NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = F.Malaguti Found 39 matches. 2010DR03 Int.J.Mod.Phys. E19, 1227 (2010) V.A.Drozdov, D.O.Eremenko, O.V.Fotina, S.Yu.Platonov, O.A.Yuminov, G.Giardina, G.Fazio, F.Malaguti, P.Olivo, V.Togo Fission time of α-induced reactions measured by the crystal blocking technique NUCLEAR REACTIONS 232Th, 235U(α, xnf), E<33 MeV; measured reaction products; deduced fission probabilities, anysotropy σ(θ), temperature dependence of nuclear viscosity.
doi: 10.1142/S0218301310015710
2009DE22 Bull.Rus.Acad.Sci.Phys. 73, 835 (2009); Izv.Akad.Nauk RAS, Ser.Fiz 73, 882 (2009) A.A.Dermenev, V.A.Drozdov, D.O.Eremenko, F.Malaguti, P.Olivo, S.Yu.Platonov, V.Togo, A.Uguzzoni, O.V.Fotina, O.A.Yuminov Dynamical analysis of the induced fission time obtained by the crystal blocking technique for the 235U + α reaction NUCLEAR REACTIONS 235U(α, F), E=25.9-31.2 MeV; measured angular distribution of fission fragments; deduced fission lifetime, fissionabilities of Pu isotopes. Comparison with theoretical calculations.
doi: 10.3103/S106287380906029X
2009YU02 Nucl.Instrum.Methods Phys.Res. B267, 2592 (2009) O.A.Yuminov, A.M.Borisov, V.A.Drozdov, D.O.Eremenko, O.V.Fotina, F.Malaguti, P.Olivo, S.Yu.Platonov, V.Togo, A.F.Tulinov Fission time for the 235U + α reaction measured by the crystal blocking technique NUCLEAR REACTIONS 235U(α, F), E=25.9-31.2 MeV; measured angular distribution of fission fragments; deduced fission lifetime, fissionabilities of Pu isotopes. Comparison with theoretical calculations.
doi: 10.1016/j.nimb.2009.05.018
2008AN14 Phys.Rev. C 78, 064609 (2008) J.U.Andersen, J.Chevallier, J.S.Forster, S.A.Karamian, C.R.Vane, J.R.Beene, A.Galindo-Uribarri, J.Gomez del Campo, C.J.Gross, H.F.Krause, E.Padilla-Rodal, D.Radford, D.Shapira, C.Broude, F.Malaguti, A.Uguzzoni Attosecond time delays in heavy-ion induced fission measured by crystal blocking NUCLEAR REACTIONS W(32S, 32S), (32S, X), E=180 MeV; W(48Ti, 48Ti), (48Ti, X), E=240-255 MeV; W(58Ni, 58Ni), (58Ni, 58Ni'), (58Ni, X), E=330-375 MeV; W(74Ge, 74Ge), (74Ge, X), E=390 MeV; measured fission energy spectra, σ; calculated blocking dips. Continuum model calculations.
doi: 10.1103/PhysRevC.78.064609
2007AN29 Phys.Rev.Lett. 99, 162502 (2007) J.U.Andersen, J.Chevallier, J.S.Forster, S.A.Karamian, C.R.Vane, J.R.Beene, A.Galindo-Uribarri, J.Gomez del Campo, H.F.Krause, E.Padilla-Rodal, D.Radford, C.Broude, F.Malaguti, A.Uguzzoni Crystal Blocking Measurements of the Time Delay of Fission Induced by 32S, 48Ti, and 58Ni Bombardment of W NUCLEAR REACTIONS W(32S, F), E=180 MeV; W(48Ti, F), E=240-255 MeV; W(58Ni, F), E=315-375 MeV; measured fission yields. Deduced fission delay.
