NSR Query Results
Output year order : Descending NSR database version of May 2, 2024. Search: Author = D.Paya Found 24 matches. 1995BL01 Nucl.Phys. A582, 296 (1995) J.Blons, D.Goutte, A.Lepretre, R.Letourneau, R.Lucas, V.Meot, D.Paya, X.H.Phan, J.Girard, G.Barreau, T.P.Doan, G.Pedemey, Ph.Dessagne, Ch.Miehe A New Isomeric State in 65Ni NUCLEAR REACTIONS 64Ni(18O, 17O), E=72 MeV; measured Eγ, pγ-coin. 65Ni deduced levels, T1/2.
doi: 10.1016/0375-9474(94)00448-V
1988BL03 Nucl.Phys. A477, 231 (1988) J.Blons, B.Fabbro, C.Mazur, D.Paya, M.Ribrag, Y.Patin High Resolution Fission Probabilities for 229,230,232Th(d, pf) and 233,236U(d, pf) Reactions NUCLEAR REACTIONS 229,230,232Th, 233,236U(d, pF), E=11.5-14 MeV; measured fission fragment σ(E(p), θ). 230,231,233Th, 237U deduced triple-humped fission barriers, rotational levels, inertia parameters.
doi: 10.1016/0375-9474(88)90320-X
1986BL11 Radiat.Eff. 92, 311 (1986) J.Blons, B.Fabbro, J.M.Hisleur, C.Mazur, Y.Patin, D.Paya, M.Ribrag High Resolution Fission Probabilites for 229,230,232Th and 233,236U in (d, pf) Reactions NUCLEAR REACTIONS 229,230,232Th, 233,236U(d, pF), E=11, 12.5, 13 MeV; measured fission probability vs excitation, σ(fragment θ). 230,231,233Th, 234,237U deduced fission characteristics.
doi: 10.1080/00337578608208341
1984BL04 Nucl.Phys. A414, 1 (1984) J.Blons, C.Mazur, D.Paya, M.Ribrag, H.Weigmann On the Existence of Triple-Humped Fission Barriers in 231,233Th NUCLEAR REACTIONS 230Th(n, F), E=0.7-2.2 MeV; 232Th(n, F), E=1-12 MeV; measured fission σ(E), fragment anisotropy. 231,233Th deduced triple-humped fission barrier parameters, two rotational bands, associated moment of inertia parameter.
doi: 10.1016/0375-9474(84)90494-9
1984FA08 J.Phys.(Paris), Lett. 45, L-843 (1984) B.Fabbro, J.Blons, A.Greiner, J.M.Hisleur, C.Mazur, Y.Patin, D.Paya, M.Ribrag Observation of New States in the Third Well of the 231Th Fission Barrier NUCLEAR REACTIONS 230Th(d, pF), E=12 MeV; measured fission fragment σ(θ), fission probability. 231Th deduced fission barrier third well states, J, π, rotational bands.
doi: 10.1051/jphyslet:019840045017084300
1980GE12 J.Phys.(Paris), Colloq.C-10, 239 (1980) C.Gerschel, N.Perrin, L.Valentin, H.Tricoire, B.Ader, D.Paya How Fast α Particles are Emitted in Massive Transfer Reactions < Question > NUCLEAR REACTIONS 116Sn(16O, α), E=125 MeV; 92Zr(40Ar, α), E=193 MeV; measured σ(Eα), γα-coin, γ-multiplicity. 132Ce deduced α-decay mechanisms.
1979GE01 Nucl.Phys. A317, 473 (1979) C.Gerschel, M.A.Deleplanque, M.Ishihara, C.Ngo, N.Perrin, J.Peter, B.Tamain, L.Valentin, D.Paya, Y.Sugiyama, M.Berlanger, F.Hanappe Angular Momentum Transfer in Deep Inelastic Collisions for the Ar + Au and Cu + Au Systems NUCLEAR REACTIONS Au(Ar, X), E=227 MeV; Au(63Cu, X), E=365, 443 MeV; measured γ-ray multiplicities of the hot fragments; deduced L-transfer. Comparison with theory.
doi: 10.1016/0375-9474(79)90493-7
1979TR10 J.Phys.(Paris), Lett. 40, L-181 (1979) H.Tricoire, P.Colombani, C.Gerschel, D.Paya, N.Perrin, L.Valentin, N.Frascaria, J.P.Garron, C.Stephan New Experimental Results Supporting the Hypothesis of the Excitation of Collective Modes in the 40Ca + 40Ca Reaction NUCLEAR REACTIONS 40Ca(40Ca, X), E=400 MeV; measured σ(fragment E, θ), γ-multiplicity vs excitation energy for fragment Z=17, 18; deduced evidence for collective mode excitation.
doi: 10.1051/jphyslet:01979004008018100
1978BL01 Phys.Rev.Lett. 41, 1282 (1978) J.Blons, C.Mazur, D.Paya, M.Ribrag, H.Weigmann Rotational Bands in Asymmetrically Deformed 231Th NUCLEAR REACTIONS 230Th(n, F), E=680-760 keV; measured σ(E), absolute σ. 231Th deduced levels, K, J, π.
