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Search: Author = R.J.Philpott

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1993PE13      Nucl.Phys. A563, 387 (1993)

F.Petrovich, S.K.Yoon, M.J.Threapleton, R.J.Philpott, J.A.Carr, F.S.Dietrich, L.F.Hansen

Consistent Folding Model Description of Nucleon Elastic, Inelastic, and Charge-Exchange Scattering from 6,7Li at 25-50 MeV

NUCLEAR REACTIONS 6Li(p, p), E=24.4-49.75 MeV; analyzed σ(θ). 7Li(polarized p, p), (polarized p, p'), E=24.4, 49.75, 200 MeV; analyzed σ(θ), analyzing power vs θ. Folding model.

doi: 10.1016/0375-9474(93)90120-M
Citations: PlumX Metrics

1992CA05      Phys.Rev. C45, 1145 (1992)

J.A.Carr, S.D.Bloom, F.Petrovich, R.J.Philpott

Fragmentation of Stretched Spin Strength in N = Z sd-Shell Nuclei

NUCLEAR STRUCTURE 20Ne, 24Mg, 28Si, 32S, 36Ar; calculated levels transition strengths, stretched states spin strength fragmentation. Effective interactions.

doi: 10.1103/PhysRevC.45.1145
Citations: PlumX Metrics

1991GL01      Phys.Rev. C43, 1664 (1991)

C.W.Glover, C.C.Foster, P.Schwandt, J.R.Comfort, J.Rapaport, T.N.Taddeucci, D.Wang, G.J.Wagner, J.Seubert, A.W.Carpenter, J.A.Carr, F.Petrovich, R.J.Philpott, M.J.Threapleton

Scattering of Polarized Protons from 7Li at 200 MeV

NUCLEAR REACTIONS 7Li(polarized p, p), (polarized p, p'), E=200 MeV; measured σ(θ), analyzing power vs θ. 6,7Li deduced radial density shape differences. Single scattering model.

doi: 10.1103/PhysRevC.43.1664
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0581.

1990GL04      Phys.Rev. C41, 2487 (1990)

C.W.Glover, C.C.Foster, P.Schwandt, J.R.Comfort, J.Rapaport, T.N.Taddeucci, D.Wang, G.J.Wagner, J.Seubert, A.W.Carpenter, J.A.Carr, F.Petrovich, R.J.Philpott, M.J.Threapleton

Scattering of Polarized Protons from 6Li at 200 MeV

NUCLEAR REACTIONS 6Li(polarized p, p), (polarized p, p'), E=200 MeV; measured σ(θ), analyzing power vs (θ). Microscopic single scattering model with free, Pauli corrected effective nucleon-nucleon interactions.

doi: 10.1103/PhysRevC.41.2487
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0582.

1989CA07      Phys.Rev.Lett. 62, 2249 (1989); Erratum Phys.Rev.Lett. 63, 918 (1989)

J.A.Carr, S.D.Bloom, F.Petrovich, R.J.Philpott

Fragmentation of Stretched Spin Strength in 28Si

NUCLEAR STRUCTURE 28Si; calculated stretched states fragmentation, spectroscopic factors, M6 transition strength function. Large basis.

doi: 10.1103/PhysRevLett.62.2249
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1988CO16      Phys.Rev. C38, 1619 (1988)

P.D.Cottle, V.Hnizdo, R.J.Philpott, K.A.Stuckey, K.W.Kemper, J.A.Carr

Negative Parity States of Even-A Pt Isotopes from Proton Inelastic Scattering

NUCLEAR REACTIONS 194,196,198Pt(p, p'), E=35 MeV; analyzed σ(θ); deduced 3- state systematics in Os, Pt, Hg region. 194,196,198Pt level deduced β3, B(E3).

doi: 10.1103/PhysRevC.38.1619
Citations: PlumX Metrics

1988HA07      Phys.Rev. C37, 1104 (1988)

