NSR Query Results
Output year order : Descending NSR database version of May 3, 2024. Search: Author = P.Guichon Found 55 matches. 2023LE09 Phys.Rev. C 108, 015804 (2023) J.Leong, T.F.Motta, A.W.Thomas, P.A.M.Guichon Dense nuclear matter with phenomenological short distance repulsion
doi: 10.1103/PhysRevC.108.015804
2021MO08 Nucl.Phys. A1009, 122157 (2021) T.F.Motta, P.A.M.Guichon, A.W.Thomas On the sound speed in hyperonic stars
doi: 10.1016/j.nuclphysa.2021.122157
2020AN18 Phys.Rev. C 102, 065801 (2020) S.Antic, J.R.Stone, J.C.Miller, K.L.Martinez, P.A.M.Guichon, A.W.Thomas Outer crust of a cold, nonaccreting neutron star within the quark-meson-coupling model NUCLEAR STRUCTURE Z=26-50, N=20-90; calculated nuclear binding energies, two-neutron drip line using the QMCπ-III mass model, and compared with experimental data. 56Fe, 62,64,66,78Ni, 80Zn, 82Ge, 84Se, 86,118,120Kr, 120,122,124Sr, 121Y, 122Zr, 124Mo, 126Ru; calculated numerical results of the equation of state (EOSs) in the outer crust of cold nonaccreting, nonrotating neutron stars, such as baryon number densities at the bottom and top of each layer, and neutron and electron chemical potentials, and properties of individual layers in the outer crust. Comparison with results from FRDM, HFB24, and NL3 mass models.
doi: 10.1103/PhysRevC.102.065801
2020BA15 Acta Phys.Pol. B51, 611 (2020) P.Baczyk, M.Konieczka, K.M.L.Martinez, S.Antic, P.A.M.Guichon, W.Satula, J.R.Stone, A.W.Thomas On Introducing Charge-Symmetry-Breaking Terms to Nuclear Energy Density Functionals
doi: 10.5506/APhysPolB.51.611
2020MA43 Phys.Rev. C 102, 034304 (2020) K.L.Martinez, A.W.Thomas, P.A.M.Guichon, J.R.Stone Tensor and pairing interactions within the quark-meson coupling energy-density functional NUCLEAR STRUCTURE Z=20, N=14-38; Z=28, N=20-50; Z=50, N=50-88; Z=82, N=96-138; calculated binding energies with and without tensor contribution, two-neutron shell gaps. 40,48Ca, 56,78Ni, 100,132Sn; calculated proton and neutron single-particle states, deformation energies, spin-orbit splittings with and without tensor contribution. 90,92,94,96,98,100,102,104,106,108,110,112Zr; calculated β2 deformation parameters and deformation energies. 254,256,254,256,258,260,262,264Fm, 254,256,258,260,262,264,266,268Rf; calculated two-neutron shell gaps. Quark-meson coupling (QMC) model (QMCπ-III-T), with the density functional which included tensor component, and pairing interaction from the QMC framework. Comparison with experimental data.
doi: 10.1103/PhysRevC.102.034304
2019MA57 Phys.Rev. C 100, 024333 (2019) K.L.Martinez, A.W.Thomas, J.R.Stone, P.A.M.Guichon Parameter optimization for the latest quark-meson coupling energy-density functional NUCLEAR STRUCTURE Z=20, 28, 50, 82; N=20, 28, 50, 82, 126; calculated binding energies, rms charge radii, and pairing gaps for 70 nuclei. Z=8-96, N=8-160; calculated binding energies, rms charge radii, and S(2n) for 739 even-even nuclei. Z=20, N=16-36; Z=28, N=26-52; Z=50, N=52-86; Z=82, N=98-142; calculated S(2n) for even-even nuclei. Z=20, A=34-58; Z=82, A=178-220; calculated isotopic shifts for even-even nuclei. 36,38,40,48Ca, 54Fe, 58,60,64Ni, 90Zr, 112,116,124Sn, 208Pb; calculated skin thicknesses. 40Ca, 78Ni, 132Sn; calculated proton and neutron single-particle states. Z=64, A=134-170; calculated B(E2) and β2 for the first 2+ states in even-even nuclei. 90Zr, 116Sn, 144Sm, 208Pb; calculated energies of giant monopole resonances (GMR). Z>96, A=232-294; calculated binding energies for superheavy nuclei. HF+BCS calculations with quark-meson-coupling (QMC) model, using QMCπ-II energy density functional. Optimization of model parameters by detailed comparisons and fittings with the experimental data. Comparison with other theoretical calculations.