doi: 10.1103/PhysRevLett.99.162502
2004DR03 Nucl.Phys. A734, 225 (2004) V.A.Drozdov, D.O.Eremenko, O.V.Fotina, G.Giardina, F.Malaguti, S.Yu.Platonov, O.A.Yuminov Decay time of heavy excited nuclei NUCLEAR REACTIONS 232Th(p, xnF), (d, xnF), (α, xnF), E* ≈ 10-250 MeV; analyzed induced fission lifetimes. 238U(α, F), E=20-120 MeV; 232Th, 238U, 248Cm(16O, F), E=80-160 MeV; analyzed fission fragments angular anisotropy.
doi: 10.1016/j.nuclphysa.2004.01.040
2003KA15 Eur.Phys.J. A 17, 49 (2003) S.A.Karamian, J.S.Forster, J.U.Andersen, W.Assmann, C.Broude, J.Chevallier, J.S.Geiger, F.Gruner, V.A.Khodyrev, F.Malaguti, A.Uguzzoni Fission lifetimes of Th nuclei measured by crystal blocking NUCLEAR REACTIONS W(32S, 32S), (32S, F), E=170-180 MeV; measured scattered particle and fission fragment spectra, blocking pattern due to target crystal; deduced fission lifetime features. 214Th calculated compound nucleus T1/2, fission probability vs energy, spin. Crystal blocking technique.
doi: 10.1140/epja/i2002-10139-0
2002DR07 Nucl.Instrum.Methods Phys.Res. B193, 846 (2002) V.A.Drozdov, D.O.Eremenko, O.V.Fotina, G.Giardina, F.Malaguti, S.Yu.Platonov, A.F.Tulinov, O.A.Yuminov Crystal Blocking Measurements of the Induced Fission Time in the 232Th + p and 232Th + 3He Reactions NUCLEAR REACTIONS 232Th(p, F), E=6.8-7.8 MeV; 232Th(3He, F), E=20.8-23.4 MeV; measured mean fission lifetime vs excitation energy; deduced shell effects. 232,233Pa deduced level densities in second potential well. Crystal blocking technique, statistical model analysis.
doi: 10.1016/S0168-583X(02)00914-X
2002ER01 Yad.Fiz. 65, 20 (2002); Phys.Atomic Nuclei 65, 18 (2002) D.O.Eremenko, O.V.Fotina, G.Giardina, A.Lamberto, F.Malaguti, S.Yu.Platonov, A.Taccone, O.A.Yuminov Fission Time in the 28Si + natPt Reaction NUCLEAR REACTIONS Pt(28Si, F), E=140-170 MeV; measured fission fragment energies and angular distributions; deduced induced fission delay times, fission barrier features. 196Pt(28Si, F), E=140-170 MeV; calculated neutron spectra, fragment yields. Crystal-blocking technique.
doi: 10.1134/1.1446550
2001YU04 J.Phys.Soc.Jpn. 70, 689 (2001) O.A.Yuminov, S.Yu.Platonov, D.O.Eremenko, O.V.Fotina, E.Fuschini, F.Malaguti, G.Vannini, G.Giardina, G.Fazio, A.Lamberto, A.Taccone, A.Moroni, E.Fioretto, R.A.Ricci, L.Vannucci, R.Palamara Experimental Evidence of Shell Effects in the Fission Time of Heavy Nuclei NUCLEAR REACTIONS Pt(28Si, F), E=140-170 MeV; measured fission fragments angular distributions, decay time; deduced fission barrier features. Crystal blocking technique.
doi: 10.1143/JPSJ.70.689
1998DA27 Bull.Rus.Acad.Sci.Phys. 62, 1736 (1998) P.d'Agostino, G.Fazio, G.Giardina, M.Herman, A.Lamberto, G.F.Rappazzo, R.Sturiale, F.Malaguti, D.O.Eremenko, N.V.Eremin, S.Yu.Platonov, O.A.Yuminov Effect of Nuclear Deformation on Giant Dipole Resonances NUCLEAR STRUCTURE A=51-239; analyzed GDR parameters vs deformation. NUCLEAR REACTIONS 154Sm(12C, X), 27Al, 109Ag(18O, X), E not given; analyzed Eγ, Iγ; deduced GDR deformation effects.
