NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = D.O.Riska Found 101 matches. Showing 1 to 100. [Next]2017RI02 Int.J.Mod.Phys. E26, 1740022 (2017) Chiral electroweak currents in nuclei NUCLEAR STRUCTURE 2,3H, 3,4He, 9,7Be, 8B, 6,7,8Li; calculated M1, E2 transition widths, magnetic moments, magnetic form factors. Comparison with available data.
doi: 10.1142/S0218301317400225
2008AC01 Int.J.Mod.Phys. E17, 212 (2008) A.Acus, E.Norvaisas, D.O.Riska Nuclei as superposition of topological solitons
doi: 10.1142/S0218301308009719
2008AN13 Eur.Phys.J. A 37, 263 (2008) The small axial charge of the N(1535)-resonance
doi: 10.1140/epja/2008-10642-2
2008LI16 Phys.Rev. C 77, 045207 (2008) Sea-quark effects in the pion charge form factor
doi: 10.1103/PhysRevC.77.045207
2007LI57 Nucl.Phys. A791, 406 (2007) The role of 5-quark components on the nucleon form factors
doi: 10.1016/j.nuclphysa.2007.05.002
2007RI16 Eur.Phys.J. A 32, 389 (2007) Quark model analysis of strangeness form factors of the proton
doi: 10.1140/epja/i2006-10399-6
2006AC06 Phys.Rev. C 74, 025203 (2006) A.Acus, E.Norvaisas, D.O.Riska The α particle as a canonically quantized multiskyrmion NUCLEAR STRUCTURE 4He; calculated binding energy, charge radius, electric form factors. Skyrme model, rational map approximation.
doi: 10.1103/PhysRevC.74.025203
2006AN09 Phys.Rev. C 73, 035207 (2006) Strangeness spin, magnetic moment, and strangeness configurations of the proton NUCLEAR STRUCTURE 1H; calculated quark configurations, strange quark contributions, strangeness magnetic moment.
doi: 10.1103/PhysRevC.73.035207
2006AN30 Phys.Rev. C 74, 055205 (2006); Erratum Phys.Rev. C 75, 069901 (2007) C.S.An, Q.B.Li, D.O.Riska, B.S.Zou The qqqq(q-bar) components and hidden flavor contributions to the baryon magnetic moments
doi: 10.1103/PhysRevC.74.055205
2006JU04 Nucl.Phys. A780, 175 (2006) The role of qqqq(q-bar) components in the nucleon and the N(1440) resonance
doi: 10.1016/j.nuclphysa.2006.09.016
2006LI06 Nucl.Phys. A766, 172 (2006) The role of five-quark components in gamma decay of the Δ(1232)
doi: 10.1016/j.nuclphysa.2005.11.020
2006LI12 Phys.Rev. C 73, 035201 (2006) Five-quark components in Δ(1232) → N π decay
doi: 10.1103/PhysRevC.73.035201
2006LI33 Phys.Rev. C 74, 015202 (2006) Role of q(q-bar) components in the N(1440) resonance
doi: 10.1103/PhysRevC.74.015202
2006RI07 Phys.Lett. B 636, 265 (2006) The strangeness form factors of the proton NUCLEAR STRUCTURE 1H; calculated quark configurations, strange magnetic moment and radii, strangeness form factors.
doi: 10.1016/j.physletb.2006.03.065
2005FR05 Nucl.Phys. A750, 337 (2005) F.Fromel, B.Julia-Diaz, D.O.Riska Bound states of heavy flavor hyperons
doi: 10.1016/j.nuclphysa.2005.01.022
2005JU07 Nucl.Phys. A755, 431c (2005) Nuclei of Double-Charm Hyperons
doi: 10.1016/j.nuclphysa.2005.03.050
2005JU10 Nucl.Phys. A757, 441 (2005) D-state configurations in the electromagnetic form factors of the nucleon and the Δ(1232) resonance NUCLEAR STRUCTURE 1n, 1H; calculated electromagnetic form factors, Δ-N form factors, effect of D-state admixtures.
