NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = M.Avrigeanu Found 81 matches. 2023AV03 Phys.Rev. C 107, 034613 (2023) Consistent optical potential for incident and emitted low-energy α particles. III. Nonstatistical processes induced by neutrons on Zr, Nb, and Mo nuclei NUCLEAR REACTIONS 93Nb, 92,94,95,96,97,98,100Mo(n, X), E<12 MeV; calculated total σ(E), s- and p-wave neutron strength functions, potential scattering radius. 92Zr(p, γ), E=2-5 MeV; 92Zr(p, n), E=3-7 MeV; 94Zr(p, n), E=2-7 MeV; 96Zr(p, n), E=2-10 MeV; 93Nb(p, n), 93Nb(p, γ), E=1-MeV; calculated σ(E). 90,91,92Zr(α, γ), E=9-12 MeV; calculated σ, γ-strength functions. 88Sr(3He, α), E=36 MeV; 90,96Zr(3He, α), E=39 MeV; calculated σ(θ). 96Zr(α, n), E=6-15 MeV; 100Mo(α, xn)102Ru/103Ru, E=7.5-15 MeV; calculated σ(E). 93Nb(n, γ), E=0.0003-1.2 MeV; 93Nb(n, 2n), E=8-24 MeV; 93Nb(n, xp)92Zr/93Zr, E=5-24 MeV; calculated σ(E). 92Mo(n, p), E=4-21 MeV; 92Mo(n, 2n), E=13-22MeV; 90,92,94,96Zr(n, α), E=6-22 MeV; 93Nb(n, α), E=4-22 MeV; 92,95,98,100Mo(α, n), E=5-21 MeV; calculated σ(E) for ground and isomeric state excitation. 90Zr, 93Nb, 92Mo(n, α), (n, nα), E=14.5-14.8 MeV; calculated σ(E). Statistical calculations with Hauser-Feshbach and preequilibrium emission models combined with direct reaction DWBA analysis using FRESCO code. Increase of the α emission beyond the compound nuclei+preequlibrium emission predictions was obtained through consideration of additional Giant Quadrupole Resonance-like decay of excited nuclei. Detailed comparison with experimental data, with TALYS-1.8 calculations and evaluated data library TENDL-2021.
doi: 10.1103/PhysRevC.107.034613
2022AV01 Eur.Phys.J. A 58, 3 (2022) M.Avrigeanu, D.Rochman, A.J.Koning, U.Fischer, D.Leichtle, C.Costache, V.Avrigeanu Advanced breakup-nucleon enhancement of deuteron-induced reaction cross sections NUCLEAR REACTIONS 58Ni, 96Zr, 231Pa(d, X), (d, 2n), (d, 2p), E<200 MeV; calculated σ using TALYS-1.95 nuclear model code. Comparison with available data.
doi: 10.1140/epja/s10050-021-00659-6
2022AV02 Phys.Rev. C 106, 024615 (2022) Charged-particle optical potentials tested by first direct measurement of the 59Cu(p, α)56Ni reaction NUCLEAR REACTIONS 59Cu(p, α), E<6.6 MeV; calculated σ(E). Comparison to the evaluated TENDL data and recent experimental results. Hauser-Feshbach based statistical model TALYS-1.95 calculations. Reached agreement with experimental data by consideration of proton optical–model potential (OMP) anomalies at sub-Coulomb energies for medium–weight nuclei.
doi: 10.1103/PhysRevC.106.024615
2022AV03 Eur.Phys.J. A 58, 189 (2022) Validation of an optical potential for incident and emitted low-energy α-particles in the A ≈ 60 mass range NUCLEAR REACTIONS 58,60,61,62,64Ni, 59Co(n, X), (n, p), (n, 2n), (n, α), E<60 MeV; analyzed available data; deduced optical model parameters.
doi: 10.1140/epja/s10050-022-00831-6
2021AV01 Eur.Phys.J. A 57, 54 (2021) Validation of an optical potential for incident and emitted low-energy α-particles in the A ∼ 60 mass range NUCLEAR STRUCTURE 50,51,52,53,54,55,56Cr, 52,53,54,55,56,57,58Mn, 52,53,54,55,56,57,58,59,60,61Fe, 55,56,57,58,59,60,61,62,63Co, 58,59,60,61,62,63,64,65,66Ni, 61,62,63,64,65,66,67Cu, 62,63,64,65,66,67,68Zn; analyzed available data; deduced nuclear level densities, consistent set of statistical-model input parameters.
doi: 10.1140/epja/s10050-020-00336-0
2021SI31 Phys.Rev. C 104, 044615 (2021) E.Simeckova, M.Avrigeanu, J.Mrazek, J.Novak, M.Stefanik, C.Costache, V.Avrigeanu Deuteron-induced reactions on natZr up to 60 MeV NUCLEAR REACTIONS Zr(d, xn), (d, p), (d, xnp), (d, xn2p), 90Nb/91mNb/92mNb/94mNb/95Nb/95mNb/96Nb/97Nb/89Zr/89mZr/95Zr/97Zr/87Y/87mY/88Y/90mY/91mY/94Y, E=4.32-19.80 MeV from U-120M cyclotron of CANAM-NPI-CAS; measured Eγ, Iγ, activation σ(E) by stacked-foil technique and off-line γ-ray spectroscopy using two HPGe detectors, natural Zr target. 90Zr(d, d), E=5.5, 9, 10, 11, 12, 13, 15, 23.2, 28.8, 56 MeV; 90,91,92,94,96Zr(d, d), E=34.4 MeV; analyzed available experimental σ(θ, E) data using global optical model potential (OMP), and used to analyze literature particle-transfer σ(θ) data for excited states in residual nuclei. 90Zr(d, p), E=15.89 MeV; 91,92Zr(d, p), E=12 MeV; 92,96Zr(d, p), E=33.3 MeV; 94Zr(d, p), E not given; 90Zr(d, n), E=12 MeV; 90Zr(d, α), E=17 MeV; 94,96Zr(d, α), E=11.5, 28 MeV; 90Zr(d, t), E=21.14 MeV; 91,92,94,96Zr(d, t), E=11.8 MeV; 91Zr(3He, d), E=17 MeV; Zr(d, xn)91,95Nb, 94Zr(d, n), 96Zr(d, 3n), E=10-60 MeV; Zr(d, xnp)88Zr, E=20-60 MeV; Zr(d, x)86Y/87Y/87mY/88Y/90mY, E=5-60 MeV; 94Zr(d, xnp)88Zr, E=20-60 MeV; 94Zr(d, xn2p)86Y, E=20-60 MeV; analyzed literature experimental σ(θ) and σ(E) data using pre-equilibrium emission (PE) and compound nucleus (CN) decay statistical emission mechanisms, with the inclusion of deuteron breakup (BU). Comparison of activation cross section data with TENDL-2019 evaluation and model calculations. For particle transfer reactions data taken from literature, level energies, J, π and spectroscopic factors are given in the Supplemental Material.
doi: 10.1103/PhysRevC.104.044615
2020AV01 Phys.Rev. C 101, 024605 (2020) M.Avrigeanu, E.Simeckova, U.Fischer, J.Mrazek, J.Novak, M.Stefanik, C.Costache, V.Avrigeanu Deuteron-induced reactions on manganese at low energies NUCLEAR REACTIONS 55Mn(d, p), (d, t), (d, 2nα), E=3.13-19.49 MeV; measured Eγ, Iγ, σ(E), by activation method at the variable-energy cyclotron U-120M facility of NPI-CAS, Rez. 55Mn(d, p), (d, t), (d, 2nt), (d, 2nα), E<50 MeV; analyzed present and previous data for σ(E). 55Mn(d, p)56Mn, E=7.5 MeV; 55Mn(d, t)54Mn, E=17, 18 MeV; analyzed previous differential σ(θ) data for 20 levels in 56Mn up to 4.54 MeV, and for 25 levels in 54Mn up to 3.42 MeV. Comparison with TALYS-1.9 theoretical calculations. Discussed deuteron breakup (BU) and direct reaction (DR) mechanisms.
