Symmetry Model NUCLEAR STRUCTURE Z ≥ 82; N ≥ 126; calculated neutron, proton separation pairing gap energies. Z=98, 114; calculated mass shell corrections components. Fermion dynamical symmetry model.
doi: 10.1103/PhysRevC.45.1127
1992WU06 Phys.Rev. C46, 1339 (1992) Is There Objective Evidence for Quantized Spin Alignment in Superdeformed Nuclei ( Question ) NUCLEAR STRUCTURE 192,191,193,194Hg, 194Pb, 194Tl; analyzed superdeformed band γ-transition energy analyses for spin determination; deduced quantized spin alignment related characteristics.
doi: 10.1103/PhysRevC.46.1339
1991CH17 Phys.Rev. C44, 559 (1991) J.-Q.Chen, D.H.Feng, M.W.Guidry, C.-L.Wu Comment on ' Comparison of Realistic and Symmetry-Determined S and D Pairs of 156Gd ' NUCLEAR STRUCTURE 156Gd; analyzed S-, D-pair determination criteria.
doi: 10.1103/PhysRevC.44.559
1991KE04 Nucl.Phys. A524, 344 (1991) W.J.Kernan, C.Y.Wu, X.T.Liu, X.L.Han, D.Cline, T.Czosnyka, M.W.Guidry, M.L.Halbert, S.Juutinen, A.E.Kavka, R.W.Kincaid, J.O.Rasmussen, S.P.Sorensen, M.A.Stoyer, E.G.Vogt Heavy-Ion Induced Transfer Reactions with Spherical and Deformed Nuclei NUCLEAR REACTIONS 117,118Sn, 161,162,163,164Dy(58Ni, X), (112Sn, X), (116Sn, X), E=285-637 MeV; measured Eγ, Iγ, γ(fragment)-coin; deduced quasielastic channels σ. DWBA, semi-classical calculations, pairing degrees of freedom. 4π soectrometer.
doi: 10.1016/0375-9474(91)90030-A
1991LI01 Phys.Rev. C43, R1 (1991) X.T.Liu, D.Cline, T.Czosnyka, M.W.Guidry, X.L.Han, A.E.Kavka, W.J.Kernan, R.W.Kincaid, S.P.Sorensen, E.G.Vogt, C.Y.Wu Two-Neutron Pairing Enhancement Factors NUCLEAR REACTIONS 162Dy(116Sn, 118Sn), 161Dy(116Sn, 117Sn), E=637 MeV; 162Dy(58Ni, 60Ni), 161Dy(58Ni, 59Ni), E=345 MeV; measured γ-spectra; deduced two-neutron pairing enhancement factors. 160Dy levels deduced one-, two-neutron pickup probabilities.
doi: 10.1103/PhysRevC.43.R1
1991WU04 Phys.Rev.Lett. 66, 1377 (1991) Comment on ' Spin Alignment in Superdeformed Hg Nuclei ' NUCLEAR STRUCTURE 192,194Hg; analyzed superdeformed band data; deduced spin alignment features.
doi: 10.1103/PhysRevLett.66.1377
1990CA21 Phys.Lett. 241B, 295 (1990) L.F.Canto, R.J.Donangelo, M.W.Guidry, A.F.Farhan, J.O.Rasmussen, P.Ring, M.A.Stoyer Alder-Winther-De Boer Method Applied to Diabolical Two-Neutron Transfer NUCLEAR REACTIONS 160Dy(208Pb, X), E=1100 MeV; calculated nucleon transfer probability fpr X=206Pb; deduced Berry phase signature.
doi: 10.1016/0370-2693(90)91645-R
1990WU05 Fizika(Zagreb) 22, 123 (1990) C.-L.Wu, M.W.Guidry, D.H.Feng, J.Q.Chen β-γ Vibrations and SU3 Symmetry in the Fermion Dynamical Symmetry Model NUCLEAR STRUCTURE A > 228; calculated (β-γ) vibrational bandhead energies. Fermion dynamical symmetry model.
