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NSR database version of April 27, 2024.

Search: Author = C.M.Shakin

Found 81 matches.

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2005LI25      Phys.Rev. C 71, 068203 (2005)

H.Li, C.M.Shakin, X.Li

Relativistic calculation of the width of the Θ+(1540) pentaquark

doi: 10.1103/PhysRevC.71.068203
Citations: PlumX Metrics


2004LI43      Phys.Rev. C 69, 065201 (2004)

X.Li, H.Li, C.M.Shakin, Q.Sun

Quark propagation in the quark-gluon plasma

doi: 10.1103/PhysRevC.69.065201
Citations: PlumX Metrics


2004LI65      Phys.Rev. C 70, 048201 (2004)

X.Li, H.Li, C.M.Shakin, Q.Sun

Calculation of screening masses in a chiral quark model

doi: 10.1103/PhysRevC.70.048201
Citations: PlumX Metrics


2004LI77      Phys.Rev. C 70, 068201 (2004)

X.Li, C.M.Shakin

Comparison of models of critical opacity in the quark-gluon plasma

doi: 10.1103/PhysRevC.70.068201
Citations: PlumX Metrics


2003HE04      Phys.Rev. D 67, 014022 (2003)

B.He, H.Li, C.M.Shakin, Q.Sun

Calculation of the pseudoscalar-isoscalar hadronic current correlation functions of the quark-gluon plasma

doi: 10.1103/PhysRevD.67.014022
Citations: PlumX Metrics


2003HE09      Phys.Rev. C 67, 065203 (2003)

B.He, H.Li, C.M.Shakin, Q.Sun

Comparison of temperature-dependent hadronic current correlation functions calculated in lattice simulations of QCD and with a chiral Lagrangian model

doi: 10.1103/PhysRevC.67.065203
Citations: PlumX Metrics


2002CE07      Phys.Rev. D66, 054010 (2002)

L.S.Celenza, H.Li, C.M.Shakin, Q.Sun

Quark and nucleon self-energy in dense matter

doi: 10.1103/PhysRevD.66.054010
Citations: PlumX Metrics


2002LI26      Phys.Rev. C65, 045205 (2002)

H.Li, Q.Sun, C.M.Shakin

Calculation of 1/Nc Corrections to the SU(3)-Flavor Nambu-Jona-Lasino Model

doi: 10.1103/PhysRevC.65.045205
Citations: PlumX Metrics


2001CE01      Phys.Rev. C63, 025209 (2001)

L.S.Celenza, H.Wang, C.M.Shakin

Application of a Generalized Nambu-Jona-Lasinio Model to the Calculation of the Properties of Scalar Mesons and Nuclear Matter

doi: 10.1103/PhysRevC.63.025209
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2000CE01      Phys.Rev. C61, 035201 (2000)

L.S.Celenza, S.-F.Gao, B.Huang, H.Wang, C.M.Shakin

Covariant Confinement Model for the Calculation of the Properties of Scalar Mesons

doi: 10.1103/PhysRevC.61.035201
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2000CE03      Phys.Rev. C62, 068201 (2000)

L.S.Celenza, B.Huang, H.Wang, C.M.Shakin

Calculation of the Distribution of Scalar Glueball Strength

doi: 10.1103/PhysRevC.62.068201
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1999CE01      Phys.Rev. C59, 1030 (1999)

L.S.Celenza, B.Huang, C.M.Shakin

T Matrices and Current Correlation Functions for a Relativistic Quark Model with Confinement

doi: 10.1103/PhysRevC.59.1030
Citations: PlumX Metrics


1999CE02      Phys.Rev. C59, 1041 (1999)

L.S.Celenza, B.Huang, C.M.Shakin

Covariant Confinement Model for the Calculation of Radial Excitations of the Pion

doi: 10.1103/PhysRevC.59.1041
Citations: PlumX Metrics


1999CE04      Phys.Rev. C59, 1700 (1999)

