NSR Query Results
Output year order : Descending NSR database version of May 6, 2024. Search: Author = D.R.Lehman Found 48 matches. 2001FO06 Nucl.Phys. A684, 467c (2001) Tests of Effective Two-Body Models in 1H(d(pol), γ)3He Reactions NUCLEAR REACTIONS 1H(polarized d, γ), E=0-100 MeV; calculated analyzing powers. Effective two-body models, comparison with data.
doi: 10.1016/S0375-9474(01)00508-5
2000FO11 Few-Body Systems 28, 189 (2000) Dynamical Study of 1H(d(pol), γ)3He Tensor Observables in the Energy Range of 80 keV to 95 MeV: Tests of effective two-body models NUCLEAR REACTIONS 1H(polarized d, γ), E=0.08-95 MeV; calculated σ(θ), tensor analyzing powers. 3He(γ, p), E=5-40 MeV; calculated σ(θ). Comparisons with data. Validity of effective two-body models discussed.
doi: 10.1007/s006010070021
1997KO63 Few-Body Systems 23, 53 (1997) Y.Koike, W.C.Parke, L.C.Maximon, D.R.Lehman Accurate Three-Nucleon Bound-State Calculation with an Extended Separable Expansion of the Two-Body T-Matrix NUCLEAR STRUCTURE 3H; calculated binding energy. Extended seperable expansion, two-potential formalism.
doi: 10.1007/s006010050064
1996SC01 Phys.Rev. C53, 35 (1996) G.J.Schmid, R.M.Chasteler, H.R.Weller, D.R.Tilley, A.C.Fonseca, D.R.Lehman T20 Measurements for 1H(d(pol), γ)3He and the P-Wave Component of the Nucleon-Nucleon Force NUCLEAR REACTIONS 1H(polarized d, γ), E=12.7-19.8 MeV; measured T20(θ); deduced sensitivity to P-wave component of NN-force. Compared measurements to 3-body calculations.
doi: 10.1103/PhysRevC.53.35
1994GI18 Prog.Theor.Phys.(Kyoto), Suppl. 117, 339 (1994) B.F.Gibson, I.R.Afnan, J.A.Carlson, D.R.Lehman Importance of Baryon-Baryon Coupling in Hypernuclei
doi: 10.1143/PTPS.117.339
1994WE18 At.Data Nucl.Data Tables 58, 219 (1994) H.R.Weller, R.M.Chasteler, B.S.Marks, R.G.Seyler, D.R.Lehman Angular Distribution Coefficients for (γ, X) Reactions with Circularly Polarized Photons and Polarized Targets and a Correction to Previous Tables
doi: 10.1006/adnd.1994.1028
1993FO04 Phys.Rev. C48, R503 (1993) Full Three-Body Calculation for d(pol) + p → 3He + γ with a Realistic NN Interaction NUCLEAR REACTIONS 1H(polarized d, γ), E=10-95 MeV; analyzed vector, tensor analyzing power data. Realistic NN-interaction, full three-body calculation.
doi: 10.1103/PhysRevC.48.R503
1993FO08 Phys.Rev. C48, 2528 (1993) A.C.Fonseca, B.F.Gibson, D.R.Lehman Approximate Ways to Treat the Nucleon-Nucleon Tensor Force in the Four-Nucleon Bound State
doi: 10.1103/PhysRevC.48.2528
1992PU03 Phys.Rev. C46, 984 (1992) V.Punjabi, C.F.Perdrisat, E.Cheung, J.Yonnet, M.Boivin, E.Tomasi-Gustafsson, R.Siebert, R.Frascaria, E.Warde, S.Belostotsky, O.Miklukho, V.Sulimov, R.Abegg, D.R.Lehman T20 in the Inclusive Breakup of 4.5 GeV Polarized 6Li NUCLEAR REACTIONS 1H(polarized 6Li, X), E=4.5 GeV; measured inclusive breakup reaction analyzing power. 6Li deduced D-state characteristics.
doi: 10.1103/PhysRevC.46.984
1991FO07 Phys.Lett. 267B, 159 (1991) Exact Three-Body Calculation of Polarization Observables in 1H(d(pol), γ)3He NUCLEAR REACTIONS 1H(polarized d, γ), E=19.6 MeV; calculated T20(θ); deduced initial state three-body dynamics role. 3He deduced D-state role.
doi: 10.1016/0370-2693(91)91240-V
1991PA25 Few-Body Systems 11, 89 (1991) W.C.Parke, Y.Koike, D.R.Lehman, L.C.Maximon Quality of the Three-Nucleon Bound-State Wave Function from a Two-Nucleon Separable Expansion Method NUCLEAR STRUCTURE 3H; calculated binding energy, convergence; deduced wave function quality. Separable expansion method.
doi: 10.1007/BF01318554
1990LE24 J.Phys.(Paris), Colloq.C-6, 47 (1990) Evidence for and Explication of the D-State in Few-Nucleon Systems COMPILATION 2,3H, 3,4He, 6Li; compiled, reviewed D-state properties.