doi: 10.1103/PhysRevC.101.024605
2019AV01 Phys.Rev. C 99, 044613 (2019) Role of consistent parameter sets in an assessment of the α-particle optical potential below the Coulomb barrier NUCLEAR STRUCTURE 67Ga, 67,68Ge, 112Sn, 117,119Sb, 124,125,126,127I, 195,198Au; deduced BSFG level-density parameter, and average s-wave radiation widths Γγ corresponding to the SLO, GLO, and EGLO models from fitting of low-lying levels used in shell-model calculations. 61,62,63,64,65Cu, 64,66Zn, 69Ga, 76Ge; comparison of measured dipole γ-ray strength functions with the sum of calculated γ-ray strength functions using the SLO model for M1 radiations, and SLO, GLO and EGLO models for E1-radiation. NUCLEAR REACTIONS 64Zn(α, p)67Ga, E=6-16 MeV; 64Zn(α, n)67Ge, E=10-16 MeV; 108Cd(α, γ)112Sn, 108Cd(α, n)111Sn, E=9.8-13.6 MeV; 113In(α, γ)117Sb, 113In(α, n)116Sb/116mSb, E=9.4-14.2 MeV; 115In(α, γ)119Sb, 115In(α, n)118Sb/118mSb, E=9.4-16.4 MeV; 121Sb(α, γ)125I, E=9.9-14.1 MeV; 121Sb(α, n)124I, E=10-16.6; 123Sb(α, n)126I, E=11.8-16.6 MeV; 191,193Ir(α, n)194Au/196Au, E=13.6-17 MeV; 197Au(n, γ)198Au, E=0.005-8 MeV; calculated σ(E) for α-induced reactions using the electric-dipole RSF models SLO, GLO, EGLO models along with the SLO model for M1 radiation, as well as EGLO and the M1-radiation upbend with the proton Optical model potential (OMP), and compared with the measured values, and with the data in evaluated TENDL-2017 library; deduced uncertainties and/or systematic errors of an α-particle OMP, and that α-particle optical potential is valid at incident energies below the Coulomb barrier using statistical-model parameters.
doi: 10.1103/PhysRevC.99.044613
2019KR03 Phys.Rev. C 99, 034611 (2019) A.Kreisel, L.Weissman, A.Cohen, T.Hirsh, A.Shor, O.Aviv, I.Eliyahu, M.Avrigeanu, V.Avrigeanu Measurements of 59Co(d, p)60m, gCo, 51V(d, p)52V and natV(d, xn)51Cr cross sections in the 2.7-5.4- MeV energy range NUCLEAR REACTIONS 59Co(d, p)60Co/60mCo, E=3.4, 3.8, 4.3, 4.8, 5.4 MeV; 51V(d, p), E=2.7, 3.0, 3.4, 3.8, 4.3, 4.8, 5.4 MeV; 50V(d, n), (d, 2n), E=3.0, 3.4, 3.8, 4.3, 4.8, 5.4 MeV; measured Eγ, Iγ, and σ(E) by activation method at Soreq Applied Research Accelerator Facility (SARAF); deduced total breakup, direct stripping, and total direct interaction excitation functions. 50V(d, d), (d, p), E=7.5 MeV; 59Co(d, d), (d, p), E=6.5 MeV; 51V(d, p), E=1.5-7 MeV; V(d, xn), E=2.7-7.5 MeV; 59Co(d, p), E=2-17 MeV; 59Co(d, 2p), E=2-17 MeV; analyzed previous and present σ(E) σ(E, θ) data using the structure data from the ENSDF database, and theoretical calculations using the optical model, and processes of pre-equilibrium emission (PE) and evaporation from the compound nucleus (CN) using the STAPRE-H code.
doi: 10.1103/PhysRevC.99.034611
2018MA39 Eur.Phys.J. A 54, 91 (2018) I.Mardor, O.Aviv, M.Avrigeanu, D.Berkovits, A.Dahan, T.Dickel, I.Eliyahu, M.Gai, I.Gavish-Segev, S.Halfon, M.Hass, T.Hirsh, B.Kaiser, D.Kijel, A.Kreisel, Y.Mishnayot, I.Mukul, B.Ohayon, M.Paul, A.Perry, H.Rahangdale, J.Rodnizki, G.Ron, R.Sasson-Zukran, A.Shor, I.Silverman, M.Tessler, S.Vaintraub, L.Weissman The Soreq Applied Research Accelerator Facility (SARAF): Overview, research programs and future plans
doi: 10.1140/epja/i2018-12526-2
2018SI23 Phys.Rev. C 98, 034606 (2018) E.Simeckova, M.Avrigeanu, U.Fischer, J.Mrazek, J.Novak, M.Stefanik, C.Costache, V.Avrigeanu Consistent account of deuteron-induced reactions on natCr up to 60 MeV NUCLEAR REACTIONS Cr(d, xn)54Mn/52Mn/52mMn/51Mn, E=4-20 MeV; Cr(d, X)51Cr/48V, E=4-20 MeV; measured Eγ, Iγ from radioactive reaction product, σ(E) by activation method using the variable-energy cyclotron U-120M at CANAM-NPI-CAS at Rez, Czech Republic. 50,52,53,54Cr(d, d), (d, xn), (d, X), E=3-60 MeV; 50Cr(d, p)51Cr, E=12 MeV; 52Cr(d, p)53Cr, E=7.5 MeV; 52Cr(d, α)50V, E=17 MeV; 53Cr(d, t)52Cr, E=11.8 MeV; 54Cr(d, p)55Cr, E=10 MeV; 54Cr(d, t)53Cr, E=11.8, 12 MeV; analyzed data from literature for elastic scattering differential σ(θ, E), and total reaction σ(θ, E) for direct reaction (DR), and break-up (BU) reaction channels. Comparison with theoretical predictions, and TENDL-2017 evaluations.
doi: 10.1103/PhysRevC.98.034606
2017AV01 Phys.Rev. C 95, 024607 (2017) Additive empirical parametrization and microscopic study of deuteron breakup NUCLEAR REACTIONS 12C, 27Al, 54,56,57,58Fe, 58,60,61,62,64Ni, 63,65Cu, 90Zr, 93Nb, 119Sn, 209Bi, 238U(d, X), E<80 MeV; analyzed and compared experimental deuteron breakup (BU) process with the results of microscopic description for targets from 12C to 209Bi at E(d) of 56 MeV; deduced mass dependencies of the elastic breakup (EB) cross sections.
doi: 10.1103/PhysRevC.95.024607
2017AV04 Phys.Rev. C 96, 044610 (2017) Consistent optical potential for incident and emitted low-energy α particles. II. α emission in fast-neutron-induced reactions on Zr isotopes NUCLEAR REACTIONS 88Sr, 89Y(p, n), E=3-11 MeV; calculated σ(E) and compared with experimental values. 88Sr, 89Y(p, γ), E=1-6 MeV; 70,74Ge, 90,91,92Zr(α, γ), E=6-12 MeV; 89Y, 90,91,92,94,96Zr(n, γ), E=0.001-3 MeV; 90,91,92,94,96Zr(n, p), (n, d), E=5-22 MeV; 90,96Zr(n, 2n), E=5-22 MeV; 90,92,94,96Zr(n, α), E=7-22 MeV; 91Zr(n, nα), E=15-22 MeV; calculated σ(E) and γ-strength functions of E1 and M1 radiations for (p, γ) and (α, γ) reactions using several models: former Lorentzian (SLO), generalized Lorentzian (GLO), enhanced generalized Lorentzian (EGLO), EGLO+SR (small resonance). Statistical model (SM) Hauser-Feshbach (HF) and pre-equilibrium emission (PE) geometry dependent hybrid (GDH) model calculations using STAPRE-H95 code, and the optical-model (OM) code SCAT2. Direct interaction (DI) distorted-wave Born approximation (DWBA) method using DWUCK4 code for the calculation of collective inelastic scattering cross sections. Detailed comparison with experimental data, and also with calculations using TALYS-1.8 code, and evaluated data library TENDL-2015.
