NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = D.H.Feng Found 67 matches. 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
1996CH08 Phys.Lett. 366B, 1 (1996) H.-T.Chen, C.L.Wu, D.H.Feng, A.Arima The Quadrupole-Quadrupole Interaction and the Inverted Pairing
doi: 10.1016/0370-2693(95)01322-9
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
1996PA28 Phys.Rep. 264, 311 (1996) X.-W.Pan, T.T.S.Kuo, M.Vallieres, D.H.Feng, A.Novoselsky Nuclear Shell-Model Calculations with Fundamental Nucleon-Nucleon Interactions NUCLEAR STRUCTURE 18O, 18F, 18Ne; calculated levels, binding energies, single particle energies in some cases. Shell model, fundamental NN-interaction.
doi: 10.1016/0370-1573(95)00045-3
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
1996SU12 Phys.Rep. 264, 375 (1996) High Spin Spectroscopy with the Projected Shell Model NUCLEAR STRUCTURE 162,164,166,168,170,172Hf, 160,162,164,166,168,170Yb, 158,160,162,164,166,168Er; calculated backbending plots, high-spins. 175Ta; calculated high-spin levels, band structure, ω vs spin. 174Hf, 176W; calculated ω vs spin. 173,175,177,179,181Ir, 171,173,175,177,179Re, 167,169,171,173,175Ta, 165,167,169Lu, 161,163,165,167,169,171Er; calculated high-spin levels transition energy. 169Ta; calculated high-spin levels, band structure.
doi: 10.1016/0370-1573(95)00049-6
1996WE07 Phys.Rev. C54, 1015 (1996) S.-X.Wen, H.Zheng, S.-G.Li, G.-S.Li, G.-J.Yuan, P.-F.Hua, P.-K.Weng, L.-K.Zhang, P.-S.Yu, C.-X.Yang, H.-B.Sun, Y.-B.Liu, Y.-Z.Liu, Y.Sun, D.H.Feng High Spin States in 175Ta: An acute example of delayed crossing frequency NUCLEAR REACTIONS 160Gd(19F, 4n), E=87 MeV; measured γγ-coin, DCO ratios. 175Ta deduced high-spin levels, J, π, B(λ) ratios, configurations, band structure. Cranking shell model.
doi: 10.1103/PhysRevC.54.1015
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
1995WA25 Phys.Rev. C52, 1792 (1995) J.C.Walpe, B.F.Davis, S.Naguleswaran, W.Reviol, U.Garg, X.-W.Pan, D.H.Feng, J.X.Saladin Lifetime Measurements in 120Xe NUCLEAR REACTIONS 106Pd(18O, 4n), E=70 MeV; measured Eγ, Iγ, recoil distance method spectra. 120Xe levels deduced T1/2, B(λ), quadrupole moments.
doi: 10.1103/PhysRevC.52.1792
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
1994FE08 Nucl.Phys. A570, 77c (1994) Dynamical Symmetry in Heavy Nuclei and Complementarity of Bosons and Fermions NUCLEAR STRUCTURE 196Pt; compiled, reviewed level predictions; deduced models complementarity features. Interacting boson, dynamical supersymmetry models, other nuclei discussed.
doi: 10.1016/0375-9474(94)90271-2
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
1994PA24 Phys.Rev. C50, 818 (1994) Normal and Exotic Collective States in the Fermion Dynamical Symmetry Model NUCLEAR STRUCTURE 134Ba; calculated levels, B(λ); deduced normal, exotic states unification, n-p quadrupole interaction role. Fermion dynamical symmetry model.
doi: 10.1103/PhysRevC.50.818
1994PA38 Phys.Lett. 336B, 285 (1994) A Revisit of SO(6) Dynamical Symmetry in Nuclear Structure NUCLEAR STRUCTURE 126,130Xe; analyzed γ-branching ratios. 128Xe, 196Pt; analyzed γ-branching ratios, B(λ) data; deduced similarity to SO(7), SO(6) symmetries transitional nuclei. Fermion dynamical symmetry model.
doi: 10.1016/0370-2693(94)90533-9
1994SU17 Phys.Rev. C50, 2351 (1994) Varied Signature Splitting Phenomena in Odd Proton Nuclei NUCLEAR STRUCTURE 169Ta; calculated levels; deduced signature splitting related features. Angular momentum projection theory, particle rotor model.
doi: 10.1103/PhysRevC.50.2351
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
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
1992WA16 Phys.Lett. 284B, 196 (1992) R.-P.Wang, F.-K.Thielemann, D.H.Feng, C.-L.Wu Microscopic Nuclear Masses and Their Astrophysical Implications NUCLEAR STRUCTURE A ≈ 210-260; calculated masses; deduced accurate level densities. Microscopic fermion dynamical symmetry model.