doi: 10.1103/PhysRevC.100.024333
2019ST10 Phys.Rev. C 100, 044302 (2019) J.R.Stone, K.Morita, P.A.M.Guichon, A.W.Thomas Physics of even-even superheavy nuclei with 96 < Z < 110 in the quark-meson-coupling model NUCLEAR STRUCTURE 244,246,248,250,252,254Cf, 246,248,250,252,254,256Fm; calculated ground state binding energies and compared to values in AME-2016. 234,236,238,240,242,244,246,248,250,252,254,256,258,260,262,264,266,268,270,272,274,276,278,280Cm, 236,238,240,242,244,246,248,250,252,254,256,258,260,262,264,266,268,270,272,274,276,278,280,282Cf, 238,240,242,244,246,248,250,252,254,256,258,260,262,264,266,268,270,272,274,276,278,280,282,284Fm, 240,242,244,246,248,250,252,254,256,258,260,262,264,266,268,270,272,274,276,278,280,282,284,286No, 242,244,246,248,250,252,254,256,258,260,262,264,266,268,270,272,274,276,278,280,282,284,286,288Rf, 244,246,248,250,252,254,256,258,260,262,264,266,268,270,272,274,276,278,280,282,284,286,288,290Sg, 246,248,250,252,254,256,258,260,262,264,266,268,270,272,274,276,278,280,282,284,286,288,290,292Hs, 248,250,252,254,256,258,260,262,264,266,268,270,272,274,276,278,280,282,284,286,288,290,292,294Ds; calculated deformation energies and neutron pairing energies as a function of the quadrupole deformation parameter β2, S(2n), Q(α), shape coexistence in N=168-184 Sg nuclei. 40,48Ca, 56,68,78Ni, 90Zr, 100,132Sn, 146Gd, 208Pb; calculated proton and neutron single-particle energies. 244Cm, 248Cf, 252Fm, 256No, 260Rf, 264Sg, 268Hs, 272Ds; calculated neutron single-particle states. Quark-meson-coupling (QMC) model. Comparison with available experimental data from AME-2016 and databases at NNDC.
doi: 10.1103/PhysRevC.100.044302
2016ST07 Phys.Rev.Lett. 116, 092501 (2016) J.R.Stone, P.A.M.Guichon, P.G.Reinhard, A.W.Thomas Finite Nuclei in the Quark-Meson Coupling Model NUCLEAR STRUCTURE 270Db, 264,255Hs, 260,262Sg, 256,258Rf, 254,256No, 246,248,250,252,254,256Fm; calculated ground-state binding energies, deformation parameters. Effective quark-meson coupling (QMC) energy density functional (EDF), comparison with available data.
doi: 10.1103/PhysRevLett.116.092501
2010TS03 Int.J.Mod.Phys. E19, 2546 (2010) K.Tsushima, P.A.M.Guichon, R.Shyam, A.W.Thomas Binding of hypernuclei, and photoproduction of Λ-hypernuclei in the latest quark-meson coupling model NUCLEAR STRUCTURE 16,17O, 40,41,49Ca, 89Y, 91Zr, 208,209Pb; calculated hypernuclei single-particle energies. Quark-meson coupling model, comparison with experimental data.
doi: 10.1142/S021830131001706X
2008GU18 Nucl.Phys. A814, 66 (2008) P.A.M.Guichon, A.W.Thomas, K.Tsushima Binding of hypernuclei in the latest quark-meson coupling model NUCLEAR STRUCTURE 17O, 41,49Ca, 91Zr, 209Pb; calculated hypernuclei binding energies using quark-meson coupling model. Comparison with data.
