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NSR database version of May 24, 2024.

Search: Author = G.Fazio

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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD5129. Data from this article have been entered in the XUNDL database. For more information, click here.


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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD5131.


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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset41551.


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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1213.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0085.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1991FA10      J.Phys.Soc.Jpn. 60, 2475 (1991)

G.Fazio, G.Giardina

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1108.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0695.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0546.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0253.


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