NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = D.Baye Found 164 matches. Showing 1 to 100. [Next]2023BA38 Phys.Rev. C 108, 064610 (2023) Ambiguity of Siegert transformations for isospin-forbidden electric dipole transitions
doi: 10.1103/PhysRevC.108.064610
2020BA13 Phys.Rev. A 101, 022507 (2020) Quasibound states of an antiproton and a hydrogen atom ATOMIC PHYSICS H; calculated three-body quantal system composed of a proton, an antiproton, and an electron are performed in perimetric coordinates with the Lagrange-mesh method.
doi: 10.1103/PhysRevA.101.022507
2020HE12 Phys.Rev. C 101, 054609 (2020) Simplified dynamical eikonal approximation NUCLEAR REACTIONS 12C(11Be, X), E=67 MeV/nucleon; 208Pb(11Be, X), E=69 MeV/nucleon; calculated break-up σ as function of 10Be-n parallel momentum, Coulomb contribution to break-up σ; compared energy and parallel-momentum cross sections obtained with the dynamical eikonal approximation (DEA), the usual eikonal approximation (CCE), and the simplified dynamical eikonal approximation (S-DEA); developed Coulomb-corrected eikonal method (CCE) using the Coulomb first-order-perturbation approximation. Relevance to the nuclear structure of halo nuclei.
doi: 10.1103/PhysRevC.101.054609
2019GA27 Phys.Rev. C 100, 035805 (2019) D.Gaspard, J.-M.Sparenberg, Q.Wenda, D.Baye Complex-energy analysis of proton-proton fusion NUCLEAR REACTIONS 1H(p, e+ν)2H, E=0-5 MeV; calculated effective-range functions of the proton-proton 1S0 scattering for the Reid93 potential, correction functions for different potential models, linearized matrix element of the weak capture, three dimensional plots of model-independent parameterization Λ, bound state and resonance poles, astrophysical S factor for an energy range covering solar-core and early Universe temperatures.
doi: 10.1103/PhysRevC.100.035805
2018AO02 Phys.Rev. C 97, 054305 (2018) Ab initio study of the Jπ = 0± continuum structures in 4He NUCLEAR STRUCTURE 4He; calculated elastic phase shift and magnitudes of the S matrix, off diagonal part of the S matrix, and eigenphases of the t+p, 3He+n, and d+d channels in the continuum structure of 0+ and 0- states. Calculations performed using an ab initio reaction theory with the microscopic R-matrix method (MRM).
doi: 10.1103/PhysRevC.97.054305
2018AR03 Nucl.Phys. A977, 82 (2018) Analyzing supersymmetric transformed α-nucleus potentials with electric-multipole transitions NUCLEAR STRUCTURE 20Ne, 44Ti; calculated levels, J, null point-matter radius, γ decay widths, B(E2), B(E4) for individual transitions assuming nucleus treated as 16O+α (20Ne) and 40Ca+α (44Ti) using α-cluster model (and its generalizations) with three different α-nucleus potentials and using supersymmetric transformations to avoid redundant bound states. Compared with available data.
doi: 10.1016/j.nuclphysa.2018.06.004
2018BA25 J.Phys.(London) G45, 085102 (2018) Isospin-forbidden electric dipole capture and the α(d, γ)6Li reaction NUCLEAR REACTIONS 4He(d, γ), E<3 MeV; calculated S-factor using isovector E1 transitions involving small isospin-one admixtures in the wave functions. Comparison with experimental data.
doi: 10.1088/1361-6471/aacbfa
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
2014DO11 Phys.Rev. C 90, 034611 (2014) Comparison of potential models of nucleus-nucleus bremsstrahlung
doi: 10.1103/PhysRevC.90.034611
2013DO18 Phys.Rev. C 88, 024602 (2013) Siegert approach within a microscopic description of nucleus-nucleus bremsstrahlung NUCLEAR REACTIONS 4He(α, αγ)4He, E<24 MeV; calculated differential σ(E) for nuclear bremsstrahlung; comparison between Siegart and non-Siegart approaches. Microscopic cluster model of nucleus-nucleus bremsstrahlung. Comparison with experimental data.
doi: 10.1103/PhysRevC.88.024602
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
2012BA39 Phys.Rev. C 86, 034306 (2012) Extension of the Siegert theorem for photon emission
doi: 10.1103/PhysRevC.86.034306
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
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
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
2011BA01 Phys.Lett. B 696, 464 (2011) β delayed emission of a proton by a one-neutron halo nucleus RADIOACTIVITY 11Be, 19C, 31Ne(β-p); calculated decay probability for β-delayed proton emission as a function of separation energy.
