NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = C.M.Shakin Found 81 matches. 2005LI25 Phys.Rev. C 71, 068203 (2005) Relativistic calculation of the width of the Θ+(1540) pentaquark
doi: 10.1103/PhysRevC.71.068203
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
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
2004LI77 Phys.Rev. C 70, 068201 (2004) Comparison of models of critical opacity in the quark-gluon plasma
doi: 10.1103/PhysRevC.70.068201
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
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
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
2002LI26 Phys.Rev. C65, 045205 (2002) Calculation of 1/Nc Corrections to the SU(3)-Flavor Nambu-Jona-Lasino Model
doi: 10.1103/PhysRevC.65.045205
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
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
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
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
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
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
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
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
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
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
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
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
1998HU21 Phys.Rev. C58, 3648 (1998) Radial Excitations in the Analysis of φ-ω and η-η' Mixing
doi: 10.1103/PhysRevC.58.3648
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
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
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
1997SH05 Phys.Rev. C55, 614 (1997) Scalar-Isoscalar Meson Exchange in the Calculation of the Nucleon-Nucleon Interaction
doi: 10.1103/PhysRevC.55.614
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
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
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
1996SH07 Phys.Rev. C53, 3152 (1996) Use of Quark Wave Functions in the Calculation of Structure Functions of Mesons
doi: 10.1103/PhysRevC.53.3152
1996SH14 Phys.Rev. C54, 1414 (1996) Gauge Invariance and Confinement in a Generalized Nambu-Jona-Lasinio Model
doi: 10.1103/PhysRevC.54.1414
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
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
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
1995SH05 Phys.Rev. C51, 2171 (1995) Deep-Inelastic Scattering from the Pion and the Choice of Phenomenological Wave Functions
doi: 10.1103/PhysRevC.51.2171
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
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
1994SH03 Phys.Rev. C49, 1185 (1994) Properties of the rho Meson in Nuclear Matter
doi: 10.1103/PhysRevC.49.1185
1994SH14 Phys.Rev. C50, 1129 (1994) Relation of QCD Sum Rules in Matter and the Nuclear Many-Body Problem
doi: 10.1103/PhysRevC.50.1129
1994SH22 Phys.Rev. C50, 2553 (1994) Structure Function of Off-Mass-Shell Pions and the Calculation of the Sullivan Process
doi: 10.1103/PhysRevC.50.2553
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
1979LI01 Phys.Rev. C19, 129 (1979) 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
1979LI15 Nuovo Cim. 53A, 142 (1979) 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
1977LI11 Phys.Rev. C16, 333 (1977) 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
1977LI18 Phys.Rev. C16, 1963 (1977) 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
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
1976LI24 Phys.Rev. C14, 1885 (1976) 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
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
1974SH08 Phys.Rev. C9, 1679 (1974) 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
1974WA12 Phys.Rev. C9, 2144 (1974) 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
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
1973SH03 Phys.Rev. C7, 494 (1973) Elastic Scattering of Nucleons from Correlated Nuclei
doi: 10.1103/PhysRevC.7.494
1973SH08 Phys.Rev. C7, 1820 (1973) 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
1973SH12 Phys.Rev. C8, 411 (1973) Nuclear Polarication and the Muonic X-Ray Spectrum of Pb NUCLEAR STRUCTURE, Mesic-Atoms 208Pb; calculated muonic levels.
doi: 10.1103/PhysRevC.8.411
1973WA03 Phys.Rev.Lett. 30, 301 (1973) 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
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
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
1972DA15 Phys.Rev. C6, 1455 (1972) Three-Body Clusters in Nuclear Matter
doi: 10.1103/PhysRevC.6.1455
1972LO11 Phys.Rev.Lett. 28, 1729 (1972) 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
1972WA13 Phys.Rev. C5, 1898 (1972) 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
1971PR16 Phys.Lett. 37B, 151 (1971) 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
1971SH05 Phys.Rev.Lett. 26, 902 (1971) 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
1970SH15 Phys.Rev. C2, 1809 (1970) 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
1964LE20 Ann.Phys.(N.Y.) 27, 13 (1964) Resonance Reactions and the Nuclear Shell Model I
doi: 10.1016/0003-4916(64)90081-8
1962KE07 Phys.Letters, 1, 151 (1962) 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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