NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = M.Dupuis Found 33 matches. 2024DE02 Phys.Rev. C 109, 014320 (2024) J.-P.Delaroche, J.Libert, M.Girod, I.Deloncle, M.Dupuis Investigations of electric monopole transitions in medium-mass to heavy nuclei: Beyond mean field calculations with the Gogny force
doi: 10.1103/PhysRevC.109.014320
2023HE08 J.Phys.(London) G50, 060501 (2023) C.Hebborn, F.M.Nunes, G.Potel, W.H.Dickhoff, J.W.Holt, M.C.Atkinson, R.B.Baker, C.Barbieri, G.Blanchon, M.Burrows, R.Capote, P.Danielewicz, M.Dupuis, C.Elster, J.E.Escher, L.Hlophe, A.Idini, H.Jayatissa, B.P.Kay, K.Kravvaris, J.J.Manfredi, A.Mercenne, B.Morillon, G.Perdikakis, C.D.Pruitt, G.H.Sargsyan, I.J.Thompson, M.Vorabbi, T.R.Whitehead Optical potentials for the rare-isotope beam era
doi: 10.1088/1361-6471/acc348
2023MU06 Phys.Rev. C 107, 034606 (2023) M.R.Mumpower, D.Neudecker, H.Sasaki, T.Kawano, A.E.Lovell, M.W.Herman, I.Stetcu, M.Dupuis Collective enhancement in the exciton model NUCLEAR REACTIONS 239Pu(n, 2n), E=6-24 MeV; calculated σ(E). 239Pu(n, xn), E=14 MeV; 181Ta, 165(n, xn), E=20 MeV; calculated neutron emission spectra. Calculation with statistical model framework CoH3 with increased one-particle-one-hole state density used in the exciton model. Comparison to experimental data and ENDF/B-VIII.0. NUCLEAR STRUCTURE 239Pu; calculated 1p-1h state densities.
doi: 10.1103/PhysRevC.107.034606
2021BL03 Eur.Phys.J. A 57, 13 (2021) G.Blanchon, M.Dupuis, H.F.Arellano, R.N.Bernard, B.Morillon, P.Romain Diving into Raynal's DWBA code
doi: 10.1140/epja/s10050-020-00331-5
2021KE09 Phys.Rev. C 104, 044605 (2021) M.Kerveno, M.Dupuis, A.Bacquias, F.Belloni, D.Bernard, C.Borcea, M.Boromiza, R.Capote, C.De Saint Jean, P.Dessagne, J.C.Drohe, G.Henning, S.Hilaire, T.Kawano, P.Leconte, N.Nankov, A.Negret, M.Nyman, A.Olacel, A.J.M.Plompen, P.Romain, C.Rouki, G.Rudolf, M.Stanoiu, R.Wynants Measurement of 238U(n, n'γ) cross section data and their impact on reaction models NUCLEAR REACTIONS 238U(n, n'γ), E<20 MeV from GELINA facility at EC-JRC Geel; measured Eγ, Iγ, γ(TOF)-plot, angle-integrated γ-production σ(E, θ) using time-of-flight (TOF) and prompt γ-ray spectroscopy methods using the GRAPhEME spectrometer at GELINA. 238U; deduced levels, γ transitions, Iγ values, multipolarities, σ for E2 transitions, discrete structure and interband transition; discussed new or revised γ ray energies and intensities for 218.1-, 270.1-, 680.11-, 931.1-, 950.12- and 997.58-keV γ rays, as compared to evaluated data in the ENSDF database and those in 2014Go06 (Phys. Atomic Nuclei 77, 131). Comparison with previous experimental and evaluated reaction cross section data, and with TALYS, EMPIRE and CoH theoretical calculations using nuclear reaction codes dealing with compound nucleus, and pre-equilibrium mechanisms. Relevance to microscopic improving the modeling of the (n, n') reaction.