1989ES05 Phys.Rev. C39, 1685 (1989) A.Eskandarian, D.R.Lehman, W.C.Parke Inelastic (1+ → 0+) Electromagnetic Form Factor of 6Li from Three-Body Models NUCLEAR REACTIONS 6Li(e, e'), E not given; calculated charge form factor. 6Li level deduced deexcitation Γγ. Three-body models.
doi: 10.1103/PhysRevC.39.1685
1989LA13 Phys.Rev.Lett. 62, 2925 (1989) J.B.J.M.Lanen, A.M.van den Berg, H.P.Blok, J.F.J.van den Brand, C.T.Christou, R.Ent, A.G.M.van Hees, E.Jans, G.J.Kramer, L.Lapikas, D.R.Lehman, W.C.Parke, E.N.M.Quint, G.van der Steenhoven, P.K.A.de Witt Huberts Electrodisintegration of 6Li Studied with the Reaction 6Li(e, e'p) NUCLEAR REACTIONS 6Li(e, e'p), E not given; measured missing energy spectra, momentum distributions; deduced spectroscopic strength. Three-body model.
doi: 10.1103/PhysRevLett.62.2925
1988CH05 Phys.Rev. C37, 445 (1988) C.T.Christou, D.R.Lehman, W.C.Parke Structure of the 6Li → p + (nα) Vertex: Three-body formalism NUCLEAR STRUCTURE 6Li; calculated three-body vertex structure.
doi: 10.1103/PhysRevC.37.445
1988CH06 Phys.Rev. C37, 458 (1988) C.T.Christou, D.R.Lehman, W.C.Parke Structure of the 6Li → p + (nα) Vertex: 6Li(p, 2p)nα reaction NUCLEAR REACTIONS, MECPD 6Li(p, 2p), E=100-460 MeV; calculated σ(θ1, θ2, E1, E2). Three-body models.
doi: 10.1103/PhysRevC.37.458
1988ES01 Phys.Rev. C38, 2341 (1988); Erratum Phys.Rev. C39, 1188 (1989) A.Eskandarian, D.R.Lehman, W.C.Parke Elastic Electromagnetic Form Factors of 6Li from Three-Body Models NUCLEAR STRUCTURE 6Li; calculated monopole, quadrupole, magnetic form factors. Three-body model, Pauli repulsion for the valence nucleons.
doi: 10.1103/PhysRevC.38.2341
1988FR12 Phys.Rev. C37, 2859 (1988) J.L.Friar, B.F.Gibson, D.R.Lehman, G.L.Payne Trinucleon Asymptotic Normalization Constants: Comparison of 3He and 3H NUCLEAR STRUCTURE 3H, 3He; calculated asymptotic normalization constants. Configuration space Faddeev calculation.
doi: 10.1103/PhysRevC.37.2859
1988LE01 Phys.Rev. C37, 336 (1988) D.R.Lehman, L.C.Maximon, J.L.Friar Coulomb Effects in Asymptotic Normalization Constants: A soluble model NUCLEAR STRUCTURE 3H, 3He; calculated asymptotic normalization constant.
doi: 10.1103/PhysRevC.37.336
1988WE20 Ann.Rev.Nucl.Part.Sci. 38, 563 (1988) Manifestations of the D-State in Light Nuclei
doi: 10.1146/annurev.ns.38.120188.003023
1987LE04 Nucl.Phys. A463, 117c (1987) Low-Energy Photonuclear Reactions with 3He and 3H: A status report NUCLEAR REACTIONS 3H, 3He(γ, p), (γ, n), E=low; analyzed three-body photonuclear calculations.
doi: 10.1016/0375-9474(87)90653-1
1986EN05 Phys.Rev.Lett. 57, 2367 (1986) R.Ent, H.P.Blok, J.F.A.van Hienen, G.van der Steenhoven, J.F.J.van den Brand, J.W.A.den Herder, E.Jans, P.H.M.Keizer, L.Lapikas, E.N.M.Quint, P.K.A.de Witt Huberts, B.L.Berman, W.J.Briscoe, C.T.Christou, D.R.Lehman, B.E.Norum, A.Saha Reaction 6Li(e, e'd)4He and the α-d Momentum Distribution in the Ground State of 6Li NUCLEAR REACTIONS 6Li(e, e'd), E=480 MeV; measured missing mass spectrum, σ(θ(e'), E(e'), θd) vs momentum transfer, α-d momentum distribution; deduced reaction mechanism. Partial kinematics, enriched target. DWIA analysis, α-nucleon-nucleon model.
