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NSR database version of April 27, 2024.

Search: Author = G.Gosselin

Found 16 matches.

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2024GO03      Nuovo Cim. C 47, 46 (2024)

S.Goriely, S.Hilaire, S.Peru, G.Gosselin

A new approach to nuclear level densities: The QRPA plus boson expansion

NUCLEAR STRUCTURE 170,172Yb, 150Nd; calculated nuclear level densities with one boson expansion of QRPA excitations. Comparison with available data.

doi: 10.1393/ncc/i2024-24046-7
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2023LE05      Phys.Rev. C 107, 054609 (2023)

I.Lee, G.Gosselin, A.Diaz-Torres

Thermal and atomic effects on coupled-channels heavy-ion fusion

NUCLEAR REACTIONS 188Os(16O, X), E(cm)=65-78 MeV; calculated fusion probability in the presence of a thermal plasma environment, radial position probability as a function of internuclear radius and time for a head-on collision. Coupled-channels density-matrix method based on the theory of open quantum systems to include thermal and atomic effects on subbarrier fusion dynamics.

doi: 10.1103/PhysRevC.107.054609
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2022GO01      Phys.Rev. C 105, 014608 (2022)

F.Gobet, A.Ya.Dzyublik, G.Gosselin, V.Meot, M.Versteegen

Expected yields of 181Ta(e, e')181Ta* in the multi-keV range with a plasma-cathode electron beam

NUCLEAR REACTIONS 181Ta(e, e'), E=10-30 keV electron beam from a biased laser plasma; calculated inelastic excitation σ(E) using DWBA method in screened and unscreened Coulomb nuclear field, and compared with other theoretical calculations, energy distributions of the electrons impinging the anode, number of γ-ray photons and conversion electrons exiting the anode as a function of the tantalum anode thickness for various target voltages at various target voltages, nuclear excitation yields and DWBA σ(E) through the detection of conversion electrons for the 6.2-keV transition in 181Ta, and with the inclusion of effects of electron-beam heating and the plasma deposition on the tantalum target, number of nuclear excitations in tantalum anode as a function of the thickness of the aluminum layer. 181Ta; calculated internal-conversion coefficients and probability of electron emission for E1 transition using the code CATAR for the 6.2-keV transition in 181Ta.

doi: 10.1103/PhysRevC.105.014608
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2017DE22      Phys.Rev. C 96, 024604 (2017)

D.Denis-Petit, G.Gosselin, F.Hannachi, M.Tarisien, T.Bonnet, M.Comet, F.Gobet, M.Versteegen, P.Morel, V.Meot, I.Matea

Calculation of the rate of nuclear excitation by electron transition in an 84mRb plasma under the hypothesis of local thermodynamic equilibrium using a multiconfiguration Dirac-Fock approach

NUCLEAR REACTIONS 84mRb(γ, γ'), E=3.5 keV; calculated rate of nuclear excitation by electron transition (NEET) for the 6- to 5- transition in 84Rb as a function of the plasma temperature for the M1 and E2 components, total excitation rate, charge state distribution of an 84Rb plasma at 400 eV, M1 NEET rate as a function of the energy uncertainty and the charge state of 84Rb. Relativistic average atom model (RAAM), and multiconfiguration Dirac Fock (MCDF) atomic calculations using the ISOMEX computer code. 76Ge(11B, 3n)84Rb, E=40 MeV; measured Eγ, γγ-coin using the ORGAM Ge detector array at Orsay Tandem accelerator facility, precise energy of the 219-keV γ ray; deduced precise energy of 3.5-keV transition between the 466.6, 5- and 463.6, 6- levels.

RADIOACTIVITY 84mRb(IT)[from 85Rb(γ, n), E=bremsstrahlung photons from the ELSA electron beam facility of the CEA/DAM/DIF]; measured Eγ, Iγ, γγ-coin, precise energies of 215.6-, 248.0-, and 463.6-keV γ rays.

doi: 10.1103/PhysRevC.96.024604
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Data from this article have been entered in the XUNDL database. For more information, click here.