doi: 10.1016/0370-2693(92)90419-5
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
1991PI05 Phys.Rev. C43, 2224 (1991) J.-L.Pin, J.-Q.Chen, C.-L.Wu, D.H.Feng Nuclear Stretching NUCLEAR STRUCTURE 152Sm, 158Gd, 160Dy, 166Er, 166Yb, 170Hf, 188W; calculated B(λ). 162,164,166,168,170,172Er, 168,170,172,174,176,178,180Yb, 230,232,234,236,238,240U, 238,240,242,244,246Cm; calculated levels. Fermion dynamical symmetry model, stretching.
doi: 10.1103/PhysRevC.43.2224
1991WA11 Phys.Rev. C43, 2268 (1991) K.-X.Wang, G.-Z.Liu, D.F.Collinson, D.H.Feng, C.-L.Wu Test of the Composite Particle Representation Theory NUCLEAR STRUCTURE 20O, 20F, 20Ne; calculated levels. Composite particle representation theory.
doi: 10.1103/PhysRevC.43.2268
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
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.
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.
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
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
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
1986CA10 Phys.Rev.Lett. 56, 2578 (1986) R.F.Casten, C.-L.Wu, Da Hsuan Feng, J.N.Ginocchio, Xiao-Ling Han Empirical Evidence for an SO(7) Fermion Dynamical Symmetry in Nuclei NUCLEAR STRUCTURE 98,100,102,104,106Pd, 104,106,108,110,112Pd; calculated levels, B(E2) ratios; deduced dynamical symmetry evidence. Ginocchio model, SO(7) fermion dynamical symmetry.
doi: 10.1103/PhysRevLett.56.2578
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
1985SU05 Phys.Rev. C31, 1899 (1985) H.-Z.Sun, Da Hsuan Feng, M.Vallieres, R.Gilmore, P.van Isacker, A.Frank Spectroscopy of the Platinum Isotopes and the Dynamical Supersymmetry U(6/12) NUCLEAR STRUCTURE 195,196,197,198,199Pt; calculated levels, B(E2); deduced dynamical supersymmetry evidence. Interacting boson model.
doi: 10.1103/PhysRevC.31.1899
1985SU13 Phys.Lett. 163B, 7 (1985) The Analytic Wavefunctions of the Interacting Boson Model NUCLEAR STRUCTURE 134Ba; calculated levels. Interacting boson model, O(6) wave functions.
doi: 10.1016/0370-2693(85)90181-9
1985ZH08 Phys.Rev. C32, 1076 (1985) M.Zhang, M.Vallieres, R.Gilmore, Da Hsuan Feng, R.W.Hoff, H.-Z.Sun Structure of the Actinides by the Interacting Boson Model NUCLEAR REACTIONS 232Th, 236,234U(p, t), 232,234U, 230Th(t, p), E not given; calculated σ ratios. Interacting boson model wave functions. NUCLEAR STRUCTURE 232,234,236U, 230,232Th; calculated levels. 234U; calculated B(E2). Interacting boson model.
doi: 10.1103/PhysRevC.32.1076
1984FE11 Nucl.Phys. A421, 167c (1984) D.H.Feng, H.-Z.Sun, M.Vallieres, R.Gilmore, A.Frank, P.Van Isacker Dynamical Supersymmetry and Collective Nuclear Structure Physics NUCLEAR STRUCTURE 194,195,198,199Pt; analyzed levels; deduced dynamical supersymmetry unifying role.
doi: 10.1016/0375-9474(84)90344-0
1984LI20 Phys.Lett. 148B, 13 (1984) Y.-S.Ling, M.Zhang, J.-M.Xu, M.Vallieres, R.Gilmore, D.H.Feng, H.-Z.Sun The Multi-j Nuclear Dynamical Supersymmetry U(6/20) NUCLEAR STRUCTURE 196Pt, 197Au; calculated levels, B(E2); deduced supersymmetry model scheme. Groups, U(6/4), U(6/20).
doi: 10.1016/0370-2693(84)91600-9
1984PI14 Phys.Rev. C30, 1431 (1984) Transfer Reaction Sum Rules and the Interacting Boson-Fermion Model NUCLEAR STRUCTURE 194,196,198Pt; calculated pickup, stripping sum rule spectroscopic factors. Interacting boson-fermion model.
