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NSR database version of May 24, 2024.

Search: Author = P.Napolitani

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2023FA02      Phys.Rev. C 107, 014604 (2023)

Q.Fable, A.Chbihi, J.D.Frankland, P.Napolitani, G.Verde, E.Bonnet, B.Borderie, R.Bougault, E.Galichet, T.Genard, D.Gruyer, M.Henri, M.La Commara, A.Le Fevre, J.Lemarie, N.Le Neindre, O.Lopez, P.Marini, M.Parlog, A.Rebillard-Soulie, W.Trautmann, E.Vient, M.Vigilante

Experimental study of isospin transport with 40, 48Ca + 40, 48Ca reactions at 35 MeV/nucleon

NUCLEAR REACTIONS 40,48Ca(40Ca, X), E=34.81 MeV/nucleon; 40,48Ca(48Ca, X), E=34.83 MeV/nucleon; measured reaction products; deduced transverse energy distributions of light charged particles, distribution of the average asymmetry as a function of the experimental centrality for the projectile-like fragments (PLF) and quasiprojectile (QP), isospin transport ratios, average N/Z ratio for the emitted clusters, average light charged particles multiplicities. Combined VAMOS high acceptance spectrometer and the INDRA charged particle multidetector setup at GANIL.

doi: 10.1103/PhysRevC.107.014604
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2022FA07      Phys.Rev. C 106, 024605 (2022)

Q.Fable, A.Chbihi, M.Boisjoli, J.D.Frankland, A.Le Fevre, N.Le Neindre, P.Marini, G.Verde, G.Ademard, L.Bardelli, C.Bhattacharya, S.Bhattacharya, E.Bonnet, B.Borderie, R.Bougault, G.Casini, M.La Commara, R.Dayras, J.E.Ducret, F.Farget, E.Galichet, T.Genard, F.Gramegna, D.Gruyer, M.Henri, S.Kundu, J.Lemarie, O.Lopez, J.Lukasik, L.Manduci, J.Moisan, G.Mukherjee, P.Napolitani, A.Olmi, M.Parlog, S.Piantelli, G.Poggi, A.Rebillard-Soulie, R.Roy, B.Sorgunlu, S.Velardita, E.Vient, M.Vigilante, J.P.Wieleczko

Experimental study of the 40, 48Ca + 40, 48Ca reactions at 35 MeV/nucleon

NUCLEAR REACTIONS 40,48Ca(40Ca, X), (48Ca, X), E=35 MeV/nucleon; measured reaction products; deduced average neutron excess of the fragments, average forward-emitted multiplicities, average neutron multiplicities, angular distributions of quasiprojectile fragments, mass and isotopic fission fragments distributions, average excitation energy per nucleon. Comparison to simulations performed in the framework of the antisymmetrized molecular dynamics (AMD) model coupled to the statistical decay code GEMINI++ as afterburner. 4π charged particle multidetector array INDRA and VAMOS spectrometer at GANIL.

doi: 10.1103/PhysRevC.106.024605
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2020BE11      Phys.Rev. C 101, 054608 (2020)

G.Besse, V.de la Mota, E.Bonnet, P.Eudes, P.Napolitani, Z.Basrak

Reexamining an extended-mean-field approach in heavy-ion collisions near the Fermi energy

NUCLEAR REACTIONS 58Ni(58Ni, X), 129Xe(120Sn, X), 40Ar(63Cu, X), (107Ag, X), (197Au, X), 197Au(197Au, X), E=20-120 MeV/nucleon; calculated stopping observables, energy isotropy ratio, large fluctuations, and linear momentum transfer using extended time-dependent Hartree-Fock (ETDHF) mean-field approach. Comparison with experimental data. Modeling of heavy-ion reactions at intermediate energies, and static and dynamical aspects of nuclear systems. 40Ar, 58Ni, 63Cu, 107Ag, 120Sn, 129Xe, 197Au; calculated binding energies and mean-square radii using Hartree-Fock equations, and compared with experimental data.

doi: 10.1103/PhysRevC.101.054608
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2019NA26      Phys.Rev. C 100, 054614 (2019)

P.Napolitani, A.Sainte-Marie, M.Colonna

Dynamic description of ternary and quaternary splits of heavy nuclear systems in the deep-inelastic regime

NUCLEAR REACTIONS 197Au(197Au, X), E=15 MeV/nucleon; calculated fragment chronology as a function of the impact parameter, probability of split or emission of fragments with A>2 as a function of time, distribution of fragment formation sites, fragment-multiplicity contributions as function of impact parameter, topologies of binary, ternary and quaternary exit channels, velocity and mass distribution of fragments, mean neutron-to-proton ratio of fragments, temperature-versus-density correlation in ternary and quaternary collisions. Boltzmann-Langevin one-body approach for shape fluctuations and exotic fragmentation modes in very heavy nonfusing systems in the deep-inelastic regime.

doi: 10.1103/PhysRevC.100.054614
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2018BO15      Phys.Lett. B 782, 291 (2018)

B.Borderie, N.Le Neindre, M.F.Rivet, P.Desesquelles, E.Bonnet, R.Bougault, A.Chbihi, D.Dell'Aquila, Q.Fable, J.D.Frankland, E.Galichet, D.Gruyer, D.Guinet, M.La Commara, I.Lombardo, O.Lopez, L.Manduci, P.Napolitani, M.Parlog, E.Rosato, R.Roy, P.St-Onge, G.Verde, E.Vient, M.Vigilante, J.P.Wieleczko, for the INDRA Collaboration

Phase transition dynamics for hot nuclei

NUCLEAR REACTIONS 112,124Sn(124Xe, X), (136Xe, X), E=32, 45 MeV/nucleon; measured reaction products; deduced differential charge multiplicity distribution, charge correlation functions, abnormal presence of equal-sized fragments.

doi: 10.1016/j.physletb.2018.05.040
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2017NA32      Phys.Rev. C 96, 054609 (2017)

P.Napolitani, M.Colonna

Inhomogeneity growth in two-component fermionic systems

NUCLEAR REACTIONS 136Xe(124Sn, X), E=32 MeV/nucleon; investigated nuclear phase transitions, EOS, intermediate-mass fragments, multifragmentation nuclear matter, spinodal instability, Langevin fluctuations, Fermi fluids by Boltzman-Langevin-one-body (BLOB) model, transport models, dynamical models, and stochastic mean field models.