doi: 10.1103/PhysRevC.96.044610
2016AV03 Phys.Rev. C 94, 014606 (2016) M.Avrigeanu, E.Simeckova, U.Fischer, J.Mrazek, J.Novak, M.Stefanik, C.Costache, V.Avrigeanu Deuteron-induced reactions on Ni isotopes up to 60 MeV NUCLEAR REACTIONS Ni(d, X)55Co/56Co/57Co/58Co/58mCo/60Co/57Ni/65Ni/60Cu/61Cu/64Cu, E=1.5-19.59 MeV; measured Eγ, Iγ, σ(E) using stacked-foil technique and γ-activation method at U-120M cyclotron of CANAM, NPI CAS. Optical model analysis. Deuteron breakup and direct reactions. Comparison with previous experimental data. 58,64Ni(d, d), E=12-56 MeV; 60Ni(d, d), E=4.86-56 MeV; 61Ni(d, d), E=12.3 MeV; 62Ni(d, d), E=12, 22 MeV; 58Ni(d, p)59Ni, E=10 MeV; 58Ni(d, n)59Cu, E=7 MeV; 58Ni(d, t)57Ni, E=24 MeV; 58Ni(d, α)56Co, E=17 MeV; 58Ni(d, n)59Cu, E=10 MeV; 60Ni(d, p)61Ni, E=7.5 MeV; 61Ni(d, p)62Ni, E=12.3 MeV; 62Ni(d, p)63Ni, E=7.5 MeV; 64Ni(d, p)65Ni, E=7.5 MeV; analyzed σ(θ, E) data. 58,60,61,62,64Ni(d, X), 60Ni(d, n)61Cu, 60Ni(d, 2n)60Cu, 61Ni(d, 2n)61Cu, 61Ni(d, 3n)60Cu, Ni(d, X)61Cu, 62Ni(d, 3n)61Cu, Ni(d, X)60Cu, 60Ni(d, 4n)60Cu, 64Ni(d, 5n)61Cu, Ni(d, X)64Cu, 64Ni(d, 2n)64Cu, Ni(d, X)57Ni, 58Ni(d, t)57Ni, Ni, 58Ni(d, X)56Ni, Ni, 62,64Ni(d, X)61Co, 61Ni(d, 2p)61Co, Ni, 61,62Ni(d, X)60Co, 60Ni(d, 2p)60Co, Ni, 60,61,62,64Ni(d, X)58Co/58mCo, 58Ni(d, 2p)58Co/58mCo, Ni, 58,60,61Ni(d, X)57Co, Ni, 58,60Ni(d, X)56Co, Ni, 58,60Ni(d, X)55Co, Ni, 58,60,61Ni(d, X)56Mn, Ni, 58,60,61Ni(d, X)54Mn, Ni, 58,60,61Ni(d, X)51Cr, 58Ni(d, X)51Mn, Ni, 58,60,61Ni(d, X)52Mn, E=5-65 MeV; Ni(d, X)65Ni, 64Ni(d, p), E=2-30 MeV; analyzed activation σ(E) data by consideration of the pre-equilibrium (PE) and compound nucleus (CN) contributions corrected for decrease of the total-reaction cross section from the leakage of the initial deuteron flux due to the deuteron breakup (BU) and direct reaction (DR) processes. Comparison with TENDL-2015 evaluation, and model calculations.
doi: 10.1103/PhysRevC.94.014606
2016AV04 Phys.Rev. C 94, 024621 (2016) Analysis of uncertainties in α-particle optical-potential assessment below the Coulomb barrier NUCLEAR REACTIONS 63,65Cu(p, n), E=1-8 MeV; 63,65Cu(p, n), E=1-4.5 MeV; calculated reaction σ(E) using proton OMP parameters, and compared with measured values. 61,62,63,64,65Cu, 64,66,68Zn, 69Ga, 76Ge, 105,106,111,112Cd, 116,117,118,119,121,122Sn; calculated E1 and M1 γ-ray strength functions using SLO, GLO, and EGLO models for E1, and SLO model for M1, compared with experimental data from (α, X) reactions. 58Ni(α, p), (α, n), (α, γ), E=4-11.5 MeV; 62Ni(α, p), (α, n), (α, γ), E=4.5-9 MeV; 64Ni(α, n), (α, γ), E=4-9 MeV; 60,61Ni(α, γ), E=5-7.5 MeV; 107Ag(α, n), (α, γ), E=8-13 MeV; 106Ag(α, p), (α, n), (α, γ), E=7.5-13 MeV; 112Sn(α, p), (α, γ), E=7.5-12.5 MeV; 164,166Er, 187Re(α, n), E=13-17 MeV; analyzed σ(E) data using the α-particle global OMPs. Relevance to statistical model calculations. Comparison with experimental data.
doi: 10.1103/PhysRevC.94.024621
2015AV03 Phys.Rev. C 91, 064611 (2015) Consistent optical potential for incident and emitted low-energy α particles NUCLEAR REACTIONS 64Zn(α, p), (α, n), (α, γ), E=6-13.5 MeV; 64,68,70Zn(p, α), E=3-22 MeV; calculated σ(E) using the α-particle global OMPs. Ga(n, X), E=0.1-20 MeV; 70Ge(n, X), E=0.1-5 MeV; calculated total σ(E) using local 69Ga or global OMP parameter sets of Koning and Delaroche, and energy-dependent geometry parameters. 66,67,68,70Zn(p, n), E=2-11 MeV; calculated σ(E) using global OMP or finally adopted parameters. 61,62,63,64,65Cu, 64,66Zn, 65,69Ga, 68Ge(γ, γ'), E<12 MeV; calculated B(E1), B(M1) γ-ray strength functions using former Lorentzian (SLO), generalized Lorentzian (GLO) and enhanced generalized Lorentzian (EGLO) models for E1, and SLO model for M1 radiation. 64,66,68Zn(p, γ), E=1-8 MeV; calculated σ(E) using the proton OMPs and EGLO-model radiative strength functions (RSFs). Pre-equilibrium emission (PE) and compound-nucleus (CN) model calculations using a consistent set of nucleon and γ-ray transmission coefficients, and back-shifted Fermi gas (BSFG) nuclear level densities. Comparison with experimental data, and with predictions of TALYS calculations.
doi: 10.1103/PhysRevC.91.064611
2015AV04 Phys.Rev. C 92, 021601 (2015) Role of breakup and direct processes in deuteron-induced reactions at low energies NUCLEAR REACTIONS 27Al, 56Fe, 63,65Cu, 89Y(d, X), E=4-8 MeV; analyzed compound-nucleus (CN) fractions of reaction σ(E) from measured neutron angular distributions, and unitary and consistent breakup (BU) and direct reactions (DR). Statistical model of nuclear reactions. Comparison with available data for 27Al, 54,56,57,58Fe, 63,65Cu, 93Nb, natural Fe and Cu, targets.
doi: 10.1103/PhysRevC.92.021601
2014AV01 Phys.Rev. C 89, 044613 (2014) M.Avrigeanu, V.Avrigeanu, P.Bem, U.Fischer, M.Honusek, K.Katovsky, C.Manailescu, J.Mrazek, E.Simeckova, L.Zavorka Low energy deuteron-induced reactions on Fe isotopes NUCLEAR REACTIONS 54Fe(d, n)55Co, 54Fe(d, α)52Mn/52mMn, 58Fe(d, p)59Fe, Fe(d, X)51Cr/54Mn/56Mn/56Co/57Co/58Co, E=4.11-19.74 MeV; measured reaction σ(E); comparison with theoretical calculations by FRESCO and TALYS-1.4 optical model codes, with TENDL-2013 library, and with previous experimental results. 54,56,58Fe(d, d), E=5-60 MeV; comparison of previously measured elastic σ(E) with theoretical calculations using various optical potentials. 27Al, 54,56,57Fe, 58,62Ni, 90Zr, 93Nb, 119Sn, 181Ta, 208Pb, 232Th(d, X), E=5-60 MeV; comparison of previously measured total reaction σ(E) and the total proton-emission breakup σ(E) with theory. 54Fe(d, p), E=14 MeV; comparison of previously measured and theoretical σ(θ) distributions for 14 levels in 55Fe. 54,56,58Fe(d, p), 54,56,57Fe(d, n), 56,57,58Fe(d, 2n), (d, 3n), 57,58Fe(d, 4n), 58Fe(d, 5n), 54Fe(d, α), 54,56,57,58Fe, Fe(d, X), (d, xn)51Cr/52Mn/52mMn/54Mn/56Mn/55Co/56Co/57Co/58Co/58mCo/53Fe/55Fe/59Fe, E=5-60 MeV; calculated total reaction, breakup and transfer σ(E). Comparison of theoretical calculations with present and previous measurements, and with TENDL-2013 library.
