NSR Query Results
Output year order : Descending NSR database version of April 24, 2024. Search: Author = A.Marcinkowski Found 75 matches. 2005MB04 Acta Phys.Pol. B36, 3041 (2005) On multistep direct emission of one and two nucleons and the gradual absorption that follows NUCLEAR REACTIONS 93Nb(n, n'), (n, nX), E=26 MeV; 90Zr(p, nX), E=80, 120 MeV; calculated En, σ(E). 54Fe(p, pX), E=39, 62 MeV; calculated Ep, σ(E). Multistep-direct reaction theory, comparisons with data.
2004MA42 Acta Phys.Pol. B35, 767 (2004) Multistep direct processes in neutron scattering at 26 MeV NUCLEAR REACTIONS 93Nb(n, n'), (n, xn), E=26 MeV; calculated one-step and multistep direct reactions σ(En). Feshbach-Kerman-Koonin framework, comparison with data.
2004MA75 Eur.Phys.J. A 21, 287 (2004) Multistep direct emission from nucleon-induced reactions NUCLEAR REACTIONS 90Zr(p, nX), E=25, 120 MeV; 54Fe(p, pX), E=61.7 MeV; calculated En, σ(E), multistep contributions. 90Zr(p, n), E=25, 45, 80, 120 MeV; calculated integrated σ. Contribution from 1p1h unbound states discussed. Comparison with data.
doi: 10.1140/epja/i2003-10208-x
2003DE01 Nucl.Phys. A714, 75 (2003) Multistep charge-exchange reactions at energies up to 120 MeV NUCLEAR REACTIONS 90Zr(p, n), E=25, 45, 80, 120 MeV; calculated multistep-direct σ. 90Zr(p, xn), E=25, 45, 80, 120 MeV; calculated σ(En), reaction mechanism features. Comparison with data.
doi: 10.1016/S0375-9474(02)01364-7
2002DE01 Nucl.Phys. A697, 171 (2002) P.Demetriou, A.Marcinkowski, B.Marianski Multistep Processes in Charge-Exchange Reactions NUCLEAR REACTIONS 65Cu(p, n), E=27 MeV; 100Mo(p, n), E=26 MeV; calculated σ, σ(θ), neutron spectra; deduced multistep contributions. Comparisons with data.
doi: 10.1016/S0375-9474(01)01243-X
2002DE40 Nucl.Phys. A707, 354 (2002) P.Demetriou, A.Marcinkowski, B.Marianski Multistep Proton Scattering-Towards Higher Energies NUCLEAR REACTIONS 54Fe(p, p'), E=39 MeV; 54Fe(p, pX), E=29, 39, 62 MeV; calculated Ep, σ(E), multistep contributions.
doi: 10.1016/S0375-9474(02)01005-9
2002MA84 Acta Phys.Hung.N.S. 16, 35 (2002) A.Marcinkowski, P.Demetriou, B.Marianski Multistep Direct Reactions at Low Energies NUCLEAR REACTIONS 93Nb(n, n'), E=20 MeV; 65Cu(p, n), E=20 MeV; calculated En, σ(θ). Multistep direct reaction theory, comparison with data.
doi: 10.1556/APH.16.2002.1-4.5
2001DE40 Acta Phys.Pol. B32, 3003 (2001) P.Demetriou, A.Marcinkowski, B.Marianski Multistep Direct Reactions of 14 MeV Neutrons NUCLEAR REACTIONS 93Nb(n, n'), (n, xn), E=14.1 MeV; calculated σ(E), σ(θ), one-step and multi-step components. Comparisons with data.
2001MA71 Nucl.Phys. A694, 312 (2001) A.Marcinkowski, P.Demetriou, B.Marianski Cross Sections for Multistep Direct Neutron Scattering on Niobium NUCLEAR REACTIONS 93Nb(n, xn), E=20, 26 MeV; calculated σ(E), σ(θ). Multistep direct reactions, comparison with data.
doi: 10.1016/S0375-9474(01)00924-1
2000DE51 Phys.Lett. 493B, 281 (2000) P.Demetriou, A.Marcinkowski, B.Marianski Multistep Direct Reactions at Low Energies NUCLEAR REACTIONS 93Nb(n, n'), E=26 MeV; calculated σ(E); deduced multistep contributions, related reaction mechanism features. Comparison with data.
doi: 10.1016/S0370-2693(00)01169-2
1999MA40 Nucl.Phys. A653, 3 (1999) Analysis of Low-Energy Direct Reactions and the Novel One-Step Cross Section NUCLEAR REACTIONS 93Nb(n, xn), E=14, 20, 26, 32 MeV; 65Cu(p, xn), E=27 MeV; 159Tb(p, xn), E=18 MeV; analyzed σ; deduced reaction mechanism features. Sum rule analysis, new formula for one-step direct reactions.
doi: 10.1016/S0375-9474(99)00169-4
1999MA65 Acta Phys.Pol. B30, 1471 (1999) Sum Rule Analysis of Low-Energy Onestep Direct Reactions NUCLEAR REACTIONS 93Nb(n, xn), E=14, 20, 26 MeV; calculated σ. Fesbach, Kerman and Koonin direct reaction theory, sum rule analysis.
