NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = P.Descouvemont Found 222 matches. Showing 1 to 100. [Next]2023CH49 Phys.Rev. C 108, 044605 (2023) Analysis of the 16C (d, p)17C reaction from microscopic 17C wave functions
doi: 10.1103/PhysRevC.108.044605
2023DE03 Phys.Rev. C 107, 014312 (2023) Spectroscopic amplitudes in microscopic three-cluster systems NUCLEAR STRUCTURE 6He, 11Li, 14Be; calculated radial functions for ground states, probability distribution of the ground state. Microscopic three cluster model based on resonating group method (RGM) and generator coordinate method (GCM).
doi: 10.1103/PhysRevC.107.014312
2022DE32 Eur.Phys.J. A 58, 193 (2022) A semi-microscopic approach to transfer reactions NUCLEAR REACTIONS 14C(d, p), 6He(d, n), E not given; calculated energy levels, J, π, σ(θ) using a natural extension of the standard DWBA method.
doi: 10.1140/epja/s10050-022-00840-5
2022SH08 Phys.Rev. C 105, 024605 (2022) Breakup effects in the 16C+p and 16C+d reactions NUCLEAR STRUCTURE 16C; calculated levels, J, π, B(E2). Description of 16C as a three-body structure 14C+n+n in hyperspherical coordinates. Comparison to experimental data. NUCLEAR REACTIONS 1H, 2H(16C, 16C), E=5, 15, 24, 33, 40 MeV/nucleon; calculated elastic and inelastic σ(θ). Continuum discretized coupled channel (CDCC) method. Comparison to experimental data.
doi: 10.1103/PhysRevC.105.024605
2021DE04 Eur.Phys.J. A 57, 29 (2021) Resonances in 12C and 24Mg: what do we learn from a microscopic cluster theory? NUCLEAR STRUCTURE 12C, 24Mg; analyzed available data; calculated energy curves, r.m.s. radii, Hoyle states using a microscopic cluster model, where the generator coordinate is defined in the hyperspherical formalism.
doi: 10.1140/epja/s10050-020-00337-z
2021DE28 Phys.Rev. C 104, 024613 (2021) Halo effects in the 11Li (p, t) 9Li reaction NUCLEAR REACTIONS 11Li(p, t)9Li, (p, p)11Li, E=33 MeV; calculated three-body wave functions for 11Li treated as 9Li+n+n and 3H as p+n+n, 9Li+t elastic scattering wave functions and σ(θ) using continuum discretized coupled channel (CDCC) method and optical model potential, integrated cross section, and 2n-transfer σ using distorted wave Born approximation (DWBA), with 11Li and 3He described in hyperspherical formalism as 9Li+n+n and p+n+n, respectively; deduced that transfer process is sensitive to halo structure of 11Li. Comparison with σ(θ) experimental data for 11Li(p, t) transfer reaction.
doi: 10.1103/PhysRevC.104.024613
2021DO04 Phys.Rev. C 103, 034619 (2021) Exchange effects in nucleus-nucleus reactions NUCLEAR REACTIONS 13C(12C, 12C), (12C, 12C'), E(cm)=7.8, 14.2 MeV; 13N(12C, 12C), E(cm)=7.8, 9.6 MeV; 16O(12C, 12C), E(cm)=23.4 MeV; calculated elastic scattering σ(E, q), inelastic σ(Ε, θ) for 13C+12C, amplitudes of scattering matrices, local effective potentials, contributions of the overlap, kinetic energy, and potentials to the nonlocal kernels. Scattering three-body model with coupled-channel system, including nonlocal terms, and R-matrix method using Lagrange functions, an extension of continuum discretized coupled channel (CDCC) formalism, with treatment of exchange effects in nucleus-nucleus scattering. Comparison with experimental data.
doi: 10.1103/PhysRevC.103.034619
2020CU03 Phys.Rev. C 102, 024622 (2020) D.C.Cuong, P.Descouvemont, D.T.Khoa, N.H.Phuc Coupled-reaction-channel study of the 12C(α, 8Be) reaction and the 8Be + 8Be optical potential NUCLEAR REACTIONS 8Be(8Be, 8Be), E(cm)=41.3 MeV; 8Be(α, α), E(cm)=43.3 MeV; 8Be(α, α), E=65 MeV; calculated differential σ(θ) using three- and four-body continuum-discretized coupled-channel (CDCC) methods, with realistic α + α interaction, and explicit accounting of the breakup effect; deduced local equivalent optical potential parameters. 12C(α, 8Be)8Be, E=65 MeV; calculated differential σ(θ) using the coupled-reaction channel (CRC) calculation with optical potentials from the CDCC calculations, and α spectroscopic factors from the complex scaling method (CSM) cluster model calculation; deduced cluster structure of 12C. Comparison with experimental data for elastic 12+α scattering.
doi: 10.1103/PhysRevC.102.024622
2020DE06 Prog.Theor.Exp.Phys. 2020, 023D02 (2020) A stochastic microscopic approach to the 10Be and 11Be nuclei NUCLEAR STRUCTURE 10,11Be; calculated energy spectra, J, π, proton and neutron monopole densities using microscopic multicluster model.
doi: 10.1093/ptep/ptz169
2020DE22 Phys.Rev. C 101, 064611 (2020) Low-energy 11Li + p and 11Li + d scattering in a multicluster model NUCLEAR STRUCTURE 11Li; calculated phase shift of 1- level, E1 strength distribution, pseudostate energies, J, π using the hyperspherical method for a three-body description (9Li+n+n) of 11Li. NUCLEAR REACTIONS 11Li(p, p), (p, X), E=66 MeV; 11Li(d, d), (d, X), E=55.3 MeV; calculated elastic and breakup σ, real and imaginary 11Li+p, 11Li+n, and 11Li+d potentials using the continuum discretized coupled channel (CDCC) method. Comparison with experimental data.
doi: 10.1103/PhysRevC.101.064611
2020LE08 Phys.Rev. C 102, 014608 (2020) Lagrange-mesh R-matrix method for inhomogeneous equations NUCLEAR REACTIONS 93Nb(d, pX), E=25.5 MeV; calculated double differential σ(E, θ), real and imaginary parts of the source term function for an outgoing proton using Lagrange-mesh R-matrix method. Comparisons with Green's function and Numerov methods.
doi: 10.1103/PhysRevC.102.014608
2019BR07 Phys.Lett. B 790, 237 (2019) C.G.Bruno, M.Aliotta, P.Descouvemont, A.Best, T.Davinson, D.Bemmerer, A.Boeltzig, C.Broggini, A.Caciolli, F.Cavanna, T.Chillery, G.F.Ciani, P.Corvisiero, R.Depalo, A.Di Leva, Z.Elekes, F.Ferraro, A.Formicola, Zs.Fulop, G.Gervino, A.Guglielmetti, C.Gustavino, Gy.Gyurky, G.Imbriani, M.Junker, M.Lugaro, P.Marigo, R.Menegazzo, V.Mossa, F.R.Pantaleo, D.Piatti, P.Prati, K.Stockel, O.Straniero, F.Strieder, T.Szucs, M.P.Takacs, D.Trezzi Improved astrophysical rate for the 18O(p, α)15N reaction by underground measurements NUCLEAR REACTIONS 18O(p, α)15N, E=60-360 keV; measured reaction products, Ep, Ip, Eα, Iα; deduced differential yield, resonance energies, S-factor, J, π, reaction rates.