doi: 10.1016/j.physletb.2010.12.069
2011BA21 Int.J.Mod.Phys. E20, 769 (2011) On the cluster-model description of collisions
doi: 10.1142/S0218301311018642
2011DO13 Phys.Rev. C 84, 014604 (2011) Microscopic cluster model of α + n, α + p, α+ 3He, and α + α elastic scattering from a realistic effective nuclear interaction NUCLEAR REACTIONS 1n, 1H, 3He, 4He(α, α), E<14 MeV; calculated elastic phase shifts. Microscopic cluster model with UCOM realistic nucleon-nucleon interaction. Comparison with experimental data.
doi: 10.1103/PhysRevC.84.014604
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
2011PU02 Phys.Rev.Lett. 106, 152301 (2011) A.Pupasov, B.F.Samsonov, J.-M.Sparenberg, D.Baye Reconstructing the Nucleon-Nucleon Potential by a New Coupled-Channel Inversion Method
doi: 10.1103/PhysRevLett.106.152301
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
2011SP03 J.Phys.:Conf.Ser. 312, 082040 (2011) J.-M.Sparenberg, P.Capel, D.Baye Deducing physical properties of weakly bound states from low-energy scattering data. Application to 16O and 12C+α NUCLEAR REACTIONS 12C(α, α'), E=low; calculated d-wave inversion potentials, effective-range function using published data close to 245 keV 2+ state of 16O; deduced ANC (asymptotic normalization constant).
doi: 10.1088/1742-6596/312/4/082040
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
2011YA12 Phys.Rev. C 84, 024603 (2011) Connection between effective-range expansion and nuclear vertex constant or asymptotic normalization coefficient NUCLEAR REACTIONS 16O(p, p), E<8 MeV; 4He(t, t), E<5 MeV; 4He(3He, 3He), E<8 MeV; analyzed scattering length, phase shifts, asymptotic normalization coefficients (ANC).
doi: 10.1103/PhysRevC.84.024603
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
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
2010HO03 Phys.Rev. C 81, 024606 (2010) W.Horiuchi, Y.Suzuki, P.Capel, D.Baye Probing the weakly-bound neutron orbit of 31Ne with total reaction and one-neutron removal cross sections NUCLEAR REACTIONS 12C, 208Pb(31Ne, 30Ne), E=40-1000 MeV/nucleon; calculated total σ and one-neutron removal σ, matter density, E1 strengths, parallel-momentum distribution for the elastic breakup of 31Ne using Glauber and eikonal models. NUCLEAR STRUCTURE 31Ne; calculated single-particle energies and discussed halo structure in the context of one-neutron removal reactions on 31Ne.
doi: 10.1103/PhysRevC.81.024606
2010SP01 Phys.Rev. C 81, 011601 (2010) J.-M.Sparenberg, P.Capel, D.Baye Influence of low-energy scattering on loosely bound states NUCLEAR REACTIONS 16O(n, γ), (p, γ), E not given; 12C(α, γ), E not given; calculated asymptotic normalization constants (ANC) as a function of binding energy for subthreshold bound states using the analytic continuation of the scattering (S) matrix in the complex wave-number plane.
doi: 10.1103/PhysRevC.81.011601
2010SU22 Nucl.Phys. A838, 20 (2010) Solving a coupled-channels scattering problem by adding confining potentials NUCLEAR REACTIONS 1H(p, p), (n, n), E=0-200 MeV; calculated phase shifts using coupled-channels Green function and Runge-Kutta methods.
doi: 10.1016/j.nuclphysa.2010.03.002
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
2009WA17 Phys.Rev. C 80, 034611 (2009) Parametrization of low-energy cross sections for nonresonant neutron capture NUCLEAR REACTIONS 7Li, 12,14C, 16,18O(n, γ), E(cm)<1 MeV; analyzed σ, spectroscopic factors and other parameters for nonresonant neutron capture using simple polynomials obtained from Taylor expansions. Comparison with experimental data.
doi: 10.1103/PhysRevC.80.034611
2008BA16 Eur.Phys.J. Special Topics 156, 93 (2008) Breakup reaction models for exotic nuclei
doi: 10.1140\epjst/e2008-00610-6
2008BA55 Int.J.Mod.Phys. E17, 2301 (2008) Three and four-body breakup reactions
doi: 10.1142/S0218301308011513
2008CA26 Phys.Rev. C 78, 054602 (2008) Coulomb-corrected eikonal description of the breakup of halo nuclei NUCLEAR REACTIONS 12C, 208Pb(11Be, X), E=67, 69 MeV/nucleon; calculated σ. Coulomb-corrected eikonal approximation.
