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NSR database version of May 24, 2024.

Search: Author = H.Goutte

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2016CL01      Phys.Rev.Lett. 116, 022701 (2016)

E.Clement, M.Zielinska, A.Gorgen, W.Korten, S.Peru, J.Libert, H.Goutte, S.Hilaire, B.Bastin, C.Bauer, A.Blazhev, N.Bree, B.Bruyneel, P.A.Butler, J.Butterworth, P.Delahaye, A.Dijon, D.T.Doherty, A.Ekstrom, C.Fitzpatrick, C.Fransen, G.Georgiev, R.Gernhauser, H.Hess, J.Iwanicki, D.G.Jenkins, A.C.Larsen, J.Ljungvall, R.Lutter, P.Marley, K.Moschner, P.J.Napiorkowski, J.Pakarinen, A.Petts, P.Reiter, T.Renstrom, M.Seidlitz, B.Siebeck, S.Siem, C.Sotty, J.Srebrny, I.Stefanescu, G.M.Tveten, J.Van de Walle, M.Vermeulen, D.Voulot, N.Warr, F.Wenander, A.Wiens, H.De Witte, K.Wrzosek-Lipska

Spectroscopic Quadrupole Moments in 96, 98Sr: Evidence for Shape Coexistence in Neutron-Rich Strontium Isotopes at N=60

NUCLEAR REACTIONS 109Ag, 120Sn(96Sr, 96Sr'), E=275 MeV;60Ni, 208Pb(98Sr, 98Sr'), E=276 MeV; measured reaction products, Eγ, Iγ. 96,98Sr; deduced B(E2) and B(M1)values, spectroscopic quadrupole moments. Comparison with beyond-mean-field calculations using the Gogny D1S interaction, least squares fitting code GOSIA.

NUCLEAR STRUCTURE 96,98Sr; calculated B(E2) values with the Gogny D1S interaction in a five-dimensional collective Hamiltonian (5DCH) formalism.

doi: 10.1103/PhysRevLett.116.022701
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2016CL03      Phys.Rev. C 94, 054326 (2016)

E.Clement, M.Zielinska, S.Peru, H.Goutte, S.Hilaire, A.Gorgen, W.Korten, D.T.Doherty, B.Bastin, C.Bauer, A.Blazhev, N.Bree, B.Bruyneel, P.A.Butler, J.Butterworth, J.Cederkall, P.Delahaye, A.Dijon, A.Ekstrom, C.Fitzpatrick, C.Fransen, G.Georgiev, R.Gernhauser, H.Hess, J.Iwanicki, D.G.Jenkins, A.C.Larsen, J.Ljungvall, R.Lutter, P.Marley, K.Moschner, P.J.Napiorkowski, J.Pakarinen, A.Petts, P.Reiter, T.Renstrom, M.Seidlitz, B.Siebeck, S.Siem, C.Sotty, J.Srebrny, I.Stefanescu, G.M.Tveten, J.Van de Walle, M.Vermeulen, D.Voulot, N.Warr, F.Wenander, A.Wiens, H.De Witte, K.Wrzosek-Lipska

Low-energy Coulomb excitation of 96, 98Sr beams

NUCLEAR REACTIONS 60Ni, 208Pb(98Sr, 98Sr'), E=276.3 MeV; 109Ag, 120Sn(96Sr, 96Sr'), E=275.5 MeV; measured Eγ, Iγ, scattered Sr ions and target recoils, (particle)γ-coin, γ(θ), differential Coulomb excitation cross sections using Miniball array for γ detection and Si strip detectors for ions at REX-ISOLDE-CERN facility. 96,98Sr; deduced levels, E2 and M1 matrix elements, B(E2) and level half-lives, quadrupole moments and deformation parameters, E0 monopole transition strengths using GOSIA2 analysis. Comparison with previous experimental data and five-dimensional collective Hamiltonian and Gogny D1S force, and using complex excited VAMPIR approach. Systematics of level energies, transitional and spectroscopic quadrupole moments in 94,96Kr, 96,98Sr, 98,100Zr, 100,102Mo. Systematics of energy and B(E2) for first 2+ state, and energies of second 0+ states in 90,92,94,96,98,100,102Sr. 60Ni, 208Pb(98Rb, 98Rb'), E=276 MeV; measured Eγ, Iγ, scattered Rb ions and target recoils, (particle)γ-coin, γ(θ), level half-lives by recoil-distance Doppler shift method. 98Rb; deduced levels.

doi: 10.1103/PhysRevC.94.054326
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2012PA40      Phys.Rev. C 86, 064601 (2012)