2015CO16      Phys.Rev. C 92, 054609 (2015)

M.Comet, G.Gosselin, V.Meot, P.Morel, J.-C.Pain, D.Denis-Petit, F.Gobet, F.Hannachi, M.Tarisien, M.Versteegen

Nuclear excitation by electron transition rate confidence interval in a 201Hg local thermodynamic equilibrium plasma

NUCLEAR REACTIONS 201Hg(γ, γ'), (e, e')201mHg; calculated average charge state as function of plasma temperature using relativistic average atom model (RAAM), nuclear excitation by electron transition (NEET) rates for excitation of 1.56-keV isomer in 201Hg as function of temperature and average charge state using average atom Gaussian (AAG) model and ADAM, E2 radiative spectrum with ADAM and CNFM approaches, and detailed configuration accounting (DCA).

doi: 10.1103/PhysRevC.92.054609
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2013DZ01      Europhys.Lett. 102, 62001 (2013)

A.Ya.Dzyublik, G.Gosselin, V.Meot, P.Morel

Role of screening in Coulomb excitation of nuclei by electrons in hot plasma

NUCLEAR REACTIONS 201Hg(E, E'), E<6 keV; calculated Coulomb excitation σ on the energy of incident electrons for different screening radii.

doi: 10.1209/0295-5075/102/62001
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2012BA38      Eur.Phys.J. A 48, 113 (2012)

E.Bauge, G.Belier, J.Cartier, A.Chatillon, J.M.Daugas, J.P.Delaroche, P.Dossantos-Uzarralde, H.Duarte, N.Dubray, M.Ducauze-Philippe, L.Gaudefroy, G.Gosselin, T.Granier, S.Hilaire, H.-T.P.Chau, J.M.Laborie, B.Laurent, X.Ledoux, C.Le Luel, V.Meot, P.Morel, B.Morillon, O.Roig, P.Romain, J.Taieb, C.Varignon, N.Authier, P.Casoli, B.Richard

Coherent investigation of nuclear data at CEA DAM: Theoretical models, experiments and evaluated data

NUCLEAR REACTIONS 175,176Lu(n, γ), E≈0.02-100 eV; measured Eγ, Iγ, γγ-coin; deduced σ, resonances. Compared with ENDF/B-VII.0 with SAMMY7. 176Lu(n, γ), E=80-40000 eV; measured Eγ, Iγ, γγ-coin; deduced σ. Compared with ENDF/B-VII.0 and other data. 174Lu(3He, p), E=60-600 keV; measured prompt and delayed Eγ, Iγ, γγ-coin; deduced γ ray emission probability vs energy; calculated γ ray emission probability using TALYS.177mLu(n, γ), (n, X), E=thermal; measured measured Eγ, Iγ, γγ-coin; deduced σ, resonance parameters. 239Pu(n, F), E not given; measured prompt En, In using FIGARO. Compared with other data, ENDF/B-VII and BRC evaluation. 2H(n, 2n), E=4-26 MeV; measured En, In using CARMEN; deduced σ. Compared with other data, ENDF/B-VII, Ac18, NJOY. 234U(n, F), E=0.15-1.2 MeV;236U(n, F), E=0.75-2.0 MeV;238U(n, F), E=0.01-1 MeV; calculated σ using TALYS. Compared with data. 238U(n, F), E=2, 2.9, 6.01, 7.02, 8.01, 8.94, 14.3, 14.7 MeV; calculated prompt fission σ(n, En). Compared with data. 239Pu(n, γ), (n, F), (n, n'), (n, 2n), (n, 3n), E=0.001-20 MeV; calculated σ, uncertainties, correlation matrix using BFMC.

doi: 10.1140/epja/i2012-12113-7
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2012PL01      Eur.Phys.J. A 48, 68 (2012)

C.Plaisir, F.Hannachi, F.Gobet, M.Tarisien, M.M.Aleonard, V.Meot, G.Gosselin, P.Morel, B.Morillon

Measurement of the 85Rb(γ, n)84mRb cross-section in the energy range 10-19 MeV with bremsstrahlung photons

NUCLEAR REACTIONS 85Rb(γ, n)84mRb, E=10-19 MeV; measured activation Eγ, Iγ from bremsstrahlung γ; deduced yields, σ, GDR parameters using GEANT4 and relative to 197Au(γ, n) and 63Cu(γ, n). Compared with other data.

doi: 10.1140/epja/i2012-12068-7
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetG0033.