doi: 10.1016/j.nuclphysa.2005.04.008
2005ZO02 Phys.Rev.Lett. 95, 072001 (2005) s(s-bar) Component of the Proton and the Strangeness Magnetic Moment NUCLEAR STRUCTURE 1H; analyzed strangeness magnetic moment; deduced quark configurations.
doi: 10.1103/PhysRevLett.95.072001
2004AC05 Phys.Scr. 69, 260 (2004) A.Acus, J.Matuzas, E.Norvaisas, D.O.Riska The Deuteron as a Canonically Quantized Biskyrmion NUCLEAR STRUCTURE 2H; calculated binding energy, radii, quadrupole moment, form factor. Topological soliton model.
doi: 10.1238/Physica.Regular.069a00260
2004JU02 Phys.Rev. C 69, 035212 (2004); Erratum Phys.Rev. C 75, 069902 (2007) B.Julia-Diaz, D.O.Riska, F.Coester Baryon form factors of relativistic constituent-quark models NUCLEAR STRUCTURE 1n, 1H; calculated electromagnetic and axial form factors. Constituent-quark models.
2004JU04 Nucl.Phys. A739, 69 (2004) Baryon magnetic moments in relativistic quark models
doi: 10.1016/j.nuclphysa.2004.03.078
2004JU07 Phys.Rev. C 70, 045204 (2004) B.Julia-Diaz, D.O.Riska, F.Coester Axial transition form factors and pion decay of baryon resonances
doi: 10.1103/PhysRevC.70.045204
2003CO19 Nucl.Phys. A728, 439 (2003) Scaling of hadronic form factors in point form kinematics NUCLEAR STRUCTURE 1H; calculated electric and magnetic form factors. Point form kinematics.
doi: 10.1016/j.nuclphysa.2003.09.003
2003RI06 Eur.Phys.J. A 17, 297 (2003) Nucleon structure vs. theoretical models
doi: 10.1140/epja/i2002-10170-1
2003RI12 Eur.Phys.J. A 18, 201 (2003) Nuclear forces and currents in large-Nc QCD
doi: 10.1140/epja/i2002-10299-9
2002HE04 Nucl.Phys. A699, 624 (2002) Low-Lying qqqq(q-bar) States in the Baryon Spectrum
doi: 10.1016/S0375-9474(01)01294-5
2002LA17 Nucl.Phys. A707, 425 (2002) Pion Rescattering in Two-Pion Decay of Heavy Quarkonia
doi: 10.1016/S0375-9474(02)00964-8
2002LA22 Nucl.Phys. A710, 99 (2002) The coupling of η mesons to quarks and baryons from DS* → DSπ0 decay
doi: 10.1016/S0375-9474(02)01125-9
2002RI02 Nucl.Phys. A699, 234c (2002) Quark and Gluon Dynamics from Heavy Meson Spectroscopy
doi: 10.1016/S0375-9474(01)01498-1
2002RI10 Nucl.Phys. A710, 55 (2002) Dynamical interpretation of the nucleon-nucleon interaction and exchange currents in the large NC limit
doi: 10.1016/S0375-9474(02)01091-6
2001AC02 Phys.Scr. 64, 113 (2001) A.Acus, E.Norvaisas, D.O.Riska Nucleon Form Factors in the Canonically Quantized Skyrme Model NUCLEAR STRUCTURE 1n, 1H; calculated electric, magnetic, axial and induced pseudoscalar form factors. Canonically quantized Skyrme model, comparisons with data.