doi: 10.1103/PhysRevC.78.054602
2008CA30 Int.J.Mod.Phys. E17, 2315 (2008) P.Capel, G.Goldstein, D.Baye, Y.Suzuki Breakup of halo nuclei within a Dynamical Eikonal Approximation NUCLEAR REACTIONS C, Pb(11Be, X), E=67, 69 MeV; calculated break-up σ, σ(E), σ(p). Coulomb Corrected Eikonal (CCE) model.
doi: 10.1142/S0218301308011537
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
2007GO26 Phys.Rev. C 76, 024608 (2007) Analysis of Coulomb breakup experiments of 8B with a dynamical eikonal approximation NUCLEAR REACTIONS Pb(8B, p), E=44, 52, 81, 83 MeV/nucleon; analyzed σ and angular distributions within the dynamical eikonal approximation. Analyzed the accuracy of the astrophysical S-factor extracted from coulomb breakup measurements.
doi: 10.1103/PhysRevC.76.024608
2007KA47 Nucl.Phys. A791, 68 (2007) Scattering length and effective range for collisions between light ions within a microscopic model NUCLEAR REACTIONS 4He, 14C, 16O(n, n), 4He, 14,16o(p, p), 3H, 3,4He(α, α), E < 8 MeV; calculated phase shifts.
doi: 10.1016/j.nuclphysa.2007.04.009
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
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
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
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
2006GO05 Phys.Rev. C 73, 024602 (2006) Dynamical eikonal approximation in breakup reactions of 11Be NUCLEAR REACTIONS 12C, 208Pb(11Be, X), E ≈ 68 MeV/nucleon; calculated breakup σ(E, θ), σ. Dynamical eikonal approximation, comparison with data.
doi: 10.1103/PhysRevC.73.024602
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
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
2005BA72 Phys.Rev.Lett. 95, 082502 (2005) Collisions of Halo Nuclei within a Dynamical Eikonal Approximation NUCLEAR REACTIONS 12C(11Be, 11Be), E=49.3 MeV/nucleon; 208Pb(11Be, 11Be), E=20 MeV/nucleon; calculated elastic σ(θ). 208Pb(11Be, X), E=20, 69 MeV/nucleon; calculated breakup σ(θ). Dynamical eikonal approximation, comparison with data.
doi: 10.1103/PhysRevLett.95.082502
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
2005BA80 Nucl.Phys. A758, 114c (2005) Behaviour of radiative-capture reactions near zero energy NUCLEAR REACTIONS 14N(p, γ), E < 0.2 MeV; 13C(n, γ), E < 0.6 MeV; calculated S-factors.
doi: 10.1016/j.nuclphysa.2005.05.023
2005CA22 Phys.Rev. C 71, 044609 (2005) Coupling-in-the-continuum effects in Coulomb dissociation of halo nuclei NUCLEAR REACTIONS 208Pb(11Be, n10Be), (8B, p7Be), E ≈ 50 MeV/nucleon; calculated Coulomb breakup, partial wave components, continuum effects, resonance contributions.
doi: 10.1103/PhysRevC.71.044609
2005TH05 Nucl.Phys. A753, 233 (2005) M.Theeten, D.Baye, P.Descouvemont Three-body models of the 6ΛΛHe and 9ΛBe hypernuclei with non-local interactions NUCLEAR STRUCTURE 6He, 9Be; calculated hypernucleus energies, radii. Three-body models, non-local interactions.
doi: 10.1016/j.nuclphysa.2005.02.129
2004BA62 Phys.Rev. C 70, 015801 (2004) Cross section expansion for direct neutron radiative capture NUCLEAR REACTIONS 12C(n, γ), E=0-0.6 MeV; calculated S-factors, σ(E) for radiative capture. Taylor expansion.
doi: 10.1103/PhysRevC.70.015801
2004CA50 Phys.Rev. C 70, 064605 (2004) Time-dependent analysis of the breakup of 11Be on 12C at 67 MeV/nucleon NUCLEAR REACTIONS 12C(11Be, n10Be), E=67 MeV/nucleon; analyzed breakup σ(E); deduced resonance contribution, other reaction mechanism features. Semiclassical framework, time-dependent Schrodinger equation.
