NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = Z.Zelazny Found 33 matches. 1997BO21 Z.Phys. A358, 329 (1997) A.Bonaccorso, Z.Zelazny, E.Piasecki Separation of Coulomb Fission from Nuclear Fission at Medium Energies NUCLEAR REACTIONS 197Au(238U, 239U), E=8.1-50 MeV/nucleon; calculated electromagnetic field induced fission σ vs E; deduced Coulomb, nuclear fission separation related features.
doi: 10.1007/s002180050336
1997KI14 Acta Phys.Pol. B28, 219 (1997) M.Kicinska-Habior, Z.Trznadel, M.Kisielinski, M.Augsburg, D.Chmielewska, J.Dworski, A.Kordyasz, M.Kowalczyk, J.Kownacki, A.Krzyczkowska, J.Kwiecinski, A.Maj, T.Matulewicz, J.Romanowski, Z.Sujkowski, Z.Zelazny Progress with the Statistical Giant Dipole Resonance Decay Experiment at the Warsaw Cyclotron NUCLEAR REACTIONS 58Ni(12C, γ), E=47.5 MeV; measured Eγ, Iγ. 70Se deduced GDR E, Γ. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1404. 1997PO08 Acta Phys.Pol. B28, 139 (1997) M.Popkiewicz, S.Osuch, Z.Szeflinski, A.Sztampke, M.Wolinska, R.Zaganczyk, Z.Wilhelmi, Z.Zelazny Test of Modular Neutron Spectrometer in Measurement of Neutron Spectra from Fission of 252Cf RADIOACTIVITY 252Cf(SF); measured fission-associated En, In; deduced detector characteristics.
1996KI12 Acta Phys.Pol. B27, 547 (1996) M.Kicinska-Habior, A.Maj, Z.Sujkowski, J.Kownacki, M.Kisielinski, Z.Zelazny, M.Moszynski, M.Kowalczyk, T.Matulewicz, Z.Trznadel, D.Chmielewska, J.Styczen, B.Fornal, W.Krolas, E.Kulczycka, M.Augsburg, J.Romanowski, M.Kmiecik Experimental Set-Up for High-Energy γ-Ray Studies at the Warsaw Cyclotron and First Experiments NUCLEAR REACTIONS 27Al(12C, X), E=34.2 MeV; measured high energy γ spectra. Multi-detector set-up.
1996MA34 Acta Phys.Pol. B27, 541 (1996) A.Maj, M.Kmiecik, F.Camera, B.Herskind, J.J.Gaardhoje, A.Bracco, A.Atac, R.A.Bark, I.G.Bearden, P.Bosetti, S.Leoni, M.Mattiuzzi, T.S.Tveter, Z.Zelazny Array of Anti-Compton Spectrometers as a Trigger in GDR Studies NUCLEAR REACTIONS 110Pd(37Cl, xn), E=160, 170 MeV; measured high energy particle gated γ-spectra; deduced GDR decay characteristics. 143Eu deduced possible GDR low lying component.
1995BR11 Phys.Rev.Lett. 74, 3748 (1995) A.Bracco, F.Camera, M.Mattiuzzi, B.Million, M.Pignanelli, J.J.Gaardhoje, A.Maj, T.Ramsoy, T.Tveter, Z.Zelazny Increase in Width of the Giant Dipole Resonance in Hot Nuclei: Shape change or collisional damping ( Question ) NUCLEAR REACTIONS 62,61Ni(48Ti, X), E=223, 203 MeV; measured γ(θ), strength function. 109,110Sn deduced GDR, Γ.
doi: 10.1103/PhysRevLett.74.3748
1995BR19 Acta Phys.Pol. B26, 407 (1995) A.Bracco, F.Camera, M.Mattiuzzi, B.Million, M.Pignanelli, J.J.Gaardhoje, T.Ramsoy, T.Tveter, Z.Zelazny, A.Maj The Damping of the GDR at Finite Temperature: Recent progress NUCLEAR REACTIONS 70Zn(36Ar, X), E=27 MeV/nucleon; 62,61Ni(48Ti, X), E=203, 223 MeV; 148Nd(28Si, X), E=147 MeV; compiled, reviewed γ-spectra data; deduced GDR damping, other characteristic vs T for mass 110, 170. Hot rotating nuclei.