doi: 10.1016/j.nuclphysa.2008.10.001
2007RI13 Nucl.Phys. A792, 341 (2007) J.Rikovska Stone, P.A.M.Guichon, H.H.Matevosyan, A.W.Thomas Cold uniform matter and neutron stars in the quark-meson-coupling model
doi: 10.1016/j.nuclphysa.2007.05.011
2006GU11 Nucl.Phys. A772, 1 (2006) P.A.M.Guichon, H.H.Matevosyan, N.Sandulescu, A.W.Thomas Physical origin of density dependent forces of Skyrme type within the quark meson coupling model NUCLEAR STRUCTURE 16O, 40,48Ca, 208Pb; calculated binding energies, radii, proton and neutron densities. Ni, Zr; calculated two-neutron drip line. 42Si, 60Ge; calculated two-neutron separation energy, shell quenching features. Quark-meson coupling model, comparison with Skyrme models, astrophysical implications discussed.
doi: 10.1016/j.nuclphysa.2006.04.002
2005GO08 Eur.Phys.J. A 24, Supplement 2, 33 (2005) M.Gorchtein, P.A.M.Guichon, M.Vanderhaeghen Transverse single spin asymmetry in elastic electron-proton scattering NUCLEAR REACTIONS 1H(e, e), E=3-11 GeV; calculated spin asymmetries, two-photon exchange contributions.
doi: 10.1140/epjad/s2005-04-006-2
2005GO23 Nucl.Phys. A755, 273c (2005) M.Gorchtein, P.A.M.Guichon, M.Vanderhaeghen Normal Spin Asymmetries in Elastic Electron-Proton Scattering NUCLEAR REACTIONS 1n, 1H(polarized e, e), E=3, 6, 11 GeV; calculated spin asymmetry, two-photon exchange contributions.
doi: 10.1016/j.nuclphysa.2005.03.026
2005GU05 Eur.Phys.J. A 24, Supplement 2, 23 (2005) Two photon effects in electron scattering NUCLEAR STRUCTURE 1H; analyzed electron scattering data, form factor ratios, two photon effects.
doi: 10.1140/epjad/s2005-04-004-4
2004DH01 Eur.Phys.J. A 19, Supplement 1, 47 (2004) N.d'Hose, E.Burtin, P.A.M.Guichon, J.Marroncle Feasibility study of deeply virtual compton scattering using COMPASS at CERN
doi: 10.1140/epjad/s2004-03-008-x
2004GO41 Nucl.Phys. A741, 234 (2004) M.Gorchtein, P.A.M.Guichon, M.Vanderhaeghen Beam normal spin asymmetry in elastic lepton-nucleon scattering NUCLEAR REACTIONS 1H(polarized e, e), E=3-11 GeV; calculated spin asymmetry, two-photon exchange contribution. Parton model.
doi: 10.1016/j.nuclphysa.2004.06.008
2004GU16 Phys.Rev.Lett. 93, 132502 (2004) Quark Structure and Nuclear Effective Forces
doi: 10.1103/PhysRevLett.93.132502
2004TH14 Prog.Theor.Phys.(Kyoto), Suppl. 156, 124 (2004) A.W.Thomas, P.A.M.Guichon, D.B.Leinweber, R.D.Young Towards a Connection between Nuclear Structure and QCD
doi: 10.1143/PTPS.156.124
2003BU16 Nucl.Phys. A721, 368c (2003) E.Burtin, N.d'Hose, P.A.M.Guichon, J.Marroncle Deeply Virtual Compton Scattering using COMPASS at CERN
doi: 10.1016/S0375-9474(03)01071-6
2003CH50 Phys.Rev. C 68, 035209 (2003) G.Chanfray, M.Ericson, P.A.M.Guichon Scalar susceptibility and chiral symmetry restoration in nuclei
doi: 10.1103/PhysRevC.68.035209
2003GU15 Phys.Rev.Lett. 91, 142303 (2003) P.A.M.Guichon, M.Vanderhaeghen How to Reconcile the Rosenbluth and the Polarization Transfer Methods in the Measurement of the Proton Form Factors NUCLEAR STRUCTURE 1H; analyzed data; deduced form factor ratio, two-photon exchange correction. Comparison of Rosenbluth and polarization transfer analysis.