doi: 10.1103/PhysRevC.104.044605
2021NA24 Eur.Phys.J. A 57, 279 (2021) A.Nasri, M.Dupuis, G.Blanchon, H.F.Arellano, P.Tamagno Following J. Raynal's DWBA and ECIS codes: coupled channels with microscopic non-local potential
doi: 10.1140/epja/s10050-021-00585-7
2020PE08 Phys.Rev.Lett. 125, 122502 (2020) R.Perez Sanchez, B.Jurado, V.Meot, O.Roig, M.Dupuis, O.Bouland, D.Denis-Petit, P.Marini, L.Mathieu, I.Tsekhanovich, M.Aiche, L.Audouin, C.Cannes, S.Czajkowski, S.Delpech, A.Gorgen, M.Guttormsen, A.Henriques, G.Kessedjian, K.Nishio, D.Ramos, S.Siem, F.Zeiser Simultaneous Determination of Neutron-Induced Fission and Radiative Capture Cross Sections from Decay Probabilities Obtained with a Surrogate Reaction NUCLEAR REACTIONS 240Pu(α, α'), (α, F), E=30 MeV; 239Pu(n, F), (n, γ), E<2 MeV; measured reaction products, Eγ, Iγ, Eα, Iα, α-fission fragment-γ ray triple coin.; deduced 239Pu σ as a function of energy. Comparison with ENDF/B-VIII.0, JENDL 4.0. JEFF 3.3 libraries.
doi: 10.1103/PhysRevLett.125.122502
2019DU20 Phys.Rev. C 100, 044607 (2019) M.Dupuis, G.Haouat, J.-P.Delaroche, E.Bauge, J.Lachkar Challenging microscopic structure and reaction models for nucleon scattering off nuclei in the A=208 mass region NUCLEAR REACTIONS 206,207,208Pb, 209Bi(n, n), (n, n'), E=7.50, 9.50, 11.50, 13.00, 13.50, 15.50 MeV; measured neutron time of flight spectra, En, In, differential σ(θ, E) at the CEA DAM Ile-de-France tandem accelerator laboratory; deduced ground state and transition radial neutron and proton densities, differential σ(θ, E) for the low-lying states in 206,207,208Pb, 209Bi. 206Pb(n, n), E=3.04, 3.11, 3.19, 3.47, 3.97, 4.2, 4.6, 5, 7, 21.6 MeV; 208Pb(n, n), E=1, 1.1, 1.2, 1.27, 1.34, 1.43, 1.59, 1.65, 1.75, 2.5, 3.4, 4, 4.5, 5, 5.5, 6, 6.5, 7, 7.97, 8.5, 9, 9.97, 11, 13.9, 14.6, 16.9, 20, 22, 24, 26 MeV; 209Bi(n, n), E=6.5, 7, 7.14, 8, 8.4, 9, 9.99, 10.4, 11, 12, 14, 14.5, 14.76, 15.2, 20, 21.6, 24 MeV; 206Pb(n, n'), E=2.45, 2.53, 2.71, 2.94, 3.4, 4.02, 4.6, 6, 7, 8, 8.5 MeV; 207Pb(n, n'), E=3.56, 5.5, 6, 6.49, 7, 8.01, 8.5 MeV; 208Pb(n, n'), E=3.96, 5.5, 6, 6.49, 7, 8.01, 8.5, 11, 20, 22, 25.7 MeV; 209Bi(n, n'), E=3.06, 3.55, 7, 14 MeV; 206Pb(p, p'), E=19.64, 24.5, 35 MeV; analyzed previous experimental differential σ(θ, E) data for elastic scattering and inelastic scattering, the latter to the first 2+, 3-, 4+, 5- and 7- states in 206Pb, 5/2+ to 7/2+ multiplet in 207Pb, first 2+, 3- and 5- states in 208Pb, and 3/2+ to 15/2+ multiplet in 209Bi. All analyses based on the semimicroscopic Jeukenne, Lejeune, Mahaux (JLM-B) folding model and DWBA formalism, with the nuclear diagonal and transition densities calculated from quasiparticle random phase approximation QRPA model with the Gogny D1S interaction. NUCLEAR STRUCTURE 208Pb; calculated level energies and B(Eλ) values for the first 3-, 5-, 2+, 4+ and 6+ states. 206Pb; calculated level energies, B(Eλ) values, and neutron-to-proton reduced matrix element ratio for the first 2+, 4+, 7-, 2-, 3- states and the 2+ quadrupole surface vibrational state. QRPA predictions with the Gogny D1S force. Comparison with experimental values.
