NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = J.Crancon Found 38 matches. 1991PI01 Phys.Rev. C43, 1331 (1991) L.Pienkowski, J.Jastrzebski, W.Kurcewicz, A.Gizon, J.Blachot, J.Crancon Interaction of 8-46 MeV/Nucleon 20Ne with Cu NUCLEAR REACTIONS, ICPND Cu(20Ne, X), E=8-46 MeV/nucleon; measured residuals production σ(E) for X=43K-77Kr, thick target yields; deduced reaction dynamics features.
doi: 10.1103/PhysRevC.43.1331
1989DJ01 Nucl.Phys. A496, 346 (1989) M.Djebara, M.Asghar, J.P.Bocquet, R.Brissot, J.Crancon, Ch.Ristori, E.Aker, D.Engelhardt, J.Gindler, B.D.Wilkins, U.Quade, K.Rudolph Mass and Nuclear-Charge Yields for 249Cf(n(th), F) at Different Fission-Product Kinetic Energies NUCLEAR REACTIONS 249Cf(n, F), E=thermal; measured light fission product mass, nuclear-charge distributions vs kinetic energies; deduced fractional independent yields, odd-even effects, mean kinetic energies of masses, elements and isotones.
doi: 10.1016/0375-9474(89)90179-6
1989HA42 Radiochim.Acta 46, 23 (1989) M.Haddad, J.Crancon, G.Lhospice, M.Asghar Post-Neutron Mass Distribution for 232U(n(th), f) NUCLEAR REACTIONS 232U(n, F), E=thermal; measured fission yields for Kr, Sr, Y, Zr, Mo, Sb, I, Te, Xe, Cs, La, Ce isotopes. γ-spectroscopy. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22119. 1989PI13 Z.Phys. A334, 315 (1989) L.Pienkowski, A.Lleres, H.Nifenecker, J.Blachot, J.Crancon, A.Gizon, M.Maurel, C.Ristori Influence of the Mass Asymmetry of the Entrance Channel on Incomplete Fusion Processes NUCLEAR REACTIONS 45Sc, Ca, Ti, Cu(40Ar, X), E=30 MeV/nucleon; Ti, Cu(32S, X), E=32 MeV/nucleon; measured σ(fragment θ), fragment velocity vs θ; deduced reaction mechanism c.m. velocities dependence.
1988HA17 Nucl.Phys. A481, 333 (1988) M.Haddad, J.Crancon, G.Lhospice, M.Asghar Post-Neutron Mass Distribution for 238Pu(n(th), f) NUCLEAR REACTIONS 238Pu(n, F), E=thermal; measured fission products mass distribution; deduced independent yields, proton odd-even effect.
doi: 10.1016/0375-9474(88)90500-3
1987BA28 Phys.Lett. 189B, 287 (1987) T.Batsch, J.Blachot, Q.Chen, J.Crancon, M.Fatyga, A.Gizon, J.Jastrzebski, H.Karwowski, W.Kurcewicz, A.Lleres, T.Mroz, L.Pienkowski, P.P.Singh, S.E.Vigdor, I.Zychor Target Mass Dependence of the Average Linear Momentum Transfer NUCLEAR REACTIONS Co, Cu, Ag(3He, X), (α, X), (14N, X), (20Ne, X), E=10-90 MeV/nucleon; measured σ, forward recoil ranges; deduced average transferred linear momentum. Thick-target-thick-catcher recoil range techniques.
doi: 10.1016/0370-2693(87)91433-X
1987HA43 Radiochim.Acta 42, 165 (1987) M.Haddad, J.Crancon, G.Lhospice, M.Asghar, J.Blachot Post-Neutron Mass Distribution of 229Th(n(th), f) NUCLEAR REACTIONS 229Th(n, F), E=thermal; measured light, heavy fission product yield vs mass. Activation technique. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset23702. 1986HA15 Radiat.Eff. 93, 17 (1986) M.Haddad, J.Crancon, Ch.Hamelin, G.Lhospice, M.Asghar, J.Blachot Post-Neutron Mass Distribution for 232U(n(th), f) NUCLEAR REACTIONS 235U(n, F)85Kr/85mKr/87Kr/88Kr/89Rb/91Sr/92Sr/93Y/94Y/95Zr/97Zr/99Mo/127Sb/129Sb/131I/132Te/133I/135Xe/138Cs/139Ba/140Ba/141Ce/142La/143Ce, E=thermal; measured fission fragment mass distribution, post-neutron residuals absolute mass yields.