1989WU02 Phys.Rev. C39, 298 (1989) C.Y.Wu, X.T.Liu, W.J.Kernan, D.Cline, T.Czosnyka, M.W.Guidry, A.E.Kavka, R.W.Kincaid, B.Kotlinski, S.P.Sorensen, E.Vogt Evidence for Oscillating Two-Neutron Transfer Probabilities at Large Radial Separation in Heavy-Ion Reactions NUCLEAR REACTIONS 162Dy(58Ni, 60Ni), E=285, 345 MeV; 162Dy(116Sn, 118Sn), E=637 MeV; measured σ(E(γ), θ), total Eγ, γ-multiplicity; deduced two-nucleon transfer probability features.
doi: 10.1103/PhysRevC.39.298
1988FE01 Phys.Rev. C37, 101 (1988) M.P.Fewell, N.R.Johnson, F.K.McGowan, J.S.Hattula, I.Y.Lee, C.Baktash, Y.Schutz, J.C.Wells, L.L.Riedinger, M.W.Guidry, S.C.Pancholi Lifetimes of Yrast and Near-Yrast States of 159,160,161Yb NUCLEAR REACTIONS 116Cd(48Ti, xn), E=205 MeV; 48Ti(116Cd, xn), E=495 MeV; measured Eγ, Iγ, total energy spectra, recoil distance. 159,160,161Yb deduced levels, J, π, sidefeeding Iγ, transition quadrupole moments, band structure.
doi: 10.1103/PhysRevC.37.101
1988FE03 Phys.Lett. 205B, 157 (1988) D.H.Feng, C.-L.Wu, M.W.Guidry, Z.-P.Li Dynamical Pauli Effects and the Saturation of Nuclear Collectivity NUCLEAR STRUCTURE Z=52-82; N=52-82; Z=82-126; N=126-184; analyzed B(E2). Fermion dynamical symmetry model.
1988KR16 Phys.Rev. C38, 2674 (1988) A.J.Kreiner, J.Davidson, M.Davidson, H.Mosca, L.L.Riedinger, C.R.Bingham, M.W.Guidry, A.C.Kahler Shape Coexistence in 189Tl NUCLEAR REACTIONS 169Tm(24Mg, 4n), E=125 MeV; 165Ho(28Si, 4n), E=140 MeV; 175Lu(20Ne, 6n), E=128 MeV; measured σ(Eγ, θγ), Eγ, Iγ, Iγ(θ). 189Tl deduced levels, J, π. Ge detectors.
doi: 10.1103/PhysRevC.38.2674
1987BU10 Phys.Lett. 191B, 333 (1987) P.A.Butler, C.Baktash, C.R.Bingham, M.Carpenter, D.Cline, B.Cox, M.W.Guidry, S.Juutinen, A.E.Kavka, W.J.Kernan, R.W.Kincaid, A.Larabee, I.Y.Lee, X.T.Liu, S.P.Sorensen, E.Vogt, C.Y.Wu Observation of Intrinsic Excitation in 160Dy following Heavy-Ion Transfer Reactions NUCLEAR REACTIONS 161Dy(58Ni, 59Ni), E=270 MeV; measured Eγ, Iγ, γγ-coin. 160Dy deduced levels, J, π, decay, band characteristics. Ge, NaI detectors.
doi: 10.1016/0370-2693(87)90618-6
1987GU06 Phys.Lett. 187B, 210 (1987) M.W.Guidry, C.-L.Wu, Z.-P.Li, D.H.Feng, J.N.Ginocchio An Algerbraic Fermion Description of Band Termination and Loss of Collectivity in Heavy Nuclei NUCLEAR STRUCTURE 162Dy, 160,166,174,176Yb, 168,172W; calculated B(E2) ratio relative to rigid rotor value. Algebraic fermion model.