doi: 10.1103/PhysRevC.30.1431
1984SU01 Phys.Rev. C29, 352 (1984) H.-Z.Sun, M.Vallieres, Da Hsuan Feng, R.Gilmore, R.F.Casten Multi-j Supersymmetric Hamiltonian in the Pt Region NUCLEAR STRUCTURE 194,195,196,197,198,199Pt; analyzed levels; deduced supersymmetry parameter variation. Multi-j supersymmetry.
doi: 10.1103/PhysRevC.29.352
1984VA03 Phys.Lett. 135B, 339 (1984) M.Vallieres, H.-Z.Sun, D.H.Feng, R.Gilmore, R.F.Casten Structure of Alternative Supersymmetry Schemes in Nuclei NUCLEAR STRUCTURE 197Pt; calculated levels; deduced stretched configurations role, alternative supersymmetry schemes.
doi: 10.1016/0370-2693(84)90289-2
1980FE01 Phys.Rev.Lett. 44, 1037 (1980) D.H.Feng, M.A.Nagarajan, M.R.Strayer, M.Vallieres, W.T.Pinkston Exact Finite-Range Distorted-Wave Born-Approximation Analyses of the Reactions 18O(p, t)16O, 48Ca(t, p)50Ca, and 90Zr(t, p)93Zr Using Realistic Triton and Nuclear Wave Functions NUCLEAR REACTIONS 18O(p, t), E=20 MeV; 48Ca(t, p), E=12.08 MeV; 90Zr(t, p), E=11.89 MeV; calculated σ(θ). Finite-range DWBA, realistic t-, structure overlap-functions.
doi: 10.1103/PhysRevLett.44.1037
1980LI11 Nucl.Phys. A342, 165 (1980) J.S.Lilley, M.A.Franey, D.H.Feng Alpha Inelastic Scattering by 208Pb Near the Coulomb Barrier NUCLEAR REACTIONS 208Pb(α, α), (α, α'), E=23.5 MeV; measured σ(θ); deduced nuclear matter surface distribution, transition density, potential parameters. 208Pb level deduced B(E3), β. Deformed potential model, folding model.
doi: 10.1016/0375-9474(80)90512-6
1980ZH01 Phys.Scr. 22, 426 (1980) M.V.Zhukov, D.H.Feng, Cheng-li Wu, J.Bang Study of the Two-Nucleon Surface Correlation Via a Simple Three Body System NUCLEAR STRUCTURE 6He, 6Be, 18O, 18Ne, 42Ca, 42Ti; calculated levels. Three-body problem, two-nucleon surface clustering, Pauli effects.
doi: 10.1088/0031-8949/22/5/003
1979VA07 Phys.Lett. 83B, 267 (1979) M.Vallieres, D.H.Feng, W.T.Pinkston Angular Momentum and Binding Energy Effects in Two-Nucleon Transfer NUCLEAR STRUCTURE 42Ca, 42Sc, 42Ti; calculated two-nucleon transfer overlaps. 18O, 18F, 18Ne; calculated zero-range form factors for ground states. Extended basis shell model, well-depth model.
doi: 10.1016/0370-2693(79)91104-3
1978FE01 Lett.Nuovo Cim. 21, 195 (1978) D.H.Feng, W.W.Eidson, R.V.Kollarits Possible Compound-Nucleus Formation of Back-Angle Inelastic α-Particle Scattering NUCLEAR REACTIONS 24Mg(α, α'), E=28, 40 MeV; measured σ(Eα', θ).
doi: 10.1007/BF02822249
1978FE03 Phys.Rev. C18, 33 (1978) Exact Finite-Range Analysis of 12C(3He, n)14O Reaction NUCLEAR REACTIONS 12C(3He, n), E=10-22 MeV; measured σ(E, En, θ). Exact finite-range, zero-range DWBA analysis; normalization factors.
doi: 10.1103/PhysRevC.18.33
1978HU09 Phys.Rev. C18, 1534 (1978) H.S.Huber, T.K.Lim, Da Hsuan Feng Search for Efimov States in 12C NUCLEAR STRUCTURE 12C; calculated 0+ state Efimov characteristics through αα force.
doi: 10.1103/PhysRevC.18.1534
1978PI10 Phys.Rev. C18, 1011 (1978) W.T.Pinkston, M.Vallieres, D.H.Feng Two-Nucleon Transfer: Random-Phase Approximation Theory, Pairing Vibrations, and the Extended Basis Shell Model NUCLEAR REACTIONS 16O(p, t), E=40 MeV; 16O(t, p), E=10 MeV; calculated σ(θ).