L.S.Celenza, B.Huang, C.M.Shakin

Role of a Covariant Confinement Model in the Calculation of the Two-Photon Decay of the η and η'

doi: 10.1103/PhysRevC.59.1700
Citations: PlumX Metrics


1999CE05      Phys.Rev. C59, 2814 (1999)

L.S.Celenza, B.Huang, C.M.Shakin

Importance of Pseudoscalar-Axial-Vector Mixing in Calculation of the Properties of the π, η, and η' Mesons

doi: 10.1103/PhysRevC.59.2814
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1999CE07      Phys.Rev. C60, 025202 (1999); Erratum Phys.Rev. C60, 039901 (1999)

L.S.Celenza, B.Huang, H.Wang, C.M.Shakin

Covariant Confinement Model for the Study of the Properties of Light Mesons

doi: 10.1103/PhysRevC.60.025202
Citations: PlumX Metrics


1999CE08      Phys.Rev. C60, 035206 (1999)

L.S.Celenza, B.Huang, H.Wang, C.M.Shakin

Convariant Calculation of the Properties of f2 Mesons in a Generalized Nambu-Jona-Lasinio Model

doi: 10.1103/PhysRevC.60.035206
Citations: PlumX Metrics


1999CE10      Phys.Rev. C60, 065209 (1999)

L.S.Celenza, B.Huang, H.Wang, C.M.Shakin

Pseudoscalar-Axial-Vector Mixing for the Kaon and Its Radial Excitations

doi: 10.1103/PhysRevC.60.065209
Citations: PlumX Metrics


1999CE11      Phys.Rev. C60, 065210 (1999)

L.S.Celenza, B.Huang, H.Wang, C.M.Shakin

Regularization of Covariant Calculations of Meson Decay Amplitudes at One-Loop Order: Properties of the a0(980) Resonance

doi: 10.1103/PhysRevC.60.065210
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1998CE09      Phys.Rev. C58, 1845 (1998)

L.S.Celenza, B.Huang, C.M.Shakin

π a1 Mixing at Intermediate Energies

doi: 10.1103/PhysRevC.58.1845
Citations: PlumX Metrics


1998HU21      Phys.Rev. C58, 3648 (1998)

B.Huang, X.-D.Li, C.M.Shakin

Radial Excitations in the Analysis of φ-ω and η-η' Mixing

doi: 10.1103/PhysRevC.58.3648
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1997CE02      Phys.Rev. C55, 1492 (1997)

L.S.Celenza, X.-D.Li, C.M.Shakin

Chiral Symmetry Breaking in the Presence of a Confining Interaction

doi: 10.1103/PhysRevC.55.1492
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1997CE04      Phys.Rev. C55, 3083 (1997)

L.S.Celenza, X.-D.Li, C.M.Shakin

Calculation of the Properties of the σ Meson in a Generalized Nambu-Jona-Lasinio Model with Lorentz-Vector Confinement

doi: 10.1103/PhysRevC.55.3083
Citations: PlumX Metrics


1997CE07      Phys.Rev. C56, 3326 (1997)

L.S.Celenza, X.-D.Li, C.M.Shakin

Singlet-Octet Mixing of Scalar Mesons in a Generalized Nambu-Jona-Lasinio Model

doi: 10.1103/PhysRevC.56.3326
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1997SH05      Phys.Rev. C55, 614 (1997)

C.M.Shakin, W.-D.Sun

Scalar-Isoscalar Meson Exchange in the Calculation of the Nucleon-Nucleon Interaction

doi: 10.1103/PhysRevC.55.614
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1996CE05      Phys.Rev. C54, 487 (1996)

L.S.Celenza, C.M.Shakin, W.-D.Sun

Calculation of the Nucleon-Nucleon Interaction Due to Vector-Meson Exchange

doi: 10.1103/PhysRevC.54.487
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1996GA04      Phys.Rev. C53, 1374 (1996)