doi: 10.1103/PhysRevLett.57.2367
1986LE21 Few-Body Systems 1, 193 (1986) L-S Coupling and the Magnetic Moment of 6Li from Three-Body Models NUCLEAR MOMENTS 6Li; calculated μ, L-S orbital probabilities. Three-body models.
doi: 10.1007/BF01076711
1985CH01 Phys.Rev. C31, 250 (1985) C.T.Christou, C.J.Seftor, W.J.Briscoe, W.C.Parke, D.R.Lehman Consequences of Pauli Effects in 6Li and the Reaction 6Li(e, e'd)4He NUCLEAR REACTIONS 6Li(e, e'd), E=400 MeV; calculated σ(θd, θ(e), E(e)); deduced α-d cluster momentum, Pauli effect role. One-photon exchange, deuteron pole dominance.
doi: 10.1103/PhysRevC.31.250
1985LE08 Phys.Rev. C31, 1920 (1985); Erratum Phys.Rev. C37, 2266 (1988) 6Li → α + d Distorted-Wave Born Approximation Parameter D2 NUCLEAR REACTIONS 4He(d, d), E not given; calculated S-, D-wave function, D2 parameter; deduced relevance to 6Li three-body model interpretation, tensor force α-nucleon interaction roles.
doi: 10.1103/PhysRevC.31.1920
1984GI01 Phys.Rev. C29, 1017 (1984) Structure of the 3H → n + d(d(*)) Vertexes NUCLEAR STRUCTURE 3H; calculated binding energy, n-d component wave function percentages, asymptotic normalization constants, deuteron D-wave effects on vertex structure. Faddeev calculations, separable interactions.
doi: 10.1103/PhysRevC.29.1017
1984PA08 Phys.Rev. C29, 2319 (1984); Erratum Phys.Rev. C34, 1496 (1986) Further Consequences of the Excluded Bound State S1/2 α - N Interaction in 6He and 6Li NUCLEAR STRUCTURE 6Li, 6He; calculated spectator wave function parameters, wave function normalization, single nucleon radial densities, rms orbital radii. 6Li calculated cluster α+d l=0, 1, 2 partial wave momentum distributions. Atractive α-nucleus interaction, three-body models. RADIOACTIVITY 6He(β-); calculated β-decay rate, ft. Three-body models.
doi: 10.1103/PhysRevC.29.2319
1983LE01 Phys.Rev.Lett. 50, 98 (1983) A = 6 Shell Structure from Three-Body Dynamics NUCLEAR STRUCTURE 6Li, 6He; calculated single particle radial densities, orbital probabilities. Shell model, three-body dynamics.
doi: 10.1103/PhysRevLett.50.98
1983LE14 Phys.Rev. C28, 364 (1983) Shell Structure of the A = 6 Ground States from Three-Body Dynamics NUCLEAR STRUCTURE 6He, 6Li; calculated orbital probabilities, single particle radial densities. Three-body model.
doi: 10.1103/PhysRevC.28.364
1982FR07 Phys.Rev. C25, 1616 (1982) J.L.Friar, B.F.Gibson, D.R.Lehman, G.L.Payne Trinucleon Asymptotic Normalization Constants Including Coulomb Effects NUCLEAR STRUCTURE 3H, 3He; calculated asymptotic normalization constant. Faddeev calculations, Coulomb effects.
doi: 10.1103/PhysRevC.25.1616
1982LE08 Phys.Rev. C25, 2743 (1982) Alpha-Deuteron Structure of 6Li as Predicted by Three-Body Models NUCLEAR STRUCTURE 6Li; calculated spectroscopic factors, momentum distributions, asymptotic normalization factors. Three-body model, alpha-deuteron clusters.
doi: 10.1103/PhysRevC.25.2743
1982LE11 Phys.Rev. C25, 3146 (1982) Excluded Bound State in the S1/2 α - N Interaction and the Three-Body Binding Energies of 6He and 6Li NUCLEAR STRUCTURE 6He, 6Li; calculated binding energies. Three-body calculations, Pauli effects, Levinson theorem.
doi: 10.1103/PhysRevC.25.3146
1980HA03 Phys.Rev.Lett. 44, 237 (1980) E.P.Harper, D.R.Lehman, F.Prats Triton s-Wave Asymptotic Normalization Constants. NUCLEAR STRUCTURE 3H; calculated S-wave asymptotic normalization constant. One-boson-exchange model.
doi: 10.1103/PhysRevLett.44.237
1979LE03 Phys.Rev. C19, 310 (1979) D.R.Lehman, F.Prats, B.F.Gibson Suppression of the Isospin-1/2, Three-Body Photodisintegration of 3He NUCLEAR REACTIONS 3He(γ, d), (γ, n), E=10-40 MeV; calculated σ(θ, E); deduced isospin dependence. Exact three-body breakup formalism.