doi: 10.1016/0370-2693(87)91082-3
1987GU14 Phys.Rev. C36, 609 (1987) M.W.Guidry, R.Donangelo, J.O.Rasmussen, M.S.Hussein Zero-Point Fluctuations and the Diffuseness of the Nuclear Surface NUCLEAR REACTIONS 114Cd(58Ni, X), E=230 MeV; 114Cd(16O, X), E=50 MeV; 114Cd(α, X), E=15 MeV; calculated photon number vs phase angle. Zero point fluctuations. NUCLEAR STRUCTURE 114Cd, 106,110Pd, 104Ru, 126,130Te; calculated inertial parameters, spring constants, zero point amplitudes.
doi: 10.1103/PhysRevC.36.609
1987HA18 Phys.Lett. 192B, 253 (1987) X.-L.Han, M.W.Guidry, D.H.Feng, K.-X.Wang, C.-L.Wu Evidence for Nuclear Shell Symmetries NUCLEAR STRUCTURE Z=36-100; calculated even-even nuclei B(E2) ratios; deduced shell symmetry evidence. Fermion dynamical symmetry model.
doi: 10.1016/0370-2693(87)90100-6
1987HA36 Phys.Rev. C36, 2132 (1987) R.L.Hahn, K.S.Toth, Y.LeBeyec, B.Lagarde, M.W.Guidry Reactions with 40Ar and 84Kr Leading to the same Compound Nucleus, 200Po NUCLEAR REACTIONS 160Dy(40Ar, xn)200Po, E=160-225 MeV; 116Cd(84Kr, xn)200Po, E=320-420 MeV; measured residual production σ(E). Statiscal model.
doi: 10.1103/PhysRevC.36.2132
1987JU03 Phys.Lett. 192B, 307 (1987) S.Juutinen, X.T.Liu, S.Sorensen, B.Cox, R.W.Kincaid, C.R.Bingham, M.W.Guidry, W.J.Kernan, C.Y.Wu, E.Vogt, T.Czosnyka, D.Cline, M.L.Halbert, I.Y.Lee, C.Baktash Anomalous Two-Neutron Transfer Cross Sections at Large Separation in Heavy Ion Reactions NUCLEAR REACTIONS 161,163Dy(116Sn, 117Sn), 162,164Dy(116Sn, 118Sn), E=637 MeV; 161Dy(58Ni, 59Ni), 162Dy(58Ni, 60Ni), E=345 MeV; measured two-particle transfer probabilities vs closest approach distance, Eγ vs γ-multiplicity; deduced slope parameters. Position sensitive detectors, spin spectrometer.
doi: 10.1016/0370-2693(87)90111-0
1987MC01 Phys.Rev. C35, 968 (1987) F.K.McGowan, N.R.Johnson, I.Y.Lee, W.T.Milner, C.Roulet, R.M.Diamond, F.S.Stephens, M.W.Guidry Test of the Triaxial Rotor Model and the Interacting Boson-Fermion Approximation Model Description of Collective States in 193Ir NUCLEAR REACTIONS 191,193Ir(40Ar, 40Ar'), E=160 MeV; 191,193Ir(136Xe, 136Xe'), E=617 MeV; measured Eγ, Iγ, relative γ-ray yields following Coulomb excitation. 191,193Ir deduced levels, J, π, K, B(E2). Enriched targets, parallel plate avalanche counters.
doi: 10.1103/PhysRevC.35.968
1987WU03 Phys.Lett. 188B, 25 (1987) C.Y.Wu, X.T.Liu, S.P.Sorensen, R.W.Kincaid, M.W.Guidry, D.Cline, W.J.Kernan, E.Vogt, T.Czosnyka, A.E.Kavka, M.A.Stoyer, J.O.Rasmussen, M.L.Halbert Population of High-Spin States in the Actinide Region by Heavy-Ion Transfer Reactions NUCLEAR REACTIONS 235U(58Ni, 59Ni), E=325 MeV; measured Eγ, Iγ, γ-multiplicity; deduced reaction mechanism. 234U deduced levels, J, π. Enriched Target.
