NSR Query Results
Output year order : Descending NSR database version of May 2, 2024. Search: Author = R.Wunsch Found 12 matches. 1998SC03 Int.J.Mod.Phys. E7, 121 (1998) M.Schleif, R.Wunsch, T.Meissner Self-Consistent Pushing and Cranking Corrections to the Meson Fields of the Chiral Quark-Loop Soliton
doi: 10.1142/S0218301398000063
1998SC05 Eur.Phys.J. A 1, 171 (1998) Thermodynamic Properties of the SU(2)(f) Chiral Quark-Loop Soliton
doi: 10.1007/s100500050046
1994WU04 Z.Phys. A348, 111 (1994) R.Wunsch, K.Goeke, Th.Meissner On Size and Shape of the Average Meson Fields in the Semibosonized Nambu and Jona-Lasinio Model
1992WU08 Czech.J.Phys. B42, 1061 (1992) Unified Description of Quasi-Free and Resonant Processes of Hypernuclear Production and Decay NUCLEAR REACTIONS 28Si(π+, K+), 12C(K+, π+), E at 1050 MeV/c; 12C(K-, π-), E at 800 MeV/c; 16O(K-, π+), E at 450 MeV/c; 14N(K-, π-), E not given; compiled, reviewed data, analyses; deduced hypernuclear disintegration mechanism.
1988MO23 Phys.Rev. C38, 1322 (1988) T.Motoba, H.Bando, R.Wunsch, J.Zofka Hypernuclear Production by the (π+, K+) Reaction NUCLEAR REACTIONS 12C, 16O, 28Si, 40Ca, 56Fe, 90Zr, 208Pb(π+, K+), E at 1040 MeV/c; calculated σ(θ), strength function; deduced effects of resonance and quasifree processes. Kapur-Peierls method, continuum shell model, DWIA analyses.
doi: 10.1103/PhysRevC.38.1322
1987WU05 Phys.Lett. 193B, 7 (1987) Resonant and Quasi-Free Mechanisms of Sigma Production on Nuclei NUCLEAR REACTIONS 12C, 16O(K-, π+), E=450 MeV/c; calculated effective nucleon number vs hypernuclear binding energy. Continuum shell model.
doi: 10.1016/0370-2693(87)90447-3
1984KA28 Nucl.Phys. A426, 301 (1984) The Unified Description of Direct and Resonant Processes in the Inelastic Scattering of Medium-Energy Projectiles on 40Ca NUCLEAR REACTIONS 40Ca(e, e'), (e, e'p), E not given; calculated longitudinal form factors, angular correlation functions. 40Ca(α, α'), (α, α'p), (α, α'n), E=129.4 MeV; calculated isoscalar form factor. NUCLEAR STRUCTURE 40Ca; calculated levels, reduced B(λ), EWSR. Shell model, 1p-1h approximation, continuum effects.
doi: 10.1016/0375-9474(84)90110-6
1984WU05 J.Phys.(London) G10, 1361 (1984) On the Role of Complicated Shell-Model Configurations in the Description of Radiative Pion Capture on 16O NUCLEAR REACTIONS 16O(π-, γ), E at rest; calculated σ(Eγ). Many particle-many hole basis, renormalization effects. NUCLEAR STRUCTURE 16O; calculated wave function, radiative pion capture rate. Renormalization effects, many particle-many hole basis.
doi: 10.1088/0305-4616/10/10/008
1982BA17 Czech.J.Phys. B32, 335 (1982) The Description of Hypernuclei in the Continuum Shell-Model NUCLEAR REACTIONS 12C(K-, π-), E at 800 MeV/c; 16O(K-, π-), E at 715 MeV/c; calculated σ(θ). Continuum shell model.
doi: 10.1007/BF01602082
1980WU01 Nucl.Phys. A336, 446 (1980) Radiative Pion Capture within the Unified Theory of Direct and Resonance Reactions NUCLEAR REACTIONS 16O(π-, γ), (π-, nγ), E at rest; calculated σ(Eγ), σ(En), γn(θ). Continuum shell model.
doi: 10.1016/0375-9474(80)90221-3
1978BA55 J.Phys.(London) G4, L239 (1978) Unified Description of Direct and Resonance Processes in the (π-, γ) Reaction NUCLEAR REACTIONS 16O(π-, nγ), (π-, γ); calculated σ(Eγ), nγ(θ).
doi: 10.1088/0305-4616/4/2/013
1975RO31 Fiz.Elem.Chastits At.Yadra 6, 435 (1975); Sov.J.Particles Nucl. 6, 175 (1976) I.Rotter, H.W.Barz, R.Wunsch, J.Hohn Coupled-Channels Method of Calculations in the Shell Model with Allowance for the Continuous Spectrum NUCLEAR REACTIONS 15N(n, n), E=13-17 MeV; 15N(p, n), E=7.5-8.5 MeV; 16O(μ-, X); calculated σ.
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