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NSR database version of May 23, 2024.

Search: Author = S.A.Coon

Found 35 matches.

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2012CO20      Phys.Rev. C 86, 054002 (2012)

S.A.Coon, M.I.Avetian, M.K.G.Kruse, U.van Kolck, P.Maris, J.P.Vary

Convergence properties of ab initio calculations of light nuclei in a harmonic oscillator basis

NUCLEAR STRUCTURE 2,3H, 4,6He; calculated ground-state energy of light nuclei as function of momentum using shell model with the bare and soft NN interactions Idaho N3LO and JISP16.

doi: 10.1103/PhysRevC.86.054002
Citations: PlumX Metrics


2003FR20      Phys.Rev. C 68, 024003 (2003)

J.L.Friar, U.van Kolck, G.L.Payne, S.A.Coon

Charge-symmetry breaking and the two-pion-exchange two-nucleon interaction

NUCLEAR STRUCTURE 3H, 3He; calculated binding energy difference, charge-symmetry breaking effects. Effective field theory.

doi: 10.1103/PhysRevC.68.024003
Citations: PlumX Metrics


2002MA59      Phys.Rev. C66, 044007 (2002)

D.C.J.Marsden, P.Navratil, S.A.Coon, B.R.Barrett

Feasibility study of a three-nucleon force in the no-core shell model: 3H binding energy

NUCLEAR STRUCTURE 3H; calculated binding energy, excited states energies, dependence on cutoff parameter. Two-pion exchange three-body interaction.

doi: 10.1103/PhysRevC.66.044007
Citations: PlumX Metrics


2001BA64      Nucl.Phys. A689, 475c (2001)

M.Bawin, S.A.Coon

Darwin-Foldy Term and Proton Charge Radius

doi: 10.1016/S0375-9474(01)00885-5
Citations: PlumX Metrics


2001CO13      Few-Body Systems 30, 131 (2001)

S.A.Coon, H.K.Han

Reworking the Tucson-Melbourne Three-Nucleon Potential

NUCLEAR STRUCTURE 3H; calculated binding energy; deduced three-nucleon force effects, potential features.

doi: 10.1007/s006010170022
Citations: PlumX Metrics


2001CO15      Nucl.Phys. A689, 119c (2001)

S.A.Coon

The u-d Quark Mass Difference and Nuclear Charge Symmetry Breaking

doi: 10.1016/S0375-9474(01)00826-0
Citations: PlumX Metrics


2000GI10      Phys.Rev. C61, 064003 (2000)

W.R.Gibbs, S.A.Coon, H.K.Han, B.F.Gibson

Λ-Neutron Scattering Lengths from Radiative K- Capture

NUCLEAR REACTIONS 2H(K-, γX), E=not given; analyzed data; deduced hyperon-neutron triplet and singlet scattering lengths.

doi: 10.1103/PhysRevC.61.064003
Citations: PlumX Metrics


1999BA67      Phys.Rev. C60, 025207 (1999)

M.Bawin, S.A.Coon

Neutron Charge Radius and the Dirac Equation

doi: 10.1103/PhysRevC.60.025207
Citations: PlumX Metrics


1999CO26      Czech.J.Phys. 49, 1235 (1999)

S.A.Coon

Chiral Symmetry and Low Energy Pion-Nucleon Scattering

doi: 10.1023/A:1022868110424
Citations: PlumX Metrics


1998CO31      Phys.Rev. C58, 2958 (1998)

S.A.Coon, M.D.Scadron

Vector Meson Dominance and ρ-ω Mixing

doi: 10.1103/PhysRevC.58.2958
Citations: PlumX Metrics


1997BA02      Phys.Rev. C55, 419 (1997)

M.Bawin, S.A.Coon

Dirac-Foldy Term and the Electromagnetic Polarizability of the Neutron

NUCLEAR STRUCTURE 1n; calculated Dirac-Foldy term contribution to electric polarizability.

doi: 10.1103/PhysRevC.55.419
Citations: PlumX Metrics


1996CO02      Phys.Rev. C53, 1154 (1996)

S.A.Coon, J.A.Niskanen

Two-Pion Exchange Contributions to Nuclear Charge Asymmetry

NUCLEAR STRUCTURE 3H, 3He; calculated binding energy difference. Charge-symmetry-breaking two-pion exchange interaction.

doi: 10.1103/PhysRevC.53.1154
Citations: PlumX Metrics


1996CO19      Phys.Lett. 385B, 25 (1996)

S.A.Coon, B.H.J.McKellar, V.G.J.Stoks

ΔI = 1 Axial-Vector Mixing and Charge Symmetry Breaking

NUCLEAR STRUCTURE 3H, 3He; calculated binding energy difference. Different realistic potentials.