1995CA23 Acta Phys.Pol. B26, 479 (1995) F.Camera, A.Bracco, P.Bosetti, M.Mattiuzzi, G.Lo Bianco, M.Pignanelli, J.J.Gaardhoje, Z.Zelazny, I.G.Bearden, A.Maj Detecting High Energy γ-Rays with HPGe Detectors NUCLEAR REACTIONS 2H(11B, n), E=19 MeV; measured Eγ, Iγ. Hyperpure Ge detector, ' adding mode ' technique.
1995JE04 Nucl.Phys. A593, 162 (1995) D.Jerrestam, B.Fogelberg, A.Kerek, W.Klamra, F.Liden, L.O.Norlin, J.Kownacki, D.Seweryniak, Z.Zelazny, C.Fahlander, J.Nyberg, M.Guttormsen, J.Rekstad, T.Spedstad-Tveter, A.Gizon, J.Gizon, R.Bark, G.Sletten, M.Piiparinen, Z.Preibisz, T.F.Thorsteinsen, E.Ideguchi, S.Mitarai In-Beam Spectroscopic Studies of the Nucleus 105Cd NUCLEAR REACTIONS 106Cd(p, np), E=30 MeV; 106Cd(3He, 2n2p), E=75 MeV; 92Zr(16O, 3n), E=77 MeV; 76Ge(34S, 5n), E=148 MeV; measured γγ, γγ(particle)-coin, Eγ, Iγ, DCO ratios. 105Cd deduced levels, J, π, band structure, configuration. Compton suppressed Ge-detector array. Model calculations.
doi: 10.1016/0375-9474(95)00334-W
1995MA55 Acta Phys.Pol. B26, 467 (1995) M.Mattiuzzi, A.Bracco, F.Camera, B.Million, J.J.Gaardhoje, A.Maj, T.Tveter, Z.Zelazny Angular Momentum Dependence of the GDR Observables of A = 170 Nuclei at Finite Temperature NUCLEAR REACTIONS 148Nd(28Si, X), E=147 MeV; measured Eγ, Iγ(θ), strength function. 176W deduced GDR observables angular momentum at finite temperature dependence.
1995MA84 Phys.Lett. 364B, 13 (1995) M.Mattiuzzi, A.Bracco, F.Camera, B.Million, M.Pignanelli, J.J.Gaardhoje, A.Maj, T.Ramsoy, T.Tveter, Z.Zelazny Thermal Fluctuation and Collisional Damping Effects in the GDR Observables in Hot Rotating 176W Nuclei NUCLEAR REACTIONS 148Nd(28Si, X), E=147 MeV; measured γγ-coin, Eγ, Iγ. 176W deduced GDR width, thermal fluctuation, collisional damping effects role.
doi: 10.1016/0370-2693(95)01230-5
1995VA24 Phys.Rev. C52, 1915 (1995) H.van der Ploeg, J.C.S.Bacelar, A.Buda, C.R.Laurens, A.van der Woude, J.J.Gaardhoje, Z.Zelazny, G.van't Hof, N.Kalantar-Nayestanaki Emission of Photons in Spontaneous Fission of 252Cf RADIOACTIVITY 252Cf(SF); measured fission fragment masses, σ(θ), neutron multiplicities, γ-anisotropy; deduced mass dependence of Eγ, effective level density parameters, anisotropy of Eγ with fission axis. Statistical code reproduction of data.
doi: 10.1103/PhysRevC.52.1915
1995ZE03 Acta Phys.Pol. B26, 459 (1995) Z.Zelazny, J.J.Gaardhoje, A.Maj, T.S.Tveter, F.Camera, M.Mattiuzzi, A.Bracco, B.Million, M.Pignanelli Does the Compound Nucleus Remember Its Way of Formation ( Question ); Hot GDR spectroscopy in the Yb-Dy region NUCLEAR REACTIONS 144Sm(17O, X), (18O, X), 113,114Cd(48Ti, X), 128,130Te(28Si, X), (29Si, X), E not given; analyzed Iγ, other data. 162Yb, 158Dy deduced GDR decay features. Hot compound systems.