1998EG02 Bull.Rus.Acad.Sci.Phys. 62, 834 (1998) I.M.Egorova, D.O.Eremenko, S.Yu.Platonov, O.A.Yuminov, F.Malaguti, A.Uguzzoni, G.Forster Angular Correlations of Fission Fragments in the Study of Nuclear Reaction Mechanisms NUCLEAR REACTIONS 2H(238U, 239U), E=5 MeV/nucleon; calculated fragment energy, angular distributions following projectile fission. Stopping method.
1998ER09 Bull.Rus.Acad.Sci.Phys. 62, 721 (1998) D.O.Eremenko, Yu.L.Parfenova, S.Yu.Platonov, O.V.Fotina, O.A.Yuminov, E.Fuschini, F.Malaguti, A.D'Arrigo, G.Giardina, R.Sturiale, G.Vannini, A.Moroni, E.Fioretto, R.A.Ricci, L.Vannucci Shell Effects in Fusion-Fission Nucleus-Nucleus Reactions NUCLEAR REACTIONS Pt(28Si, X), E=140-170 MeV; measured fission time scale; deduced fission barrier features, shell effects. Blocking technique.
1997ER08 Bull.Rus.Acad.Sci.Phys. 61, 18 (1997) D.O.Eremenko, G.Giardina, F.Malaguti, B.Mellado, S.Yu.Platonov, O.V.Fotina, O.A.Yuminov Angular Distributions of Fission Fragments of Nuclei with Two Types of Excited States NUCLEAR REACTIONS 238U(α, F), E=37, 43 MeV; calculated fission fragment σ(θ); deduced viscosity, energy dependence. Halpern-Strutinsky model.
1996EG02 Bull.Rus.Acad.Sci.Phys. 60, 772 (1996) I.M.Egorova, D.O.Eremenko, F.Malaguti, S.Yu.Platonov, O.V.Fotina, O.A.Yuminov Slowing-Down Method for Investigating the Near-Barrier Fission of Heavy Nuclei NUCLEAR STRUCTURE 239U; calculated fission fragments energy spectra, product yields time dependence, different decay channels durations. 266Sg; calculated induced fission duration energy dependence. Slowing down method. NUCLEAR REACTIONS 32S(238U, α), E=5.5 MeV/nucleon; calculated residual nucleus fission fragment spectra. 90Zr(180W, α), E=5.5 MeV/nucleon; calculated α-spectra. Slowing down method. RADIOACTIVITY 266Cn(α) [from 90Zr(180W, α), E=5.5 MeV/nucleon]; calculated α-spectra. Slowing down method.
1996ER02 J.Phys.(London) G22, 1077 (1996) D.O.Eremenko, B.Mellado, S.Yu.Platonov, O.V.Fotina, O.A.Yuminov, G.Giardina, G.F.Rappazzo, F.Malaguti Fragment Angular Distribution as a Probe of Fission Dynamics in Nuclei with Two Classes of Excited States NUCLEAR REACTIONS 238U(α, F), E=37, 43 MeV; analyzed fission fragment σ(θ), other data; deduced Pu isotopes reduced dissipation coefficient. Multi-chance fission, double humped fission barrier.
doi: 10.1088/0954-3899/22/7/013
1995DA06 Nucl.Phys. A583, 157c (1995) A.D'Arrigo, N.V.Eremin, E.Fioretto, E.Fuschini, G.Giardina, F.Malaguti, A.Moroni, R.A.Ricci, A.Taccone, G.Vannini, L.Vannucci, O.A.Yuminov Crystal Blocking: Experimental evidence of long delay times in the reaction induced on nickel by oxygen ions NUCLEAR REACTIONS Ni(16O, X), E=135 MeV; measured nuclear time delays for fragment Z=13-18. Crystal blocking techniques. Different model analyses.