doi: 10.1016/0370-2693(87)90699-X
1987WU06 Phys.Lett. 194B, 447 (1987) C.-L.Wu, X.-L.Han, Z.-P.Li, M.W.Guidry, D.H.Feng A Microscopic Formula for Actinide Masses NUCLEAR STRUCTURE Z=82-126; calculated masses. Dynamical symmetry, microscopic approach.
doi: 10.1016/0370-2693(87)90214-0
1986GU11 Phys.Lett. 176B, 1 (1986) M.W.Guidry, C.-L.Wu, D.H.Feng, J.N.Ginocchio, X.-G.Chen, J.-Q.Chen A Fermion Dynamical Symmetry Model for High-Spin Physics NUCLEAR STRUCTURE 232Th; calculated levels, E2 matrix elements. 160Yb; calculated levels, alignment. Interacting boson model, dynamical symmetry.
doi: 10.1016/0370-2693(86)90913-5
1986MC01 Phys.Rev. C33, 855 (1986) F.K.McGowan, N.R.Johnson, I.Y.Lee, W.T.Milner, C.Roulet, J.Hattula, M.P.Fewell, Y.A.Ellis-Akovali, R.M.Diamond, F.S.Stephens, M.W.Guidry Test of the Triaxial Rotor Model and the Interacting Boson Fermion Approximation Model Description of Collective States in 191Ir NUCLEAR REACTIONS 191Ir(40Ar, 40Ar'), E=160 MeV; 191Ir(136Xe, 136Xe'), E=617 MeV; measured Eγ, Iγ(θ) following Coulomb excitation. 191Ir deduced levels, J, π, B(λ).
doi: 10.1103/PhysRevC.33.855
1985BU22 Nucl.Instrum.Methods 239, 221 (1985) P.A.Butler, K.A.Connell, J.D.Burrows, A.M.Y.El-Lawindy, M.W.Guidry, A.N.James, G.D.Jones, C.Lauterbach, T.P.Morrison, J.Simpson The Application of a Multiple Gas Counter Spectrometer to the Study of Heavy Ion Reactions NUCLEAR REACTIONS 163Dy(58Ni, 58Ni'), (58Ni, 59Ni), E=280-304 MeV; measured (particle)γ-coin, s(θ). Multiple gas counter spectrometer.
doi: 10.1016/0168-9002(85)90719-3
1985FE02 Phys.Rev. C31, 1057 (1985) M.P.Fewell, N.R.Johnson, F.K.McGowan, J.S.Hattula, I.Y.Lee, C.Baktash, Y.Schutz, J.C.Wells, L.L.Riedinger, M.W.Guidry, S.C.Pancholi Collectivity of 160,161Yb at High Spin NUCLEAR REACTIONS 116Cd(48Ti, xn), 48Ti(116Cd, xn), E(cm)=145 MeV; measured γ-spectra, recoil distance. 160,161Yb levels deduced T1/2, γ-branching, quadrupole moments, yrast sequence, quasiparticle alignment role, induced triaxiality.
doi: 10.1103/PhysRevC.31.1057
1985GU04 Phys.Lett. 150B, 265 (1985) M.W.Guidry, R.W.Kincaid, R.Donangelo Angular Momentum Transfer in very Heavy Ion Direct Reactions NUCLEAR REACTIONS 156Gd, 238U(208Pb, X), (120Sn, X), (58Ni, X), (16O, X), E not given; calculated particle transfer probability vs angular momentum.