doi: 10.1103/PhysRevC.100.044607
2018CO06 Phys.Rev. C 97, 044315 (2018) M.L.Cortes, P.Doornenbal, M.Dupuis, S.M.Lenzi, F.Nowacki, A.Obertelli, S.Peru, N.Pietralla, V.Werner, K.Wimmer, G.Authelet, H.Baba, D.Calvet, F.Chateau, A.Corsi, A.Delbart, J.-M.Gheller, A.Gillibert, T.Isobe, V.Lapoux, C.Louchart, M.Matsushita, S.Momiyama, T.Motobayashi, M.Niikura, H.Otsu, C.Peron, A.Peyaud, E.C.Pollacco, J.-Y.Rousse, H.Sakurai, C.Santamaria, M.Sasano, Y.Shiga, S.Takeuchi, R.Taniuchi, T.Uesaka, H.Wang, K.Yoneda, F.Browne, L.X.Chung, Zs.Dombradi, S.Franchoo, F.Giacoppo, A.Gottardo, K.Hadynska-Klek, Z.Korkulu, S.Koyama, Y.Kubota, J.Lee, M.Lettmann, R.Lozeva, K.Matsui, T.Miyazaki, S.Nishimura, L.Olivier, S.Ota, Z.Patel, E.Sahin, C.M.Shand, P-A.Soderstrom, I.Stefan, D.Steppenbeck, T.Sumikama, D.Suzuki, Zs.Vajta, J.Wu, Z.Xu Inelastic scattering of neutron-rich Ni and Zn isotopes off a proton target NUCLEAR REACTIONS 1H(72Ni, p'), E=271.0 MeV/nucleon; 1H(74Ni, p'), E=263.5 MeV/nucleon; 1H(76Zn, p'), E=275.5 MeV/nucleon; 1H(80Zn, p'), E=263.4 MeV/nucleon, [secondary 72,74Ni, 76,80Zn beams from 9Be(238U, X), E=345 MeV/nucleon primary reaction, followed by separation of fragments using BigRIPS separator]; measured reaction products, yields, Eγ, Iγ, particles, (particle)γ-coin, angular integrated proton inelastic scattering σ using MINOS target device, DALI2 array for γ detection and ZeroDegree spectrometer for particles at RIBF-RIKEN facility. 72,74Ni, 76,80Zn; deduced first 2+ and 4+ levels, and second 2+ levels in 72,74Ni; analyzed B(E2) values and matrix elements for the first 2+ states. Comparison with shell-model calculations, and with previous measurements. Systematics of β2 deformation parameters in 62Zn to 80Zn, and 54Ni to 74Ni isotopes. Comparison of experimental σ for inelastic scattering with calculations using Jeukenne-Lejeune-Mahaux (JLM) folding model with quasiparticle random-phase approximation (QRPA). 58Ni(p, p), E=295, 250, 333 MeV; 58Ni(p, p'), E=178 MeV; analyzed σ(θ) data using the JLM reaction model and KD02 potential.
doi: 10.1103/PhysRevC.97.044315
2017AL40 Eur.Phys.J. A 53, 231 (2017) N.Alamanos, M.Dupuis, N.Pillet Topical Issue on Finite Range Effective Interactions and Associated Many-Body Methods - A Tribute to Daniel Gogny
doi: 10.1140/epja/i2017-12437-8
2017BL05 Eur.Phys.J. A 53, 88 (2017) G.Blanchon, M.Dupuis, R.N.Bernard, H.F.Arellano Asymmetry dependence of Gogny-based optical potential NUCLEAR REACTIONS 40,48Ca(n, n'), (p, p'), E=0-36 MeV; calculated σ(θ), analyzing power, inelastic σ using potentials generated by NSM (Nuclear Structure Method) with Gogny effective interaction. 40,48Ca(p, p), E=0-36 MeV; calculated σ(θ) using Perey-Buck equivalent potential and NSM.
