NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = Z.Basrak Found 63 matches. 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
2016BA24 Phys.Rev. C 93, 054609 (2016) Z.Basrak, P.Eudes, V.de la Mota Aspects of the momentum dependence of the equation of state and of the residual NN cross section, and their effects on nuclear stopping NUCLEAR REACTIONS 129Xe(120Sn, X), E=12-100 MeV/nucleon; calculated nuclear stopping, energy-based isotropy ratio as stopping observable; investigated nuclear equation of state, effects of zero-range and non-local nuclear mean field, role of nucleon-nucleon residual interaction, isospin, energy and angular dependence of nucleon-nucleon cross section, in-medium modifications of nucleon-nucleon cross section, simplified parametrization of angular dependence of neutron-proton and proton-proton cross section; deduced fixed set of model parameters for energies below Fermi energy, for energies above Fermi energy model reproduces experimental data by parameters of in-medium modification of nucleon-nucleon cross section that smoothly evolve with energy, strong reduction of free nucleon-nucleon cross section around Fermi energy, effects of reaction centrality. Through Heavy-Ion Phase-Space Event generator (HIPSE) deduced that high multiplicity events are spread over a broad impact parameter range. Semiclassical Landau-Vlasov transport model (BUU type).
doi: 10.1103/PhysRevC.93.054609
2016GA21 Eur.Phys.J. A 52, 177 (2016) P.Gasik, K.Piasecki, N.Herrmann, Y.Leifels, T.Matulewicz, A.Andronic, R.Averbeck, V.Barret, Z.Basrak, N.Bastid, M.L.Benabderrahmane, M.Berger, P.Buehler, M.Cargnelli, R.Caplar, P.Crochet, O.Czerwiakowa, I.Deppner, P.Dupieux, M.Dzelalija, L.Fabbietti, Z.Fodor, I.Gasparic, Y.Grishkin, O.N.Hartmann, K.D.Hildenbrand, B.Hong, T.I.Kang, J.Kecskemeti, Y.J.Kim, M.Kirejczyk, M.Kis, P.Koczon, R.Kotte, A.Lebedev, A.Le Fevre, J.L.Liu, X.Lopez, V.Manko, J.Marton, R.Munzer, M.Petrovici, F.Rami, A.Reischl, W.Reisdorf, M.S.Ryu, P.Schmidt, A.Schuttauf, Z.Seres, B.Sikora, K.S.Sim, V.Simion, K.Siwek-Wilczynska, V.Smolyankin, K.Suzuki, Z.Tyminski, P.Wagner, I.Weber, E.Widmann, K.Wisniewski, Z.G.Xiao, I.Yushmanov, Y.Zhang, A.Zhilin, V.Zinyuk, J.Zmeskal Strange meson production in Al+Al collisions at 1.9 A GeV
doi: 10.1140/epja/i2016-16177-y
2016RU03 Phys.Rev. C 94, 034608 (2016) P.Russotto, S.Gannon, S.Kupny, P.Lasko, L.Acosta, M.Adamczyk, A.Al-Ajlan, M.Al-Garawi, S.Al-Homaidhi, F.Amorini, L.Auditore, T.Aumann, Y.Ayyad, Z.Basrak, J.Benlliure, M.Boisjoli, K.Boretzky, J.Brzychczyk, A.Budzanowski, C.Caesar, G.Cardella, P.Cammarata, Z.Chajecki, M.Chartier, A.Chbihi, M.Colonna, M.D.Cozma, B.Czech, E.De Filippo, M.Di Toro, M.Famiano, I.Gasparic, L.Grassi, C.Guazzoni, P.Guazzoni, M.Heil, L.Heilborn, R.Introzzi, T.Isobe, K.Kezzar, M.Kis, A.Krasznahorkay, N.Kurz, E.La Guidara, G.Lanzalone, A.Le Fevre, Y.Leifels, R.C.Lemmon, Q.F.Li, I.Lombardo, J.Lukasik, W.G.Lynch, P.Marini, Z.Matthews, L.May, T.Minniti, M.Mostazo, A.Pagano, E.V.Pagano, M.Papa, P.Pawlowski, S.Pirrone, G.Politi, F.Porto, W.Reviol, F.Riccio, F.Rizzo, E.Rosato, D.Rossi, S.Santoro, D.G.Sarantites, H.Simon, I.Skwirczynska, Z.Sosin, L.Stuhl, W.Trautmann, A.Trifiro, M.Trimarchi, M.B.Tsang, G.Verde, M.Veselsky, M.Vigilante, Y.Wang, A.Wieloch, P.Wigg, J.Winkelbauer, H.H.Wolter, P.Wu, S.Yennello, P.Zambon, L.Zetta, M.Zoric Results of the ASY-EOS experiment at GSI: The symmetry energy at suprasaturation density NUCLEAR REACTIONS 197Au(197Au, X), E=400 MeV/nucleon; measured directed and elliptic flow of neutrons and charged particles as a function of rapidity and transverse momentum in central and semi-central collisions using Large Area Neutron Detector (LAND), parts of CHIMERA multidetector, ALADIN Time-of-flight Wall, KRATTA telescopes, and Washington University Microball detector as part of ASY-EOS experimental campaign at GSI facility; deduced density dependence of nuclear symmetry energy, equation-of-state (EOS) of neutron-rich matter. Comparison with UrQMD transport model calculations.
