NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = B.Blankleider Found 25 matches. 2021BL08 Few-Body Systems 62, 87 (2021) B.Blankleider, S.S.Kumar, A.N.Kvinikhidze Effect of Nucleon Dressing on Triton Binding Energy NUCLEAR STRUCTURE 3H; calculated triton binding energy shifts due to nucleon dressing, nucleon dressing model parameters.
doi: 10.1007/s00601-021-01676-3
2019SK01 Phys.Rev. C 99, 034001 (2019) T.Skawronski, B.Blankleider, A.N.Kvinikhidze Electromagnetic currents of the pion-nucleon system
doi: 10.1103/PhysRevC.99.034001
2009KV02 Phys.Rev. C 80, 044004 (2009) A.N.Kvinikhidze, B.Blankleider, E.Epelbaum, C.Hanhart, M.Pavon Valderrama Gauge invariance in the presence of a cutoff
doi: 10.1103/PhysRevC.80.044004
2007KV01 Nucl.Phys. A784, 259 (2007) A.N.Kvinikhidze, B.Blankleider Generalized parton distributions for dynamical equation models
doi: 10.1016/j.nuclphysa.2006.11.161
2007KV06 Phys.Rev. C 76, 064003 (2007) A.N.Kvinikhidze, B.Blankleider Wilsonian renormalization group equation for nuclear current operators
doi: 10.1103/PhysRevC.76.064003
2005KV01 Phys.Rev. C 72, 054001 (2005) A.N.Kvinikhidze, B.Blankleider Three-body problem at finite temperature and density
doi: 10.1103/PhysRevC.72.054001
2002KV02 Phys.Rev. C66, 045203 (2002) A.N.Kvinikhidze, M.C.Birse, B.Blankleider Pionic dressing of baryons in chiral quark models
doi: 10.1103/PhysRevC.66.045203
2000KV02 Nucl.Phys. A670, 210c (2000) A.N.Kvinikhidze, B.Blankleider Complete Set of Electromagnetic Corrections to the Nucleon Mass in the Nambu-Jona-Lasinio Model
doi: 10.1016/S0375-9474(00)00101-9
1999KV01 Phys.Rev. C59, 1263 (1999) A.N.Kvinikhidze, B.Blankleider Unified Relativistic Description of πNN and γπNN
doi: 10.1103/PhysRevC.59.1263
1999KV02 Phys.Rev. C60, 044003 (1999) A.N.Kvinikhidze, B.Blankleider Gauging of Equations Method. I. Electromagnetic Currents of Three Distinguishable Particles
doi: 10.1103/PhysRevC.60.044003
1999KV03 Phys.Rev. C60, 044004 (1999) A.N.Kvinikhidze, B.Blankleider Gauging of Equations Method. II. Electromagnetic Currents of Three Identical Particles
doi: 10.1103/PhysRevC.60.044004
1998KV01 Nucl.Phys. A631, 559c (1998) A.N.Kvinikhidze, B.Blankleider Gauging Hadronic Systems
doi: 10.1016/S0375-9474(98)00067-0
1997KV01 Phys.Rev. C56, 2963 (1997) A.N.Kvinikhidze, B.Blankleider Gauging the Spectator Equations
doi: 10.1103/PhysRevC.56.2963
1997KV02 Phys.Rev. C56, 2973 (1997) A.N.Kvinikhidze, B.Blankleider Gauging the Three-Nucleon Spectator Equation
doi: 10.1103/PhysRevC.56.2973
1995WE05 Phys.Rev. C51, 2575 (1995) M.Wessler, E.Boschitz, B.Brinkmoller, J.Buhler, H.Garcilazo, W.Gyles, W.List, R.Meier, S.Ritt, R.Tacik, J.A.Konter, D.Gill, S.Mango, D.Renker, B.van den Brandt, G.Wait, V.A.Efimovykh, A.I.Kovalev, A.N.Prokofiev, W.Thiel, B.Blankleider Polarization Observables in πd(pol) Elastic Scattering: Analyzing powers τ22 and iT11 in the Forward Hemisphere NUCLEAR REACTIONS 2H(π+, π+), E=100-294 MeV; measured analyzing powers, other observables. Polarized target, two different methods. Model comparison.
