NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = J.M.Lambert Found 35 matches. 2005SE05 Phys.Rev. C 71, 034006 (2005) H.R.Setze, C.R.Howell, W.Tornow, R.T.Braun, D.E.Gonzalez Trotter, A.H.Hussein, R.S.Pedroni, C.D.Roper, F.Salinas, I.Slaus, B.Vlahovic, R.L.Walter, G.Mertens, J.M.Lambert, H.Witala, W.Glockle Cross-section measurements of neutron-deuteron breakup at 13.0 MeV NUCLEAR REACTIONS 2H(n, n), (n, 2n), E=13 MeV; measured En, nn-coin, σ(θ1, θ2) for seven exit-channel configurations. Comparison with model predictions.
doi: 10.1103/PhysRevC.71.034006
1998HO08 Nucl.Phys. A631, 692c (1998) C.R.Howell, H.R.Setze, W.Tornow, R.T.Braun, W.Glockle, A.H.Hussein, J.M.Lambert, G.Mertens, C.D.Roper, F.Salinas, I.Slaus, D.E.Gonzalez Trotter, B.Vlahovic, R.L.Walter, H.Witala Implications of the Space-Star Anomaly in nd Breakup NUCLEAR REACTIONS 2H(n, np), E=13.0 MeV; measured σ(φ(12), θ(n1), θ(n2)); deduced space-star configuration anomaly.
doi: 10.1016/S0375-9474(98)00093-1
1997FE06 Phys.Rev. C56, 38 (1997) P.D.Felsher, C.R.Howell, W.Tornow, M.L.Roberts, J.M.Hanly, G.J.Weisel, M.Al Ohali, R.L.Walter, I.Slaus, J.M.Lambert, P.A.Treado, G.Mertens, A.C.Fonseca, A.Soldi, B.Vlahovic Analyzing Power Measurements for the d(pol) + d → d + p + n Breakup Reaction at 12 MeV NUCLEAR REACTIONS 2H(polarized d, nd), E=12 MeV; measured d, p, n spectra, σ(θ1, θ2) vs arc length, vector, tensor analyzing powers vs (θ1, θ2, arc length); deduced contributions from nucleon-nucleon P interactions. Impulse approximation calculations.
doi: 10.1103/PhysRevC.56.38
1996SE14 Phys.Lett. 388B, 229 (1996) H.R.Setze, C.R.Howell, W.Tornow, R.T.Braun, W.Glockle, A.H.Hussein, J.M.Lambert, G.Mertens, C.D.Roper, F.Salinas, I.Slaus, D.E.Gonzalez Trotter, B.Vlahovic, R.L.Walter, H.Witala Verification of the Space-Star Anomaly in nd Breakup NUCLEAR REACTIONS 2H(n, np), E=1-15 MeV; measured σ(θ1, θ2) vs arc length, total energy spectra, space-star, coplanar-star configurations; deduced space-star configuration related anomaly evidence.
doi: 10.1016/S0370-2693(96)01069-6
1995HO24 Nucl.Instrum.Methods Phys.Res. B99, 316 (1995) C.R.Howell, H.R.Setze, R.T.Braun, D.E.Gonzalez Trotter, A.H.Hussein, C.D.Roper, F.Salinas, I.Slaus, W.Tornow, B.Vlahovic, R.L.Walter, G.Mertens, J.M.Lambert, H.Witala Probing the Three-Nucleon Force using Nucleon-Deuteron Breakup Reactions NUCLEAR REACTIONS 2H(n, X), E=13 MeV; measured σ(θ1, θ2) vs arc length in space-star, coplanar-star configurations following target breakup; deduced implications related to 3N-forces.
doi: 10.1016/0168-583X(94)00680-6
1994BO54 Phys.Rev. D49, 3091 (1994) P.E.Bosted, R.G.Arnold, C.C.Chang, J.Gomez, A.T.Katramatou, C.J.Martoff, G.G.Petratos, A.A.Rahbar, S.E.Rock, A.F.Sill, Z.M.Szalata, D.J.Sherden, J.M.Lambert, R.M.Lombard-Nelsen Threshold Inelastic Electron Scattering from the Proton at High Momentum Transfers NUCLEAR REACTIONS 1H(e, e), E ≈ threshold; measured σ, missing mass squared region; deduced structure function scaling.