doi: 10.1103/PhysRevC.94.034608
2014EU01 Phys.Rev. C 90, 034609 (2014) P.Eudes, Z.Basrak, F.Sebille, V.de la Mota, G.Royer Comprehensive analysis of fusion data well above the barrier NUCLEAR REACTIONS 12C(14N, X)26Al*, E=3.14, 3.80, 4.29, 6.16, 7.59, 10.39, 11.29, 11.94, 12.72, 17.71 MeV/nucleon; 16O(20Ne, X)36Ar*, E=3.40, 5.74, 6.10, 6.85, 7.80 MeV/nucleon; 12C(24Mg, X)36Ar*, E=25.0, 35.0, 45.0 MeV/nucleon; 27Al(12C, X)39K*, E=5.32, 6.75, 7.14, 8.04, 8.13, 15.00 MeV/nucleon; 24Mg(16O, X)40Ca*, E=3.00, 3.25, 3.50, 3.81, 4.13, 4.50, 5.06 MeV/nucleon; 20Ne(20Ne, X)40Ca*, E=3.40, 5.85, 6.30, 7.00, 7.80 MeV/nucleon; 12C(28Si, X)40Ca*, E=3.57, 4.46, 5.36, 5.71, 6.36, 6.43, 11.04, 14.18, 16.14 MeV/nucleon; 27Al(14N, X)41Ca*, E=11.21, 18.7 MeV/nucleon; 26Mg(16O, X)42Ca*, E=3.11, 3.36, 3.67, 3.85, 4.04, 4.49, 5.06 MeV/nucleon; 24Mg(18O, X)42Ca*, E=3.05, 3.33, 3.50, 3.72, 4.00 MeV/nucleon; 27Al(16O, X)43Sc*, E=3.13, 3.75, 4.06, 4.38, 4.69, 5.00, 5.06, 6.56, 7.88, 10.50, 13.44 MeV/nucleon; 12C(32S, X)44Ti*, E=3.21, 3.40, 4.10, 4.53, 5.00, 19.50 MeV/nucleon; 26Mg(20Ne, X)46Ti*, E=3.00, 4.20, 4.65, 5.25, 6.00, 7.50, 10.10, 14.50, 19.75 MeV/nucleon; 27Al(20Ne, X)47V*, E=3.00, 4.05, 4.25, 4.65, 5.25, 6.00, 6.90, 7.50, 9.00, 10.50, 14.50, 19.75 MeV/nucleon; 12C(35Cl, X)47V*, E=3.57, 4.00, 4.40, 5.14, 5.71, 7.94 MeV/nucleon; 32S(16O, X)48Cr*, E=10.50 MeV/nucleon; 40Ca(16O, X)56Ni*, E=3.11, 3.47, 3.92, 4.65, 6.47, 8.73, 13.38 MeV/nucleon; 28Si(28Si, X)56Ni*, E=3.21, 3.57, 3.93, 4.29, 5.00, 6.21, 7.68, 8.57, 11.04, 12.04, 14.18, 16.14, 19.70, 20.00, 22.00, 26.00, 30.00, 35.00 MeV/nucleon; 24Mg(32S, X)56Ni*, E=3.95, 4.40, 5.00, 5.75, 6.06, 6.25, 7.47, 8.69 MeV/nucleon; 40Ca(19F, X)59Cu*, E=3.45, 4.13, 5.03, 5.42, 6.00, 9.00, 11.37 MeV/nucleon; 27Al(32S, X)59Cu*, E=4.43, 4.77, 5.47, 5.86, 7.09, 7.94, 10.00, 10.50, 11.44, 12.28 MeV/nucleon; 24Mg(35Cl, X)59Cu*, E=7.86, 8.07 MeV/nucleon; 48Ti(12C, X)60Ni*, E=6.75, 8.13, 15.00 MeV/nucleon; 40Ca(23Na, X)63Ga*, E=11.30, 12.48 MeV/nucleon; Ti(16O, X), E=14.19, 19.38 MeV/nucleon; 52Cr(14N, X)66Ga*, E=11.21, 18.71 MeV/nucleon; 27Al(40Ar, X)67Ga*, E=55.00 MeV/nucleon; 40Ca(28Si, X)68Se*, E=10.64, 11.04, 11.68, 14.18, 16.14 MeV/nucleon; 58Ni(12C, X)70Se*, E=5.32, 6.75, 8.04, 8.13, 15.00 MeV/nucleon; 58Ni(14N, X)72Br*, E=11.21, 18.71 MeV/nucleon; K, Cl(36Ar, X), E=31.58, 40.03, 51.78 MeV/nucleon; 63Cu(12C, X)75Br*, E=5.32, 6.75, 8.04, 8.13 MeV/nucleon; 40Ca(40Ar, X)80Sr*, E=4.02, 4.75, 5.90, 6.83, 15.00, 20.00, 30.00 MeV/nucleon; 40Ca(40Ca, X)80Zr*, E=3.55, 3.67, 3.85, 4.05, 4.25, 4.38, 4.55, 4.88, 7.50 MeV/nucleon; 27Al(58Ni, X)85Nb*, E=28.00 MeV/nucleon; 63Cu(24Mg, X)87Nb*, E=6.71, 9.38, 11.71, 14.21 MeV/nucleon; 45Sc(48Ti, X)93Tc*, E=15.98 MeV/nucleon; 58Ni(36Ar, X)94Pd*, E=31.58, 40.03, 51.78 MeV/nucleon; 92Mo(16O, X)108Sn*, E=11.70 MeV/nucleon; 76Ge(32S, X)108Cd*, E=4.94, 5.56, 6.19, 6.81, 7.03 MeV/nucleon; 68Zn(40Ar, X)108Cd*, E=14.60, 19.60, 27.55, 35.00 MeV/nucleon; 56Fe(52Cr, X)108Sn*, E=5.10 MeV/nucleon; 93Nb(19F, X)112Sn*, E=3.84, 5.00 MeV/nucleon; 48Ti(64Zn, X)112Te*, E=35.00, 50.00 MeV/nucleon; 58Ni(58Ni, X)116Ba*, E=32.00, 40.50, 51.50, 63.50 MeV/nucleon; 100Mo(18O, X)118Sn*, E=5.56, 8.33, 9.39, 10.28, 12.06 MeV/nucleon; 40Ca(78Kr, X)118Ba*, E=5.50 MeV/nucleon; 40Ca(82Kr, X)122Ba*, E=5.50 MeV/nucleon; 124Sn(12C, X)136Ba*, E=30.00, 49.00, 84.00 MeV/nucleon; 124Sn(14N, X)138La*, E=10.00, 20.00, 30.00 MeV/nucleon; 124Sn(20Ne, X)144Nd*, E=20.00, 30.00 MeV/nucleon; 108Ag(40Ar, X)148Tb*, E=4.22, 4.93, 5.90, 7.20, 8.40, 8.43, 27.40 MeV/nucleon; 65Cu(84Kr, X)149Ho*, E=5.88, 7.19 MeV/nucleon; 116Sn(40Ar, X)156Er*, E=4.63, 5.50, 6.78, 8.48 MeV/nucleon; 121Sb(40Ar, X)161Tm*, E=4.97, 5.65, 7.05, 7.50 MeV/nucleon; 146Nd(16O, X)162Er*, E=10.06 MeV/nucleon; 30Si(132Xe, X)162Er*, E=5.40, 5.90, 6.60, 7.50, 8.20 MeV/nucleon; 124Sn(40Ar, X)164Er*, E=24.00, 27.00 MeV/nucleon; 154Sm(14N, X)168Tm*, E=35.00, 100.00, 130.00, 135.00 MeV/nucleon; 159Tb(14N, X)173Hf*, E=22.07, 35.00, 100.00 MeV/nucleon; 159Tb(16O, X)175Ta*, E=14.00, 25.00 MeV/nucleon; 159Tb(20Ne, X)179Re*, E=8.00, 10.00, 13.00, 16.00 MeV/nucleon; 124Sn(58Ni, X)182Pt*, E=3.96, 4.12.4.28.4.66.5.00 MeV/nucleon; 165Ho(20Ne, X)185Ir*, E=30.00 MeV/nucleon; 169Tm(20Ne, X)189Au*, E=8.00, 10.00, 13.00, 16.00 MeV/nucleon; 182W(12C, X)194Hg*, E=10.08, 13.92 MeV/nucleon; 175Lu(19F, X)194Hg*, E=7.11, 9.68 MeV/nucleon; 154Sm(40Ar, X)194Hg*, E=5.53, 6.80, 8.50 MeV/nucleon; 181Ta(14N, X)195Hg*, E=35.00 MeV/nucleon; 181Ta(16O, X)197Tl*, E=14.00, 25.00 MeV/nucleon; 164Dy(40Ar, X)204Po*, E=5.53, 6.80, 8.48 MeV/nucleon; 181Ta(24Mg, X)205At*, E=11.25, 13.96, 14.17 MeV/nucleon; 165Ho(40Ar, X)205At*, E=5.65, 7.00, 7.50, 7.88, 8.50, 9.77 MeV/nucleon; 197Au(12C, X)209At*, E=86.00 MeV/nucleon; 197Au(14N, X)211Rn*, E=35.00, 100.00, 130.00, 155.00 MeV/nucleon; 197Au(16O, X)213Fr*, E=14.00, 107.00 MeV/nucleon; 197Au(20Ne, X)217Ac*, E=7.50, 11.00, 14.50, 20.00, 30.00 MeV/nucleon; 197Au(40Ar, X)237Bk*, E=5.47, 5.68, 6.20, 6.75, 8.40, 8.48, 8.57 MeV/nucleon; 209Bi(20Ne, X)229Np*, E=30.00 MeV/nucleon; 232Th(14N, X)246Bk*, E=30.00 MeV/nucleon; 238U(40Ar, X)278Ds*, E=6.25, 7.50, 8.50, 10.40 MeV/nucleon; Analyzed 382 complete and incomplete fusion σ data relative to 81 systems, A=26-278, E ≈ 3-155 MeV/nucleon; distinguished evaporation and fusion-fission mechanisms; deduced universal homographic law of fusion from properly normalized and scaled fusion σ(E) data, threshold for incomplete fusion, energy of vanishing of complete and incomplete fusion; proposed a reaction mechanism for fusion disappearance.