doi: 10.1238/Physica.Regular.064a00113
2001GL03 Nucl.Phys. A684, 287c (2001) Pion Loop Fluctuations of Constituent Quarks and Baryons
doi: 10.1016/S0375-9474(01)00423-7
2001HE06 Nucl.Phys. A686, 355 (2001) K.O.E.Henriksson, T.A.Lahde, C.J.Nyfalt, D.O.Riska Pion Decay Widths of D Mesons
doi: 10.1016/S0375-9474(00)00522-4
2001LA20 Nucl.Phys. A693, 755 (2001) Two-Pion Decay Widths of Excited Charm Mesons
doi: 10.1016/S0375-9474(01)00917-4
2001PE03 Nucl.Phys. A683, 322 (2001) M.T.Pena, H.Garcilazo, D.O.Riska The Reaction pp → ppη and the eta-Nucleon and Nucleon-Nucleon Interactions NUCLEAR REACTIONS 1H(p, pX), E=1260-1340 MeV; calculated η meson production σ, meson exchange contributions; deduced coupling constant. Comparison with data.
doi: 10.1016/S0375-9474(00)00449-8
2001RI03 Nucl.Phys. A679, 577 (2001) Nucleon Resonance Transition Couplings to Vector Mesons
doi: 10.1016/S0375-9474(00)00362-6
2001RI10 Nucl.Phys. A689, 3c (2001) Currents, Interactions and the Nuclear Few-Body Systems
doi: 10.1016/S0375-9474(01)00813-2
2000HA10 Nucl.Phys. A665, 353 (2000) L.Hannelius, D.O.Riska, L.Ya.Glozman The Strangeness Magnetic Moment of the Proton in the Chiral Quark Model NUCLEAR STRUCTURE 1H; calculated the strangeness magnetic moment. Comparison with experimental value.
doi: 10.1016/S0375-9474(99)00812-X
2000HA51 Phys.Rev. C62, 045204 (2000) Strangeness Form Factors of the Proton in the Chiral Quark Model
doi: 10.1103/PhysRevC.62.045204
2000LA22 Nucl.Phys. A674, 141 (2000) T.A.Lahde, C.J.Nyfalt, D.O.Riska Spectra and M1 Decay Widths of Heavy-Light Mesons
doi: 10.1016/S0375-9474(00)00154-8
2000RI05 Nucl.Phys. A663-664, 663c (2000) D.O.Riska, T.A.Lahde, C.J.Nyfalt The Confining Interaction and the M1 Decay Rates of Heavy Quarkonia
doi: 10.1016/S0375-9474(99)00809-X
2000RI17 Nucl.Phys. A678, 79 (2000) Mesonic Anapole Form Factors of the Nucleons NUCLEAR STRUCTURE 1n, 1H; calculated anapole form factors.
doi: 10.1016/S0375-9474(00)00315-8
1999GL03 Phys.Lett. 459B, 49 (1999) Pionic Fluctuations of Constituent Quarks and the Neutron Charge Radius NUCLEAR STRUCTURE 1n; calculated contributions to charge radius.
doi: 10.1016/S0370-2693(99)00718-2
1999LA01 Nucl.Phys. A645, 587 (1999); Erratum Nucl.Phys. A665, 447 (2000) T.A.Lahde, C.J.Nyfalt, D.O.Riska The Confining Interaction and Radiative Decays of Heavy Quarkonia
doi: 10.1016/S0375-9474(98)00620-4
1999PE16 Phys.Rev. C60, 045201 (1999) M.T.Pena, D.O.Riska, A.Stadler Nucleon Resonance Effects in pp → ppπ0 Near Threshold NUCLEAR REACTIONS 1H(p, pπ0), E=280-320 MeV; calculated σ; deduced resonance contributions. Comparisons with data.
doi: 10.1103/PhysRevC.60.045201
1999RI09 Nucl.Phys. A653, 251 (1999) Two-Pion Exchange Interaction between Constituent Quarks
doi: 10.1016/S0375-9474(99)00260-2
1998AC03 Phys.Rev. C57, 2597 (1998) A.Acus, E.Norvaisas, D.O.Riska Stability and Representation Dependence of the Quantum Skyrmion
doi: 10.1103/PhysRevC.57.2597
1998CO15 Nucl.Phys. A634, 335 (1998) F.Coester, K.Dannbom, D.O.Riska Convariant Quark Model for the Baryons
doi: 10.1016/S0375-9474(98)00142-0
1998CO41 Few-Body Systems 25, 29 (1998) Poincare-Convariant Quark Models of Baryon Form Factors NUCLEAR STRUCTURE 1n, 1H; calculated wavefunctions, form factors, helicity amplitudes for resonance transitions, related features. Poincare-invariant quark model.