doi: 10.1016/j.physletb.2019.01.017
2019DE13 Few-Body Systems 60, 11 (2019) Microscopic Description of 8Li + Nucleus and of 8B + Nucleus Scattering NUCLEAR STRUCTURE 8Li, 8B; calculated radii, quadrupole moments, B(E2), energy levels, neutron and proton densities. Generator Coordinate Method. NUCLEAR REACTIONS 12C(8Li, 8Li), E=14 MeV; 209Bi(8Li, 8Li), E=37 MeV; 12C(8B, 8B), E=25.8 MeV; 208Pb(8B, 8B), E=164 MeV; 58Ni(8B, 8B), E=29.3 MeV; calculated σ. Comparison with available data.
doi: 10.1007/s00601-018-1476-6
2019DE20 Phys.Rev. C 99, 064308 (2019) Microscopic three-cluster study of light exotic nuclei NUCLEAR STRUCTURE 11Li, 14Be, 15B, 17N, 15,17Ne; calculated ground-state energies, levels, J, π, proton-, neutron-, and matter-radii, and B(E2) in 17Ne using a microscopic three-cluster model with hyperspherical formalism. Comparison with experimental data.
doi: 10.1103/PhysRevC.99.064308
2019SH35 Phys.Rev. C 100, 034611 (2019) Transfer reactions with the Lagrange-mesh method NUCLEAR REACTIONS 16O(d, p)17O, E=25.4, 36 MeV; 12C(7Li, t)16O, E=28, 34 MeV; calculated σ(θ, E) for the (5/2+) g.s. and the first (1/2+) state in 17O, and 0+ g.s. and the first 2+ state in 16O. R-matrix method in distorted wave Born approximation (DWBA) calculations.
doi: 10.1103/PhysRevC.100.034611
2018DE03 Phys.Rev. C 97, 014612 (2018) 9B scattering with microscopic wave functions and the continuum-discretized coupled-channel method NUCLEAR STRUCTURE 9Be; calculated energies and neutron and proton monopole densities of the 3/2- and 1/2+ states, pseudostate energies for 1/2, 3/2, and 5/2 levels using microscopic wave functions defined in α+α+n multicluster model. NUCLEAR REACTIONS 208Pb(9Be, 9Be), E=38, 44, 50, 75 MeV; 27Al(9Be, 9Be), E=12, 22, 32 MeV; calculated σ(θ) and compared with experimental data. Continuum-discretized coupled-channel (CDCC) calculations.
doi: 10.1103/PhysRevC.97.014612
2018DE22 Phys.Rev. C 97, 064607 (2018) Four-body extension of the continuum-discretized coupled-channels method NUCLEAR REACTIONS 1,2H(11Be, 11Be), (11Be, 11Be'), E=26.9 MeV/nucleon; 7Li(d, d), (d, d'), E=25 MeV; 3H(p, p), E=12 MeV; calculated elastic scattering σ with and without breakup channels, and breakup differential σ(θ) with and without core excitation for 11Be+d and 11Be+p reactions. Calculations used four body continuum-discretized coupled-channels (CDCC) method. Comparison with experimental values. NUCLEAR STRUCTURE 16O; calculated energy of the 4α system as a function of 8Be truncation energy for J=0+, 2+ states using CDCC method with Ali-Bodmer potential.
doi: 10.1103/PhysRevC.97.064607
2018TU02 Phys.Rev. C 97, 014302 (2018) E.M.Tursunov, D.Baye, P.Descouvemont Updated three-body model of 6He β decay into the α + d continuum RADIOACTIVITY 6He(β-); calculated transition probability into α+d continuum and compared with experimental data, Gamow-Teller reduced transition probability. Three-body model (α+n+n for 6He) based on the hyperspherical Lagrange-mesh method.
doi: 10.1103/PhysRevC.97.014302
2017AD32 Phys.Rev. C 96, 054319 (2017) Three-body continuum of 26O NUCLEAR STRUCTURE 26O; calculated 24O+n+n three-body eigenphases for J=0+, 1- and 2+; deduced narrow resonance for J=2+ near 1.3 MeV with Γ ≈ 0.4 MeV, in agreement with recent experimental data. Hyperspherical formalism for 24O+n and n+n interactions, and R-matrix technique to derive wave functions and associated phase shifts.
doi: 10.1103/PhysRevC.96.054319
2017DE03 Phys.Rev. C 95, 014604 (2017) P.Descouvemont, L.F.Canto, M.S.Hussein Coulomb and nuclear effects in breakup and reaction cross sections NUCLEAR REACTIONS 208Pb(7Li, X), E(cm)=26.34, 42 MeV; calculated breakup and reaction σ(E), angular-momentum distribution of the breakup cross sections; deduced nuclear and Coulomb contributions. Continuum Discretized Coupled Channel (CDCC) method.
doi: 10.1103/PhysRevC.95.014604
2016DE07 Phys.Rev. C 93, 034616 (2016) Low-energy 6He scattering in a microscopic model NUCLEAR REACTIONS 27Al(6He, 6He), E=9.64, 11, 12, 13.4 MeV; 58Ni(6He, 6He), E=12.2, 16.5, 21.7 MeV; 120Sn(6He, 6He), E=17.4, 18.05, 19.8, 20.5 MeV; 208Pb(6He, 6He), E=18, 22, 27 MeV; calculated σ(E), and σ(θ) for 6He+208Pb system considering 6He halo nucleus as an α+n+n three-cluster system; investigated breakup effects, optical potentials, and polarization effects. Continuum discretized coupled channel (CDCC) method. Comparison with experimental data.
doi: 10.1103/PhysRevC.93.034616
2016PI12 Phys.Rev. C 94, 024620 (2016) Coulomb breakup of 22C in a four-body model NUCLEAR REACTIONS 208Pb(22C, X), E=240 MeV/nucleon; calculated three-body 20C+n+n eigenphases for 1-, 0+ and 2+ resonances, breakup cross sections with different 20C+n potentials, E1 strengths distributions using a four-body eikonal model; predicted a 2+ narrow resonance between 0.5 and 1 MeV.
