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Search: Author = R.G.Allas

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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

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

1977WA05      Nucl.Phys. A281, 418 (1977)

C.N.Waddell, E.M.Diener, R.G.Allas, L.A.Beach, R.O.Bondelid, E.L.Petersen, A.G.Pieper, R.B.Theus, C.C.Chang, N.S.Chant

Study of the (p, pn) Reaction in Light Nuclei

NUCLEAR REACTIONS 2H, 6,7Li, 9Be(p, pn), E=45, 47 MeV; measured excitation energy, energy sharing spectra. 6Be deduced energy levels (15.5, 24 MeV), parentage. PWIA, DWIA calculations.

doi: 10.1016/0375-9474(77)90506-1
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

1973BO28      Phys.Rev. C8, 114 (1973); Erratum Phys.Rev. C8, 1551 (1973)

D.I.Bonbright, R.G.Allas, R.O.Bondelid, E.L.Petersen, A.G.Pieper, R.B.Theus, I.Slaus

2H(2H, dp)n Reaction

NUCLEAR REACTIONS 2H(d, dp), E=14-36 MeV; measured σ(E;Ep, Ed, θ(pd), θ), pd-coin.

doi: 10.1103/PhysRevC.8.114
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.

1972AL04      Phys.Rev.Lett. 28, 569 (1972)

R.G.Allas, D.I.Bonbright, R.O.Bondelid, E.L.Petersen, A.G.Pieper, R.B.Theus

Energy Dependence of Quasifree Scattering in Deuteron Breakup under α-Particle Bombardment from 30 to 80 MeV

NUCLEAR REACTIONS 2H(α, αn), (α, αp), E=30-80 MeV; measured σ(E;Eα, En), σ(E;Eα, Ep).

doi: 10.1103/PhysRevLett.28.569
Citations: PlumX Metrics

1971PE12      Phys.Rev.Lett. 27, 1454 (1971)

E.L.Petersen, R.G.Allas, R.O.Bondelid, D.I.Bonbright, A.G.Pieper, R.B.Theus

Impulse Approximation and Low-Energy Deuteron Breakup

NUCLEAR REACTIONS 2H(p, pn), 2H(p, 2p), E=22.8 MeV; measured σ(θ(p), θ(n)), σ(θ(p1), θ(p2)).

doi: 10.1103/PhysRevLett.27.1454
Citations: PlumX Metrics

1970PE02      Phys.Lett. 31B, 209 (1970)

E.L.Petersen, R.G.Allas, R.O.Bondelid, A.G.Pieper, R.B.Theus

Quasi-Free Scattering in the D(p, pn)p Reaction from 15 to 50 MeV

NUCLEAR REACTIONS 2H(p, pn), E=10-50 MeV; measured σ(E;Ep, En).

doi: 10.1016/0370-2693(70)90106-1
Citations: PlumX Metrics

1967SE02      Nucl.Phys. A93, 31(1967)

R.E.Segel, Z.Vager, L.Meyer-Schutzmeister, P.P.Singh, R.G.Allas

Radiative Capture by 19F: The Giant Dipole Resonances in 20Ne

NUCLEAR REACTIONS 19F(p, γ), E = 2.88-12.80 MeV; measured σ(E; Eγ, θ); deduced correlation functions. 20Ne compound-nucleus deduced J, π.

doi: 10.1016/0375-9474(67)90169-8
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0200.

1966ME09      Phys.Rev. 147, 743 (1966)

L.Meyer-Schutzmeister, D.Von Ehrenstein, R.G.Allas

Isospin Selection Rule in the C12(d, α)B10 Reaction

NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.147.743
Citations: PlumX Metrics

1966VO01      Nucl.Phys. 79, 625(1966)

D.Von Ehrenstein, L.Meyer-Schutzmeister, R.G.Allas

Study of the 39K(p, α)36Ar Reaction

NUCLEAR REACTIONS 39K(p, α), E = 10.0-13.0 MeV; measured σ(E, Eα, θ). 36Ar levels deduced, J, statistical properties. Enriched target.

doi: 10.1016/0029-5582(66)90268-9
Citations: PlumX Metrics

1965AL06      Nucl.Phys. 61, 289 (1965)

R.G.Allas, L.Meyer-Schutzmeister, D.Von Ehrenstein

Energy Levels of Ar36 and Ar38

NUCLEAR REACTIONS 39K(p, α), E=10.4 MeV; 41K(p, α), Ep=9.0, 10.5 MeV; measured σ(Eα). 36,38Ar deduced levels. Enriched targets.

doi: 10.1016/0029-5582(65)90902-8
Citations: PlumX Metrics

1965SE06      Phys.Rev. 139, B818 (1965)

R.E.Segel, S.S.Hanna, R.G.Allas

States in C12 Between 16.4 and 19.6 MeV

NUCLEAR STRUCTURE 12C, 11B; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.139.B818
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0332.

1965SI11      Nucl.Phys. 65, 577(1965)

P.P.Singh, R.E.Segel, L.Meyer-Schutzmeister, S.S.Hanna, R.G.Allas

Giant Resonances and Fine Structure in Si28 from the Al27(p, γ)Si28 Reaction

NUCLEAR REACTIONS 27Al(p, γ), E=4-12.5 MeV; measured σ(E; Eγ, θ). 28Si deduced mean level width. Natural target.

doi: 10.1016/0029-5582(65)90326-3
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1485.