doi: 10.1140/epja/i2017-12268-7
2017DU06 Eur.Phys.J. A 53, 111 (2017) Microscopic description of elastic and direct inelastic nucleon scattering off spherical nuclei NUCLEAR REACTIONS 90Zr(p, p), E=12.7-185 MeV;90Zr(p, p), (p, p'), E=57.5, 185 MeV;90Zr(p, xp), E=68-200 MeV;208Pb(p, p'), E=35-200 MeV; calculated σ(θ) using microscopic parameter-free approach based on Melbourne g-matrix and RPA and by TALYS code. Compared with available data. NUCLEAR STRUCTURE 90Zr, 208Pb; calculated B(E2), B(E3), B(E5) between discrete states using RPA/D1S model. Compared to available data.
doi: 10.1140/epja/i2017-12293-6
2017PI06 Eur.Phys.J. A 53, 49 (2017) N.Pillet, C.Robin, M.Dupuis, G.Hupin, J.-F.Berger The self-consistent multiparticle-multihole configuration mixing - Motivations, state of the art and perspectives
doi: 10.1140/epja/i2017-12232-7
2017RO08 Phys.Rev. C 95, 044315 (2017) C.Robin, N.Pillet, M.Dupuis, J.Le Bloas, D.Pena Arteaga, J.-F.Berger Description of nuclear systems with a self-consistent configuration-mixing approach. II. Application to structure and reactions in even-even sd-shell nuclei NUCLEAR STRUCTURE 20,22,24,26,28Ne, 24Mg, 28Si, 32S; calculated HFB potential energy surfaces (PES) in (β, γ) plane, main configuration components of the ground-states, differences between Hartree-Fock and self-consistent single-particle energies, squared modulus of the radial part of the single-particle orbitals. 28Si, 32S and 20Ne; calculated radial proton and neutron densities, proton, neutron, and proton-neutron correlations, excitation energies, B(E2) and charge transition densities and form factors from inelastic electron and proton scattering. 20,22,24,26,28Ne, 22,24,26,28,30Mg, 24,26,28,30,32Si, 28,30,32,34S, 32,34,36Ar; calculated low-energy levels, J, π, energies of the first 2+ states, binding energies and charge radii. Variational multiparticle-multihole (MPMH) configuration mixing approach using the D1S Gogny force. Comparison with experimental data.
doi: 10.1103/PhysRevC.95.044315
2016HI08 Eur.Phys.J. A 52, 336 (2016) S.Hilaire, S.Goriely, S.Peru, N.Dubray, M.Dupuis, E.Bauge Nuclear reaction inputs based on effective interactions NUCLEAR STRUCTURE A=20-250; calculated s-wave neutron resonance mean spacing using ab initio calculations with BSk9 Skyrme interaction. 240Pu; calculated potential energy surface, quadrupole moment using Gogny-type interaction. NUCLEAR REACTIONS 235U(n, F), E=0.02-12 MeV; calculated σ using ab initio Skyrme interactions. 40Ca, 48Cr, 89Y, 165Ho, 181Ta, 208Pb, 233Th, 238U, 242Pu(n, x), E=0.01-200 MeV; calculated total reaction σ using JLM approach with D1M nuclear matter densities. Compared with available data.
doi: 10.1140/epja/i2016-16336-2
2015BL01 Phys.Rev. C 91, 014612 (2015) G.Blanchon, M.Dupuis, H.F.Arellano, N.Vinh Mau Microscopic positive-energy potential based on the Gogny interaction NUCLEAR REACTIONS 40Ca(p, p), E=9.86, 10.37, 13.49, 14.51, 15.97, 18.57, 19.57, 21, 23.5, 25, 26.3, 27.5, 30.3, 40 MeV; 40Ca(n, n), E=2.06, 3.29, 5.3, 5.88, 6.5, 7.91, 9.91, 13.9, 16.9, 19, 21.7, 25.5, 30.3, 40 MeV; 40Ca(polarized p, p), E=14.51, 15.97, 18.57, 40 MeV; 40Ca(polarized n, n), E=9.91, 11, 13.9, 16.9 MeV; analyzed differential σ(E, θ), integral σ(E), and analyzing power Ay(θ, E). Calculation based on Greens function formalism in the random-phase approximation with the finite-range Gogny effective interaction, and including effects of intermediate single-particle resonances.
