NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = L.Zemlo Found 31 matches. 2003KY01 Nucl.Phys. A726, 231 (2003) V.M.Kyryanchuk, A.T.Rudchik, A.Budzanowski, V.K.Chernievsky, T.Czosnyka, B.Czech, L.Glowacka, S.Kliczewski, E.I.Koshchy, S.Yu.Mezhevych, A.V.Mokhnach, K.Rusek, S.B.Sakuta, R.Siudak, I.Skwirczynska, A.Szczurek, L.Zemlo One-nucleon transfer reaction 9Be(11B, 10B)10Be and optical potential for the 10B + 10Be interaction NUCLEAR REACTIONS 9Be(11B, 10B), (11B, 10Be), E=45 MeV; measured σ(E, θ); 10B(9Be, 9Be), (9Be, 10B), E(cm)=8.42-47.37 MeV; analyzed data; deduced reaction mechanism features, optical model parameters. Coupled reaction channels analysis.
doi: 10.1016/S0375-9474(03)01623-3
2003ME13 Nucl.Phys. A724, 29 (2003) S.Yu.Mezhevych, K.Rusek, A.T.Rudchik, A.Budzanowski, V.K.Chernievsky, B.Czech, J.Choinski, L.Glowacka, S.Kliczewski, E.I.Koshchy, V.M.Kyryanchuk, A.V.Mokhnach, A.A.Rudchik, S.B.Sakuta, R.Siudak, I.Skwirczynska, A.Szczurek, L.Zemlo The 13C + 11B elastic and inelastic scattering and isotopic effects in the 12, 13C + 11B scattering NUCLEAR REACTIONS 13C(11B, 11B), (11B, 11B'), (11B, 13C), E=45 MeV; measured σ(θ); deduced optical model parameters, isotopic effects. 11B, 13C deduced deformation parameters. Optical model and coupled-reaction-channels analysis, anomalous large-angle scattering.
doi: 10.1016/S0375-9474(03)01478-7
2003RU02 Nucl.Phys. A714, 391 (2003) A.T.Rudchik, V.M.Kyryanchuk, A.Budzanowski, V.K.Chernievsky, B.Czech, T.Czosnyka, A.V.Glowacka, S.Kliczewski, E.I.Koshchy, S.Yu.Mezhevych, A.V.Mokhnach, K.Rusek, S.B.Sakuta, R.Siudak, I.Skwirczynska, A.Szczurek, L.Zemlo Mechanism of large angle enhancement of the 9Be+11B scattering NUCLEAR REACTIONS 9Be(11B, 11B), (11B, 9Be), E=45 MeV; measured σ(E), σ(θ); deduced optical model parameters, anomalous large angle scattering mechanism. 9Be, 11B; deduced deformation parameters. Optical model and coupled-channels analysis.
doi: 10.1016/S0375-9474(02)01391-X
2003RU11 Iader.Fiz.Enerh. 4 no.3, 32 (2003) A.A.Rudchik, V.K.Chernievsky, A.T.Rudchik, A.Budzanowski, L.Glovacka, L.Zemlo, S.Kliczewski, E.I.Koshchy, O.A.Ponkratenko, O.A.Momotyuk, A.V.Mokhnach, V.M.Pirnak, K.Rusek, I.Skwirszynska, R.Siudak, B.Czech, A.Szczurek Mechanisms of the 12C(11B, 15N)8Be reaction NUCLEAR REACTIONS 12C(11B, 15N), E=49 MeV; measured reaction products; deduced σ(θ); 12C(11B, 8Be), E(cm)=10-17 MeV; analyzed σ(θ);deduced reaction mechanism features, optical model parameters. Coupled channels analysis.