doi: 10.1103/PhysRevC.94.024620
2016SU25 Phys.Rev. C 94, 054607 (2016) H.Suno, Y.Suzuki, P.Descouvemont Precise calculation of the triple-α reaction rates using the transmission-free complex absorbing potential method NUCLEAR REACTIONS 12C(γ, 3α); calculated photodissociation σ(Eγ) as function of 3α energy, energy-averaged triple-α reaction rate as a function of temperature T=0.01 to 1 GK, adjusted and 3α-model triple-α reaction rates as functions of temperature T=1-10 GK. Solution of Schrodinger equation for three α particles using the modified Smith-Whitten hyperspherical coordinates and a complex absorbing potential. Comparison with CDCC and HHR theoretical approaches, and with the rates in NACRE database. NUCLEAR STRUCTURE 12C; calculated energies, rms radii, B(E2), E0 strengths for the first two 0+ and first 2+ states using angular-momentum-independent α-α potential and three-body potentials to reproduce the energies of both the Hoyle state and the first 2+ state. Comparison with other theoretical calculations, and with experimental values.
doi: 10.1103/PhysRevC.94.054607
2015DE04 Phys.Rev. C 91, 024606 (2015) P.Descouvemont, T.Druet, L.F.Canto, M.S.Hussein Low-energy 9Be 208Pb scattering, breakup, and fusion within a four-body model NUCLEAR STRUCTURE 9Be; calculated electric quadrupole moment, magnetic dipole moment, rms radius, B(E2), pseudostates using the hyperspherical coordinate method for α+α+n three-body model. Comparison with experimental data. NUCLEAR REACTIONS 208Pb(9Be, 9Be), (9Be, X), E=38, 50 MeV; calculated elastic scattering σ(θ), fusion σ, breakup σ using continuum discretized coupled channel method. Comparison with experimental data.
doi: 10.1103/PhysRevC.91.024606
2015FE02 Phys.Rev. C 91, 024307 (2015) B.Fernandez-Dominguez, X.Pereira-Lopez, N.K.Timofeyuk, P.Descouvemont, W.N.Catford, F.Delaunay Spectroscopic study of the exotic nucleus 25P NUCLEAR STRUCTURE 25P, 25Ne; calculated levels, J, π, spectroscopic factors, ANCs from (d, p) transfer, partial gamma and proton widths. Proposed possible experiments to investigate levels in unbound 25P nucleus, and searches of the mirror analog of the island of inversion near N=16. Shell model, a potential model, and a microscopic-cluster model. Comparison with experimental data for 25Ne.
doi: 10.1103/PhysRevC.91.024307
2015SU03 Phys.Rev. C 91, 014004 (2015) H.Suno, Y.Suzuki, P.Descouvemont Triple-α continuum structure and Hoyle resonance of 12C using the hyperspherical slow variable discretization NUCLEAR STRUCTURE 12C; calculated levels, J, π, bound and continuum energy spectra, energy of the second 0+ (Hoyle) state, ten lowest adiabatic hyperspherical potential curves, and contour plots of the 2D probability density functions of the three-α system for Jπ=0+ and 2+. Calculations based on 3α-particle model, the three particles interacting through both short-range and Coulomb potentials. 8Be; calculated resonance parameters with Legendre polynomial basis.
doi: 10.1103/PhysRevC.91.014004
2015TU03 Phys.Atomic Nuclei 78, 193 (2015) E.M.Tursunov, S.A.Turakulov, P.Descouvemont Theoretical analysis of the astrophysical S-factor for the capture reaction α+d → 6Li + γ in the two-body model NUCLEAR REACTIONS 2H(α, γ), E<12 MeV; analyzed available data; deduced S-wave phase shifts, Contributions of E1, E2, and E1+E2 transitions to the astrophysical S-factor, theoretical estimate for reaction rates.
doi: 10.1134/S1063778815010196
2014CH06 J.Phys.(London) G41, 035101 (2014) L.C.Chamon, L.R.Gasques, L.F.M.Alves, V.Guimaraes, P.Descouvemont, R.J.de Boer, M.Wiescher Effect of the inelastic couplings on the scattering of alpha particles by 12C at low energies NUCLEAR REACTIONS 12C(α, α), (α, X)16O, E=7.85-10.42 MeV; analyzed available data, σ and S-factors; deduced the effect of the coupling of the first 2+ state in 12C.
doi: 10.1088/0954-3899/41/3/035101
2014DU05 Nucl.Phys. A927, 134 (2014) 12C(0+2) + α molecular states in a microscopic four α model NUCLEAR STRUCTURE 20O; calculated molecular states, resonances using four α multicluster model applied to 12C+α combined with microscopic R-matrix; deduced 0+ states energy spectra, α reduced widths for 0+, 2+, 4+ resonances. Compared with available data.
doi: 10.1016/j.nuclphysa.2014.04.010
2014GR12 Phys.Rev. C 90, 034616 (2014) J.Grineviciute, P.Descouvemont Elastic scattering of 17F, 17O, and 19F on a heavy target in a microscopic continuum discretized coupled-channels method NUCLEAR REACTIONS 58Ni(17O, 17O), E=55 MeV; 58Ni(17F, 17F), E=58.5, 170 MeV; 208Pb(p, p), E=11 MeV; 208Pb(n, n), E=5.5, 10 MeV; 208Pb(17O, 17O), E=78 MeV; 208Pb(17F, 17F), E=90.4, 98, 170 MeV; 208Pb(19F, 19F), E=91, 102 MeV; analyzed data for Differential elastic σ(E, θ) using microscopic continuum discretized coupled-channels (MCDCC) method with solution of Coupled equations by R-matrix method on a Lagrange mesh. Dependence on the choice of effective NN interaction.
doi: 10.1103/PhysRevC.90.034616
2014MO35 Nucl.Instrum.Methods Phys.Res. A767, 359 (2014) D.J.Mountford, R.J.de Boer, P.Descouvemont, A.St.J.Murphy, E.Uberseder, M.Wiescher Evaluation of the implementation of the R-matrix formalism with reference to the astrophysically important 18F(pα)15O reaction NUCLEAR REACTIONS 18F(p, α), E(cm)=0.6-1.6 MeV; calculated resonance parameter widths, σ(θ), S-factors. R-matrix formalism, AZURE code.
doi: 10.1016/j.nima.2014.08.047
2014PI02 Phys.Rev. C 89, 054615 (2014) Microscopic description of 7Li in 7Li + 12C and 7LI + 28Si elastic scattering at high energies NUCLEAR REACTIONS 12C, 28Si(7Li, 7Li), (7Li, 7Li'), E=350 MeV; calculated CDCC elastic, breakup in α+t, and eikonal-CDCC σ(θ). Comparison between CDCC and eikonal-CDCC σ(θ). Microscopic continuum-discretized coupled-channels reaction framework (MCDCC). Comparison with experimental data.
doi: 10.1103/PhysRevC.89.054615
2013AS06 Phys.Lett. B 723, 355 (2013) Role of the Hoyle state in 12C + 12C fusion NUCLEAR REACTIONS 12C(12C, X)24Mg, E(cm)=26 MeV; calculated σ(θ), S factors, energy levels, J, π. Multichannel folding model, using the density-dependent DDM3Y nucleon-nucleon interaction, comparison with available data.