1998MA25 Nucl.Phys. A633, 446 (1998) A.Marcinkowski, B.Marianski, Z.Moroz, J.Wojtkowska, P.Demetriou Nucleon Scattering to the Continuum in Terms of the Two-Fermion Theory of Multistep Direct Reactions NUCLEAR REACTIONS 93Nb(p, xp), E=26.5 MeV; measured σ(E', θ). 93Nb(p, xp), (n, xn), E=18-26 MeV; analyzed σ(E'), σ(E', θ). Statistical multistep theory.
doi: 10.1016/S0375-9474(98)00128-6
1998MA47 Phys.Lett. 433B, 223 (1998) Are Low-Energy Direct Reactions Mainly Onestep ? NUCLEAR REACTIONS 93Nb(n, xn), E=14, 20, 25.7 MeV; analyzed σ(En); deduced one-step direct reaction contribution. Sum-rule analysis. Feshbach-Kerman-Koonin model.
doi: 10.1016/S0370-2693(98)00725-4
1997KU15 Z.Phys. A358, 69 (1997) S.Yu.Kun, A.V.Vagov, A.Marcinkowski Forward Peaking of Near Coulomb Energy Protons in (n, p) Reactions at 14.1 MeV NUCLEAR REACTIONS Ag, In, 93Nb(n, p), E=14.1 MeV; analyzed sigma(theta, Ep); deduced modified compound nucleus model parameters.
doi: 10.1007/s002180050277
1996DE01 Nucl.Phys. A596, 67 (1996) P.Demetriou, A.Marcinkowski, P.E.Hodgson A New Multistep Direct Reaction Mechanism: Collective excitations in the continuum NUCLEAR REACTIONS 56Fe, 58Ni, 90Zr, 93Nb, 208Pb, 209Bi(n, n'), E=14.1 MeV; analyzed σ(θ, En); deduced collective components role. Multi-step compound, direct mechanisms, collective excitations.
doi: 10.1016/0375-9474(95)00378-9
1996DE23 J.Phys.(London) G22, 629 (1996) P.Demetriou, P.E.Hodgson, A.Marcinkowski, Y.Watanabe A Consistent Analysis of (n, n'), (p, p'), (n, p) and (p, n) Multistep Reactions using the Feshbach-Kerman-Koonin Theory NUCLEAR REACTIONS 63,65Cu(n, p), E=14.8 MeV; 93Nb(n, p), E=14.1 MeV; 93Nb(n, n'), (p, p'), 98Mo(p, p'), E=18, 25.6 MeV; analyzed σ(θ, E). Feshbach-Kerman-Koonin multi-step reaction theory.
doi: 10.1088/0954-3899/22/5/010
1996MA46 J.Phys.(London) G22, 1219 (1996) A.Marcinkowski, P.Demetriou, P.E.Hodgson Pre-Equilibrium and Collective Reactions in Neutron Inelastic Scattering by the Rotational Nuclei 184,186W NUCLEAR REACTIONS 184W(n, n'), E=26 MeV; 186W(n, n'), E=14.1 MeV; analyzed angle integrated σ vs E(n), σ(θ).
doi: 10.1088/0954-3899/22/8/010
1995KI11 Z.Phys. A352, 137 (1995) Cross Sections for (n, p) Reaction on Zinc Isotopes in Terms of the Novel Multistep Compound Reaction Model NUCLEAR REACTIONS 64,66,67,68Zn(n, p), E ≈ 13-17 MeV; measured σ. Statistical multi-step direct, compound reaction models analysis. Activation method.
doi: 10.1007/BF01298899
1995MA47 J.Phys.(London) G21, 1089 (1995) A.Marcinkowski, P.Demetriou, P.E.Hodgson Are Pre-Equilibrium Reactions Mainly Direct ( Question ) NUCLEAR REACTIONS 49Ti, 58Fe(p, n), E=9.6, 14 MeV; 63Cu(p, n), E=14.8 MeV; 169Tm, 159Tb(p, xn), E=18 MeV; 98Mo(p, xn), (p, n), 100Mo(p, n), E=25.6 MeV; 65Cu(p, xn), E=26.7 MeV; calculated σ(θ, En); deduced preequilibrium process dominance over direct process conditions, model parameters. Multi-step, statistical direct reaction approaches.