doi: 10.1103/PhysRevC.18.1011
1977IB01 Nucl.Phys. A288, 397 (1977) R.H.Ibarra, N.Austern, M.Vallieres, D.H.Feng Two-Body Surface Correlations in 18O NUCLEAR STRUCTURE 18O; analyzed ground state wave function for surface clustering of the two active neutrons.
doi: 10.1016/0375-9474(77)90339-6
1977TA02 Phys.Lett. 66B, 109 (1977) T.Tamura, T.Udagawa, D.H.Feng, K.-K.Kan Deep Inelastic Reactions Treated as Multi-Step Direct Reaction Processes. Application to (p, p') Reaction NUCLEAR REACTIONS 27Al, 209Bi(p, p'), E=62 MeV; calculated σ(θ).
doi: 10.1016/0370-2693(77)90151-4
1976FE01 Phys.Rev. C13, 1151 (1976) D.H.Feng, A.R.Barnett, L.J.B.Goldfarb Systematics of Coulomb Excitation with Limited Effects from Nuclear Distortion NUCLEAR REACTIONS 152Sm, 208Pb, 234U(α, α'), E ≈ 15 MeV; measured calculated σ. Coulomb excitation systematics.
doi: 10.1103/PhysRevC.13.1151
1976FE08 Phys.Rev. C14, 1484 (1976) D.H.Feng, T.Tamura, T.Udagawa, J.Lynch, K.S.Low Absolute Cross Section of the Reaction 48Ca(18O, 16O)50Ca NUCLEAR REACTIONS 48Ca(18O, 16O), E=50 MeV; calculated σ(θ) to levels in 50Ca. DWBA, coupled-reaction-channel analyses.
doi: 10.1103/PhysRevC.14.1484
1976FE09 Nucl.Phys. A274, 262 (1976) Absolute Magnitude of Heavy-Ion Induced Two-Nucleon Transfer Reactions NUCLEAR REACTIONS 42,48Ca(16O, 18O), (16O, 14C), E=56 MeV; 48Ca(18O, 16O), E=50 MeV; 62Ni(18O, 16O), E=65 MeV; analyzed σ.
doi: 10.1016/0375-9474(76)90241-4
1976VA01 Nucl.Phys. A256, 21 (1976) M.Vallieres, D.H.Feng, R.H.Ibarra Note on the Harmonic Oscillator Calculation of Two-Nucleon Transfer Form Factors NUCLEAR REACTIONS 42Ca(p, t), 40Ca(t, p); calculated bound-state overlap; deduced form factor.
doi: 10.1016/0375-9474(76)90092-0
1976YA05 Phys.Rev. C14, 351 (1976) K.Yagi, D.L.Hendrie, U.Jahnke, C.F.Maguire, J.Mahoney, D.K.Scott, D.H.Feng, T.Udagawa, K.S.Low, T.Tamura 142Nd(18O, 16O)144Nd Reaction and its Contrast to 144Nd(12C, 14C)142Nd Reaction NUCLEAR REACTIONS 142Nd(18O, 16O), E=98 MeV; measured σ(E(16O), θ); deduced reaction mechanism. DWBA analysis.
doi: 10.1103/PhysRevC.14.351
1975IB01 Nucl.Phys. A241, 386 (1975) R.H.Ibarra, M.Vallieres, D.H.Feng Extended Basis Shell-Model Study of Two-Neutron Transfer Reactions NUCLEAR REACTIONS 18O(p, t), E=18 MeV; calculated σ(Et, θ). 16O(t, p), E=10 MeV; calculated σ(Ep, θ).
doi: 10.1016/0375-9474(75)90394-2
1974BA10 Phys.Lett. 48B, 290 (1974) A.R.Barnett, D.H.Feng, L.J.B.Goldfarb A Quantal Treatment of Octupole Coulomb-Nuclear Interference NUCLEAR REACTIONS 208Pb(α, α'), E=21, 22 MeV; measured σ(θ), calculated nuclear-Coulomb interference.
doi: 10.1016/0370-2693(74)90592-9
1973BA18 Nucl.Phys. A205, 513 (1973) Monte Carlo Calculations of Two-Neutron Transfer Cross Sections NUCLEAR REACTIONS 40Ca(t, p), E=10 MeV; 22Ne, 48Ca(p, t), E=40 MeV; calculated σ(θ).
doi: 10.1016/0375-9474(73)90703-3
1973FE06 Phys.Lett. 46B, 37 (1973) D.H.Feng, R.H.Ibarra, M.Vallieres Large Basis Shell-Model Study of Nucleon-Transfer Overlaps NUCLEAR STRUCTURE 16,18O; calculated overlap of groundstate wave functions.
doi: 10.1016/0370-2693(73)90469-3
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