NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = G.Fazio Found 71 matches. 2018GI03 Nucl.Phys. A970, 169 (2018) G.Giardina, G.Mandaglio, A.K.Nasirov, A.Anastasi, F.Curciarello, G.Fazio Uncertainties and understanding of experimental and theoretical results regarding reactions forming heavy and superheavy nuclei COMPILATION Z=102-122; calculated fusion probability of colliding nuclei (target W to Cf, projectile Mg to Kr) to form given composite system and survival probability vs E(cm) and vs angular momentum. Compared with other results and with data. 240Pu(48Ca, n), E*=35.89 MeV; calculated neutron energy spectra σ(En) separately from 285,286,287,288Fl. 240Pu(48Ca, n), (48Ca, p), 240Pu(48Ca, α), E*=40.06 MeV; calculated first emitted n-spectra, p-spectra, α-spectra σ(out).
doi: 10.1016/j.nuclphysa.2017.11.010
2018MA60 Nucl.Phys. A979, 204 (2018) G.Mandaglio, A.K.Nasirov, A.Anastasi, F.Curciarello, G.Fazio, G.Giardina Role of charged particle emission on the evaporation residue formation in the 82Se+138Ba reaction leading to the 220Th compound nucleus NUCLEAR REACTIONS 138Ba(82Se, xnypzα)220Th, E*=12-70 MeV; calculated ER (Evaporation Residue) σ considering both quasifission of DNS (Double-Nuclear System) leading to ER, and the channel via creation of compound nucleus and its decay; deduced calculated total ER σ overpredict available experimental data at some cases.
doi: 10.1016/j.nuclphysa.2018.09.057
2018MA63 Phys.Rev. C 98, 044616 (2018) G.Mandaglio, A.Anastasi, F.Curciarello, G.Fazio, G.Giardina, A.K.Nasirov Effects of entrance channels on the deexcitation properties of the same compound nucleus formed by different pairs of collision partners NUCLEAR REACTIONS 204Pb(16O, X), 180Hf(40Ar, X), 138Ba(82Se, X), 124Sn(96Zr, X)220Th*/219Th*/218Th*/217Th*/216Th*, E*=35.5, 46, 61, 10-75 MeV; calculated partial fusion σ(E) as function of angular momentum effective fission barriers, neutron emission and fission probabilities for the excited 220Th* compound nucleus and isotopes formed after successive neutron evaporation up to emission of four neutron, ratio of evaporation residues with Z>90 and Z=90. 249Cf(48Ca, X)297Og*, E*=22.5-50 MeV; calculated evaporation residue σ(E) for one-neutron as well as charged particle emission.
doi: 10.1103/PhysRevC.98.044616
2012PO11 Phys.Rev. C 85, 064330 (2012) O.M.Povoroznyk, O.K.Gorpinich, O.O.Jachmenjov, H.V.Mokhnach, O.Ponkratenko, G.Mandaglio, F.Curciarello, V.De Leo, G.Fazio, G.Giardina Experimental evidence of the 6He level at E* = 18.3 Mev via the 4He + 3H three-body reaction NUCLEAR REACTIONS 3H(α, 2t)1H, (α, pt)3H, E=67.2 MeV; measured tt-, pt-coin; 4,6He; deduced levels, resonances, widths.
doi: 10.1103/PhysRevC.85.064330
2011NA12 Int.J.Mod.Phys. E20, 406 (2011) A.Nasirov, G.Fazio, G.Giardina, G.Mandaglio, M.Manganaro, A.Muminov Appearance of nuclear shell effects and initial charge (mass) asymmetry in the formation of products of heavy ion collisions NUCLEAR REACTIONS 249Cf(50Ti, X), 248Cm(54Cr, X), E(cm)<260 MeV; calculated σ, fission barrier. Comparison with experimental data.
doi: 10.1142/S021830131101779X
2011PO10 J.Phys.Soc.Jpn. 80, 094204 (2011) O.Povoroznyk, O.K.Gorpinich, O.O.Jachmenjov, H.V.Mokhnach, O.Ponkratenko, G.Mandaglio, F.Curciarello, V.De Leo, G.Fazio, G.Giardina High-Lying 6Li Levels at Excitation Energy of around 21 MeV NUCLEAR REACTIONS 3H(α, nt)3He, E=67.2 MeV; measured reaction products, Eα, Iα. 6Li; deduced higher lying states in 6Li, resonances. Comparison with experimental data.
doi: 10.1143/JPSJ.80.094204
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
2010ER04 Int.J.Mod.Phys. E19, 1183 (2010) N.V.Eremin, A.A.Paskhalov, S.S.Markochev, E.A.Tsvetkov, G.Mandaglio, M.Manganaro, G.Fazio, G.Giardina, M.V.Romaniuk New experimental method of investigation the rare nuclear transformations accompanying atomic processes: bremsstrahung emission in spontaneous fission of 252Cf RADIOACTIVITY 252Cf(SF); measured Eγ, Iγ, γγ-coin., neutron-γ-coin.; deduced high-energy bremsstrahlung emission during spontaneous fission, energy spectrum of photons.