doi: 10.1016/j.physletb.2013.05.030
2013DE26 Phys.Rev.Lett. 111, 082701 (2013) Towards a Microscopic Description of Reactions Involving Exotic Nuclei NUCLEAR REACTIONS 208Pb(7Li, 7Li), (7Li, 7Li'), E=27, 35 MeV; calculated σ(θ). Microscopic generalization of the continuum discretized coupled channels method, comparison with available data.
doi: 10.1103/PhysRevLett.111.082701
2012AR10 Prog.Theor.Phys.(Kyoto), Suppl. 196, 483 (2012) K.Arai, S.Aoyama, Y.Suzuki, P.Descouvemont, D.Baye Tensor Force Manifestations in Ab Initio Study of the 2H(d, γ)4He, 2H(d, p)3H, and 2H(d, n)3He Reactions NUCLEAR REACTIONS 2H(d, γ)4He, 2H(d, p)3H, 2H(d, n)3He, E(cm)<10 MeV; calculated S-factors. Extended microscopic cluster model with realistic nucleon-nucleon interaction, comparison with available data.
doi: 10.1143/PTPS.196.483
2012DE23 Prog.Theor.Phys.(Kyoto), Suppl. 196, 1 (2012) P.Descouvemont, E.Pinilla, D.Baye Comparative Study of Three-Body Models for Continuum States NUCLEAR STRUCTURE 6He; calculate dipole strength distributions, phase shifts, B(E1). Complex scaling method, R-matrix calculations.
doi: 10.1143/PTPS.196.1
2012DR10 Eur.Phys.J. A 48, 147 (2012) Continuum effects in the scattering of exotic nuclei NUCLEAR REACTIONS 64Zn(11Be, 11Be), (11Be, 11Be'), (11Be, n10Be), E(cm)=20.5, 24.5, 44.5 MeV; calculated scattering σ(θ), breakup σ(k) using CDCC; deduced high angular momenta. Compared with data.
doi: 10.1140/epja/i2012-12147-9
2012ME11 Phys.Rev. C 86, 064321 (2012), Erratum Phys.Rev. C 98, 069901 (2018) D.R.Mendes, A.Lepine-Szily, P.Descouvemont, R.Lichtenthaler, V.Guimaraes, P.N.de Faria, A.Barioni, K.C.C.Pires, V.Morcelle, R.P.Condori, M.C.Morais, E.Leistenschneider, C.E.F.Lima, J.C.Zamora, J.A.Alcantara, V.Zagatto, M.Assuncao, J.M.B.Shorto The 8Li(p, α)5He reaction at low energies, and 9Be spectroscopy around the proton threshold NUCLEAR REACTIONS 1H(8Li, α), [secondary 8Li beam from 9Be (7Li, 8Li), E=16-22 MeV primary reaction], E=13.2, 14.5, 17.0, 19.0 MeV; measured particle spectra, differential σ(E). 9Be; deduced proton resonances, levels, J, π, isospin, widths. Three-body and sequential decays. R-matrix analysis. Comparison with previous experimental results. 8Li(p, α)5He; deduced integrated σ, astrophysical S factor and reaction rates.
doi: 10.1103/PhysRevC.86.064321
2012MO03 Phys.Rev. C 85, 022801 (2012) D.J.Mountford, A.StJ.Murphy, N.L.Achouri, C.Angulo, J.R.Brown, T.Davinson, F.de Oliveira Santos, N.de Sereville, P.Descouvemont, O.Kamalou, A.M.Laird, S.T.Pittman, P.Ujic, P.J.Woods Resonances in 19Ne with relevance to the astrophysically important 18F(p, α)15O reaction NUCLEAR REACTIONS 1H(18F, α), (18F, p), [secondary 18F beam from C(20Ne, X), E=95 MeV/nucleon primary reaction], E(cm)=0.5-1.9 MeV; measured particle spectra, time of flight, differential cross sections at GANIL-SPIRAL facility. 19Ne; deduced resonance energies, J, π, α and proton partial widths, covariance matrix, astrophysical S factor for 18F(p, α)15O reaction. R-matrix analysis. Astrophysical implications. Comparison with previous experimental results.
doi: 10.1103/PhysRevC.85.022801
2012OU01 Phys.Rev. C 85, 035804 (2012) N.Oulebsir, F.Hammache, P.Roussel, M.G.Pellegriti, L.Audouin, D.Beaumel, A.Bouda, P.Descouvemont, S.Fortier, L.Gaudefroy, J.Kiener, A.Lefebvre-Schuhl, V.Tatischeff Indirect study of the 12C(α, γ)16O reaction via the 12C(7Li, t)16O transfer reaction NUCLEAR REACTIONS 12C(7Li, t)16O, E=28, 34 MeV; measured E(t), I(t), σ(θ) using Enge split-pole magnetic spectrometer; deduced levels, J, π, yields, width, spectroscopic factors, ANC, α-reduced width. HF+FR-DWBA analysis of σ(θ) data. 12C(α, α'), E(cm)=1-5 MeV; analyzed data by R-matrix analysis; deduced E2 and E1 components. 12C(α, γ)16O, E(cm)=0.3-3.5 MeV; deduced astrophysical S factor with R-matrix calculations of the E2 and E1 components. Comparison with earlier results and NACRE evaluation. RADIOACTIVITY 16N(β-); analyzed β-delayed α spectrum by R-matrix fit for validation purpose.
doi: 10.1103/PhysRevC.85.035804
2012PI10 Phys.Rev. C 85, 054610 (2012) E.C.Pinilla, P.Descouvemont, D.Baye Three-body breakup of 11Li with the eikonal method NUCLEAR REACTIONS 208Pb(11Li, X), E=70 MeV/nucleon; calculated B(E1) strength distribution, total breakup σ(E), double differential σ(θ), total σ(θ), R-matrix method. Coulomb-corrected eikonal approximation, hyperspherical formalism. 208Pb(11Li, 11Li), (9Li, 9Li), E=70 MeV/nucleon; calculated σ(θ) in four-body eikonal model for 11Li and two-body eikonal model for 9Li. Comparison with experimental data.
doi: 10.1103/PhysRevC.85.054610
2012TI03 Phys.Rev. C 86, 034305 (2012) N.K.Timofeyuk, B.Fernandez-Dominguez, P.Descouvemont, W.N.Catford, F.Delaunay, J.S.Thomas Core excitations and narrow states beyond the proton dripline: The exotic nucleus 21Al NUCLEAR STRUCTURE 21Al; calculated levels, resonances, J, π, widths with respect to 20Mg+p channel and asymptotic normalization coefficients (ANC) for mirror states in 21O using multichannel and single-channel microscopic cluster model (MCM), and in two versions of the potential model. 21O; calculated levels, J, π, asymptotic normalization coefficients (ANC), spectroscopic factors using MCM; compared with experimental data for 20O(d, p)21O reaction.
