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NSR database version of May 3, 2024.

Search: Author = C.M.Vincent

Found 17 matches.

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1978AU09      Phys.Rev. C18, 1577 (1978)

N.Austern, J.P.Farrell, Jr., K.Kabir, C.M.Vincent

Effects of Imaginary Potentials in a Three-Body Deuteron-Nucleus Scattering Model

NUCLEAR REACTIONS 40Ca(d, p), E=25.5 MeV; calculated σ(θ).

doi: 10.1103/PhysRevC.18.1577
Citations: PlumX Metrics


1978DA03      Phys.Rev. C17, 1461 (1978)

F.Darema-Rogers, C.M.Vincent

Energies and Bounds from Perturbative Approximations to the Bloch-Horowitz Effective Hamiltonian

NUCLEAR STRUCTURE 18O; calculated structure. Bloch-Horowitz perturbation theory.

doi: 10.1103/PhysRevC.17.1461
Citations: PlumX Metrics


1978EP02      Phys.Rev. C17, 1501 (1978)

G.N.Epstein, F.Tabakin, C.M.Vincent, A.Gal, L.S.Kisslinger

Distorted-Wave Impulse-Approximation Evaluation of Sum Rule for Hypernuclear Formation in Forward (K-, π-)

NUCLEAR REACTIONS 12C, 40Ca(K-, π-), E=900 MeV/c; calculated σ.

doi: 10.1103/PhysRevC.17.1501
Citations: PlumX Metrics


1976CO01      Phys.Rev.Lett. 36, 21 (1976)

S.R.Cotanch, C.M.Vincent

Simple Approximation for Multistep Amplitudes

NUCLEAR REACTIONS 16O(d, d), E=10.49 MeV; 17O(p, p), E=10.98 MeV; calculated σ(θ).

doi: 10.1103/PhysRevLett.36.21
Citations: PlumX Metrics


1976CO29      Phys.Rev. C14, 1739 (1976)

S.R.Cotanch, C.M.Vincent

Channel Coupling and Nonorthogonality in Elastic and Transfer Processes

NUCLEAR REACTIONS 16O(d, d), (d, p), E=10.49, 14.8, 20 MeV; 17O(p, p), E=10.98 MeV; 90Zr(d, d), (d, p), E=12 MeV; 28Si(16O, 16O), (16O, 12C), E=42, 48 MeV; 32S(12C, 12C), E=41.71 MeV; calculated σ(θ). Folded-potential DWBA plus multistep contribution of rearranged intermediate channels, corrected for nonorthogonality. Surface approximation with separable Green function.

doi: 10.1103/PhysRevC.14.1739
Citations: PlumX Metrics


1976FA07      Ann.Phys.(New York) 96, 333 (1976)

J.P.Farrell, Jr., C.M.Vincent, N.Austern

Three-Body Model of Deuteron Breakup and Stripping

NUCLEAR REACTIONS 40Ca(d, p); E(lab)=25.5 MeV; calculated σ.

doi: 10.1016/0003-4916(76)90195-0
Citations: PlumX Metrics


1976PI01      Phys.Rev. C13, 412 (1976)

S.Pittel, C.M.Vincent, J.D.Vergados

Perturbative Approximations to the Effective Interaction: Comparisons with Exact Results for Large Matrices

NUCLEAR STRUCTURE 18O; calculated perturbative approximations to the effective interaction. Pade approximants.

doi: 10.1103/PhysRevC.13.412
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1974FO17      Phys.Rev. C10, 1233 (1974)

H.T.Fortune, C.M.Vincent

Neutron Strength of the 5.08-MeV 3/2+ State of 17O

NUCLEAR REACTIONS 16O(d, p), E=12 MeV; 16O(n, n)E=940 keV; calculated σ(Ep, θ), σ. 17O resonance deduced n-width.

doi: 10.1103/PhysRevC.10.1233
Citations: PlumX Metrics


1973VI01      Phys.Rev. C7, 865 (1973)

C.M.Vincent, H.T.Fortune

Stripping to an Unbound State with Multiple Decay Channels

doi: 10.1103/PhysRevC.7.856
Citations: PlumX Metrics


1973VI08      Phys.Rev. C8, 1084 (1973)

C.M.Vincent, H.T.Fortune

Effect of Fine Structure on Nucleon Transfer to Analog States

NUCLEAR REACTIONS 92Mo(d, n); measured nothing. Deduced background, asymmetry phaser.

doi: 10.1103/PhysRevC.8.1084
Citations: PlumX Metrics


1973VI11      Phys.Lett. 47B, 327 (1973)

C.M.Vincent, S.Pittel

Perturbative Approximations to the Effective Hamiltonian in the Presence of an Intruder State

NUCLEAR STRUCTURE 18O; calculated matrix elements.

doi: 10.1016/0370-2693(73)90614-X
Citations: PlumX Metrics


1971FO18      Phys.Rev. C4, 1994 (1971)

H.T.Fortune, C.M.Vincent

Spectroscopic Factors for T = 3/2 States in A = 19 Nuclei

NUCLEAR REACTIONS 18O(d, p), E=12 MeV; 18O(3He, d), E=16 MeV; analyzed σ(θ). 19F, 19O levels deduced S.

doi: 10.1103/PhysRevC.4.1994
Citations: PlumX Metrics


1971FO20      Phys.Rev.Lett. 27, 1664 (1971)

H.T.Fortune, C.M.Vincent

Accurate Description of the Reaction 92Mo(d, n)93Tc to Unbound Analog States

NUCLEAR REACTIONS 92Mo(d, n), E=12 MeV; calculated σ(θ) for unbound analog states. DWBA.

doi: 10.1103/PhysRevLett.27.1664
Citations: PlumX Metrics


1971MO14      Phys.Rev. C3, 2192 (1971)

J.E.Monahan, H.T.Fortune, C.M.Vincent, R.E.Segel

T = 1 States in the A = 12 System

NUCLEAR REACTIONS 11B(d, p), (p, X), E not given; measured nothing; analyzed σ(E). 12B levels deduced n-widths. 12C deduced resonances, level-width, isobaric analogs.

doi: 10.1103/PhysRevC.3.2192
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1970RI16      Phys.Rev.Lett. 25, 1460 (1970)

A.Richter, C.M.Vincent

Distorted-Wave Analysis of Charge Asymmetry Effects in the Reaction d(α, t)3He

NUCLEAR REACTIONS 2H(α, t), E=82 MeV; measured nothing; analyzed σ(θ), asymmetry(θ). DWBA.

doi: 10.1103/PhysRevLett.25.1460
Citations: PlumX Metrics


1970VI03      Phys.Rev. C2, 782 (1970)

C.M.Vincent, H.T.Fortune

New Method for Distorted-Wave Analysis of Stripping to Unbound States

NUCLEAR REACTIONS 16O(d, p), E=12 MeV; calculated σ(θ).

doi: 10.1103/PhysRevC.2.782
Citations: PlumX Metrics


1969FO10      Phys.Rev. 185, 1401 (1969)

H.T.Fortune, C.M.Vincent

Distorted-Wave Analysis of the 11B(d, p) Reaction Leading to the Lowest Unbound Level in 12B

NUCLEAR REACTIONS 11B(d, p), E = 12 MeV; measured σ(θ). 12B level deduced J, π. DWBA analysis.

doi: 10.1103/PhysRev.185.1401
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