doi: 10.1103/PhysRevD.49.3091
1993HO24 Phys.Rev. C48, 2855 (1993) C.R.Howell, P.D.Felsher, W.Tornow, M.L.Roberts, J.M.Hanly, G.J.Weisel, M.Al Ohali, R.L.Walter, I.Slaus, J.M.Lambert, P.A.Treado, G.Mertens Novel Probe of Charge Symmetry Breaking: Deuteron-Induced Deuteron Breakup NUCLEAR REACTIONS 2H(polarized d, pd), (polarized d, nd), (polarized d, np), E=12 MeV; measured vector, tensor analyzing power vs θ; deduced breakup reaction suitability as charge symmetry breaking probe.
doi: 10.1103/PhysRevC.48.2855
1993SI29 Phys.Rev. D48, 29 (1993) A.F.Sill, R.G.Arnold, P.E.Bosted, C.C.Chang, J.Gomez, A.T.Katramatou, C.J.Martoff, G.G.Petratos, A.A.Rahbar, S.E.Rock, Z.M.Szalata, D.J.Sherden, J.M.Lambert, R.M.Lombard-Nelsen Measurements of Elastic Electron-Proton Scattering at Large Momentum Transfer NUCLEAR REACTIONS 1H(e, e), E at GeV/c; measured σ(θ). 1H deduced magnetic, Dirac form factors.
doi: 10.1103/PhysRevD.48.29
1992WE10 Phys.Rev. C46, 1599 (1992) G.J.Weisel, W.Tornow, C.R.Howell, P.D.Felsher, M.Al Ohali, Z.P.Chen, R.L.Walter, J.M.Lambert, P.A.Treado, I.Slaus Neutron-Proton Analyzing Power Data between 7.6 and 18.5 MeV NUCLEAR REACTIONS 1H(polarized n, n), E=7.6-18.5 MeV; measured analyzing power vs θ. Comparison with theory.
doi: 10.1103/PhysRevC.46.1599
1991HO26 Nucl.Instrum.Methods Phys.Res. B56/57, 459 (1991) C.R.Howell, W.Tornow, H.G.Pfutzner, M.L.Roberts, K.Murphy, P.D.Felsher, G.J.Weisel, G.Mertens, R.L.Walter, J.M.Lambert, P.A.Treado, I.Slaus Neutron-Deuteron Elastic Scattering and Breakup Reactions Below 20 MeV NUCLEAR REACTIONS 2H(polarized n, n), E=12 MeV; 2H(n, X), E=13 MeV; compiled, reviewed analyzing power vs θ, σ(θ1, θ2) vs arc length data for breakup.
doi: 10.1016/0168-583X(91)96070-2
1990HO14 Nucl.Instrum.Methods Phys.Res. A290, 424 (1990) C.R.Howell, W.Tornow, H.G.Pfutzner, A.Li, M.L.Roberts, K.Murphy, P.D.Felsher, G.J.Weisel, A.Naqvi, R.L.Walter, J.M.Lambert, P.A.Treado, I.Slaus Techniques for Vector Analyzing Power Measurements of the 2H(n(pol), np)n Breakup Reaction at Low Energies NUCLEAR REACTIONS 2H(polarized n, np), E=12 MeV; measured σ(En), vector analyzing power. High accuracy, breakup reaction.
doi: 10.1016/0168-9002(90)90560-S
1990WE13 J.Phys.(Paris), Colloq.C-6, 515 (1990) G.J.Weisel, W.Tornow, C.R.Howell, P.D.Felsher, M.Alohali, Z.P.Chen, R.L.Walter, J.M.Lambert, P.A.Treado Neutron-Proton Analyzing Power Data at 7.6, 12.0, 14.1, 16.0, 18.5 MeV NUCLEAR REACTIONS 1H(polarized n, n), E=7.6-18.5 MeV; measured analyzing power vs θ, spin correlation coefficient.