doi: 10.1103/PhysRevC.90.034609
2014EU02 Nucl.Phys. A930, 131 (2014) P.Eudes, Z.Basrak, V.de la Mota, G.Royer Is there incomplete fusion mechanism beyond 100A MeV?
doi: 10.1016/j.nuclphysa.2014.07.035
2013EU01 Europhys.Lett. 104, 22001 (2013) P.Eudes, Z.Basrak, F.Sebille, V.de la Mota, G.Royer Towards a unified description of evaporation-residue fusion cross-sections above the barrier NUCLEAR REACTIONS 124Sn(12C, X), 28Si(28Si, X), 96Zr(36Ar, X), E<20 MeV/nucleon; analyzed available data for 300 fusion evaporation σ; deduced a universal homographic law. DYWAN microscopic transport model.
doi: 10.1209/0295-5075/104/22001
2006SZ06 Nucl.Phys. A779, 21 (2006) S.Szilner, F.Haas, Z.Basrak, R.M.Freeman, A.Morsad, M.P.Nicoli Competition between direct and dissipative processes in the binary channels of the 16O + 12C and 18O + 12C reactions NUCLEAR REACTIONS 12C(16O, 16O'), (16O, 15O), (16O, 14N), E=62-124 MeV; 12C(18O, 18O'), (18O, 17O), (18O, 16O), (18O, 15N), (18O, 19F), (18O, 20Ne), E=66-120 MeV; measured particle spectra, σ(E, θ), σ; deduced reaction mechanism features.
doi: 10.1016/j.nuclphysa.2006.09.007
2004BA56 Nucl.Phys. A738, 463 (2004) Weakened nuclear opacity and binary reactions
doi: 10.1016/j.nuclphysa.2004.04.087
2004DZ02 Nucl.Phys. A738, 483 (2004) M.Dzelalija, Z.Basrak, R.Caplar Cell-size and generalized entropy determination in heavy-ion reactions
doi: 10.1016/j.nuclphysa.2004.04.092
2004WO09 Acta Phys.Pol. B35, 1165 (2004) K.Wosinska, J.Pluta, F.Hanappe, L.Stuttge, J.C.Angelique, Z.Basrak, B.Benoit, E.de Goes Brennand, G.Bizard, J.Colin, G.Costa, P.Desesquelles, O.Dorvaux, D.Durand, B.Erazmus, S.Kuleshov, R.Lednicky, P.Leszczynski, M.Marques, Th.Materna, K.Mikhailov, G.Papatheofanous, T.Pawlak, M.Przewlocki, A.Staranowicz, A.Stavinskiy, A.Sztenkiel, B.Tamain, A.Vlasov, L.Vorobyev Influence of the Coulomb Field on Charged Particle Emission in Ar + Ni Reaction at 77 MeV/u NUCLEAR REACTIONS 58Ni(40Ar, X), E=77 MeV/nucleon; measured Ep, En, angular distributions; deduced mean quasi-projectile charge. Comparison with model predictions.
2003BB16 Fizika(Zagreb) B 12, 145 (2003) Orbiting-cluster model with combinatorial level density NUCLEAR REACTIONS 12C, 16,18O, 20Ne, 24Mg, 28Si, 32S(12C, X), 16O(14C, X), 16O, 24Mg, 28Si(16O, X), 24Mg, 28Si(24Mg, X), 28Si(28Si, X), 58,60,62Ni(58Ni, X), 64Zn(54Fe, X), 60Ni(60Ni, X), 70Ge(50Cr, X), E not given; calculated statistical and combinatorial level densities; deduced molecular resonance features. Orbiting-cluster model.
2003DZ04 Fizika(Zagreb) B 12, 73 (2003) M.Dzelalija, Z.Basrak, R.Caplar Determination of generalized entropy in heavy-ion collisions
2003MA01 Nucl.Phys. A714, 89 (2003) A.Mangiarotti, N.Herrmann, P.R.Maurenzig, A.Gobbi, R.Kotte, J.Kecskemeti, Y.Leifels, J.P.Alard, A.Andronic, R.Averbeck, V.Barret, Z.Basrak, N.Bastid, I.Belyaev, A.Bendarag, G.Berek, R.Caplar, P.Crochet, A.Devismes, P.Dupieux, M.Dzelalija, Ch.Finck, Z.Fodor, Y.Grishkin, O.Hartmann, K.D.Hildenbrand, B.Hong, Y.J.Kim, M.Kirejczyk, P.Koczon, M.Korolija, T.Kress, R.Kutsche, A.Lebedev, V.Manko, M.Merschmeyer, D.Moisa, A.Nianine, W.Neubert, D.Pelte, M.Petrovici, C.Plettner, F.Rami, W.Reisdorf, B.de Schauenburg, D.Schull, Z.Seres, B.Sikora, K.S.Sim, V.Simion, K.Siwek-Wilczynska, V.Smolyankin, M.Stockmeier, G.Stoicea, M.Vasiliev, P.Wagner, K.Wisniewski, D.Wohlfarth, I.Yushmanov, A.Zhilin Sub-Threshold φ-meson yield in central 58Ni + 58Ni collisions NUCLEAR REACTIONS 58Ni(58Ni, X), E=1.93 GeV/nucleon; measured charged particle spectra, multiplicities, φ-meson production σ. Comparison with model predictions.
doi: 10.1016/S0375-9474(02)01366-0
2003SZ11 Fizika(Zagreb) B 12, 117 (2003) Weak absorption and resonances in light heavy-ion reactions induced by the non-α-type 14C nucleus NUCLEAR REACTIONS 12,14C, 16O(14C, 14C), (14C, 14C'), (14C, X), E(cm) ≈ 6-35 MeV; measured excitation functions, σ(θ); deduced resonance features, refractive effects.
