NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = E.Betak Found 36 matches. 2014BE13 Nucl.Data Sheets 118, 284 (2014) Cluster Emission for the Pre-equilibrium Exciton Model with Spin Variables NUCLEAR REACTIONS 197Au(p, n), (p, p'), (p, α), (p, γ), E=62 MeV; calculated σ(Eα) using pre-equilibrium exciton model with angular momentum couplings and generalized Iwamoto-Harada model for cluster emission. Compared with data.
doi: 10.1016/j.nds.2014.04.059
2014PR09 Nucl.Data Sheets 120, 291 (2014) B.Pritychenko, E.Betak, B.Singh, J.Totans Nuclear Science References Database
doi: 10.1016/j.nds.2014.07.070
2012UR05 J.Phys.:Conf.Ser. 337, 012021 (2012) M.Urbanec, E.Betak, Z.Stuchlik Macroscopic properties of neutron stars including deformation
doi: 10.1088/1742-6596/337/1/012021
2011LA05 Phys.Rev. C 83, 034315 (2011); Erratum Phys.Rev. C 97, 094901 (2018) A.C.Larsen, M.Guttormsen, M.Krticka, E.Betak, A.Burger, A.Gorgen, H.T.Nyhus, J.Rekstad, A.Schiller, S.Siem, H.K.Toft, G.M.Tveten, A.V.Voinov, K.Wikan Analysis of possible systematic errors in the Oslo method NUCLEAR REACTIONS 50V, 117Sn, 160,164Dy(3He, α), E not given; 50V, 160,162,164Dy(3He, 3He'), E not given; 46Ti(p, p'), E=15-32 MeV; analyzed previous experimental data and simulated data for particle and γ spectra, (particle)γ-coin, γ-ray transmission coefficients and strength functions, level densities. 56,57,58Fe, 96,97,98Mo(3He, 3He'); analyzed first generation matrix, parity distributions. Analysis of systematic errors in Oslo method for the simultaneous extraction of the level density and γ-ray transmission coefficient from (particle)γ-coincidence data.
doi: 10.1103/PhysRevC.83.034315
2011PR03 Nucl.Instrum.Methods Phys.Res. A640, 213 (2011) B.Pritychenko, E.Betak, M.A.Kellett, B.Singh, J.Totans The Nuclear Science References (NSR) database and Web Retrieval System
doi: 10.1016/j.nima.2011.03.018
2005BE75 Radiochim.Acta 93, 311 (2005) E.Betak, R.Mikolajczak, J.Staniszewska, S.Mikolajewski, E.Rurarz Activation cross sections for reactions induced by 14 MeV neutrons on natural tin and enriched 112Sn targets with reference to 111In production via radioisotope generator 112Sn(n, 2n)111Sn → 111In NUCLEAR REACTIONS 112,114,118,124Sn(n, 2n), E=14.4 MeV; 112,114,115,116,117Sn(n, p), E=14.4 MeV; 117Sn(n, n'), (n, np), E=14.4 MeV; 118,120Sn(n, α), E=14.4 MeV; measured σ. Activation technique.
doi: 10.1524/ract.93.6.311.65644
2004BE09 Int.J.Mod.Phys. E13, 63 (2004) Pre-equilibrium cluster emission NUCLEAR REACTIONS 197Au(p, dX), (p, αX), E=62 MeV; calculated deuteron and α spectra, pre-equilibrium effects. Several models compared.
doi: 10.1142/S0218301304001734
2003BE71 Fizika(Zagreb) B 12, 11 (2003) Pre-equilibrium heavy-ion collisions with spin: A toy model
2003BE76 Acta Phys.Hung.N.S. 18, 353 (2003) Iwamoto-Harada-Bisplinghoff Model Generalized NUCLEAR REACTIONS 197Au(p, dX), (p, αX), E=62 MeV; calculated deuteron and α spectra. Generalized Iwamoto-Harada-Bisplinghoff model, comparison with data.