1988HO14 Phys.Rev.Lett. 61, 1565 (1988) C.R.Howell, W.Tornow, I.Slaus, P.D.Felsher, M.L.Roberts, H.G.Pfutzner, Anli Li, K.Murphy, R.L.Walter, J.M.Lambert, P.A.Treado, H.Witala, W.Glockle, T.Cornelius Rigorous Calculations and Measurements of A(y)(θ) for n + d Elastic-Scattering and Breakup Processes NUCLEAR REACTIONS 2H(polarized n, np), E=12 MeV; measured vector analyzing power vs θ. Three-nucleon calculations.
doi: 10.1103/PhysRevLett.61.1565
1988SU12 Few-Body Systems 4, 39 (1988) I.Supek, I.Slaus, Y.Koike, P.A.Treado, J.M.Lambert Two-Body Forces and Amplitudes in the Three-Body Model for the 4He(d(pol), pα)n Reaction with E(d) = 12 and 17 MeV NUCLEAR REACTIONS 4He(polarized d, pα), E=12, 17 MeV; analyzed σ(θα, θp), analyzing power vs arc length; deduced impulse, multiple scattering amplitudes roles. Three-body forces.
doi: 10.1007/BF01076274
1987CO34 Nucl.Phys. A475, 407 (1987) F.D.Correll, R.E.Brown, G.G.Ohlsen, R.A.Hardekopf, N.Jarmie, J.M.Lambert, P.A.Treado, I.Slaus, P.Schwandt, P.Doleschall Study of the Reaction H(d(pol), 2p)n at 16 MeV Around Collinear Configurations NUCLEAR REACTIONS, MECPD 1H(polarized d, 2p), E=16 MeV; measured σ(E(p3), θ(p3), E(p4), θ(p4)), analyzing powers vs arc length. Three-body Faddeev analysis.
doi: 10.1016/0375-9474(87)90071-6
1985BR33 Nucl.Instrum.Methods Phys.Res. B10/11, 356 (1985) R.E.Brown, R.A.Hardekopf, N.Jarmie, F.D.Correll, J.M.Lambert, P.A.Treado, I.Slaus, P.Schwandt, W.W.Jacobs, H.O.Meyer, E.J.Stephenson, J.Q.Yang, W.T.H.van Oers, P.Doleschall, J.A.Tjon Polarization in Three-Nucleon Breakup: Experiment and theory NUCLEAR REACTIONS 1H(polarized d, d), E=16, 79 MeV; measured vector analyzing power vs rotation angle. Faddeev formalism.
doi: 10.1016/0168-583X(85)90268-X
1983MY01 Phys.Rev. C28, 29 (1983) L.T.Myers, J.M.Lambert, P.A.Treado, I.Slaus, E.P.Harper, D.W.Devins, R.G.Allas 3He(p, pp)2H and 3He(p, pp)2H(*) at 136 MeV NUCLEAR REACTIONS 3He(p, 2p), E=136 MeV; measured σ(E1, E2, θ1, θ2); deduced deuteron, neutron-proton final state production σ ratio. Plane wave impulse approximation, one boson exchange, Reid soft core potential, quasifree scattering.
doi: 10.1103/PhysRevC.28.29
1983SL01 Nucl.Phys. A397, 205 (1983) I.Slaus, J.M.Lambert, P.A.Treado, F.D.Correll, R.E.Brown, R.A.Hardekopf, N.Jarmie, Y.Koike, W.Gruebler The 4He(d(pol), αp)n Reaction at 12 and 17 MeV NUCLEAR REACTIONS 4He(polarized d, pα), E=12, 17 MeV; measured σ(E(α), θ(α), E(p), θ(p)), analyzing powers vs arc length. Three-body Fadeev analysis, energy and angle dependence.
doi: 10.1016/0375-9474(83)90102-1
1982LA14 Phys.Rev. C26, 357 (1982) J.M.Lambert, P.A.Treado, P.G.Roos, N.S.Chant, A.Nadasen, I.Slaus, Y.Koike Deuteron Breakup by 140 MeV Alpha Particles at Quasifree Scattering Conditions NUCLEAR REACTIONS 2H(α, αp), E=140 MeV; measured σ(Eα, Ep, θα, θp). Three-body Faddeev analysis.