doi: 10.1016/0370-2693(96)00896-9
Citations: PlumX Metrics


1996FR02      Phys.Rev. C53, 588 (1996)

J.L.Friar, S.A.Coon

Leading-Order Nuclear π-γ Exchange Force

doi: 10.1103/PhysRevC.53.588
Citations: PlumX Metrics


1995CO11      Phys.Rev. C51, 2923 (1995)

S.A.Coon, M.D.Scadron

Universality of ΔI = 1 Meson Mixing and Charge Symmetry Breaking

NUCLEAR STRUCTURE 1H, 1n; calculated SU(2) mass splitting; deduced ΔI=1 meson mixing, charge symmetry breaking related features. Coleman-Glashow scheme.

doi: 10.1103/PhysRevC.51.2923
Citations: PlumX Metrics


1995CO27      Phys.Rev. C52, 2925 (1995)

S.A.Coon, M.T.Pena, D.O.Riska

Repulsive Short-Range Three-Nucleon Interaction

doi: 10.1103/PhysRevC.52.2925
Citations: PlumX Metrics


1994FR04      Phys.Rev. C49, 1272 (1994)

J.L.Friar, S.A.Coon

Non-Adiabatic Contributions to Static Two-Pion-Exchange Nuclear Potentials

doi: 10.1103/PhysRevC.49.1272
Citations: PlumX Metrics


1993CO14      Phys.Rev. C48, 2559 (1993)

S.A.Coon, M.T.Pena

Momentum and Coordinate Space Three-Nucleon Potentials

NUCLEAR STRUCTURE 3H; calculated three-body force contributions to binding energy. Potentials with ρ, π exchange, momentum, coordinate space.

doi: 10.1103/PhysRevC.48.2559
Citations: PlumX Metrics


1993SC30      Phys.Rev. C48, 2714 (1993); Erratum Phys.Rev. C52, 439 (1995)

N.W.Schellingerhout, L.P.Kok, S.A.Coon, R.M.Adam

Nucleon Polarization in Three-Body Models of Polarized 6Li

NUCLEAR STRUCTURE 6Li; calculated charge radius vs breakup binding energy, quadrupole moment, αd-cluster probability, μ vs neutron polarization. Three-body models, polarized 6Li.

NUCLEAR REACTIONS 6Li(e, e), E not given; calculated charge form factors. Three-body models, polarized 6Li.

doi: 10.1103/PhysRevC.48.2714
Citations: PlumX Metrics


1991CO12      Phys.Rev. C44, 203 (1991)

S.A.Coon, L.Jaqua

Wave Function Effects and the Elastic Magnetic Form Factor of 17O

NUCLEAR REACTIONS 17O(e, e), E not given; calculated magnetic form factor; deduced valence neutron radial wave function model dependence.

doi: 10.1103/PhysRevC.44.203
Citations: PlumX Metrics


1991PO07      J.Phys.(London) G17, 1375 (1991)

O.Portilho, S.A.Coon

9Be(Lambda) and 6He(Lambda Lambda) Hypernuclei Calculations

NUCLEAR STRUCTURE A=6, 9; calculated levels, reduced transition probabilities for hypernuclei. Variational approach.

doi: 10.1088/0954-3899/17/9/011
Citations: PlumX Metrics


1988FR24      Few-Body Systems 5, 13 (1988)

J.R.Friar, B.F.Gibson, G.L.Payne, S.A.Coon

S-Wave πN Scattering Effects in the Nuclear Three-Body Force

NUCLEAR STRUCTURE 3H; calculated binding energy; deduced off-mass shell, s-wave pion-nucleon scattering amplitude roles.

doi: 10.1007/BF01080469
Citations: PlumX Metrics


1987CO35      Phys.Rev. C36, 2189 (1987)

S.A.Coon, R.C.Barrett

ρ-Omega Mixing in Nuclear Charge Asymmetry

NUCLEAR REACTIONS 1H(p, p), 1n(n, n), E not given; calculated scattering length changes; deduced charge asymmetric nucleon-nucleon potential. Low energy NN-scattering parameters, vector meson mixing parameters.