S.Panebianco, J.-L.Sida, H.Goutte, J.-F.Lemaitre, N.Dubray, S.Hilaire

Role of deformed shell effects on the mass asymmetry in nuclear fission of mercury isotopes

RADIOACTIVITY 180,198Hg, 235U(SF); calculated minimum absolute available energy at scission for all possible fragmentations, symmetric and asymmetric fission. Microscopic scission-point model.

doi: 10.1103/PhysRevC.86.064601
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2011BE35      Phys.Rev. C 84, 044308 (2011)

R.Bernard, H.Goutte, D.Gogny, W.Younes

Microscopic and nonadiabatic Schrodinger equation derived from the generator coordinate method based on zero- and two-quasiparticle states

NUCLEAR STRUCTURE 236U; calculated intrinsic excitations, collective modes. Generator coordinate method. Nuclear fission. Collective intrinsic Schrodinger model.

doi: 10.1103/PhysRevC.84.044308
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2011CL03      Int.J.Mod.Phys. E20, 415 (2011)

E.Clement, G.De France, J.M.Casandjian, A.Gorgen, W.Korten, E.Bouchez, A.Chatillon, A.Hurstel, Y.Le Coz, A.Obertelli, C.Theisen, J.N.Wilson, J.-P.Delaroche, M.Girod, H.Goutte, S.Peru, T.Czosnyka, J.Iwanicki, P.J.Napiorkowski, J.Srebrny, K.Wrzosek-Lipska, M.Zielinska, N.Bree, I.Stefanescu, J.Van De Walle, C.Andreoiu, P.A.Butler, R.-D.Herzberg, D.G.Jenkins, G.D.Jones, A.Petts, F.Becker, J.Gerl, W.N.Catford, C.N.Timis, G.Sletten, G.Georgiev, J.Ljungvall

Experimental measurement of the deformation through the electromagnetic probe: shape coexistence in exotic Kr and Sr isotopes

NUCLEAR REACTIONS 208Pb(72Kr, 72Kr'), (74Kr, 74Kr'), (76Kr, 76Kr'), (78Kr, 78Kr'), E=4.5 MeV/nucleon; 109Ag, 120Sn(96Sr, 96Sr'), E not given; measured reaction products, Eγ, Iγ. 72,74,76,78Kr, 96Sr; deduced static quadrupole moments, B(E2). Comparison with systematics and HFB calculations.

doi: 10.1142/S0218301311017806
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2010DE02      Phys.Rev. C 81, 014303 (2010)

J.-P.Delaroche, M.Girod, J.Libert, H.Goutte, S.Hilaire, S.Peru, N.Pillet, G.F.Bertsch

Structure of even-even nuclei using a mapped collective Hamiltonian and the D1S Gogny interaction

NUCLEAR STRUCTURE A=2-250; analyzed charge radii, two-particle separation energies, correlation energies, excitation energies, transition matrix elements, deformation parameters, and transition strengths using the Hartree-Fock-Bogoliubov theory by the generator coordinate method and mapped onto a five-dimensional collective quadrupole Hamiltonian. Calculated properties of 1712 even-even nuclei.Evaluated performance of the CHFB+5DCH theory based on the Gogny D1S interaction.

doi: 10.1103/PhysRevC.81.014303
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2010LI51      J.Phys.:Conf.Ser. 205, 012007 (2010)

J.Libert, J.-P.Delaroche, M.Girod, H.Goutte, S.Hilaire, S.Peru, N.Pillet, G.F.Bertsch

Microscopic study of low energy collective states in even-even nuclei: A prospective analysis of dynamical corrections to vibrational mass parameters

NUCLEAR STRUCTURE 110Ru; calculated levels, J, π, inertia moment, deformation. 150,152,154,156,158,160,162,164Gd;calculated low-lying levels, J, π, rotational band. Z=20-110; calculated even-even nuclei 0+, 2+ levels. GCM mapped onto 5-Dimensional Collective Quadrupole Hamiltonian with quadrupole constraints deduced from Cogny D1S force. Compared with data.

doi: 10.1088/1742-6596/205/1/012007
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2008DO07      Int.J.Mod.Phys. E17, 81 (2008)

A.Dobrowolski, H.Goutte, J.-F.Berger

Collective-dynamics effects in fission of 256, 258Fm isotopes

NUCLEAR REACTIONS 256,258Fm(n, F), E not given; calculated fragment mass distribution using Hartree-Fock-Bogoliubov method.

doi: 10.1142/S0218301308009574
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2008DU01      Phys.Rev. C 77, 014310 (2008)

N.Dubray, H.Goutte, J.-P.Delaroche

Structure properties of 226Th and 256, 258, 260Fm fission fragments: Mean-field analysis with the Gogny force