doi: 10.1142/S0218301310015655
2010GI04 Int.J.Mod.Phys. E19, 882 (2010) G.Giardina, G.Fazio, G.Mandaglio, M.Manganaro, A.K.Nasirov, M.V.Romaniuk, C.Sacca Expectations and limits to synthesize nuclei with Z ≥ 120 NUCLEAR REACTIONS 124,132Sn(96Zr, X), 136Xe(86Kr, X), (136Xe, X), 174Yb(48Ca, X), (132Sn, X), 182W(32S, X), 181Ta(40Ar, X), 208Pb(32S, X), (48Ca, X), (50Ti, X), (58Fe, X), (86Kr, X), 238U(16O, X), (64Ni, X), 226Ra(48Ca, X), 248Cm(26Mg, X), (48Ca, X), (54Cr, X), 243Am(48Ca, X), 248Bk(48Ca, X), 249Cf(48Ca, X), (54Cr, X), (64Ni, X), 244Pu(58Fe, X), 176Hf(132Sn, X), 186W(132Sn, X), 232Th(84Kr, X), E not given; calculated evaporation residue σ, fusion probabilities; deduced projectile restrictions for synthesis of super-heavy elements.
doi: 10.1142/S0218301310015333
2010MA28 Int.J.Mod.Phys. E19, 1189 (2010) S.P.Maydanyuk, V.S.Olkhovsky, G.Mandaglio, M.Manganaro, G.Fazio, G.Giardina Bremsstrahlung emission accompanying decays and spontaneous fission of heavy nuclei RADIOACTIVITY 252Cf(SF), 226Ra(α); calculated bremsstrahlung emission during spontaneous fission. Comparison with experiment.
doi: 10.1142/S0218301310015667
2010MA34 Phys.Rev. C 82, 014602 (2010) S.P.Maydanyuk, V.S.Olkhovsky, G.Mandaglio, M.Manganaro, G.Fazio, G.Giardina Bremsstrahlung emission of high energy accompanying spontaneous fission of 252Cf RADIOACTIVITY 252Cf(SF); calculated bremsstrahlung photon emission probabilities obtained for the participation of 4He, 9Be, 12C, 24Mg, 95Zr, 97Nb, 100Mo, 103Tc, 105Ru, 110,115Rh fragments during the spontaneous fission process. 214Po, 226Ra, 252Cf(α); calculated bremsstrahlung photon emission probabilities. Fully quantum approach using the spherical wave approximation for the description of photon wave functions. Comparison with experimental data.
doi: 10.1103/PhysRevC.82.014602
2010NA09 Phys.Lett. B 686, 72 (2010) A.K.Nasirov, G.Mandaglio, M.Manganaro, A.I.Muminov, G.Fazio, G.Giardina Quasifission and difference in formation of evaporation residues in the 16O + 184W and 19F + 181Ta reactions NUCLEAR REACTIONS 181Ta(19F, X), 184W(16O, X), E(cm)=65-120 MeV; analyzed fusion, fission and evaporation residue σ, ratios and reaction mechanism features, L-dependence using statistical model for a dinuclear system.
doi: 10.1016/j.physletb.2010.02.018
2009MA14 Nucl.Phys. A823, 38 (2009) S.P.Maydanyuk, V.S.Olkhovsky, G.Giardina, G.Fazio, G.Mandaglio, M.Manganaro Bremsstrahlung emission accompanying α-decay of deformed nuclei RADIOACTIVITY 226Ra(α); calculated bremsstrahlung emission probability, spectrum, angular distribution including effect of nuclear deformation. Comparison with earlier results and data.
doi: 10.1016/j.nuclphysa.2009.03.007
2009NA14 Int.J.Mod.Phys. E18, 841 (2009) A.Nasirov, G.Fazio, G.Giardina, G.Mandaglio, M.Manganaro, F.Hanappe, A.Muminov, W.Scheid Comparison of the fusion-fission and quasifission mechanism in heavy-ion collisions
doi: 10.1142/S021830130901294X
2009NA38 Bull.Rus.Acad.Sci.Phys. 73, 1476 (2009); Izv.Akad.Nauk RAS, Ser.Fiz. 73, 1571 (2009) A.K.Nasirov, G.Fazio, S.Hofmann, G.Giardina, A.I.Muminov, G.Mandaglio, M.Manganaro, W.Scheid Comparison of the characteristics of the fusion-fission and quasifission products in reactions with heavy ions NUCLEAR REACTIONS 154Sm(48Ca, X), 248Cm(54Cr, X), 244Pu(58Fe, X), 238U(64Ni, X) E(cm)<280 MeV; analyzed fusion-fission product mass distribution, yields, σ for heavy ion reactions;calculated σ; deduced large value of σ of evaporation residues in the 248Cm + 54Cr reaction.
doi: 10.3103/S1062873809110112
2008GI03 Eur.Phys.J. A 36, 31 (2008) G.Giardina, G.Fazio, G.Mandaglio, M.Manganaro, C.Sacca, N.V.Eremin, A.A.Paskhalov, D.A.Smirnov, S.P.Maydanyuk, V.S.Olkhovsky Bremsstrahlung emission accompanying the α -decay of 214Po RADIOACTIVITY 214Po(α); measured Eα, Iα, Eγ, Iγ, αγ-coin; deduced bremsstrahlung emission probability vs Eγ, K-shell ionization probabilities. Comparison with quantum-mechanical model.
doi: 10.1140/epja/i2007-10548-5
2007NA34 Eur.Phys.J. A 34, 325 (2007) A.K.Nasirov, A.I.Muminov, R.K.Utamuratov, G.Fazio, G.Giardina, F.Hanappe, G.Mandaglio, M.Manganaro, W.Scheid Angular anisotropy of the fusion-fission and quasifission fragments NUCLEAR REACTIONS 238U(16O, X), E=80-160 MeV; 208Pb(19F, X), E(cm)=70-180 MeV; 208Pb(32S, X), E=160-280 MeV; analyzed capture, fusion and quasi-fission σ, angular anisotropy of fission fragments and charge distribution. Reaction mechanism discussed.