doi: 10.1103/PhysRevC.89.044613
2014AV02 Nucl.Data Sheets 118, 262 (2014) Consistent Treatment of (α, x) Reaction Cross Sections and α-particle Emission Particularly in Fast-neutron Induced Reactions NUCLEAR REACTIONS 91Zr(α, γ), E=9.2-11.6 MeV;92Mo(n, α), E=5-20 MeV;95Mo(n, α), E=0.001-2 MeV;120Te(α, n), 127I(α, n), (α, γ), E=9.5-16 MeV;130Ba(α, γ), E=12-17 MeV;132Ba(α, n), E=12-17 MeV;141Pr(α, n), E=11-15.5 MeV;144Sm(α, γ), E=10.3-15.5 MeV;169Tm(α, γ), E=12-18 MeV;169Tm(α, n), E=11-20 MeV; calculated σ using optical model; deduced optical model parameters, influence of parameters on σ. Compared with available data.
doi: 10.1016/j.nds.2014.04.053
2014AV03 Nucl.Data Sheets 118, 301 (2014) Consistent Analysis of the Nuclear Reaction Mechanisms Involved in Deuteron-induced Activation at Low and Medium Energies NUCLEAR REACTIONS 54,56,57Fe, Fe(d, x), (d, xn), (d, p), E=threshold-60 MeV;54Fe(d, t), E=threshold-30 MeV; calculated total σ. Compared with available data and TENDL. 54,56,57,58Fe(d, x), E=threshold-60 MeV; calculated total σ, breakup, stripping, pick-up σ. 54Fe(d, p), E=14 MeV; calculated σ(θ) to discrete states; compared to data. TALYS-1.4 code.
doi: 10.1016/j.nds.2014.04.064
2014AV06 Phys.Rev. C 90, 044612 (2014) V.Avrigeanu, M.Avrigeanu, C.Manailescu Further explorations of the α-particle optical model potential at low energies for the mass range A ≈ 45-209 NUCLEAR REACTIONS 148,149Sm, 156,157,158Gd, 160,161,162,163,164Dy, 166,167Er, 170,171,172Yb(α, γ), E below Coulomb barrier; calculated electric-dipole γ-ray strength function using the former Lorentzian (SLO), generalized Lorentzian (GLO) and enhanced generalized Lorentzian (EGLO) models. 113In, 120Te, 127I, 130Ba, 141Pr, 151Eu, 165Ho, 162,166Er, 169Tm, 168Yb(α, n), E=10-16 MeV; 113In, 127I, 130Ba, 144Sm, 162Er, 169Tm, 168Yb(α, γ), E=9-17 MeV; 174,176,177,178,179,180Hf, Hf(n, X), E=0.001-1 MeV; 45Sc, 58Ni, 112Sn, 141Pr, 169Tm, 197Au(α, X), E<50 MeV; calculated reaction σ(E). 50Ti, 51V, 50,52,53Cr, 56,58Fe, 59Co, 58,60,62,64Ni, 63Cu, 70,72,74,76Ge, 76,78,80Se, 89Y, 90,91,92Zr, 94Mo, 107Ag, 112,116,122,124Sn, 132,134,136,138Ba, 140Ce, 144Sm, 182,184,186W, 192Os, 197Au, 208Pb, 209Bi(α, α), E=15-28 MeV; calculated σ(θ, E); deduced α-particle optical model parameters for A=45-209 target nuclei. Comparison with experimental data.
doi: 10.1103/PhysRevC.90.044612
2014FI12 Nucl.Data Sheets 120, 226 (2014) U.Fischer, M.Avrigeanu, V.Avrigeanu, O.Cabellos, I.Kodeli, A.Koning, A.Yu.Konobeyev, H.Leeb, D.Rochman, P.Pereslavtsev, P.Sauvan, J.-C.Sublet, A.Trkov, E.Dupont, D.Leichtle, J.Izquierdo The Activities of the European Consortium on Nuclear Data Development and Analysis for Fusion
doi: 10.1016/j.nds.2014.07.053
2014LE24 Nucl.Data Sheets 119, 353 (2014) X.Ledoux, M.Aiche, M.Avrigeanu, V.Avrigeanu, L.Audouin, E.Balanzat, B.Ban-detat, G.Ban, G.Barreau, E.Bauge, G.Belier, P.Bem, V.Blideanu, C.Borcea, S.Bouffard, T.Caillaud, A.Chatillon, S.Czajkowski, P.Dessagne, D.Dore, M.Fallot, F.Farget, U.Fischer, L.Giot, T.Granier, S.Guillous, F.Gunsing, C.Gustavsson, B.Jacquot, K.Jansson, B.Jurado, M.Kerveno, A.Klix, O.Landoas, F.R.Lecolley, J.L.Lecouey, M.Majerle, N.Marie, T.Materna, J.Mrazek, F.Negoita, J.Novak, S.Oberstedt, A.Oberstedt, S.Panebianco, L.Perrot, A.J.M.Plompen, S.Pomp, J.M.Ramillon, D.Ridikas, B.Rosse, G.Rudolf, O.Serot, S.P.Simakov, E.Simeckova, A.G.Smith, J.C.Sublet, J.Taieb, L.Tassan-Got, D.Tarrio, A.Takibayev, I.Thfoin, I.Tsekhanovich, C.Varignon The Neutrons for Science Facility at SPIRAL-2
doi: 10.1016/j.nds.2014.08.097
2014NI11 Phys.Rev. C 89, 064314 (2014) C.R.Nita, D.Bucurescu, N.Marginean, M.Avrigeanu, G.Bocchi, S.Bottoni, A.Bracco, A.M.Bruce, G.Cata-Danil, G.Colo, D.Deleanu, D.Filipescu, D.G.Ghita, T.Glodariu, S.Leoni, C.Mihai, P.J.R.Mason, R.Marginean, A.Negret, D.Pantelica, Z.Podolyak, P.H.Regan, T.Sava, L.Stroe, S.Toma, C.A.Ur, E.Wilson Fast-timing lifetime measurements of excited states in 67Cu NUCLEAR REACTIONS 64Ni(α, p), E=18 MeV; measured Eγ, Iγ, γγ-coin, level half-lives by γγ(t) using a fast-timing technique at IFIN-HH tandem accelerator facility. 67Cu; deduced levels, J, π, B(E1), B(M1), B(E2), B(M2), B(E3), Comparison with particle-vibration weak-coupling scheme, and shell-model calculations. Comparison of calculated and experimental spectroscopic factors in proton pickup reaction 68Zn(d, 3He)67Cu and proton stripping reaction 62Ni(α, p)65Cu.
doi: 10.1103/PhysRevC.89.064314
2013AV05 Phys.Rev. C 88, 014612 (2013) M.Avrigeanu, V.Avrigeanu, P.Bem, U.Fischer, M.Honusek, A.J.Koning, J.Mrazek, E.Simeckova, M.Stefanik, L.Zavorka Low-energy deuteron-induced reactions on 93Nb NUCLEAR REACTIONS 93Nb(d, p)94mNb; 93Nb(d, 2n)93mMo; 93Nb(d, X)92mNb; 93Nb(d, 2nα)89Zr; 93Nb(d, pα)90mY, E=1-20 MeV; measured Eγ, Iγ, σ(E) by activation method and stacked-foil technique. Comparison with previous experimental data. 93Nb(d, d), E=11.8, 15, 34.4, 52 MeV; analyzed σ(θ, E) data; deduced optical model parameters. 93,94,95Mo; comparison of previously measured and calculated E1 strength functions. Comparisons with calculations which included deuteron breakup effects, one-nucleon transfer (DR), pre-equilibrium (PE) and compound nucleus mechanisms, spin distribution of nuclear level densities and radiative strength functions using FRESCO and STAPRE-H computer codes. Comparison with calculations using TALYS-1.4 computer code, and with TENDL-2012 evaluated data.
doi: 10.1103/PhysRevC.88.014612
2012AV02 Phys.Rev. C 85, 034603 (2012) M.Avrigeanu, V.Avrigeanu, A.J.Koning Investigation of deuteron breakup and deuteron-induced fission on actinide nuclei at low incident energies NUCLEAR REACTIONS 231Pa(d, 3n)230U, E=10-20 MeV; analyzed deuteron breakup cross section as function of energy, excitation function, neutron- and proton-emission cross sections. Investigated dominance of the deuteron breakup mechanism. Comparison with Evaluated data.