NUCLEAR STRUCTURE 3He, 3H; calculated binding energy differences. Vector meson mixing amplitudes, charge asymmetric nucleon-nucleon potential.

doi: 10.1103/PhysRevC.36.2189
Citations: PlumX Metrics


1986CO01      Phys.Rev. C33, 605 (1986)

S.A.Coon, B.M.Preedom

π0(Eta) and π0(Eta') Mixing and the Reaction d + d → π0 + 4He

NUCLEAR REACTIONS 2H(d, π0), E=1.95 GeV; calculated σ(θ). Virtual eta, eta' production, pion-eta mixing.

doi: 10.1103/PhysRevC.33.605
Citations: PlumX Metrics


1986SA02      Phys.Rev. C33, 1062 (1986)

M.Sato, S.A.Coon, H.J.Pirner, J.P.Vary

Quark Cluster Probabilities in Nuclei

NUCLEAR STRUCTURE 2,3H, 3,4He; calculated quark cluster probabilities, color singlet cluster of 3, 6, 9, 12 quarks. 9Be, 12C, 16O, 20Ne, 24Mg, 27Al, 40Ca, 56Fe, 58Ni, 90Zr, 107Ag, 184W, 197Au, 208Pb, 238U deduced quark cluster probabilities. Realistic nuclear interactions.

doi: 10.1103/PhysRevC.33.1062
Citations: PlumX Metrics


1984CO18      Phys.Rev. C30, 1366 (1984)

S.A.Coon, M.T.Pena, R.G.Ellis

Three-Nucleon Forces and the Triton Binding Energy

NUCLEAR STRUCTURE 3H; calculated binding energy. Faddeev equations, s-wave potentials, three-nucleon forces.

doi: 10.1103/PhysRevC.30.1366
Citations: PlumX Metrics


1983PO03      Phys.Rev. C27, 2923 (1983)

O.Portilho, D.A.Agrello, S.A.Coon

Three-Body Potential among Alpha Particles

NUCLEAR STRUCTURE 12C; calculated levels, 0+ to 0+ reduced transition probabilities. Three α-particle potential model.

NUCLEAR REACTIONS 12C(e, e), (e, e'), E not given; calculated form factors. Three α-particle potential model.

doi: 10.1103/PhysRevC.27.2923
Citations: PlumX Metrics


1982CO03      Phys.Rev. C25, 756 (1982)

S.A.Coon, R.J.McCarthy, J.P.Vary

Three-Body Force Effects in the 17O Magnetic Form Factor

NUCLEAR REACTIONS 17O(e, e), E not given; calculated magnetic form factor; deduced three-body force, two-pion exchange effects.

doi: 10.1103/PhysRevC.25.756
Citations: PlumX Metrics


1979PO03      Z.Phys. A290, 93 (1979)

O.Portilho, S.A.Coon

Three-Alpha Force and the 3-α Model of 12C

NUCLEAR STRUCTURE 12C; calculated energies of low-lying states using 3-α force, 3α-model. Influence of Gaussian 3-body potential on elastic, inelastic form factors, coulmb energy, charge radius examined.

doi: 10.1007/BF01408484
Citations: PlumX Metrics


1978BR03      Nucl.Phys. A294, 305 (1978)

R.A.Brandenburg, S.A.Coon, P.U.Sauer

Nuclear Charge Asymmetry in the A = 3 Nuclei

NUCLEAR STRUCTURE 3H, 3He; calculated charge asymmetry, binding energy difference.

doi: 10.1016/0375-9474(78)90220-8
Citations: PlumX Metrics


1978CO08      J.Phys.(London) G4, 183 (1978)

S.A.Coon, R.J.McCarthy, C.P.Malta

A Three-Nucleon Force and A = 18 Shell-Model Spectra

NUCLEAR STRUCTURE 18O, 18F; calculated levels.

doi: 10.1088/0305-4616/4/2/009
Citations: PlumX Metrics


1974CO30      Nucl.Phys. A231, 95 (1974)

S.A.Coon, H.S.Kohler

Density-Dependent Effective Interactions in Nuclei

NUCLEAR STRUCTURE 16O, 40,48Ca, 90Zr, 208Pb; calculated binding energies, levels.

doi: 10.1016/0375-9474(74)90295-4
Citations: PlumX Metrics


1963NO02      Phys.Rev. 130, 1971 (1963)

E.Norbeck, S.A.Coon, R.R.Carlson, E.Berkowitz

Gamma Rays Rays from Lithium Bombardment of Be9, B10, B11, and C12

NUCLEAR STRUCTURE 12C, 9Be, 11B, 10B; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.130.1971
Citations: PlumX Metrics


1962BE24      Phys.Rev. 128, 247 (1962)

E.Berkowitz, S.Bashkin, R.R.Carlson, S.A.Coon, E.Norbeck

Gamma Radiation from Lithium-Lithium Nuclear Reactions

NUCLEAR STRUCTURE 7Li, 6Li; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.128.247
Citations: PlumX Metrics


1961BE27      SUI-61-21 (1961)

E.H.Berkowitz, V.P.Hart, R.L.McGrath, S.A.Coon, S.Bashkin, J.Landstreet, E.Norbeck

Gamma rays from the bombardment of B10 B11and C12 by Li6 and Li7

NUCLEAR STRUCTURE 10B, 11B, 12C; measured not abstracted; deduced nuclear properties.


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