NSR Query Results
Output year order : Descending NSR database version of May 24, 2024. Search: Author = M.Verriere Found 7 matches. 2023SC05 Phys.Rev. C 107, 044312 (2023) N.Schunck, M.Verriere, G.Potel Aguilar, R.C.Malone, J.A.Silano, A.P.D.Ramirez, A.P.Tonchev Microscopic calculation of fission product yields for odd-mass nuclei NUCLEAR REACTIONS ^{236,238}U(n, F), E=2.2-7.2 MeV; calculated mass distribution of the light fission fragment before prompt emission, fission fragment mass distribution after neutron emission, ratio of neutron over proton numbers in the fission fragments, axial quadrupole and octupole deformation in the fission fragments, probability to populate a given spin projection. Hartree-Fock-Bogoliubov theory with Skyrme energy functionals combined with FREYA calculations. Comparison to available experimental data, GEF-2021/1.1 calculations and ENDF/B-VIII.0, JEFF-3.3, and JENDL-5 evaluations. NUCLEAR STRUCTURE ^{237,239}U; calculated levels, J, π, spectrum of quasi-bound states for each spin projection, potential energy curves in as a function of the axial quadrupole moment. Generator coordinate method with Gaussian overlap approximation.
doi: 10.1103/PhysRevC.107.044312
2021VE03 Phys.Rev. C 103, 034617 (2021) Improvements to the macroscopic-microscopic approach of nuclear fission NUCLEAR REACTIONS ^{233,235}U(n, F), E=thermal; calculated fission fragment charge yields, isobaric fragment charge yields and the independent charge yields after prompt neutron emission, fragment mass and charge yields before prompt neutron emission, scission probabilities. Semiclassical method based on the macroscopic finite-range liquid-drop model (FRLDM) with microscopic corrections or enhanced finite-range liquid-drop model (eFRLDM), with Lipkin-Nogami equations. Comparison with experimental data.
doi: 10.1103/PhysRevC.103.034617
2021VE05 Phys.Rev. C 103, 054602 (2021) M.Verriere, N.Schunck, D.Regnier Microscopic calculation of fission product yields with particle-number projection NUCLEAR REACTIONS ^{235}U, ^{239}Pu(n, F), E=0.5-10 MeV; calculated mass and charge distributions of fission fragments, odd-even staggering in the charge yields of fission fragments, two-dimensional isotopic fission yields as functions of charge and atomic mass, average neutron excess of fragments, isotopic yields. ^{236}U, ^{240}Pu; calculated potential energy surfaces (PES) in (Q_{20}, Q_{30}) planes as a function of the axial quadrupole and axial octupole moments using SkM* density functional. Microscopic collective model calculations of fission fragment distributions within the time-dependent generator coordinate method (TDGCM) under the Gaussian overlap approximation (GOA) framework, with the number of particles in fission fragments extracted from direct particle-number projection method. Comparison with experimental data.
doi: 10.1103/PhysRevC.103.054602
2020BE28 J.Phys.(London) G47, 113002 (2020) M.Bender, R.Bernard, G.Bertsch, S.Chiba, J.Dobaczewski, N.Dubray, S.A.Giuliani, K.Hagino, D.Lacroix, Z.Li, P.Magierski, J.Maruhn, W.Nazarewicz, J.Pei, S.Peru, N.Pillet, J.Randrup, D.Regnier, P.G.Reinhard, L.M.Robledo, W.Ryssens, J.Sadhukhan, G.Scamps, N.Schunck, C.Simenel, J.Skalski, I.Stetcu, P.Stevenson, S.Umar, M.Verriere, D.Vretenar, M.Warda, S.Aberg Future of nuclear fission theory
doi: 10.1088/1361-6471/abab4f
2020MU06 Phys.Rev. C 101, 054607 (2020) M.R.Mumpower, P.Jaffke, M.Verriere, J.Randrup Primary fission fragment mass yields across the chart of nuclides NUCLEAR REACTIONS ^{226}Th, ^{235}U, ^{259}Md, ^{276}No(n, F)^{227}Th/^{236}U/^{260}Md/^{277}No, T=0.5-1.5 MeV; ^{229}Th, ^{237}Np, ^{239}Pu, ^{245}Cm, ^{255,257}Fm(n, F)^{230}Th/^{238}Np/^{240}Pu/^{246}Cm/^{256}Fm/^{258}Fm, E^{*}=5.8-6.8 MeV; ^{205}At, ^{208}Rn, ^{209}Fr, ^{211}Ra, ^{216}Ac, ^{222}Th, ^{230}Pa, ^{233}U(n, F)^{206}At/^{209}Rn/^{210}Fr/^{212}Ra/^{217}Ac/^{223}Th/^{231}Pa/^{234}U, E^{*}=11 MeV; calculated mass yield distributions. ^{236}U, ^{240}Pu, ^{234}Cm; calculated projected potential energy surfaces. Z=80-130, A=171-330: calculated mass yield distributions for 3800 nuclei listed as tabular text files in the supplementary material. Finite-Range Liquid-Drop Model (FRLDM). Comparison with experimental data.
doi: 10.1103/PhysRevC.101.054607
2019VE06 Phys.Rev. C 100, 024612 (2019) M.Verriere, N.Schunck, T.Kawano Number of particles in fission fragments RADIOACTIVITY ^{240}Pu(SF); calculated mass, neutron and charge fragmentation probabilities for several scission configurations in ^{240}Pu using a macroscopic-microscopic approach or full Hartree-Fock-Bogoliubov calculations. Discussed two methods to estimate particle-number dispersion in fission fragments, Monte Carlo sampling of single-particle configurations, and extended standard projection techniques.
doi: 10.1103/PhysRevC.100.024612
2016RE10 Phys.Rev. C 93, 054611 (2016) D.Regnier, N.Dubray, N.Schunck, M.Verriere Fission fragment charge and mass distributions in ^{239}Pu (n, f) in the adiabatic nuclear energy density functional theory NUCLEAR REACTIONS ^{239}Pu(n, F), E=low; calculated pre-neutron emission charge and mass distributions of the fission fragments. Potential energy surfaces. Nuclear energy density functional (EDF) method, with the time-dependent generator coordinate method (TDGCM) and Gaussian overlap approximation (GOA). Comparison with available experimental data.
doi: 10.1103/PhysRevC.93.054611
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