doi: 10.1088/0954-3899/21/8/007
1995MA67 Phys.Rev. C52, 2021 (1995) A.Marcinkowski, B.Marianski, P.Demetriou, P.E.Hodgson Collective Reactions to the Continuum in Neutron Scattering by Niobium NUCLEAR REACTIONS 93Nb(n, xn), E=14-26 MeV; analyzed σ(θ, En), angle integrated σ. Combined multi-step direct, compound plus preequilibrium components.
doi: 10.1103/PhysRevC.52.2021
1994CH20 Phys.Rev. C49, R2885 (1994) M.B.Chadwick, P.G.Young, P.Oblozinsky, A.Marcinkowski Preequilibrium Spin Effects in Feshbach-Kerman-Koonin and Exciton Models and Application to High-Spin Isomer Production NUCLEAR REACTIONS 179Hf(n, xn), E=14 MeV; calculated total, preequilibrium neutron emission spectra, isomers production σ. Exciton preequilibrium, Feshbach-Kerman-Koonin models.
doi: 10.1103/PhysRevC.49.R2885
1994KI24 Acta Phys.Pol. B25, 1219 (1994) Cross Sections for (n, p) Reaction on Ruthenium Isotopes in Terms of the Novel Multistep Compound Reaction Model NUCLEAR REACTIONS 96,99,101,102,104Ru(n, p), E ≤ 20 MeV; analyzed σ(E). Multi-step direct, compound reaction model.
1994MA38 Nucl.Phys. A578, 168 (1994); Erratum Nucl.Phys. A585, 762 (1995) Gradual Absorption of Fast Neutrons in Niobium NUCLEAR REACTIONS 93Nb(n, xn), E=7-25.7 MeV; analyzed σ(θ), double differential σ data. Statistical multi-step theory.
doi: 10.1016/0375-9474(94)90974-1
1993KI13 Nucl.Phys. A559, 333 (1993) D.Kielan, A.Marcinkowski, U.Garuska Isotopic Effect in (n, p) Reaction on Ruthenium NUCLEAR REACTIONS 96,99,101,102,104Ru(n, p), E=13-16.6 MeV; measured σ(E); deduced isotope effect. Statistical multistep theory analysis.
doi: 10.1016/0375-9474(93)90157-S
1993MA33 Nucl.Phys. A561, 387 (1993) A.Marcinkowski, J.Rapaport, R.W.Finlay, C.Brient, M.Herman, M.B.Chadwick Neutron Emission Cross Sections at Low Bombarding Energies and the Novelty in Multistep Compound Reaction Model NUCLEAR REACTIONS 165Ho, 181Ta(n, xn), E=6.7, 20 MeV; measured σ(E(n), θ); deduced reaction mechanism. Modified statistical multistep model analysis.
doi: 10.1016/0375-9474(93)90018-S
1992HO06 Z.Phys. A342, 283 (1992) H.M.Hoang, U.Garuska, D.Kielan, A.Marcinkowski, B.Zwieglinski Energy Dependence of the Isotopic Effect in the (n, p) Reaction on the Germanium Isotopes NUCLEAR REACTIONS 70,72,73,74Ge(n, p), 70Ge(n, 2n), 72,74Ge(n, α), E=13-16.6 MeV; measured σ. Activation technique. Preequilibrium, equilibrium mechanisms included in model analysis.
doi: 10.1007/BF01291511
1991HO23 Acta Phys.Acad.Sci.Hung. 69, 131 (1991) H.M.Hoang, U.Garuska, D.Kielan, A.Marcinkowski, B.Zwieglinski Cross Sections for the (n, p) Reaction of Pd Isotopes NUCLEAR REACTIONS 105,106,108Pd(n, p), E ≈ 13-18 MeV; 108Pd(n, α), E=13.4-15.4 MeV; measured σ(E), ground, isomer state of residual nucleus; deduced reaction mechanism. Activation techniques. Model comparison.
1991MA32 Nucl.Phys. A530, 75 (1991) A.Marcinkowski, J.Rapaport, R.Finlay, X.Aslanoglou, D.Kielan Neutron Emission Cross Sections on 93Nb and 209Bi at 20 MeV Incident Energy NUCLEAR REACTIONS 93Nb, 209Bi(n, xn), E=20 MeV; measured σ(En, θ). Statistical multistep theory analysis.
doi: 10.1016/0375-9474(91)90756-V
1990MA17 Nucl.Phys. A510, 93 (1990) A.Marcinkowski, U.Garuska, H.M.Hoang, D.Kielan, B.Zwieglinski Cross Sections of the (n, p) Reaction on Zirconium Isotopes NUCLEAR REACTIONS 90,91,92,94Zr(n, p), E=13-16.6 MeV; measured σ(E). Statistical, DWBA multistep theory analysis.