doi: 10.1016/0375-9474(94)00652-4
1995DA31 Int.J.Mod.Phys. E4, 443 (1995) A.D'Arrigo, G.Giardina, A.Lamberto, D.O.Eremenko, O.V.Fotina, S.Yu.Platonov, O.A.Yuminov, F.Malaguti The Probability of Populating the Second Potential Well States in Fission Dynamics NUCLEAR STRUCTURE 239,238,235,236Np, 237,238,240Pu, 232,233Pa; calculated second well states population probability, double-humped fission barriers; deduced parameters. Fission diffusion model.
doi: 10.1142/S021830139500016X
1995ER02 Nucl.Phys. A589, 395 (1995) D.O.Eremenko, V.O.Kordyukevich, S.Yu.Platonov, O.V.Fotina, O.A.Yuminov, G.Giardina, F.Malaguti, G.Vannini Lifetime Measurement of Fissionable Nuclei Produced in the Development of Neutron Emission (III) Lifetime of Protactinium Isotopes NUCLEAR REACTIONS 232Th(d, xnF), E=8-15.6 MeV; measured fission fragment σ(θ). 233,232Pa deduced fission characteristics, T1/2. Blocking technique.
doi: 10.1016/0375-9474(95)00169-2
1995ER04 Bull.Rus.Acad.Sci.Phys. 59, 135 (1995) D.O.Eremenko, S.Yu.Platonov, O.V.Fotina, O.A.Yuminov, E.Fuschini, F.Malaguti, G.Vannini, A.Moroni, R.A.Ricci, L.Vannucci, A.d'Arrigo, G.Giardina, A.Taccone Possible Measurement of Excited State Lifetimes in Resonance Reactions on Light Nuclei by the Method Based on Stopping Effect NUCLEAR REACTIONS 7Li(16O, α), (16O, t), E=120 MeV; measured α-spectra following residuals α-decay. 19F, 20Ne level deduced α-decay T1/2 estimates, Γα/Γ. Fast charged particle energy loss technique.
1995ER09 Nuovo Cim. 108, 883 (1995) D.O.Eremenko, O.V.Fotina, G.Giardina, A.Lamberto, F.Malaguti, S.Yu.Platonov, R.Sturiale, O.A.Yuminov Level Density Dependence of the Transient States on the Nuclear Shape Symmetry in Fissionable Nuclei NUCLEAR STRUCTURE 232,233Pa, 235,236,238,239Np; calculated level density in second potential well.
doi: 10.1007/BF02731028
1995YU04 J.Phys.(London) G21, 1243 (1995) O.A.Yuminov, S.Yu.Platonov, O.V.Fotina, D.O.Eremenko, F.Malaguti, G.Giardina, A.Lamberto Statistical Description of the Decay of Nuclei Having Two Classes of Excited States NUCLEAR STRUCTURE 233Pa, 239Np; calculated mean fission time vs mean excitation energy. 238,239Np; calculated decay time characteristics, other fission characteristics. 236,235,238,239Np, 233,232Pa, 238,240Pu; calculated induced fission time delay vs minimum fission barrier, second well depth energies difference. Statistical theory, double-humped fission barrier model, comparison with data.
doi: 10.1088/0954-3899/21/9/010
1995YU05 Nucl.Instrum.Methods Phys.Res. B95, 543 (1995) O.A.Yuminov, S.Yu.Platonov, D.O.Eremenko, N.V.Eremin, I.M.Egorova, V.O.Kordyukevich, O.V.Fotina, F.Malaguti, A.D'Arrigo, G.Giardina, A.Taccone, G.Vannini, A.Moroni, R.A.Ricci, L.Vannucci A Novel Experimental Technique of Nuclear Lifetime Measurements NUCLEAR REACTIONS 7Li(16O, α), (16O, t), E=120 MeV; measured α-spectra. 19F, 20Ne levels deduced T1/2, Γα/Γ. Layered target technique, comparison with other methods.
