NSR Query Results
Output year order : Descending NSR database version of April 29, 2024. Search: Author = G.Mouze Found 36 matches. 2008MO19 Int.J.Mod.Phys. E17, 2240 (2008) New arguments in favor of an intermediary nucleon phase in binary fission
doi: 10.1142/S0218301308011410
2004MO39 Eur.Phys.J. A 21, 179 (2004) Relativistic effects in ternary fission RADIOACTIVITY 252Cf(SF); calculated light particle kinetic energy in ternary fission, relativistic effects. Comparison with data.
doi: 10.1140/epja/i2003-10197-8
2002MO26 Europhys.Lett. 58, 363 (2002) Cluster-Fission, a New Fission Mode NUCLEAR STRUCTURE 286Cn, 292Fl, 296Lv, 294Og, 306122; calculated cluster-fission decay modes, Coulomb barriers.
doi: 10.1209/epl/i2002-00647-9
2001HA56 Chin.Phys.Lett. 18, 1454 (2001) Is the Double Giant Dipole Resonance Process Responsible for Alpha Emission in Ternary Fission ? RADIOACTIVITY 252Cf(SF); calculated α-spectra from ternary fission; deduced role of double GDR. Monte Carlo approach, comparison with data.
doi: 10.1088/0256-307X/18/11/309
2001MO23 Europhys.Lett. 54, 7 (2001) On the Energy Shift of the 21+-00+ Transition of 10Be Emitted in the Ternary Fission of 252Cf RADIOACTIVITY 252Cf(SF); calculated energy shift in de-excitation of 10Be ternary fission fragment.
doi: 10.1209/epl/i2001-00275-y
2000MO32 J.Radioanal.Nucl.Chem. 246, 191 (2000) Why Does 258Fm Fission Symmetrically ? NUCLEAR STRUCTURE 256,258,264Fm; analyzed data; deduced fission fragment mass distribution features. Cluster model.
doi: 10.1023/A:1006798912943
2000MO33 Eur.Phys.J. A 9, 365 (2000) On the 34Si Emission of 242Cm RADIOACTIVITY 242Cm(34Si), (SF); calculated 34Si-decay spectrum, fission fragment kinetic energy. Observation of 34Si due to cluster emission or ternary fission discussed.
doi: 10.1007/s100500070021
1998MO23 Nuovo Cim. 111A, 281 (1998) Second Mode of Fission of 252Cf: Role of the 146Ba-106Mo Mass Split RADIOACTIVITY 252Cf(SF); analyzed fission fragments yields; deduced anomaly, cluster emission role.
1998MO32 Nuovo Cim. 111A, 467 (1998) On the Two Modes of Cluster Emission Accompanying Nuclear Fission RADIOACTIVITY 252Cf(SF); calculated ternary fission cluster formation features; deduced cluster emission from fission fragments.
1997DR03 Nucl.Phys. A614, 137 (1997) S.Drissi, P.A.Tercier, H.G.Borner, M.Deleze, F.Hoyler, S.Judge, J.Kern, S.J.Mannanal, G.Mouze, K.Schreckenbach, J.P.Vorlet, N.Warr, A.Williams, C.Ythier The 112Cd Laboratory: An extension. E0 strengths, multiphonon states and coupled vibrations NUCLEAR REACTIONS 110Pd(α, 2nγ), E=12.2, 14.9, 16.2, 18 MeV; measured Eγ, Iγ, σ(E, Eγ), γγ-coin. 111Cd(n, γ), E=thermal; measured Eγ, Iγ, I(ce); deduced Q. 112Cd deduced levels, J, π, B(λ). Enriched targets, Compton suppressed Ge detectors, pair-spectrometer, curved-crystal spectrometer, magnetic spectrometer. Interacting boson model.
doi: 10.1016/S0375-9474(96)00451-4
1997MO15 Nuovo Cim. 110A, 119 (1997); Erratum Nuovo Cim. 110A, 563 (1997) Alpha-Particle Emission in Ternary Fission RADIOACTIVITY 252Cf(SF); analyzed α-accompanied fission data; deduced spherical clusters role. Cluster model of fission.
1997MO32 Nuovo Cim. 110A, 665 (1997) On the Second Mode of Spontaneous Fission of 252Cf RADIOACTIVITY 252Cf(SF); analyzed data; deduced cluster role in fission dynamics.