2003SZ12 Acta Phys.Hung.N.S. 18, 285 (2003) Consequences of Weak Absorption in Light Heavy-Ion Reactions: Molecular Resonances and Nuclear Rainbows NUCLEAR REACTIONS 12C(12C, 12C), E=102 MeV; 12C(16O, 16O), E=116 MeV; 16O(16O, 16O), E=124 MeV; analyzed σ(θ); deduced optical potential features.
doi: 10.1556/APH.18.2003.2-4.27
2002SZ03 Eur.Phys.J. A 13, 273 (2002) S.Szilner, W.von Oertzen, Z.Basrak, F.Haas, M.Milin Elastic α-Transfer in the Elastic Scattering of 16O + 12C NUCLEAR REACTIONS 12C(16O, 16O), E=100-124 MeV; calculated σ(θ) including the effect of α-transfer. Comparison with data, coupled-channels.
doi: 10.1007/s10050-002-8754-9
2002WO04 Acta Phys.Pol. B33, 507 (2002) K.Wosinska, J.Pluta, F.Hanappe, L.Stuttge, J.C.Angelique, Z.Basrak, B.Benoit, E.de Goes Brennand, G.Bizard, J.Colin, G.Costa, P.Desesquelles, O.Dorvaux, D.Durand, B.Erazmus, A.Kieliszek, S.Kuleshov, R.Lednicky, P.Leszczynski, M.Marques, Th.Materna, K.Mikhailov, K.Miller, G.Papatheofanous, T.Pawlak, M.Przewlocki, A.Staranowicz, A.Stavinsky, B.Tamain, A.Vlasov Parameters of Emitting Sources in Ar-Ni Reaction at 77 MeV/u NUCLEAR REACTIONS Ni(Ar, X), E=77 MeV/nucleon; analyzed neutron spectra, two-neutron correlation functions; deduced source features.
2001SZ05 Phys.Rev. C64, 064614 (2001) S.Szilner, M.P.Nicoli, Z.Basrak, R.M.Freeman, F.Haas, A.Morsad, M.E.Brandan, G.R.Satchler Refractive Elastic Scattering of Carbon and Oxygen Nuclei: The mean field analysis and Airy structures NUCLEAR REACTIONS 12C(16O, 16O), E=62-124 MeV; 12C(18O, 18O), E=66-120 MeV; measured σ(θ); deduced potential features. Optical model analysis, Airy structures.
doi: 10.1103/PhysRevC.64.064614
2001TU06 Eur.Phys.J. A 12, 327 (2001) A.Tumino, M.Lattuada, S.Romano, C.Spitaleri, D.Vinciguerra, Z.Basrak, O.Yu.Goryunov, V.V.Ostashko, S.Szilner, P.Figuera, D.Lo Presti, C.Petta, N.Randazzo, S.Reito, G.V.Russo, S.Tudisco 16O-8Be Break-Up States and Cluster Structure of 24Mg NUCLEAR REACTIONS 12C(16O, α), E=109 MeV; measured (particle)(particle)-coin, σ(θ) following breakup of residual nucleus. 24Mg deduced resonance energies, possible J, π. Comparison with earlier data and Cranked Cluster model calculations.
doi: 10.1007/s100500170010
2000BA44 Acta Phys.Pol. B31, 361 (2000) Onset of Binary Processes: A new observable for the in-medium NN cross section NUCLEAR REACTIONS 36Ar(36Ar, X), E=29, 30 MeV/nucleon; calculated density contours vs time; deduced binary mechanism threshold energy, dependence on nucleon-nucleon cross section. Landau-Vlasov semiclassical transport model.
2000EU04 Eur.Phys.J. A 9, 207 (2000) Dynamical Effects on the Quasiprojectile Temperature in the Ar + Al Reaction NUCLEAR REACTIONS 27Al(Ar, X), E=65 MeV/nucleon; calculated fragment energy spectra, quasiprojectile temperature features. Landau-Vlasov semiclassical transport model.
doi: 10.1007/s100500070039
2000NI03 Phys.Rev. C61, 034609 (2000) M.P.Nicoli, F.Haas, R.M.Freeman, S.Szilner, Z.Basrak, A.Morsad, G.R.Satchler, M.E.Brandan Detailed Study and Mean Field Interpretation of 16O + 12C Elastic Scattering at Seven Medium Energies NUCLEAR REACTIONS 12C(16O, 16O), E=62-124 MeV; measured σ(θ); deduced parameters. Optical model analysis, Woods-Saxon and folding-model potentials. Comparison with potentials at higher energies and for similar systems.
doi: 10.1103/PhysRevC.61.034609
2000PL12 Eur.Phys.J. A 9, 63 (2000) J.Pluta, K.Wosinska, Z.Basrak, G.Bizard, B.Benoit, P.Desesquelles, O.Dorvaux, D.Durand, B.Erazmus, F.Hanappe, B.Jakobsson, C.Lebrun, F.R.Lecolley, R.Lednicky, P.Leszczynski, K.Mikhailov, K.Miller, B.Noren, T.Pawlak, M.Przewlocki, O.Skeppstedt, A.Staranowicz, A.Stavinsky, L.Stuttge, B.Tamain Two-Neutron Correlations at Small Relative Momenta in 40Ar + 197Au Collisions at 60 MeV/nucleon NUCLEAR REACTIONS 197Au(40Ar, nX), E=60 MeV/nucleon; measured neutron spectra, angular distributions, two-neutron correlations; deduced emission source features. Dynamical Landau-Vlasov model.
doi: 10.1007/s100500070056
1999EU01 Nucl.Phys. (Supplement) A654, 769c (1999) Does One Create Very Hot Nuclei in Heavy-Ion Reactions Below 100 MeV/u ? NUCLEAR REACTIONS Al(Ar, X), E=65 MeV/nucleon; calculated density profile plots, charged particle multiplicities and rapidity distributions vs impact parameter, charged particle spectra slope parameters. Landau-Vlasov approach.
doi: 10.1016/S0375-9474(00)88544-9
1999FR07 Eur.Phys.J. A 4, 239 (1999) R.M.Freeman, F.Haas, M.-P.Nicoli, A.Morsad, Z.Basrak Recurring Angular Distribution Patterns in Resonant Heavy-Ion Reactions NUCLEAR REACTIONS 12C(12C, 8Be), E(cm)=32.5 MeV; 16O(14C, 15N), E(cm)=23.4, 27.4 MeV; 12C(18O, 16O), E(cm)=22.4, 23.4, 24.3 MeV; analyzed σ(θ); deduced resonance-like structures partial wave interference effects.