doi: 10.1016/0375-9474(90)90289-X
1989HO20 Z.Phys. A334, 285 (1989) H.M.Hoang, U.Garuska, A.Marcinkowski, B.Zwieglinski Cross Sections of Fast Neutron Induced Reactions on Selenium Isotopes NUCLEAR REACTIONS 74,76,77,78Se(n, p), 76Se(n, 2n), 80Se(n, α), E=13-16.6 MeV; measured σ. Activation technique. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset32108. 1989MA42 Nucl.Phys. A501, 1 (1989) A.Marcinkowski, R.W.Finlay, J.Rapaport, P.E.Hodgson, M.B.Chadwick Neutron Emission Cross Sections on 184W at 11.5 and 26 MeV and the Neutron-Nucleus Scattering Mechanism NUCLEAR REACTIONS 184W(n, xn), (n, n), E=11.5, 26 MeV; measured σ(En, θ). Statistical multistep theory analysis. Tof.
doi: 10.1016/0375-9474(89)90562-9
1987BU18 Nucl.Phys. A473, 179 (1987) S.Burzynski, K.Czerski, A.Marcinkowski, P.Zupranski The 3H(α, γ)7Li Reaction in the Energy Range from 0.7 To 2.0 MeV NUCLEAR REACTIONS, ICPND 7Li(α, γ), E=0.7-2 MeV; measured Eγ, Iγ, σ(θγ). 3H(α, γ), E=0.7-2 MeV; measured Eγ, Iγ, σ(θγ), σ(E), S-factor vs E. Comparison with resonating group model predictions.
doi: 10.1016/0375-9474(87)90160-6
1986MA09 Z.Phys. A323, 91 (1986) A.Marcinkowski, K.Stankiewicz, U.Garuska, M.Herman Cross Sections of Fast Neutron Induced Reactions on Molybdenum Isotopes NUCLEAR REACTIONS 92,95,96,97,98Mo(n, p), E=13-16.6 MeV; 92,100Mo(n, α), (n, 2n), 92,94Mo(n, 2n), E=13.4-16.6 MeV; 100Mo(n, 2n), E=13-16.6 MeV; measured residual, isomer production σ(E); deduced evaporation, preequilibrium emission role. Activation technique. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset30809. 1986MA26 Radiat.Eff. 93, 265 (1986) A.Marcinkowski, M.Herman, K.Stankiewicz, U.Garuska Cross Sections of Fast Neutron Induced Reactions on Molybdenum Isotopes NUCLEAR REACTIONS 95,92,96,97Mo(n, p), 100Mo(n, α), E=threshold-16 MeV; 92Mo(n, α), E=6-20 MeV; 92Mo(n, 2n), E=12-19 MeV; 100Mo(n, 2n), E=8-19 MeV; measured σ(E). Activation technique, evaporation, preequilibrium emission model analyses.
doi: 10.1080/00337578608207468
1985AN21 Nucl.Phys. A443, 404 (1985) P.Andersson, R.Zorro, I.Bergqvist, M.Herman, A.Marcinkowski Cross Sections for 197Au(n, γ)198Au and 115In(n, γ)116mIn in the Neutron Energy Region 2.0-7.7 MeV NUCLEAR REACTIONS 197Au, 115In(n, γ), E=2-7.7 MeV; measured σ(E). Compound nucleus analysis.
doi: 10.1016/0375-9474(85)90408-7
1985HE05 Acta Phys.Pol. B16, 87 (1985) M.Herman, A.Marcinkowski, G.Reffo Fast Neutron Capture on Ir Isotopes NUCLEAR REACTIONS 191,193Ir(n, γ), E=0.5-1 MeV; measured capture σ(E); deduced reaction mechanism, level density parameter systematics.
1985ST03 Nucl.Phys. A435, 67 (1985) K.Stankiewicz, A.Marcinkowski, M.Herman Particle-Hole State Densities for Calculation of the Multi-Step Compound Emission NUCLEAR STRUCTURE 30P; calculated level density; 93Nb; calculated level density, particle state density. Statistical multi-step compound emission.
doi: 10.1016/0375-9474(85)90303-3
1984AN01 J.Phys.(London) G10, 91 (1984) An Jong Do, J.Dresler, U.Garuska, M.Herman, A.Marcinkowski The Cross Sections of the (n, 2n) Reactions on 134Ba, 142Nd, 150Nd and 144Sm NUCLEAR REACTIONS 134Ba, 142,150Nd, 144Sm(n, 2n), E=13-18 MeV; measured σ(E). Activation method. Compound nucleus, precompound theory analyses.