doi: 10.1007/s006010050092
1998HE31 Phys.Rev. C58, 2928 (1998) π-Gluon Exchange Interaction between Constituent Quarks
doi: 10.1103/PhysRevC.58.2928
1998MA78 Phys.Rev. C58, 3069 (1998) L.E.Marcucci, D.O.Riska, R.Schiavilla Electromagnetic Structure of Trinucleons NUCLEAR STRUCTURE 3H, 3He; calculated charge, magnetic form factors; deduced contributions. Argonne v18 two-nucleon and Urbana IX three-nucleon interactions. Comparison with data.
doi: 10.1103/PhysRevC.58.3069
1998RI09 Acta Phys.Pol. B29, 2389 (1998) The Interaction between Constituent Quarks
1998SC46 Phys.Lett. 444B, 21 (1998) η-4He Bound States in the Skyrme Model NUCLEAR STRUCTURE 4He; calulated η-nucleus resonance features; deduced bound state. Skyrme model, rational map ansatz.
doi: 10.1016/S0370-2693(98)01370-7
1997AC01 Nucl.Phys. A614, 361 (1997) A.Acus, E.Norvaisas, D.O.Riska The Quantum Skyrmion in Representations of General Dimension NUCLEAR STRUCTURE 1H, 1n; calculated μ. Quantum Skyrme model.
doi: 10.1016/S0375-9474(96)00456-3
1997AM07 Nucl.Phys. A622, 315c (1997) C.Amsler, T.Bressani, F.E.Close, E.De Sanctis, B.Frois, D.von Harrach, F.Kunne, J.M.Laget, V.Metag, P.J.Mulders, D.O.Riska Perspective in Hadron and Quark Dynamics NUCLEAR REACTIONS 208Pb(e, e'p), 12C, 16O(e, e'X), 12C(γ, X), E not given; compiled, reviewed data, analyses. Reviewed available accelerator facilities.
doi: 10.1016/S0375-9474(97)00348-5
1997DA05 Nucl.Phys. A616, 555 (1997) K.Dannbom, L.Ya.Glozman, C.Helminen, D.O.Riska Baryon Magnetic Moments and Axial Coupling Constants with Relativistic and Exchange Current Effects NUCLEAR STRUCTURE 1H, 1n; calculated μ. Relativistic, exchange current effects.
doi: 10.1016/S0375-9474(97)00005-5
1996GL02 Nucl.Phys. A603, 326 (1996); Erratum Nucl.Phys. A620, 510 (1997) The Charm and Bottom Hyperons in a Chiral Quark Model
doi: 10.1016/0375-9474(96)80005-C
1996GL03 Phys.Rep. 268, 263 (1996) The Spectrum of the Nucleons and the Strange Hyperons and Chiral Dynamics
doi: 10.1016/0370-1573(95)00062-3
1996RI10 Nucl.Phys. A606, 251 (1996) The Long Road to Short Range Exchange Currents
doi: 10.1016/0375-9474(96)00208-4
1996VA18 Phys.Lett. 388B, 679 (1996) U.van Kolck, G.A.Miller, D.O.Riska Meson Exchange and Pion Rescattering Contributions to the Cross Section for pp → ppπ0 NUCLEAR REACTIONS 1H(p, pπ0), E not given; analyzed σ. Meson exchange and pion rescattering included.