doi: 10.1007/s100500050226
1999HA45 Phys.Rev. C60, 031603 (1999) F.Haddad, Ph.Eudes, Z.Basrak, F.Sebille Signature of Geometrical Effects in Heavy-Ion Reactions below 100 MeV/Nucleon NUCLEAR REACTIONS 27Al, 107Ag(40Ar, X), 40Ar(107Ag, X), 58Ni(36Ar, X), 129Sn(120Xe, X), E=41-100 MeV/nucleon; calculated charged particle dynamical emission percentage vs energy, impact parameter. Landau-Vlasov model, comparison with data.
doi: 10.1103/PhysRevC.60.031603
1999NI08 Phys.Rev. C60, 064608 (1999) M.P.Nicoli, F.Haas, R.M.Freeman, N.Aissaoui, C.Beck, A.Elanique, R.Nouicer, A.Morsad, S.Szilner, Z.Basrak, M.E.Brandan, G.R.Satchler Elastic Scattering of 16O + 16O at Energies E/A between 5 and 8 MeV NUCLEAR REACTIONS 16O(16O, 16O), E=75-124 MeV; measured σ(θ); deduced phenomenological and microscopic potentials. Optical model, interpretation in terms of Airy minima and the dispersion relation.
doi: 10.1103/PhysRevC.60.064608
1999NI14 Nucl.Phys. (Supplement) A654, 882c (1999) M.P.Nicoli, F.Haas, R.M.Freeman, N.Aissaoui, C.Beck, A.Elanique, R.Nouicer, A.Morsad, S.Szilner, Z.Basrak, M.E.Brandan Refractive Effects in the Elastic Scattering of Light Heavy Ions between 5 and 10 MeV/n: The 16O + 16O reaction NUCLEAR REACTIONS 16O(16O, 16O), E=75-124 MeV; measured σ(θ); deduced refractive effects. Optical model analysis.
doi: 10.1016/S0375-9474(00)88565-6
1999SZ01 J.Phys.(London) G25, 1927 (1999) S.Szilner, Z.Basrak, R.M.Freeman, F.Haas, A.Morsad, M.P.Nicoli, C.Beck Excitation Functions of Inelastic and Transfer Channels in 12C + 12C between Ec.m. = 30 and 60 MeV NUCLEAR REACTIONS 12C(12C, 12C'), (12C, 10B), (12C, 11B), E(cm)=30-60 MeV; measured σ(E); deduced intermediate structure resonances.
doi: 10.1088/0954-3899/25/9/311
1998DZ03 Int.J.Mod.Phys. E7, 593 (1998) M.Dzelalija, N.Cindro, Z.Basrak, R.Caplar, M.Korolija, I.Mishustin A Simple Method for Estimating Temperatures in Central Nucleus-Nucleus Collisions: Application to Au + Au from 100 to 400 A MeV NUCLEAR REACTIONS 197Au(197Au, X), E=100, 150, 250, 400 MeV/nucleon; analyzed data; deduced temperature, thermal, collective flow components.
doi: 10.1142/S0218301398000336
1997BA79 Nucl.Phys. A624, 472 (1997) Z.Basrak, P.Eudes, P.Abgrall, F.Haddad, F.Sebille Effects of the Mean-Field Dynamics and the Phase-Space Geometry on the Cluster Formation NUCLEAR REACTIONS 27Al(40Ar, X), E=65 MeV/nucleon; calculated density vs time, charge, rapidity, multiplicity distributions. Dynamically generated one-body phase space, Landau-Vlasov model.
doi: 10.1016/S0375-9474(97)00393-X
1997EU01 Phys.Rev. C56, 2003 (1997) Dynamical Aspects of Particle Emission in Binary Dissipative Collisions: Effects on hot-nuclei formation NUCLEAR REACTIONS 27Al(40Ar, X), E=65 MeV/nucleon; analyzed light charged particle rapidity distributions, multiplicity, invariant σ; deduced dynamical effects. Landau-Vlasov model.
doi: 10.1103/PhysRevC.56.2003
1997HA63 Nuovo Cim. 110A, 989 (1997) F.Haas, A.Elanique, R.M.Freeman, C.Beck, R.Nouicer, D.L.Watson, C.Jones, R.Cowin, P.Lee, Z.Basrak Search for Electromagnetic Transitions between 12C-12C Cluster States in 24Mg NUCLEAR REACTIONS 12C(12C, 12C'), (12C, 8Be), (12C, α), E=32.9 MeV; measured Eγ, Iγ, γγ-, (fragment)γ-, (fragment)(fragment)-coin, Q-value spectra. 24Mg deduced resonance cluster configuration.
doi: 10.1007/BF03035936
1997RO06 Z.Phys. A358, 73 (1997) C.Roy, C.Kuhn, J.P.Coffin, P.Crochet, P.Fintz, G.Guillaume, F.Jundt, C.Maazouzi, F.Rami, L.Tizniti, P.Wagner, J.P.Alard, V.Amouroux, Z.Basrak, N.Bastid, I.Belyaev, D.Best, J.Biegansky, A.Buta, R.Caplar, N.Cindro, R.Dona, P.Dupieux, M.Dzelalija, Z.G.Fan, Z.Fodor, L.Fraysse, A.Gobbi, N.Herrmann, K.D.Hildenbrand, S.Holbling, B.Hong, S.C.Jeong, J.Kecskemeti, M.Kirejczyk, P.Koncz, Y.Korchagin, R.Kotte, A.Lebedev, I.Legrand, Y.Leifels, V.Manko, G.Mgebrishvili, D.Moisa, J.Mosner, W.Neubert, D.Pelte, M.Petrovici, C.Pinkenburg, P.Pras, W.Reisdorf, J.L.Ritman, A.G.Sadchikov, D.Schull, Z.Seres, B.Sikora, V.Simion, V.Smolyankin, U.Sodan, M.Trzaska, M.Vasiliev, G.S.Wang, J.P.Wessels, T.Wienold, D.Wohlfarth, A.Zhilin, J.Konopka, H.Stocker Shape of Collective Flow in Highly Central Au(150 A MeV)+Au Collisions NUCLEAR REACTIONS 197Au(197Au, X), E=150 MeV/nucleon; measured fragment transverse momentum per nucleon vs rapidity, light charged-particle σ(θ); deduced flow pattern in highly central collisions. FOPI detector.
doi: 10.1007/s002180050278
1997SZ01 Phys.Rev. C55, 1312 (1997) S.Szilner, Z.Basrak, R.M.Freeman, F.Haas, A.Morsad, C.Beck Excitation Functions of Inelastic and Transfer Channels in 12C + 12C Around E(cm) = 32.5 MeV NUCLEAR REACTIONS 12C(12C, 12C), (12C, 12C'), (12C, 16O), E(cm)=30-35 MeV; measured σ(θ), σ(E); deduced intermediate structure.
doi: 10.1103/PhysRevC.55.1312
1996DZ03 Acta Phys.Hung.N.S. 3, 245 (1996) M.Dzelalija, M.Korolija, N.Cindro, Z.Basrak, R.Caplar, K.Sparavec Neutron-to-Proton Ratios in Heavy-Ion Reactions NUCLEAR REACTIONS 58Ni(36Ar, X), E=52-95 MeV/nucleon; calculated fragments neutron-to-proton ratios. Comparison with data.