doi: 10.1140/epja/i2007-10504-5
2005FA01 J.Phys.Soc.Jpn. 74, 307 (2005) G.Fazio, G.Giardina, A.Lamberto, C.Sacca, R.Palamara, A.I.Muminov, A.K.Nasirov, K.V.Pavliy, F.Hanappe, T.Materna, L.Stuttge Effect of the Entrance Channel on the Fission of the Compound Nucleus NUCLEAR REACTIONS 204Pb(16O, X), 124Sn(96Zr, X), 234U(20Ne, X), 176Yb(78Ge, X), 232U(24Mg, X), 192Os(64Ni, X), E* ≈ 10-100 MeV; calculated fusion σ, evaporation residue production, compound nucleus fission probability; deduced entrance channel effects.
doi: 10.1143/JPSJ.74.307
2005FA17 Phys.Rev. C 72, 064614 (2005) G.Fazio, G.Giardina, G.Mandaglio, R.Ruggeri, A.I.Muminov, A.K.Nasirov, Yu.Ts.Oganessian, A.G.Popeko, R.N.Sagaidak, A.V.Yeremin, S.Hofmann, F.Hanappe, C.Stodel Strong influence of the entrance channel on the formation of compound nuclei 216, 222Th* and their evaporation residues NUCLEAR REACTIONS 176Hf(40Ar, X), 130,136Xe(86Kr, X), 92Zr(124Sn, X), 174Yb(48Ca, X), E* ≈ 10-100 MeV; calculated capture and complete fusion σ; analyzed evaporation residue σ, related data; deduced entrance channel effects.
doi: 10.1103/PhysRevC.72.064614
2004FA03 Eur.Phys.J. A 19, 89 (2004) G.Fazio, G.Giardina, A.Lamberto, R.Ruggeri, C.Sacca, R.Palamara, A.I.Muminov, A.K.Nasirov, U.T.Yakhshiev, F.Hanappe, T.Materna, L.Stuttge Formation of heavy and superheavy elements by reactions with massive nuclei NUCLEAR REACTIONS 182W(32S, X), 166Er(48Ti, X), 154Sm(60Ni, X), E* ≈ 30-110 MeV; 181Ta(40Ar, X), E* ≈ 160-220 MeV; 248Cm(48Ca, X), E* ≈ 220-280 MeV; analyzed capture, fusion, evaporation residue σ; deduced entrance channel and shell structure effects. 248Cm, 243Am, 249Cf(48Ca, 2n), (48Ca, 3n), (48Ca, 4n), (48Ca, 5n), E=220-270 MeV; calculated excitation functions.
doi: 10.1140/epja/i2003-10103-6
2004FA29 Eur.Phys.J. A 22, 75 (2004) G.Fazio, G.Giardina, A.Lamberto, A.I.Muminov, A.K.Nasirov, F.Hanappe, L.Stuttge The influence of the entrance channel dynamics on the evaporation residue formation NUCLEAR REACTIONS 204Pb(16O, X), 124Sn(96Zr, X), E* ≈ 10-100 MeV; calculated fusion, fission, evaporation residue σ; deduced entrance channel effects.
doi: 10.1140/epja/i2004-10030-0
2004GI11 Acta Phys.Hung.N.S. 19, 101 (2004) G.Giardina, G.Fazio, A.Lamberto, A.I.Muminov, A.K.Nasirov, U.T.Yakhshiev, R.Palamara, R.Ruggeri Reactions of Massive Nuclei for the Synthesis of Heavy and Superheavy Nuclei NUCLEAR REACTIONS 182W(32S, X), 166Er(48Ti, X), 154Sm(60Ni, X), 248Cm(48Ca, X), E* ≈ 20-130 MeV; analyzed fusion, evaporation residue σ, entrance channel effects.
doi: 10.1556/APH.19.2004.1-2.15
2003FA08 Yad.Fiz. 66, 1107 (2003); Phys.Atomic Nuclei 66, 1071 (2003) G.Fazio, G.Giardina, A.Lamberto, R.Ruggeri, F.Bonsignore, R.Palamara, A.I.Muminov, A.K.Nasirov, B.Benoit, F.Hanappe, T.Materna, L.Stuttge Synthesis of Heavy and Superheavy Elements by Reactions of Massive Nuclei NUCLEAR REACTIONS 176Hf(40Ar, X), 92Zr(124Sn, X), 130Xe(86Kr, X), 182W(32S, X), 154Sm(60Ni, X), 248Cm(48Ca, X), E* ≈ 20-100 MeV; analyzed capture, fusion, and evaporation residue σ; deduced entrance channel effects. Dinuclear system approach.
doi: 10.1134/1.1586420
2003FA12 J.Phys.Soc.Jpn. 72, 2509 (2003) G.Fazio, G.Giardina, A.Lamberto, R.Ruggeri, C.Sacca, R.Palmara, A.I.Muminov, A.K.Nasirov, U.T.Yakhshiev, F.Hanappe, T.Materna, L.Stuttge Entrance Channel Effect on the Formation of Heavy and Superheavy Nuclei NUCLEAR REACTIONS 176Hf, 181Ta(40Ar, X), 92Zr(124Sn, X), 130Xe(86Kr, X), 182W(32S, X), 166Er(48Ti, X), 154Sm(60Ni, X), 248Cm(48Ca, X), E* ≈ 15-140 MeV; calculated fusion, capture, and evaporation residue σ; deduced entrance channel and shell structure effects.