doi: 10.1103/PhysRevC.70.064605
2004FU15 Nucl.Phys. A738, 495 (2004) Y.Fujiwara, K.Miyagawa, M.Kohno, Y.Suzuki, D.Baye, J.-M.Sparenberg A Consistent 3α and 2αΛ Faddeev Calculation using the 2α RGM Kernel
doi: 10.1016/j.nuclphysa.2004.04.095
2004FU19 Phys.Rev. C 70, 024002 (2004) Y.Fujiwara, K.Miyagawa, M.Kohno, Y.Suzuki, D.Baye, J.-M.Sparenberg Faddeev calculation of 3α and ααΛ systems using αα resonating-group method kernels NUCLEAR STRUCTURE 12C; calculated 3α-cluster states energies. 9Be; calculated hypernucleus ground and excited states energies. Faddeev calculations, two-cluster resonating-group method kernels.
doi: 10.1103/PhysRevC.70.024002
2003AN06 Nucl.Phys. A716, 211 (2003) C.Angulo, M.Azzouz, P.Descouvemont, G.Tabacaru, D.Baye, M.Cogneau, M.Couder, T.Davinson, A.Di Pietro, P.Figuera, M.Gaelens, P.Leleux, M.Loiselet, A.Ninane, F.de Oliveira Santos, R.G.Pizzone, G.Ryckewaert, N.de Sereville, F.Vanderbist Experimental determination of the 7Be+p scattering lengths NUCLEAR REACTIONS 1H(7Be, 7Be), E=4.4, 5.7, 6.3 MeV; measured recoil proton spectra, σ(θ); deduced scattering lengths. Astrophysical implications discussed.
doi: 10.1016/S0375-9474(02)01584-1
2003AN29 Nucl.Phys. A719, 300c (2003) C.Angulo, P.Descouvemont, M.Cogneau, M.Couder, M.Gaelens, P.Leleux, M.Loiselet, G.Ryckewaert, G.Tabacaru, F.Vanderbist, T.Davinson, M.Azzouz, D.Baye, A.Di Pietro, P.Figuera, R.G.Pizzone, F.de Oliveira Santos, N.de Sereville The elastic scattering 7Be + p at low energies: implications on the 7Be(p, γ)8Be S-factor NUCLEAR REACTIONS 1H(7Be, p), E(cm)=0.3-0.75 MeV; measured recoil proton spectra, σ(θ); deduced scattering lengths. 8B deduced resonance parameters. R-matrix analysis, astrophysical implications discussed.
doi: 10.1016/S0375-9474(03)00936-9
2003AR11 Phys.Rev. C 68, 014310 (2003) K.Arai, P.Descouvemont, D.Baye, W.N.Catford Resonance structure of 9Be and 9B in a microscopic cluster model NUCLEAR STRUCTURE 9Be, 9B; calculated resonance energies, J, π, widths. Microscopic multicluster model, comparisons with data.
doi: 10.1103/PhysRevC.68.014310
2003BA97 Nucl.Phys. A722, 328c (2003) Time-dependent analysis of the Coulomb breakup of weakly-bound nuclei
doi: 10.1016/S0375-9474(03)01385-X
2003CA01 Phys.Lett. 552B, 145 (2003) Supersymmetric elimination of forbidden states in the Coulomb breakup of the 11Be halo nucleus NUCLEAR REACTIONS Pb(11Be, 10Be), E=72 MeV/nucleon; calculated Coulomb breakup σ vs fragment relative energy. Time-dependent calculations, phase-equivalent potentials, comparison with data.
doi: 10.1016/S0370-2693(02)03128-3
2003CA25 Phys.Rev. C 68, 014612 (2003) Time-dependent analysis of the breakup of halo nuclei NUCLEAR REACTIONS 208Pb(11Be, n10Be), (15C, n14C), (11Be, 11Be'), (15C, 15C'), E ≈ 70 MeV/nucleon; calculated breakup and inelastic σ. Semiclassical time-dependent Schrodinger equation.
doi: 10.1103/PhysRevC.68.014612
2003DE12 Phys.Rev. C 67, 044309 (2003) P.Descouvemont, C.Daniel, D.Baye Three-body systems with Lagrange-mesh techniques in hyperspherical coordinates NUCLEAR STRUCTURE 6He, 12C; calculated level energies, radii, B(E2), wave functions. Three-body systems, Lagrange mesh technique.