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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2010GO10      Phys.Rev. C 81, 055808 (2010)

G.Gosselin, P.Morel, P.Mohr

Modification of nuclear transitions in stellar plasma by electronic processes: K isomers in 176Lu and 180Ta under s-process conditions

NUCLEAR STRUCTURE 176Lu, 180Ta; calculated transition rates enhancements for nuclear excitation by electron capture (NEEC) process for transitions between high-K, low-K and intermediate states, and partial half-lives as function of temperature in stellar plasma environment.

doi: 10.1103/PhysRevC.81.055808
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2010MO04      Phys.Rev. C 81, 034609 (2010)

P.Morel, V.Meot, G.Gosselin, G.Faussurier, C.Blancard

Calculations of nuclear excitation by electron capture (NEET) in nonlocal thermodynamic equilibrium plasmas

NUCLEAR REACTIONS 201Hg(e, e')201mHg, E=low; calculated rates of nuclear excitation of isomer by electron capture (NEET) in local thermodynamic equilibrium (LTE) and non-local thermodynamic equilibrium (NLTE) approaches. Discussed excitation of 1.65-keV isomer by laser techniques.

doi: 10.1103/PhysRevC.81.034609
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2009GO02      Phys.Rev. C 79, 014604 (2009)

G.Gosselin, N.Pillet, V.Meot, P.Morel, A.Ya.Dzyublik

Nuclear transition induced by low-energy unscreened electron inelastic scattering

NUCLEAR REACTIONS 110Ag, 201Hg(e, e'), E=1-100 keV; calculated σusing DWBA, PWBA, and WKB formalism.

doi: 10.1103/PhysRevC.79.014604
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2007GO37      Phys.Rev. C 76, 044611 (2007)

G.Gosselin, V.Meot, P.Morel

Modified nuclear level lifetime in hot dense plasmas

NUCLEAR STRUCTURE 93Mo, 201Hg; calculated variations in half-lives of isomeric states due to conditions in plasma. NEET process.

doi: 10.1103/PhysRevC.76.044611
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2007ME12      Phys.Rev. C 75, 064306 (2007)

V.Meot, J.Aupiais, P.Morel, G.Gosselin, F.Gobet, J.N.Scheurer, M.Tarisien

Half-life of the first excited state of 201Hg

RADIOACTIVITY 201Hg[from 201Tl(EC)]; measured Eγ, Iγ, eγ-coinc, T1/2 of the first excited state. 201Hg deduced B(M1) and B(E2).

doi: 10.1103/PhysRevC.75.064306
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Data from this article have been entered in the XUNDL database. For more information, click here.


2004GO53      Phys.Rev. C 70, 064603 (2004)

G.Gosselin, P.Morel

Enhanced nuclear level decay in hot dense plasmas

NUCLEAR STRUCTURE 93Mo, 237U; calculated excitation and decay rates in plasma environment.

RADIOACTIVITY 44Sc, 45Ti, 52Mn, 93Mo, 96,99Tc, 202,204Pb, 242Am(IT); calculated enhanced isomer decay rates in plasma environment.

doi: 10.1103/PhysRevC.70.064603
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2004MO49      Nucl.Phys. A746, 608c (2004)

P.Morel, J.M.Daugas, G.Gosselin, V.Meot, D.Gogny

Nuclear excitation by electronic processes: NEEC and NEET effects

doi: 10.1016/j.nuclphysa.2004.09.097
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