doi: 10.1556/APH.18.2003.2-4.40
2003HO01 Phys.Rep. 374, 1 (2003) Cluster emission, transfer and capture in nuclear reactions
doi: 10.1016/S0370-1573(02)00268-5
2001BE15 Nucl.Phys. A686, 204 (2001) E.Betak, F.Cvelbar, A.Likar, T.Vidmar Model Calculations of the Radiative Capture Process and the Brink-Axel Hypothesis NUCLEAR REACTIONS 140Ce, 208Pb(n, γ), E=4-18 MeV; calculated σ(E), excitation functions. Consistent direct-semidirect and preequilibrium exciton models. Comparisons with data.
doi: 10.1016/S0375-9474(00)00562-5
1999BE40 Acta Phys.Pol. B30, 1511 (1999) Pre-Equilibrium Cluster Emission: Some examples NUCLEAR REACTIONS 92,94,96,98,100Mo(n, α), E=14 MeV; callated reaction σ; 120Sn(p, α), E=62 MeV; calculated σ(Eα). Pre-equilibriumα emission.
1998BE23 Rep.Prog.Phys. 61, 483 (1998) Particle-Hole State Densities in Pre-Equilibrium Nuclear Reaction Models
doi: 10.1088/0034-4885/61/5/002
1998BE61 Acta Phys.Pol. B29, 2285 (1998) Energetic Particles and Gammas from Low-Energy Nuclear Reactions
1995CV01 J.Phys.(London) G21, 377 (1995) Pre-Equilibrium and Direct-Semi-Direct Model Calculations of Nucleon Radiative Capture Excitation Functions on Heavy Nuclei NUCLEAR REACTIONS, ICPND 142Ce, 176Yb, 208Pb, 130Te(p, γ), 89Y, 208Pb, 140Ce(n, γ), E ≈ 4-24 MeV; analyzed σ(E). Preequilibrium, direct-semi-direct models, radiative capture.
doi: 10.1088/0954-3899/21/3/012
1994BA45 Nucl.Phys. A575, 348 (1994) A.Balanda, J.C.S.Bacelar, E.Betak, J.A.Bordewijk, A.Krasznahorkay, H.van der Ploeg, R.H.Siemssen, H.W.Wilschut, A.van der Woude Photons in the Proton-Induced Reaction with In at E(p) = 50 MeV NUCLEAR REACTIONS, ICPND 115In(p, γ), E-50 MeV; measured inclusive γ spectra, γ-yield; deduced hard γ-emission probability per pn-collision. 116Sn deduced GDR parameters. Compound, preequilibrium model analysis.
doi: 10.1016/0375-9474(94)90194-5
1993CV01 J.Phys.(London) G19, 1937 (1993) Pre-Equilibrium and Direct-Semi-Direct Model Calculations of Proton Radiative Capture Excitation Functions Near A = 60 NUCLEAR REACTIONS, ICPND 56Fe, 58,60,61Ni, 59Co, 63Cu, 64Zn(p, γ), E ≤ 24 MeV; calculated σ(E). Preequilibrium, direct-semidirect models, radiative capture.
doi: 10.1088/0954-3899/19/11/020
1992BE26 Phys.Rev. C46, 945 (1992) Another Possible Manifestation of the Energy-Dependent Width of the Giant Dipole Resonance NUCLEAR REACTIONS 130Te, 176Yb(p, γ), E ≈ 5-25 MeV; calculated σ(E). 208Pb, 141Pr(n, γ), 142Ce, 130Te(p, γ), E=3-25 MeV; calculated activation, integrated σ(E) ratio; deduced composite nuclei GDR energy dependent width possible manifestation.
doi: 10.1103/PhysRevC.46.945
1992CI07 Fizika(Zagreb) B1, 51 (1992) N.Cindro, E.Betak, M.Korolija, J.J.Griffin A Microscopic Model for Calculating the Inital Number of Excitons in Nucleus-Nucleus Collisions NUCLEAR REACTIONS 48Ti, 60Ni, 120,124Sn, 197Au, 27Al(16O, X), E=403 MeV; 48Ti, 60Ni, 120,124Sn, 197Au, 27Al(32S, X), E=504, 679 MeV; 48Ti, 60Ni, 120,124Sn, 197Au, 27Al(58Ni, X), E=876 MeV; calculated inital exciton number. Comparison with data.