doi: 10.1103/PhysRevC.91.014612
2015BL08 Eur.Phys.J. A 51, 165 (2015) G.Blanchon, M.Dupuis, H.F.Arellano Prospective study on microscopic potential with Gogny interaction
doi: 10.1140/epja/i2015-15165-1
2015CO03 Phys.Lett. B 743, 451 (2015) A.Corsi, S.Boissinot, A.Obertelli, P.Doornenbal, M.Dupuis, F.Lechaftois, M.Matsushita, S.Peru, S.Takeuchi, H.Wang, N.Aoi, H.Baba, P.Bednarczyk, M.Ciemala, A.Gillibert, T.Isobe, A.Jungclaus, V.Lapoux, J.Lee, M.Martini, K.Matsui, T.Motobayashi, D.Nishimura, S.Ota, E.Pollacco, H.Sakurai, C.Santamaria, Y.Shiga, D.Sohler, D.Steppenbeck, R.Taniuchi Neutron-driven collectivity in light tin isotopes: Proton inelastic scattering from 104Sn NUCLEAR REACTIONS 1H(104Sn, 104Sn'), E=150 MeV/nucleon; measured reaction products, Eγ, Iγ. 104Sn; deduced σ(θ), energy levels, J, π. QRPA with the D1M Gogny interaction calculations.
doi: 10.1016/j.physletb.2015.03.018
2015DU16 Eur.Phys.J. A 51, 168 (2015) M.Dupuis, E.Bauge, S.Hilaire, F.Lechaftois, S.Peru, N.Pillet, C.Robin Progress in microscopic direct reaction modeling of nucleon induced reactions
doi: 10.1140/epja/i2015-15168-x
2014BA22 Nucl.Data Sheets 118, 32 (2014) E.Bauge, M.Dupuis, S.Hilaire, S.Peru, A.J.Koning, D.Rochman, S.Goriely Connecting the Dots, or Nuclear Data in the Age of Supercomputing NUCLEAR REACTIONS 238U(n, xn), E=14.1 MeV; calculated σ(En, θ=300, σ(En, θ=900 using TMC )TALYS/TEFAL/NJOY) code system. Compared to data. NUCLEAR STRUCTURE N=4-170; calculated binding energy, Q using beyond-the-mean-field level using different interactions.
doi: 10.1016/j.nds.2014.04.004
2014LE03 Phys.Rev. C 89, 011306 (2014) J.Le Bloas, N.Pillet, M.Dupuis, J.M.Daugas, L.M.Robledo, C.Robin, V.G.Zelevinsky First characterization of sd-shell nuclei with a multiconfiguration approach NUCLEAR STRUCTURE 20,22,24,26,28Ne, 22,24,26,28,30Mg, 24,26,28,30,32Si, 26,28,30,32,34S, 30,32,34,36Ar; calculated binding energies, S(2n), S(2p), energies and B(E2) of first 2+ states, magnetic dipole and electric static quadrupole moments, B(M1) for transitions between low-lying 1+, 2+ and 3+ states in spherical Hartree-Fock (HF) and multiparticle-multihole configuration mixing (CM) approximations with D1S Gogny interaction. Comparison with experimental values.
doi: 10.1103/PhysRevC.89.011306
2013LE08 Acta Phys.Pol. B44, 299 (2013) J.Le Bloas, N.Pillet, J.-M.Daugas, M.Dupuis Description of Light Nuclei (10 ≤ Z, N ≤ 18) Within the Multiparticle-Multihole Gogny Energy Density Functional NUCLEAR STRUCTURE Ne, Mg, Si, S, Ar; calculated excitation energies, dipole moments. Comparison with experimental data. NUCLEAR STRUCTURE 24,26Mg, 26,24,26,28,30,32Si, 34S, 28,30,32,34,36Ar; calculated B(E2), B(M1). D1S Gogny interaction, comparison with experimental data.