1994BR08 Nucl.Phys. A569, 51c (1994) A.Bracco, F.Camera, M.Mattiuzzi, B.Million, M.Pignanelli, C.Volpe, J.J.Gaardhoje, A.Maj, Z.Zelazny, T.Tveter Thermal and Quantal Fluctuations as Probed by the GDR Observables NUCLEAR REACTIONS 61,62Ni(48Ti, X), E not given; analyzed Iγ(θ), γ strength function data. 110Sn deduced GDR parameters.
doi: 10.1016/0375-9474(94)90095-7
1994CA11 Nucl.Phys. A572, 401 (1994) F.Camera, A.Bracco, B.Million, M.Pignanelli, J.J.Gaardhoje, Z.Zelazny, T.Ramsoy, A.Maj Large Effects of Orientation Fluctuations in the Angular Distribution of the GDR Photons NUCLEAR REACTIONS 148Nd(17O, xnpα), E=70 MeV; 148Nd(18O, xnpα), E=78 MeV; 150Nd(17O, xnpα), E=85 MeV; 158Gd(17O, xnpα), E=74 MeV; 160Gd(16O, xnpα), E=85 MeV; 94Mo(16O, xnpα), E=85 MeV; measured σ(Eγ, θ), Iγ(θ). 165,166,167Er, 175,176Hf, 110Sn deduced GDR features, shape, orientation fluctuations role, effective nuclear deformation. Hot nuclei.
doi: 10.1016/0375-9474(94)90182-1
1994CA47 Nucl.Instrum.Methods Phys.Res. A351, 401 (1994) F.Camera, A.Bracco, M.Mattiuzzi, G.Lo Bianco, M.Pignanelli, J.J.Gaardhoje, I.G.Bearden, Z.Zelazny, A.Maj The response of a HPGe Detector with a BGO Shield to High Energy γ-Rays NUCLEAR REACTIONS 2H(11B, n), E=19 MeV; measured Eγ, Iγ; deduced detector response. Hyperpure Ge detector with a BGO anti-Compton shield.
doi: 10.1016/0168-9002(94)91369-2
1994VA05 Nucl.Phys. A569, 83c (1994) H.van der Ploeg, C.R.Laurens, J.C.S.Bacelar, A.Buda, J.J.Gaardhoje, G.van't Hof, N.Kalantar-Nayestanaki, A.van der Woude, Z.Zelazny Study of the Gamma Emission Probability Accompanying the Spontaneous Fission of 252Cf RADIOACTIVITY 252Cf(SF); measured γ-yield following SF-decay, fission (fragment)γ(θ); deduced photon emission probability vs excitation.
doi: 10.1016/0375-9474(94)90098-1
1994ZE01 Nucl.Phys. A569, 1c (1994) Z.Zelazny, J.J.Gaardhoje, A.Maj, T.S.Tveter, T.Ramsoy, W.Korten, A.Bracco, F.Camera, M.Matiuzzi, B.Million, M.Pignanelli Some Open Problems in Hot GDR Spectroscopy NUCLEAR REACTIONS 114Cd(48Ti, X), E=225 MeV; analyzed γ-spectra fold distribution, Iγ data; deduced shape degrees of freedom equilibration features. Other data reviewed.
doi: 10.1016/0375-9474(94)90091-4
1993BR09 Nucl.Phys. A557, 237c (1993) A.Bracco, F.Camera, B.Million, M.Pignanelli, J.J.Gaardhoje, A.Maj, Z.Zelazny, W.Korten Probing the Shapes of Hot Nuclei with the GDR NUCLEAR REACTIONS 150Nd(17O, X), E=85 MeV; 148Nd(18O, X), E=78 MeV; 148Nd(17O, X), E=70 MeV; 158Gd(17O, X), E=74 MeV; 160Gd(16O, X), E=85 MeV; 61Ni(48Ti, X), E=209 MeV; 62Ni(48Ti, X), E=223 MeV; measured γ spectra, Iγ(θ). 165,166,167Er, 175,176Hf, 109,110Sn deduced GDR decay features, shapes. Adiabatic model.
doi: 10.1016/0375-9474(93)90544-8
1993CA08 Acta Phys.Pol. B24, 437 (1993) F.Camera, A.Bracco, B.Million, M.Pignanelli, J.J.Gaardhoje, Z.Zelazny, A.Maj The Shape of Hot Nuclei and the Angular Distribution of Hard Dipole Photons NUCLEAR REACTIONS 62Ni(48Ti, X), E=79 MeV; 148Nd(17O, X), E=45 MeV; 148Nd(18O, X), E=51 MeV; 150Nd(17O, X), E=61 MeV; analyzed Iγ(θ). 110Sn, 165,166,167Er deduced shape change, orientation dependence on angular momentum.