S.-F.Gao, C.M.Shakin, W.-D.Sun

Many-Body Theory of ρ-ω Mixing

doi: 10.1103/PhysRevC.53.1374
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1996GA07      Phys.Rev. C53, 1936 (1996)

S.-F.Gao, L.S.Celenza, C.M.Shakin, W.-D.Sun, J.Szweda

Bosonization in the Presence of Confinement: Calculation of the nucleon-nucleon interaction

doi: 10.1103/PhysRevC.53.1936
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1996SH07      Phys.Rev. C53, 3152 (1996)

C.M.Shakin, W.-D.Sun

Use of Quark Wave Functions in the Calculation of Structure Functions of Mesons

doi: 10.1103/PhysRevC.53.3152
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1996SH14      Phys.Rev. C54, 1414 (1996)

C.M.Shakin, W.-D.Sun

Gauge Invariance and Confinement in a Generalized Nambu-Jona-Lasinio Model

doi: 10.1103/PhysRevC.54.1414
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1996SZ08      Few-Body Systems 20, 93 (1996)

J.Szweda, L.S.Celenza, C.M.Shakin, W.-D.Sun

Quark-Quark Correlations in the Nucleon in a Generalized Nambu-Jona-Lasinio Model

NUCLEAR STRUCTURE 1H, 1n; calculated μ. Generalized Nambu-Jona-Lasinio model, quark-quark correlations.

doi: 10.1007/s006010050034
Citations: PlumX Metrics


1995CE02      Phys.Rev. C51, 937 (1995)

L.S.Celenza, C.M.Shakin, W.-D.Sun, J.Szweda

Use of the Nambu-Jona-Lasino Model in the Calculation of the Density Dependence of Four-Quark Condensates

doi: 10.1103/PhysRevC.51.937
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1995CE05      Phys.Rev. C51, 3372 (1995)

L.S.Celenza, C.M.Shakin, W.-D.Sun, J.Szweda

Nuclear Many-Body Theory for the Study of QCD Sum Rules in Matter

doi: 10.1103/PhysRevC.51.3372
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1995SH05      Phys.Rev. C51, 2171 (1995)

C.M.Shakin, W.-D.Sun

Deep-Inelastic Scattering from the Pion and the Choice of Phenomenological Wave Functions

doi: 10.1103/PhysRevC.51.2171
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1995SH32      Phys.Rev. C52, 3353 (1995)

C.M.Shakin, W.-D.Sun, J.Szweda

Generalized Nambu-Jona-Lasinio Model in a Study of the Boson-Exchange Model of Nuclear Forces

doi: 10.1103/PhysRevC.52.3353
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1995SH33      Phys.Rev. C52, 3502 (1995)

C.M.Shakin, W.-D.Sun, J.Szweda

Meson-Mode Mixing in the Calculation of the Nucleon-Nucleon Interaction

doi: 10.1103/PhysRevC.52.3502
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1994SH03      Phys.Rev. C49, 1185 (1994)

C.M.Shakin, W.-D.Sun

Properties of the rho Meson in Nuclear Matter

doi: 10.1103/PhysRevC.49.1185
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1994SH14      Phys.Rev. C50, 1129 (1994)

C.M.Shakin

Relation of QCD Sum Rules in Matter and the Nuclear Many-Body Problem

doi: 10.1103/PhysRevC.50.1129
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1994SH22      Phys.Rev. C50, 2553 (1994)

C.M.Shakin, W.-D.Sun

Structure Function of Off-Mass-Shell Pions and the Calculation of the Sullivan Process

doi: 10.1103/PhysRevC.50.2553
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1993CE10      Int.J.Mod.Phys. E2, 603 (1993)

L.S.Celenza, C.M.Shakin, W.-D.Sun, J.Szweda, X.Zhu

Scalar-Isoscalar Correlator in a Phenomenological Coupled-Channel Quark Model

doi: 10.1142/S0218301393000261
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1991CE07      Phys.Rev. C44, 1460 (1991)