doi: 10.1016/0370-2693(85)91008-1
1985GU15 Phys.Lett. 163B, 79 (1985) M.W.Guidry, S.Juutinen, X.T.Liu, C.R.Bingham, A.J.Larabee, L.L.Riedinger, C.Baktash, I.Y.Lee, M.L.Halbert, D.Cline, B.Kotlinski, W.J.Kernan, T.M.Semkow, D.G.Sarantites, K.Honkanen, M.Rajagopalan Population of High Spin States in Transfer Reactions with very Heavy Ions NUCLEAR REACTIONS 161Dy(58Ni, 59Ni), E=270 MeV; measured (particle)(particle)γ-coin; deduced reaction mechanism. 160Dy deduced levels, J, π, yrast sequence.
doi: 10.1016/0370-2693(85)90196-0
1984DO05 Phys.Rev. C29, 1925 (1984) R.Donangelo, M.W.Guidry, R.E.Neese, M.J.Rhoades-Brown Angular Localization and Approximations to the Deformed Nuclear Potential in Heavy-Ion Reactions NUCLEAR REACTIONS 160Gd(40Ar, 40Ar'), E=140-180 MeV; calculated projectile excitation probability vs E. Deformed potential, Woods-Saxon form factors.
doi: 10.1103/PhysRevC.29.1925
1984GU22 Nucl.Phys. A430, 485 (1984) M.W.Guidry, R.E.Neese, C.R.Bingham, L.L.Riedinger, J.A.Vrba, I.Y.Lee, N.R.Johnson, G.R.Satchler, P.A.Butler, R.Donangelo, J.O.Rasmussen, D.L.Hillis, H.H.Kluge Heavy-Ion Inelastic Scattering from Deformed Nuclei NUCLEAR REACTIONS 162Dy(16O, 16O'), E=50-68 MeV; 232Th(86Kr, 86Kr'), E=350-450 MeV; 160Gd(40Ar, 40Ar'), E=100-170 MeV; 162Dy(40Ar, 40Ar'), E=120-170 MeV; 180Hf(40Ar, 40Ar'), E=135-175 MeV; 156Gd, 164Dy(40Ar, 40Ar'), E=120-160 MeV; measured γ(particle)-coin, σ(E); deduced ion-ion potentials. Gamma spectroscopy. Classical limit.
doi: 10.1016/0375-9474(84)90050-2
1982JO04 Phys.Rev. C26, 1004 (1982) N.R.Johnson, I.Y.Lee, F.K.McGowan, T.T.Sugihara, S.W.Yates, M.W.Guidry Lifetimes of States in the Transitional Nucleus 152Gd NUCLEAR REACTIONS 152Gd(40Ar, 40Ar'), E=147.2 MeV; measured Coulomb excitation, DSA, recoil. 152Gd levels deduced T1/2, B(E2).
doi: 10.1103/PhysRevC.26.1004
1982LE07 Phys.Rev. C25, 1865 (1982) I.Y.Lee, N.R.Johnson, F.K.McGowan, R.L.Robinson, M.W.Guidry, L.L.Riedinger, S.W.Yates Structure of Multiphonon Vibrational States in 108,110Pd NUCLEAR REACTIONS 108,110Pd(40Ar, 40Ar'), E=120, 129.1 MeV; measured Eγ, Iγ, γ-yields, Coulomb excitation, γ(θ). 108,110Pd deduced levels, γ-branching, B(E2), multiphonon vibrational character. Boson expansion, interacting boson model.
doi: 10.1103/PhysRevC.25.1865
1981GU05 Nucl.Phys. A361, 275 (1981) M.W.Guidry, T.L.Nichols, R.E.Neese, J.O.Rasmussen, L.F.Oliveira, R.Donangelo Two-Nucleon Transfer Reactions in Deformed Nuclei using very Heavy Ions NUCLEAR REACTIONS 154Sm(132Xe, 134Xe), E=500-580 MeV; calculated two-nucleon transfer probability to ground state bands. 158Gd(132Xe, 132Xe'), E=540 MeV; calculated ground state band excitation probability. Semiclassical method.