doi: 10.1103/PhysRevC.85.034603
2012AV04 Phys.Rev. C 85, 044618 (2012) M.Avrigeanu, V.Avrigeanu, M.Diakaki, R.Vlastou Isomeric cross sections of fast-neutron-induced reactions on 197Au NUCLEAR REACTIONS 197Au(n, xn)194Au/195Au/196Au/196mAu, E=8-40 MeV; 197Au(n, p)197Pt/197mPt, E=8-20 MeV; 197Au(n, α)194Ir/194mIr, E=8-20 MeV; analyzed σ(E); deduced model parameters. Optical potential model with level density from backshifted Fermi gas (BSFG) formula. Comparison with evaluated data libraries.
doi: 10.1103/PhysRevC.85.044618
2011AV02 Phys.Rev. C 83, 017601 (2011) Analysis of α-induced reactions on 151Eu below the Coulomb barrier017601 NUCLEAR REACTIONS 151Eu(α, γ), (α, n), E=12-17 MeV; calculated σ using optical model potential (OMP). Comparison with measured cross sections. 154Tb; deduced level, isomer, J, π.
doi: 10.1103/PhysRevC.83.017601
2011AV07 J.Korean Phys.Soc. 59, 891s (2011) Key Issues for Consistent Description of Neutron-induced Reactions on Cr Isotopes NUCLEAR REACTIONS 50,52,53,54Cr(n, X), E=0.1-60 MeV;50,52,53,54Cr(n, γ), E=0.001-1 MeV;50,52Cr(n, n'), E=0-60 MeV;52Cr(n, p), E=5-22 MeV;52Cr(n, 2n), E=10-40 MeV;51V(p, n), E=0-25 MeV;51V(p, γ), E=1-5 MeV;51V, 55Mn, 59Co, 63,65Cu(p, X), E=0-50 MeV; calculated σ using TALYS and EMPIRE-II codes with different optical model parameters. Comparison with data.
doi: 10.3938/jkps.59.891
2011AV08 J.Korean Phys.Soc. 59, 903s (2011) Analysis of Deuteron Breakup and Induced Activation on Medium Nuclei NUCLEAR REACTIONS 59Co(d, d), E=6.5, 17 MeV;93Nb(d, d), E=11.8, 15, 34.4, 52 MeV; calculated σ(θ); 59Co(d, d), E=0-60 MeV; calculated σ; 59Co, 63,65Cu, 93Nb(d, X), (d, p), E=0-30 MeV; calculated σ and separately elastic and inelastic breakup σ; 93Nb(n, 2n), E=0-30 MeV;93Nb(p, d), E=10-45 MeV;93Nb(p, n), E=3-60 MeV;93Nb(n, α), E=3-30 MeV;93Nb(n, nα), E=15-70 MeV;93Nb(d, x)92mNb, (d, 2n), E=5-45 MeV;93Nb(d, x)90mY, E=13-45 MeV;93Nb(d, x)89Zr, E=15-45 MeV; calculated σ; 59Co(d, xn), (d, xp), E=7.5 MeV; calculated σ(En), σ(Ep). TALYS 1.2 code with components from individual processes. Comparison with data and other calculations.
doi: 10.3938/jkps.59.903
2011SI17 Phys.Rev. C 84, 014605 (2011) E.Simeckova, P.Bem, M.Honusek, M.Stefanik, U.Fischer, S.P.Simakov, R.A.Forrest, A.J.Koning, J.-C.Sublet, M.Avrigeanu, F.L.Roman, V.Avrigeanu Low and medium energy deuteron-induced reactions on 63, 65Cu nuclei NUCLEAR REACTIONS Cu(d, X)64Cu, E=1.5-19.88 MeV; 63Cu(d, 2n)63Zn, E=4.56-19.49 MeV; 63Cu(d, 3n)62Zn, E=16.44-19.88 MeV; 65Cu(d, p)66Cu, E=4.56-19.49 MeV; 65Cu(d, 2n)65Zn, E=4.25-19.88 MeV; 65Cu(d, 2p)65Ni, E=11.36-19.88 MeV; measured Eγ, Iγ, σ(E), activation method. Comparison with previous experimental data, and with evaluated data files. Cu(d, d), E=11.8, 15, 21.6 MeV; 63,65Cu(d, d), E=12, 34.4 MeV; analyzed σ(θ) data; Cu(d, d), 63,65Cu(d, d), E<60 MeV; analyzed σ(E) data; deduced optical potential model parameters for reaction cross sections. Deuteron breakup mechanism, and direct reaction stripping discussed.
doi: 10.1103/PhysRevC.84.014605
2011SI29 J.Korean Phys.Soc. 59, 1928s (2011) E.Simeckova, P.Bem, M.Honusek, L.Zavorka, U.Fischer, S.P.Simakov, R.A.Forrest, M.Avrigeanu, V.Avrigeanu, F.L.Roman On Low and Medium Energy Deuteron-Induced Reactions on 63, 65Cu NUCLEAR REACTIONS 63,65Cu(d, p), (d, 2n), (d, 3n), (d, 2p), E=4-20 MeV; measured Eγ, Iγ using stacked-foil; deduced activation σ; calculated σ using optical model with CC code FRESCO and TALYS-1.0, STAPRE-H. Comparison with available data, TENDL-2009.
doi: 10.3938/jkps.59.1928
2010AV02 Phys.Rev. C 81, 038801 (2010) Additional α-particle optical potential tests below the Coulomb barrier NUCLEAR REACTIONS 113In(α, n), (α, γ)116Sb/116mSb/117Sb, E=8-14 MeV; 115In(α, n), (α, γ)118Sb/118mSb/119Sb, E=8-25 MeV; calculated total α capture σ using optical model potential (OMP). Comparison with experimental data.
doi: 10.1103/PhysRevC.81.038801
2010AV05 Phys.Rev. C 82, 014606 (2010) α-particle nuclear surface absorption below the Coulomb barrier in heavy nuclei NUCLEAR REACTIONS 113,115In, 121,123Sb, 139La, 141Pr, 150Nd, 159Tb, 165Ho, 169Tm, 181Ta, 191Ir, 192Os, 197Au(α, n), 113,115In, 127I, 136Xe, 139La, 144Sm, 197Au(α, γ), 121Sb(α, 2n), E=8-25 MeV; analyzed σ using optical model potential (OMP). Energy dependence of the surface imaginary potential depth.
doi: 10.1103/PhysRevC.82.014606
2010AV07 Phys.Rev. C 82, 037601 (2010) Improved deuteron elastic breakup energy dependence via the continuum-discretized coupled-channels method NUCLEAR REACTIONS 63Cu, 93Nb(d, d), calculated σ, σ(θ) using continuum-discretized coupled-channels (CDCC) method. Comparison with experimental data.
doi: 10.1103/PhysRevC.82.037601
2010AV09 J.Phys.:Conf.Ser. 205, 012014 (2010) Deuteron breakup effects on activation cross sections at low and medium energies NUCLEAR REACTIONS 27Al(d, d), E=5-15 MeV; calculated σ(θ) using optical model with three different potentials; deduced optical model parameters. 27Al, 63,65Cu(d, X), (d, np), E=3-60 MeV; calculated σ. 27Al(d, n), (d, p), (d, α), (d, 2n), (d, 2p), (d, pα), E=3-60 MeV; calculated σ using different computer codes. Compared with available data.
doi: 10.1088/1742-6596/205/1/012014
2009AV01 Phys.Rev. C 79, 027601 (2009) α-particle optical potential tests below the Coulomb barrier NUCLEAR REACTIONS 92Mo, 94Mo, 112Sn(α, n), (α, X), E(c.m.)=7.5-11.5 MeV; 117Sn, 118Sn(α, γ), (α, X), E(c.m.)=7.5-11.5 MeV; 117Sn(α, p)120mSb, E(c.m.)=7.5-11.5 MeV 121Sb(p, n), (p, p'), (p, γ), E(c.m.)=4.5-9.5 MeV; calculated σ using different α-particle optical potential parameters. Discussed limitations of statistical-model calculations. Comparisons with experimental data.
doi: 10.1103/PhysRevC.79.027601
2009AV03 At.Data Nucl.Data Tables 95, 501 (2009) M.Avrigeanu, A.C.Obreja, F.L.Roman, V.Avrigeanu, W.von Oertzen Complementary optical-potential analysis of α-particle elastic scattering and induced reactions at low energies COMPILATION A=50-120; 45Sc, 118Sn(α, γ), (α, n), (α, p); Analyzed reaction σ. Double Folding Model.
