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Search: Author = J.M.Lambert

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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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13988.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0892.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13536.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13682.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0010.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA1048.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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