doi: 10.1103/PhysRevLett.91.142303
2002DH02 Nucl.Phys. A711, 160c (2002) N.d'Hose, E.Burtin, P.A.M.Guichon, S.Kerhoas-Cavata, J.Marroncle, L.Mosse Feasibility Study of Deeply Virtual Compton Scattering using COMPASS
doi: 10.1016/S0375-9474(02)01208-3
2002DH03 Acta Phys.Pol. B33, 3773 (2002) N.d'Hose, E.Burtin, P.A.M.Guichon, S.Kerhoas-Cavata, J.Marroncle, L.Mosse Feasibility Study of Deeply Virtual Compton Scattering Using Compass at CERN
2001CH27 Phys.Rev. C63, 055202 (2001) G.Chanfray, M.Ericson, P.A.M.Guichon Chiral Symmetry and Quantum Hadrodynamics
doi: 10.1103/PhysRevC.63.055202
2001DE03 Nucl.Phys. A680, 250c (2001) J.Delorme, M.Ericson, P.A.M.Guichon, A.W.Thomas Mass Reduction as Signal of Chiral Symmetry Restoration
doi: 10.1016/S0375-9474(00)00422-X
2001GU06 Nucl.Phys. A680, 229c (2001) Quark Models of Nuclear Physics
doi: 10.1016/S0375-9474(00)00419-X
2000DE06 Phys.Rev. C61, 025202 (2000) J.Delorme, M.Ericson, P.A.M.Guichon, A.W.Thomas Correlator Mixing and Mass Reduction as Signals of Chiral Symmetry Restoration
doi: 10.1103/PhysRevC.61.025202
2000FR07 Nucl.Phys. A663-664, 389c (2000) J.M.Friedrich, P.Bartsch, D.Baumann, J.Berthot, P.Y.Bertin, V.Breton, W.U.Boeglin, R.Bohm, N.d'Hose, T.Caprano, S.Derber, N.Degrande, M.Ding, M.O.Distler, J.E.Ducret, R.Edelhoff, I.Ewald, H.Fonvieille, J.Friedrich, R.Geiges, Th.Gousset, P.A.M.Guichon, H.Holvoet, Ch.Hyde-Wright, P.Jennewein, M.Kahrau, S.Kerhoas, M.Korn, H.Kramer, K.W.Krygier, V.Kunde, B.Lannoy, D.Lhuillier, A.Liesenfeld, C.Marchand, D.Marchand, J.Martino, H.Merkel, K.Merle, P.Merle, G.De Meyer, J.Mougey, R.Neuhausen, E.Offermann, Th.Pospischil, G.Quemener, O.Ravel, Y.Roblin, J.Roche, D.Rohe, G.Rosner, D.Ryckbosch, P.Sauer, H.Schmieden, S.Schardt, G.Tamas, M.Tytgat, M.Vanderhaeghen, L.Van Hoorebeke, R.Van de Vyver, J.Van de Wiele, P.Vernin, A.Wagner, Th.Walcher The First Dedicated Virtual Compton Scattering Experiment at MAMI NUCLEAR REACTIONS 1H(e, e'γ), E not given; measured ep-coin, σ(E, θ(e), θ(p)); deduced structure function.
doi: 10.1016/S0375-9474(99)00624-7
2000GU10 Nucl.Phys. A666-667, 234c (2000) P.A.M.Guichon, M.Guidal, M.Vanderhaeghen Deeply Virtual Compton Scattering
doi: 10.1016/S0375-9474(00)00032-4
2000RO21 Phys.Rev.Lett. 85, 708 (2000) J.Roche, J.M.Friedrich, D.Lhuillier, P.Bartsch, D.Baumann, J.Berthot, P.Y.Bertin, V.Breton, W.U.Boeglin, R.Bohm, N.D'Hose, S.Derber, N.Degrande, M.Ding, M.O.Distler, J.E.Ducret, I.Ewald, H.Fonvieille, J.Friedrich, P.A.M.Guichon, H.Holvoet, Ch.E.Hyde-Wright, P.Jennewein, M.Kahrau, S.Kerhoas, K.W.Krygier, B.Lannoy, A.Liesenfeld, C.Marchand, D.Marchand, J.Marroncle, J.Martino, H.Merkel, P.Merle, G.De Meyer, J.Mougey, U.Muller, R.Neuhausen, Th.Pospischil, G.Quemener, O.Ravel, Y.Roblin, D.Rohe, G.Rosner, D.Ryckbosch, H.Schmieden, G.Tamas, M.Tytgat, M.Vanderhaeghen, L.Van Hoorebeke, R.Van de Vyver, J.Van de Wiele, P.Vernin, A.Wagner, Th.Walcher, M.Weiss First Determination of Generalized Polarizabilities of the Proton by a Virtual Compton Scattering Experiment NUCLEAR REACTIONS 1H(polarized e, e'γ), E=855 MeV; measured σ(E, θ(e), θ(p)). 1H deduced dynamic structure functions, generalized polarizibilities. High-resolution spectrometers, virtual Compton scattering.