doi: 10.1143/JPSJ.72.2509
2002MA21 Phys.Rev. C65, 044006 (2002) F.M.Marques, M.Labiche, N.A.Orr, J.C.Angelique, L.Axelsson, B.Benoit, U.C.Bergmann, M.J.G.Borge, W.N.Catford, S.P.G.Chappell, N.M.Clarke, G.Costa, N.Curtis, A.D'Arrigo, E.de Goes Brennand, F.de Oliveira Santos, O.Dorvaux, G.Fazio, M.Freer, B.R.Fulton, G.Giardina, S.Grevy, D.Guillemaud-Mueller, F.Hanappe, B.Heusch, B.Jonson, C.Le Brun, S.Leenhardt, M.Lewitowicz, M.J.Lopez, K.Markenroth, A.C.Mueller, T.Nilsson, A.Ninane, G.Nyman, I.Piqueras, K.Riisager, M.G.Saint Laurent, F.Sarazin, S.M.Singer, O.Sorlin, L.Stuttge Detection of Neutron Clusters NUCLEAR REACTIONS C(14Be, nX), E=35 MeV/nucleon; C(11Li, nX), E=30 MeV/nucleon; C(15B, X), E=48 MeV/nucleon; measured En, (charged particle)n-, nn-coin, angular distributions; deduced possible neutron cluster formation.
doi: 10.1103/PhysRevC.65.044006
2001LA02 Phys.Rev.Lett. 86, 600 (2001) M.Labiche, N.A.Orr, F.M.Marques, J.C.Angelique, L.Axelsson, B.Benoit, U.C.Bergmann, M.J.G.Borge, W.N.Catford, S.P.G.Chappell, N.M.Clarke, G.Costa, N.Curtis, A.D'Arrigo, E.de Goes Brennand, O.Dorvaux, G.Fazio, M.Freer, B.R.Fulton, G.Giardina, S.Grevy, D.Guillemaud-Mueller, F.Hanappe, B.Heusch, K.L.Jones, B.Jonson, C.Le Brun, S.Leenhardt, M.Lewitowicz, M.J.Lopez, K.Markenroth, A.C.Mueller, T.Nilsson, A.Ninane, G.Nyman, F.de Oliveira, I.Piqueras, K.Riisager, M.G.Saint Laurent, F.Sarazin, S.M.Singer, O.Sorlin, L.Stuttge Halo Structure of 14Be NUCLEAR REACTIONS C, Pb(14Be, 2n12Be), E=35 MeV/nucleon; measured σ, neutron angular and momentum distributions, decay energy spectra. 14Be deduced halo features. Kinematically complete measurement, secondary beam from 18O fragmentation. Comparison with three-body model calculations.
doi: 10.1103/PhysRevLett.86.600
2001MA90 Phys.Rev. C64, 061301 (2001) F.M.Marques, M.Labiche, N.A.Orr, J.C.Angelique, L.Axelsson, B.Benoit, U.C.Bergmann, M.J.G.Borge, W.N.Catford, S.P.G.Chappell, N.M.Clarke, G.Costa, N.Curtis, A.D'Arrigo, E.de Goes Brennand, F.de Oliveira Santos, O.Dorvaux, G.Fazio, M.Freer, B.R.Fulton, G.Giardina, S.Grevy, D.Guillemaud-Mueller, F.Hanappe, B.Heusch, B.Jonson, C.Le Brun, S.Leenhardt, M.Lewitowicz, M.J.Lopez, K.Markenroth, A.C.Mueller, T.Nilsson, A.Ninane, G.Nyman, I.Piqueras, K.Riisager, M.G.Saint Laurent, F.Sarazin, S.M.Singer, O.Sorlin, L.Stuttge Three-Body Correlations in Borromean Halo Nuclei NUCLEAR REACTIONS C, Pb(14Be, 2n12Be), E=35 MeV/nucleon; analyzed particle spectra, invariant mass, three-body correlations. Intensity interferometry, Dalitz plots.
doi: 10.1103/PhysRevC.64.061301
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
2000GI18 Bull.Rus.Acad.Sci.Phys. 64, 689 (2000) G.Giardina, P.D'Agostino, A.I.Muminov, A.K.Nasirov, G.Oliva, R.Palamara, R.Ruggeri, A.Taccone, G.Fazio, M.Herman Formation of Evaporation Residues in Synthesis of Superheavy Elements NUCLEAR REACTIONS 232Th, 238U, 244Pu(48Ca, F), (48Ca, 2n), (48Ca, 3n), (48Ca, 4n), E=215-255 MeV; calculated fusion, quasi-fission, evaporation residue σ, compound nucleus fission barrier vs bombarding energy. Dinuclear system concept, comparison with data.
1999GI16 Pramana 53, 409 (1999) G.Giardina, P.D'Agostino, G.Fazio, M.Herman, A.I.Muninov, A.Nasirov, G.Oliva, R.Palamara, R.Ruggeri Fusion-Fission Dynamics in the Superheavy Nucleus Production NUCLEAR REACTIONS 208Pb(64Ni, X), E=300-320 MeV; 238U, 244Pu(48Ca, X), E=220-280 MeV; calculated fusion, quasifission σ. 238U, 244Pu(48Ca, 2n), (48Ca, 3n), (48Ca, 4n), E=220-260 MeV; 208Pb(64Ni, n), E ≈ 310 MeV; calculated excitation functions. Comparisons with data.
doi: 10.1007/s12043-999-0007-x
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.