L.S.Celenza, C.M.Shakin, H.-W.Wang

Role of Final-State Interactions in the Calculation of the Hadronic Tensor of Nuclear Matter

NUCLEAR STRUCTURE 40Ca; calculated response functions. Nuclear matter hadronic tensor, final state interactions.

doi: 10.1103/PhysRevC.44.1460
Citations: PlumX Metrics


1991KO02      Phys.Rev. C43, 425 (1991)

W.Koepf, L.S.Celenza, C.M.Shakin

Kinematic Factors in the Theory of y Scaling

NUCLEAR REACTIONS 2H(e, e), (e, e'X), E not given; calculated scaling function. Convariant solvable model.

doi: 10.1103/PhysRevC.43.425
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1990CE01      Phys.Rev. C41, 1768 (1990)

L.S.Celenza, S.-F.Gao, C.M.Shakin

Relativistic Quasiparticle Description of the Structure of Finite Nuclei

NUCLEAR STRUCTURE 40Ca, 16O; calculated binding energy per particle, charge distribution, charge radius. Relativistic quasiparticle description.

doi: 10.1103/PhysRevC.41.1768
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1990CE02      Phys.Rev. C41, 2241 (1990)

L.S.Celenza, S.-f.Gao, A.Pantziris, C.M.Shakin

Asymmetry in Deep-Inelastic Scattering of Polarized Leptons from Polarized 2H and 3He

NUCLEAR STRUCTURE 2H, 3He; calculated structure function, polarized lepton scattering asymmetry. Polarized targets.

doi: 10.1103/PhysRevC.41.2241
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1986CE01      Phys.Rev. C33, 1012 (1986)

L.S.Celenza, A.Harindranath, C.M.Shakin

Sum Rules for the Longitudinal Response in Inclusive Electron Scattering

NUCLEAR REACTIONS 56Fe(e, e'X), E not given; calculated longitudinal response function. Relativistic Fermi gas model.

doi: 10.1103/PhysRevC.33.1012
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1985CE02      Phys.Rev. C31, 63 (1985)

L.S.Celenza, A.Harindranath, C.M.Shakin

Microscopic Foundations of Dirac Phenomenology

NUCLEAR REACTIONS 40Ca(p, p), E=80 MeV; calculated potentials. Dirac phenomenology.

doi: 10.1103/PhysRevC.31.63
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1985CE03      Phys.Rev. C31, 212 (1985)

L.S.Celenza, A.Rosenthal, C.M.Shakin

Covariant Soliton Dynamics: Structure of the nucleon

NUCLEAR STRUCTURE 1H, 1n; calculated rms radii, μ, model parameters. Covariant soliton dynamics.

doi: 10.1103/PhysRevC.31.212
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1985CE04      Phys.Rev. C31, 232 (1985)

L.S.Celenza, A.Rosenthal, C.M.Shakin

Many-Body Soliton Dynamics: Modification of nucleon properties in nuclei

NUCLEAR STRUCTURE 1n, 1H; calculated rms radii, μ, model parameters vs quark self energy parameter. Many-body soliton dynamics.

doi: 10.1103/PhysRevC.31.232
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1985CE05      Phys.Rev. C31, 946 (1985)

L.S.Celenza, A.Harindranath, A.Rosenthal, C.M.Shakin

Evidence for the Modification of Nucleon Properties in Nuclei from Traditional Nuclear Physics Experiments

NUCLEAR STRUCTURE 208Pb; calculated charge density. Relativistic mean field theory matter densities.

doi: 10.1103/PhysRevC.31.946
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1985CE08      Phys.Rev. C31, 1944 (1985)

L.S.Celenza, A.Harindranath, C.M.Shakin, A.Rosenthal

Quark Effects in the Charge Distribution of 208Pb

NUCLEAR STRUCTURE 208Pb; calculated charge distribution. Quark effects, RPA.