doi: 10.1103/PhysRevLett.85.708
2000VA06 Nucl.Phys. A663-664, 324c (2000) M.Vanderhaeghen, P.A.M.Guichon, M.Guidal Deeply Virtual Electroproduction of Photons and Mesons on the Nucleon NUCLEAR REACTIONS 1H(μ+, X), (e+, X), (e, X), E=high; calculated ρ, pion production σ(θ).
doi: 10.1016/S0375-9474(99)00608-9
1999RO30 Nucl.Phys. (Supplement) A654, 547c (1999) J.Roche, P.Bartsch, J.Berthot, P.Y.Bertin, V.Breton, W.U.Boeglin, R.Bohm, N.d'Hose, T.Caprano, S.Derber, N.Degrande, M.Distler, J.E.Ducret, R.Edelhoff, I.Ewald, H.Fonvieille, J.Friedrich, J.M.Friedrich, R.Geiges, Th.Gousset, P.A.M.Guichon, H.Holvoet, Ch.Hyde-Wright, P.Jennewein, M.Kahrau, S.Kerhoas, M.Korn, H.Kramer, K.W.Krygier, V.Kunde, B.Lannoy, D.Lhuillier, A.Liesenfeld, C.Marchand, D.Marchand, J.Martino, H.Merkel, K.Merle, P.Merle, G.De Meyer, J.Mougey, R.Neuhausen, E.Offermann, Th.Pospischil, G.Quemener, O.Ravel, Y.Roblin, G.Rosner, D.Ryckbosch, P.Sauer, H.Schmieden, S.Schardt, G.Tamas, M.Tytgat, M.Vanderhaeghen, L.Van Hoorebeke, R.Van de Vyver, J.Van de Wiele, P.Vernin, A.Wagner, Th.Walcher, S.Wolf Virtual Compton Scattering Under π0 Threshold at Q2 = 0.33 GeV2. Preliminary Results. NUCLEAR REACTIONS 1H(e, e'γ), E=750-855 MeV; measured ep-coin, photon polarization, σ(θ). Virtual Compton scattering.
doi: 10.1016/S0375-9474(00)88498-5
1999VA13 Phys.Rev. D60, 094017 (1999) M.Vanderhaeghen, P.A.Guichon, M.Guidal Deeply Virtual Electroproduction of Photons and Mesons on the Nucleon: Leading order amplitudes and power corrections NUCLEAR REACTIONS 1H(e, X), E not given; calculated exclusive meson, photon production σ(θ). Skewed parton distribution formalism.
doi: 10.1103/PhysRevD.60.094017
1999VA24 Nucl.Phys. (Supplement) A654, 602c (1999) M.Vanderhaeghen, P.A.M.Guichon, M.Guidal Exclusive Electroproduction of Vector Mesons, Pseudoscalar Mesons and Photons in the Bjorken Regime NUCLEAR REACTIONS 1H(e, X), E=6 GeV; 1H(e+, X), E=27 GeV; 1H(μ+, X), E=200 GeV; calculated σ for the production of vector mesons, pseudoscalar mesons and photons. Comparison between different experimental conditions.