1998SA08 J.Phys.(London) G24, 611 (1998) R.N.Sagaidak, V.I.Chepigin, A.P.Kabachenko, J.Rohac, Yu.Ts.Oganessian, A.G.Popeko, A.V.Yeremin, A.D'Arrigo, G.Fazio, G.Giardina, M.Herman, R.Ruggeri, R.Sturiale Fission-Evaporation Competition in Excited Uranium and Fermium Nuclei NUCLEAR REACTIONS, ICPND 208Pb(20Ne, xn), (22Ne, xn), E=100-160 MeV; 232Th(20Ne, xn), (22Ne, xn)245Fm/246Fm/247Fm/248Fm, E=130-150 MeV; analyzed evaporation residues production σ; deduced compound nuclei neutron evaporation mechanism features. Advanced statistical model calculations.
doi: 10.1088/0954-3899/24/3/012
1996FA05 Int.J.Mod.Phys. E5, 175 (1996) G.Fazio, G.Giardina, F.I.Karmanov, V.L.Shablov Properties of the Resonance Scattering in Two-Fragment Systems Formed in Many-Particle Nuclear Reactions NUCLEAR REACTIONS 6Li(3He, α), E=8-14 MeV; calculated reaction amplitude. 5Li level deduced Γ. Two-fragment systems resonant scattering.
doi: 10.1142/S0218301396000086
1996FA23 Fizika(Zagreb) B5, 255 (1996) G.Fazio, G.Giardina, R.Sturiale, O.Yu.Goryunov, A.A.Shvedov The 27Al(14N, X) Reaction Mechanisms at the 129.3 MeV Bombarding Energy NUCLEAR REACTIONS 27Al(14N, X), E=129.3 MeV; measured absolute σ(θ) for 6,7Li, 7,9Be, 10,11Be, 12C fragments; deduced fragment production mechanism.
1995AR14 Yad.Fiz. 58, No 2, 215 (1995); Phys.Atomic Nuclei 58, 173 (1995) N.Arena, Seb.Cavallaro, P.D'Agostino, A.D'Arrigo, N.V.Eremin, G.Fazio, G.Giardina, M.Lombardi, M.Sacchi, T.U.Klochko, R.Palamara, A.Taccone Width Measurement of the 6Li(4.31) State by the 7Li(3He, αd)α Reaction NUCLEAR REACTIONS 7Li(3He, dα), E=4.5, 6 MeV; measured dα-coin. 6Li level deduced width.
1995AR25 J.Phys.(London) G21, 1403 (1995) N.Arena, Seb.Cavallaro, P.D'Agostino, G.Fazio, G.Giardina, O.Yu.Goryunov, V.V.Ostashko, R.Palamara, A.A.Shvedov The Short-Lived 8Be Level at E(x) = 11.4 MeV NUCLEAR REACTIONS 7Li(d, 2α), E=19.7 MeV; measured σ(θ1, θ2) vs arc length. 8Be deduced level energy, width.
doi: 10.1088/0954-3899/21/10/013
1995BO31 Nuovo Cim. 108, 901 (1995) F.Bonsignore, P.D'Agostino, G.Fazio, G.Giardina, O.Yu.Goryunov, A.A.Shvedov, R.Sturiale Clustering Phenomena in the (α, 7Li) Reaction at E(α) = 27.2 MeV NUCLEAR REACTIONS 11B, 15N, 19F(α, 7Li), E=27.2 MeV; measured σ(θ), spectra; deduced model parameters. 11B, 15N, 19F deduced cluster configuration spectroscopic factors. Direct plus compound reaction mechanisms.
doi: 10.1007/BF02731030
1995DA08 Nucl.Phys. A583, 437c (1995) P.D'Agostino, G.Fazio, G.Giardina, O.Yu.Goryunov, M.Sacchi, A.A.Shvedov, I.N.Vishnevsky, I.Yu.Zaiatz Nuclear-Rainbow Effect by Transfer Reactions NUCLEAR REACTIONS 12C(3He, 3He), (3He, 3He'), (3He, d), (3He, α), E=98 MeV; 12C(α, t), (α, 6He), (α, α), (α, α'), (α, 3He), E=90 MeV; measured σ(θ); deduced nuclear rainbow effect evidence, model parameters. Fuller's model, near/far-side formalism.
doi: 10.1016/0375-9474(94)00700-W
1995DA21 Nuovo Cim. 108A, 29 (1995) P.D'Agostino, A.D'Arrigo, G.Fazio, G.Giardina, O.Yu.Goryunov, A.P.Ilyin, M.Sacchi, A.A.Shvedov, A.Taccone, I.N.Vishnevsky, I.Yu.Zaiats, V.V.Zerkin Reaction Mechanism and Nuclear-Rainbow Effect in the 3He + 12C Interaction at E(3He) = 98 MeV NUCLEAR REACTIONS 12C(3He, 3He), (3He, 3He'), (3He, α), (3He, d), E=98 MeV; measured σ(θ); deduced rainbow effect evidence. Fuller's model, near/far-side formalism.
doi: 10.1007/BF02814854
1995FA21 J.Phys.Soc.Jpn. 64, 1141 (1995) G.Fazio, G.Giardina, O.Yu.Goryunov, A.A.Shvedov, R.Palamara The (α, 6Li) Reaction Mechanism at E(α) = 27.2 MeV NUCLEAR REACTIONS 10B, 14,15N, 19F(α, 6Li), E=27.2 MeV; measured σ(θ); deduced model parameters, spectroscopic factors. Finite-range DWBA.