doi: 10.1016/0375-9474(81)90479-6
1981LE11 Phys.Rev. C24, 293 (1981) I.Y.Lee, N.R.Johnson, F.K.McGowan, G.R.Young, M.W.Guidry, S.W.Yates Isomeric and High-Spin States of 94Tc and the Search for Yrast Isomers near N ≈ 50 NUCLEAR REACTIONS 76Ge, 78Se(20Ne, xnyp), E=80.9 MeV; 89Y, 93Nb(10B, xnyp), E=52, 58.4, 62.8 MeV; measured Eγ, Iγ, γγ-, γ(X-ray)-coin, γγ(t). 94Tc deduced levels, isomer T1/2, yrast transition sequence.
doi: 10.1103/PhysRevC.24.293
1981RH01 Phys.Rev. C24, 2747 (1981) M.J.Rhoades-Brown, R.J.Donangelo, M.W.Guidry, R.E.Neese Quantum-Mechanical and Classical-Limit Coupled-Channels Calculations for very Heavy Systems NUCLEAR REACTIONS 160Gd(40Ar, 40Ar'), E=120-180 MeV; calculated collective state excitation probabilities. Coupled-channels calculation, quantum, classical limits.
doi: 10.1103/PhysRevC.24.2747
1980JO08 Phys.Rev. C22, 2416 (1980) N.R.Johnson, M.W.Guidry, R.J.Sturm, E.Eichler, R.O.Sayer, D.C.Hensley, N.C.Singhal Lifetimes of Rotational States in 154Sm NUCLEAR REACTIONS 154Sm(40Ar, 40Ar'), E=146, 153 MeV; measured Doppler shift, recoil, Coulomb excitation, Eγ, Iγ. 154Sm levels deduced T1/2, B(E2). Ridid rotor model.
doi: 10.1103/PhysRevC.22.2416
1980RA11 Nucl.Phys. A341, 149 (1980) J.Rasmussen, P.Moller, M.Guidry, R.Neese Giant Resonance Polarization Terms in the Nucleus-Nucleus Potential NUCLEAR REACTIONS 140Gd(40Ar, 40Ar'γ), E=100-155 MeV; 208Pb(208Pb, 208Pb'γ), E not given; calculated effective polarization potentials; deduced strength relative to real nuclear ion-ion potential. Giant resonances, adiabatic Coulomb coupling.
doi: 10.1016/0375-9474(80)90367-X
1980VR01 Phys.Rev. C22, 755 (1980) J.A.Vrba, C.R.Bingham, M.W.Guidry, R.E.Neese, E.E.Gross, T.P.Cleary, D.C.Hensley, E.V.Hungerford Search for α-Decay of High Spin Isomers in Rare Earth Nuclei NUCLEAR REACTIONS 142Nd(16O, xnypzα), E=146, 144, 135, 126 MeV; 139La, 141Pr(16O, xnypzα), E=146 MeV; measured limits on Eα, Iα, T1/2. 146,147,149Gd, 148Tb, 149,150,151,152Dy, 150,151,152Ho, 150,151,154Er levels deduced α-branching limit. Decay-in-flight technique.
doi: 10.1103/PhysRevC.22.755
1980YA03 Phys.Rev. C21, 2366 (1980) S.W.Yates, I.Y.Lee, N.R.Johnson, E.Eichler, L.L.Riedinger, M.W.Guidry, A.C.Kahler, D.Cline, R.S.Simon, P.A.Butler, P.Colombani, F.S.Stephens, R.M.Diamond, R.M.Ronningen, R.D.Hichwa, J.H.Hamilton, E.L.Robinson High-Spin Properties of 164Er in the Multiple Band Crossing Region NUCLEAR REACTIONS 150Nd(18O, 4n), E=69.6 MeV; 164Dy(α, 4n), E=51 MeV; 164Er(136Xe, 136Xe'γ), E=547, 612, 620 MeV; measured Eγ, Iγ, γγ-coin, Doppler-broadened lineshapes, multiple Coulomb excitation probabilities. 164Er deduced levels, J, π, T1/2, B(E2). Two quasiparticle plus rotor model.