doi: 10.1103/PhysRevC.96.054609
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2017PA10      Phys.Rev. C 95, 044606 (2017)

C.Paradela, L.Tassan-Got, J.Benlliure, J.L.Rodriguez-Sanchez, L.Audouin, A.Boudard, E.Casarejos, T.Enqvist, J.E.Ducret, F.Farget, B.Fernandez-Dominguez, M.Fernandez-Ordonez, L.Giot, A.Heinz, V.Henzl, D.Henzlova, A.Kelic-Heil, A.Lafriaskh, S.Leray, P.Napolitani, J.Pereira, D.Perez-Loureiro, M.V.Ricciardi, C.Stephan, K.-H.Schmidt, C.Schmitt, C.Villagrasa, C.Volant, O.Yordanov

Isotopic production cross sections of residual nuclei in the spallation reaction 136Xe (200A MeV) + p

NUCLEAR REACTIONS 1H(136Xe, X)115Cd/116Cd/115In/116In/117In/118In/119In/120In/115Sn/116Sn/117Sn/118Sn/119Sn/120Sn/121Sn/122Sn/123Sn/115Sb/116Sb/117Sb/118Sb/119Sb/120Sb/121Sb/122Sb/123Sb/124Sb/125Sb/126Sb/127Sb/128Sb/117Te/118Te/119Te/120Te/121Te/122Te/123Te/124Te/125Te/126Te/127Te/128Te/129Te/130Te/131Te/132Te/119I/120I/121I/122I/123I/124I/125I/126I/127I/128I/129I/130I/131I/132I/133I/134I/135I/120Xe/121Xe/122Xe/123Xe/124Xe/125Xe/126Xe/127Xe/128Xe/129Xe/130Xe/131Xe/132Xe/133Xe/134Xe/135Xe/121Cs/122Cs/123Cs/124Cs/125Cs/126Cs/127Cs/128Cs/129Cs/130Cs/131Cs/132Cs/133Cs/134Cs/135Cs/136Cs, E=200 MeV/nucleon; measured charge distribution, energy loss and isotopic σ(A, Z) and isobaric σ(A) of the fragments using the FRS separator and multisampling ionization chambers (MUSICs) at GSI; deduced correlation plot between atomic number (Z) and mass-over-charge ratio (A/Z), identification plot, correlation between the mass identification in the two FRS sections, momentum distribution of the 125Xe. Comparison with theoretical predictions using INCL4.6 and ISABEL codes coupled to the deexcitation code ABLA07.

doi: 10.1103/PhysRevC.95.044606
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2407.


2016XU03      Phys.Rev. C 93, 044609 (2016)

J.Xu, L.-W.Chen, M.Y.B.Tsang, H.Wolter, Y.-X.Zhang, J.Aichelin, M.Colonna, D.Cozma, P.Danielewicz, Z.-Q.Feng, A.Le Fevre, T.Gaitanos, C.Hartnack, K.Kim, Y.Kim, C.-M.Ko, B.-A.Li, Q.-F.Li, Z.-X.Li, P.Napolitani, A.Ono, M.Papa, T.Song, J.Su, J.-L.Tian, N.Wang, Y.-J.Wang, J.Weil, W.-J.Xie, F.-S.Zhang, G.-Q.Zhang

Understanding transport simulations of heavy-ion collisions at 100A and 400A MeV: Comparison of heavy-ion transport codes under controlled conditions

doi: 10.1103/PhysRevC.93.044609
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2015AL19      Phys.Rev. C 92, 024607 (2015)

J.Alcantara-Nunez, J.Benlliure, C.Paradela, C.Perez-Loureiro, J.L.Rodriguez-Sanchez, L.Audouin, A.Boudard, E.Casarejos, T.Enqvist, F.Farget, M.Fernandez-Ordonez, A.Heinz, V.Henzl, D.Henzlova, A.Kelic-Heil, A.Lafriaskh, S.Leray, P.Napolitani, J.Pereira, M.V.Ricciardi, C.Stephan, K.-H.Schmidt, C.Schmitt, L.Tassan-Got, C.Villagrasa, C.Volant, O.Yordanov

Isotopic yields of spallation residues produced in 136Xe-induced reactions on deuterium at 500 A MeV