doi: 10.1016/j.adt.2009.02.001
2009BE16 Phys.Rev. C 79, 044610 (2009) P.Bem, E.Simeckova, M.Honusek, U.Fischer, S.P.Simakov, R.A.Forrest, M.Avrigeanu, A.C.Obreja, F.L.Roman, V.Avrigeanu Low and medium energy deuteron-induced reactions on 27Al NUCLEAR REACTIONS 27Al(d, p), (d, 2p), (d, pα), E=3.38-20.18 MeV; 63Cu(d, 2n), E=4-20 MeV; measured excitation functions. 27Al(d, n), (d, 2n), (d, α), E<25 MeV; comparison of cross section data. Comparison with calculations from TALYS and ACSELAM computer codes, and experimental data.
doi: 10.1103/PhysRevC.79.044610
2009CA27 Nucl.Data Sheets 110, 3107 (2009) R.Capote, M.Herman, P.Oblozinsky, P.G.Young, S.Goriely, T.Belgya, A.V.Ignatyuk, A.J.Koning, S.Hilaire, V.A.Plujko, M.Avrigeanu, O.Bersillon, M.B.Chadwick, T.Fukahori, Z.Ge, Y.Han, S.Kailas, J.Kopecky, V.M.Maslov, G.Reffo, M.Sin, E.Sh.Soukhovitskii, P.Talou RIPL - Reference Input Parameter Library for Calculation of Nuclear Reactions and Nuclear Data Evaluations
doi: 10.1016/j.nds.2009.10.004
2009KI16 Phys.Rev. C 80, 045807 (2009) G.G.Kiss, P.Mohr, Zs.Fulop, D.Galaviz, Gy.Gyurky, Z.Elekes, E.Somorjai, A.Kretschmer, K.Sonnabend, A.Zilges, M.Avrigeanu High precision 89Y(α, α)89Y scattering at low energies NUCLEAR REACTIONS 89Y(α, α), E(cm)=15.51, 18.63 MeV; measured Eα, Iα, σ; deduced parameters for local scattering potentials. 89Y(α, α), E(cm)=20.1, 22.0, 23.9, 40.2, 62.2, 158.9 MeV; 92Mo(α, α), E(cm)=15.69, 18.62 MeV; analyzed σ and σ(θ) measurements with different potential parameters. 93Nb; analyzed α-cluster states in 89Y+α system, bands, and B(E2) using potential parameters close to those for the scattering potential.
doi: 10.1103/PhysRevC.80.045807
2008AV03 Nucl.Phys. A806, 15 (2008) M.Avrigeanu, S.V.Chuvaev, A.A.Filatenkov, R.A.Forrest, M.Herman, A.J.Koning, A.J.M.Plompen, F.L.Roman, V.Avrigeanu Fast-neutron induced pre-equilibrium reactions on 55Mn and 63, 65Cu at energies up to 40 MeV NUCLEAR REACTIONS 55Mn, 63,65Cu(n, X), (n, γ), E=0.001?50 MeV; 52,53,54Cr, 55Mn, 54,56,57,58Fe, 59Co, 58,60,61,62,64Ni, 63,65Cu, 64,66,68Zn(p, X), (p, n), (p, γ), E=1?20 MeV; analyzed total, activation and capture σ and particle emission spectra using an optical model with emphasis on pre-equilibrium emission. Comparison with all available data.
doi: 10.1016/j.nuclphysa.2008.03.010
2008KI06 J.Phys.(London) G35, 014037 (2008) G.G.Kiss, G.Gyurky, Z.Fulop, E.Somorjai, D.Galaviz, A.Kretschmer, K.Sonnabend, A.Zilges, P.Mohr, M.Avrigeanu Study of the 89Y(α, α)89Y reaction close to the Coulomb barrier NUCLEAR REACTIONS 89Y(α, α), E(cm)=15.5, 18.6 MeV; measured Eα, Iα, σ(θ).
doi: 10.1088/0954-3899/35/1/014037
2008PE23 Nucl.Instrum.Methods Phys.Res. B266, 3501 (2008) P.Pereslavtsev, U.Fischer, S.Simakov, M.Avrigeanu Evaluation of d + 6, 7Li data for deuteron incident energies up to 50 MeV NUCLEAR REACTIONS 6,7Li(d, d'), (d, n), (d, p), (d.t), (d, α), E=4-50 MeV; calculated neutron energy spectra, σ, σ(θ), σ(E, θ); particle evaporation, pre-equilibrium emission, stripping and direct interaction processes; GNASH, ECIS96, Serber model, DWUCK4 code.
doi: 10.1016/j.nimb.2008.05.014
2006AV02 Nucl.Phys. A764, 246 (2006) M.Avrigeanu, W.von Oertzen, V.Avrigeanu On temperature dependence of the optical potential for alpha-particles at low energies NUCLEAR REACTIONS 92,95,98,100Mo(n, α), 89,96Zr(α, n), E < 20 MeV; analyzed σ; deduced parameters, temperature dependence features. Woods-Saxon potential and optical model.
doi: 10.1016/j.nuclphysa.2005.10.001
2006AV03 Phys.Rev. C 73, 038801 (2006) Addendum to "Elastic α-scattering on 112Sn and 124Sn at astrophysically relevant energies" NUCLEAR REACTIONS 112Sn(α, α), E=14.4, 19.5 MeV; 124Sn(α, α), E=19.5 MeV; analyzed elastic σ(θ); deduced improved optical potential parameters.
doi: 10.1103/PhysRevC.73.038801
2005AV06 Nucl.Phys. A759, 327 (2005) M.Avrigeanu, W.von Oertzen, U.Fischer, V.Avrigeanu Analysis of deuteron elastic scattering on 6, 7Li up to 50 MeV NUCLEAR REACTIONS 6,7Li(d, d), E=3-50 MeV; analyzed angular distributions; deduced optical model parameters.
doi: 10.1016/j.nuclphysa.2005.05.153
2003AV04 Nucl.Phys. A723, 104 (2003) M.Avrigeanu, W.von Oertzen, A.J.M.Plompen, V.Avrigeanu Optical model potentials for α-particles scattering around the Coulomb barrier on A ∼ 100 nuclei NUCLEAR REACTIONS 4He(α, α), E < 35 MeV; analyzed σ(θ); deduced density distribution. 89Y, 90,91Zr, 92,94,96,98,100Mo, 107Ag, 116,122,124Sn(α, α), E ≈ 14-32 MeV; analyzed σ(θ); deduced optical potential features.
doi: 10.1016/S0375-9474(03)01159-X
2002AV02 Int.J.Mod.Phys. E11, 249 (2002) M.Avrigeanu, G.S.Anagnostatos, A.N.Antonov, V.Avrigeanu Elastic Scattering as a Test of Density Distributions in 6He and 8He NUCLEAR REACTIONS 1H(6He, 6He), (8He, 8He), E = 25-72 MeV/nucleon; calculated σ(θ), optical potential features. 6,8He deduced matter density distribution features. Comparison with data.
doi: 10.1142/S021830130200082X
2001AN24 Yad.Fiz. 64, No 7, 1304 (2001); Phys.Atomic Nuclei 64, 1229 (2001) G.S.Anagnostatos, C.Politis, A.Vahlas, J.Giapitzakis, A.N.Antonov, M.Avrigeanu Light Exotic Nuclei: A new explanation of halo NUCLEAR STRUCTURE 6,8He; calculated neutron and proton density distributions. 7,8,9,10Be; calculated binding energies, radii, internal vibrational and rotational energies.
doi: 10.1134/1.1389547
2001AV03 Nucl.Phys. A693, 616 (2001) M.Avrigeanu, A.N.Antonov, H.Lenske, I.Stetcu Effective Interactions for Multistep Processes NUCLEAR REACTIONS 93Nb, 90Zr(p, p), E ≈ 22 MeV; 90Zr(p, n), E=25.6 MeV; 94,95,96,97,98,100Mo(p, xn), E=25.6 MeV; calculated σ(E, θ). Effective interactions, multistep direct processes, comparisons with data.
