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NSR database version of April 11, 2024.

Search: Author = M.Dupuis

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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
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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22795. Data from this article have been entered in the XUNDL database. For more information, click here.


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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset23769.


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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2584. Data from this article have been entered in the XUNDL database. For more information, click here.


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
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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
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2017DU06      Eur.Phys.J. A 53, 111 (2017)

M.Dupuis

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
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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
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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
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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
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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 Green¬Ěs 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
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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
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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
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Data from this article have been entered in the XUNDL database. For more information, click here.


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
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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
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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
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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
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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
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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
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2011MA18      Phys.Rev. C 83, 034309 (2011)

M.Martini, S.Peru, M.Dupuis

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
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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
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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset32684.


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
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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
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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
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