doi: 10.15407/jnpae
2001RU14 Nucl.Phys. A695, 51 (2001) A.T.Rudchik, A.Budzanowski, V.K.Chernievsky, B.Czech, L.Glowacka, S.Kliczewski, A.V.Mokhnach, O.A.Momotyuk, S.E.Omelchuk, V.M.Pirnak, K.Rusek, R.Siudak, I.Skwirczynska, A.Szczurek, L.Zemlo The 11B + 12C Elastic and Inelastic Scattering at Elab(11B) = 49 MeV and Energy Dependence of the 11B + 12C Interaction NUCLEAR REACTIONS 12C(11B, 11B), (11B, 12C), E=49 MeV; measured σ(θ); deduced optical model parameters, energy dependence. 11B, 12C deduced deformation parameters. Optical model and coupled reaction channels method analysis.
doi: 10.1016/S0375-9474(01)01106-X
1997IW02 Acta Phys.Pol. B28, 153 (1997) J.Iwanicki, J.Choinski, T.Czosnyka, J.Kownacki, M.Kisielinski, P.Napiorkowski, L.Zemlo, J.Srebrny, J.de Boer, M.Loewe, M.Wurkner Coulomb Excitation at the Warsaw Cyclotron NUCLEAR REACTIONS 150Nd(14N, 14N'), E not given; measured not given. 150Nd deduced transition B(E4). Other Coulomb excitation results discussed.
1992BR11 Phys.Rev. C45, 2272 (1992) B.Brinkmoller, P.Decowski, B.Marianski, H.P.Morsch, D.Paul, M.Rogge, R.Siebert, W.Spang, P.Turek, L.Zemlo Fission Decay of Giant Resonances in 238U Excited in α Scattering at Small Momentum Transfer NUCLEAR REACTIONS 238U(α, α'F), E=172 MeV; measured σ(θα, Eα) following fission, (fragment)(α)-coin. 238U deduced multipole excitation strength for L=0-5, isoscalar giant resonances, fission probability. Statistical model.
doi: 10.1103/PhysRevC.45.2272
1991TE02 Phys.Rev.Lett. 66, 872 (1991) P.-E.Tegner, B.Marianski, H.P.Morsch, M.Rogge, Chr.Bargholtz, P.Decowski, L.Zemlo Enhanced Emission of High-Energy Photons Perpendicular to the Reaction Plane in α + Th Reactions NUCLEAR REACTIONS 232Th(α, F), E=170 MeV; measured fission (fragment)γ-, (fragment)n-coin; deduced photon emission mechanism.
doi: 10.1103/PhysRevLett.66.872
1986AU06 Radiat.Eff. 94, 269 (1986) W.Augustyniak, L.Glowacka, M.Jaskola, J.Turkiewicz, L.Zemlo, J.Dalmas, E.Gadioli, E.Gadioli Erba Influence of the Shell Structure of the Target Nucleus on Alpha Emission in (n, α) Reactions NUCLEAR REACTIONS 143Nd(n, α), E=14.1, 18.2 MeV; 142Nd(n, α), E=14.3, 18.1 MeV; measured σ(θ, Eα); deduced unpaired neutron outside magic shell rule. 140,139Ce deduced levels, excitation differences.
doi: 10.1080/00337578608208389
1986GA23 Phys.Rev. C34, 2065 (1986) E.Gadioli, E.Gadioli Erba, L.Glowacka, M.Jaskola, J.Turkiewicz, L.Zemlo, J.Dalmas, A.Chiadli 90,91Zr(n, α)87,88Sr Reactions at 14.3 and 18.15 MeV Incident Neutron Energy NUCLEAR REACTIONS 90,91Zr(n, α), E=14.3, 18.15 MeV; measured σ(θα), σ(Eα); deduced reaction mechanism, model parameters. 87,88Sr levels deduced spectroscopic amplitudes. Pick-up, knock-on theories.
doi: 10.1103/PhysRevC.34.2065
1985AU03 Nuovo Cim. 85A, 217 (1985) W.Augustyniak, L.Glowacka, M.Jaskola, J.Turkiewicz, L.Zemlo, J.Dalmas, E.Gadioli, E.Gadioli Erba Investigation of the 149Sm(n, α)146Nd Reaction Induced by Fast Neutrons NUCLEAR REACTIONS 149Sm(n, α), E=12, 14, 18 MeV; measured σ(Eα), σ(θ); deduced reaction mechanism. Statistical, preequilibrium, knockon models.