doi: 10.1016/S0370-2693(96)01225-7
1995BJ01 Nucl.Phys. A582, 621 (1995) M.Bjornberg, K.Dannbom, D.O.Riska The Anharmonic Correction in the Soliton Model of the Hyperons
doi: 10.1016/0375-9474(94)00473-Z
1995CO27 Phys.Rev. C52, 2925 (1995) Repulsive Short-Range Three-Nucleon Interaction
doi: 10.1103/PhysRevC.52.2925
1995KI17 Nucl.Phys. A594, 419 (1995) The Coupling of the f1(1285) Meson to the Isoscalar Axial Current of the Nucleon
doi: 10.1016/0375-9474(95)00357-7
1994CO24 Ann.Phys.(New York) 234, 141 (1994) Electromagnetic Currents and the Blankenbecler-Sugar Equation
doi: 10.1006/aphy.1994.1076
1994GO04 Nucl.Phys. A568, 779 (1994); Erratum Nucl.Phys. A577, 832 (1994) Electromagnetic Properties of Predicted Bound States of Heavy Quarkonia and Nucleons
doi: 10.1016/0375-9474(94)90359-X
1994GU01 Nucl.Phys. A571, 645 (1994) Bag Structure of the Infinite Order Skyrmion
doi: 10.1016/0375-9474(94)90714-5
1994KI15 Nucl.Phys. A578, 511 (1994) The Effective Induced Pseudoscalar Coupling Constant NUCLEAR STRUCTURE 40Ca; calculated weak-coupling parameters in-medium renormalizations.
doi: 10.1016/0375-9474(94)90758-7
1994KI18 Phys.Rev. C50, 2703 (1994) L.L.Kiang, T.-S.H.Lee, D.O.Riska Two-Body Pion Absorption on 3He at Threshold NUCLEAR REACTIONS 3He(π-, nn), (π-, np), E at rest; calculated pion absorption probabilities ratio. Realistic NN- interaction, axial charge operator short range two-nucleon components effect.
doi: 10.1103/PhysRevC.50.2703
1994NO11 Phys.Scr. 50, 634 (1994) Representations of General Dimension for the Skyrme Model
doi: 10.1088/0031-8949/50/6/006
1994TS01 Phys.Lett. 333B, 17 (1994) The πσ-Axial Exchange Current
doi: 10.1016/0370-2693(94)91001-4
1993LE04 Phys.Rev.Lett. 70, 2237 (1993) Short Range Exchange Contributions to the Cross Section for pp → ppπ0 Near Threshold NUCLEAR REACTIONS 1H(p, pπ0), E=280-310 MeV; calculated σ(E); deduced NN-interaction short range components features. Bonn, Paris potentials.
doi: 10.1103/PhysRevLett.70.2237
1992BL03 Nucl.Phys. A536, 697 (1992) The Isoscalar Electromagnetic Current Operator and the Nucleon-Nucleon Interaction NUCLEAR STRUCTURE 2H; calculated structure function, magnetic form factor. Exchange currents.
doi: 10.1016/0375-9474(92)90119-5
1992GO11 Nucl.Phys. A547, 633 (1992) Mean Square Radii of Hyperons in the Bound-State Soliton Model NUCLEAR STRUCTURE 1n, 1H; calculated electric, magnetic mean square radii. Bound state soliton model.
doi: 10.1016/0375-9474(92)90655-4
1991CA16 Phys.Rev. C44, 619 (1991) J.Carlson, D.O.Riska, R.Schiavilla, R.B.Wiringa Weak Proton Capture Reactions on 1H and 3He and Tritium β Decay NUCLEAR REACTIONS 3He, 1H(p, e+ν), E=low; calculated weak capture σ; deduced exchange contribution role. Realistic wave function.
doi: 10.1103/PhysRevC.44.619
1991SC01 Phys.Rev. C43, 437 (1991) Threshold Electrodisintegration and Electromagnetic Form Factors of the Deuteron NUCLEAR REACTIONS 2H(e, X), E=threshold; calculated disintegration σ vs momentum transfer square. NUCLEAR STRUCTURE 2H; calculated electromagnetic form factors, tensor polarization. Electron scattering data input.
doi: 10.1103/PhysRevC.43.437
1990CA28 Phys.Rev. C42, 830 (1990) J.Carlson, D.O.Riska, R.Schiavilla, R.B.Wiringa Radiative Neutron Capture on 3He NUCLEAR REACTIONS 3He(n, γ), E=thermal; calculated σ; deduced scattering length dependence. Monte Carlo variational methods.