D.Halderson, R.J.Philpott

Realistic Calculations for Strangeness Exchange at Rest

NUCLEAR REACTIONS 12C(K-, π-), E at rest; calculated K-capture rates.

doi: 10.1103/PhysRevC.37.1104
Citations: PlumX Metrics

1988PE09      Phys.Lett. 207B, 1 (1988)

F.Petrovich, J.A.Carr, R.J.Philpott, A.W.Carpenter

Spectroscopic Considerations and the Exchange Non-Locality in Nucleon-Nucleus Scattering

NUCLEAR REACTIONS 90Zr(p, p'), E=50 MeV; 16O(p, p'), E=135 MeV; calculated σ(θ). Exact plane wave approximation.

doi: 10.1016/0370-2693(88)90874-X
Citations: PlumX Metrics

1986HA39      Nucl.Phys. A458, 605 (1986)

D.Halderson, P.Ning, R.J.Philpott

Strangeness Exchange Reactions with the Recoil Corrected Continuum Shell Model

NUCLEAR REACTIONS 12C, 40Ca(K-, K-), (π-, π-), E at 800 MeV/c; 12C(K-, π-), E not given; calculated σ(θ). 16O(K-, π-), E at 790 MeV/c; 40Ca(K-, π-), E not given; calculated σ(θ(π), E(π)). Recoil corrected continuum shell model.

doi: 10.1016/0375-9474(86)90189-2
Citations: PlumX Metrics

1985CA03      Phys.Rev.Lett. 54, 881 (1985): Erratum Phys.Rev.Lett. 54, 1736 (1985)

J.A.Carr, F.Petrovich, R.J.Philpott, M.J.Threapleton, O.Scholten, H.McManus

Inelastic Proton Scattering as a Test of the New Collective - ' Current ' M1 Mode in Deformed Nuclei

NUCLEAR REACTIONS 156Gd(p, p'), E=200 MeV; 156Gd(e, e'), E=40 MeV; calculated σ(θ), transition densities, t-interaction components, transverse magnetic form factors vs θ, momentum transfer. 156Gd deduced M1 transitions character. Born approximation.

doi: 10.1103/PhysRevLett.54.881
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1985PE14      Phys.Lett. 165B, 19 (1985)

F.Petrovich, J.A.Carr, R.J.Philpott, A.W.Carpenter, J.Kelly

Spin-Current Effects in Inelastic Scattering from Nuclei

NUCLEAR REACTIONS 16O(π+, π+), E=164 MeV; 16O(p, p), (p, p'), E=135 MeV: calculated σ(θ). 16O(e, e'), E not given; calculated form factors; deduced spin-orbit interaction role in nonnormal parity transfer.

doi: 10.1016/0370-2693(85)90682-3
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1985PH01      Nucl.Phys. A439, 397 (1985)


Intrinsic-State Coefficients of Fractional Parentage in the Oscillator Shell Model

NUCLEAR STRUCTURE A=15; calculated intrinsic state fractional parentage coefficients. Oscillator shell model, no center-of-mass coordinate.

doi: 10.1016/0375-9474(85)90418-X
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1984PE12      Nucl.Phys. A425, 609 (1984)

F.Petrovich, R.J.Philpott, A.W.Carpenter, J.A.Carr

Spin Dependence in the Nucleus-Nucleus Optical Potential

NUCLEAR REACTIONS 58Ni(polarized 7Li, 7Li), E=20.3 MeV; calculated σ(θ), vector, tensor analyzing power vs θ. Coupled-channels formalism, realistic nucleon-nucleon interaction.

doi: 10.1016/0375-9474(84)90026-5
Citations: PlumX Metrics

1983HA21      Phys.Rev. C28, 1000 (1983)