NUCLEAR REACTIONS 2H(136Xe, X)37Ar/38Ar/39Ar/40Ar/41Ar/42Ar/38K/39K/40K/41K/42K/43K/44K/45K/40Ca/41Ca/42Ca/43Ca/44Ca/45Ca/46Ca/47Ca/42Sc/43Sc/44Sc/45Sc/46Sc/47Sc/48Sc/49Sc/50Sc/44Ti/45Ti/46Ti/47Ti/48Ti/49Ti/50Ti/51Ti/52Ti/46V/47V/48V/49V/50V/51V/52V/53V/54V/55V/56V/48Cr/49Cr/50Cr/51Cr/52Cr/53Cr/54Cr/55Cr/56Cr/57Cr/58Cr/50Mn/51Mn/52Mn/53Mn/54Mn/55Mn/56Mn/57Mn/58Mn/59Mn/60Mn/61Mn/52Fe/53Fe/54Fe/55Fe/56Fe/57Fe/58Fe/59Fe/60Fe/61Fe/62Fe/63Fe/54Co/55Co/56Co/57Co/58Co/59Co/60Co/61Co/62Co/63Co/64Co/65Co/56Ni/57Ni/58Ni/59Ni/60Ni/61Ni/62Ni/63Ni/64Ni/65Ni/66Ni/67Ni/68Ni/59Cu/60Cu/61Cu/62Cu/63Cu/64Cu/65Cu/66Cu/67Cu/68Cu/69Cu/70Cu/61Zn/62Zn/63Zn/64Zn/65Zn/66Zn/67Zn/68Zn/69Zn/70Zn/71Zn/72Zn/73Zn/63Ga/64Ga/65Ga/66Ga/67Ga/68Ga/69Ga/70Ga/71Ga/72Ga/73Ga/74Ga/75Ga/65Ge/66Ge/67Ge/68Ge/69Ge/70Ge/71Ge/72Ge/73Ge/74Ge/75Ge/76Ge/77Ge/78Ge/67As/68As/69As/70As/71As/72As/73As/74As/75As/76As/77As/78As/79As/80As/69Se/70Se/71Se/72Se/73Se/74Se/75Se/76Se/77Se/78Se/79Se/80Se/81Se/82Se/83Se/71Br/72Br/73Br/74Br/75Br/76Br/77Br/78Br/79Br/80Br/81Br/82Br/83Br/84Br/85Br/86Br/73Kr/74Kr/75Kr/76Kr/77Kr/78Kr/79Kr/80Kr/81Kr/82Kr/83Kr/84Kr/85Kr/86Kr/87Kr/88Kr/76Rb/77Rb/78Rb/79Rb/80Rb/81Rb/82Rb/83Rb/84Rb/85Rb/86Rb/87Rb/88Rb/89Rb/90Rb/78Sr/79Sr/80Sr/81Sr/82Sr/83Sr/84Sr/85Sr/86Sr/87Sr/88Sr/89Sr/90Sr/91Sr/92Sr/93Sr/94Sr, E=500 MeV/nucleon; measured yields and cross sections of spallation reaction residue products using the FRS magnetic spectrometer and multisampling ionization chambers at GSI facility. 2H(136Xe, X)79Y/80Y/81Y/82Y/83Y/84Y/85Y/86Y/87Y/88Y/89Y/90Y/91Y/92Y/93Y/94Y/95Y/96Y/97Y/81Zr/82Zr/83Zr/84Zr/85Zr/86Zr/87Zr/88Zr/89Zr/90Zr/91Zr/92Zr/93Zr/94Zr/95Zr/96Zr/97Zr/98Zr/99Zr/83Nb/84Nb/85Nb/86Nb/87Nb/88Nb/89Nb/90Nb/91Nb/92Nb/93Nb/94Nb/95Nb/96Nb/97Nb/98Nb/99Nb/100Nb/101Nb/102Nb/85Mo/86Mo/87Mo/88Mo/89Mo/90Mo/91Mo/92Mo/93Mo/94Mo/95Mo/96Mo/97Mo/98Mo/99Mo/100Mo/101Mo/102Mo/102Mo/104Mo/105Mo/88Tc/89Tc/90Tc/91Tc/92Tc/93Tc/94Tc/95Tc/96Tc/97Tc/98Tc/99Tc/100Tc/101Tc/102Tc/103Tc/104Tc/105Tc/106Tc/107Tc/108Tc/90Ru/91Ru/92Ru/93Ru/94Ru/95Ru/96Ru/97Ru/98Ru/99Ru/100Ru/101Ru/102Ru/103Ru/104Ru/105Ru/106Ru/107Ru/108Ru/109Ru/110Ru/111Ru/112Ru/92Rh/93Rh/94Rh/95Rh/96Rh/97Rh/98Rh/99Rh/100Rh/101Rh/102Rh/103Rh/104Rh/105Rh/106Rh/107Rh/108Rh/109Rh/110Rh/111Rh/112Rh/113Rh/114Rh/115Rh/116Rh/94Pd/95Pd/96Pd/97Pd/98Pd/99Pd/100Pd/101Pd/102Pd/103Pd/104Pd/105Pd/106Pd/107Pd/108Pd/109Pd/110Pd/111Pd/112Pd/113Pd/114Pd/115Pd/116Pd/117Pd/118Pd/119Pd/120Pd/98Ag/99Ag/100Ag/101Ag/102Ag/103Ag/104Ag/105Ag/106Ag/107Ag/108Ag/109Ag/110Ag/111Ag/112Ag/113Ag/114Ag/115Ag/116Ag/117Ag/118Ag/119Ag/120Ag/121Ag/122Ag/123Ag/100Cd/101Cd/102Cd/103Cd/104Cd/105Cd/106Cd/107Cd/108Cd/109Cd/110Cd/111Cd/112Cd/113Cd/114Cd/115Cd/116Cd/117Cd/118Cd/119Cd/120Cd/121Cd/122Cd/123Cd/124Cd/125Cd/126Cd, E=500 MeV/nucleon; measured yields and cross sections of spallation reaction residue products using the FRS magnetic spectrometer and multisampling ionization chambers at GSI facility. 2H(136Xe, X)102In/103In/104In/105In/106In/107In/108In/109In/110In/111In/112In/113In/114In/115In/116In/117In/118In/119In/120In/121In/122In/123In/124In/125In/126In/127In/128In/129In/105Sn/106Sn/107Sn/108Sn/109Sn/110Sn/111Sn/112Sn/113Sn/114Sn/115Sn/116Sn/117Sn/118Sn/119Sn/120Sn/121Sn/122Sn/123Sn/124Sn/125Sn/126Sn/127Sn/128Sn/129Sn/130Sn/131Sn/132Sn/107Sb/108Sb/109Sb/110Sb/111Sb/112Sb/113Sb/114Sb/115Sb/116Sb/117Sb/118Sb/119Sb/120Sb/121Sb/122Sb/123Sb/124Sb/125Sb/126Sb/127Sb/128Sb/129Sb/130Sb/131Sb/132Sb/133Sb/134Sb/110Te/111Te/112Te/113Te/114Te/115Te/116Te/117Te/118Te/119Te/120Te/121Te/122Te/123Te/124Te/125Te/126Te/127Te/128Te/129Te/130Te/131Te/132Te/133Te/134Te/135Te/112I/113I/114I/115I/116I/117I/118I/119I/120I/121I/122I/123I/124I/125I/126I/127I/128I/129I/130I/131I/132I/133I/134I/135I/136I/116Xe/117Xe/118Xe/119Xe/120Xe/121Xe/122Xe/123Xe/124Xe/125Xe/126Xe/127Xe/128Xe/129Xe/130Xe/131Xe/132Xe/133Xe/134Xe/135Xe/119Cs/120Cs/121Cs/122Cs/123Cs/124Cs/125Cs/126Cs/127Cs/128Cs/129Cs/130Cs/131Cs/132Cs/133Cs/134Cs/135Cs/136Cs/123Ba/124Ba/125Ba/126Ba/127Ba/128Ba/129Ba/130Ba/131Ba/132Ba/133Ba/134Ba/135Ba, E=500 MeV/nucleon; measured yields and cross sections of spallation reaction residue products using the FRS magnetic spectrometer and multisampling ionization chambers at GSI facility. Benchmarked reference model calculations describing spallation reactions. Comparison with the measured production yields in 1H(136Xe, X), E=500, 1000 MeV/nucleon.

doi: 10.1103/PhysRevC.92.024607
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1889.