doi: 10.1103/PhysRevC.67.044309
2003RA18 Phys.Rev. C 67, 044602 (2003) R.Raabe, A.Andreyev, M.Huyse, A.Piechaczek, P.Van Duppen, L.Weissman, A.Wohr, C.Angulo, S.Cherubini, A.Musumarra, D.Baye, P.Descouvemont, T.Davinson, A.Di Pietro, A.M.Laird, A.Ostrowski, A.Shotter, L.I.Galanina, N.S.Zelenskaya 2n-transfer contribution in the 4He(6He, 6He)4He cross section at Ec.m.=11.6 MeV NUCLEAR REACTIONS 4He(6He, 6He), E=11.6 MeV; measured σ(θ); deduced two-neutron transfer contribution. DWBA and double-folding potential analysis.
doi: 10.1103/PhysRevC.67.044602
2003TU04 Nucl.Phys. A723, 365 (2003) E.M.Tursunov, D.Baye, P.Descouvemont Comparative variational studies of 0+ states in three-α models NUCLEAR STRUCTURE 12C; calculated 0+ state energies in 3α models. Several approaches compared.
doi: 10.1016/S0375-9474(03)01323-X
2002AR04 Nucl.Phys. A699, 963 (2002) K.Arai, D.Baye, P.Descouvemont Microscopic Study of the 6Li(p, γ)7Be and 6Li(p, α)3He Reactions NUCLEAR REACTIONS 3He(α, α), 6Li(p, p), E(cm)=0.5-6 MeV; calculated elastic phase shifts. 3H, 3He(α, γ), E(cm) < 2.5 MeV; 6Li(p, α)(p, γ), E(cm) < 10 MeV; calculated S-factors. 6Li(n, α), E(cm) < 1 MeV; 6Li(n, γ), E=thermal; calculated σ. Four-cluster microscopic model.
doi: 10.1016/S0375-9474(01)01298-2
2002HE20 Nucl.Phys. A709, 184 (2002) Solving the Resonating-Group Equation on a Lagrange Mesh NUCLEAR REACTIONS 4He(n, n), (p, p), E=0.1-100 MeV; calculated phase shifts. Lagrange mesh method, resonating-group equation, comparison with other approaches.
doi: 10.1016/S0375-9474(02)01040-0
2002ME27 Prog.Theor.Phys.(Kyoto), Suppl. 146, 457 (2002) Time-Dependent Analysis of the Coulomb Breakup Determination of the Astrophysical S Factor NUCLEAR REACTIONS 208Pb(17F, p16O), E not given; analyzed Coulomb breakup data. 16O(p, γ), E=0-2 MeV; deduced astrophysical S-factor.
doi: 10.1143/PTPS.146.457
2002RA27 Nucl.Phys. A701, 387c (2002) R.Raabe, L.Weissman, A.Andreyev, C.Angulo, D.Baye, W.Bradfield-Smith, S.Cherubini, T.Davinson, P.Descouvemont, A.Di Pietro, M.Huyse, A.M.Laird, W.F.Mueller, A.Musumarra, A.Ostrowski, A.Piechaczek, A.Shotter, G.Terwagne, P.Van Duppen, A.Wohr Measurement of the 4He(6He, 6He)4He Cross Section with a 4He-Implanted Al Target NUCLEAR REACTIONS 4He(6He, 6He), E=29.6 MeV; measured σ(θ). Target nuclei implanted in aluminum. Comparisons with previous results.
doi: 10.1016/S0375-9474(01)01616-5
2002YA10 Nucl.Phys. A705, 335 (2002) R.Yarmukhamedov, D.Baye, C.Leclercq-Willain Asymptotics of Three-Body Bound State Radial Wave Functions of Halo Nuclei NUCLEAR STRUCTURE 6He; calculated wave functions, asymptotic normalization.
doi: 10.1016/S0375-9474(02)00672-3
2001AR05 Phys.Rev. C63, 044611 (2001) K.Arai, P.Descouvemont, D.Baye Low-Energy 6He + p Reactions in a Microscopic Multicluster Model NUCLEAR REACTIONS 6He(p, p), (p, n), (p, α), E(cm)=0-5 MeV; calculated σ(θ), σ(E). Microscopic multicluster model.
doi: 10.1103/PhysRevC.63.044611
2001BA01 Phys.Rev. C63, 014605 (2001) Lagrange Mesh Calculation of the Effective Range Expansion NUCLEAR REACTIONS 9Li(n, X), 4He(3He, X), 7Be, 16O(p, X), E not given; calculated coefficients for effective range expansion. Lagrange mesh technique.