doi: 10.1103/PhysRevC.86.034305
2011AO01 Int.J.Mod.Phys. E20, 775 (2011) S.Aoyama, K.Arai, P.Descouvemont, Y.Suzuki, D.Baye Extended microscopic cluster model study of four nucleon scattering
doi: 10.1142/S0218301311018654
2011AR12 Phys.Rev.Lett. 107, 132502 (2011) K.Arai, S.Aoyama, Y.Suzuki, P.Descouvemont, D.Baye Tensor Force Manifestations in Ab Initio Study of the 2H(d, γ)4He, 2H(d, p)3H, and 2H(d, n)3He Reactions NUCLEAR REACTIONS 2H(d, γ), (d, p), (d, n), E(cm)<10 MeV; calculated wave functions, phase shifts, σ, S-factors. Multichannel microscopic cluster model, ab initio calculations, comparison with experimental data.
doi: 10.1103/PhysRevLett.107.132501
2011DA10 Int.J.Mod.Phys. E20, 819 (2011) Microscopic study of three-body scattering states
doi: 10.1142/S0218301311018757
2011DU01 Phys.Lett. B 696, 237 (2011) Low-lying resonances in the 16B nucleus NUCLEAR STRUCTURE 15,16B; calculated energy of low-lying states, J, π, wave functions, total widths. Generator coordinate method.
doi: 10.1016/j.physletb.2010.12.032
2011DU11 Int.J.Mod.Phys. E20, 393 (2011) Microscopic cluster models NUCLEAR STRUCTURE 12Be; calculated cluster states. NUCLEAR REACTIONS 12C(α, γ), E(cm)<4 Mev; calculated S-factors.
doi: 10.1142/S0218301311017776
2011DU16 Int.J.Mod.Phys. E20, 1022 (2011) Multichannel analysis of the 16B nucleus NUCLEAR STRUCTURE 16B; calculated energy levels, J, π, eigenphaseshift. GCM calculations, comparison with experimental data.
doi: 10.1142/S0218301311019180
2011PI10 Nucl.Phys. A865, 43 (2011) E.C.Pinilla, D.Baye, P.Descouvemont, W.Horiuchi, Y.Suzuki Tests of the discretized-continuum method in three-body dipole strengths NUCLEAR STRUCTURE 6He; calculated B(E1), halo structure. α+n+n model, R-matrix, discrete-continuum method, pseudostate method.
doi: 10.1016/j.nuclphysa.2011.06.030
2011SF01 Int.J.Mod.Phys. E20, 831 (2011) C.Sfienti, G.Raciti, P.Capel, D.Baye, M.De Napoli, F.Giacoppo, E.Rapisarda, G.Cardella, P.Descouvemont, J.-M.Sparenberg, C.Mazzocchi 17F breakup reactions: A touchstone for indirect measurements
doi: 10.1142/S0218301311018782
2011SF02 J.Phys.:Conf.Ser. 312, 042022 (2011) C.Sfienti, G.Raciti, P.Capel, D.Baye, M.De Napoli, F.Giacoppo, E.Rapisarda, G.Cardella, P.Descouvemont, C.Mazzocchi, J.-M.Sparenberg 17F breakup reactions: A touchstone for indirect measurements NUCLEAR REACTIONS Pb(17F, p16O), E=40 MeV/nucleon;measured reaction fragments using Si-strip detector; deduced breakup unnormalized σ(Erelative); calculated breakup σ(Erelative).
doi: 10.1088/1742-6596/312/4/042022
2011TU07 Int.J.Mod.Phys. E20, 803 (2011) E.M.Tursunov, D.Baye, P.Descouvemont Theoretical study of the 11Li β decay into the deuteron channel in a cluster model RADIOACTIVITY 11Li(β-), (d); calculated transition probabilities, phase shifts.
doi: 10.1142/S021830131101871X
2010AD02 J.Phys.(London) G37, 045102 (2010) Three-body structure of 18Ne in a microscopic model NUCLEAR STRUCTURE 18Ne, 18O; analyzed spectroscopy of low-lying states; deduced the resonance width. Analytical Continuation in the Coupling Constant (ACCC).
doi: 10.1088/0954-3899/37/4/045102
2010BA44 Phys.Rev. C 82, 054318 (2010) D.Baye, P.Descouvemont, E.M.Tursunov Unique decay process: β-delayed emission of a proton and a neutron by the 11Li halo nucleus RADIOACTIVITY 11Li(β-pn); calculated branching ratio, probable total energies of emitted neutron and proton with Coulomb three-body final scattering states. Theoretical formulas for the Fermi and Gamow-Teller transitions leading to three-body final states.
doi: 10.1103/PhysRevC.82.054318
2010DE07 Phys.Rev. C 81, 029803 (2010) P.Descouvemont, M.Dufour, J.-M.Sparenberg Comment on "Low-energy cross sections in the 12C(α, γ)16O reaction" NUCLEAR REACTIONS 12C(α, γ)16O; analyzed σ, E1 and E2 S factors. Discussed validity of potential model.
doi: 10.1103/PhysRevC.81.029803
2010DE13 Phys.Rev. C 81, 039802 (2010) N.de Sereville, C.Angulo, A.Coc, N.L.Achouri, E.Casarejos, T.Davinson, P.Descouvemont, P.Figuera, S.Fox, F.Hammache, J.Kiener, A.Laird, A.Lefebvre-Schuhl, P.Leleux, P.Mumby-Croft, N.A.Orr, I.Stefan, K.Vaughan, V.Tatischeff Reply to "Comment on 'Low-energy 18F(p, α)15O cross section measurements relevant to nova γ-ray emission' " NUCLEAR REACTIONS 18F(p, α)15O, E(cm)=0-1 MeV; analyzed astrophysical S factors and sign of interference terms.
doi: 10.1103/PhysRevC.81.039802
2010DR06 Nucl.Phys. A845, 88 (2010) T.Druet, D.Baye, P.Descouvemont, J.-M.Sparenberg CDCC calculations with the Lagrange-mesh technique NUCLEAR REACTIONS 58Ni(d, d), (d, X), E=80 MeV; calculated elastic and breakup σ(θ) using Lagrange-mesh technique with continuum discretized coupled-channel model. Comparison with data normalized to Rutherford σ.
doi: 10.1016/j.nuclphysa.2010.04.058
2010DU08 Nucl.Phys. A836, 242 (2010) M.Dufour, P.Descouvemont, F.Nowacki Microscopic investigation of the 12Be spectroscopy NUCLEAR STRUCTURE 12Be; calculated levels, J, π, B(E2), widths. Comparison of Generator Coordinate Method (GCM) and no-core shell model (NCSM) with experimental data.
doi: 10.1016/j.nuclphysa.2010.02.002
2010GE08 J.Phys.:Conf.Ser. 202, 012015 (2010) G.Genard, P.Descouvemont, G.Terwagne S-factor measurement of the 13C(p, γ)14N reaction in reverse kinematics NUCLEAR REACTIONS 1H(13C, γ), E=3200-7900 keV; measured Eγ, Iγ around 511 keV resonance; deduced S-factor, resonance parameters; calculated S-factor using R-matrix. Compared with other results.