2015NA16      Phys.Rev. C 92, 034607 (2015)

P.Napolitani, M.Colonna

Frustrated fragmentation and re-aggregation in nuclei: A non-equilibrium description in spallation

NUCLEAR REACTIONS 1H(136Xe, X), (124Xe, X), E=1 GeV/nucleon; 1H(208Pb, X), E=750, 1000 MeV/nucleon; 2H(208Pb, X), (197Au, X), E=750 MeV/nucleon; 136Xe, 208Pb(p, X), E=1 GeV; analyzed zero-angle invariant velocity distributions from isotopic cross sections measured in the intermediate-mass fragment (IMF) region; calculated mean number of emitted nucleons per interval of time, average excitation energy for the fraction of bound matter during the reaction, average isotopic content of bound matter as a function of time, normalized yields as a function of the multiplicity of fragments with Z>4, production yields and kinetic energies for spallation reactions as a function of mass number, correlation among the three heaviest IMFs and Dalitz plots, density profiles as function of time. Boltzmann-Langevin one-body (BLOB) approach for the dynamics of hot nuclear systems produced in spallation reactions.

doi: 10.1103/PhysRevC.92.034607
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2014AD02      Eur.Phys.J. A 50, 33 (2014)

G.Ademard, B.Borderie, A.Chbihi, O.Lopez, P.Napolitani, M.F.Rivet, M.Boisjoli, E.Bonnet, R.Bougault, J.D.Frankland, E.Galichet, D.Gruyer, D.Guinet, M.Kabtoul, G.Lehaut, P.Lautesse, M.La Commara, N.Le Neindre, P.Marini, M.Parlog, P.Pawlowski, E.Rosato, R.Roy, G.Spadaccini, E.Vient, M.Vigilante, J.P.Wieleczko, for the INDRA Collaboration

Isospin effects and symmetry energy studies with INDRA

NUCLEAR REACTIONS 112,124Sn(124Xe, X), (136Xe, X), E=32, 45 MeV/nucleon; measured reaction products; deduced mean fragment, light charged particle multiplicity vs neutron-to-proton ratio, mass and energy systematic trends; calculated fragment, light charged particle multiplicity vs neutron-to-proton ratio, energy isotropy ratio using stochastic mean-field model. 40,48Ca(40Ca, X), (48Ca, X), E=35 MeV/nucleon; measured reaction products; deduced isotopic distribution yield. 112,124Sn(124Xe, X), (136Xe, X), E=24, 32, 45, 58 MeV/nucleon; measured reaction products; deduced central collisions fragment multiplicity distribution, yield.

doi: 10.1140/epja/i2014-14033-x
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2014LO13      Phys.Rev. C 90, 064602 (2014); Pub.Note Phys.Rev. C 90, 069903 (2014)

O.Lopez, D.Durand, G.Lehaut, B.Borderie, J.D.Frankland, M.F.Rivet, R.Bougault, A.Chbihi, E.Galichet, D.Guinet, M.La Commara, N.Le Neindre, I.Lombardo, L.Manduci, P.Marini, P.Napolitani, M.Parlog, E.Rosato, G.Spadaccini, E.Vient, M.Vigilante, for the INDRA Collaboration

In-medium effects for nuclear matter in the Fermi-energy domain

NUCLEAR REACTIONS K, Cl(36Ar, X), E=32-74 MeV/nucleon; 58Ni(36Ar, X), E=32-95 MeV/nucleon; 58Ni(58Ni, X), E=32-90 MeV/nucleon; 129Sn(129Xe, X), E=15-100 MeV/nucleon; 181Ta(197Au, X), E=33, 40 MeV/nucleon; 197Au(197Au, X), E=40-100 MeV/nucleon; 155Gd(238U, X), E=36 MeV/nucleon; 208Pb(197Au, X), E=29 MeV/nucleon; 238U(238U, X), E=24 MeV/nucleon; analyzed nuclear stopping as a function of system mass and bombarding energy using data from measurements with the 4π array INDRA. Role of in-medium effects in the Fermi-energy domain.

doi: 10.1103/PhysRevC.90.064602
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2013GI02      Nucl.Phys. A899, 116 (2013)

L.Giot, J.A.Alcantara-Nunez, J.Benlliure, D.Perez-Loureiro, L.Audouin, A.Boudard, E.Casarejos, T.Enqvist, J.E.Ducret, B.Fernandez-Dominguez, M.Fernandez-Ordonez, F.Farget, A.Heinz, V.Henzl, D.Henzlova, A.Kelic-Heil, A.Lafriaskh, S.Leray, P.Napolitani, C.Paradela, J.Pereira, M.V.Ricciardi, C.Stephan, K.-H.Schmidt, C.Schmitt, L.Tassan-Got, C.Villagrasa, C.Volant, O.Yordanov

Isotopic production cross sections of the residual nuclei in spallation reactions induced by 136Xe projectiles on proton at 500 A MeV

NUCLEAR REACTIONS 1H(136Xe, X), E=500 MeV/nucleon; measured spallation products mass, charge distribution using FRS magnetic spectrometer; deduced fragment isotopes yields, production σ, longitudinal momentum distributions. Compared with published data at 1000 MeV/nucleon.

doi: 10.1016/j.nuclphysa.2012.12.119
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2143.


2012BE38      J.Phys.:Conf.Ser. 337, 012070 (2012)

J.Benlliure, H.Alvarez-Pol, T.Kurtukian-Nieto, A.I.Morales, L.Audouin, F.Becker, B.Blank, I.Borzov, E.Casarejos, D.Cortina-Gil, B.Fernandez, J.Giovinazzo, D.Henzlova, B.Jurado, L.Langanke, G.Martinez-Pinedo, P.Napolitani, J.Pereira, F.Rejmund, K.-H.Schmidt, O.Yordanov, for the RISING Collaboration

Approaching r-process nuclei at N = 126

RADIOACTIVITY 194,195,196Re, 199,200Os, 198,201,202Ir, 203,204Pt, 204Au(β-); measured Iβ(t) using DSSSD; deduced T1/2; calculated T1/2 using Gross theory, FR droplet model and energy-density functional.

doi: 10.1088/1742-6596/337/1/012070
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2012GA42      Phys.Rev. C 86, 044617 (2012)