doi: 10.1103/PhysRevC.19.310
1978GI10 Phys.Rev. C18, 1042 (1978) 3H and 4He Binding Energies in the 'Truncated t-Matrix' Approximation NUCLEAR STRUCTURE 3H, 4He; calculated binding energies. Faddeev-Yacubovsky calculation.
doi: 10.1103/PhysRevC.18.1042
1978LE05 Phys.Rev. C17, 744 (1978) D.R.Lehman, M.Rai, A.Ghovanlou Separable-Potential Three-Body Model of the A = 6 System. II. 6Li Ground State NUCLEAR STRUCTURE 6Li; calculated binding energy, wave function, wave function components, normalization. Three body separable-potential model.
doi: 10.1103/PhysRevC.17.744
1978PA02 Phys.Lett. 74B, 158 (1978) W.C.Parke, A.Ghovanlou, C.T.Noguchi, M.Rajan, D.R.Lehman 6He β-Decay from a Three-Body Model of the A=6 System RADIOACTIVITY 6He; calculated β-decay rate, ft.
doi: 10.1016/0370-2693(78)90542-7
1977GI01 Phys.Rev. C15, 545 (1977) 3He(γ, 2p)n Reaction NUCLEAR REACTIONS 3He(γ, 2p), E=15-50 MeV; calculated σ(E). Exact 3-body calculations, separable potentials.
doi: 10.1103/PhysRevC.15.545
1977HE03 Phys.Lett. 66B, 1 (1977) C.R.Heimbach, D.R.Lehman, J.S.O'Connell Two-Body Electrodisintegration of 3He: Faddeev Calculation NUCLEAR REACTIONS 3He(e, e'), (e, e'p), E=56.6, 90 MeV; calculated σ.
doi: 10.1016/0370-2693(77)90597-4
1977HE22 Phys.Rev. C16, 2135 (1977) C.R.Heimbach, D.R.Lehman, J.S.O'Connell Three-Body Calculation of Two-Body Threshold Electrodisintegration of 3He and 3H NUCLEAR REACTIONS 3H, 3He(e, X); calculated two-body electrodisintegration.
doi: 10.1103/PhysRevC.16.2135
1976GI02 Phys.Rev. C13, 477 (1976) Three-Body Photodisintegration of 3He NUCLEAR REACTIONS 3He(γ, X); calculated σ.
doi: 10.1103/PhysRevC.13.477
1976GI09 Phys.Rev. C14, 685 (1976); Erratum Phys.Rev. C15, 2257 (1977) Four-Body Bound States from the Schroder Equation with Separable Potentials NUCLEAR STRUCTURE 4He; calculated 4-body bound state. Schrodinger equation with separable potentials.
doi: 10.1103/PhysRevC.14.685
1976LE01 Phys.Rev. C13, 35 (1976) Integral Relation for the Asymptotic Normalization of the Triton NUCLEAR STRUCTURE 3H; calculated integral relation for asymptotic normalization constant of n-d tail in triton wave function.
doi: 10.1103/PhysRevC.13.35
1975GI01 Phys.Rev. C11, 29 (1975) Two-Body Photodisintegration of 3He and 3H NUCLEAR REACTIONS 3H, 3He(γ, X), E < 40 MeV; calculated wavefunctions.
doi: 10.1103/PhysRevC.11.29
1974GH01 Phys.Rev. C9, 1730 (1974) Separable-Potential Three-Body Model of the A = 6 System. I. 6He Ground State NUCLEAR STRUCTURE 6He; calculated binding energy, wave function, contribution of wave function components to normalization. Three-body, separable-potential model.
doi: 10.1103/PhysRevC.9.1730
1972KI11 Phys.Rev. C6, 769 (1972) P.Kitching, G.A.Moss, W.C.Olsen, W.J.Roberts, J.C.Alder, W.Dollhopf, W.J.Kossler, C.F.Perdrisat, D.R.Lehman, J.R.Priest Reactions (p, pd) and (p, 2p) on Helium-3 at 590 MeV NUCLEAR REACTIONS 3He(p, 2p), (p, pd), E=590 MeV; measured σ(Ep).
doi: 10.1103/PhysRevC.6.769
1972LE42 Phys.Rev. C6, 2023 (1972) Quasifree Proton-Proton and Proton-Deuteron Scattering on 3He NUCLEAR REACTIONS 3He(p, 2p), (p, pd), E=155, 587 MeV; calculated σ. Pole-dominance approximation.
doi: 10.1103/PhysRevC.6.2023
1971LE08 Phys.Rev. C3, 1827 (1971); Erratum Phys.Rev. C4, 1010 (1971) Quasielastic Electron Scattering from 3He and 3H NUCLEAR REACTIONS 3H, 3He(e, e'p), E=250, 450 MeV; calculated σ(Ee', Ep, θ(p)).
doi: 10.1103/PhysRevC.3.1827
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