doi: 10.1103/PhysRevC.51.2575
1994KV01 Nucl.Phys. A574, 788 (1994) A.N.Kvinikhidze, B.Blankleider Covariant Three-Body Equations in φ3 Field Theory
doi: 10.1016/0375-9474(94)90959-8
1990AL21 Phys.Rev. C42, 517 (1990) Effects of Short Range ΔN Interaction on Observables of the πNN System NUCLEAR REACTIONS 2H(π, π), E=140-256 MeV; calculated σ(θ), iT11(θ). 1H(p, π+), (polarized p, π+), E=567-800 MeV; calculated σ(θ), analyzing power vs θ; deduced nucleon-isobar interaction role. Polarized, unpolarized targets.
doi: 10.1103/PhysRevC.42.517
1990NO01 Phys.Rev. C41, 213 (1990) S.Nozawa, T.-S.H.Lee, B.Blankleider Neutral Pion Photoproduction on the Nucleon Near Threshold NUCLEAR REACTIONS 1H(γ, π0), E=145-160 MeV; calculated σ(E); deduced final state interaction role. Dynamical model.
doi: 10.1103/PhysRevC.41.213
1990NO03 Nucl.Phys. A508, 355c (1990) S.Nozawa, T.-S.H.Lee, B.Blankleider Neutral Pion Photoproduction of the Nucleon Near Threshold NUCLEAR REACTIONS 1H(γ, π0), (γ, π+), (γ, π-), E at threshold; calculated amplitudes; deduced π0 production mechanism. Dynamical model.
doi: 10.1016/0375-9474(90)90497-A
1990NO05 Nucl.Phys. A513, 459 (1990) S.Nozawa, B.Blankleider, T.-S.H.Lee A Dynamical Model of Pion Photoproduction on the Nucleon NUCLEAR REACTIONS 1n(γ, π-), 1H(γ, π+), (γ, π0), E=180-450 MeV; calculated σ(θ), recoil nucleon asymmetries. Dynamical model.
doi: 10.1016/0375-9474(90)90395-3
1987BL03 Nucl.Phys. A463, 77c (1987) Few Body Physics at SIN NUCLEAR REACTIONS 2H(π, π), E=100-400 MeV; compiled, analyzed σ(E, θ), tensor polarization; 2H(π+, π+p), E=294 MeV; compiled, analyzed σ(Ep, θp, θπ); 3He(π+, γ), (π-, γ), E=120 MeV; compiled, analyzed σ(θ).
doi: 10.1016/0375-9474(87)90649-X
1985BL08 Phys.Rev. C31, 1380 (1985) Relatioship between Partial Wave Amplitudes and Polarization Observables in pp → dπ+ and πd → πd NUCLEAR REACTIONS 1H(polarized p, π+), E=567, 383, 800 MeV; calculated σ(θ), polarization transfer, correlation observables vs θ; deduced relation to partial wave amplitudes. Orthogonal function expansion.
doi: 10.1103/PhysRevC.31.1380
1984BL02 Phys.Rev. C29, 538 (1984) Quasi-Elastic Scattering of Polarized Electrons on Polarized 3He NUCLEAR REACTIONS 3He(e, e'), E=0.2488, 0.3984, 0.5, 7.26 GeV; calculated σ(θ, E(e')). 3He(polarized e, e'), E=0.25-2.75 GeV; calculated σ(θ, E(e')), asymmetry vs E. Polarized target, longitudinal beam polarization, impulse approximation.
doi: 10.1103/PhysRevC.29.538
1981BL12 Phys.Rev. C24, 1572 (1981) Unified Theory of NN → πd, πd → πd, and NN → NN Reactions NUCLEAR REACTIONS 2H(π+, d), E=25-250 MeV; calculated σ(total, E); 1H(p, π+), E=382.9-799.3 MeV; calculated σ(θ); 2H(π+, π+), E=47.7 MeV; calculated σ(θ); 2H(π+, π+), E=50-350 MeV; calculated σ(total, E); 2H(π+, π+), E=140, 256 MeV; calculated iT11(θ, d), T20(θ, d). Nucleon-nucleon phase shift input, unified theory.
doi: 10.1103/PhysRevC.24.1572
1980AF01 Phys.Lett. 93B, 367 (1980) The Effect of Absorption on Low Energy π-d Scattering NUCLEAR REACTIONS 2H(π+, π+), (π+, p), E=47.7 MeV; calculated σ(θ); deduced absorption effects. 1H(p, p), E=380, 425 MeV; calculated phase shifts. Faddeev equations, channel coupling effects.
doi: 10.1016/0370-2693(80)90344-5
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