F.Gagnon-Moisan, E.Galichet, M.-F.Rivet, B.Borderie, M.Colonna, R.Roy, G.Ademard, M.Boisjoli, E.Bonnet, R.Bougault, A.Chbihi, J.D.Frankland, D.Guinet, P.Lautesse, E.Legouee, N.Le Neindre, L.Manduci, P.Marini, P.Napolitani, M.Parlog, P.Pawlowski, E.Rosato, M.Vigilante

New isospin effects in central heavy-ion collisions at Fermi energies

NUCLEAR REACTIONS 112Sn, 124Sn(124Xe, X), (136Xe, X), E=36, 45 MeV/nucleon; measured particle spectra, multiplicity distributions of charged products, light charged particles and fragments, fragment kinetic energy using 4π INDRA array at GANIL; deduced isospin effects on measured total charged product multiplicities and total charge bound in fragments. Comparison with stochastic mean field (SMF) calculations.

doi: 10.1103/PhysRevC.86.044617
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2011RA18      Int.J.Mod.Phys. E20, 902 (2011)

Ad.R.Raduta, B.Borderie, N.Le Neindre, P.Napolitani, M.F.Rivet, E.Geraci

Production of α-particle condensate states in heavy-ion collisions

doi: 10.1142/S0218301311018939
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2011RA43      Phys.Lett. B 705, 65 (2011)

Ad.R.Raduta, B.Borderie, E.Geraci, N.Le Neindre, P.Napolitani, M.F.Rivet, R.Alba, F.Amorini, G.Cardella, M.Chatterjee, E.De Filippo, D.Guinet, P.Lautesse, E.La Guidara, G.Lanzalone, G.Lanzano, I.Lombardo, O.Lopez, C.Maiolino, A.Pagano, S.Pirrone, G.Politi, F.Porto, F.Rizzo, P.Russotto, J.P.Wieleczko

Evidence for α-particle condensation in nuclei from the Hoyle state deexcitation

NUCLEAR REACTIONS 12C(40Ca, X), E=25 MeV/nucleon; measured reaction products, deuteron spectrum, Eα, Iα, α-α, α-d and 3α correlations; deduced particle decays of the Hoyle state to direct decays in three equal-energy α-particles.

doi: 10.1016/j.physletb.2011.10.008
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Data from this article have been entered in the XUNDL database. For more information, click here.


2010AL24      Phys.Rev. C 82, 041602 (2010)

H.Alvarez-Pol, J.Benlliure, E.Casarejos, L.Audouin, D.Cortina-Gil, T.Enqvist, B.Fernandez-Dominguez, A.R.Junghans, B.Jurado, P.Napolitani, J.Pereira, F.Rejmund, K.-H.Schmidt, O.Yordanov

Production of new neutron-rich isotopes of heavy elements in fragmentation reactions of 238U projectiles at 1A GeV

NUCLEAR REACTIONS 9Be(238U, X), E=1 GeV/nucleon; measured fragment residues using a high resolution magnetic spectrometer Fragment Separator, σ, yields. 203,204,205Pt, 207,208,209,210Au, 210,211,212,213,214,215,216Hg, 210,211,212,213,214,215,216,217Tl, 214,215,216,217,218,219,220Pb, 217,218,219,220,221,222,223,224Bi, 220,221,222,223,224,225,226,227Po, 222,223,224,225,226,227,228,229At, 225,226,227,228,229,230,231Rn, 228,229,230,232,232,233Fr; deduced yields, production σ. Comparisons of σ with the predictions obtained using the computer codes COFRA and EPAX.

doi: 10.1103/PhysRevC.82.041602
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2010LE07      Phys.Rev.Lett. 104, 232701 (2010)

G.Lehaut, D.Durand, O.Lopez, E.Vient, A.Chbihi, J.D.Frankland, E.Bonnet, B.Borderie, R.Bougault, E.Galichet, D.Guinet, Ph.Lautesse, N.Le Neindre, P.Napolitani, M.Parlog, M.F.Rivet, E.Rosato, for the INDRA and ALADIN Collaborations

Study of Nuclear Stopping in Central Collisions at Intermediate Energies

NUCLEAR REACTIONS Sn(Sn, X), (Xe, X), E<100 MeV/nucleon; 119Sn(129Xe, X), E=50 MeV/nucleon; measured reaction products; deduced nuclear stopping power, mean isotropy ratio. Comparison with IQMD calculations.

doi: 10.1103/PhysRevLett.104.232701
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2010NA06      Phys.Rev. C 81, 044619 (2010)

P.Napolitani, M.Colonna, F.Gulminelli, E.Galichet, S.Piantelli, G.Verde, E.Vient

Probing the nuclear equation of state in heavy-ion collisions at Fermi energy in isospin-sensitive exclusive experiments

NUCLEAR REACTIONS 58,68Ni(58Ni, X), E=15, 40 MeV/nucleon; 68Ni(68Ni, X), E=15, 40 MeV/nucleon; calculated isotopic composition of largest fragment, impact parameters versus transverse energy per nucleon, proton and neutron yields within the framework of the Stochastic Mean Field (SMF) model.

doi: 10.1103/PhysRevC.81.044619
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2009AL32      Eur.Phys.J. A 42, 485 (2009)

H.Alvarez-Pol, J.Benlliure, E.Casarejos, L.Audouin, D.Cortina-Gil, T.Enqvist, B.Fernandez, A.R.Junghans, B.Jurado, P.Napolitani, J.Pereira, F.Rejmund, K.-H.Schmidt, O.Yordanov

Production cross-sections of neutron-rich Pb and Bi isotopes in the fragmentation of 238U

NUCLEAR REACTIONS 9Be(238U, X)196Pb/197Pb/198Pb/199Pb/200Pb/201Pb/202Pb/203Pb/204Pb/205Pb/206Pb/207Pb/208Pb/209Pb/210Pb/214Pb/215Pb/216Pb/217Pb/218Pb/219Pb/199Bi/200Bi/201Bi/202Bi/203Bi/204Bi/205Bi/206Bi/207Bi/208Bi/209Bi/210Bi/211Bi/212Bi/213Bi/214Bi/218Bi/219Bi/220Bi/221Bi/222Bi/223Bi, E=1 GeV/nucleon; measured production σ. Comparison with other data.