doi: 10.1088/0305-4616/10/1/014
1984HE15 Nucl.Phys. A430, 69 (1984) M.Herman, A.Marcinkowski, K.Stankiewicz Statistical Multi-step Compound Emission in (n, 2n) Reactions NUCLEAR REACTIONS 191,193Ir(n, 2n), E=13-18 MeV; measured σ(E). 93Nb(n, xn), E=14.6 MeV; 93Nb(n, xp), E=14.1 MeV; calculated σ(En). 191Ir, 181Ta, 93Nb(n, 2n), (n, 3n), E=threshold-24 MeV; calculated σ(E). 193Ir(n, n'), E ≈ 7-19 MeV; 193Ir(n, 2n), E=8-22 MeV; calculated σ(E). Compound, multi-step compound emission theory.
doi: 10.1016/0375-9474(84)90193-3
1983MA19 Nucl.Sci.Eng. 83, 13 (1983) A.Marcinkowski, R.W.Finlay, G.Randers-Pehrson, C.E.Brient, R.Kurup, S.Mellema, A.Meigooni, R.Tailor Neutron Emission Cross Sections at 25.7 MeV: 51V, 56Fe, 65Cu, 93Nb, and 209Bi NUCLEAR REACTIONS 51V, 56Fe, 65Cu, 93Nb, 209Bi(n, xn), E=25.7 MeV; measured σ(θ), σ(En, θ). Monoisotopic targets, tof.
doi: 10.13182/NSE83-13
1983MA24 Nucl.Phys. A402, 220 (1983) A.Marcinkowski, R.W.Finlay, G.Randers-Pehrson, C.E.Brient, J.E.O'Donnell, K.Stankiewicz Neutron Emission Spectra and Angular Distributions at 25.7 MeV Neutron Bombarding Energies NUCLEAR REACTIONS 51V, 56Fe, 65Cu, 93Nb, 209Bi(n, xn), E=25.7 MeV; measured σ(θ, En). Pre-equilibrium theory analysis. Enriched targets.
doi: 10.1016/0375-9474(83)90495-5
1983NI04 Nucl.Phys. A401, 460 (1983) K.Nilson, B.Erlandsson, L.Spanier, A.Marcinkowski The 69Ga γ-Ray Strength Function between 6-10 MeV NUCLEAR REACTIONS 68Zn(p, γ), E=2.18-2.69, 3.13-3.56 MeV; measured Eγ, Iγ. 69Ga deduced levels, γ-ray strength function. Enriched target, Ge(Li) detector.
doi: 10.1016/0375-9474(83)90360-3
1982FI08 Nucl.Instrum.Methods 198, 197 (1982) R.W.Finlay, C.E.Brient, D.E.Carter, A.Marcinkowski, S.Mellema, G.Randers-Pehrson, J.Rapaport The Ohio University Beam Swinger Facility NUCLEAR REACTIONS B(d, n), E=8 MeV; 12C(n, n), (n, n'), E=24 MeV; measured σ(En); 208Pb(n, n), (n, n'), E=7.2 MeV; measured σ(θ). Tof, beam swinger magnet.
doi: 10.1016/0167-5087(82)90256-3
1982NI05 Nucl.Phys. A391, 61 (1982) K.Nilson, B.Erlandsson, A.Marcinkowski Gamma-Ray Strength Function Measurements for 59Co, 61Cu and 62Cu NUCLEAR REACTIONS 58Fe(p, γ), E=2.27-2.93 MeV; 60Ni(p, γ), E=3.13-3.88 MeV; 61Ni(p, γ), E=2.21-2.43 MeV; measured Eγ, Iγ. 59Co, 61,62Cu deduced γ-ray strength functions. Enriched target, Ge(Li) detector.
doi: 10.1016/0375-9474(82)90219-6
1982YA05 Nucl.Phys. A390, 449 (1982) Yan Yiming, C.E.Brient, R.W.Finlay, G.Randers-Pehrson, A.Marcinkowski, R.C.Tailor, J.Rapaport Interaction of 11 MeV Neutrons with 89Y NUCLEAR REACTIONS 89Y(n, n), (n, n'), E=11 MeV; measured σ(E, θ); deduced optical model parameters. 89Y levels deduced deformation parameters. DWBA, collective model.
doi: 10.1016/0375-9474(82)90278-0
1981HE03 Nucl.Phys. A357, 1 (1981) Cross Sections for Fast Neutron Capture on the Se, Pd, Cd, Os and Pt Isotopes NUCLEAR REACTIONS 78,80,82Se, 108,110Pd, 114,116Cd, 190,192Os, 196,198Pt(n, γ), E=0.5-1.3 MeV; measured σ(E). Activation technique. Compound nucleus model.