1993GA06 Acta Phys.Pol. B24, 139 (1993) J.J.Gaardhoje, A.Maj, T.Tveter, Z.Zelazny, F.Camera, A.Bracco, B.Million, M.Pignanelli Atomic Nuclei at High Excitation Energy Studied with Giant Resonances NUCLEAR REACTIONS 70Ge(40Ar, X), E=10 MeV/nucleon; 93Nb(19F, X), E=80-160 MeV; 94Mo(16O, X), E=140 MeV; analyzed γ-decay data; deduced features of time for equilibration, collective motion build up, nucleonic, large scale mass arrangements. GDR decay, other systems studied.
1993MA11 Acta Phys.Pol. B24, 429 (1993) A.Maj, J.J.Gaardhoje, Z.Zelazny, A.Bracco, F.Camera, M.Matiuzzi, B.Million, M.Pignanelli E(*) and I Selection Techniques for Hot Nuclei Studies NUCLEAR REACTIONS 114Cd(48Ti, X), E=225 MeV; measured Iγ(θ) for 162Yb decay; deduced hot nuclei GDR decay, width features.
1991GU04 Nucl.Phys. A531, 370 (1991) M.Guttormsen, A.Atac, K.Klungland, S.Messelt, T.Ramsoy, J.Rekstad, T.S.Tveter, Z.Zelazny Gross Properties of Statistical γ-Decay in 172Yb NUCLEAR REACTIONS 173Yb(3He, α), E=45 MeV; measured σ(Eα), Eγ, Iγ, αγ-coin. 172Yb deduced γ-ray multiplicity, statistical γ-decay features. Enriched target, Ge, NaI, Si detectors.
doi: 10.1016/0375-9474(91)90617-F
1990GU14 Phys.Scr. T32, 54 (1990) M.Guttormsen, A.Atac, G.Lovhoiden, S.Messelt, T.Ramsoy, J.Rekstad, T.F.Thorsteinsen, T.S.Tveter, Z.Zelazny Statistical Gamma-Decay at Low Angular Momentum NUCLEAR REACTIONS 170Yb, 162Dy(3He, 3He'), 173Yb, 162Dy(3He, α), E=45 MeV; measured γ(ejectile)-coin; deduced γ-emission mechanism.
doi: 10.1088/0031-8949/1990/T32/010
1989ZE01 Nucl.Phys. A499, 100 (1989) Z.Zelazny, T.S.Tveter, A.Atac, M.Guttormsen, T.Ramsoy, J.Rekstad First-Generation γ-Rays from Highly-Excited Even Rare-Earth Nuclei NUCLEAR REACTIONS 161,163Dy, 171,173Yb(3He, α), E=45 MeV; measured σ(Eα, Eγ), γ(θ), Eγ, Iγ, αγ-coin. 160,162Dy, 170,172Yb deduced first generation γ-ray transitions, branching ratios. Enriched targets, Ge, NaI, Si counters. Fermi-gas model analysis.
doi: 10.1016/0375-9474(89)90271-6
1988BA32 Phys.Scr. 37, 843 (1988) T.Batsch, J.Kownacki, Z.Zelazny, M.Guttormsen, T.Ramsoy, J.Rekstad Particle-Core Multiplets in 89Y NUCLEAR REACTIONS 87Rb(α, 2n), E=24-34 MeV; measured Eγ, Iγ, γγ-coin, γ(θ). 89Y deduced levels, J, π, configuration.