doi: 10.1007/BF02902449
1985AU06 Lett.Nuovo Cim. 42, 425 (1985) W.Augustyniak, L.Glowacka, M.Jaskola, J.Turkiewicz, L.Zemlo, J.Dalmas, E.Gadioli, E.Gadioli Erba Structure Effects in (n, α) Reactions on Nd Isotopes NUCLEAR REACTIONS 142,144Nd(n, α), E ≈ 14.2, 18.1 MeV; measured σ(θ), σ(Eα); deduced proton, neutron pairing in target before α emission.
doi: 10.1007/BF02749448
1985MA23 Nucl.Phys. A438, 429 (1985) A.Marinov, W.Oelert, S.Gopal, B.Brinkmoller, G.Hlawatsch, C.Mayer-Boricke, J.Meissburger, D.Paul, M.Rogge, J.G.M.Romer, J.L.Tain, P.Turek, L.Zemlo, R.B.M.Mooy, P.W.M.Glaudemans, S.Brant, V.Paar, M.Vouk, V.Lopac Proton-Hole States in 57Co Studied with the 58Ni(d, 3He)57Co Reaction at 78 MeV NUCLEAR REACTIONS 58Ni(d, 3He), E=78 MeV; measured σ(E(3He)), σ(θ). 57Co deduced levels L, spectroscopic factors. DWBA analysis, shell model, particle-vibration model calculations.
doi: 10.1016/0375-9474(85)90384-7
1984DE22 Phys.Lett. 141B, 49 (1984) P.Decowski, H.P.Morsch, M.Rogge, P.Turek, L.Zemlo, G.Gaul, R.Glasow, B.Ludewigt, R.Santo, W.Schumacher Importance of Fast Nucleon Emission in 172 MeV α Scattering From 238U NUCLEAR REACTIONS 238U(α, α'F), (α, α'p), E=172 MeV; measured fission (fragment)(fragment)(θ) vs Eα, σ(θα, θp, Eα), αp-coin, energy sharing spectra; deduced fission mechanism. 238U deduced momentum transfer.
doi: 10.1016/0370-2693(84)90556-2
1984MA60 Nucl.Phys. A431, 317 (1984) A.Marinov, W.Oelert, S.Gopal, G.P.A.Berg, J.Bojowald, W.Hurlimann, I.Katayama, S.A.Martin, C.Mayer-Boricke, J.Meissburger, J.G.M.Romer, M.Rogge, J.L.Tain, P.Turek, L.Zemlo, R.B.M.Mooy, P.W.M.Glaudemans, S.Brant, V.Paar, M.Vouk, V.Lopac Study of Proton-Hole States in 61Co using the 62Ni(d, 3He)61Co Reaction at 78 MeV NUCLEAR REACTIONS 62Ni(d, 3He), E=78 MeV; measured σ(E(3He)), σ(θ). 61Co deduced levels. DWBA analysis, shell, particle-vibration models.
doi: 10.1016/0375-9474(84)90178-7
1983MO17 Phys.Rev. C28, 1947 (1983) H.P.Morsch, P.Decowski, M.Rogge, P.Turek, L.Zemlo, S.A.Martin, G.P.A.Berg, W.Hurlimann, J.Meissburger, J.G.M.Romer Isoscalar Giant Resonances on 208Pb - in Particular 2(h-bar x omega) L = 0, 2, 4, and 6 Excitations - Studied in Small Angle α Scattering NUCLEAR REACTIONS 208Pb(α, α'), E=172 MeV; measured σ(θ). 208Pb deduced giant resonances, T, Γ, L, EWSR, multipolarity.
