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NSR database version of May 24, 2024.

Search: Author = D.Baye

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2023BA38      Phys.Rev. C 108, 064610 (2023)

D.Baye

Ambiguity of Siegert transformations for isospin-forbidden electric dipole transitions

doi: 10.1103/PhysRevC.108.064610
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2020BA13      Phys.Rev. A 101, 022507 (2020)

D.Baye, J.Dohet-Eraly

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
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2020HE12      Phys.Rev. C 101, 054609 (2020)

C.Hebborn, D.Baye

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
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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
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2018AO02      Phys.Rev. C 97, 054305 (2018)

S.Aoyama, D.Baye

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
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2018AR03      Nucl.Phys. A977, 82 (2018)

T.Arai, W.Horiuchi, D.Baye

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
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2018BA25      J.Phys.(London) G45, 085102 (2018)

D.Baye, E.M.Tursunov

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
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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
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2014DO11      Phys.Rev. C 90, 034611 (2014)

J.Dohet-Eraly, D.Baye

Comparison of potential models of nucleus-nucleus bremsstrahlung

doi: 10.1103/PhysRevC.90.034611
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2013DO18      Phys.Rev. C 88, 024602 (2013)

J.Dohet-Eraly, D.Baye

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
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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
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2012BA39      Phys.Rev. C 86, 034306 (2012)

D.Baye

Extension of the Siegert theorem for photon emission

doi: 10.1103/PhysRevC.86.034306
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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
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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
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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
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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.107.132502
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2011BA01      Phys.Lett. B 696, 464 (2011)

D.Baye, E.M.Tursunov

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
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2011BA21      Int.J.Mod.Phys. E20, 769 (2011)

D.Baye

On the cluster-model description of collisions

doi: 10.1142/S0218301311018642
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2011DO13      Phys.Rev. C 84, 014604 (2011)

J.Dohet-Eraly, D.Baye

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
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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
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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
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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
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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
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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
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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
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2011YA12      Phys.Rev. C 84, 024603 (2011)

R.Yarmukhamedov, D.Baye

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
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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
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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
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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
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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
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2010SU22      Nucl.Phys. A838, 20 (2010)

Y.Suzuki, D.Baye, A.Kievsky

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
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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
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2009WA17      Phys.Rev. C 80, 034611 (2009)

C.Wang, O.I.Cisse, D.Baye

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
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2008BA16      Eur.Phys.J. Special Topics 156, 93 (2008)

D.Baye

Breakup reaction models for exotic nuclei

doi: 10.1140\epjst/e2008-00610-6
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2008BA55      Int.J.Mod.Phys. E17, 2301 (2008)

D.Baye

Three and four-body breakup reactions

doi: 10.1142/S0218301308011513
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2008CA26      Phys.Rev. C 78, 054602 (2008)

P.Capel, D.Baye, Y.Suzuki

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
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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
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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
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2007GO26      Phys.Rev. C 76, 024608 (2007)

G.Goldstein, P.Capel, D.Baye

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
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2007KA47      Nucl.Phys. A791, 68 (2007)

R.Kamouni, D.Baye

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
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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
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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
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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
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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
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2006GO05      Phys.Rev. C 73, 024602 (2006)

G.Goldstein, D.Baye, P.Capel

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
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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
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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
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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
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2005BA72      Phys.Rev.Lett. 95, 082502 (2005)

D.Baye, P.Capel, G.Goldstein

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
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2005BA73      Phys.Rev. C 72, 024309 (2005)

D.Baye, P.Descouvemont, F.Leo

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
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2005BA80      Nucl.Phys. A758, 114c (2005)

D.Baye

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
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2005CA22      Phys.Rev. C 71, 044609 (2005)

P.Capel, D.Baye

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
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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
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2004BA62      Phys.Rev. C 70, 015801 (2004)

D.Baye

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
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2004CA50      Phys.Rev. C 70, 064605 (2004)

P.Capel, G.Goldstein, D.Baye

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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0495.


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
Citations: PlumX Metrics

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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
Citations: PlumX Metrics


2003BA97      Nucl.Phys. A722, 328c (2003)

D.Baye, P.Capel, V.S.Melezhik

Time-dependent analysis of the Coulomb breakup of weakly-bound nuclei

doi: 10.1016/S0375-9474(03)01385-X
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2003CA01      Phys.Lett. 552B, 145 (2003)

P.Capel, D.Baye, V.S.Melezhik

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
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2003CA25      Phys.Rev. C 68, 014612 (2003)

P.Capel, D.Baye, V.S.Melezhik

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
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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
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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
Citations: PlumX Metrics

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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2002HE20      Nucl.Phys. A709, 184 (2002)

M.Hesse, J.Roland, D.Baye

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
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2002ME27      Prog.Theor.Phys.(Kyoto), Suppl. 146, 457 (2002)

V.S.Melezhik, D.Baye

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
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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
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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
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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
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2001BA01      Phys.Rev. C63, 014605 (2001)

D.Baye, M.Hesse, R.Kamouni

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
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2001DE20      Phys.Lett. 505B, 71 (2001)

P.Descouvemont, D.Baye

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
Citations: PlumX Metrics


2001ME18      Nucl.Phys. A689, 563c (2001)

V.S.Melezhik, D.Baye

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
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2001ME25      Phys.Rev. C64, 054612 (2001)

V.S.Melezhik, D.Baye

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
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2000BA09      Phys.Rev. C61, 025801 (2000)

D.Baye, E.Brainis

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
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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
Citations: PlumX Metrics


2000BB09      Phys.Rev. C62, 065803 (2000)

D.Baye

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
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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
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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
Citations: PlumX Metrics


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
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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
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1999DE23      Phys.Rev. C60, 015803 (1999)

P.Descouvemont, D.Baye

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
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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1999ME12      Phys.Rev. C59, 3232 (1999)

V.S.Melezhik, D.Baye

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
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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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0173.


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
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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
Citations: PlumX Metrics


1997BA94      Nucl.Phys. A627, 305 (1997)

D.Baye

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
Citations: PlumX Metrics


1997BB13      Nuovo Cim. 110A, 913 (1997)

D.Baye

Lagrange-Mesh Calculations of Halo Nuclei

NUCLEAR STRUCTURE 6He, 11Li, 14Be; calculated binding energies, radii. Lagrange-mesh calculations.

doi: 10.1007/BF03035926
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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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0808.


1997SP02      Phys.Rev. C55, 2175 (1997)

J.-M.Sparenberg, D.Baye

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
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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
Citations: PlumX Metrics


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
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1996BA45      Nucl.Phys. A604, 103 (1996)

D.Baye, D.Herschkowitz

Time Evolution of a System of Two Alpha Particles

doi: 10.1016/0375-9474(96)00114-5
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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
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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
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1996SP02      Phys.Rev. C54, 1309 (1996)

J.-M.Sparenberg, D.Baye

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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