doi: 10.1103/PhysRevC.31.1944
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1985CE09      Phys.Rev. C32, 248 (1985)

L.S.Celenza, A.Harindranath, C.M.Shakin

Effects of Medium-Modified Form Factors in Quasielastic Electron Scattering from 12C

NUCLEAR REACTIONS 12C(e, e'X), E not given; calculated longitudinal, transverse response functions vs momentum, energy transfer. Impulse approximation, medium modified electromagnetic form factors.

doi: 10.1103/PhysRevC.32.248
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1985CE10      Phys.Rev. C32, 650 (1985)

L.S.Celenza, A.Harindranath, C.M.Shakin, A.Rosenthal

Quark Effects in Nuclear Longitudinal Response Functions

NUCLEAR REACTIONS 40Ca, 56Fe(e, e'), E not given; calculated longitudinal response functions.

doi: 10.1103/PhysRevC.32.650
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1985CE14      Phys.Rev. C32, 2095 (1985)

L.S.Celenza, C.A.Matyas, C.M.Shakin

Nuclear Collective Response Calculated with Realistic Forces

NUCLEAR REACTIONS 2H, 208Pb(polarized p, p), E=500 MeV; calculated longitudinal, transverse response functions. TDA, realistic forces.

doi: 10.1103/PhysRevC.32.2095
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1985CE15      Phys.Rev. C32, 2173 (1985)

L.S.Celenza, A.Harindranath, C.M.Shakin

Distribution of Charge and Matter in Nuclei: Charge density difference of 206Pb and 205Tl

NUCLEAR STRUCTURE 205Tl, 206Pb; calculated charge density differences. Medium modified nucleon form factors.

doi: 10.1103/PhysRevC.32.2173
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1983CE03      Phys.Rev. C27, 2792 (1983)

L.S.Celenza, W.S.Pong, C.M.Shakin

Longitudinal and Transverse Response Functions for Quasielastic Electron Scattering

NUCLEAR REACTIONS 56Fe(e, e'), E not given; calculated quasielastic, longitudinal, transverse response functions. Impulse approximation, nucleon-nucleus, nucleon-isobar transition amplitudes.

doi: 10.1103/PhysRevC.27.2792
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1982CE03      Phys.Rev. C26, 320 (1982)

L.S.Celenza, W.S.Pong, M.M.Rahman, C.M.Shakin

Nuclear Dynamics and Quasi-Elastic Electron Scattering

NUCLEAR REACTIONS 56Fe, 12C(e, e'), E not given; calculated longitudinal, transverse response functions. Modified impulse approximation.

doi: 10.1103/PhysRevC.26.320
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1980BH01      Phys.Rev. C21, 1903 (1980)

R.S.Bhalerao, L.C.Liu, C.M.Shakin

Systematic Features of the Pion-Nucleus Interaction

NUCLEAR REACTIONS 40Ca(π+, π+), E=40, 50, 115.5, 130, 163.5, 241 MeV; 40Ca(π-, π-), E=115.5, 130, 163.5, 241 MeV; 48Ca(π+, π+), (π-, π-), E=130 MeV; analyzed data; deduced pion-nucleus interaction systematics. First, second order optical potentials.

doi: 10.1103/PhysRevC.21.1903
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1979LI01      Phys.Rev. C19, 129 (1979)

L.C.Liu, C.M.Shakin

Role of Second-Order Optical Potential in Pion-Oxygen Scattering

NUCLEAR REACTIONS 16O(π+, π+), E=40-342.6 MeV; calculated σ(θ) including second-order optical potential; deduced possibility of universal parametrization.

doi: 10.1103/PhysRevC.19.129
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1979LI15      Nuovo Cim. 53A, 142 (1979)

L.C.Liu, C.M.Shakin

Determination of Spectroscopic Amplitudes from Electron Scattering Data

NUCLEAR REACTIONS 16O(e, e), E not given; calculated spectroscopic amplitudes. Translationally invariant theory, experimental charge form factors.