1964AL03      Bull. Am. Phys. Soc. 9, No. 1, 79, HC12 (1964)

R.G.Allas, L.Meyer-Schutzmeister, D.von Ehrenstein

States in Ar36 with Excitation Energies below 7 MeV

NUCLEAR STRUCTURE 36Ar; measured not abstracted; deduced nuclear properties.

1964AL10      Bull. Am. Phys. Soc. 9, No. 5, 553, N6 (1964)

R.G.Allas, L.Meyer-Schutzmeister, D.von Ehrenstein

States in 38A with Excitation Energies below 6.3 MeV

NUCLEAR STRUCTURE 38Ar; measured not abstracted; deduced nuclear properties.

1964AL20      Nucl. Phys. 58, 122 (1964)

R.G.Allas, S.S.Hanna, L.Meyer-Schutzmeister, R.E.Segel

Radiative Capture of Protons by B11 and the Giant Dipole Resonance in C12

NUCLEAR REACTIONS 11B(p, γ), Ep=4-14 MeV; measured σ(E, θ), Eγ. Enriched target.

doi: 10.1016/0029-5582(64)90527-9
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0344.

1964SI03      Bull.Am.Phys.Soc. 9, No.1, 56, FA8 (1964)

P.P.Singh, R.E.Segel, R.G.Allas, S.S.Hanna, M.A.Grace

Missing Transitions in B10

NUCLEAR STRUCTURE 9B, 10B; measured not abstracted; deduced nuclear properties.

1963AL01      Bull.Am.Phys.Soc. 8, No.1, 11, BA6 (1963)

R.G.Allas, S.S.Hanna, L.L.Lee, Jr., L.Meyer-Schutzmeister, R.E.Segel

Reaction B11(p, γ)C12 in the Range 4 < Ep < 10 MeV

NUCLEAR STRUCTURE 11B; measured not abstracted; deduced nuclear properties.

1963AL02      Bull.Am.Phys.Soc. 8, No.1, 48, NA7 (1963)

R.G.Allas, D.von Ehrenstein, L.Meyer-Schutzmeister, J.A.Weinman

K39(p, α)Ar36 Reaction

NUCLEAR STRUCTURE 36Ar; measured not abstracted; deduced nuclear properties.

1963AL16      Bull.Am.Phys.Soc. 8, No.7, 538, S7 (1963)

R.G.Allas, J.R.Erskine, L.Meyer-Schutzmeister, D.von Ehrenstein

Population of the First T=1 State in B10 by the Reaction C12(d, α)B10

NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.

1963AL17      Bull.Am.Phys.Soc. 8, No.7, 538, S11 (1963)

R.G.Allas, S.S.Hanna, L.Meyer-Schutzmeister, R.E.Segel, P.P.Singh

Capture Reactions Al27(p, γ)Si28,28* in the Giant-Dipole Region of Si28*

NUCLEAR STRUCTURE 28Si; measured not abstracted; deduced nuclear properties.

1963AL27      ANL-6719, p.10 (1963)

R.G.Allas, S.S.Hanna, L.S.Meyer, R.E.Segel

Excited States of Light Nuclei

NUCLEAR STRUCTURE 11B; measured not abstracted; deduced nuclear properties.

1963SE14      Phys.Rev.Letters 10, 345 (1963)

B.E.Segel, P.P.Singh, R.G.Allas, S.S.Hanna

3.86-MeV Level in F17

NUCLEAR STRUCTURE 16O; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRevLett.10.345
Citations: PlumX Metrics

1962AL03      Phys.Rev. 125, 941 (1962)

R.G.Allas, F.B.Shull

Polarization of Protons in C12(d, p)C13

NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.125.941
Citations: PlumX Metrics

1962AL09      Bull.Am.Phys.Soc. 7, No. 6, 411, S1 (1962)

R.G.Allas, T.H.Braid, L.L.Lee, Jr., J.P.Schiffer

N14(d, α)C12 Reaction

NUCLEAR STRUCTURE 14N; measured not abstracted; deduced nuclear properties.

1962AL10      Phys.Rev. 127, 1252 (1962)

R.G.Allas, R.W.Bercaw, F.B.Shull

Polarization of Protons in Be9(d, p)Be10

NUCLEAR STRUCTURE 9Be; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.127.1252
Citations: PlumX Metrics

1962AL14      Bull.Am.Phys.Soc. 7, No.8, 550, T7 (1962)

R.G.Allas, S.S.Hanna, R.E.Segel

States in C12 between 17.5 and 19.5 MeV

NUCLEAR STRUCTURE 11B; measured not abstracted; deduced nuclear properties.

1962AL20      Bull.Am.Phys.Soc. 7, No.7, 453, GA3 (1962)

R.G.Allas, S.S.Hanna, R.E.Segel

State in C12 at 18.85 MeV

NUCLEAR STRUCTURE 11B; measured not abstracted; deduced nuclear properties.

1961AL02      Bull.Am.Phys.Soc. 6, No.1, 24, I3 (1961)

R.G.Allas, F.B.Shull

NUCLEAR STRUCTURE 10Be; measured not abstracted; deduced nuclear properties.

1959AL09      Phys.Rev. 116, 996 (1959)

R.G.Allas, F.B.Shull

Polarization of Protons in C12(d, p)C13

doi: 10.1103/PhysRev.116.996
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