doi: 10.1016/0375-9474(81)90622-9
1980AD05 Ann.Nucl.Energy 7, 397 (1980) L.Adamski, M.Herman, A.Marcinkowski Cross Section Measurements of the 23Na(n, 2n)22Na, 58Ni(n, 2n)57Ni and 115In(n, n')115mIn Reactions NUCLEAR REACTIONS 23Na, 58Ni(n, 2n), E=14-18 MeV; 115In(n, n'), E=0.5-1.3 MeV; measured σ(E).
doi: 10.1016/0306-4549(80)90055-9
1980ER05 Nucl.Phys. A343, 197 (1980) B.Erlandsson, K.Nilson, A.Marcinkowski Investigation of the γ-Ray Strength Function in 64,66Zn by Means of the Average Resonance Method NUCLEAR REACTIONS 63Cu(p, γ), E=2.1-3.1 MeV; 65Cu(p, γ), E=1.7-7.2 MeV; measured Eγ, Iγ. 64,66Zn deduced levels, γ-ray strength functions, J, π. Enriched target, Ge(Li) detector.
doi: 10.1016/0375-9474(80)90649-1
1980ER08 Phys.Scr. 22, 432 (1980) B.Erlandsson, J.Lyttkens, K.Nilson, A.Marcinkowski Low Spin States in 64Zn and 66Zn NUCLEAR REACTIONS 63,65Cu(p, γ), E=2 MeV; measured Eγ, Iγ. 64,66Zn deduced levels.
doi: 10.1088/0031-8949/22/5/004
1980ER09 Nucl.Phys. A348, 1 (1980) B.Erlandsson, K.Nilson, A.Marcinkowski Gamma-Ray Strength Function Measurement for 63Cu NUCLEAR REACTIONS 62Ni(p, γ), E=1.9-2.4 MeV; measured Eγ, Iγ. 63Cu deduced γ-ray strength functions. Enriched target, Ge(Li) detector.
doi: 10.1016/0375-9474(80)90541-2
1979AU09 Acta Phys.Pol. B10, 357 (1979) Angular Momentum Effects in Highly Excited Nuclei NUCLEAR STRUCTURE 56Fe, 76Se, 108Pd; calculated yrast states, rotational properties; deduced appearance of back-bending in shell-model approach. Statistical model, pairing interaction.
1979ER03 Phys.Scr. 19, 251 (1979) B.Erlandsson, A.Marcinkowski, K.Nilson Cross Section of Rb at 14 MeV Neutron Energy and the Decay of Rb RADIOACTIVITY 84mRb [from 85Rb(n, 2n), E=14.8 MeV; 85Rb(γ, n), E < 25 MeV]; measured Eγ, Iγ; deduced weak feeding of excited states of 84Kr, decay to 84Rb ground state. NUCLEAR REACTIONS 85,87Rb(n, 2n), (n, p), 85Rb(n, α), E=14.8 MeV; measured σ. Activation method.
doi: 10.1088/0031-8949/19/3/006
1979ER05 Nucl.Phys. A329, 1 (1979) B.Erlandsson, K.Nilson, A.Marcinkowski Investigation of the γ-Ray Strength Function in 51V by Means of the Average Resonance Method NUCLEAR REACTIONS 50Ti(p, γ), E=2.1-2.5, 2.6-3.1 MeV; measured Eγ, Iγ. 51V deduced levels, γ-ray strength function, J, π. Enriched target, Ge(Li) detector.
doi: 10.1016/0375-9474(79)90276-8
1979ER10 Z.Phys. A293, 43 (1979) B.Erlandsson, K.Nilson, A.Marcinkowski, J.Piotrowski Investigation of 65Cu by Means of the Average Resonance Proton Capture Method NUCLEAR REACTIONS 64Ni(p, γ), E=2.05-2.55 MeV; measured Eγ, Iγ. 65Cu deduced γ-strength function. Three-crystal spectrometer. Hauser-Feshbach theory.
doi: 10.1007/BF01414783
1978CO18 Nucl.Phys. A307, 445 (1978) V.Corcalciuc, B.Holmqvist, A.Marcinkowski, G.A.Prokopets A Study of the Neutron Induced Reactions for 19F, 56Fe and 50Co in the Energy Interval 16 to 22 MeV NUCLEAR REACTIONS 19F, 56Fe, 59Co(n, X), E=16.2, 18.1, 19.3, 20.5, 21.8 MeV; measured Eγ, σ(En, Eγ) at θ=55°. Ge(Li) detector. Time of flight. Natural targets. Compound statistical model calculations.