doi: 10.1080/00337578608207419
1985BL13 Z.Phys. A321, 645 (1985) J.Blachot, J.Crancon, B.de Goncourt, A.Gizon, A.Lleres 124Sn Target Residues in the Interaction of Heavy Ions at Intermediate Energies NUCLEAR REACTIONS 124Sn(14N, X), (20Ne, X), (40Ar, X), E=10-70 MeV/nucleon; measured fragment mass yield for A=75-121; deduced residue σ(fragment E, mass) for X=111In, 125Xe.
doi: 10.1007/BF01432441
1983BE05 Z.Phys. A309, 253 (1983) D.Belhafaf, J.P.Bocquet, R.Brissot, Ch.Ristori, J.Crancon, H.Nifenecker, J.Mougey, V.S.Ramamurthy Kinetic Energy Distributions around Symmetric Thermal Fission of U234 and U236 NUCLEAR REACTIONS 233,235U(n, F), E=thermal; measured fission fragment kinetic energy vs mass. 234,236U deduced symmetric fission characteristics.
doi: 10.1007/BF01413757
1983LL01 Z.Phys. A312, 177 (1983) A.Lleres, J.Blachot, J.Crancon, A.Gizon, H.Nifenecker Heavy Fragment Energies and Angular Distributions in the Reaction of 86 MeV/Nucleon 12C with Medium-A Targets NUCLEAR REACTIONS Cu, 89Y, Ag, 112,118,124Sn(12C, X), E=86 MeV/nucleon; measured fragment yield vs mass, target residue recoil energies, σ(fragment θ); deduced reaction mechanism, production σ for 28Mg, 44,46,47Sc, 48Cr, 48V, 51Cr, 52,54Mn, 56,57,58Co. Thin target, thin catcher technique.
doi: 10.1007/BF01412161
1982KR11 Z.Phys. A306, 239 (1982) K.-L.Kratz, A.Schroder, H.Ohm, M.Zendel, H.Gabelmann, W.Ziegert, P.Peuser, G.Jung, B.Pfeiffer, K.D.Wunsch, H.Wollnik, C.Ristori, J.Crancon Beta-Delayed Neutron Emission from 93-100Rb to Excited States in the Residual Sr Isotopes. RADIOACTIVITY 93,94,95,96,97,98,99,100Rb [from 235U(n, F)]; measured Eγ, Iγ, β-delayed nγ-, βγ-, γγ-coin; deduced β-strength function role. 92,93,94,95,96,97,98Sr levels deduced delayed neutron branching ratios.
doi: 10.1007/BF01415126
1981BL11 Z.Phys. A301, 91 (1981) J.Blachot, J.Crancon, J.Genevey, A.Gizon, A.Lleres Mass, Charge, Angular and Energy Distributions in the Interaction of 84 MeV/A 12C with Silver and Tin NUCLEAR REACTIONS Ag(12C, X), E=84 MeV/nucleon; measured Eγ, Iγ, γ(X-ray)-coin; deduced σ(fragment θ, Z, mass), production σ(θ) for 52Mn, 48V, 71As, 87Y, 97Ru, reaction mechanism.
doi: 10.1007/BF01412469
1981BL15 Z.Phys. A303, 85 (1981) J.Blachot, J.Crancon, H.Nifenecker, A.Lleres, A.Gizon, J.Genevey Quasi-Compound Nucleus Formation with 84 MeV/N 12C Projectiles NUCLEAR REACTIONS Ag, 112,118,124Sn(12C, X), E=84 MeV/nucleon; measured σ(fragment θ, mass); deduced reaction mechanism. Evaporation model calculations.
doi: 10.1007/BF01420014
1981MA07 Nucl.Phys. A361, 213 (1981) G.Mariolopoulos, Ch.Hamelin, J.Blachot, J.P.Bocquet, R.Brissot, J.Crancon, H.Nifenecker, Ch.Ristori Charge Distributions in Low-Energy Nuclear Fission and Their Relevance to Fission Dynamics NUCLEAR REACTIONS, Fission 229Th(n, F), E=thermal; 235U(n, F), E=3 MeV; measured fragment charge distribution; deduced strong even-odd effects, pair breaking probability variation from saddle point to scission. RADIOACTIVITY, Fission 252Cf(SF); measured fragment charge distribution.