doi: 10.1103/PhysRevC.28.1947
1982MO27 Phys.Lett. 119B, 311 (1982) H.P.Morsch, M.Rogge, P.Turek, P.Decowski, L.Zemlo, C.Mayer-Boricke, S.A.Martin, G.P.A.Berg, I.Katayama, J.Meissburger, J.G.M.Romer, J.Reich, P.Wucherer, W.Brautigam The Giant Octupole Resonance in Deformed Nuclei NUCLEAR REACTIONS 120Sn, 140Ce, 159Tb, 169Tm, 175Lu, 181Ta, Pt, 208Pb, 232Th, 238U(α, α'), E=172 MeV; measured σ(Eα') vs θ; deduced giant octupole excitation mass dependence. 120Sn, 140Ce, 159Tb, 169Tm, 175Lu, 181Ta, Pt, 208Pb, 232Th, 238U deduced giant octupole parameters, EWSR. DWBA analysis.
doi: 10.1016/0370-2693(82)90677-3
1982ZE03 Nucl.Phys. A380, 493 (1982) L.Zemlo, W.Drenckhahn, A.Feigel, E.Finckh, K.Ruskamp, P.Urbainsky, M.Wangler The 209Bi(d, γ)211,211mPo Reaction NUCLEAR REACTIONS, ICPND 209Bi(d, γ), E=8-11.5 MeV; measured σ(E), (ground state)σ/(isomer)σ. 211,211mPo deduced γ, particle emission branching ratio.
doi: 10.1016/0375-9474(82)90573-5
1981AU09 Izv.Akad.Nauk SSSR, Ser.Fiz. 45, 2172 (1981) V.Augustynyak, L.Glovatska, Zh.Dalmas, L.Zemlo, Ya.Turkevich, M.Yaskula, Le Van Khoi Study of Energy and Angular Distribution of α-Particles in the Reaction 143Nd(n, α)140Ce Induced by Fast Neutrons NUCLEAR REACTIONS 143Nd(n, α), E=12.3, 14.1, 16 MeV; measured σ(θ), σ(θ, Eα). Quasifree scattering model. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset30477. 1981GA30 Phys.Rev. C24, 2331 (1981) E.Gadioli, E.Gadioli Erba, L.Glowacka, M.Jaskola, J.Turkiewicz, L.Zemlo Influence of the Shell Structure of the Target Nucleus on α Emission in (Nucleon, α) Reactions NUCLEAR REACTIONS 143Nd(n, α), E=12-18 MeV; measured σ(Eα, E), σ(Eα, θ); deduced reaction mechanism, target structure effects.
doi: 10.1103/PhysRevC.24.2331
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
1980AU05 Izv.Akad.Nauk SSSR, Ser.Fiz. 44, 159 (1980); Bull.Acad.Sci.USSR, Phys.Ser. 44, No.1, 131 (1980) V.Augustynyak, L.Glowacka, L.Zemlo, J.Turkiewicz, M.Jaskola, Le Van Khoi Nonstatistical Effects in the Reaction 149Sm(n, α)146Nd NUCLEAR REACTIONS 149Sm(n, α), E=12.3, 14.1, 18.3 MeV; measured σ(E, Eα); deduced non-statistical effects.
1980DR03 Nucl.Phys. A339, 13 (1980) W.Drenckhahn, A.Feigel, E.Finckh, G.Gademann, K.Ruskamp, M.Wangler, L.Zemlo Investigation of the Sn(p, p0) and (p, n) Reaction at Sub-Coulomb Energies NUCLEAR REACTIONS 116,118,120,122,124Sn(p, n), E=4-10 MeV; measured σ(E). 116,120,124Sn(polarized p, p), E=7.75, 8.80 MeV; 120Sn(polarized p, p), E-6.77 MeV; measured A(θ); deduced optical-model parameters. Enriched targets.
doi: 10.1016/0375-9474(80)90238-9
1979GL02 Nucl.Phys. A329, 215 (1979) L.Glowacka, M.Jaskola, J.Turkiewicz, L.Zemlo, M.Kozlowski Study of the 147Sm(n, α)144Nd Reaction Induced by Fast Neutrons NUCLEAR REACTIONS 147Sm(n, α), E=12.4, 14.1, 18.2 MeV; measured σ(Eα), σ(θ). Enriched target.