1991CI05 Phys.Rev.Lett. 66, 868 (1991) N.Cindro, M.Korolija, E.Betak, J.J.Griffin Early Stages of Nucleus-Nucleus Collisions: A microscopic calculation of the initial number of degrees of freedom NUCLEAR REACTIONS 27Al, 46Ti, 60Ni, 120,124Sn, 197Au(16O, X), (32S, X), (58Ni, X), E=403-876 MeV; calculated preequilibrium nucleon emission initial degrees of freedom. Microscopic model.
doi: 10.1103/PhysRevLett.66.868
1991CV01 J.Phys.(London) G17, 113 (1991) Pre-Equilibrium-Equilibrium Model Calculations of Nucleon Radiative Capture Excitation Functions NUCLEAR REACTIONS, ICPND 130Te, 176Yb(p, γ), E ≈ 5-25 MeV; 209Bi(p, γ), E ≈ 10-80 MeV; 142Ce(p, γ), E ≈ 5-50 MeV; 140Ce, 89Y(n, γ), E ≈ 5-20 MeV; calculated σ(E). Preequilibrium-equilibrium exciton model.
doi: 10.1088/0954-3899/17/2/005
1989CV01 Z.Phys. A332, 163 (1989) Exciton Model Comparison of the Activation and the Integrated 14 MeV Neutron Radiative Capture Cross Sections NUCLEAR REACTIONS 27Al, 51V, 45Sc, 55Mn, 127I, 141Pr, 208Pb, 209Bi(n, γ), E=14.1 MeV; calculated σ(E(γ)). Exciton model.
1987BE31 Fizika(Zagreb) 19, Supplement 1, 49 (1987) Gamma-Decay Calculations within the Exciton Model: The case of 64Zn + 68Zn and 20Ne + 112Sn reactions NUCLEAR REACTIONS 68Zn(64Zn, X), E=290 MeV; 112Sn(20Ne, X), E=110 MeV; calculated γ multiplicity. Exciton model.
1987BE49 Rev.Roum.Phys. 32, 589 (1987) Nuclear Molecular Dynamics Approach to the Nucleus-Nucleus Potential NUCLEAR REACTIONS 40Ca(40Ca, 40Ca), E(cm)=5, 10, 20 MeV/nucleon; calculated interaction potentials. Nuclear molecular dynamics.
1985BE45 Izv.Akad.Nauk SSSR, Ser.Fiz. 49, 1023 (1985); Bull.Acad.Sci.USSR, Phys.Ser. 49, No.5, 176 (1985) E.Betak, I.Breznik, S.Hlavac, P.Oblozhinsky Study of Neutrons Emitted in Coincidence with γ-Quanta in Reactions with 14-MeV Neutrons. NUCLEAR REACTIONS 52Cr, 56Fe, 58Ni(n, xnyp), E=14.6 MeV; measured neutron spectra. 56Fe, 58Ni, 58Co deduced Γγ/Γ. Exciton model.
1984BE43 Czech.J.Phys. B34, 850 (1984) Light Particles in Low-Energy Heavy-Ion Reactions NUCLEAR REACTIONS 197Au(22Ne, xα), E=178 MeV; calculated σ(θα, Eα); deduced different mechanism contributions. Preequilibrium, direct, deep inelastic processes.