doi: 10.1088/1742-6596/202/1/012015
2010LE14 Nucl.Phys. A834, 491c (2010) A.Lepine-Szily, R.Lichtenthaler, V.Guimaraes, D.R.Mendes, Jr, P.N.de Faria, A.Barioni, E.A.Benjamim, K.C.C.Pires, V.Morcelle, R.P.Condori, M.C.Morais, P.Descouvemont, A.M.Moro, M.Rodriguez Gallardo, M.M.Assuncao, J.A.Alcantara Nunez, J.M.B.Shorto, J.C.Zamora, E.Leistenschneider, C.E.F.Lima Scientific program of the Radioactive Ion Beams Facility in Brasil (RIBRAS) NUCLEAR REACTIONS 1H(8Li, α), E=13.2, 14.5, 17.4, 19.0 MeV; measured Eα, Iα(θ=forward); deduced σ(θ=forward), effect of halo nuclei. 9Be(6He, 6He), E=16.2 MeV; measured σ(θ); deduced effect of halo nuclei.
doi: 10.1016/j.nuclphysa.2010.01.074
2010PI08 Nucl.Phys. A834, 499c (2010) High-energy α-nucleus scattering with microscopic wave functions NUCLEAR REACTIONS 58Ni, 208Pb(α, α), E=288 MeV; calculated σ(θ) using an eikonal approximation. Comparison with data.
doi: 10.1016/j.nuclphysa.2010.01.076
2010TI02 Phys.Rev. C 81, 051301 (2010) Narrow states in the three-proton emitter 17Na NUCLEAR STRUCTURE 16C, 16Ne, 17C, 17Na; calculated levels, J, π, spectroscopic factors using microscopic cluster model calculations. Comparison with shell model calculations and experimental data. RADIOACTIVITY 17Na(p), (3p); calculated Ep, widths using microscopic cluster model calculations. Sequential three-proton decay via intermediate states in 16Ne. Comparison with shell model calculations experimental data.
doi: 10.1103/PhysRevC.81.051301
2009BA07 Phys.Rev. C 79, 024607 (2009) D.Baye, P.Capel, P.Descouvemont, Y.Suzuki Four-body calculation of 6He breakup with the Coulomb-corrected eikonal method NUCLEAR REACTIONS 208Pb(6He, X), E=70, 240 MeV/nucleon; calculated E1 strength functions, total and partial cross section using Coulomb corrected eikonal method and breakup of 6He halo nucleus treated as 3 body α+n+n model. $Comparison with experimental data.
doi: 10.1103/PhysRevC.79.024607
2009DA17 Phys.Rev. C 80, 044310 (2009) Three-body continuum states in a microscopic cluster model NUCLEAR STRUCTURE 6He; calculated energy dependence of α+n+n eigenphases for 0+, 1- and 2+ states with the application of R-matrix theory to a microscopic cluster model for three-body continuum states in the hyperspherical formalism.
doi: 10.1103/PhysRevC.80.044310
2009DE03 Phys.Rev. C 79, 015801 (2009) N.De Sereville, C.Angulo, A.Coc, N.L.Achouri, E.Casarejos, T.Davinson, P.Descouvemont, P.Figuera, S.Fox, F.Hammache, J.Kiener, A.Laird, A.Lefebvre-Schuhl, P.Leleux, P.Mumby-Croft, N.A.Orr, I.Stefan, K.Vaughan, V.Tatischeff Low-energy 18F(p, α)15O cross section measurements relevant to nova γ-ray emission NUCLEAR REACTIONS 1H(18F, α), E=13.8 MeV; measured (particle)-(particle) coin, σ, σ(θ); deduced S-factor. Comparison with R-matrix calculations.
doi: 10.1103/PhysRevC.79.015801
2009DE08 Phys.Rev. C 79, 024605 (2009) A.S.Denikin, V.I.Zagrebaev, P.Descouvemont Generalized optical potential for weakly bound nuclei: Two-cluster projectiles NUCLEAR REACTIONS 12C(d, d), E=56 MeV; calculated cross section, S matrices, weighted local polarization potential, deuteron survival probability and deflection function. 12C(d, np), E=56 MeV; calculated correlation angle between protons and neutrons and energy spectrum of protons in coincidence with neutrons for elastic scattering. 58Ni(d, d), E=80 MeV; 120Sn(d, d), E=85 MeV; 208Pb(d, d), E=110 MeV; calculated cross sections. Feshbach projection operator method for generalized optical potential calculations. Comparison with experimental data.
doi: 10.1103/PhysRevC.79.024605
2009MU07 Phys.Rev. C 79, 058801 (2009) A.St.J.Murphy, A.M.Laird, C.Angulo, L.Buchmann, T.Davinson, P.Descouvemont, S.P.Fox, J.Jose, R.Lewis, C.Ruiz, K.Vaughan, P.Walden Simultaneous measurement of the 18F(p, p)18F and 18F(p, α)15O reactions: Implications for the level structure of 19Ne, and for 18F production in novae NUCLEAR REACTIONS 1H(18F, α), (18F, p), E=1.750 MeV/nucleon; measured particle spectra, σ. 19Ne; deduced levels, J, π, resonances, α widths, proton widths. R-matrix analysis. 18F(p, α)15O; deduced reaction rates.
doi: 10.1103/PhysRevC.79.058801
2008AD16 Nucl.Phys. A813, 252 (2008) Microscopic cluster model of 5H and 5He (T = 3/2) NUCLEAR STRUCTURE 5H, 5He; calculated levels, cluster configurations. Microscopic three cluster model with hyperspherical formalism. Comparison with other models.
doi: 10.1016/j.nuclphysa.2008.09.008
2008DE07 J.Phys.(London) G35, 014006 (2008) Cluster models in nuclear astrophysics NUCLEAR REACTIONS 12C(α, γ)16O, E(cm)=0-4 MeV; analyzed S-factor using cluster model. Review of cluster models used in nuclear astrophysics.
doi: 10.1088/0954-3899/35/1/014006
2008DE36 Int.J.Mod.Phys. E17, 2165 (2008) Cross sections for nuclear astrophysics
doi: 10.1142/S0218301308011288
2008DE38 Int.J.Mod.Phys. E17, 2326 (2008) A.S.Denikin, V.I.Zagrebaev, P.Descouvemont Generalized optical potential of light weakly bound cluster nuclei NUCLEAR REACTIONS 12C(6He, X), E=230MeV; calculated elastic σ. Continuum-Discretized Couples Channel (CDCC) method.
doi: 10.1142/S0218301308011550
2008DU14 Phys.Rev. C 78, 015808 (2008) 12C(α, γ)16O E2 cross section: R-matrix fits combined with a microscopic cluster model NUCLEAR REACTIONS 12C(α, γ); calculated S-factors, E2 component of σ. Microscopic cluster model, R-matrix fits. 16O; calculated B(E2), widths of excited states. Comparison with experimental data.
doi: 10.1103/PhysRevC.78.015808
2008DU22 Int.J.Mod.Phys. E17, 2176 (2008) Theoretical investigations of the 12C(α, γ)16O E2 cross section NUCLEAR REACTIONS 12C(α, γ), E=300 keV; calculated s-factors.