doi: 10.1007/BF02776411
Citations: PlumX Metrics


1977LI11      Phys.Rev. C16, 333 (1977)

L.C.Liu, C.M.Shakin

Can Multiple-Scattering Theory Explain the Low-Energy Pion-Nucleus Interaction (Question)

NUCLEAR REACTIONS 4He, 12C(π-, π-), E=50 MeV; calculated σ(θ).

doi: 10.1103/PhysRevC.16.333
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1977LI18      Phys.Rev. C16, 1963 (1977)

L.C.Liu, C.M.Shakin

How Useful Is the Fixed-Scatterer Approximation in Pion Physics (Question)

NUCLEAR REACTIONS 4He(π-, π-), E=50-260 MeV; calculated σ(E, θ). Fixed scatterer approximation.

doi: 10.1103/PhysRevC.16.1963
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1976CE01      Phys.Rev. C13, 2451 (1976)

L.S.Celenza, L.C.Liu, C.M.Shakin

Covariant Calculation on Pion-4He Elastic Scattering in the (3, 3) Resonance Region

NUCLEAR REACTIONS 4He(π-, π-), E=110-260 MeV; calculated σ(θ). Covariant optical potential.

doi: 10.1103/PhysRevC.13.2451
Citations: PlumX Metrics


1976LI24      Phys.Rev. C14, 1885 (1976)

L.C.Liu, C.M.Shakin

Nuclear Structure Studied via Pion-Nucleus Elastic Scattering at 1 GeV

NUCLEAR REACTIONS 4He, 12C, 16O(π, π), E=1.12 GeV; calculated σ. Covariant optical model.

doi: 10.1103/PhysRevC.14.1885
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1975CE03      Phys.Rev. C12, 1983 (1975)

L.Celenza, L.C.Liu, C.M.Shakin

Calculation of the Covariant Pion-Nucleus Optical Potential. I. Kinematical Aspects

NUCLEAR REACTIONS 12C(π, π), E=80 MeV; calculated potential.

doi: 10.1103/PhysRevC.12.1983
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1974SH08      Phys.Rev. C9, 1679 (1974)

C.M.Shakin, M.S.Weiss

Cluster Model and the Photodisintegration of 6Li

NUCLEAR REACTIONS 6Li(γ, p), (γ, X); calculated σ(E). Coupled channels, cluster model.

doi: 10.1103/PhysRevC.9.1679
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1974WA12      Phys.Rev. C9, 2144 (1974)

W.L.Wang, C.M.Shakin

Angular Distribution and Polarization of 16O(γ, n0)15O

NUCLEAR REACTIONS 16O(γ, n), E=21-26 MeV; calculated σ(E, En, θ), deduced giant resonances.

doi: 10.1103/PhysRevC.9.2144
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1973ER10      Phys.Rev. C8, 440 (1973)

D.J.Ernst, C.M.Shakin, R.M.Thaler

Center-of-Mass Motion and Angular Momentum Projection

NUCLEAR STRUCTURE 12C, 20Ne, 28Si, 36Ar; calculated rotational energies.

doi: 10.1103/PhysRevC.8.440
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1973SH03      Phys.Rev. C7, 494 (1973)

C.M.Shakin, R.M.Thaler

Elastic Scattering of Nucleons from Correlated Nuclei

doi: 10.1103/PhysRevC.7.494
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1973SH08      Phys.Rev. C7, 1820 (1973)

C.M.Shakin, M.S.Weiss

Threshold Photodisintegration of 6Li

NUCLEAR REACTIONS 6Li(γ, X), E=threshold-12 MeV; calculated σ(E), average neutron energy (E).

doi: 10.1103/PhysRevC.7.1820
Citations: PlumX Metrics


1973SH12      Phys.Rev. C8, 411 (1973)