1983BE02 J.Phys.(London) G9, L47 (1983) Very Light Fragments from Deep-Inelastic Collisions NUCLEAR REACTIONS 232Th(22Ne, X), E=175 MeV; calculated fragment yield vs Z, σ(fragment θ, E) for 10B, 15C, 16O, 20F fragments. Master equation, full, reduced shell effects.
doi: 10.1088/0305-4616/9/2/004
1983BE46 Phys.Lett. 130B, 350 (1983) Exclusive (α, 2nγ) Neutron Spectra and the Pre-Equilibrium Exciton Model NUCLEAR REACTIONS 108Pd, 150Nd(α, 2nγ), E=32 MeV; 112,124Sn(α, 2nγ), E=35 MeV; analyzed exclusive neutron spectra. Preequilibrium exciton model.
doi: 10.1016/0370-2693(83)91519-8
1983BE57 Yad.Fiz. 38, 1179 (1983) Analysis of α-Particle Emission Mechansims in Heavy-Ion Reactions NUCLEAR REACTIONS 197Au(22Ne, α), E=178 MeV; calculated σ(θ, Eα); deduced reaction mechanism.
1983DO04 Z.Phys. A310, 329 (1983) Two-Component Exciton Model NUCLEAR REACTIONS 54Fe(p, p'), (p, n), E=29, 39, 62 MeV; 209Bi(p, p'), E=39, 62 MeV; 48Ca(p, n), E=25, 35, 45 MeV; 208Pb(p, n), E=35, 45 MeV; 103Rh(p, p'), (p, n), E=18 MeV; calculated particle spectra. Two-component exciton model.
doi: 10.1007/BF01419519
1982RE02 J.Phys.(London) G8, 257 (1982) R.Reif, B.Weissbach, E.Betak, Ch.Stoyanov, A.I.Vdovin Direct Inelastic Proton Scattering from Odd-A Nuclei within the Semimicroscopic Quasiparticle-Phonon Model NUCLEAR REACTIONS 88Sr(p, p'), E=20.2 MeV; 89Y(p, p'), E=24.5 MeV; calculated σ(θ). 88Sr, 89Y levels deduced configuration. Semi-microscopic, quasiparticle-phonon model, DWBA, CCBA analyses.
doi: 10.1088/0305-4616/8/2/012
1979BE24 Phys.Lett. 84B, 368 (1979) Gamma Emission in the Pre-Equilibrium Exciton Model NUCLEAR REACTIONS 93Nb, 137La(n, γ), E=14.1 MeV; calculated σ(Eγ). Pre-equilibrium exciton model.
doi: 10.1016/0370-2693(79)91217-6
1976BE36 Acta Phys.Slovaca 26, 21 (1976) Complex Particle Emission in the Exciton Model of Nuclear Reactions NUCLEAR REACTIONS 197Au, 120Sn(p, p), (p, d), (p, t), (p, 3He), (p, α), E=61.5 MeV; 197Au(p, α), (p, d), (p, t), E=28.8 MeV; 93Nb, 163Dy, 197Au(n, α), E ≈ 20 MeV; calculated σ, forming probability of complex particles.
1976BE57 Z.Phys. A279, 319 (1976) The Finite Depth of the Nuclear Potential Well in the Exciton Model of Preequilibrium Decay NUCLEAR REACTIONS 120Sn(p, p), (p, d), E=10-50 MeV; calculated σ(E).
1975BE57 Acta Phys.Slovaca 25, 264 (1975) Analysis of the 41K(α, n) Reaction in the Pre-Equilibrium Model of Nuclear Reactions NUCLEAR REACTIONS 41K(α, n), E=8-40 MeV; calculated σ(E, En). Exciton model.
1973RI16 Nucl.Phys. A205, 545 (1973) I.Ribansky, P.Oblozinsky, E.Betak Pre-equilibrium decay and the exciton model NUCLEAR REACTIONS 197Au(α, n), E<38 MeV; calculated σ. Pre-equilibrium decay, Griffin exciton model calculations, comparison with available data.
doi: 10.1016/0375-9474(73)90705-7
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