doi: 10.1103/PhysRevC.21.2366
1979GU15 Phys.Rev. C20, 1814 (1979) M.W.Guidry, I.Y.Lee, N.R.Johnson, P.A.Butler, D.Cline, P.Colombani, R.M.Diamond, F.S.Stephens Reduced Transition Probabilities and Energies of High-Spin States in 162Dy NUCLEAR REACTIONS 162Dy(136Xe, 136Xe'), E(lab)=547, 612 MeV; measured T1/2, Eγ. 162Dy levels deduced B(E2).
doi: 10.1103/PhysRevC.20.1814
1979NE05 Phys.Lett. 85B, 201 (1979) R.E.Neese, M.W.Guidry, R.Donangelo, J.O.Rasmussen Surface Structure of Deformed Nuclei by Radial and Angular Localization in Heavy Ion Scattering NUCLEAR REACTIONS 160Gd(40Ar, 40Ar'), E=100-160 MeV; calculated excitation functions; deduced HI potential, semi-classical model, deformed nuclei.
doi: 10.1016/0370-2693(79)90578-1
1979RA34 Nucl.Phys. A332, 82 (1979) J.O.Rasmussen, M.W.Guidry, T.E.Ward, C.Castaneda, L.K.Peker, E.Leber, J.H.Hamilton Rotational Energy Expressions and Least-Squares Fitting of Backbenders and Similar Nuclei NUCLEAR STRUCTURE 130,132,134Ce, 158,160,162,164Er, 158Dy, 164,166,168Yb, 170W, 182Os; calculated rotational energies. Yrast, yrare states, band mixing, pairing interaction, Coriolis coupling.
doi: 10.1016/0375-9474(79)90096-4
1978DO11 Nucl.Phys. A308, 136 (1978) R.Donangelo, L.F.Oliveira, J.O.Rasmussen, M.W.Guidry Classical-Limit Description of Rotation-Vibrational Band Excitation in Deformed Even-Even Nuclei NUCLEAR REACTIONS 238U(40Ar, 40Ar'), E=170 MeV; 238U(86Kr, 86Kr'), E=400 MeV; calculated Coulomb excitation probability for K=0 octupole band in 238U.
doi: 10.1016/0375-9474(78)90446-3
1978GU03 Phys.Rev.Lett. 40, 1016 (1978) M.W.Guidry, P.A.Butler, R.Donangelo, E.Grosse, Y.El Masri, L.Y.Lee, F.S.Stephens, R.M.Diamond, L.L.Riedinger, C.R.Bingham, A.C.Kahler, J.A.Vrba, E.L.Robinson, N.R.Johnson Coulomb-Nuclear Interference for High-Spin States Excited by 86Kr, 40Ar, and 16O Projectiles NUCLEAR REACTIONS 232Th(86Kr, 86Kr'γ), E=350-450 MeV; 238U(40Ar, 40Ar'γ), E=140-220 MeV; 162Dy(16O, 16O'γ), E=50-70 MeV; measured HI γ-coin; deduced Coulomb-nuclear interference.
doi: 10.1103/PhysRevLett.40.1016
1978SA03 Phys.Rev. C17, 1026 (1978) R.O.Sayer, E.Eichler, N.C.Singhal, R.Sturm, N.R.Johnson, M.W.Guidry Recoil-Distance Measurement of Lifetimes of Rotational States in 164Dy NUCLEAR REACTIONS 164Dy(40Ar, 40Ar'), E=152.6 MeV; measured Eγ, recoil distance DSA. 164Dy levels deduced T1/2, B(E2).