doi: 10.1016/S0375-9474(00)88509-7
1998GU25 Prog.Part.Nucl.Phys. 41, 125 (1998) P.A.M.Guichon, M.Vanderhaeghen Virtual Compton Scattering Off the Nucleon
doi: 10.1016/S0146-6410(98)00056-8
1997VA19 Nucl.Phys. A622, 144c (1997) M.Vanderhaeghen, P.A.M.Guichon, J.Van de Wiele Compton Scattering and the Nucleon Valence Wavefuntion NUCLEAR REACTIONS 1H(polarized γ, γ), (γ, γ), E=2-6 GeV; calculated Compton scattering σ, asymmetry. Perturbative QCD formalism, different nucleon quark distribution amplitudes, extensions to model independent approach.
doi: 10.1016/S0375-9474(97)00339-4
1996GU12 Nucl.Phys. A601, 349 (1996) P.A.M.Guichon, K.Saito, E.Rodionov, A.W.Thomas The Role of Nucleon Structure in Finite Nuclei NUCLEAR STRUCTURE 40Ca; calculated nucleon spectra, charge density. 16O; calculated charge density, scalar, vector, Coulomb potentials. Quark-meson coupling model.
doi: 10.1016/0375-9474(96)00033-4
1996KR03 Nucl.Phys. A598, 435 (1996) P.Kroll, M.Schurmann, P.A.M.Guichon Virtual Compton Scattering Off Protons at Moderately Large Momentum Transfer NUCLEAR REACTIONS 1H(γ, γ), E=high; calculated real Compton scattering σ. Diquark model, virtual scattering.
doi: 10.1016/S0375-9474(96)00002-4
1995GU12 Nucl.Phys. A591, 606 (1995) P.A.M.Guichon, G.Q.Liu, A.W.Thomas Virtual Compton Scattering and Generalized Polarizabilities of the Proton NUCLEAR REACTIONS 1H(e, e), E=threshold; analyzed photon electroproduction characteristics. 1H deduced polarizabilities associated features. Virtual Compton scattering.
doi: 10.1016/0375-9474(95)00217-O
1991DE31 Phys.Lett. 263B, 157 (1991) The (3He, t) Reaction as a Probe of the Nuclear Pionic Mode NUCLEAR REACTIONS 12C, 208Pb(3He, t), E=2 GeV; calculated σ(θ) vs momentum. One-step isobar excitation.
doi: 10.1016/0370-2693(91)90579-F
1984GU04 Phys.Lett. 134B, 15 (1984) Quarks and the Deuteron Asymptotic D State NUCLEAR STRUCTURE 2H; calculated asymptotic D- to S-state ratio, limits to quadrupole moment change; deduced pion, gluon exchange induced tensor force role. Quark model.
doi: 10.1016/0370-2693(84)90974-2
1983GU09 Nucl.Phys. A402, 541 (1983) Forward (p, n) Reactions and Nucleon-Nucleon Scattering NUCLEAR REACTIONS 13C(p, n), E=30-300 MeV; calculated Fermi, Gamow-Teller transition, reaction probability ratio vs E. Nucleon-nucleon phase shift input, T-matrix formalism.
doi: 10.1016/0375-9474(83)90218-X
1983GU17 Phys.Lett. 132B, 265 (1983) Spin-Flip Versus Non-Spin-Flip Interaction in Forward (p, n) Reactions NUCLEAR REACTIONS 7Li, 13,14C, 26Mg, 37Cl, 42Ca(p, n), E=60-200 MeV; 2H(p, n), E=212-495 MeV; 1H(n, n), E=40-770 MeV; calculated Gamow-Teller to Fermi transition probability ratio vs E; deduced inconsistensies between values from (p, n), free nucleon-nucleon data.
doi: 10.1016/0370-2693(83)90304-0
1982GU09 Nucl.Phys. A382, 461 (1982) Chiral Symmetry and Axial Charge density in the Isovector 0+ → 1+, 1+ → 0+ Transition in the A = 12 System NUCLEAR STRUCTURE A=12; analyzed β-decay, μ-capture, electron scattering data; deduced weak, electromagnetic nuclear current form factors.
doi: 10.1016/0375-9474(82)90356-6
1981DE07 Phys.Lett. 99B, 187 (1981) J.Delorme, A.Figureau, P.Guichon Nuclear Critical Opalescence and the M1 Form Factors of 12C and 13C NUCLEAR REACTIONS 12C(e, e'), 13C(e, e), E not given; calculated M1 form factors; deduced possible critical opalescence effects. Static limit, coupled integral equations, effective spin operators.