doi: 10.1016/S0375-9474(01)00810-7
2001KR25 Eur.Phys.J. A 12, 399 (2001) I.V.Krouglov, M.Avrigeanu, W.von Oertzen Two-Neutron Elastic Transfer 4He(6He, 4He)6He at E = 151 MeV NUCLEAR REACTIONS 4He(6He, α), (6He, 6He), E=151 MeV; analyzed σ(θ); deduced reaction mechanism features. Coupled channels analysis.
doi: 10.1007/s10050-001-8663-3
2000AV02 Phys.Rev. C62, 017001 (2000) M.Avrigeanu, G.S.Anagnostatos, A.N.Antonov, J.Giapitzakis Dynamics of Two-Neutron Transfer Reactions on the Borromean Nucleus 6He Reexamined NUCLEAR REACTIONS 1H, 4He(6He, 6He), E=151 MeV; calculated σ(θ). 4,6He deduced density distribution features. Comparisons with data.
doi: 10.1103/PhysRevC.62.017001
2000AV05 Trans.Bulg.Nucl.Soc. 5, 3 (2000) M.Avrigeanu, I.Stetcu, V.Avrigeanu Realistic Effective NN Interactions for Multistep Direct Reactions to the Continuum NUCLEAR REACTIONS 90Zr, 93Nb, 96,98,100Mo(n, n), E=17-26 MeV; 90Zr, 93Nb(p, p), E=22 MeV; calculated σ(θ). 90Zr(p, n), E=25.6 MeV; 94,95,96,97,98,100Mo(p, xn), E=25.6 MeV; calculated σ(E, θ). Multistep direct reaction theory, several effective interactions compared. Comparisons with data.
1998AV04 Comput.Phys.Commun. 112, 191 (1998) Partial Level Densities for Nuclear Data Calculations NUCLEAR STRUCTURE 23C; calculated partial level densities vs excitation energy. Equidistant spacing model. Application to pre-equilibrium reaction models discussed.
doi: 10.1016/S0010-4655(98)00050-2
1998HA33 Phys.Rev. C58, 295 (1998) A.Harangozo, I.Stetcu, M.Avrigeanu, V.Avrigeanu Particle-Hole State Densities with Nonequidistant Single-Particle Levels
doi: 10.1103/PhysRevC.58.295
1997AV02 Phys.Rev. C56, 1633 (1997) M.Avrigeanu, A.Harangozo, V.Avrigeanu, A.N.Antonov Average Strength of the Effective Interaction in Multistep Direct Reactions NUCLEAR REACTIONS 93Nb(p, p'), (n, n'), E=20-80 MeV; calculated first NN-collision probability radial dependence, effective NN interaction strengths; deduced surface effects, nuclear density dependence features. Optical model potential, local density approximation.
doi: 10.1103/PhysRevC.56.1633
1997PA10 J.Phys.(London) G23, 79 (1997) K.A.Pavlova, M.Avrigeanu, A.N.Antonov Short-Range Nucleon Correlations in the Semiclassical Nuclear Models NUCLEAR STRUCTURE 93Nb, 208Pb, 118Sn; calculated nucleon number fraction in volume with given radius, other aspects. Local density approximation, short-range correlations.
doi: 10.1088/0954-3899/23/1/006
1996AV04 Roum.J.Phys. 41, 77 (1996) M.Avrigeanu, A.Harangozo, V.Avrigeanu Surface Effects in Feshbach-Kerman-Koonin Analysis of (n, n') and (n, p) Reactions at 7 to 26 MeV NUCLEAR STRUCTURE A=45-94; analyzed resonance data; deduced level density parameters. NUCLEAR REACTIONS 93Nb(n, 2n), (n, α), (n, 3n), E < 24 MeV; analyzed σ(E). 93Nb(n, n'), E=7 MeV; 93Nb(n, xn), E=14.1-25.7 MeV; 93Nb(n, xp), E=14.1, 15 MeV; 93Nb(n, xα), E=14.1, 15 MeV; analyzed particle emission spectra. 56Fe, 48Ti, 93Nb(n, n'), 93Nb(n, p), E=14.1 MeV; 56Fe(n, n'), E=25.7 MeV; 93Nb(n, n'), E=7-25.7 MeV; analyzed σ(θ, E(nucleon)). Ti(n, xn), 46,48Ti(n, xp), E=14.1 MeV; analyzed angle integrated spectra; deduced surface effects role. Feshbach-Kerman-Koonin approach, other aspects of these reactions also included.
1996AV05 Phys.Rev. C54, 2538 (1996) M.Avrigeanu, A.Harangozo, V.Avrigeanu, A.N.Antonov Nuclear Surface Localization of Preequilibrium Reactions at Low Energies NUCLEAR REACTIONS 93Nb(n, n'), E=10-50 MeV; calculated first NN-collision probability, average local Fermi energy, other aspects in preequilibrium reactions.
doi: 10.1103/PhysRevC.54.2538
1995AV03 J.Phys.(London) G21, 837 (1995) M.Avrigeanu, V.Avrigeanu, A.N.Antonov, M.B.Chadwick, P.E.Hodgson, M.V.Stoitsov Pauli-Blocking Effects in Neutron-Alpha Reactions NUCLEAR REACTIONS 54Fe, 51V, 55Mn, 59Co, 48Ti, 52Cr(n, α), E ≈ 4-20 MeV; analyzed σ(E); deduced model parameters variations range limitations, Pauli-blocking effects.
doi: 10.1088/0954-3899/21/6/011
1995AV06 Roum.J.Phys. 40, 453 (1995) M.Avrigeanu, A.Harangozo, V.Avrigeanu Surface Effects in Multistep Reaction Calculations NUCLEAR REACTIONS 56Fe(n, xn), (n, xp), E=14.8 MeV; 48Ti(n, xn), E=14.1 MeV; 46,48Ti(n, xp), E=14.8 MeV; calculated angle integrated proton, neutron emission spectra. Feschbach-Kerman-Koonim theory, surface effects.
1994AV01 Phys.Rev. C49, 2136 (1994) V.Avrigeanu, P.E.Hodgson, M.Avrigeanu Global Optical Potentials for Emitted Alpha Particles NUCLEAR REACTIONS 54Fe, 52Cr, 59Co, 48,50Ti, 51V(n, α), E < 10 MeV; calculated σ(E). 40Ca, 55Mn, 59Co(α, X), E < 13 MeV; calculated reaction σ(E). Global optical potentials.
doi: 10.1103/PhysRevC.49.2136
1994AV02 J.Phys.(London) G20, 613 (1994) Energy-Dependent Single-Particle State Density Effects in the Hybrid Model of Pre-Equilibrium Nuclear Reactions NUCLEAR REACTIONS 51V, 56Fe(n, xn), (n, xp), (n, xα), E=14.1 MeV; calculated angle integrated σ vs excitation energy. 56Fe, 51V(n, p), (n, 2n), (n, α), E=threshold-20 MeV; calculated reaction σ(E). Fermi gas model type energy dependences of single-hole, excited-particle densities, preequilibrium, hybrid models.
doi: 10.1088/0954-3899/20/4/009
1993AV02 J.Phys.(London) G19, 745 (1993) M.Avrigeanu, P.E.Hodgson, A.J.Koning Semiclassical and Quantum Mechanical Pre-Equilibrium Neutron Emission NUCLEAR REACTIONS 56Fe, 58Ni, 51V, 55Mn, 52Cr, 59Co(n, xn), E=14 MeV; analyzed angle-integrated σ data. 58Fe(p, n), E=14 MeV; 59Co(p, n), E=14.7 MeV; analyzed σ(θn, En) data. Semi-classical, quantum approach, preequilibrium neutron emission.
doi: 10.1088/0954-3899/19/5/008
1993AV04 Roum.J.Phys. 38, 407 (1993) Energy-Dependent Single-Particle State Density NUCLEAR STRUCTURE 56,57Fe, 56Mn; calculated particle-hole state density. Different models.