doi: 10.1016/0168-583X(94)00602-4
1994FU08 Phys.Rev. C50, 1964 (1994) E.Fuschini, F.Malaguti, E.Fioretto, R.A.Ricci, L.Vannucci, A.D'Arrigo, G.Giardina, A.Taccone, A.Moroni, N.Eremin, O.Yuminov, G.Vannini Experimental Observation of Long Delay Times in the Reaction Induced by Oxygen Ions on Nickel Crystals NUCLEAR REACTIONS Ni(16O, X), E=135 MeV; measured axial blocking patterns; deduced delay times for fission-like fragments, Z=13-18. Model for dechanneling due to secondary decay.
doi: 10.1103/PhysRevC.50.1964
1992DA21 J.Phys.(London) G18, 2009 (1992) A.D'Arrigo, G.Giardina, M.Herman, F.Malaguti, A.Taccone, G.Vannini Influence of Angular Momentum on Fission Probability Energy Distribution NUCLEAR REACTIONS 133Cs(16O, F), E=166 MeV; 159Tb(16O, F), E=93-166 MeV; 169Tm(12C, F), 165Ho(16O, F), E not given; calculated fission probability vs excitation; deduced angular momendum role. 28Si(16O, F), E=100 MeV; 28Si(28Si, F), E=150 MeV; calculated compound system fission T1/2.
doi: 10.1088/0954-3899/18/12/016
1992FU05 Phys.Rev. C46, R25 (1992) E.Fuschini, F.Malaguti, S.Ostuni, E.Verondini, G.Vannini, A.Bracco, I.Iori, A.Moroni, E.Fioretto, R.A.Ricci, P.Boccaccio, L.Vannucci, A.D'Arrigo, G.Giardina, A.Taccone Measurements of Mean Reaction Times for Fusion-Fission and Fusion-Evaporation Processes in the 28Si + 28Si Interaction NUCLEAR REACTIONS 28Si(28Si, X), E=150 MeV; measured reaction product axial, planar blocking patterns; deduced fusion-fission, fusion evaporation reaction times.
doi: 10.1103/PhysRevC.46.R25
1991DA22 Nuovo Cim. 104A, 1771 (1991) A.D'Arrigo, G.Giardina, A.Taccone, E.Fuschini, F.Malaguti, E.Verondini, G.Vannini Fission of the 44Ti, 56Ni and 74,76Kr Nuclei Formed by Heavy-Ion Reactions NUCLEAR STRUCTURE 44Ti, 56Ni, 74,76Kr; calculated fission probability, mean T1/2, decay width. Data from 28Si(16O, F), 28Si(28Si, F), 58,60Ni(16O, F) reactions compared with statistical model.
doi: 10.1007/BF02812491
1990MA51 Europhys.Lett. 12, 313 (1990) F.Malaguti, S.Ostuni, E.Verondini, E.Fuschini, G.Vannini, I.Iori, A.Bracco, A.Moroni, E.Fioretto, R.A.Ricci, P.Boccaccio, L.Vannucci Measurement of Nuclear Time Delay for Different Reaction Mechanisms in the 16O + 28Si Interaction NUCLEAR REACTIONS 28Si(16O, X), E=100 MeV; measured fragment spectra blocking dips; deduced fusion-fission, fusion-evaporation mechanism time delays.
doi: 10.1209/0295-5075/12/4/005
1989MA23 Nuovo Cim. 101A, 517 (1989) F.Malaguti, E.Verondini, E.Fuschini, G.Vannini, I.Iori, A.Bracco, A.Moroni, E.Fioretto, R.A.Ricci, P.Boccaccio, L.Vannucci Crystal Blocking Measurement of Time Delays in the 16O + 28Si Reaction NUCLEAR REACTIONS 28Si(16O, X), E=100 MeV; measured blocking pattern, σ(fragment θ) for Z=8, 9, 10, 11, 12, 13 around (110) axis; deduced nuclear time delays.