doi: 10.1016/0370-2693(81)91104-7
1981ER11 Nucl.Phys. A372, 377 (1981) M.Ericson, P.Guichon, R.D.Viollier Nuclear Axial Polarizability and the α + α Interaction NUCLEAR REACTIONS 4He(α, α), E=25-50 MeV; calculated phase shifts, (L)≥4; deduced nuclear polarization. Two pion exchange, static pion field.
doi: 10.1016/0375-9474(81)90041-5
1981GI08 Phys.Rev. C24, 241 (1981) M.Giffon, A.Goncalves, P.A.M.Guichon, J.Julien, L.Roussel, C.Samour μ- Partical Capture Rates in 10B, 12C, and 14N ATOMIC PHYSICS, Mesic-Atoms 10B, 12C, 14N, 16O(μ-, X), E at rest; measured E(X-ray). Hyperpure Ge detectors. NUCLEAR REACTIONS 10B, 12C, 14N(μ-, ν), E at rest; measured Eγ, Iγ; deduced partial capture rates. Ge(Li) detector. Shell model, meson exchange corrections.
doi: 10.1103/PhysRevC.24.241
1979DE01 Phys.Rev. C19, 120 (1979) One-Pion Exchange Currents Effect on Partial Muon Capture Rates for 1p Shell Nuclei NUCLEAR REACTIONS 6Li, 10,11B, 12,13C, 14N(μ-, ν), E=at rest; calculated partial capture rates using 1p-shell model with one-pion exchange currents.
doi: 10.1103/PhysRevC.19.120
1979DE15 Z.Phys. A290, 373 (1979) One-Pion Exchange Currents Effect on the Allowed Beta-Decays in the 1p Shell Nuclei NUCLEAR STRUCTURE A=6-14; calculated log ft for allowed β-decay transitions. 1p-shell model with one pion exchange; deduced state dependence of mesonic corections.
doi: 10.1007/BF01408398
1979GU06 Phys.Rev. C19, 987 (1979) P.Guichon, B.Bihoreau, M.Giffon, A.Goncalves, J.Julien, L.Roussel, C.Samour μ- Partial Capture Rates in 16O NUCLEAR REACTIONS 16O(μ-, ν), E=at rest; measured Iγ; deduced partial capture rates. Mesonic exchange corrections considered.
doi: 10.1103/PhysRevC.19.987
1979GU08 Phys.Lett. 82B, 28 (1979) Nuclear Wave Functions and Mesonic Exchange Currents in the Weak Transition 16O(0+) → 16N(0-) NUCLEAR REACTIONS 16O(μ-, ν), E at rest; calculated transition probability. RADIOACTIVITY 16N [from 16O(μ-, ν)]; calculated β decay probability to 16O ground state; deduced sensitivity to deviations from closed core description of 16O (ground state), importance of meson exchange effects.
doi: 10.1016/0370-2693(79)90417-9
1978DE15 Nuovo Cim. 43A, 475 (1978) P.Desgrolard, P.A.M.Guichon, J.Joseph Muon Capture Rates for A = 6-14 Nuclei ATOMIC PHYSICS 6,7Li, 9Be, 10,11B, 12,13C, 14N(μ-, X); calculated muon capture rates.
doi: 10.1007/BF02730442
1978GU05 Z.Phys. A285, 183 (1978) P.Guichon, M.Giffon, J.Joseph, R.Laverriere, C.Samour Exchange Current Corrections for Partial Capture Rates of Muons in Nuclei NUCLEAR REACTIONS 12C, 16O, 32S, 40Ca(μ-, γ); calculated exchange current corrections for partial capture rates.
doi: 10.1007/BF01408745
1978GU07 Phys.Lett. 74B, 15 (1978) P.A.M.Guichon, M.Giffon, C.Samour Possible Evidence for Mesonic Exchange Correction in 16N(0-) → 16O(0+)β-Decay and μ-Capture Reactions RADIOACTIVITY 16N; calculated mesonic exchange correction. NUCLEAR REACTIONS 16O(μ-, γ); calculated mesonic exchange correction.
doi: 10.1016/0370-2693(78)90047-3
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