doi: 10.1103/PhysRevC.42.830
1990KI06 Nucl.Phys. A511, 592 (1990) M.Kirchbach, R.Mach, D.O.Riska The Axial Charge Sum Rule for Complex Nuclei NUCLEAR STRUCTURE 15C, 15N; calculated one-body transition density for states; deduced effective axial charge form factor features.
doi: 10.1016/0375-9474(90)90112-Y
1990SC01 Phys.Rev. C41, 309 (1990) R.Schiavilla, V.R.Pandharipande, D.O.Riska Charge Form Factors of the Three- and Four-Body Nuclei NUCLEAR STRUCTURE 3H, 3,4He; calculated charge form factors. Monte Carlo, variational procedures.
doi: 10.1103/PhysRevC.41.309
1990SC25 Phys.Lett. 244B, 373 (1990) Isovector Magnetic Structure of the Two- and Three-Nucleon Systems NUCLEAR REACTIONS 2H(e, e'p), E not given; calculated σ(θ(e'), E(e')) vs energy transfer. Realistic interactions. NUCLEAR STRUCTURE 3H, 3He; calculated magnetic form factors. Realistic interactions.
doi: 10.1016/0370-2693(90)90331-Y
1989SC27 Phys.Rev. C40, 2294 (1989) R.Schiavilla, V.R.Pandharipande, D.O.Riska Magnetic Form Factors of the Trinucleons NUCLEAR STRUCTURE 3H, 3He; calculated magnetic form factors; deduced giant dipole sum rule enhancement factor, mesonic contribution to orbital g-factor. Monte Carlo techniques, two-, three-nucleon interactions.
doi: 10.1103/PhysRevC.40.2294
1988NY01 Phys.Lett. 211B, 6 (1988) Exchange Currents in Pion-Induced Deuteron Breakup NUCLEAR REACTIONS 2H(π-, π-n), E ≈ breakup threshold; calculated form factor. Exchange currents.
doi: 10.1016/0370-2693(88)90796-4
1987NY01 Nucl.Phys. A468, 473 (1987) Deuteron Form Factors in the Topological Soliton Approach NUCLEAR STRUCTURE 1n, 1,2H; calculated magnetic form factors. Soliton model.
doi: 10.1016/0375-9474(87)90179-5
1986NY03 Nucl.Phys. A454, 498 (1986) Static Electromagnetic Properties of the Deuteron in the Skyrme Model. NUCLEAR STRUCTURE 2H; calculated rms radius, μ, electric quadrupole moment. Skyrme model.
doi: 10.1016/0375-9474(86)90101-6
1986NY04 Phys.Rev.Lett. 57, 3007 (1986) Topological-Exchange-Current Contribution to the Deuteron Magnetic Form Factor NUCLEAR STRUCTURE 2H; calculated magnetic form factor; deduced exchange current contribution. Chiral soliton Skyrme model.
doi: 10.1103/PhysRevLett.57.3007
1985RI03 Phys.Scr. 31, 107 (1985) The Magnetic Exchange Current and the Spin-Orbit Interaction NUCLEAR STRUCTURE A=15, 17, 39, 41; calculated magnetic moment combinations. 2H; calculated magnetic form factor.
doi: 10.1088/0031-8949/31/2/003
1985RI06 Phys.Scr. 31, 471 (1985) Isovector Electromagnetic Exchange Currents and the Nucleon-Nucleon Interaction NUCLEAR REACTIONS 2H(e, e'n), E(cm)=1.5 MeV; calculated breakup σ(θ) vs momentum. Projected isovector electromagnetic exchange currents from nucleon-nucleon interaction.
doi: 10.1088/0031-8949/31/6/007
1985RI12 Phys.Scr. 32, 581 (1985) Velocity Dependence and Nuclear Magnetic Structure NUCLEAR STRUCTURE 2H; calculated magnetic form factor; deduced velocity dependent interaction characteristics.