doi: 10.1007/BF02789435
1983FU02 Phys.Rev. C27, 1332 (1983) E.Fuschini, F.Malaguti, A.Uguzzoni, E.Verondini Blocking Measurement of a Relatively Long Lifetime: 28Si 12.073 MeV level NUCLEAR REACTIONS 27Al(p, α), E=0.505 MeV; measured resonance yield, blocking effect vs displacement. 28Si resonance deduced Γ, T1/2. Single crystal thick target, cellulose nitrate detectors.
doi: 10.1103/PhysRevC.27.1332
1981FU07 Phys.Rev. C23, 2748 (1981) E.Fuschini, F.Malaguti, A.Uguzzoni, E.Verondini Lifetime of the 28Si 12.195 MeV Level NUCLEAR REACTIONS 27Al(p, α), E=0.632 MeV; measured yields. 28Si level deduced T1/2, Γ. Thick single crystal target, LR-115 plastic detectors, axial blocking technique.
doi: 10.1103/PhysRevC.23.2748
1980FU02 Phys.Rev. C21, 1646 (1980) E.Fuschini, F.Malaguti, A.Uguzzoni, E.Verondini Axial Blocking Measurement of the 28Si 12.291 MeV Level Width NUCLEAR REACTIONS 27Al(p, α0), E=0.731 MeV; measured blocking effect. 28Si deduced level width. Single crystal thick Al targets. LR 115 cellulose nitrate detectors.
doi: 10.1103/PhysRevC.21.1646
1979MA10 Nuovo Cim. 49A, 412 (1979) F.Malaguti, A.Uguzzoni, E.Verondini, P.E.Hodgson Charge Density and Single-Particle Structure: the Nuclei 39K, 40Ca and 48Ca NUCLEAR STRUCTURE 39K, 40,48Ca; calculated charge distributions. One-body nonlocal potential.
doi: 10.1007/BF02773455
1979MA12 Phys.Rev. C19, 1606 (1979) F.Malaguti, A.Uguzzoni, E.Verondini Lifetime of the 937- and 885-keV Resonances in the 27Al(p, α) Reaction NUCLEAR REACTIONS 27Al(p, α), E=0.731-1.183 MeV; measured thin-target yields, blocking effect. 28Si resonances deduced T1/2. Single crystal.
doi: 10.1103/PhysRevC.19.1606
1979MA33 Nuovo Cim. 53A, 1 (1979) F.Malaguti, A.Uguzzoni, E.Verondini, P.E.Hodgson The Charge Densities and Single-Particle Structure of the Even Zirconium Isotopes NUCLEAR STRUCTURE 90,92,94Zr; calculated densities, squared one-body potential single-particle functions, weighted by occupation numbers.
1978MA09 Nucl.Phys. A297, 287 (1978) F.Malaguti, A.Uguzzoni, E.Verondini, P.E.Hodgson Charge Density and Single-Particle Structure of 58Ni NUCLEAR STRUCTURE 58Ni; calculated charge distribution.
doi: 10.1016/0375-9474(78)90277-4
1976MA04 Nucl.Phys. A257, 37 (1976) The Systematics of Nuclear Single-Particle States (III). Widths and Rearrangement Energies NUCLEAR STRUCTURE A=6-65; calculated single-particle level widths, rearrangement energies.
doi: 10.1016/0375-9474(76)90473-5
1973MA48 Nucl.Phys. A215, 243 (1973) The Systematics of Nuclear Single-Particle States (II). The Region A < 35 NUCLEAR STRUCTURE 4He, 6,7Li, 9,10Be, 10,11B, 12,13,14C, 14,15N, 16,17,18O, 19F, 20,21,22Ne, 23Na, 24,25,26Mg, 27Al, 28,29,30Si, 31P, 32,33,34S, 35Cl; levels calculated binding energies.
doi: 10.1016/0375-9474(73)90653-2
1972FU17 Nuovo Cim. 10A, 177 (1972) E.Fuschini, F.Malaguti, C.Maroni, I.Massa, A.Uguzzoni, E.Verondini, G.J.Clark Multiple-Scattering Effects in Mean-Lifetime Experiments by Blocking Technique
doi: 10.1007/BF02895756
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