doi: 10.5506/APhysPolB.44.299
2012PI07 Phys.Rev. C 85, 044315 (2012) N.Pillet, V.G.Zelevinsky, M.Dupuis, J.-F.Berger, J.M.Daugas Low-lying spectroscopy of a few even-even silicon isotopes investigated with the multiparticle-multihole Gogny energy density functional NUCLEAR STRUCTURE 26,28,30,32Si; calculated triaxial HFB potential energy surfaces, β and γ deformation parameters, ground state collective wavefunctions, levels, J, π, proton and neutron single particle orbitals, E(4+)/E(2+) ratios, proton and neutron occupation probabilities, strength functions, Slater determinants, statistical properties of highly excited configurations. Multiconfiguration (mp-mh) microscopic method with DIS Gogny effective interaction. Comparison with calculations from five-dimensional (5DCH) approximate generator coordinate method (GCM), and with experimental data.
doi: 10.1103/PhysRevC.85.044315
2011DU03 Phys.Rev. C 83, 014602 (2011) M.Dupuis, T.Kawano, J.-P.Delaroche, E.Bauge Microscopic model approach to (n, xn) pre-equilibrium reactions for medium-energy neutrons NUCLEAR REACTIONS 90Zr, 208Pb(n, xn), E=0-20 MeV; calculated E3 and E5 strengths as function of incident neutron energy, σ, differential σ, σ(θ) using self-consistent random-phase approximation (RPA) with the Gogny D1S force. Comparison with experimental data.
doi: 10.1103/PhysRevC.83.014602
2011MA18 Phys.Rev. C 83, 034309 (2011) Low-energy dipole excitations in neon isotopes and N = 16 isotones within the quasiparticle random-phase approximation and the Gogny force NUCLEAR STRUCTURE 24O, 18,20,22,24,26,28,30Ne, 28Mg, 30Si; calculated B(E1) distributions, neutron and proton ground state density profiles, particle-hole configurations and energies for low-energy dipole excitation (GDR), neutron and proton transition densities. Fully consistent axially-symmetric-deformed quasiparticle random phase approximation (QRPA) approach based on Hartree-Fock-Bogolyubov (HFB) states.
doi: 10.1103/PhysRevC.83.034309
2011NO17 Phys.Rev. C 84, 064609 (2011) G.P.A.Nobre, F.S.Dietrich, J.E.Escher, I.J.Thompson, M.Dupuis, J.Terasaki, J.Engel Toward a microscopic reaction description based on energy-density-functional structure models NUCLEAR REACTIONS 90Zr(n, X), E=10, 20, 30 MeV; 58Ni(n, X), E=20, 30 MeV; 58Ni(p, X), E=10-70 MeV; 48Ca(p, X), E=10-50 MeV; 40,48Ca, 58Ni, 144Sm(n, X), (p, X), E=30 MeV; 90Zr(p, X), E=20-70 MeV; calculated reaction cross section. 90Zr(p, p), E=40, 65 MeV; calculated σ(θ). Random-phase, Hartree-Fock-Bogoliubov (HFB) framework and Skyrme density functional with coupling to all RPA and QRPA inelastic channels including deuteron formation. Assessed effects of couplings between inelastic resonances from higher-order channels. Comparison with experimental data.
doi: 10.1103/PhysRevC.84.064609
2011PE01 Phys.Rev. C 83, 014314 (2011) S.Peru, G.Gosselin, M.Martini, M.Dupuis, S.Hilaire, J.-C.Devaux Giant resonances in 238U within the quasiparticle random-phase approximation with the Gogny force NUCLEAR STRUCTURE 238U; calculated Kπ=0-, 0+, 1-, 1+ eigenvalues, B(E0), B(E1), B(E2) and B(E3) strengths for dipole, monopole, quadrupole, and octupole giant resonances and low-energy states. Fully consistent microscopic axially-symmetric deformed quasiparticle random-phase approximation (QRPA) approach using a finite-range Gogny force for Hartree-Fock-Bogolyubov mean field and QRPA matrix. Comparison with experimental data.