doi: 10.1140/epja/i2009-10856-8
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2008BE33      Phys.Rev. C 78, 054605 (2008)

J.Benlliure, M.Fernandez-Ordonez, L.Audouin, A.Boudard, E.Casarejos, J.E.Ducret, T.Enqvist, A.Heinz, D.Henzlova, V.Henzl, A.Kelic, S.Leray, P.Napolitani, J.Pereira, F.Rejmund, M.V.Ricciardi, K.-H.Schmidt, C.Schmitt, C.Stephan, L.Tassan-Got, C.Volant, C.Villagrasa, O.Yordanov

Production of medium-mass neutron-rich nuclei in reactions induced by 136Xe projectiles at 1 A GeV on a beryllium target

NUCLEAR REACTIONS 9Be(136Xe, X)132Cs/133Cs/134Cs/135Cs/136Cs/129Xe/130Xe/131Xe/132Xe/133Xe/134Xe/135Xe/127I/128I/129I/130I/131I/132I/133I/134I/135I/136I/125Te/126Te/127Te/128Te/129Te/130Te/131Te/132Te/133Te/134Te/135Te/123Sb/124Sb/125Sb/126Sb/127Sb/128Sb/129Sb/130Sb/131Sb/132Sb/133Sb/134Sb/120Sn/121Sn/122Sn/123Sn/124Sn/125Sn/126Sn/127Sn/128Sn/129Sn/130Sn/131Sn/132Sn/118In/119In/120In/121In/122In/123In/124In/125In/126In/127In/128In/129In/130In/131In/115Cd/116Cd/117Cd/118Cd/119Cd/120Cd/121Cd/122Cd/123Cd/124Cd/125Cd/126Cd/127Cd/128Cd/129Cd/130Cd/122Ag/123Ag/124Ag/125Ag/126Ag/127Ag/128Ag/119Pd/120Pd/121Pd/122Pd/123Pd/124Pd/125Pd/117Rh/118Rh/119Rh/120Rh/121Rh/122Rh/118Ru/119Ru/115Tc/116Tc/117Tc/113Mo/110Nb/111Nb/108Zr, E=1 GeV/nucleon; measured σ.

doi: 10.1103/PhysRevC.78.054605
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2008GR18      Nucl.Phys. A811, 233 (2008)

F.Grenier, A.Chbihi, R.Roy, G.Verde, D.Theriault, J.D.Frankland, J.P.Wieleczko, B.Borderie, R.Bougault, R.Dayras, E.Galichet, D.Guinet, P.Lautesse, N.Le Neindre, O.Lopez, J.Moisan, L.Nalpas, P.Napolitani, M.Parlog, M.F.Rivet, E.Rosato, B.Tamain, E.Vient, M.Vigilante, and the INDRA Collaboration

Multi-particle correlation function to study short-lived nuclei

NUCLEAR REACTIONS 24Mg(12C, X), E=53, 95 MeV/nucleon; measured fragments velocity and total kinetic energy distributions with the INDRA array; deduced quasi-projectile breakup mechanism, related features.

doi: 10.1016/j.nuclphysa.2008.07.018
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2008HE13      Phys.Rev. C 78, 044616 (2008)

D.Henzlova, K.-H.Schmidt, M.V.Ricciardi, A.Kelic, V.Henzl, P.Napolitani, L.Audouin, J.Benlliure, A.Boudard, E.Casarejos, J.E.Ducret, T.Enqvist, A.Heinz, A.Junghans, B.Jurado, A.Krasa, T.Kurtukian, S.Leray, M.F.Ordonez, J.Pereira, R.Pleskac, F.Rejmund, C.Schmitt, C.Stephan, L.Tassan-Got, C.Villagrasa, C.Volant, A.Wagner, O.Yordanov

Experimental investigation of the residues produced in the 136Xe + Pb and 124Xe + Pb fragmentation reactions at 1A GeV

NUCLEAR REACTIONS Pb(124Xe, X), (136Xe, X)Z=3-56, E=1 GeV/nucleon; measured σ. Production cross sections for over 1100 individual nuclides measured.

doi: 10.1103/PhysRevC.78.044616
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2007CH63      Nucl.Phys. A787, 603c (2007)

P.Chomaz, C.Ducoin, F.Gulminelli, K.Hasnaoui, P.Napolitani

Thermodynamics of compact-star matter within an Ising approach

doi: 10.1016/j.nuclphysa.2006.12.090
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2007DU14      Phys.Rev. C 75, 065805 (2007)

C.Ducoin, K.H.O.Hasnaoui, P.Napolitani, Ph.Chomaz, F.Gulminelli

Anomalous thermodynamics and phase transitions in neutron star matter

doi: 10.1103/PhysRevC.75.065805
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2007NA31      Phys.Rev. C 76, 064609 (2007)

P.Napolitani, K.-H.Schmidt, L.Tassan-Got, P.Armbruster, T.Enqvist, A.Heinz, V.Henzl, D.Henzlova, A.Kelic, R.Pleskac, M.V.Ricciardi, C.Schmitt, O.Yordanov, L.Audouin, M.Bernas, A.Lafriaskh, F.Rejmund, C.Stephan, J.Benlliure, E.Casarejos, M.Fernandez-Ordonez, J.Pereira, A.Boudard, B.Fernandez, S.Leray, C.Villagrasa, C.Volant

Measurement of the complete nuclide production and kinetic energies of the system 136Xe+hydrogen at 1 GeV per nucleon

NUCLEAR REACTIONS 136Xe(p, X), E=1 GeV/nucleon; measured isotopic cross sections, kinetic energies. 6,7,8Li, 9,10,11,12Be, 10,11,12,13B, 11,12,13,14,15C, 13,14,15,16,17N, 15,16,17,18,19O, 17,18,19,20,21F, 19,20,21,22,23Ne, 22,23,24,25Na, 23,24,25,26,27Mg, 25,26,27,28,29,30Al, 28,29,30,31,32Si, 30,31,32,33,34P, 32,33,34,35,36,37,38S, 34,35,36,37,38,39,40Cl, 36,37,38,39,40,41,42,43Ar, 39,40,41,42,43,44,45K, 41,42,43,44,45,46,47Ca, 43,44,45,46,47,48,49,50Sc, 45,46,47,48,49,50,51,52Ti, 46,47,48,49,50,51,52,53,54,55V, 49,50,51,52,53,54,55,56,57Cr, 50,51,52,53,54,55,56,57,58,59,60Mn, 55,56,57,58,59,60,61,62Fe, 57,58,59,60,61,62,63,64,65Co, 59,60,61,62,63,64,65,66,67Ni, 60,61,62,63,64,65,66,67,68,69,70Cu, 62,63,64,65,66,67,68,69,70,71,72Zn, 66,67,68,69,70,71,72,73,74,75Ga, 68,69,70,71,72,73,74,75,76,77Ge, 70,71,72,73,74,75,76,77,78,79,80,81As, 72,73,74,75,76,77,78,79,80,81,82,83Se, 74,75,76,77,78,79,80,81,82,83,84,85Br, 76,77,78,79,80,81,82,83,84,85,86,87,88Kr; measured cross sections.