doi: 10.1103/PhysRevC.63.014605
2001DE20 Phys.Lett. 505B, 71 (2001) 12B Molecular States in a Microscopic Cluster Model NUCLEAR STRUCTURE 12Be; calculated levels, J, π, radii. Cluster model, comparisons with data.
doi: 10.1016/S0370-2693(01)00349-5
2001ME18 Nucl.Phys. A689, 563c (2001) Time-Dependent Approach to Breakup of Nuclei with Neutron and Proton Halo NUCLEAR REACTIONS 208Pb(11Be, n10Be), (17F, p16O), E=0-6 MeV; calculated breakup σ.
doi: 10.1016/S0375-9474(01)00905-8
2001ME25 Phys.Rev. C64, 054612 (2001) Time-Dependent Analysis of the Coulomb Breakup Method for Determining the Astrophysical S Factor NUCLEAR REACTIONS 208Pb(17F, p16O), E ≈ 10-72 MeV/nucleon; calculated breakup σ, σ vs fragments relative energy. 16O(p, γ), E(cm) ≈ 0.3-2 MeV; calculated astrophysical S-factor. Time-dependent mesh method.
doi: 10.1103/PhysRevC.64.054612
2000BA09 Phys.Rev. C61, 025801 (2000) Zero-Energy Determination of the Astrophysical S Factor and Effective-Range Expansions NUCLEAR REACTIONS 3He(α, γ), 6Li, 7Be, 16O(p, γ), E at rest; calculated astrophysical S factors. Potential model, Taylor expansion.
doi: 10.1103/PhysRevC.61.025801
2000BB06 Few-Body Systems 29, 131 (2000) D.Baye, P.Descouvemont, R.Kamouni α + 8He Elastic Scattering with the Generator-Coordinate Method NUCLEAR REACTIONS 6,8He(α, α), E(cm) < 30 MeV; calculated phase shifts, potential features. Two-centre generator-coordinate method. NUCLEAR STRUCTURE 10,12Be; calculated levels, J, π. Two-centre generator-coordinate method.
doi: 10.1007/s006010070013
2000BB09 Phys.Rev. C62, 065803 (2000) Behavior of the 7Be(p, γ)8B Astrophysical S Factor Near Zero Energy NUCLEAR REACTIONS 7Be(p, γ), E=low; calculated zero-energy astrophysical S factor. Simplified potential model.
doi: 10.1103/PhysRevC.62.065803
2000LE34 Phys.Rev. C62, 064003 (2000) H.Leeb, S.A.Sofianos, J.-M.Sparenberg, D.Baye Supersymmetric Transformations in Coupled-Channel Systems
doi: 10.1103/PhysRevC.62.064003
2000SP03 Phys.Rev. C61, 024605 (2000) J.-M.Sparenberg, D.Baye, H.Leeb Phase-Equivalent Energy-Dependent Potentials NUCLEAR REACTIONS 16O(α, X), E=0, 150 MeV; calculated potential, bound state energies, transformation for removal of forbidden bound states. Extended supersymmetric transformations.
doi: 10.1103/PhysRevC.61.024605
2000SP07 Phys.Rev. C61, 054610 (2000) J.-M.Sparenberg, D.Baye, B.Imanishi Coupled-Reaction-Channel Calculations of the 16O + 17O and 16O + 17F Charge-Symmetric Systems NUCLEAR REACTIONS 17O, 17F(16O, 16O), (16O, 16O'), E(cm)=5-40 MeV; calculated σ(θ). 17O, 17F(16O, X), E(cm)=5-20 MeV; calculated reaction, fusion, inelastic σ. Three-body coupled-channels model, comparisons with data.