doi: 10.1103/PhysRevC.83.014314
2010BL08 Phys.Rev. C 82, 034313 (2010) G.Blanchon, N.Vinh Mau, A.Bonaccorso, M.Dupuis, N.Pillet Particle-particle random-phase approximation applied to beryllium isotopes NUCLEAR STRUCTURE 8,10,12,14Be; calculated levels, J, π, pp-RPA amplitudes, E1 strength distribution, S(2n), rms radii. Comparison to experimental data. Particle-particle random-phase approximation (pp-RPA) method using Woods-Saxon potential for the neutron-core interaction and D1S Gogny force for the neutron-neutron interaction.
doi: 10.1103/PhysRevC.82.034313
2010NO06 Phys.Rev.Lett. 105, 202502 (2010) G.P.A.Nobre, F.S.Dietrich, J.E.Escher, I.J.Thompson, M.Dupuis, J.Terasaki, J.Engel Coupled-Channel Calculation of Nonelastic Cross Sections Using a Density-Functional Structure Model NUCLEAR REACTIONS 40,48Ca, 58Ni, 90Zr, 144Sm(p, X), (n, X), E<40 MeV; calculated total reaction σ. Complete microscopic calculation, comparison with experimental data.
doi: 10.1103/PhysRevLett.105.202502
2010ZH34 Phys.Rev. C 82, 024601 (2010) Z.Zhou, X.Ruan, Y.Du, B.Qi, H.Tang, H.Xia, R.L.Walter, R.T.Braun, C.R.Howell, W.Tornow, G.J.Weisel, M.Dupuis, J.P.Delaroche, Z.Chen, Z.Chen, Y.Chen Differential cross section for neutron scattering from 209Bi at 37 MeV and the weak particle-core coupling NUCLEAR REACTIONS 209Bi(n, n), (n, n')E=37 MeV, [neutrons produced in 3H(d, n)]; measured neutron spectra, cross sections, σ(θ), TOF method. Optical model analysis of σ(θ) data. Optical-model (OM) + DWBA calculations with weak particle-core coupling for computing (n, n) and (n, n') cross sections.
doi: 10.1103/PhysRevC.82.024601
2008DU10 Phys.Lett. B 665, 152 (2008) M.Dupuis, S.Karataglidis, E.Bauge, J.-P.Delaroche, D.Gogny Challenging nuclear structure models through a microscopic description of proton inelastic scattering off 208Pb NUCLEAR REACTIONS 208Pb(p, p'), E=65-201 MeV; calculated σ(θ). Compared results to available data.
doi: 10.1016/j.physletb.2008.05.061
2007VI11 Nucl.Phys. A787, 126c (2007) A.C.C.Villari, C.Eleon, R.Alves-Conde, J.C.Angelique, C.Barue, C.Canet, M.Dubois, M.Dupuis, J.L.Flambard, G.Gaubert, P.Jardin, N.Lecesne, P.Leherissier, F.Lemagnen, R.Leroy, L.Maunoury, J.Y.Pacquet, F.Pellemoine, M.G.Saint-Laurent, C.Stodel, J.C.Thomas SPIRAL at GANIL: Latest Results and Plans for the Future NUCLEAR REACTIONS 12C(48Ca, X)8Li/9Li/25Na/26Na/27Na/29Al/37K/47K, E=60 MeV/nucleon; measured yield.
doi: 10.1016/j.nuclphysa.2006.12.023
2006DU03 Phys.Rev. C 73, 014605 (2006) M.Dupuis, S.Karataglidis, E.Bauge, J.P.Delaroche, D.Gogny Correlations in microscopic optical model for nucleon elastic scattering off doubly closed-shell nuclei NUCLEAR STRUCTURE 16O, 40,48Ca, 208Pb; calculated neutron and proton radii. Hartree-Fock plus RPA approach, comparison with data. NUCLEAR REACTIONS 208Pb(polarized p, p), E=40-201 MeV; calculated σ(θ), Ay(θ); 16O, 40,48Ca(p, p), E ≈ 200 MeV; calculated σ(θ); deduced role of long-range correlations. Hartree-Fock plus RPA approach, comparison with data.
doi: 10.1103/PhysRevC.73.014605
Back to query form |