doi: 10.1103/PhysRevC.26.357
1979LA14 Nucl.Phys. A329, 25 (1979) J.M.Lambert, L.T.Myers, P.A.Treado, R.G.Allas, R.O.Bondelid, L.A.Beach, E.L.Petersen, I.Slaus Quasifree Processes in the 3He + 3H and 3He + 3He Interactions NUCLEAR REACTIONS 3He(3He, p3He), (3He, d3He), (3He, p), (3He, d), (3He, pα), 3H(3He, p3He), (3He, 2d), (3He, pt), (3He, dt), E=50, 65, 78 MeV; measured breakup σ(E, θ1, θ2); deduced fourier transforms, energy, angle dependence. PWIA analysis.
doi: 10.1016/0375-9474(79)90278-1
1978AL21 Nucl.Phys. A304, 461 (1978) R.G.Allas, L.A.Beach, R.O.Bondelid, L.T.Myers, E.L.Petersen, J.M.Lambert, P.A.Treado, I.Slaus Two-Spectator Quasifree Processes NUCLEAR REACTIONS 3He(3He, 2d), E=50, 78 MeV; 2H(d, 2p), E=34.7 MeV; measured σ(E, θ) at two-spectator condition. PWIA analyses.
doi: 10.1016/0375-9474(78)90244-0
1977HA19 Phys.Rev. C16, 42 (1977) M.I.Haftel, R.G.Allas, L.A.Beach, R.O.Bondelid, E.L.Petersen, I.Slaus, J.M.Lambert, P.A.Treado Application of the Three-Body Model to the Reactions 6Li(3He, t3He)3He and 6Li(3He, 3He3He)3H NUCLEAR REACTIONS 6Li(3He, 3He3He), (3He, t3He), E=45 MeV; measured σ for symmetric angle pairs. Faddeev calculations, Coulomb corrections.
doi: 10.1103/PhysRevC.16.42
1977SL04 Nucl.Phys. A286, 67 (1977) I.Slaus, R.G.Allas, L.A.Beach, R.O.Bondelid, E.L.Petersen, J.M.Lambert, P.A.Treado, R.A.Moyle Quasifree Processes in the 2H + 3He Interaction NUCLEAR REACTIONS 3He(d, pd), 3He(d, p3He), 3He(d, pt), E=22.3, 35 MeV; 2H(3He, pd), 2H(3He, p3He), 2H(3He, pt), E=30, 33.5, 52.5 MeV; measured σ(E, θ1, θ2). PWIA analysis, extracted fourier transforms.
doi: 10.1016/0375-9474(77)90008-2
1976LA01 Phys.Rev. C13, 43 (1976) J.M.Lambert, P.A.Treado, R.G.Allas, L.A.Beach, R.O.Bondelid, E.M.Diener 2H(p, 2p) Reaction at 23 MeV under the Condition of Collinearity of the Final State Particles in the Center-of-Mass System NUCLEAR REACTIONS 2H(p, 2p), E=23 MeV; measured σ. Faddeev calculation, two potentials.
doi: 10.1103/PhysRevC.13.43
1974AL01 Phys.Rev. C9, 787 (1974) R.G.Allas, L.A.Beach, R.O.Bondelid, E.M.Diener, E.L.Petersen, J.M.Lambert, P.A.Treado, I.Slaus Mechanisms in the Reactions 3H + 3He and 3H + 2H and Measurement of the Reaction 3H(p, 3He)n from 13.6 to 32.8 MeV NUCLEAR REACTIONS 3H(p, 3He), E=13.6-32.8 MeV; measured σ(Ep;θ). Determined 3H content of target, reanalyzed 3H + 3He, 3H + 2H quasifree reactions.
doi: 10.1103/PhysRevC.9.787
1974PE02 Phys.Rev. C9, 508 (1974) E.L.Petersen, M.I.Haftel, R.G.Allas, L.A.Beach, R.O.Bondelid, P.A.Treado, J.M.Lambert, M.Jain, J.M.Wallace 2H(p, pp)n Reaction at 23 MeV NUCLEAR REACTIONS 2H(p, 2p), E=23 MeV; measured σ(θ(1), θ(2), E), quasielastic angles. Faddeev calculation, 3 potentials, 3 codes.
doi: 10.1103/PhysRevC.9.508
1973SL03 Phys.Rev. C8, 444 (1973) I.Slaus, R.G.Allas, L.A.Beach, R.O.Bondelid, E.L.Petersen, J.M.Lambert, D.L.Shannon Mechanisms in 3H + 3He and 3H + 2H Reactions NUCLEAR REACTIONS 3H(3He, d3He), (3He, p3He), (3He, 2d), (3He, pt), (3He, dt), E=50 MeV; 3H(d, 2d), (d, pt), E=35 MeV; measured σ. Deduced quasifree reaction mechanism.