D.Halderson, R.J.Philpott

Charge Symmetry Breaking in 4He

NUCLEAR REACTIONS 4He(γ, p), (γ, n), E=20-36 MeV; calculated σ(ratio) vs E. 3H(p, n), (polarized p, n), E=1.5-4.5 MeV; calculated P(E), A(E). 3H(p, γ), E ≈ 2-16 MeV; calculated angular distribution, asymmetry coefficients a(k), (B(k)) vs E. 3He(n, γ), E=9 MeV; calculated σ(θ); deduced charge symmetry breaking interaction role inadequacy in interpreting data. Recoil-corrected continuum shell model.

doi: 10.1103/PhysRevC.28.1000
Citations: PlumX Metrics

1982CO14      Nucl.Phys. A385, 157 (1982)

J.Cook, R.J.Philpott

Elastic Scattering of Spin-(3/2) Particles

NUCLEAR REACTIONS 58Ni(polarized 7Li, 7Li), E=20.3 MeV; analyzed polarization observables data. Hooton-Johnson scattering amplitudes.

doi: 10.1016/0375-9474(82)90494-8
Citations: PlumX Metrics

1982PH01      Nucl.Phys. A375, 169 (1982)

R.J.Philpott, D.Halderson

Single-Particle Model of Capture to Continuum States

NUCLEAR REACTIONS 12C(p, p), E=26.2, 40, 61.4, 95 MeV; 11B(p, p), E=30.3 MeV; calculated σ(θ). 11B, 12C(p, γ), E=40 MeV; calculated σ(θ, Eγ). 11B(p, γ), (polarized p, γ), E=8-55 MeV; calculated σ(θ, Eγ), asymmetry vs E. Single particle model, continuum capture.

doi: 10.1016/0375-9474(82)90408-0
Citations: PlumX Metrics

1981HA01      Phys.Rev.Lett. 46, 100 (1981)

D.Halderson, R.J.Philpott

Radiative Capture to Unbound States via a Bremsstrahlung Mechanism

NUCLEAR REACTIONS 12C(p, γ), E=40 MeV; 11B(p, γ), E=40, 80 MeV; calculated σ(θγ, Eγ). 13N, 12C deduced resonances. Bremsstrahlung mechanism, capture to unbound states.

doi: 10.1103/PhysRevLett.46.100
Citations: PlumX Metrics

1981HA10      Nucl.Phys. A359, 365 (1981)

D.Halderson, R.J.Philpott

Radiative Capture to 4He

NUCLEAR REACTIONS 4He(γ, n), (γ, p), E not given; analyzed σ(θ); 3H(polarized p, γ), E=2-26 MeV; 3He(polarized n, γ), E=1-28 MeV; analyzed analyzing power vs θ. Continuum shell model, target recoil correction, noncentral forces.

doi: 10.1016/0375-9474(81)90242-6
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1981HA29      Phys.Rev. C24, 1095 (1981)

D.Halderson, R.J.Philpott, J.A.Carr, F.Petrovich

Pion Inelastic Scattering to Particle Unbound Stretched States of 12C

NUCLEAR REACTIONS 12C(π+, π+'), (π-, π-'), E=162 MeV; calculated σ(E(π), θ(π)). 12C levels deduced isospin mixing, Γ, Γn, Γp. Recoil corrected continuum shell model.

doi: 10.1103/PhysRevC.24.1095
Citations: PlumX Metrics

1980HA35      Nucl.Phys. A345, 141 (1980)

D.Halderson, R.J.Philpott

Study of Nucleon Channel Reactions for A=12 and A=16 Systems with the Recoil Corrected Continuum Shell Model

NUCLEAR REACTIONS 11B(p, p), E=0.3-1 MeV; 11B(n, n), E=0.1-5 MeV; 11B(p, n), E=threshold-10 MeV; 15N(p, p), E=3-12 MeV; 15N(p, n), E=threshold-9 MeV; 15N(n, n), E=0.5-6 MeV; 15N(p, p'), E=8.5-11.5 MeV; calculated σ(θ, E). Continuum shell model, target recoil corrections, realistic interactions.