RADIOACTIVITY 226Th, 256,258,260Fm(SF); calculated potential energy surfaces, scission energies, scission configurations, scission lines, binding energies, neutron multiplicities, kinetic energies of fission fragments. 112Ru, 150Ce; calculated quadrupole moments, potential energy curves.

doi: 10.1103/PhysRevC.77.014310
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2008DU06      Int.J.Mod.Phys. E17, 72 (2008)

N.Dubray, H.Goutte, J.-F.Berger, J.-P.Delaroche

Fission fragment properties at scission with the Gogny force

RADIOACTIVITY 112Ru, 150Ce, 226Th, 256,258,260Fm(SF); calculated potential energy surfaces, nascent fission fragment structure properties, and fragment yields using the HFB approach.

doi: 10.1142/S0218301308009562
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2008PE10      Phys.Rev. C 77, 044313 (2008)

S.Peru, H.Goutte

Role of deformation on giant resonances within the quasiparticle random-phase approximation and the Gogny force

NUCLEAR STRUCTURE 26,28,30Si, 22,24,26,28Mg; calculated giant resonance energies, Hartree-Fock-Bogliubov potential energies, neutron and proton pairing energies, fractions of the isovector monopole, dipole and octupole EWSR. QRPA calculations using Gogny DIS effective force for Hartree-Fock-Bogoliubov and QRPA approximations. Comparison with experimental data.

doi: 10.1103/PhysRevC.77.044313
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2007BE35      Phys.Rev.Lett. 99, 032502 (2007)

G.F.Bertsch, M.Girod, S.Hilaire, J.-P.Delaroche, H.Goutte, S.Peru

Systematics of the First 2+ Excitation with the Gogny Interaction

NUCLEAR STRUCTURE A=4-244; calculated excitation energies, B(E2) and transition quadrupole moments using a microscopic theory with Gogny interaction.

doi: 10.1103/PhysRevLett.99.032502
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2007CA39      Phys.Atomic Nuclei 70, 1640 (2007)

N.Carjan, H.Goutte

Isospin dependence of scission-neutron multiplicities in Pu isotopes

NUCLEAR STRUCTURE 236,256Pu; calculated scission neutron multiplicities using the framework of sudden approximation.

doi: 10.1134/S1063778807090244
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2007CL02      Phys.Rev. C 75, 054313 (2007)

E.Clement, A.Gorgen, W.Korten, E.Bouchez, A.Chatillon, J.-P.Delaroche, M.Girod, H.Goutte, A.Hurstel, Y.Le Coz, A.Obertelli, S.Peru, Ch.Theisen, J.N.Wilson, M.Zielinska, C.Andreoiu, F.Becker, P.A.Butler, J.M.Casandjian, W.N.Catford, T.Czosnyka, G.de France, J.Gerl, R.-D.Herzberg, J.Iwanicki, D.G.Jenkins, G.D.Jones, P.J.Napiorkowski, G.Sletten, C.N.Timis

Shape coexistence in neutron-deficient krypton isotopes

NUCLEAR REACTIONS 208Pb(74Kr, 74Kr'), E=4.7 MeV/nucleon; 208Pb(76Kr, 76Kr'), E=4.4 MeV/nucleon; measured Eγ, Iγ and angular distributions; 74Kr, 76Kr; deduced level energies, J, π, B(E2), and shape coexistance. Coulomb excitation GOSIA analysis.

doi: 10.1103/PhysRevC.75.054313
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2007DO06      Int.J.Mod.Phys. E16, 431 (2007)

A.Dobrowolski, H.Goutte, J.-F.Berger

Microscopic determinations of fission barriers (mean-field and beyond)

NUCLEAR STRUCTURE 226Th, 238U; calculated potential energy vs deformation, fission barrier features.

doi: 10.1142/S0218301307005867
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2007PE24      Nucl.Phys. A788, 44c (2007)

S.Peru, H.Goutte, J.F.Berger

Giant and Pygmy Resonances within Axial-deformed QRPA with the Gogny Force

NUCLEAR STRUCTURE 26Ne, 24Mg, 28Si; calculated excited state, GMR, GDR and GQR energies, B(E1), B(E2); deduced subshell gap. Microscopic quasi-particle RPA approach, Gogny force, configuration mixing, comparison with data.

doi: 10.1016/j.nuclphysa.2007.01.047
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2007VE05      Phys.Rev. C 75, 051302 (2007)