1995DZ01 Phys.Rev. C52, 346 (1995) M.Dzelalija, N.Cindro, Z.Basrak, R.Caplar, S.Holbling, M.Bini, P.R.Maurenzig, A.Olmi, G.Pasquali, G.Poggi, N.Taccetti, C.Cerruti, J.P.Coffin, R.Dona, P.Fintz, G.Guillaume, A.Houari, F.Jundt, C.Kuhn, F.Rami, R.Tezkratt, P.Wagner, J.Biegansky, R.Kotte, J.Mosner, W.Neubert, D.Wohlfarth, J.P.Alard, V.Amouroux, N.Bastid, L.Berger, I.M.Belayev, S.Boussange, A.Buta, P.Dupieux, J.Ero, Z.Fodor, L.Fraysse, A.Gobbi, N.Herrmann, K.D.Hildenbrand, M.Ibnouzahir, J.Kecskemeti, P.Koncz, Y.Korchagin, M.Kramer, A.Lebedev, I.Legrand, V.Manko, G.Mgebrishvili, D.Moisa, G.Montarou, I.Montbel, D.Pelte, M.Petrovici, P.Pras, V.Ramillien, W.Reisdorf, D.Schull, Z.Seres, B.Sikora, V.Simion, S.Smolyankin, U.Sodan, M.Trzaska, M.A.Vasiliev, J.P.Wessels, T.Wienold, Z.Wilhelmi, A.V.Zhilin Entropy in Central Au + Au Reactions between 100 and 400A MeV NUCLEAR REACTIONS 197Au(197Au, X), E=100, 400 MeV/nucleon; measured fragment charge, kinetic energy distribution; deduced entropy created in the colliding system.
doi: 10.1103/PhysRevC.52.346
1995KO18 Phys.Rev. C51, 2686 (1995) R.Kotte, B.Kampfer, J.Mosner, W.Neubert, D.Wohlfarth, J.P.Alard, V.Amouroux, Z.Basrak, N.Bastid, I.M.Belayev, L.Berger, Th.Blaich, S.Boussange, A.Buta, R.Caplar, C.Cerruti, N.Cindro, J.P.Coffin, R.Dona, P.Dupieux, J.Ero, Z.G.Fan, P.Fintz, Z.Fodor, L.Fraysse, R.Freifelder, S.Frolov, A.Gobbi, Y.Grigorian, G.Guillaume, N.Herrmann, K.D.Hildenbrand, S.Holbling, O.Houari, M.Ibnouzahir, S.C.Jeong, F.Jundt, J.Kecskemeti, P.Koncz, Y.Korchagin, M.Kramer, C.Kuhn, I.Legrand, A.Lebedev, V.Manko, T.Matulewicz, G.Mgebrishvili, D.Moisa, G.Montarou, I.Montbel, D.Pelte, M.Petrovici, P.Pras, F.Rami, V.Ramillien, W.Reisdorf, A.Sadchikov, D.Schull, Z.Seres, B.Sikora, V.Simion, S.Smolyankin, U.Sodan, K.Teh, R.Tezkratt, M.Trzaska, M.A.Vasiliev, P.Wagner, J.P.Wessels, T.Wienold, Z.Wilhelmi, A.V.Zhilin, and the FOPI Collaboration Interplay of Collective Flow Phenomena and Velocity Correlations of Intermediate-Mass Fragments in Collisions of Au + Au at E = (100-400)A MeV NUCLEAR REACTIONS 197Au(197Au, X), E=100-400 MeV/nucleon; measured intermediate mass fragments velocity correlations; deduced nuclear matter sideward flow role, source radii.
doi: 10.1103/PhysRevC.51.2686
1995PE14 Phys.Rev.Lett. 74, 5001 (1995) M.Petrovici, N.Herrmann, I.Legrand, A.Gobbi, K.D.Hildenbrand, W.Reisdorf, A.Buta, R.Freifelder, S.C.Jeong, M.Kramer, D.Moisa, D.Schull, V.Simion, U.Sodan, K.Teh, J.P.Wessels, T.Wienold, J.P.Alard, V.Amouroux, Z.Basrak, N.Bastid, I.M.Belyaev, L.Berger, Th.Blaich, S.Boussange, R.Caplar, C.Cerruti, N.Cindro, J.P.Coffin, R.Dona, P.Dupieux, J.Ero, P.Fintz, Z.Fodor, L.Fraysse, G.Guillaume, S.Holbling, A.Houari, F.Jundt, J.Kecskemeti, P.Koncz, Y.Korchagin, R.Kotte, C.Kuhn, M.Ibnouzahir, A.Lebedev, C.Maguire, V.Manko, J.Mosner, G.Montarou, I.Montbel, P.Morel, W.Neubert, D.Pelte, F.Rami, V.Ramillien, A.Sadchikov, Z.Seres, B.Sikora, S.Smolyankin, R.Tezkratt, M.Trzaska, M.A.Vasiliev, P.Wagner, Z.Wilhelmi, D.Wohlfarth, A.V.Zhilin, and the FOPI Collaboration Cluster Formation During Expansion of Hot and Compressed Nuclear Matter Produced in Central Collisions of Au on Au at 250A MeV NUCLEAR REACTIONS 197Au(197Au, X), E=250 MeV/nucleon; measured fragment yield distribution; deduced hot, compressed transient state expansion, clustering features. Model comparison.
doi: 10.1103/PhysRevLett.74.5001
1994JE08 Phys.Rev.Lett. 72, 3468 (1994) S.C.Jeong, N.Herrmann, Z.F.Fan, R.Freifelder, A.Gobbi, K.D.Hildenbrand, M.Kramer, J.Randrup, W.Reisdorf, D.Schull, U.Sodan, K.Teh, J.P.Wessels, D.Pelte, M.Trzaska, T.Wienold, J.P.Alard, V.Amouroux, Z.Basrak, N.Bastid, I.M.Belayev, L.Berger, M.Bini, Th.Blaich, S.Boussange, A.Buta, R.Caplar, C.Cerruti, N.Cindro, J.P.Coffin, R.Dona, P.Dupieux, J.Ero, P.Fintz, Z.Fodor, L.Fraysse, S.Frolov, Y.Grigorian, G.Guillaume, S.Holbling, A.Houari, F.Jundt, J.Kecskemeti, P.Koncz, Y.Korchagin, R.Kotte, C.Kuhn, M.Ibnouzahir, I.Legrand, A.Lebedev, C.Maguire, V.Manko, P.Maurenzig, G.Mgebrishvili, J.Mosner, D.Moisa, G.Montarou, I.Montbel, P.Morel, W.Neubert, A.Olmi, G.Pasquali, M.Petrovici, G.Poggi, F.Rami, V.Ramillien, A.Sadchikov, Z.Seres, B.Sikora, V.Simion, S.Smolyankin, R.Tezkratt, M.A.Vasiliev, P.Wagner, Z.Wilhelmi, D.Wohlfarth, A.V.Zhilin, and the FOPI Collaboration Collective Motion in Selected Central Collisions of Au on Au at 150A MeV NUCLEAR REACTIONS 197Au(197Au, X), E=150 MeV/nucleon; measured fragments kinetic energy spectra; deduced collective energy.