NUCLEAR REACTIONS 136Xe(p, X), E=1 GeV/nucleon; measured isotopic cross sections, kinetic energies. 79,80,81,82,83,84,85,86,87,88,89,90Rb, 81,82,83,84,85,86,87,88,89,90,91,92,93Sr, 84,85,86,87,88,89,90,91,92,93,94,95,96Y, 86,87,88,89,90,91,92,93,94,95,96,97,98,99Zr, 87,88,89,90,91,92,93,94,95,96,97,98,99,100Nb, 90,91,92,93,94,95,96,97,98,99,100,101,102,103,104Mo, 92,93,94,95,96,97,98,99,100,101,102,103,104,105,106Tc, 95,96,97,98,99,100,101,102,103,104,105,106,107,108,109Ru, 97,98,99,100,101,102,103,104,105,106,107,108,109,110,111Rh, 99,100,101,102,103,104,105,106,107,108,109,110,111,112,113,114,115Pd, 101,102,103,104,105,106,107,108,109,110,111,112,113,114,115,116,117,118,119,120,121,122Ag, 104,105,106,107,108,109,110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125Cd, 105,106,107,108,109,110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125,126,127In, 108,109,110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130Sn, 110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132Sb, 111,112,113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134Te, 113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135I, 116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135Xe, 122,123,124,125,126,127,128,129,130,131,132,133,134,135,136Cs, 127,128,129,130,131,132Ba; measured cross sections.

doi: 10.1103/PhysRevC.76.064609
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2007VI06      Phys.Rev. C 75, 044603 (2007)

C.Villagrasa-Canton, A.Boudard, J.-E.Ducret, B.Fernandez, S.Leray, C.Volant, P.Armbruster, T.Enqvist, F.Hammache, K.Helariutta, B.Jurado, M.-V.Ricciardi, K.-H.Schmidt, K.Summerer, F.Vives, O.Yordanov, L.Audouin, C.-O.Bacri, L.Ferrant, P.Napolitani, F.Rejmund, C.Stephan, L.Tassan-Got, J.Benlliure, E.Casarejos, M.Fernandez-Ordonez, J.Pereira, S.Czajkowski, D.Karamanis, M.Pravikoff, J.S.George, R.A.Mewaldt, N.Yanasak, M.Wiedenbeck, J.J.Connell, T.Faestermann, A.Heinz, A.Junghans

Spallation residues in the reaction 56Fe+p at 0.3A, 0.5A, 0.75A, 1.0A, and 1.5A GeV

NUCLEAR REACTIONS 1H(56Fe, X), E=0.3, 0.5, 0.75, 1.0, 1.5 GeV/nucleon; measured spallation products isotopic yields, excitation functions.

doi: 10.1103/PhysRevC.75.044603
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2005HE07      Nucl.Phys. A749, 110c (2005)

D.Henzlova, L.Audouin, J.Benlliure, A.S.Botvina, A.Boudard, E.Casarejos, J.E.Ducret, T.Enqvist, L.T.Got, A.Heinz, V.Henzl, A.Junghans, B.Jurado, A.Kelic, A.Krasa, T.Kurtukian, S.Leray, P.Napolitani, M.F.Ordonez, J.Pereira, R.Pleskac, F.Rejmund, M.V.Ricciardi, K.-H.Schmidt, Ch.Schmitt, C.Stephan, C.Villagrasa, C.Volant, A.Wagner, O.Yordanov

Isotopically resolved residues from the fragmentation of projectiles with largely different N/Z - the isospin-thermometer method

NUCLEAR REACTIONS Pb(124Xe, X), (136Xe, X), E=1 GeV/nucleon; measured fragments charge and mass distributions; deduced freeze-out temperature.

doi: 10.1016/j.nuclphysa.2004.12.016
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2005RI02      Nucl.Phys. A749, 122c (2005)

M.V.Ricciardi, A.V.Ignatyuk, A.Kelic, P.Napolitani, F.Rejmund, K.-H.Schmidt, O.Yordanov

Complex nuclear-structure phenomena in the cooling down of highly excited nuclear systems

NUCLEAR REACTIONS Ti(238U, X), E=1 GeV/nucleon; measured fragments isotopic production σ; deduced structure effects. Comparison with statistical abrasion-evaporation model predictions.

doi: 10.1016/j.nuclphysa.2004.12.019
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2004AR28      Phys.Rev.Lett. 93, 212701 (2004)

P.Armbruster, J.Benlliure, M.Bernas, A.Boudard, E.Casarejos, S.Czajkowski, T.Enqvist, S.Leray, P.Napolitani, J.Pereira, F.Rejmund, M.-V.Ricciardi, K.-H.Schmidt, C.Stephan, J.Taieb, L.Tassan-Got, C.Volant

Measurement of a Complete Set of Nuclides, Cross Sections, and Kinetic Energies in Spallation of 238U 1A GeV with Protons

NUCLEAR REACTIONS 1H(238U, X), E=1 GeV/nucleon; measured spallation fragments isotopic production σ, longitudinal momentum distributions, kinetic energies.

doi: 10.1103/PhysRevLett.93.212701
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2004BE19      Nucl.Phys. A734, 609 (2004)

J.Benlliure, L.Audouin, M.Bernas, E.Casarejos, T.Enqvist, B.Fernandez, V.Henzl, A.Kelic, P.Napolitani, J.Pereira, M.V.Ricciardi, K.-H.Schmidt, J.Taieb

Momentum distributions of projectile spectators: a new tool to investigate the equation of state of nuclear matter