N.Vermeulen, S.K.Chamoli, J.M.Daugas, M.Hass, D.L.Balabanski, J.P.Delaroche, F.de Oliveira-Santos, G.Georgiev, M.Girod, G.Goldring, H.Goutte, S.Grevy, I.Matea, P.Morel, B.S.Nara Singh, Yu.-E.Penionzkevich, L.Perrot, O.Perru, S.Peru, O.Roig, F.Sarazin, G.S.Simpson, Yu.Sobolev, I.Stefan, C.Stodel, D.T.Yordanov, G.Neyens

First isomeric quadrupole moment measured in fragmentation reactions: The case of 61Fem(9/2+)

NUCLEAR REACTIONS 9Be(64Ni, X)61Fe, E=64.6 MeV/nucleon; measured Eγ, Iγ and quadrupole moment of the 9/2+ isomeric state using time dependent perturbed angular momentum technique.

doi: 10.1103/PhysRevC.75.051302
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2006DE23      Nucl.Phys. A771, 103 (2006)

J.-P.Delaroche, M.Girod, H.Goutte, J.Libert

Structure properties of even-even actinides at normal and super deformed shapes analysed using the Gogny force

NUCLEAR STRUCTURE 226,228,230,232,234,236Th, 228,230,232,234,236,238,240,242U, 232,234,236,238,240,242,244,246Pu, 238,240,242,244,246,248,250Cm, 238,240,242,244,246,248,250,252,254,256Cf, 242,244,246,248,250,252,254,256,258Fm, 250,252,254,256,258,260,262No; calculated single-particle and pairing energies, potential energy surfaces, excitation energies, potential barrier heights, rotational bands kinetic moments of inertia, T1/2, J, π; deduced charge multipole moments. Hartree-Fock-Bogolyubov approach, Gogny force, comparison with data.

doi: 10.1016/j.nuclphysa.2006.03.004
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2006GO07      Int.J.Mod.Phys. E15, 292 (2006)

H.Goutte, J.-F.Berger, D.Gogny

Fission collective dynamics in a microscopic framework

NUCLEAR STRUCTURE 238U; calculated potential energy along scission line, fission fragments kinetic energies, charge and mass distributions, deformation. Time-dependent microscopic approach.

doi: 10.1142/S0218301306004120
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2005GO03      Phys.Rev. C 71, 024316 (2005)

H.Goutte, J.F.Berger, P.Casoli, D.Gogny

Microscopic approach of fission dynamics applied to fragment kinetic energy and mass distributions in 238U

NUCLEAR STRUCTURE 238U; calculated fission fragments kinetic energy and mass distributions, dynamical effects. Hartree-Fock-Bogoliubov and time-dependent generator coordinate methods.

doi: 10.1103/PhysRevC.71.024316
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2005OB01      Phys.Rev. C 71, 024304 (2005)

A.Obertelli, S.Peru, J.-P.Delaroche, A.Gillibert, M.Girod, H.Goutte

N = 16 subshell closure from stability to the neutron drip line

NUCLEAR STRUCTURE 22C, 24O, 26Ne, 28Mg, 30Si, 32S, 34Ar; calculated deformation, pairing energies, single-particle energies, first 2+ states energies and B(E2); deduced subshell gap. Mean-field approach, Gogny force, configuration mixing, comparisons with data.

doi: 10.1103/PhysRevC.71.024304
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2004GO19      Nucl.Phys. A734, 217 (2004)

H.Goutte, P.Casoli, J.-F.Berger

Mass and kinetic energy distributions of fission fragments using the Time Dependent Generator Coordinate Method

NUCLEAR REACTIONS 238U(n, F), E=1.7 MeV; calculated fission fragments kinetic energy and mass distributions. Time-dependent generator coordinate method, comparison with data.

doi: 10.1016/j.nuclphysa.2004.01.038
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2004MA80      Phys.Rev.Lett. 93, 142503 (2004)

I.Matea, G.Georgiev, J.M.Daugas, M.Hass, G.Neyens, R.Astabatyan, L.T.Baby, D.L.Balabanski, G.Belier, D.Borremans, G.Goldring, H.Goutte, P.Himpe, M.Lewitowicz, S.Lukyanov, V.Meot, F.de Oliveira Santos, Yu.E.Penionzhkevich, O.Roig, M.Sawicka

Magnetic Moment of the Fragmentation-Aligned 61Fe (9/2+) Isomer

NUCLEAR REACTIONS 9Be(64Ni, X)61Fe, E=54.7 MeV; measured Eγ, Iγ(θ, H, t). 61Fe deduced isomeric state T1/2, g factor. Time dependent perturbed angular distribution method.

RADIOACTIVITY 61mFe(IT) [from 9Be(64Ni, X)]; measured Eγ, Iγ(θ, H, t). 61Fe deduced isomeric state T1/2, g factor. Time dependent perturbed angular distribution method.

doi: 10.1103/PhysRevLett.93.142503
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