doi: 10.1143/JPSJ.64.1141
1994AR24 J.Phys.(London) G20, 1973 (1994) N.Arena, I.Ya.Barit, Seb.Cavallaro, A.d'Arrigo, G.Fazio, G.Giardina, V.V.Ostashko, M.Sacchi, V.N.Urin, S.V.Zuyev Investigation of the High Excitation 8Be Region NUCLEAR REACTIONS, ICPND 6Li(d, α), E=18.2-44.5 MeV; measured σ(θ); deduced σ(E). 8Be deduced possible level.
doi: 10.1088/0954-3899/20/12/012
1994DA26 Phys.Lett. 332B, 25 (1994) A.D'Arrigo, N.V.Eremin, G.Fazio, G.Giardina, M.G.Glotova, T.V.Klochko, M.Sacchi, A.Taccone Investigation of Bremsstrahlung Emission in α-Decay of Heavy Nuclei RADIOACTIVITY 226Ra, 214Po(α); measured Eγ, Iγ, Eα, Iα, EγEα-coin; deduced bremsstrahlung emission probability vs Eγ. Classical electrodynamical model.
doi: 10.1016/0370-2693(94)90853-2
1994DA32 Nuovo Cim. 107A, 1353 (1994) A.D'Arrigo, G.Fazio, G.Giardina, O.Yu.Goryunov, A.P.Ilyin, M.Sacchi, A.A.Shvedov, A.Taccone, I.N.Vishnevsky, I.Yu.Zaiats Nuclear-Rainbow Effects by Transfer Reactions in the α + 12C Interaction NUCLEAR REACTIONS 12C(α, α), (α, α'), E=72-90 MeV; 12C(α, 3He), (α, t), (α, d), E=90 MeV; measured σ(θ); deduced far-side component role, rainbow effect evidence.
doi: 10.1007/BF02775774
1993AR12 Nuovo Cim. 106A, 1007 (1993) N.Arena, Seb.Cavallaro, A.D'Arrigo, G.Fazio, G.Giardina, A.Italiano, A.Taccone, D.Q.Hung, V.S.Olkhovsky Angle Independence of the 5Li(g.s.) Γ Width NUCLEAR REACTIONS 6Li(3He, pα), E=7, 9 MeV; measured σ(θ(1-23), θ(rel), E(23)). 5Li level deduced Γ. Kinematically complete experiment.
doi: 10.1007/BF02773490
1993DA16 Nucl.Phys. A564, 217 (1993) A.D'Arrigo, N.L.Doroshko, N.V.Eremin, G.Fazio, G.Giardina, B.V.Govorov, V.S.Olkhovsky, A.Taccone Delay-Advance Phenomenon Observed by Bremsstrahlung Spectrum of the 12C + p Collision NUCLEAR REACTIONS 12C(p, p), E=1.5-1.8 MeV; measured bremsstrahlung γ-spectrum; deduced time-delay spectrum near two superimposed resonances distorted by non-resonant background, total collision duration vs outgoing photon energy.
doi: 10.1016/0375-9474(93)90518-3
1993FA12 J.Phys.Soc.Jpn. 62, 1804 (1993) G.Fazio, G.Giardina, R.Palamara The P1/2 5He Level NUCLEAR REACTIONS 7Li(d, 2α), E=0.5 MeV; analyzed σ(θ1, θ2) vs arc length. 5He deduced level energy, Γ.
doi: 10.1143/JPSJ.62.1804
1992AR20 J.Phys.(London) G18, 2003 (1992) N.Arena, Seb.Cavallaro, A.D'Arrigo, G.Fazio, G.Giardina, A.Italiano, A.Taccone The Energy Independence of the 5Li(gs) Γ Width NUCLEAR REACTIONS 6Li(3He, pα), E=1.6-9 MeV; measured σ(θp, θα) vs arc length. 5Li level deduced Γ, energy dependence features.
doi: 10.1088/0954-3899/18/12/015
1992DA22 Fizika(Zagreb) B1, 139 (1992) P.D'Agostino, A.D'Arrigo, G.Fazio, G.Giardina, A.Italiano, A.Taccone, R.Palamara The J(π) = 2+ and 0+, T = 0 8Be Levels at About E(x) = 20 MeV NUCLEAR REACTIONS 7Li(d, 2α), E=7 MeV; measured σ(θα1, θα2) vs arc length. 8Be levels deduced Γ.
1991AR10 J.Phys.Soc.Jpn. 60, 100 (1991) N.Arena, S.Cavallaro, A.D'Arrigo, G.Fazio, G.Giardina, A.Italiano, F.Mezzanares, R.Palamara, A.Taccone On the Broad First Excited 5He State NUCLEAR REACTIONS 7Li(d, 2α), E=1.4, 2.1, 2.5 MeV; measured σ(θα1, θα2) vs arc length. 5He deduced level, Γ. Forward-forward, forward-backward geometries.
doi: 10.1143/JPSJ.60.100
1991AR18 J.Phys.Soc.Jpn. 60, 2175 (1991) N.Arena, S.Cavallaro, A.D'Arrigo, G.Fazio, G.Giardina, A.Italiano, A.Taccone The Even-Spin Positive-Parity 8Be Levels in the 20 MeV Region Observed by the 7Li(d, αα)n Reaction NUCLEAR REACTIONS 7Li(d, 2α), E=7 MeV; measured σ(θ1, θ2) vs arc length. 8Be levels deduced Γ.