doi: 10.1103/PhysRevLett.72.3468
1993KA19 Phys.Rev. C48, R955 (1993) B.Kampfer, R.Kotte, J.Mosner, W.Neubert, D.Wohlfarth, J.P.Alard, Z.Basrak, N.Bastid, I.M.Belayev, Th.Blaich, A.Buta, R.Caplar, C.Cerruti, N.Cindro, J.P.Coffin, P.Dupieux, J.Ero, Z.G.Fan, P.Fintz, Z.Fodor, R.Freifelder, L.Fraysse, S.Frolov, A.Gobbi, Y.Grigorian, G.Guillaume, N.Herrmann, K.D.Hildenbrand, S.Holbling, A.Houari, S.C.Jeong, M.Jorio, F.Jundt, J.Kecskemeti, P.Koncz, Y.Korchagin, M.Kramer, C.Kuhn, I.Legrand, A.Lebedev, C.Maguire, V.Manko, T.Matulewicz, G.Mgebrishvili, D.Moisa, G.Montarou, I.Montbel, P.Morel, D.Pelte, M.Petrovici, F.Rami, W.Reisdorf, A.Sadchikov, D.Schull, Z.Seres, B.Sikora, V.Simion, S.Smolyankin, U.Sodan, K.Teh, R.Tezkratt, M.Trzaska, M.A.Vasiliev, P.Wagner, J.P.Wessels, T.Wienold, Z.Wilhelmi, A.L.Zhilin Velocity Correlations of Intermediate Mass Fragments Produced in Central Collisions of Au + Au at E = 150A MeV NUCLEAR REACTIONS 197Au(197Au, X), E=150 MeV/nucleon; measured intermediate mass fragment velocity correlations; deduced source features.
doi: 10.1103/PhysRevC.48.R955
1992FR11 Z.Phys. A341, 175 (1992) R.M.Freeman, Z.Basrak, F.Haas, A.Hachem, G.A.Monnehan, M.Youlal The Resonant Behaviour of the Heavy-Ion Reaction 14C + 16O NUCLEAR REACTIONS, ICPND 16O(14C, 12C), (14C, 14C), (14C, 13C), E(cm)=21.05-32.1 MeV; measured σ(E), σ(θ); deduced resonances.
doi: 10.1007/BF01298477
1992FR13 Phys.Rev. C46, 589 (1992) R.M.Freeman, Z.Basrak, F.Haas, A.Hachem, G.A.Monnehan, M.Youlal Resonant and Nonresonant Behavior of the Heavy-Ion Reaction 14C + 12C NUCLEAR REACTIONS 12C(14C, 12C), (14C, 13C), (14C, 14C), (14C, 15N), (14C, 16O), (14C, 17O), (14C, 18O), (14C, 2α), E=42-54 MeV; measured binary channels σ(E, θ). 26Mg deduced resonances, J, π, rotational band moment of inertia.
doi: 10.1103/PhysRevC.46.589
1990AR12 Nucl.Phys. A514, 564 (1990) D.Ardouin, Z.Basrak, P.Schuck, A.Peghaire, F.Saint-Laurent, H.Delagrange, H.Doubre, C.Gregoire, A.Kyanowski, W.Mittig, J.Peter, Y.P.Viyogi, J.Quebert, C.K.Gelbke, W.G.Lynch, M.Maier, J.Pochodzalla, G.Bizard, F.Lefebvres, B.Tamain, B.Remaud, F.Sebille Preequilibrium Particles and Mean-Field Effects from Particle-Particle Correlations in Heavy-Ion Collisions NUCLEAR REACTIONS 197Au, Ti(40Ar, X), E=60 MeV/nucleon; measured (particle)(particle) correlations for X=p, d, α; deduced mean-field, two-body collisions effects. Landau-Vlasov equation analysis.
doi: 10.1016/0375-9474(90)90156-G
1989AB14 J.Phys.(London) G15, 1845 (1989) U.Abbondanno, S.Datta, N.Cindro, Z.Basrak, G.Vannini Potential-Well Approach to the Analysis of 12C + 16O and 16O + 16O Resonances NUCLEAR REACTIONS 16O(16O, 16O), (12C, 12C), E not given; analyzed resonance data; deduced model parameters. Potential well approach.
doi: 10.1088/0954-3899/15/12/010
1989OS05 Phys.Lett. 232B, 46 (1989) A.Ostrowski, W.Tiereth, D.Brandl, Z.Basrak, H.Voit Evidence for a Nuclear forward Glory in 12C + 12C Scattering NUCLEAR REACTIONS 12C(12C, 12C), E(cm)=9.5 MeV; measured sum-of-difference σ(θ); deduced nuclear forward glory existence.
doi: 10.1016/0370-2693(89)90556-X
1988AR04 Z.Phys. A329, 505 (1988) D.Ardouin, Z.Basrak, P.Schuck, A.Peghaire, H.Delagrange, H.Doubre, C.Gregoire, A.Kyanowski, W.Mittig, J.Peter, F.Saint-Laurent, B.Zwieglinski, Y.P.Viyogi, C.K.Gelbke, W.G.Lynch, M.Maier, J.Pochodzalla, J.Quebert, G.Bizard, F.Lefebvres, B.Tamain Evidence for Persisting Mean Field Effects at E/A = 60 MeV from Particle-Particle Correlation Measurements and Theoretical Investigations with the Landau Vlasov Equation NUCLEAR REACTIONS Ti, 197Au(Ar, X), E=60 MeV/nucleon; measured pp(θ); deduced mean field effects role. Landau-Vlasov equation.