NUCLEAR REACTIONS Ti, Pb(208Pb, X), (238U, X), E=500-1000 MeV/nucleon; measured fragment velocity distributions; deduced post-acceleration effects.

doi: 10.1016/j.nuclphysa.2004.01.113
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2004HE14      Prog.Part.Nucl.Phys. 53, 97 (2004)

D.Henzlova, M.V.Ricciardi, J.Benlliure, A.S.Botvina, T.Enqvist, A.Kelic, P.Napolitani, J.Pereira, K.-H.Schmidt

Investigation of the N/Z of the heavy fragmentation products-the isospin thermometer method

NUCLEAR REACTIONS Ti, Pb(238U, X), E=1 GeV/nucleon; 2H, Ti(208Pb, X), E=1 GeV/nucleon; analyzed fragments charge and mass distributions; deduced thermal properties.

doi: 10.1016/j.ppnp.2004.02.009
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2004NA06      Int.J.Mod.Phys. E13, 333 (2004)

P.Napolitani, F.Rejmund, L.Tassan-Got, M.V.Ricciardi, A.Kelic, K.-H.Schmidt, O.Yordanov, A.V.Ignatyuk, C.Villagrasa

Structural effects in the nuclide distributions of the residues of highly excited systems

NUCLEAR REACTIONS 1H, Ti(56Fe, X), E=1 GeV/nucleon; measured fragments isotopic production σ; deduced reaction mechanism features.

doi: 10.1142/S0218301304002144
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2004NA36      Phys.Rev. C 70, 054607 (2004)

P.Napolitani, K.-H.Schmidt, A.S.Botvina, F.Rejmund, L.Tassan-Got, C.Villagrasa

High-resolution velocity measurements on fully identified light nuclides produced in 56Fe + hydrogen and 56Fe + titanium systems

NUCLEAR REACTIONS 1H, Ti(56Fe, X), E=1 GeV/nucleon; measured fragments isotopic production σ, velocity and mass distributions; deduced reaction mechanism features.

doi: 10.1103/PhysRevC.70.054607
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2004RI07      Nucl.Phys. A733, 299 (2004)

M.V.Ricciardi, A.V.Ignatyuk, A.Kelic, P.Napolitani, F.Rejmund, K.-H.Schmidt, O.Yordanov

Complex nuclear-structure phenomena revealed from the nuclide production in fragmentation reactions

NUCLEAR REACTIONS Ti(238U, X), E=1 GeV/nucleon; measured isotopic production σ; deduced nuclear structure effects. High-resolution magnetic spectrometer, statistical model analysis.

doi: 10.1016/j.nuclphysa.2004.01.069
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2003BE45      Nucl.Phys. A725, 213 (2003)

M.Bernas, P.Armbruster, J.Benlliure, A.Boudard, E.Casarejos, S.Czajkowski, T.Enqvist, R.Legrain, S.Leray, B.Mustapha, P.Napolitani, J.Pereira, F.Rejmund, M.-V.Ricciardi, K.-H.Schmidt, C.Stephan, J.Taieb, L.Tassan-Got, C.Volant

Fission-residues produced in the spallation reaction 238U + p at 1 A GeV

NUCLEAR REACTIONS 1H(238U, X), E=1 GeV/nucleon; measured fission fragments isotopic production σ, velocity distributions. High-resolution magnetic spectrometer. Application to accelerator-driven subcritical reactors and radioactive beam production discussed. Comparison with model predictions.

doi: 10.1016/S0375-9474(03)01576-8
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2003NA18      Yad.Fiz. 66, 1517 (2003); Phys.Atomic Nuclei 66, 1471 (2003)

P.Napolitani, K.-H.Schmidt, P.Armbruster, A.S.Botvina, M.V.Ricciardi, L.Tassan-Got, F.Rejmund, T.Enqvist

Determination of the Freeze-Out Temperature by the Isospin Thermometer

NUCLEAR REACTIONS Pb(238U, X), 2H, Ti(208Pb, X), 1H, Ti(56Fe, X), E=1 GeV/nucleon; Be(86Kr, X), E=500 MeV/nucleon; Ta(p, X), E=5.7 GeV; Au(p, X), E=11.5 GeV; analyzed fragment mass yields; deduced thermometer based on neutron excess.

doi: 10.1134/1.1601752
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2003NA26      Nucl.Phys. A727, 120 (2003)

P.Napolitani, L.Tassan-Got, P.Armbruster, M.Bernas

A model for consecutive spallation and fragmentation reactions in inverse kinematics at relativistic energies

NUCLEAR REACTIONS 1H(238U, X), E=1 GeV/nucleon; calculated fragments isotopic yields following secondary and multiple reactions. Application to radioactive beam production discussed.

doi: 10.1016/j.nuclphysa.2003.07.001
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2003RI15      Acta Phys.Hung.N.S. 18, 371 (2003)

M.V.Ricciardi, K.-H.Schmidt, P.Napolitani, A.V.Ignatyuk, F.Rejmund

Structural Effects in Nuclide Distributions from Fission and Fragmentation

NUCLEAR REACTIONS Ti(238U, X), E=1 GeV/nucleon; analyzed fragment yields; deduced structure effects.

doi: 10.1556/APH.18.2003.2-4.44
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2002RE36      Acta Phys.Hung.N.S. 16, 85 (2002)

F.Rejmund, A.Bethenod, P.Napolitani, J.Taieb, C.Villagrasa, L.Audouin, P.Armbruster, C.O.Bacri, J.Benlliure, M.Bernas, B.Berthier, A.Boudard, E.Casajeros, S.Czajkowski, J.J.Connell, T.Enqvist, T.Faestermann, J.S.George, A.Junghans, B.Jurado, F.Hammache, S.Leray, R.Legrain, R.A.Mewaldt, J.Pereira, M.V.Ricciardi, K.-H.Schmidt, C.Stephan, K.Summerer, L.Tassan-Got, C.Volant, M.E.Wiedenbeck, W.Wlazlo, N.E.Yanasak

Disappearance of Shell Effects and Persistence of an Even-Odd Staggering in the Fragment Production in Nuclear Reactions at Relativistic Energies

NUCLEAR REACTIONS 1H(U, X), (Fe, X), E=1 GeV/nucleon; measured fragments isotopic yields; deduced shell and pairing effects.

doi: 10.1556/APH.16.2002.1-4.10
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