1990AV01 Z.Phys. A335, 299 (1990) M.Avrigeanu, M.Ivascu, V.Avrigeanu Nuclear Level Densities Below 40 MeV Excitation Energy in the Mass Region A ≈ 50 NUCLEAR STRUCTURE A=50-65; analyzed resonance data; deduced level density, other parameters. NUCLEAR REACTIONS, ICPND 52Cr, 56,54Fe, 58,60Ni(n, n'), E=2-20 MeV; calculated inelastic σ(E). 51V(α, X), (α, n), E=5.5-12 MeV; calculated reaction σ(E). 52,50Cr, 54,56Fe, 58,60Ni(n, xp), E ≈ 14.8 MeV; 50,52Cr, 54,56Fe, 58,60Ni(n, xα), E ≈ 14.5 MeV; calculated angle integrated particle emission spectra. 52,50Cr(n, 2n), E ≈ 13-20 MeV; 52Cr(n, p), (n, α), E ≈ 5-19 MeV; 53Cr(n, p), E ≈ 5-20 MeV; 61,58Ni, 54Fe(n, p), E ≈ 2-20 MeV; 54Fe(n, α), E ≈ 4-20 MeV; 58Ni, 54Fe(n, 2n), E ≈ 14-20 MeV; 56Fe(n, 2n), E=11-22 MeV; 60Ni, 56Fe(n, p), E ≈ 5-20 MeV; 58Ni(n, np), E ≈ 10-20 MeV; 62Ni(n, p), (n, α), E ≈ 6-20 MeV; calculated reaction σ(E). Statistical model.
1989AV03 J.Phys.(London) G15, L241 (1989) M.Avrigeanu, D.Bucurescu, M.Ivascu, G.Semenescu, V.Avrigeanu On the Overlap of the Pre-Equilibrium and Direct Reaction Models NUCLEAR REACTIONS 54,56Fe(n, n'), E=11 MeV; calculated σ. 56Fe(n, n'), E ≈ 14 MeV; calculated neutron emission spectra. Preequilibrium, direct reaction models overlap.
doi: 10.1088/0954-3899/15/11/004
1989AV04 J.Phys.(London) G15, L261 (1989) Consistent Exciton State and Nuclear Level Densities NUCLEAR REACTIONS 50,52Cr, 54,56Fe, 58,60Ni(n, xp), E=15 MeV; 56Fe, 60Ni(n, xα), E=14.5 MeV; calculated angle integrated proton emission spectra. Consistent exciton state, nuclear level densities. ATOMIC PHYSICS, Mesic-Atoms 56Mn, 56,57Fe; calculated one-, two-fermion exciton state densities. Comparison with nuclear state densities.
doi: 10.1088/0954-3899/15/12/001
1988AV04 Z.Phys. A329, 177 (1988) M.Avrigeanu, M.Ivascu, V.Avrigeanu Pre-Equilibrium Emission in Neutron Induced Reactions on 54,56Fe NUCLEAR REACTIONS 54,56Fe(n, p), (n, xp), (n, α), (n, xα), (n, xn), (n, 2n), E=20 MeV; 54,56Fe(n, p), (n, α), E=14.8 MeV; calculated σ(En), σ(θp, Ep), σ(θn, En), angle integrated σ. Hybrid preequilibrium emission model.
1987AV07 Rev.Roum.Phys. 32, 837 (1987) M.Avrigeanu, V.Avrigeanu, G.Cata, M.Ivascu EDBW Model for the E1 Gamma-Ray Strength Function in the Mass Region 50 ≤ A ≤ 90 NUCLEAR STRUCTURE A=40-240; analyzed GDR data; deduced E1 strength function nuclear deformation dependence for A=50-90.
1987IV03 Rev.Roum.Phys. 32, 697 (1987) M.Ivascu, V.Avrigeanu, M.Avrigeanu Nuclear Level Densities in the Mass Range 40 < A < 65 NUCLEAR STRUCTURE A=40-70; calculated level densities. Back shifted Fermi gas model.
1987IV04 Rev.Roum.Phys. 32, 713 (1987) M.Ivascu, M.Avrigeanu, V.Avrigeanu A Geometry Dependent Hybrid Pre-Equilibrium Emission Model with Conservation of Angular Momentum NUCLEAR REACTIONS 46,48Ti(n, np), E=15 MeV; calculated angle integrated σ. Geometry dependent hybrid preequilibrium model.
1986IV02 Radiat.Eff. 95, 207 (1986) M.Ivascu, M.Avrigeanu, V.Avrigeanu Preequilibrium and Statistical Model Calculations for Neutron Activation Cross Sections on Titanium Isotopes NUCLEAR REACTIONS 46,47,48,49,50Ti(n, p), (n, n'p), (n, 2n), E=threshold-20 MeV; calculated σ(E). Hauser-Feshbach, optical model, preequilibrium emission.
doi: 10.1080/00337578608208697
1986IV03 Radiat.Eff. 95, 211 (1986) M.Ivascu, M.Avrigeanu, V.Avrigeanu Level Density Shell Effects in Neutron Induced Reactions on Molybdenum Isotopes NUCLEAR REACTIONS 92,94,95,96,97,98,100Mo(n, p), (n, n'p), (n, 2n), E=threshold-20 MeV; calculated σ(En), binding energies; deduced isotopic effects. Preequilibrium, statistical models.
doi: 10.1080/00337578608208698
1981BU02 J.Phys.(London) G7, 399 (1981) D.Bucurescu, G.Constantinescu, M.Ivascu, N.V.Zamfir, M.Avrigeanu Recoil-Distance Measurements of the Lifetimes of High-Spin States in 83Sr and 85Sr NUCLEAR REACTIONS 74,76Ge(12C, 3n), E=40-45 MeV; measured γ(θ), DSA, recoil. 83,85Sr deduced levels, J, π, γ-branching, δ, T1/2, γ-multipolarity, B(M1), B(E2). Enriched targets, Ge(Li)detector. Asymmetric rotor model, variable moment of inertia.
doi: 10.1088/0305-4616/7/3/015
1981BU05 J.Phys.(London) G7, 667 (1981) D.Bucurescu, G.Constantinescu, M.Ivascu, N.V.Zamfir, M.Avrigeanu, D.Cutoiu Evidence for a g9/2 Decoupled Band in 85Y NUCLEAR REACTIONS 74Ge(14N, 3n), E=40-52 MeV; 72Ge(16O, 2np), E=45-64 MeV; 73Ge(16O, 3np), E=48-60 MeV; measured σ(Eγ, E), σ(Eγ, θ), pγ-, γγ-coin. 85Y deduced levels, J, π. Enriched targets, Ge(Li) detector.
doi: 10.1088/0305-4616/7/5/011
1978AV02 J.Phys.(London) G4, 261 (1978) M.Avrigeanu, V.Avrigeanu, D.Bucurescu, G.Constantinescu, M.Ivascu, D.Pantelica, M.Tanase, N.V.Zamfir Lifetime Measurements in 86Zr NUCLEAR REACTIONS 73Ge(16O, 3n), E=52.0 MeV; measured σ(Eγ, θ), DSA. 86Zr levels deduced T1/2. Enriched target, Ge(Li) detector.
doi: 10.1088/0305-4616/4/2/015
1978IV02 Rev.Roum.Phys. 23, 163 (1978) M.Ivascu, D.Bucurescu, G.Constantinescu, M.Avrigeanu, V.Avrigeanu On the High-Spin Sates of 83Sr and 85Sr NUCLEAR REACTIONS 74,76Ge(12C, 3nγ), (12C, xnγ), (12C, xnαγ), E=35-45 MeV; measured σ(E, Eγ). 83,85Sr deduced transitions.
1976BU08 Rev.Roum.Phys. 21, 97 (1976) D.Bucurescu, E.Dragulescu, M.Ivascu, M.Avrigeanu, G.Semenescu The (α, p) Reaction on Odd Cu and Ga Isotopes NUCLEAR REACTIONS 63,65Cu(α, p), E=19.4 MeV; 69,71Ga(α, p), E=20.0 MeV; measured σ(Ep, θ) to levels in 66,68Zn, 72,74Ge.
1974IV03 Nucl.Phys. A225, 357 (1974) M.Ivascu, D.Bucurescu, D.Popescu, V.Avrigeanu, E.Dragulescu, G.Semenescu, M.Avrigeanu Spectroscopy of the 69Ga and 71Ga Isotopes with the 69,71Ga(α, α'γ)69,71Ga and 66,68Zn(α, pγ)69,71Ga Reactions NUCLEAR REACTIONS 69,71Ga(α, α'γ), 66,68Zn(α, pγ), E=13 MeV; measured Eγ, Doppler shift attenuation. 69,71Ga levels deduced T1/2, E(X). Enriched targets.
doi: 10.1016/0375-9474(74)90546-6
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