doi: 10.1016/0375-9474(78)90459-1
1978HE05 Nucl.Phys. A297, 335 (1978); Erratum Nucl.Phys. A308, 532 (1978) M.Herman, A.Marcinkowski, J.Bielewicz, P.Oblozinsky Cross Sections for the (n, p) and (n, n') Reactions on Pd, Cd and Os NUCLEAR REACTIONS 105Pd, 112Cd(n, p), E=13-17 MeV; 111Cd, 190Os(n, n'), E=13-17 MeV; measured σ(E); compared compound nucleus, precompound emission models.
doi: 10.1016/0375-9474(78)90280-4
1977AU09 Nucl.Phys. A285, 145 (1977) W.Augustyniak, M.Herman, A.Marcinkowski, B.Zwieglinski Cross Sections for the (n, 2n) Reaction on 102Pd, 110Pd, 112Cd and 192Os NUCLEAR REACTIONS 102Pd, 110Pd, 112Cd, 192Os(n, 2n), E=13-18 MeV; 192Os(n, 3n), E=16-18 MeV; measured σ(E); compared compound nucleus, precompound emission models.
doi: 10.1016/0375-9474(77)90151-8
1976AU08 Acta Phys.Pol. B7, 347 (1976) W.Augustyniak, M.Herman, A.Marcinkowski Cross Sections for the Fast Neutron Induced Reactions on Rubidium Isotopes NUCLEAR REACTIONS 85,87Rb(n, 2n), (n, p), (n, α), E=13-18 MeV; measured σ. Activation technique. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset30350. 1976HE22 J.Phys.(London) G2, 831 (1976) M.Herman, A.Marcinkowski, B.Zwieglinski, W.Augustyniak, J.Bielewicz, W.Zych Elastic and Inelastic Scattering of 9.1 MeV Protons from Magnesium Isotopes NUCLEAR REACTIONS 24,25,26Mg(p, p), (p, p'), E=9.1 MeV; measured σ(θ), total σ; deduced optical potentials. 24,25,26Mg deduced β. Hartree-Fock calculations. Enriched targets, Si surface barrier detectors.
doi: 10.1088/0305-4616/2/11/008
1975AU04 Nucl.Phys. A247, 231 (1975) W.Augustyniak, M.Herman, A.Marcinkowski Cross Sections for the (n, n'), (n, p) and (n, 2n) Reactions on 107Ag and 109Ag Isotopes NUCLEAR REACTIONS 107Ag, 109Ag(n, n'), E=3-18 MeV; 107Ag, 109Ag(n, 2n), E=13-18 MeV; 109Ag(n, p), E=13-16 MeV; measured σ(E); compared compound nucleus, precompound emission models.
doi: 10.1016/0375-9474(75)90633-8
1975ER05 Z.Phys. A272, 67 (1975) B.Erlandsson, J.Lyttkens, A.Marcinkowski Isobaric Analogue States Excited in the 59Co(p, γ)60Ni Reaction NUCLEAR REACTIONS 59Co(p, γ), E=1365-2150 keV; measured σ(E, Eγ); deduced Q. 60Ni deduced analogs, resonances, γ-branching.
doi: 10.1007/BF01408430
1975ER07 Phys.Scr. 12, 95 (1975) A Search for Isobaric Analogue States in 58Co from the 57Fe(p, γ)58Co Reaction NUCLEAR REACTIONS 57Fe(p, γ), E=1580-2125 keV; measured σ(E, Eγ). 58Co deduced resonances, levels, γ-branching, IAS, J, π.
doi: 10.1088/0031-8949/12/1-2/011
1975GR36 Acta Phys.Pol. B6, 139 (1975) W.Grochulski, S.El-Konsol, A.Marcinkowski Excitation Curves for Fast Neutron Induced Reactions on 71Ga, 75As, 80Se, 117Sn and 118Sn Nuclei NUCLEAR REACTIONS 71Ga, 75As, 80,82Se, 118Sn(n, 2n), 71Ga, 75As, 117Sn(n, p), 117Sn(n, n'), E=13-18 MeV; measured σ(E). Data from this article have been entered in the EXFOR database. For more information, access X4 dataset30287. 1973DE11 Nucl.Phys. A204, 121 (1973) P.Decowski, W.Grochulski, J.Karolyi, A.Marcinkowski, J.Piotrowski, E.Saad, Z.Wilhelmi Cross Sections for the (n, n') and (n, 2n) Reactions on 113In and 204Pb NUCLEAR REACTIONS 113In, 204Pb(n, n'), (n, 2n), E=13-18 MeV; measured σ(E), isomeric σ ratios; compared compound-nucleus theory.
doi: 10.1016/0375-9474(73)90010-9
1972DE45 Nucl.Phys. A194, 380 (1972) P.Decowski, W.Grochulski, A.Marcinkowski On the Role of the γ-Decay of Unbound Nuclear States in Nucleon-Induced Reactions
doi: 10.1016/0375-9474(72)91045-7
1972EK02 Z.Phys. 252, 189 (1972) P.Ekstrom, B.Erlandsson, A.Marcinkowski, J.Tillman The Energy of Levels of 45Sc up to 3 MeV from the 44Ca(p, γ)45Sc Reaction NUCLEAR REACTIONS 44Ca(p, γ), E=1658 keV; measured Eγ, Iγ. 45Sc deduced levels, J, π, γ-branching.