C.M.Shakin, M.S.Weiss

Nuclear Polarication and the Muonic X-Ray Spectrum of Pb

NUCLEAR STRUCTURE, Mesic-Atoms 208Pb; calculated muonic levels.

doi: 10.1103/PhysRevC.8.411
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1973WA03      Phys.Rev.Lett. 30, 301 (1973)

W.L.Wang, C.M.Shakin

Evidence for a Giant Quadrupole Resonance in Oxygen-16

NUCLEAR REACTIONS 16O(γ, n), E < 26 MeV; calculated σ(E;θ(n)), P(n)(E;θ). 16O deduced giant quadrupole resonance structure.

doi: 10.1103/PhysRevLett.30.301
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1972AU04      Rev.Mod.Phys. 44, 48 (1972)

N.Auerbach, J.Hufner, A.K.Kerman, C.M.Shakin

A Theory of Isobaric Analog Resonances

doi: 10.1103/RevModPhys.44.48
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1972BL01      Phys.Rev. C5, 238 (1972)

S.D.Bloom, M.S.Weiss, C.M.Shakin

Nuclear γ Rays Following K- Capture

NUCLEAR REACTIONS 16O, 208Pb(K-, Xγ), E approx 0; calculated capture rates.

doi: 10.1103/PhysRevC.5.238
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1972DA15      Phys.Rev. C6, 1455 (1972)

J.da Providencia, C.M.Shakin

Three-Body Clusters in Nuclear Matter

doi: 10.1103/PhysRevC.6.1455
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1972LO11      Phys.Rev.Lett. 28, 1729 (1972)

J.T.Londergan, C.M.Shakin

Charge-Dependent Effects in the Photodisintegration of 4He

NUCLEAR REACTIONS 4He(γ, n), (γ, p), E < 34 MeV; calculated σ(E); analyzed charge-dependent effects.

doi: 10.1103/PhysRevLett.28.1729
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1972WA13      Phys.Rev. C5, 1898 (1972)

W.L.Wang, C.M.Shakin

Intermediate Structure and the Photodisintegration of O16

NUCLEAR REACTIONS 16O(γ, n), (γ, p), E=20-26 MeV; calculated σ(E). 16O; analyzed resonance structure. Projection operator formalism.

doi: 10.1103/PhysRevC.5.1898
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1971PR16      Phys.Lett. 37B, 151 (1971)

H.C.Pradhan, C.M.Shakin

Comparison of the Spectra of 18O and 18F Calculated with Woods-Saxon and Harmonic-Oscillator Wave Functions

NUCLEAR STRUCTURE 18O, 18F; calculated levels, wave functions. Woods-Saxon harmonic-oscillator wave functions.

doi: 10.1016/0370-2693(71)90038-4
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1971SH05      Phys.Rev.Lett. 26, 902 (1971)

C.M.Shakin, W.L.Wang

Intermediate Structure and the Giant-Dipole Resonance in O16

NUCLEAR REACTIONS 16O(γ, n), E < 26 MeV; calculated σ(E). 16O calculated giant dipole resonance structure. 3p-3h model.

doi: 10.1103/PhysRevLett.26.902
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1970SH15      Phys.Rev. C2, 1809 (1970)

C.M.Shakin, M.S.Weiss

Threshold Photodisintegration of Pb208

NUCLEAR REACTIONS 208Pb(γ, n), E=9-13 MeV; 207Pb(n, γ), E=thermal; measured nothing; analyzed available data.

doi: 10.1103/PhysRevC.2.1809
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1964LE20      Ann.Phys.(N.Y.) 27, 13 (1964)

R.H.Lemmer, C.M.Shakin

Resonance Reactions and the Nuclear Shell Model I

doi: 10.1016/0003-4916(64)90081-8
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1962KE07      Phys.Letters, 1, 151 (1962)

A.K.Kerman, C.M.Shakin

Vibrations of Spherical Nuclei

NUCLEAR STRUCTURE 62Ni; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(62)90331-1
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