NUCLEAR STRUCTURE 12C, 12B, 16N, 16O; calculated levels. Continuum shell model, target recoil effects, realistic interactions.

doi: 10.1016/0375-9474(80)90415-7
Citations: PlumX Metrics

1979HA22      Nucl.Phys. A321, 295 (1979)

D.Halderson, R.J.Philpott

Recoil Corrected Continuum Shell Model Calculations for Four-Nucleon Systems

NUCLEAR REACTIONS 3H(p, p), (polarized p, p), E=4.15 MeV; 3He(n, n), (polarized n, n), E=8 MeV; calculated σ(θ), A(θ). Recoil-corrected continuum shell model in 1p-1h space.

doi: 10.1016/0375-9474(79)90127-1
Citations: PlumX Metrics

1979PH06      Phys.Rev.Lett. 43, 1785 (1979)

R.J.Philpott, D.Halderson

Prediction of Observable Polarization-Analyzing-Power Differences in 11B(p, n)11C

NUCLEAR REACTIONS 11B(p, n), E < 10 MeV; calculated polarization-analyzing power differences. Recoil corrected continuum 1p-1h shell model, realistic interactions.

doi: 10.1103/PhysRevLett.43.1785
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1978PH01      Nucl.Phys. A294, 6 (1978)

R.J.Philpott, D.Mukhopadhyay, J.E.Purcell

Application of the v-w Formalism to the Continuum Shell Model

NUCLEAR REACTIONS 16O, 40Ca(p, p), E=40-50 MeV; calculated σ.

doi: 10.1016/0375-9474(78)90391-3
Citations: PlumX Metrics

1977BE02      Nucl.Phys. A275, 301 (1977)

J.J.Bevelacqua, R.J.Philpott

Microscopic Calculations for the 4He Continuum (I). General Approach

NUCLEAR REACTIONS 2H(d, d), (d, p); calculated σ. 4He; calculated levels.

doi: 10.1016/0375-9474(77)90454-7
Citations: PlumX Metrics

1977PH01      Nucl.Phys. A289, 109 (1977)


Continuum Shell Model with Full Correction for Target Recoil

NUCLEAR REACTIONS 4He(p, p), E(cm)=14, 60 MeV; 40Ca(n, n), E(cm)=49 MeV; 16O(n, n), E(cm)=60 MeV; calculated σ(θ), phase shifts.

doi: 10.1016/0375-9474(77)90524-3
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1976PE07      Phys.Rev.Lett. 37, 558 (1976)

F.Petrovich, R.J.Philpott, D.Robson, J.J.Bevelacqua, M.Golin, D.Stanley

Comments of Primordial Superheavy Elements

NUCLEAR STRUCTURE A > 200; calculated single particle levels, Qα, T1/2.

doi: 10.1103/PhysRevLett.37.558
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1975GE08      Phys.Rev. C12, 658 (1975)

J.George, R.J.Philpott

Microscopic Model Study of Nucleon Elastic Scattering from 16O

NUCLEAR REACTIONS 16O(n, n), E < 4 MeV; calculated total σ(E), polarization. 16O(p, p), E < 6 MeV; calculated σ(E), polarization. 17F, 17O deduced resonances, Γ.

doi: 10.1103/PhysRevC.12.658
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1975PH01      Nucl.Phys. A243, 260 (1975)


Reduction of the Lane-Robson 'Calculable' Reaction Theory to Standard R-Matrix Form

NUCLEAR REACTIONS 16O(n, n); calculated potential.

doi: 10.1016/0375-9474(75)90247-X
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1975PH02      Phys.Rev. C12, 1540 (1975)


R-Matrix Description of Scattering from Optical Model Potentials

NUCLEAR REACTIONS 16O(16O, 16O), E(cm)=10-35 MeV; calculated R-matrix parameters for optical potential models; deduced Γ, σ(E).