1997MO40 Nuovo Cim. 110A, 769 (1997) On Some Properties of the α-Decay of the Double Giant Dipole Resonance of Fissioning Nuclei RADIOACTIVITY 252Cf(SF); analyzed α-accompanied fission data; deduced evidence for double giant dipole resonance decay.
1997MO41 Nuovo Cim. 110A, 1097 (1997) On the Alpha- and Cluster-Decays of the Double Giant Dipole Resonance of Fissioning Nuclei
doi: 10.1007/BF03035951
1996MO10 Nuovo Cim. 109A, 445 (1996) On the Non-Statistical Component of the Fission γ-Ray Spectrum of 252Cf NUCLEAR STRUCTURE 252Cf; analyzed asymmetric fission non-statistical γ spectra; deduced dicluster molecules rearrangement role, cataclysmic valence nucleons transfer in 132Sn.
doi: 10.1007/BF02731093
1996MO20 Nuovo Cim. 109A, 527 (1996) Does a Neutron-Proton Pairing Energy Exist ( Question ) NUCLEAR STRUCTURE 40Ca; calculated pn-, 2pn-, 2p2n-interaction energy variation; deduced true np-interaction, np-pairing energies could have different properties.
doi: 10.1007/BF02731135
1994MO06 Nuovo Cim. 107A, 461 (1994) 214Po Nuclear States Fed in 214Bi Decay RADIOACTIVITY 214Bi(β-); measured γγ-coin, Eγ, Iγ; deduced log ft. 214Po deduced levels, β-branching.
doi: 10.1007/BF02831449
1994MO37 Nuovo Cim. 107A, 1565 (1994) On Some Properties of the Valence Bosons NUCLEAR STRUCTURE 16,22O, 22,28,34Si, 40Ca; calculated proton, neutron pairing energies. 23,25,27,29,31,33,35,37Si, 42,44,46,48,41,43,45,47,49Ca; calculated from-core detachment energies variations; deduced valence bosons characteristics.
doi: 10.1007/BF02780691
1993DI09 Nuovo Cim. 106A, 1321 (1993) O.Diallo, G.Mouze, C.Ythier, J.F.Comanducci Recherche de Niveaux de Haute Energie de 214Po et 210Pb par Coincidence, et Coincidence et Addition RADIOACTIVITY 226Ra(α); measured γγ-coin, sum spectra of daughter nuclei. 214Po, 210Pb deduced levels, deexcitation features.
doi: 10.1007/BF02785621
1993MO09 Nuovo Cim. 106A, 715 (1993) Asymmetric Fission at Relativistic Energies NUCLEAR STRUCTURE 238U; analyzed asymmetric fission; deduced high energy Coulomb excitation role. Relativistic 238U ions on Pb target.
doi: 10.1007/BF02787241
1993MO16 Nuovo Cim. 106A, 835 (1993) Prompt Neutron Emission and the Second Step of Asymmetric Nuclear Fission NUCLEAR REACTIONS 235U(n, F), E=thermal; calculated second-step reaction energy release following fission. RADIOACTIVITY 236U(SF); calculated second-step reaction energy release following fission.
doi: 10.1007/BF02771497
1993MO21 Nuovo Cim. 106A, 885 (1993) G.Mouze, S.Bidegainberry, A.Rocaboy, C.Ythier The Neutron-Proton Interaction Energy of the Valence Nucleons. III. - The Valence Shells of 40Ca NUCLEAR STRUCTURE A=42-56; calculated neutron-proton interaction energies; deduced shell closure effect role, anomaly features.
doi: 10.1007/BF02786659
1993MO22 Nuovo Cim. 106A, 961 (1993) On the Symmetric Mass Division of Some Trans-Bk Nuclei NUCLEAR STRUCTURE 259Lr; calculated fission fragment mass yield curve. 259,258Fm, 258,262No, 260Md; calculated symmetric mass division following fission; deduced nuclear matter phase change possibility consequences.
doi: 10.1007/BF02786663
1992MO08 Nuovo Cim. 105A, 55 (1992) The Neutron-Proton Interaction Energy of the Valence Nucleons. II. - The Valence Shell of 4He NUCLEAR STRUCTURE A=5-16; analyzed visualization of valence shell energetic organization. 7Li, 214Bi; calculated possible valence nucleons radial distributions. Empirical mass formula.