doi: 10.1143/JPSJ.60.2175
1991AR19 Few-Body Systems 10, 187 (1991) N.Arena, Seb.Cavallaro, P.D'Agostino, A.D'Arrigo, G.Fazio, G.Giardina, A.Italiano, R.Palamara, A.Taccone Spectroscopic Parameters of the J(π) = 1+, T = 0 Excited 6Li Level NUCLEAR REACTIONS 7Li(3He, dα), E=5 MeV; measured σ(θd, θα) vs arc length. 6Li level deduced spectroscopic parameters.
doi: 10.1007/BF01076294
1991AR25 Nuovo Cim. 104A, 1809 (1991) N.Arena, Seb.Cavallaro, A.D'Arrigo, G.Fazio, G.Giardina, A.Italiano, A.Taccone, V.D.Chesnokova, V.S.Olkhovsky, A.K.Zaichenko Alpha-Proton Coincidence Spectra from the 6Li(3He, ααp) Reaction NUCLEAR REACTIONS 6Li(3He, p2α), E=1.6 MeV; measured σ(θp, θα) vs arc length. 5Li level deduced Γ.
doi: 10.1007/BF02812495
1991DA11 Nuovo Cim. 104A, 655 (1991) A.D'Arrigo, G.Fazio, G.Giardina, A.Taccone, R.Palamara 5He Energy Spectrum Analysis by the 7Li(d, αn)α Reaction NUCLEAR REACTIONS 7Li(d, nα), E=0.8-1.15 MeV; measured αα-coin; deduced 5He levels role. R-matrix analysis.
doi: 10.1007/BF02821774
1991FA10 J.Phys.Soc.Jpn. 60, 2475 (1991) The Role of the Data Analysis Method in Three-Body Reactions NUCLEAR REACTIONS 7Li(d, 2α), E=1.4-2.5 MeV; analyzed data; deduced criteria to determine three-body effects correctly.
doi: 10.1143/JPSJ.60.2475
1990AR17 J.Phys.(London) G16, 1511 (1990) N.Arena, Seb.Cavallaro, A.D'Arrigo, G.Fazio, G.Giardina, A.Italiano, A.Taccone The Jπ = (3/2)+, T = (1/2) 5Li level by the 6Li(3He, α)5Li Reaction NUCLEAR REACTIONS 6Li(3He, α), E=8-14 MeV; measured σ(Eα). 5Li level deduced Γ.
doi: 10.1088/0954-3899/16/10/014
1989AR04 Phys.Rev. C40, 55 (1989) N.Arena, Seb.Cavallaro, G.Fazio, G.Giardina, A.Italiano, M.Herman, M.Bruno, F.Cannata, M.D'Agostino, M.Lombardi Three-Body Effects in the 7Li(d, ααn) Reaction NUCLEAR REACTIONS 7Li(d, 2α), E=6.8 MeV; measured σ(θ1, θ2) vs arc length; deduced three body effects. 5He deduced (3/2)+ level width. Enriched target.
doi: 10.1103/PhysRevC.40.55
1989AR08 Phys.Rev. C40, 1126 (1989) N.Arena, Seb.Cavallaro, A.D'Arrigo, G.Fazio, G.Giardina, A.Italiano, M.Herman, M.Lombardi Width of the Level at E(x) ≈ 18 MeV in 5Li NUCLEAR REACTIONS 6Li(3He, pα), E=11, 13, 14 MeV; measured σ(θα, θp) vs arc length; analyzed αα-bidimensional spectra. 5Li deduced (1/2)+ level, width. Enriched target.
doi: 10.1103/PhysRevC.40.1126
1989AR20 Nuovo Cim. 102A, 1327 (1989) N.Arena, Seb.Cavallaro, P.D'Agostino, G.Fazio, G.Giardina, A.Italiano, F.Mezzanares, M.Herman, M.Lombardi 5Li(g.s.) Energy Spectrum Deduced by the 6Li(3He, αp)α Reaction NUCLEAR REACTIONS 6Li(3He, pα), E=2.5 MeV; measured σ(θα1, θα2) vs arc length. 5Li deduced level energy, Γ. R-matrix calculation.
doi: 10.1007/BF02800341
1988AR05 Europhys.Lett. 5, 517 (1988) N.Arena, Seb.Cavallaro, G.Fazio, G.Giardina, A.Italiano, F.Mezzanares Energy and Width Measurement of the 9B First Excited State Observed by the 10B(3He, α)9B(p)8Be and 10B(3He, α)9B(α)5Li Reactions NUCLEAR REACTIONS 10B(3He, α), E=2.3, 5 MeV; measured σ(θα, θp) vs arc length. 9B deduced level, Γ.
doi: 10.1209/0295-5075/5/6/007
1988AR20 J.Phys.Soc.Jpn. 57, 3773 (1988) N.Arena, S.Cavallaro, G.Fazio, G.Giardina, A.Italiano, F.Mezzanares The 5.65 MeV 6Li Level Width by the 7Li(3He, αd)α Reaction at E(3He)=11.5 MeV NUCLEAR REACTIONS 7Li(3He, dα), E=11.5 MeV; measured σ(θd, θα) vs arc length. 6Li level deduced Γ.