doi: 10.1103/PhysRevC.12.1540
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1974GE03      Phys.Rev.Lett. 32, 901 (1974)

J.George, R.J.Philpott

Continuum-Shell-Model Description of Compound Resonances in the System 16O + n

NUCLEAR REACTIONS 16O(n, n); measured nothing, calculated σ(E) with up to 4p-4h states included.

doi: 10.1103/PhysRevLett.32.901
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1974GR21      Phys.Rev. C10, 564 (1974)

M.B.Greenfield, M.F.Werby, R.J.Philpott

6Li(α, d)8Be Reaction and the Importance of Exchange Processes

NUCLEAR REACTIONS 6Li(α, d), E=20, 24 MeV; measured σ(Ed, θ), deduced exchange contributions.

doi: 10.1103/PhysRevC.10.564
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1974PH03      Nucl.Phys. A233, 164 (1974)

R.J.Philpott, J.George

On the Practical Application of the Generalized R-Matrix Method to Problems in Nuclear Physics

NUCLEAR REACTIONS 12,14C, 16O(n, n); calculated σ; formulated convergence criteria.

doi: 10.1016/0375-9474(74)90249-8
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1973CO17      Phys.Rev.Lett. 31, 559 (1973)

S.Cotanch, R.J.Philpott

Does Pickup to Analog States Exhibit a Charge Dependence of the Nuclear Force (Question)

NUCLEAR REACTIONS 19F(d, t), (d, 3He); calculated σ(θ); deduced no charge dependence.

doi: 10.1103/PhysRevLett.31.559
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1973PH03      Nucl.Phys. A208, 236 (1973)


Continuum Shell Model Calculations for 15C

NUCLEAR REACTIONS 14C(d, p); calculated stripping form factors. 15C calculated levels, J, π, S.

doi: 10.1016/0375-9474(73)90372-2
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1972PH01      Nucl.Phys. A179, 113 (1972)


The Influence of Shell Structure on Isobaric Spin Splitting

NUCLEAR STRUCTURE 208Bi, 138La; calculated isobaric spin splitting of spectroscopic strength. Shell model.

doi: 10.1016/0375-9474(72)90109-1
Citations: PlumX Metrics

1972PH06      Phys.Rev. C5, 1457 (1972)


Nucleon-Transfer Form Factors Relative to a Microscopically Specified Core

NUCLEAR REACTIONS 16O(d, p), E=14.3 MeV; calculated σ(θ).

doi: 10.1103/PhysRevC.5.1457
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1970PH02      Phys.Rev. C2, 512 (1970)

R.J.Philpott, W.W.True

Core-Plus-Particle Model and the Low-Lying Levels of Cr53

NUCLEAR STRUCTURE 53Cr; calculated levels, B(E2), S for 52Cr(d, p). Core+particle model.

doi: 10.1103/PhysRevC.2.512
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1970PH03      Phys.Rev. C2, 1232 (1970)


Extended Shell-Model Description of Nucleon-Transfer Form Factors

NUCLEAR REACTIONS 40Ca(d, p), 40Ca(3He, d), E not given; calculated form factors.

doi: 10.1103/PhysRevC.2.1232
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1969SA17      Phys.Rev. 182, 1141 (1969)

G.R.Satchler, D.D.Armstrong, A.G.Blair, E.R.Flynn, R.J.Philpott, W.T.Pinkston

Excitation of the 3/2+, 2.02-MeV State in 41Ca by the (t, d) Reaction

NUCLEAR REACTIONS 40Ca(t, d), E=20 MeV; measured σ(θ); deduced optical model parameters. 41Ca levels deduced S.

doi: 10.1103/PhysRev.182.1141
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1967PH02      Phys.Rev. 153, 1039 (1967)

R.J.Philpott, P.P.Szydlik

Higher Random-Phase-Approximation Studies of the Structure of O16.I

doi: 10.1103/PhysRev.153.1039
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