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NSR database version of April 11, 2024.

Search: Author = Z.Basrak

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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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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
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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
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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
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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1456.


2004BA56      Nucl.Phys. A738, 463 (2004)

Z.Basrak

Weakened nuclear opacity and binary reactions

doi: 10.1016/j.nuclphysa.2004.04.087
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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
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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)

Z.Basrak, R.Pezer, S.Szilner

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
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2003SZ11      Fizika(Zagreb) B 12, 117 (2003)

S.Szilner, F.Haas, Z.Basrak

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)

S.Szilner, Z.Basrak, F.Haas

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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1535.


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
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2000BA44      Acta Phys.Pol. B31, 361 (2000)

Z.Basrak, Ph.Eudes

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)

Ph.Eudes, Z.Basrak

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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1000.


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
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1999EU01      Nucl.Phys. (Supplement) A654, 769c (1999)

Ph.Eudes, Z.Basrak

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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0999.


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
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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
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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
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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
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1997EU01      Phys.Rev. C56, 2003 (1997)

Ph.Eudes, Z.Basrak, F.Sebille

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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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)

Z.Basrak, W.Tiereth, H.Voit

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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1601.


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
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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
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1985BA34      Nucl.Phys. A441, 150 (1985)

Z.Basrak, F.Auger

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
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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
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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
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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
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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
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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
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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)

Z.Basrak, N.Cindro, M.Turk

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
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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
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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
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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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