doi: 10.1103/PhysRevLett.41.1282
1976BE52 J.Phys.(Paris), Lett. 37, L-323 (1976) M.Berlanger, M.A.Deleplanque, C.Gerschel, F.Hanappe, M.Leblanc, J.F.Mayault, C.Ngo, D.Paya, N.Perrin, J.Peter, B.Tamain, L.Valentin Gamma Ray Multiplicity in the Quasi-Fission of Cu + Au at 443 MeV NUCLEAR REACTIONS 197Au(63Cu, X), E=443 MeV; measured γ-ray multiplicity associated with quasi-fission, sequential fission.
doi: 10.1051/jphyslet:019760037012032300
1976PL04 Nucl.Sci.Eng. 61, 477 (1976) Fission Cross Section of Neptunium-237 from 3 eV to 2 MeV NUCLEAR REACTIONS 237Np(n, F), E=3 eV-2 MeV; measured σ(E). 238Np deduced resonances, resonance parameters.
doi: 10.13182/NSE76-A14485
1975BL08 Phys.Rev.Lett. 35, 1749 (1975) Evidence for Rotational Bands Near the 232Th(n, f) Fission Threshold NUCLEAR REACTIONS 232Th(n, F), E=5 MeV; measured σ(fragment mass, θ). 233Th deduced levels, K, J.
doi: 10.1103/PhysRevLett.35.1749
1973PA22 Bull.Inform.Sci.Tech.(Paris) No.179, 95 (1973) Recherche Fondamentale sur le Processus de Fission au C.E.N. De Saclay RADIOACTIVITY, Fission 252Cf(SF); measured neutron multiplicity. NUCLEAR REACTIONS, Fission 237Np, 239Pu(n, Fγ); measured σ(E, Eγ), neutron multiplicity, σ(E(X)), σ(Eα).
1973TR10 J.Phys.(Paris) 34, 131 (1973) J.Trochon, B.Lucas, A.Michaudon, D.Paya, Y.Ryabov Mesure des Variations du Nombre Moyen ν-Bar de Neutrons Prompts Emis Lors de la Fission de 239Pu Induite par des Neutrons de Resonances NUCLEAR REACTIONS, Fission 239Pu(n, F), E=resonant; measured neutron multiplicity(E).
doi: 10.1051/jphys:01973003402-3013100
1972LO02 J.Phys.(Paris) to Be Published (1972); see 1971Lo26 Etude des Spectres de Rayons 3 Emis Apres la Capture de Neutrons de Resonance par les Isotopes de l'Antimoine
1971LO26 J.Phys.(Paris) 32, 849 (1971) Etude des Spectres de Rayons γ Emis Apres la Capture de Neutrons de Resonance par les Isotopes de l'Antimoine NUCLEAR REACTIONS 121,123Sb(n, γ), E=resonance; measured Eγ, Iγ. 122,124Sb deduced resonances, level-width, J, π, γ-multipolarity.
doi: 10.1051/jphys:019710032011-12084900
1968AS04 Phys.Letters 26B, 664 (1968) An Attempt to Determine the Spins of 235U Slow Neutron Resonances NUCLEAR STRUCTURE 235U; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0370-2693(68)90383-3
1968PA17 Proc.Intern.Symp.Nucl.Struct., Dubna, Intern.At.Energy Agency, Vienna, p.483 (1968) D.Paya, J.Blons, A.Fubini, A.Michaudon The Intermediate Structure Observed in the Fission Cross-Sections of 237Np and Possibly of 239Pu NUCLEAR REACTIONS 237Np(n, F), E=10-2000 eV; 239Pu(n, F), E=0.5-4 keV; measured σ(E); deduced intermediate structure in subthreshold fission. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset20447. 1966GO38 Phys.Rev. 151, 912 (1966) W.M.Good, D.Paya, R.Wagner, T.Tamura Total Cross Sections for Kilovolt Neutrons of Even-Odd Nuclei in the Region of the 3s Strength-Function Resonances NUCLEAR REACTIONS 42Ca, 47,49Ti, 53Cr, 57Fe, 61Ni, 63,65Cu(n, n), E=30-60 keV; measured σ(E). 43Ca, 48,50Ti, 54Cr, 58Fe, 62Ni, 64,66Cu deduced resonances, J, Γn, s-wave strength function.
doi: 10.1103/PhysRev.151.912
1964GO13 WASH-1048, p.77 (1964) Total Cross Section Measurements on Ca40, Ca43, Fe57, Ni61,62,64, Cu63,65 NUCLEAR STRUCTURE 63Ni, 65Ni, 41Ca; measured not abstracted; deduced nuclear properties.
1964GO23 ORNL-3778, p.69 (1964) Study of the Even-Even Compound Nuclei at the First s-Wave Strength Function Resonance
1964PA09 WASH-1048, p.69 (1964) D.Paya, K.D.Pearce, J.A.Harvey, G.G.Slaughter Parameters of Low Energy Resonances in Tungsten NUCLEAR STRUCTURE 184W, 183W, 187W; measured not abstracted; deduced nuclear properties.
1964PA15 ORNL-3582, p.58 (1964) D.Paya, K.D.Pearce, J.A.Harvey, G.G.Slaughter Parameters of Low Energy Resonances in Tungsten NUCLEAR STRUCTURE 183W, 184W, 187W; measured not abstracted; deduced nuclear properties. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset11238. 1961NI10 J.Phys.Radium 22, 714 (1961) H.Nifenecker, Y.Hazoni, A.Michaudon, D.Paya NUCLEAR STRUCTURE 233Th; measured not abstracted; deduced nuclear properties.
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