doi: 10.1103/PhysRevC.61.054610
1999AN35 Nucl.Phys. A656, 3 (1999) C.Angulo, M.Arnould, M.Rayet, P.Descouvemont, D.Baye, C.Leclercq-Willain, A.Coc, S.Barhoumi, P.Aguer, C.Rolfs, R.Kunz, J.W.Hammer, A.Mayer, T.Paradellis, S.Kossionides, C.Chronidou, K.Spyrou, S.Degl'Innocenti, G.Fiorentini, B.Ricci, S.Zavatarelli, C.Providencia, H.Wolters, J.Soares, C.Grama, J.Rahighi, A.Shotter, M.Lamehi-Rachti A Compilation of Charged-Particle Induced Thermonuclear Reaction Rates COMPILATION 1H(p, e+ν), 2H, 6,7Li, 7,9Be, 10,11B, 12,13C, 13,14,15N, 16,17,18O, 19F, 20,21,22Ne, 22,23Na, 24,25,26Mg, 26,27Al, 28Si(p, γ), 2H(d, γ), (d, p), 2,3H(d, n), 2,3H, 3He, 7Li, 7Be, 12C, 14,15N, 16,18O, 20,22Ne(α, γ), 3He(3He, 2p), 6,7Li, 9Be, 10,11B, 14,15N, 17,18O, 19F, 20Ne, 23Na, 24Mg, 27Al(p, α), 7Li, 9Be, 13C, 14N, 17,18O, 21,22Ne, 23Na, 25,26Mg, 27Al(α, n), 9Be, 11B, 13C, 14,15N, 19F, 23Na(p, n), 9Be(p, d), E < 10 MeV; compiled, analyzed σ, S-factors; calculated astrophysical reaction rates vs T9. Analytical approximations.
doi: 10.1016/S0375-9474(99)00030-5
1999DE23 Phys.Rev. C60, 015803 (1999) Higher-Order Multipolarities in the 16O(p, γ)17F and 7Be(p, γ)8B Reactions NUCLEAR REACTIONS 7Be, 16O(p, γ), E(cm)=0.02-2.0 MeV; calculated S factors, multipole components.
doi: 10.1103/PhysRevC.60.015803
1999FU03 Phys.Rev. C59, 817 (1999) K.Fujimura, D.Baye, P.Descouvemont, Y.Suzuki, K.Varga Low-Energy α + 6He Elastic Scattering with the Resonating-Group Method NUCLEAR REACTIONS 6He(α, α), E(cm) < 15 MeV; calculated σ, phase shifts; deduced molecular states. Resonating-group method.
doi: 10.1103/PhysRevC.59.817
1999HE14 Phys.Lett. 455B, 1 (1999) M.Hesse, D.Baye, J.-M.Sparenberg Supersymmetry in a Three-Body Model of Halo Nuclei NUCLEAR STRUCTURE 6He, 11Li, 14Be; calculated binding energies, radii. Three-body model with supersymmetric transformations. Comparison with data, other models.
doi: 10.1016/S0370-2693(99)00429-3
1999ME12 Phys.Rev. C59, 3232 (1999) Nonperturbative Time-Dependent Approach to Breakup of Halo Nuclei NUCLEAR REACTIONS 208Pb(11Be, n10Be), E=72 MeV/nucleon; calculated σ(E). Nonperturbative time-dependent approach.
doi: 10.1103/PhysRevC.59.3232
1999RA15 Phys.Lett. 458B, 1 (1999) R.Raabe, A.Piechaczek, A.Andreyev, D.Baye, W.Bradfield-Smith, S.Cherubini, T.Davinson, P.Descouvemont, A.Di Pietro, W.Galster, M.Huyse, A.M.Laird, J.McKenzie, W.F.Mueller, A.Ostrowski, A.Shotter, P.Van Duppen, A.Wohr Elastic 2n-Transfer in the 4He(6He, 6He)4He Scattering NUCLEAR REACTIONS 4He(6He, 6He), E(cm)=11.6-15.9 MeV; measured elastic σ(θ); deduced contribution from 2n-transfer process. Double folding potential.
doi: 10.1016/S0370-2693(99)00586-9
1998BA40 Phys.Rev. C58, 545 (1998) D.Baye, P.Descouvemont, M.Hesse Microscopic Analysis of Extranuclear Capture on the 16O(p, γ)17F Reaction NUCLEAR REACTIONS 16O(p, p), E(cm) < 10 MeV; calculated phase shifts. 16O(p, γ), E(cm) < 2 MeV; calculated astrophysical S-factors. Fully microscopic calculation.
doi: 10.1103/PhysRevC.58.545
1998HE26 Nucl.Phys. A640, 37 (1998) M.Hesse, J.-M.Sparenberg, F.Van Raemdonck, D.Baye Coupled-Channel R-Matrix Method on a Lagrange Mesh NUCLEAR REACTIONS 1H(p, p), (n, n), E < 100 MeV; 4He(α, α), E < 20 MeV; calculated phase shifts. Lagrange mesh method. NUCLEAR STRUCTURE 2H; calculated binding energy. Lagrange mesh method.
doi: 10.1016/S0375-9474(98)00435-7
1997BA94 Nucl.Phys. A627, 305 (1997) Lagrange-Mesh Calculations of Halo Nuclei NUCLEAR STRUCTURE 6He, 11Li, 14Be; calculated binding energies, mass radii, halo features. Lagrange-mesh method, three-body systems.
