NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = A.J.Deruytter Found 47 matches. 1992SC15 Nucl.Phys. A545, 623 (1992) P.Schillebeeckx, C.Wagemans, A.J.Deruytter, R.Barthelemy Comparative Study of the Fragments' Mass and Energy Chatacteristics in the Spontaneous Fission of 238Pu, 240Pu and 242Pu and in the Thermal-Neutron-Induced Fission of 239Pu NUCLEAR REACTIONS 239Pu(n, F), E=thermal; measured complementary fission fragment kinetic energies; deduced energy, mass distributions, mass-energy correlations. Fission mode analysis. RADIOACTIVITY 238,240,242Pu(SF); measured complementary fission fragment kinetic energies; deduced energy, mass distributions, mass-energy correlations. Fission mode analysis.
doi: 10.1016/0375-9474(92)90296-V
1986WA16 Radiat.Eff. 93, 163 (1986) Sub-Thermal Fission Cross-Section Measurements NUCLEAR REACTIONS 235U(n, F), E ≤ 0.1 eV; measured fission σ(E); deduced shape influence on Westcott factor.
doi: 10.1080/00337578608207444
1982AL13 Nucl.Phys. A380, 61 (1982) E.Allaert, C.Wagemans, G.Wegener-Penning, A.J.Deruytter, R.Barthelemy Energy and Mass Distributions for 241Pu(n(th), f), 242Pu(s.f.) and 244Pu(s.f) Fragments RADIOACTIVITY, Fission 242,244Pu(SF); measured complementary fragment kinetic energies; deduced energy, mass distributions, mass-energy correlations. NUCLEAR REACTIONS, Fission 241Pu(n, F), E=thermal; measured complementary fragment kinetic energies; deduced energy, mass distributions, mass-energy correlations.
doi: 10.1016/0375-9474(82)90582-6
1981JA08 Phys.Rev. C24, 1795 (1981) E.Jacobs, A.De Clercq, H.Thierens, D.De Frenne, P.D'hondt, P.De Gelder, A.J.Deruytter Fragment Mass and Kinetic Energy Distributions for the Photofission of 235U with 12-, 15-, 20-, 30-, and 70-MeV Bremsstrahlung NUCLEAR REACTIONS, Fission 235U(γ, F), E=12, 15, 20, 30, 70 MeV bremsstrahlung; measured fragment mass, kinetic energy distributions; deduced average light, heavy fragment mass, average two-fragment total kinetic energy, standard deviations vs excitation energy. Scission point model.
doi: 10.1103/PhysRevC.24.1795
1981TH02 Phys.Rev. C23, 2104 (1981) H.Thierens, A.De Clercq, E.Jacobs, D.De Frenne, P.D'hondt, P.De Gelder, A.J.Deruytter Kinetic Energy and Fragment Mass Distributions for 240Pu(SF), 239Pu(n(thermal), f), and 240Pu(γ, f) RADIOACTIVITY, Fission 240Pu(SF); measured σ(fragment mass), average total fragment kinetic energy, (fragment)(fragment) energy correlation, total kinetic energy variance; deduced fragment shell effects. NUCLEAR REACTIONS, Fission 240Pu(γ, F), E=12, 15, 20, 30 MeV; measured σ(E), σ(fragment mass), average total fragment kinetic energy, total kinetic energy variance; 239Pu(n, F), E=thermal; measured σ(fragment mass), average total fragment kinetic energy, total kinetic energy variance.
doi: 10.1103/PhysRevC.23.2104
1980DE03 Phys.Rev. C21, 629 (1980) D.De Frenne, H.Thierens, E.Jacobs, P.De Gelder, A.De Clercq, P.D'hondt, A.J.Deruytter Charge Distribution for the Photofission of 238U with 20-MeV Bremsstrahlung NUCLEAR REACTIONS 238U(γ, F), E=20 MeV bremsstrahlung; measured Eγ, Iγ. 88Br, 90,91Kr, 93Rb, 94,95Sr, 96Nb, 100Zr, 128,131,131m,132Sn, 131,132,132m,133Sb, 131,131m,132,133,133m,135,136Te, 132,132m,133,134,136,137,138I, 135,137,139Xe, 134,136Cs deduced fractional independent, cumulative chain yields, charge distribution width.
doi: 10.1103/PhysRevC.21.629
1980DE06 Nucl.Phys. A337, 285 (1980) P.De Gelder, D.De Frenne, E.Jacobs, H.Thierens, A.De Clercq, P.D'hondt, K.Heyde, A.J.Deruytter, G.Tittel, N.Kaffrell, N.Trautmann, F.Schussler The β- Decay of 102Mo RADIOACTIVITY 102Mo [from 235U(n, F), E=th, U(γ, F)]; measured T1/2, Eγ, Iγ, γγ-coin. 102Tc deduced levels, J, π, log ft. Natural, enriched targets.