doi: 10.1016/0375-9474(81)90477-2
1980HA51 J.Phys.(Paris), Lett. 41, L-223 (1980) Ch.Hamelin, J.Crancon, J.Blachot, G.Lhospice, J.P.Bocquet, A.Moussa Determination Experimentale du Rapport Isomerique du 136I dans la Fission Thermique et par Neutrons de 3 MeV de 235U NUCLEAR REACTIONS, Fission 235U(n, F), E=thermal, 3 MeV; measured Eγ, Iγ; 136I deduced isomer yields, average angular momenta.
1980SC05 Phys.Lett. 90B, 57 (1980) A.Schroder, H.Ohm, W.Rudolph, K.Summerer, K.-L.Kratz, K.D.Wunsch, G.Jung, J.Crancon, C.Ristori Spectroscopy of Beta-Delayed Neutrons in Coincidence with Gamma-Rays Depopulating Excited States in 93Sr RADIOACTIVITY 94Rb; measured β-delayed nγ(t). 94Sr deduced resonance in β-strength function. 93Sr levels deduced p-wave n-branching. Optical model analysis.
doi: 10.1016/0370-2693(80)90050-7
1979KR10 Phys.Lett. 86B, 21 (1979) K.-L.Kratz, H.Ohm, K.Summerer, M.Zendel, G.Jung, K.D.Wunsch, C.Ristori, J.Crancon, S.G.Prussin Systematic Trends in the Beta Minus Strength Functions of Neutron-Rich Rubidium Isotopes RADIOACTIVITY 89,91,93,95,97Rb; analyzed data on β-decay properties, γ, neutron spectroscopy; deduced resonances in β-strength function.
doi: 10.1016/0370-2693(79)90611-7
1979RI09 Z.Phys. A290, 311 (1979) C.Ristori, J.Crancon, K.D.Wunsch, G.Jung, R.Decker, K.-L.Kratz Half-Lives and Delayed Neutron Emission Probabilities of Short-Lived Rb and Cs Precursors RADIOACTIVITY 94,95,96,97,98Rb, 143,144,145,146,147Cs [from on-line separator]; measured T1/2, delayed-neutron emission probabilities.
doi: 10.1007/BF01408548
1978CR03 Z.Phys. A287, 45 (1978) J.Crancon, C.Ristori, H.Ohm, W.Rudolph, K.-L.Kratz, M.Asghar Half-Lives and P(n) Values of Delayed-Neutron Precursors in the Mass Chains 85-87, 92, 135, 136 and 145 RADIOACTIVITY 85,86,87As, 92Br, 135,136Sb, 136Te, 145Cs; measured T1/2, neutron emission probability. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset23352. 1977BR11 Nucl.Phys. A282, 109 (1977) R.Brissot, J.Crancon, C.Ristori, J.P.Bocquet, A.Moussa Distributions Isotopiques des Gaz Rares et de Leurs Precurseurs dans la Fission Thermique de 239,241Pu: Etude de l'Effet 'Pair-Impair' NUCLEAR REACTIONS 239,241Pu(n, F), E=th; measured rare gas fission yields, mass, charge distributions, deduced odd-even effect. On-line isotopic separation of products.
doi: 10.1016/0375-9474(77)90174-9
1977FE03 J.Phys.(Paris) 38, 273 (1977) C.A.Feu Alvim, J.P.Bocquet, R.Brissot, J.Crancon, A.Moussa Mesure, par Une Method d'Emanation, des Rendements des Gaz Rares dans la Fission de 238U et 232Th par Neutrons de 14 MeV NUCLEAR REACTIONS 238U, 232Th(n, F), E=14 MeV; measured Kr, Xe yields, σ(A, Z). Data from this article have been entered in the EXFOR database. For more information, access X4 dataset21567. 1976BR25 J.Phys.(Paris), Lett. 37, L-241 (1976) R.Brissot, J.Crancon, C.Ristori, A.Moussa Distributions Isotopiques des Gaz Rares dans la Fission par Neutrons Thermiques de 239Pu et 241Pu. Evaluation de l'Effet de Parite en Protons NUCLEAR REACTIONS 239,241Pu(n, F), E=th; measured Kr, Xe yields.