1972MA05 Nucl.Phys. A179, 781 (1972); Erratum Nucl.Phys. A196, 636 (1972) A.Marcinkowski, A.Backlin, I.Bergqvist Levels in 115In Studied by Means of Inelastic Neutron Scattering NUCLEAR REACTIONS 115In(n, n'γ), E=0.78-1.80 MeV; measured Eγ, Iγ, σ(E;Eγ). 115In deduced levels, J, π, γ-branching. Natural target, Ge(Li) detector.
doi: 10.1016/0375-9474(72)90619-7
1971AB08 Acta Phys.Pol. B2, 527 (1971) A.Abboud, P.Decowski, W.Grochulski, A.Marcinkowski, K.Siwek, I.Turkiewicz, Z.Wilhelmi Cross-Sections for the 89Y(n, n')89mY and 89Y(n, 2n)88Y Reactions NUCLEAR REACTIONS 89Y(n, n'), (n, 2n), E=3-18, 13-18 MeV; measured σ(E). Data from this article have been entered in the EXFOR database. For more information, access X4 dataset30274. 1970ER01 Ark.Fys. 40, 139 (1970) B.Erlandsson, A.Marcinkowski, N.Wall The Decay and Half-Life of 51Mn RADIOACTIVITY 51Mn; measured T1/2, Eγ, Iγ; deduced log ft, Eβ, EC/β+-branching. 51Cr deduced transitions.
1970ER03 Nucl.Phys. A146, 43 (1970) Energy Levels in 58Co NUCLEAR REACTIONS 57Fe(p, γ), E=1.2-1.7 MeV; measured σ(E;Eγ), Eγ, Iγ, γγ-coin; deduced Q. 58Co deduced resonances, levels, γ-branching. Enriched target, Ge(Li) detector.
doi: 10.1016/0375-9474(70)91086-9
1970GR35 Acta Phys.Pol. B1, 271 (1970) W.Grochulski, J.Karolyi, A.Marcinkowski, J.Piotrowski, E.Saad, K.Siwek, Z.Wilhelmi Isomeric Cross Section Ratios and Total Cross-Sections for the 113In(n, 2n)112g, m-In and 115In(n, 2n)114g, m-In Reactions NUCLEAR REACTIONS 113,115In(n, 2n), E=13.1-18.2 MeV; measured σ(E), isomeric σ ratios. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset30104. 1969AB10 Nucl.Phys. A139, 42 (1969) A.Abboud, P.Decowski, W.Grochulski, A.Marcinkowski, J.Piotrowski, K.Siwek, Z.Wilhelmi Isomeric Cross-Section Ratios and Total Cross Sections for the 74Se(n, 2n)73g, m-Se, 90Zr(n, 2n)89g, m-Zr and 92Mo(n, 2n)91g, m-Mo Reactions NUCLEAR REACTIONS 74Se, 90Zr, 92Mo(n, 2n), E=12-18 MeV; measured σ(E), isomeric σ ratio. Natural target.
doi: 10.1016/0375-9474(69)90258-9
1968DE08 Nucl.Phys. A112, 513(1968) P.Decowski, W.Grochulski, A.Marcinkowski, K.Siwek, I.Sledzinska, Z.Wilhelmi Isomeric Cross-Section Ratios and Total Cross Sections for the 59Co(n, 2n)58g,58mCo, 58Ni(n, p)58g,58mCo and 59Co(γ, n)58g,58mCo Reactions RADIOACTIVITY 58Co; measured T1/2. 58Ni(n, p), E=2-18 MeV; 59Co(n, 2n), E=12-18 MeV; 59Co(γ, n), E < 30 MeV; measured σ(E), isomeric cross-section ratio. Natural targets.
doi: 10.1016/0375-9474(68)90075-4
1968ER04 Z.Physik 215, 39 (1968) Energy Levels in 46Ti NUCLEAR REACTIONS 45Sc(p, γ), E=1.377, 1.660 MeV; measured Eγ, Iγ. 46Ti deduced levels.
doi: 10.1007/BF01382514
Back to query form Note: The following list of authors and aliases matches the search parameter A.Marcinkowski: , A.J.MARCINKOWSKI |