doi: 10.1143/JPSJ.57.3773
1986AR14 Phys.Rev.Lett. 57, 1839 (1986) N.Arena, Seb.Cavallaro, G.Fazio, G.Giardina, A.Italiano, F.Mezzanares Measurement of the 4.8-MeV 9B State Width by the Reaction 10B(3He, α)9B(α)5Li at E(3He) = 2.3 and 5.0 MeV NUCLEAR REACTIONS 10B(3He, α), E=2.3, 5 MeV; measured αα-coin, σ(θα1, θα2) vs arc length. 9B deduced level, Γ. Surface barrier detectors.
doi: 10.1103/PhysRevLett.57.1839
1985DA29 Can.J.Phys. 63, 1438 (1985) V.D'Amico, G.Fazio, S.Femino, G.Giardina, A.Italiano, F.Mezzanares Absolute Differential Cross Section for the 7Li(3He, ααd) Reaction at E(3He) = 5.0 MeV NUCLEAR REACTIONS 7Li(3He, 2α), E=5 MeV; measured αα-, αd-coin, σ(θ1, θ2); deduced reaction mechanism, channel competition.
doi: 10.1139/p85-240
1984AR17 Lett.Nuovo Cim. 41, 59 (1984) N.Arena, S.Cavallaro, A.S.Figuera, P.D'Agostino, G.Fazio, G.Giardina, F.Mezzanares Excitation Energy and Width of the First Excited State in 5Li from the 6Li(3He, αp)α Reaction NUCLEAR REACTIONS 6Li(3He, pα), E=1.7, 2.3 MeV; measured σ(θα1, θα2) vs arc length. 5Li deduced level, Γ. Enriched target.
doi: 10.1007/BF02748463
1983AR05 Lett.Nuovo Cim. 36, 135 (1983) N.Arena, C.Barbagallo, Seb.Cavallaro, P.D'Agostino, G.Fazio, G.Giardina, F.Mezzanares The 4.3 MeV 6Li State Width Deduced from the 7Li(3He, αd)α Reaction at E(3He) = 2.5 MeV NUCLEAR REACTIONS 7Li(3He, dα), E=2.5 MeV; measured σ(θd, θα) vs arc length. 6Li level deduced width.
doi: 10.1007/BF02719441
1983DA11 Can.J.Phys. 61, 923 (1983) V.D'Amico, G.Fazio, G.Giardina, F.Mezzanares The 10B(d, α)8Be(2α) Reaction Mechanism at E(d) = 1.85 MeV NUCLEAR REACTIONS 10B(d, α), E=1.85 MeV; measured αα(θ), σ(θα1, θα2) vs arc length; deduced heavy particle stripping mechanism. Bidimensional spectrum technique, enriched target.
doi: 10.1139/p83-113
1982AR08 Lett.Nuovo Cim. 34, 97 (1982) N.Arena, Seb.Cavallaro, G.Fazio, G.Giardina, F.Mezzanares Experimental Evidence of the 13D1 6Li State at about 5.7 MeV Excitation Energy NUCLEAR REACTIONS 7Li(t, dα), E=2.5, 5 MeV; measured σ(θd, θα) vs arc length. 6Li deduced level, width, configuration.
doi: 10.1007/BF02817205
1978AR10 Lett.Nuovo Cim. 23, 1 (1978) N.Arena, S.Cavallaro, R.Potenza, V.D'Amico, G.Fazio, S.Femino, G.Giardina, S.Jannelli, M.Lombardi Prevalence of the 8Be Formation in the 7Li(d, ααn) Reaction at E = 7.0 MeV NUCLEAR REACTIONS 7Li(d, n2α), E=7 MeV; measured σ(Eα1, Eα2, θ); deduced reaction mechanism.
doi: 10.1007/BF02762454
1977AR09 Lett.Nuovo Cim. 19, 125 (1977) N.Arena, S.Cavallaro, M.Lattuada, R.Potenza, M.L.Sperduto, V.D'Amico, G.Fazio, S.Femino, S.Jannelli Competition between 5Li and 8Be Formation in the 6Li(3He, ααp) Reaction at E = 2.5 MeV NUCLEAR REACTIONS 6Li(3He, p2α), E=2.5 MeV; measured σ(θ); deduced competition between 5Li, 8Be formation.
doi: 10.1007/BF02746558
1976DA24 Lett.Nuovo Cim. 15, 563 (1976) V.D'Amico, G.Fazio, S.Jannelli, F.Mezzanares, N.Arena, G.Calvi, R.Potenza Angular Correlation in the 7Li + 3He → 2α + d Reaction at E = 4.7 MeV NUCLEAR REACTIONS 7Li(3He, dα), E=4.7 MeV; measured dα(θ), σ.
doi: 10.1007/BF02725915
1975DA15 Lett.Nuovo Cim. 13, 489 (1975) V.D'Amico, G.Fazio, S.Jannelli, F.Mezzanares, R.Potenza Asymmetries in the Angular Correlations for the 7Li + d → 2α + n Reaction at E from 0.8 MeV to 1.2 MeV NUCLEAR REACTIONS 7Li(d, 2α), E=0.8, 1.2 MeV; measured αα(θ).
doi: 10.1007/BF02753853
1974DA28 Nuovo Cim. 22A, 313 (1974) V.D'Amico, G.Fazio, S.Jannelli, F.Mezzanares, R.Potenza 7Li+d → 2α+n Reaction. II: Experimental Results at E = 1.0 MeV NUCLEAR REACTIONS 7Li(d, n2α), E=1.0 MeV; measured αα(θ); deduced polarization in nα-system.
doi: 10.1007/BF02813441
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