doi: 10.1051/jphyslet:019760037010024100
1976KR18 Phys.Lett. 65B, 231 (1976) K.-L.Kratz, W.Rudolph, H.Ohm, H.Franz, G.Herrmann, C.Ristori, J.Crancon, M.Asghar, G.I.Crawford, F.M.Nuh, S.G.Prussin Decay of Individual Levels in Delayed Neutron Emitters to Excited States in the Final Nuclei RADIOACTIVITY 85As, 135Sb, 94Rb; measured β-delayed neutrons, γ spectra. 135Te levels deduced delayed neutron branching. 134Te deduced levels.
doi: 10.1016/0370-2693(76)90170-2
1976RI06 Z.Phys. A277, 71 (1976) C.Ristori, M.Asghar, J.Crancon, J.P.Gautheron Nuclear Charge Distributions from 4π-β Measurements on Mass Separated Fragments from 235U(n(th), f) NUCLEAR REACTIONS 235U(n, F), E=th; measured β-activity of A=91, 93, 94, 95, 137, 139; deduced nuclear charge distributions, σ(Z).
doi: 10.1007/BF01547504
1976RI12 Z.Phys. A 277, 71 (1976) C.Ristori, M.Asghar, J.Crancon, J.P.Gautheron Nuclear Charge Distributions From 4π-β Measurements On Mass Separated Fragments From 235U (nth, f) NUCLEAR REACTIONS 235U(n, f), E=0.0253 eV; measured products, 139Cs, 139Xe, 137Xe, 139I, 137Te, 137I, 95Y, 95Sr, 94Sr, 93Sr, 95Rb, 94Rb, 93Rb, 91Rb, 94Kr, 93Kr, 91Kr, 91Br; deduced yields. Data were imported from EXFOR entry 21556.
doi: 10.1007/BF01547504
1975AS03 J.Inorg.Nucl.Chem. 37, 1563 (1975) M.Asghar, J.Crancon, J.P.Gautheron, C.Ristori Delayed Neutron Emission Probabilities of 92,93Kr, 92,93Rb, 141,142Xe and 141,142Cs Precursors RADIOACTIVITY 92,93Kr, 92,93Rb, 141,142Xe, 141,142Cs; measured delayed neutrons, β-activity; deduced probability of neutron emission.
doi: 10.1016/0022-1902(75)80277-6
1975AS04 Nucl.Phys. A247, 359 (1975) M.Asghar, J.P.Gautheron, G.Bailleul, J.P.Bocquet, J.Greif, H.Schrader, G.Siegert, C.Ristori, J.Crancon, G.I.Crawford The p(n) Values of the 235U(n(th), f) Produced Precursors in the Mass Chains 90, 91, 93-95, 99, 134 and 137-139 RADIOACTIVITY 90,91Br, 91Se, 93,94Kr, 93,94,95Rb, 99Y, 99Sr, 134Sn, 137,138Te, 137,138,139I [from 235U(n, F), E=thermal]; measured delayed neutrons, β-activity, T1/2; deduced delayed neutron probability.
doi: 10.1016/0375-9474(75)90642-9
1975AS05 J.Inorg.Nucl.Chem. 37, 2229 (1975) M.Asghar, J.Crancon, J.P.Gautheron, C.Ristori Delayed Neutron Emission Probabilities of 92,93Kr, 92,93Rb, 141,142Xe and 141,142Cs Precursors RADIOACTIVITY 92,93Kr, 92,93Rb, 141,142Xe, 141,142Cs; measured delayed neutron emission probabilities.
doi: 10.1016/0022-1902(75)80715-9
1975BR27 Nucl.Phys. A255, 461 (1975) R.Brissot, J.Crancon, C.Ristori, J.P.Bocquet, A.Moussa Distributions Isotopiques des Gaz Rares dans la Fission par Neutrons Thermiques de 235U et 233U NUCLEAR REACTIONS 233U, 235U(n, F), E=thermal; measured independent, cumulative yields of rare gas isotopes; deduced deviations from ucd, widths of gaussian distributions, elemental yields of Br, Kr, Xe. On-line isotopic separation of the products.