doi: 10.1103/PhysRevC.17.1026
1976DO09 Phys.Lett. 64B, 377 (1976) R.Donangelo, M.W.Guidry, J.P.Boisson, J.O.Rasmussen The Classical-Limit S-Matrix for Coulomb Excitation NUCLEAR REACTIONS 168Er(d, d'), E=7 MeV; 168Er(α, α'), E=14 MeV; 168Er(10Be, 10Be'), E=45 MeV; calculated Coulomb excitation probabilities in 168Er.
doi: 10.1016/0370-2693(76)90100-3
1976GU06 Phys.Rev. C13, 1164 (1976) M.W.Guidry, R.J.Sturm, N.R.Johnson, E.Eichler, G.D.O'Kelley, N.C.Singhal, R.O.Sayer Recoil Distance Lifetimes of Rotational States in 236U NUCLEAR REACTIONS 236U(40Ar, 40Ar'γ), E=153, 155 MeV; measured Coulomb excitation. 236U levels deduced T1/2, B(E2), quadrupole moment.
doi: 10.1103/PhysRevC.13.1164
1976GU12 Nucl.Phys. A266, 228 (1976) M.W.Guidry, P.A.Butler, P.Colombani, I.Y.Lee, D.Ward, R.M.Diamond, E.Eichler, N.R.Johnson, R.Sturm Reduced Transition Probabilities for High-Spin States in 232Th NUCLEAR REACTIONS 232Th(84Kr, 84Kr'γ), E=385 MeV; 232Th(136Xe, 136Xe'γ), E=595, 623 MeV; measured recoil distance, Doppler broadened lineshape, Coulomb excitation yields. 232Th 6+-18+ levels deduced T1/2, B(E2). Results compared with theory.
doi: 10.1016/0375-9474(76)90292-X
1976GU16 Nucl.Phys. A274, 183 (1976) M.W.Guidry, H.Massmann, R.Donangelo, J.O.Rasmussen Theory of Coulomb-Nuclear Interference for Heavy-Ion Excitation of Rotational States NUCLEAR REACTIONS 238U(40Ar, X), E=150-200 MeV; calculated Coulomb-nuclear interference.
doi: 10.1016/0375-9474(76)90236-0
1976LE18 Phys.Rev.Lett. 37, 420 (1976) I.Y.Lee, D.Cline, R.S.Simon, P.A.Butler, P.Colombani, M.W.Guidry, F.S.Stephens, R.M.Diamond, N.R.Johnson, E.Eichler Coulomb Excitation into the Backbend Region of 164Er NUCLEAR REACTIONS 164Er(136Xe, 136Xe'γ), E=612, 547 MeV; measured multiple Coulomb excitation, 136Xe'γ-coin. 164Dy(α, 4n), E=51 MeV; measured Eγ, Iγ, γγ-coin. 164Er levels deduced B(E2), backbending.
doi: 10.1103/PhysRevLett.37.420
1975GU21 Phys.Rev. C12, 1937 (1975) M.W.Guidry, E.Eichler, N.R.Johnson, G.D.O'Kelley, R.J.Sturm, R.O.Sayer Sign of the E4 Moment in 236U by Multiple Coulomb Excitation with 40Ar Ions NUCLEAR REACTIONS 236U(40Ar, 40Ar'), E=145.8, 152.4 MeV; measured multiple coulomb excitation. 236U levels deduced M(E4), sign of E4 moment.
doi: 10.1103/PhysRevC.12.1937
1975JO07 Phys.Rev. C12, 1927 (1975) N.R.Johnson, R.J.Sturm, E.Eichler, M.W.Guidry, G.D.O'Kelley, R.O.Sayer, D.C.Hensley, N.C.Singhal, J.H.Hamilton Lifetimes of Rotational States in 232Th NUCLEAR REACTIONS 232Th(40Ar, 40Ar'γ), E=152 MeV; measured recoil-distance DSA, 40Ar'γ-coin. 232Th levels deduced T1/2, B(E2). Coulomb excitation.
doi: 10.1103/PhysRevC.12.1927
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