doi: 10.1016/0375-9474(79)90290-2
1977AU11 Izv.Akad.Nauk SSSR, Ser.Fiz. 41, 2202 (1977); Bull.Acad.Sci.USSR, Phys.Ser. 41, No.10, 180 (1977) V.Augustyniak, L.Glowacka, L.Zemlo, M.Kozlowski, J.Turkiewicz, M.Jaskola Mechanism of the Fast-Neutron Reaction 143Nd(n, α)140Ce NUCLEAR REACTIONS 143Nd(n, α), E=14, 18 MeV; measured σ(Eα, θ).
1977GL04 Nucl.Phys. A284, 257 (1977) L.Glowacka, M.Jaskola, J.Turkiewicz, L.Zemlo, M.Kozlowski, W.Osakiewicz Investigation of α-Particle Emission from the Interactions of Fast Neutrons with 161Dy and 163Dy Nuclei NUCLEAR REACTIONS 161Dy, 163Dy(n, α), E=14.12, 18.18 MeV; measured σ(Eα).
doi: 10.1016/0375-9474(77)90121-X
1976GL04 Nucl.Phys. A262, 205 (1976) L.Glowacka, M.Jaskola, J.Turkiewicz, L.Zemlo, M.Kozlowski, W.Osakiewicz Energy Distributions of Alpha Particles Emitted in 171Yb(n, α)168Er and 173Yb(n, α)170Er Reactions at 14 and 18 MeV NUCLEAR REACTIONS 171,173Yb(n, α), E=14.12, 18.18 MeV; measured σ(Eα).
doi: 10.1016/0375-9474(76)90614-X
1975GL04 Nucl.Phys. A244, 117 (1975) L.Glowacka, M.Jaskola, J.Turkiewicz, L.Zemlo, M.Kozlowski, W.Osakiewicz A Study of the (n, α) Reactions Induced by 18 MeV Neutrons in 151Eu, 153Eu, 159Tb, 165Ho and 169Tm NUCLEAR REACTIONS 151Eu, 153Eu, 159Tb, 165Ho, 169Tm(n, α), E=18.15 MeV;measured σ(Eα). 165Ho(n, α), E=18.15 MeV; measured σ(θ).
doi: 10.1016/0375-9474(75)90011-1
1973GL04 Can.J.Phys. 51, 1765 (1973) L.Glowacka, M.Jaskola, M.Kozlowski, W.Osakiewicz, J.Turkiewicz, L.Zemlo Knock-on Mechanism for (n, α) Reactions Induced by Fast Neutrons on the Deformed Odd-Even Nuclei NUCLEAR REACTIONS 153Eu, 159Tb, 169Tm(n, α), E=14 MeV; calculated σ(Eα).
1972KO09 Nucl.Phys. A187, 177 (1972) M.Kozlowski, L.Glowacka, M.Jaskola, W.Osakiewicz, J.Turkiewicz, L.Zemlo On the Knock-on Mechanism for (n, α) Reactions Induced by Fast Neutrons on the Deformed Doubly Even Nuclei NUCLEAR REACTIONS 160,162,164Dy, 166Er, 168Er(n, α), E=14 MeV; calculated σ(Eα). Feynman triangular diagrams.
doi: 10.1016/0375-9474(72)90082-6
1971JA23 Acta Phys.Pol. B2, 521 (1971) M.Jaskola, J.Turkiewicz, L.Zemlo, W.Osakiewicz (n, α) Reactions on Heavy Nuclei Induced by 14.2 MeV Neutrons NUCLEAR REACTIONS 122Te, 139La, 159Tb, 160,161,163Dy, 164Dy, 166,168Er, 169Tm(n, α), E=14.2 MeV; measured σ(Eα); deduced inadequacy of evaporation theory. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset30158. Back to query form |