1988BA12 Phys.Rev. C37, 1511 (1988) J(π) = 6+ Molecular State below the Barrier of the 12C + 12C System NUCLEAR REACTIONS, MECPD 12C(12C, α), E(cm)=5.2-5.8 MeV; measured σ(θ). 24Mg deduced levels, J, π.
doi: 10.1103/PhysRevC.37.1511
1988FR15 Phys.Rev. C38, 1081 (1988) R.M.Freeman, Z.Basrak, F.Haas, A.Hachem, G.A.Monnehan, A.Morsad, M.Youlal Origin of the 13C + 17O Resonant Structure NUCLEAR REACTIONS 13C(17O, 17O'), E=42.2-46.2 MeV; measured σ(θ, E). Kinematic coincidences.
doi: 10.1103/PhysRevC.38.1081
1987FR11 Fizika(Zagreb) Supplement 1, 13 (1987) R.M.Freeman, F.Haas, G.Monnehan, V.Barci, Z.Basrak, C.Beck, R.Caplar, A.Hachem, A.Morsad, M.Youlal The 12C + 15N Reaction: Example of a coupled-channel resonance NUCLEAR REACTIONS, ICPND 12C(15N, 15N), (15N, 15N'γ), E=51-62 MeV; measured σ(E), γ yield vs E; deduced resonance structure. 15N level deduced resonant role.
1987TI01 Nucl.Phys. A464, 125 (1987) W.Tiereth, Z.Basrak, N.Bischof, B.Nees, E.Nieschler, I.Weitzenfelder, H.Voit Nuclear Glory Scattering in the 16O + 16O Collision NUCLEAR REACTIONS 16O(16O, 16O), E(cm) ≈ 17 MeV; analyzed σ(θ); deduced possible evidence for nuclear glory. Phase shift analysis.
doi: 10.1016/0375-9474(87)90426-X
1985BA34 Nucl.Phys. A441, 150 (1985) A Straightforward Model-Independent Determination of the Complete Scattering Matrix for Reactions Involving Zero-Spin Particles NUCLEAR REACTIONS 12C(12C, α), E(cm)=4.28-4.68 MeV; analyzed σ(θ). Model independent S-matrix determination.
doi: 10.1016/0375-9474(85)90172-1
1985BA43 Phys.Rev. C32, 910 (1985) Z.Basrak, W.Tiereth, N.Bischof, H.Frohlich, B.Nees, E.Nieschler, H.Voit Unambiguous Phase-Shift Analysis of the 12C(12C, α0)20Ne Reaction at Coulomb-Barrier Energies NUCLEAR REACTIONS 12C(12C, α), E=11.38-12.23 MeV; measured σ(θ). 24Mg deduced quasimolecular resonances, Γ, J, π. Differentially pumped C3H8 gas target. Phase shift analysis.
doi: 10.1103/PhysRevC.32.910
1985TI05 Nucl.Phys. A440, 143 (1985) W.Tiereth, Z.Basrak, N.Bischof, H.Frohlich, H.Voit Phase-Shift Analysis of 16O + 16O Elastic Scattering Data NUCLEAR REACTIONS, ICPND 16O(16O, 16O), E(cm)=15.5-17.95 MeV; measured σ(θ); deduced molecular resonances, parameters, reaction σ(E). Phase shift analysis.
doi: 10.1016/0375-9474(85)90046-6
1983TI01 Phys.Rev. C28, 735 (1983) W.Tiereth, Z.Basrak, H.Voit, N.Bischof, R.Caplar, P.Duck, H.Frohlich, B.Nees, E.Nieschler, W.Schuster Intermediate-Structure Resonances in the 16O + 16O Total Reaction Cross Section NUCLEAR REACTIONS 16O(16O, 16O), E(cm)=15.5-18 MeV; measured σ(θ) vs E; deduced reaction σ(E), quasimolecular resonances.
doi: 10.1103/PhysRevC.28.735
1982BA49 Phys.Rev. C26, 1774 (1982) Z.Basrak, R.Caplar, C.Beck, R.M.Freeman, F.Haas Correlation among Intermediate Structures in Binary and Fusion-Evaporation Channels of the 18O + 12C Reaction NUCLEAR REACTIONS, ICPND 12C(18O, X), (18O, 18O'), (18O, 16O)(18O, 17O), (18O, 14C), (18O, 15N), (18O, 13C), (18O, α), (18O, 2α), (18O, 5n), (18O, 5np), (18O, 5n2p), (18O, n2α), E=50-81 MeV; measured Eγ, Iγ; deduced σ(E), channel correlation effects. 30Si deduced structure in fusion evaporation, binary channel.
doi: 10.1103/PhysRevC.26.1774
1981BA26 Nucl.Phys. A363, 242 (1981) Z.Basrak, P.Duck, H.Frohlich, W.Treu, H.Voit On the Observability of 'Molecular Resonances' in 24Mg through the 10B + 14N Entrance Channel NUCLEAR REACTIONS 10B(14N, α) E=28.8-37.2 MeV; measured σ(E, θ). 24Mg deduced no resonances. Enriched target.
doi: 10.1016/0375-9474(81)90464-4
1981BA66 Fizika(Zagreb) 13, Suppl.No.1, 33 (1981) Z.Basrak, C.Beck, R.Caplar, R.M.Freeman, F.Haas Structure in the 12C + 18O Reaction Cross Sections NUCLEAR REACTIONS 12C(18O, γ), (18O, X), (18O, xn), E=50-81 MeV; measured production σ(E) for 17,18O, 13,14C, σ(fusion, E), σ(evaporation) vs E; deduced structure. Activation technique.
1978BA25 Nucl.Phys. A299, 381 (1978) The (t, α) Reaction on 121Sb and 123Sb NUCLEAR REACTIONS 121,123Sb(t, α), E=12 MeV; measured σ(Eα, θ). 120,122Sn deduced levels, L(p), π, S. Enriched targets.
doi: 10.1016/0375-9474(78)90378-0
1977CI01 Phys.Rev.Lett. 39, 1135 (1977) N.Cindro, F.Cocu, J.Uzureau, Z.Basrak, M.Cates, J.M.Fieni, E.Holub, Y.Patin, S.Plattard Evidence for a Rotational Band in 24Mg and its Fragmentation: A Rotation-Vibration Coupling (Question) NUCLEAR REACTIONS 12C(12C, α), E(cm)=6.85-15 MeV; measured σ(Eα, θ). 24Mg deduced resonances, J, π.
doi: 10.1103/PhysRevLett.39.1135
1976BA22 J.Phys.(Paris), Lett. 37, L-131 (1976) Z.Basrak, F.Auger, B.Fernandez, J.Gastebois, N.Cindro Resonant Behaviour in the Interaction of the 12C + 12C System at Energies Above the Coulomb Barrier NUCLEAR REACTIONS 12C(12C, p), (12C, α), E=14-22 MeV; measured σ(E). 24Mg deduced resonances.
doi: 10.1051/jphyslet:01976003706013100
1976BA53 Phys.Lett. 65B, 119 (1976) Z.Basrak, F.Auger, B.Fernandez, J.Gastebois, N.Cindro Spins of Resonances in the 12C + 12C System NUCLEAR REACTIONS 12C(12C, α), (12C, p), E(cm)=7.5-8.85 MeV; measured σ(θ). 24Mg resonances deduced J, π.
doi: 10.1016/0370-2693(76)90008-3
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