doi: 10.1103/PhysRevC.8.444
1973TR04 Phys.Rev. C7, 1742 (1973) P.A.Treado, J.M.Lambert, R.J.Kane, L.A.Beach, E.L.Petersen, R.B.Theus Excited States of 4He and 5He from Sequential α + d Reactions at E = 70 MeV NUCLEAR REACTIONS 2H(α, pd), (α, dt), Eα=70 MeV; measured pd-, dt-coin. Deduced level-width. 4He, 5He deduced levels.
doi: 10.1103/PhysRevC.7.1742
1972BA93 Nucl.Phys. A196, 197 (1972) S.I.Baker, C.R.Gossett, P.A.Treado, J.M.Lambert, L.A.Beach Doppler-Shift Attenuation Measurements on 24Mg by (α, α') and (p, p') Reactions NUCLEAR REACTIONS 24Mg(α, α'), E=42, 50 MeV; 24Mg(p, p'), E=22 MeV; measured Doppler-shift attenuation. 24Mg deduced T1/2.
doi: 10.1016/0375-9474(72)90960-8
1972KA08 Nucl.Phys. A179, 725 (1972) R.J.Kane, J.M.Lambert, P.A.Treado Isospin and Decay Modes of 6Li States from 7Li(tau, α)6Li and 7Li(tau, α)6Li*(d)4He Reactions at E = 1.5 MeV NUCLEAR REACTIONS 7Li(3He, α), 7Li(3He, αα), E=1.5 MeV; measured σ(Eα, E(6Li), θ(α), θ(6Li)), σ(Ed, Eα, θ(d), θ(α)), σ(Eα, Eα, θ(α), θ(α)). 6Li deduced levels, decay modes, isospins. Natural, enriched targets.
doi: 10.1016/0375-9474(72)90615-X
1972TR07 Nucl.Phys. A198, 21 (1972) P.A.Treado, J.M.Lambert, V.E.Alessi, R.J.Kane Angular Correlation and Reaction Mechanism for 11B(p, α)8Be(2.9)(α)4He with E < 1.4 MeV
doi: 10.1016/0375-9474(72)90769-5
1971LA14 Phys.Rev.Lett. 27, 820 (1971) J.M.Lambert, P.A.Treado, D.Haddad, R.A.Moyle, J.C.Sessler Reaction Mechanisms of 10B(d, α)8B2. 9(α)4He for E = 0.4, 1.0, and 1.5 MeV NUCLEAR REACTIONS 10B(d, α); E=0.4, 1.0, 1.5 MeV; measured αα(θ); deduced reaction mechanisms.
doi: 10.1103/PhysRevLett.27.820
1971LA20 Phys.Rev. C4, 2010 (1971) J.M.Lambert, R.J.Kane, P.A.Treado, L.A.Beach, E.L.Petersen, R.B.Theus Clustering Characteristics of 6Li from the 6Li(α, αx)Y Reaction at E = 50 MeV NUCLEAR REACTIONS 6Li(α, αX), E=50 MeV; measured σ(θ(α), θ(X), Eα, E(X-ray)). 6Li deduced clustering probabilities.
doi: 10.1103/PhysRevC.4.2010
1970LA14 Nucl.Phys. A152, 516 (1970) J.M.Lambert, P.A.Treado, L.A.Beach, R.B.Theus, E.L.Petersen Sequential Decay in the 7Li(α, t)8Be(α)4He and 7Li(α, α')7Li*(t)4He Reactions at E = 50 MeV NUCLEAR REACTIONS 7Li(α, tα), E=50 MeV; measured σ(Et, θ(t)), σ(Et, Eα, θ(t), θ(α)). 7Li deduced levels. 8Be deduced levels level-width. Natural target.
doi: 10.1016/0375-9474(70)90929-2
1961LA17 Phys.Rev. 124, 1959 (1961) J.M.Lambert, L.Madansky, G.E.Owen Deuteron Polarization in the Be9(p, d)Be8 Reaction NUCLEAR STRUCTURE 9Be; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.124.1959
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