doi: 10.1142/S0218301308011306
2008IL02 Phys.Rev. C 77, 045802 (2008) C.Iliadis, C.Angulo, P.Descouvemont, M.Lugaro, P.Mohr New reaction rate for 16O(p, γ)17F and its influence on the oxygen isotopic ratios in massive AGB stars NUCLEAR REACTIONS 16O(p, γ), E<3.5 MeV; evaluated σ, deduced astrophysical S-factor, reaction rate. Compared with rate of 17O(p, α) reaction.
doi: 10.1103/PhysRevC.77.045802
2008PE02 Phys.Lett. B 659, 864 (2008) M.G.Pellegriti, N.L.Achouri, C.Angulo, J.-C.Angelique, E.Berthoumieux, E.Casarejos, M.Couder, T.Davinson, C.Ghag, A.St.Murphy, N.A.Orr, I.Ray, I.G.Stefan, P.Descouvemont Evidence for core excitation in single-particle states of 19Na NUCLEAR REACTIONS 1H(18Ne, 18Ne), (18Ne, 18Ne'), E=66 MeV; measured σ(θ), proton spectra. 19Na deduced levels, J, π. Microscopic cluster model and R-matrix analysis.
doi: 10.1016/j.physletb.2007.12.017
2008PE09 Phys.Rev. C 77, 042801 (2008) M.G.Pellegriti, F.Hammache, P.Roussel, L.Audouin, D.Beaumel, P.Descouvemont, S.Fortier, L.Gaudefroy, J.Kiener, A.Lefebvre-Schuhl, M.Stanoiu, V.Tatischeff, M.Vilmay Indirect study of the 13C(α, n)16O reaction via the 13C(7Li, t)17O transfer reaction NUCLEAR REACTIONS 13C(7Li, t), (7Li, 7Li), E=28, 34 MeV; measured σ(θ). 17O; deduced levels, J, α spectroscopic factors, asymptotic normalization factors. 12C(7Li, t), (7Li, 7Li), E=28 MeV; measured yields. 13C(α, n); deduced astrophysical S-factor, reaction rates. Comparison with recommended values. DWBA analysis.
doi: 10.1103/PhysRevC.77.042801
2008SU01 Phys.Lett. B 659, 160 (2008) Y.Suzuki, H.Matsumura, M.Orabi, Y.Fujiwara, P.Descouvemont, M.Theeten, D.Baye Local versus nonlocal αα interactions in a 3α description of 12C NUCLEAR STRUCTURE 12C; calculated ground and excited 0+ states energies, radii. α-cluster model with non-local forces.
doi: 10.1016/j.physletb.2007.10.033
2008TI07 Phys.Rev. C 78, 044323 (2008) N.K.Timofeyuk, P.Descouvemont, I.J.Thompson Threshold effects in the 27P(3/2+) → 26Si + p and 27Mg(3/2+) → 26Mg + n mirror decays and the stellar reaction 26Si(p, γ)27P NUCLEAR REACTIONS 26Mg(t, d), E=36 MeV; analyzed cross sections, ANCs; 26Si(p, γ); deduced astrophysical S-factors. NUCLEAR STRUCTURE 27Mg, 27P; calculated resonance energies, widths, particle separation energies. Shell model calculations.
doi: 10.1103/PhysRevC.78.044323
2007DE61 Eur.Phys.J. Special Topics 150, 211 (2007) N.de Sereville, C.Angulo, A.Coc, N.L.Achouri, E.Casarejos, T.Davinson, P.Descouvemont, P.Figuera, S.Fox, F.Hammache, J.Kiener, A.Laird, A.Lefebvre, P.Leleux, P.Mumby-Croft, N.Orr, D.Robertson, K.Vaughan, V.Tatischeff New low-energy measurement of the 18F(p, α)15O reaction NUCLEAR REACTIONS 1H(18F, α), E=13.8 MeV; measured Eα, Iα, cross sections.
doi: 10.1140/epjst/e2007-00306-5
2007DU09 Nucl.Phys. A785, 381 (2007) The 18F(p, α)15O low-energy S-factor: A microscopic approach NUCLEAR REACTIONS 18F(p, α), E(cm)=0-1.5 MeV; calculated S-factors. 18F(p, p), E(cm)=0-2 MeV; calculated σ(θ=180°). Microscopic cluster model, generator coordinate method, comparison with data. NUCLEAR STRUCTURE 19F, 19Ne; calculated levels, J, π. Microscopic cluster model, generator coordinate method.
doi: 10.1016/j.nuclphysa.2006.12.101
2007TH16 Phys.Rev. C 76, 054003 (2007) M.Theeten, H.Matsumura, M.Orabi, D.Baye, P.Descouvemont, Y.Fujiwara, Y.Suzuki Three-body model of light nuclei with microscopic nonlocal interactions NUCLEAR STRUCTURE 6He, 9Be, 12C; calculated potential functions, phase shifts, charge densities, neutron densities. Compared to experimental energies.
doi: 10.1103/PhysRevC.76.054003
2007TI02 Phys.Rev. C 75, 034302 (2007) N.K.Timofeyuk, P.Descouvemont, R.C.Johnson Isospin symmetry in mirror α decays NUCLEAR STRUCTURE 7Li, 7Be, 11B, 11C, 19F, 19Ne; calculated mirror states asymptotic normalization coefficients, α resonance widths.
doi: 10.1103/PhysRevC.75.034302
2007TU05 Nucl.Phys. A793, 52 (2007) E.M.Tursunov, P.Descouvemont, D.Baye Gamma-delayed deuteron emission of the 6Li(0+; T = 1) halo state NUCLEAR STRUCTURE 6Li; calculated 3-body wave functions, widths, radii, μ, B(M1). Transition probabilities for decay to α+d continuum. Three-body model, comparison with data.
doi: 10.1016/j.nuclphysa.2007.06.002
2006AD22 Phys.Lett. B 639, 447 (2006) Core excitations in 8He and 7He NUCLEAR STRUCTURE 7,8He; calculated levels, cluster configurations. Microscopic three cluster model.
doi: 10.1016/j.physletb.2006.05.092
2006BA73 Phys.Rev.C 74, 064302 (2006) D.Baye, E.M.Tursunov, P.Descouvemont β decay of 11Li into 9Li and a deuteron within a three-body model NUCLEAR STRUCTURE 11Li; calculated transition probabilities for β-decay to 9Li+d channel. Three-body model, comparison with data.
doi: 10.1103/PhysRevC.74.064302
2006CA05 Phys.Rev. C 73, 014319 (2006) E.Casarejos, C.Angulo, P.J.Woods, F.C.Barker, P.Descouvemont, M.Aliotta, T.Davinson, P.Demaret, M.Gaelens, P.Leleux, Z.Liu, M.Loiselet, A.S.Murphy, A.Ninane, I.A.Roberts, G.Ryckewaert, J.S.Schweitzer, F.Vanderbist Low-lying states in the unbound 11N nucleus NUCLEAR REACTIONS 1H(10C, p), E=25.5, 32 MeV; measured recoil Ep, elastic σ(θ). 11N deduced resonance parameters. 12O deduced two-proton decay width.