doi: 10.1088/0031-8949/37/6/001
1987EL07 Nucl.Instrum.Methods Phys.Res. B22, 82 (1987) F.M.El-Ashry, L.Glowacka, M.Jaskola, M.Pfuetzner, J.Szerypo, Z.Zelazny, G.Osetynski, M.Pajek The Cross Sections for K-Shell Ionization of Heavy Elements with Low Energy Protons and Deuterons NUCLEAR REACTIONS Nd, Sm, Tb, Tm, Ta(p, X), E=0.8-3.8 MeV; Gd, Ta(d, X), E=0.9-3.2 MeV; measured K-shell ionization σ. Simple ionization, plane wave Born approximation model analysis.
doi: 10.1016/0168-583X(87)90299-0
1987PF04 J.Phys.(London) B20, 3453 (1987) M.Pfuetzner, J.Szerypo, Z.Zelazny, F.M.El-Ashry, M.Goclowski, L.Glowacka, D.Trautmann, M.Jaskola The K-Shell Ionisation of 73Ta Induced by Low-Energy Protons and Deuterons NUCLEAR REACTIONS Ta(p, X), E=1.1-3.8 MeV; Ta(d, X), E=1.2-3.2 MeV; measured K shell ionization σ.
doi: 10.1088/0022-3700/20/14/017
1986ZE05 J.Phys.(London) B19, 4185 (1986) Z.Zelazny, M.Pfuetzner, J.Szerypo, M.Jaskola, M.Goclowski The Cross Sections for K-Shell Ionisation of 60Nd, 62Sm and 69Tm by Low-Energy Protons NUCLEAR REACTIONS Nd, Sm, Tm(p, X), E=0.8-2.6 MeV; measured I(K X-ray); deduced K shell ionization σ. ATOMIC PHYSICS Nd, Sm, Tm(p, X), E=0.8-2.6 MeV; measured I(K X-ray); deduced K shell ionization σ.
doi: 10.1088/0022-3700/19/24/019
1984ZE02 J.Phys.(London) B17, 1867 (1984) The K-Shell Ionisation of 64Gd, 74W and 90Th Induced by Heavy, Charged Particles NUCLEAR REACTIONS Gd(α, α'γ), E=3.29-14.97 MeV; Gd(16O, 16O'γ), E=11.87-29.53 MeV; W(α, α'γ), E=3.44-12.99 MeV; W(12C, 12C'γ), E=8.73-33.82 MeV; W(16O, 16O'γ), E=11.88-38.68 MeV; W(19F, 19F'γ), E=14.1-40.9 MeV; Th(α, α'γ), E=4.39-15.14 MeV; Th(16O, 16O'), E=13.43-33.52 MeV; measured Eγ, Iγ; deduced K-shell ionization σ. Semi-classical approximation, Coulomb excitation, electron binding, Coulomb deflection, relativistic corrections.
doi: 10.1088/0022-3700/17/9/024
1983GO19 J.Phys.(London) B16, 3571 (1983) M.Goclowski, M.Jaskola, J.Szerypo, P.Hornshoj, Z.Zelazny The K-Shell Ionisation of 64Gd and 74W by Low-Energy Protons NUCLEAR REACTIONS Gd(p, X), (p, γ), E=0.8-2.8 MeV; W(p, X), (p, γ), E=1.1-7.7 MeV; measured K-shell ionization σ, Eγ, Iγ, E(K X-ray), I(K X-ray).
doi: 10.1088/0022-3700/16/19/015
1982KU12 Z.Phys. A306, 99 (1982) W.Kurcewicz, J.Szerypo, P.Hornshoj, N.Rud, Z.Zelazny, W.Reisdorf Fission of 232Th Induced by 4-11 MeV Protons NUCLEAR REACTIONS, ICPND 232Th(p, F), E=4-11 MeV; measured fission σ vs E, fission yield mass distribution; deduced peak to valley ratio.
doi: 10.1007/BF01415478
1981HO27 J.Phys.(London) B14, 2391 (1981) P.Hornshoj, Z.Zelazny, M.Jaskola, L.Zemlo, A.Celler, J.Szerypo The K-shell Ionisation of 90Th by Protons and Alpha Particles NUCLEAR REACTIONS 232Th(α, α'), E=2.5-16 MeV; 232Th(p, p'), E=1.2-6 MeV; measured Eγ, Iγ, E(K X-ray), I(K X-ray), Coulomb excitation; deduced K-shell σ(ionization).
doi: 10.1088/0022-3700/14/14/011
Back to query form |