doi: 10.1016/S0375-9474(97)00603-9
1997BB13 Nuovo Cim. 110A, 913 (1997) Lagrange-Mesh Calculations of Halo Nuclei NUCLEAR STRUCTURE 6He, 11Li, 14Be; calculated binding energies, radii. Lagrange-mesh calculations.
doi: 10.1007/BF03035926
1997KU18 Nucl.Phys. A621, 149c (1997) R.Kunz, A.Mayer, K.-D.Joos, H.Knee, A.Muller, J.Nickel, Ch.Plettner, J.W.Hammer, D.Baye, P.Descouvemont, M.Jaeger, V.Kolle, S.Wilmes, G.Staudt, P.Mohr, Ch.Chronidou, S.Harissopulos, K.Spyrou, Th.Paradellis Capture Reactions in the Helium Burning of Stars NUCLEAR REACTIONS, ICPND 12C(α, γ), E(cm)=0.9-3 MeV; measured Iγ(θ), preliminary results; analyzed astrophysical S-factors vs E, reaction rates vs T9. 16O(α, γ), E not given; analyzed Eγ, Iγ. Astrophysical implications.
doi: 10.1016/S0375-9474(97)00228-5
1997SP02 Phys.Rev. C55, 2175 (1997) Inverse Scattering with Singular Potentials: A supersymmetric approach NUCLEAR REACTIONS 1H(n, n), (p, p), E=low; calculated scattering length. 1H(n, n), (p, p), E ≤ 350 MeV; analyzed phase shifts; deduced potential characteristics. Inverse scattering, singular potentials, supersymmetric approach.
doi: 10.1103/PhysRevC.55.2175
1997TI03 Nucl.Phys. A620, 29 (1997) N.K.Timofeyuk, D.Baye, P.Descouvemont Microscopic Shell-Model and Cluster-Model Calculations of the 13C → 12C + n and 8B → 7Be + p Vertex Constants NUCLEAR STRUCTURE 13C, 8B; calculated nucleon decay associated vetex constants; deduced 7Be(p, γ) astrophysical S-factor implications.
doi: 10.1016/S0375-9474(97)00155-3
1996BA26 Nucl.Phys. A599, 435 (1996) D.Baye, G.Levai, J.-M.Sparenberg Phase-Equivalent Complex Potentials NUCLEAR REACTIONS 16O(α, α), E not given; calculated effective potential. 20Ne deduced level energies from potential. Phase equivalent complex potentials.
doi: 10.1016/0375-9474(95)00487-4
1996BA45 Nucl.Phys. A604, 103 (1996) Time Evolution of a System of Two Alpha Particles
doi: 10.1016/0375-9474(96)00114-5
1996BA77 Phys.Rev. C54, 2563 (1996) D.Baye, L.Desorgher, D.Guillain, D.Herschkowitz Double-Folding Interaction for 6He + α Scattering NUCLEAR STRUCTURE 6He; calculated density distribution. Realistic, microscopic three-cluster model. NUCLEAR REACTIONS 4He(6He, 6He), E not given; calculated double-folding potential. Elastic halo neutron transfer, potential parity dependence dicussed. Realistic three-cluster model based 6He density distribution.
doi: 10.1103/PhysRevC.54.2563
1996LI38 Phys.Rev. C54, 2477 (1996) E.Lienard, D.Baye, Th.Delbar, P.Descouvemont, P.Duhamel, W.Galster, M.Kurokawa, P.Leleux, I.Licot, P.Lipnik, C.Michotte, T.Motobayashi, A.Ninane, J.-M.Sparenberg, J.Vanhorenbeeck, J.Vervier Evidence for One-Pion Charge Exchange in 13N + 13C Elastic Scattering Near the Coulomb Barrier NUCLEAR REACTIONS 13C(13N, 13N), E(cm)=8.15, 10, 14.75 MeV; measured σ(θ); deduced optical model parameters, parity term.
doi: 10.1103/PhysRevC.54.2477
1996SP02 Phys.Rev. C54, 1309 (1996) Supersymmetry between Deep and Shallow Optical Potentials for 16O + 16O Scattering NUCLEAR REACTIONS 16O(16O, 16O), E(cm)=10-35 MeV; analyzed optical potentials; deduced deep, shallow potentials associated supersymmetry features. Removal of complex normalizable solutions from deep optical potenitals.
doi: 10.1103/PhysRevC.54.1309
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