doi: 10.1088/0031-8949/32/6/004
1983MA70 Phys.Lett. 133B, 23 (1983) The Nucleon Anomalous Magnetic Moment and Meson Exchange Current Operators NUCLEAR REACTIONS 2H(e, e'), E=280, 410 MeV; calculated electrodisintegration σ vs momentum transfer squared; deduced nucleon anomalous magnetic moment correction role in meson exchange operators.
doi: 10.1016/0370-2693(83)90097-7
1983RI07 Nucl.Phys. A399, 406 (1983) Medium Polarization and Short-Range Effects in the Meson Exchange Charge Operator NUCLEAR STRUCTURE 4He, 16O, 40Ca; calculated charge form factor. Medium polarization, short range effects.
doi: 10.1016/0375-9474(83)90255-5
1980CH09 Nucl.Phys. A338, 349 (1980) On the Reactions pp → dπ+ NUCLEAR REACTIONS 2H(π+, p), E < 1 GeV; calculated total σ. 1H(polarized p, π+), E < 1 GeV; calculated σ(θ), asymmetry parameters; deduced sensitivity to nucleon-nucleon interaction.
doi: 10.1016/0375-9474(80)90037-8
1980RI04 Nucl.Phys. A350, 227 (1980) The Magnetic Form Factor of 3He NUCLEAR STRUCTURE 3He; calculated magnetic form factors; deduced short range correlations. 3He deduced D-state percentage. Simple wave function models, pion, ρ-meson exchange effects.
doi: 10.1016/0375-9474(80)90457-1
1978NE03 Phys.Rev.Lett. 40, 1005 (1978) Pion-Exchange Contributions to Charge Densities of Closed-Shell Nuclei NUCLEAR STRUCTURE 12C, 16O, 40,48Ca, 90Zr, 208Pb; calculated nuclear matrix elements.
doi: 10.1103/PhysRevLett.40.1005
1977BR29 Nucl.Phys. A287, 425 (1977) Pionic Disintegration of the Deuteron NUCLEAR REACTIONS 2H(π, X); calculated reaction parameters.
doi: 10.1016/0375-9474(77)90055-0
1977RI15 Phys.Rev. C16, 2105 (1977) Many-Body Exchange Currents and the Tri- and Four-Nucleon Charge Form Factors NUCLEAR REACTIONS 3H, 3,4He(e, e); calculated charge form factors, 2-, 3-, 4-body meson-exchange operators.
doi: 10.1103/PhysRevC.16.2105
1976DA11 Nucl.Phys. A264, 507 (1976) Weak Interactions in Deuterons: Exchange Currents and Nucleon-Nucleon Interaction NUCLEAR REACTIONS 1H(p, π+d); calculated interaction.
doi: 10.1016/0375-9474(76)90420-6
1976RA34 Nucl.Phys. A274, 428 (1976) Pion Exchange Currents and Nuclear Charge Form Factors NUCLEAR STRUCTURE 16O, 40Ca; calculated form factors, charge density.
doi: 10.1016/0375-9474(76)90211-6
1976RI02 Phys.Lett. 61B, 41 (1976) Pionic Disintegration of the Deuteron NUCLEAR REACTIONS 2H(π+, 2p); calculated pionic disintegration of deuteron, σ.
doi: 10.1016/0370-2693(76)90556-6
1976RI03 Phys.Rev. C13, 1324 (1976) Comment on Observation of Two-Photon Decay in n-p Capture NUCLEAR REACTIONS 1H(n, γ); analyzed wave functions.
doi: 10.1103/PhysRevC.13.1324
1972RI02 Phys.Lett. 38B, 193 (1972) Meson Exchange Effects in n + p → d + γ NUCLEAR REACTIONS 1H(n, γ), E approx threshold; calculated exchange current corrections.
doi: 10.1016/0370-2693(72)90376-0
1972RI09 Phys.Lett. 40B, 177 (1972) Two-Pion Exchange LAMBDAN Potential
doi: 10.1016/0370-2693(72)90402-9
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