doi: 10.1016/0375-9474(75)90693-4
1975MO06 J.Phys.(Paris) 36, 1 (1975) E.Monnand, R.Brissot, J.Crancon, C.Ristori, F.Schussler, A.Moussa Niveaux de 137Cs Alimentes dans la Desintegration de 137Xe RADIOACTIVITY 137Xe; measured Eγ, Iγ, γγ-coin, Iβ; deduced β-branching, log ft. 137Cs deduced levels, γ-branching, T1/2 limit. 138Cs deduced transitions.
doi: 10.1051/jphys:019750036010100
1974CR06 J.Phys.(London) A7, L141 (1974) G.I.Crawford, S.J.Hall, J.D.Kellie, M.Asghar, G.Bailleul, J.P.Bocquet, C.Chauvin, J.P.Gautheron, H.Schrader, G.Siegert, J.Crancon, C.Ristori Population of Excited States in Delayed Neutron Emission RADIOACTIVITY 85As, 90Br, 95Rb; measured nγ-coin. 94Sr, 89Kr deduced levels.
doi: 10.1088/0305-4470/7/12/001
1974SC39 Radiochim.Acta 21, 8 (1974) F.Schussler, P.Cavallini, L.C.Carraz, R.Brissot, J.Crancon, E.Monnand, C.Ristori, A.Moussa Desintegration de 93Sr (T1/2 = 7.3 min). Niveau Isomerique de 93Y (T1/2 = 1.7 sec) RADIOACTIVITY 93Sr; measured Eβ, Eγ, Iγ, γ(t), γγ-coin, βγ-coin; deduced Q, ICC, log ft. 93Y deduced levels, J, π, T1/2.
1973SC18 Nucl.Phys. A209, 589 (1973) F.Schussler, R.Brissot, J.Crancon, E.Monnand, C.Ristori, A.Moussa Desintegration de 140Cs (T1/2 = 64 sec) RADIOACTIVITY 140Cs [from 235U(nth, F)]; measured Eβ, Iβ, Eγ, Iγ, βγ-, γγ-coin, γγ- angular correlations, Q; deduced log ft; 140Ba deduced levels, J, π.
doi: 10.1016/0375-9474(73)90848-8
1972BO25 Nucl.Phys. A189, 556 (1972) J.P.Bocquet, R.Brissot, J.Crancon, A.Moussa On-Line Measurements of Rare-Gas Fission Yields in 14 MeV Neutron Fission NUCLEAR REACTIONS, Fission 233U, 235U, 238U, 232Th(n, F), En=14 MeV; measured independent, cumulative yields of rare-gas isotopes; deduced deviations from UCD, widths of Gaussian distributions. On-line isotopic separation of the products.
doi: 10.1016/0375-9474(72)90314-4
1972MO33 Nucl.Phys. A195, 192 (1972) E.Monnand, R.Brissot, L.C.Carraz, J.Crancon, C.Ristori, F.Schussler, A.Moussa Desintegration de 138Xe RADIOACTIVITY 138Xe[from 235U(n, F)]; measured Eβ, Iβ, I(ce), Eγ, Iγ, βγ-, γγ-coin, T1/2; deduced ICC, log ft, Qβ. 138Cs deduced levels, J, π.
doi: 10.1016/0375-9474(72)90730-0
1969BO02 Nucl.Phys. A125, 613 (1969) J.P.Bocquet, R.Brissot, J.Crancon, J.A.Pinston, F.Schussler, A.Moussa Desintegration du 87Kr RADIOACTIVITY 87Kr [from 235U(n, F)]; measured Eβ, Iβ, Eγ, Iγ, βγ-, γγ-coin. 87Rb deduced levels. Mass separated sources.
doi: 10.1016/0375-9474(69)90751-9
1969FO01 Nucl.Phys. A123, 513 (1969) C.Foin, J.Oms, J.Blachot, J.Crancon Etude de la Desintegration 95Zr → 95Nb RADIOACTIVITY 95Zr [from 235U fission]; measured Eγ, Iγ; 95Nb measured T1/2, Eγ, ICC; deduced log ft. 95Nb deduced levels, J, π. Ge(Li) detector.
doi: 10.1016/0375-9474(69)91000-8
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