doi: 10.1007/BF02730739
1992MO09 Nuovo Cim. 105A, 105 (1992) G.Mouze, S.Bidegainberry, C.Ythier The Visualization of the Energetic Structure of Nuclear Molecules NUCLEAR STRUCTURE A=16-24; analyzed visualization of valence shell energetic organization. A=210-224; analyzed level data; deduced valence neutron pairs role. Nuclear molecules, clusters, chemical concepts.
doi: 10.1007/BF02730743
1991MO22 Nuovo Cim. 104A, 1525 (1991) New Points of View on the Symmetric Fission of 258Fm RADIOACTIVITY 259,258Fm, 262,256No, 260Md(SF); analyzed SF-decay data; deduced symmetric fission features, phase change role.
doi: 10.1007/BF02817435
1990DI02 Nucl.Instrum.Methods Phys.Res. A286, 379 (1990) O.Diallo, G.Mouze, P.Bechlitch, J.F.Comanducci, P.Abela, C.Ythier A New Method for the Detection and Visualization of Nuclear Levels RADIOACTIVITY 108mAg(β+), (EC), (β-); 226Ra(α); 214Bi(α), (β-) [from 226Ra(α) decay chain]; measured γ-sum coincidence spectra. 108Pd deduced level decay features. 214Bi deduced level. 214Po deduced levels, J, π. Multi-detector spectrometer.
doi: 10.1016/0168-9002(90)90882-7
1990MO08 Radiochim.Acta 49, 13 (1990) G.Mouze, O.Diallo, P.Bechlitch, J.F.Comanducci, C.Ythier On the Level Scheme of 214Bi and the α Decay of 218At RADIOACTIVITY 214Pb(β-), 218At(α) [from 226Ra-decay chain]; measured γγ-coin. 214Bi deduced levels.
1990MO11 Nuovo Cim. 103A, 105 (1990) On the Interactions between Nucleons in the Valence Shells of Trans-208Pb Nuclei NUCLEAR STRUCTURE 210,212,214Po, 214,216,218,220Rn, 216,218,218,220,222,224,226Ra, 220,222,224,226,228,230,232Th, 230,232,234,236,238U, 210,212,214Bi, 212,214,216,218At, 214,216,218,220,222,224Fr; calculated proton-neutron interaction energy. Extension of N(p)N(n) scheme.
doi: 10.1007/BF02902623
1990MO12 Nuovo Cim. 103A, 131 (1990) On Some Consequences of the Interaction Laws Holding in the Valence Shells of Trans-208Pb Nuclei NUCLEAR STRUCTURE 210,212Pb, 210,212,214Po, 212,214,216,218Rn, 214,216,218,220Ra, 220,222,224Th; analyzed level ratio variation. 214Po; analyzed γγ-coin data; deduced level J, π.
doi: 10.1007/BF02902624
1990MO26 Nuovo Cim. 103A, 1467 (1990) The Neutron-Proton Interaction Energy of the Valence Nucleons. I. - The Valence Shells of 16O NUCLEAR STRUCTURE 16O; calculated valence shell np-interaction energy.
doi: 10.1007/BF02820574
1990MO27 Nuovo Cim. 103A, 1499 (1990) The Structure of the Neutron-Halo Nuclei NUCLEAR STRUCTURE 11Be; calculated valence nucleon interaction energies, radial distributions.
doi: 10.1007/BF02820578
1990MO41 Rev.Roum.Phys. 35, 337 (1990) G.Mouze, C.Ythier, J.F.Comanducci Etude des niveaux excites de 214Po formes par desintegration beta de 214Bi
1982AK03 Radiochem.Radioanal.Lett. 51, 1 (1982) H.Akcay, G.Mouze, D.Maillard, Ch.Ythier Analyse du Rayonnement Gamma d'une Source de Radium 226 en Equilibre avec ses Derives entre 150 et 1000 keV RADIOACTIVITY 226Ra; measured Eγ, Iγ following α-decay, β-decay.
1981MO27 Compt.Rend.Acad.Sci., Ser.II 293, 795 (1981) Sur la Desexcitation du Polonium-214 Forme dans la Desintegration Beta du Bismuth-214 RADIOACTIVITY 214Bi(β-); measured Eγ, Iγ, γγ-coin following β-decay. 214Po deduced levels, γ-branching.
1981MO28 Compt.Rend.Acad.Sci., Ser.II 292, 1243 (1981) Etude du Rayonnement γ d'Une Source de Radium en Equilibre aves Ses Derives, entre 1 et 2 MeV RADIOACTIVITY 226Ra(α); measured Eγ, Iγ. Ge(Li) detector.
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