doi: 10.1103/PhysRevC.73.014319
2006DE02 Nucl.Phys. A765, 370 (2006) P.Descouvemont, E.Tursunov, D.Baye Three-body continuum states on a Lagrange mesh NUCLEAR STRUCTURE 6He, 6Be; calculated level energies, widths, radii, B(E2). 14Be; calculated level energies, radii, B(E2), wave function. Three-body unbound systems, Lagrange mesh technique.
doi: 10.1016/j.nuclphysa.2005.11.010
2006DE47 Nucl.Phys. A777, 137 (2006) Cross section predictions for hydrostatic and explosive burning NUCLEAR REACTIONS 14N(p, γ), E(cm)=0-2.5 MeV; 17F(p, γ), E(cm)=0.05-1.1 MeV; calculated astrophysical S-factor. Microscopic, R-matrix and other models described. Comparison with data.
doi: 10.1016/j.nuclphysa.2004.10.024
2006MO29 Eur.Phys.J. A 27, Supplement 1, 75 (2006) P.Mohr, C.Angulo, P.Descouvemont, H.Utsunomiya Relation between the 16O(α, γ)20Ne reaction and its reverse 20Ne(γ, α)16O reaction in stars and in the laboratory NUCLEAR REACTIONS 16O(α, γ), 20Ne(γ, α), E=low; analyzed astrophysical reaction rates.
doi: 10.1140/epja/i2006-08-010-1
2006TH09 Phys.Rev. C 74, 044304 (2006) M.Theeten, D.Baye, P.Descouvemont Comparison of local, semi-microscopic, and microscopic three-cluster models NUCLEAR STRUCTURE 6He, 9Be, 12C; calculated ground- and excited-states energies, related features. Fully antisymmetrized microscopic three-cluster model, comparison of local and semi-microscopic approaches.
doi: 10.1103/PhysRevC.74.044304
2006TI05 Phys.Rev.Lett. 96, 162501 (2006) N.K.Timofeyuk, D.Baye, P.Descouvemont, R.Kamouni, I.J.Thompson 15C-15F Charge symmetry and the 14C(n, γ)15C Reaction Puzzle NUCLEAR REACTIONS 14C(n, γ), E ≈ 10-1000 keV; analyzed σ, asymptotic normalization coefficients, E1 component, charge symmetry features in 15C, 15F nucleon decay.
doi: 10.1103/PhysRevLett.96.162501
2006TI08 Eur.Phys.J. A 27, Supplement 1, 269 (2006) N.K.Timofeyuk, P.Descouvemont, R.C.Johnson Relation between proton and neutron asymptotic normalization coefficients for light mirror nuclei and its relevance for nuclear astrophysics
doi: 10.1140/epja/i2006-08-041-6
2006TU02 Phys.Rev. C 73, 014303 (2006); Erratum Phys.Rev. C 74, 069904 (2006) E.M.Tursunov, D.Baye, P.Descouvemont Analysis of the 6He β decay into the α + d continuum within a three-body model RADIOACTIVITY 6He(β-); calculated matrix elements, transition probabilities for decay to α+d continuum. Three-body model, comparison with data.
doi: 10.1103/PhysRevC.73.014303
2006VA06 Eur.Phys.J. A 27, 183 (2006) F.Vanderbist, P.Leleux, C.Angulo, E.Casarejos, M.Couder, M.Loiselet, G.Ryckewaert, P.Descouvemont, M.Aliotta, T.Davinson, Z.Liu, P.J.Woods A first experimental approach to the 15O + α elastic scattering NUCLEAR REACTIONS 4He(15O, 15O), E=12.5 MeV; measured recoil α spectrum. 19F deduced resonant state width.
doi: 10.1140/epja/i2005-10265-1
2005AD03 Eur.Phys.J. A 23, 435 (2005) A test of the zero-range DWBA method at astrophysical energies NUCLEAR REACTIONS 13C(α, n), E=0-5 MeV; calculated phase shifts, transition amplitudes. Comparison of DWBA and microscopic cluster model.
doi: 10.1140/epja/i2004-10113-x
2005BA73 Phys.Rev. C 72, 024309 (2005) Microscopic cluster model analysis of 14O+p elastic scattering NUCLEAR REACTIONS 14O(p, p), E=0.5-4 MeV; calculated σ(E, θ), excitation functions, phase shifts. 15F deduced resonance parameters. Microscopic cluster model, resonating group method, comparisons with data.
doi: 10.1103/PhysRevC.72.024309
2005CO07 Nucl.Phys. A752, 522c (2005) A.Coc, C.Angulo, E.Vangioni-Flam, P.Descouvemont, A.Adahchour Big Bang nucleosynthesis, microwave anisotropy, and the light element abundances
doi: 10.1016/j.nuclphysa.2005.02.057
2005CO16 Nucl.Phys. A758, 383c (2005) H.Costantini, C.Angulo, D.Bemmerer, R.Bonetti, C.Broggini, F.Confortola, P.Corvisiero, J.Cruz, P.Descouvemont, A.Formicola, Z.Fulop, G.Gervino, A.Guglielmetti, C.Gustavino, G.Gyurky, G.Imbriani, A.P.Jesus, M.Junker, A.Lemut, R.Menegazzo, P.Prati, V.Roca, C.Rolfs, M.Romano, C.Rossi Alvarez, F.Schumann, E.Somorjai, O.Straniero, F.Strieder, F.Terrasi, H.P.Trautvetter, A.Vomiero, S.Zavatarelli Recent results of the 14N(p, γ)15O measurement at LUNA NUCLEAR REACTIONS 14N(p, γ), E=low; measured Eγ, Iγ; deduced S-factors.
doi: 10.1016/j.nuclphysa.2005.05.069
2005DE46 Nucl.Phys. A758, 783c (2005) P.Descouvemont, A.Adahchour, C.Angulo, A.Coc, E.Vangioni-Flam Big-Bang reaction rates within the R-matrix model NUCLEAR REACTIONS 3He(d, p), E(cm) < 1 MeV; 7Li(p, α), E(cm)<10 MeV; 2H(p, γ), (d, n), (d, p), 3H(d, n), (α, γ), 3He(n, p), (α, γ), 7Be(n, p), E=low; analyzed astrophysical S-factors, reactions rates.
doi: 10.1016/j.nuclphysa.2005.05.140
2005DU03 Nucl.Phys. A750, 218 (2005) A new effective nucleon-nucleon interaction for microscopic cluster models NUCLEAR STRUCTURE 8Li, 11B, 10,13C, 13N, 14,15,16O, 17,18F; calculated levels, J, π; deduced parameters. Extended Volkov interaction, microscopic cluster model.
doi: 10.1016/j.nuclphysa.2004.12.041
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