doi: 10.1016/0375-9474(80)90057-3
1980DH01 Phys.Rev. C21, 963 (1980) P.D'hondt, E.Jacobs, A.De Clercq, D.De Frenne, H.Thierens, P.De Gelder, A.J.Deruytter Emission of Long-Range Alpha Particles in the Photofission of 235U with 20-MeV Bremsstrahlung NUCLEAR REACTIONS 235U(γ, F), E=20 MeV bremsstrahlung; measured long range σ(Eα).
doi: 10.1103/PhysRevC.21.963
1980DH02 Ann.Nucl.Energy 7, 367 (1980) P.D'hondt, C.Wagemans, G.Barreau, A.J.Deruytter The 232Th(n, F) Cross Section for Thermal and 2.44 MeV Neutrons NUCLEAR REACTIONS 232Th(n, F), E=th, 2.44 MeV; measured σ.
doi: 10.1016/0306-4549(80)90022-5
1980JA01 Phys.Rev. C21, 237 (1980) E.Jacobs, H.Thierens, D.De Frenne, A.De Clercq, P.D'hondt, P.De Gelder, A.J.Deruytter Product Yields for the Photofission of 235U with 12-, 15-, 20-, 30-, and 70-MeV Bremsstrahlung NUCLEAR REACTIONS 235U(γ, F), E=12, 15, 20, 30, 70 MeV; measured Eγ; deduced mass distributions, most probable charges, average initial fragment spins. 126,128Sb, 131Sb, 131Te, 136I, 135Xe, 136Cs, 140La deduced fractional independent, cumulative yields. 126,128Sb, 131Te deduced isomeric σ ratio.
doi: 10.1103/PhysRevC.21.237
1980TH03 Nucl.Phys. A342, 229 (1980) H.Thierens, E.Jacobs, P.D'hondt, D.De Frenne, A.De Clercq, P.De Gelder, A.J.Deruytter, J.Blachot, P.Perrin The Thermal Neutron Sub-Barrier Fission of 237Np NUCLEAR REACTIONS 237Np(n, F), E=thermal; measured fission product γ-ray spectra; deduced post-neutron mass distribution, neutron emission curve.
doi: 10.1016/0375-9474(80)90251-1
1979CO16 Nucl.Instrum.Methods 166, 217 (1979) G.Coddens, C.Wagemans, A.J.Deruytter, W.Mampe Experimental and Theoretical Investigation of the Backscattering of Fission Fragments NUCLEAR REACTIONS 235U(n, F), E=thermal; measured fragment backscattering from Au, Cu, Al; deduced strong Z dependence.
doi: 10.1016/0029-554X(79)90579-2
1979JA02 Phys.Rev. C19, 422 (1979) E.Jacobs, H.Thierens, D.De Frenne, A.De Clercq, P.D'hondt, P.De Gelder, A.J.Deruytter Product Yields for the Photofission of 238U with 12-, 15-, 20-, 30-, and 70-MeV Bremsstrahlung NUCLEAR REACTIONS 238U(γ, F), E=12-70 MeV bremsstrahlung; measured fragment γ-ray spectra; deduced mass distributions, most probable charges, isomeric ratios, average initial fragment spins.
doi: 10.1103/PhysRevC.19.422
1979JA28 Phys.Rev. C20, 2249 (1979) E.Jacobs, A.De Clercq, H.Thierens, D.De Frenne, P.D'hondt, P.De Gelder, A.J.Deruytter Fragment Mass and Kinetic Energy Distributions for the Photofission of 238U with 12-, 15-, 20-, 30-, and 70 MeV Bremsstrahlung NUCLEAR REACTIONS 238U(γ, F), E=12, 15, 20, 30, 70 MeV bremsstrahlung; measured fragment energies; deduced dependence of mass distribution on total fragment kinetic energy, compound nucleus energy.
doi: 10.1103/PhysRevC.20.2249
1978DE19 Phys.Rev. C18, 486 (1978) D.De Frenne, H.Thierens, E.Jacobs, P.De Gelder, P.D'hondt, A.De Clercq, K.Heyde, A.J.Deruytter β- Decay of 102gTc RADIOACTIVITY 102Tc; measured Eγ, Iγ; deduced log ft. 102Ru deduced levels, J, π.
doi: 10.1103/PhysRevC.18.486
1978DH01 Nucl.Phys. A303, 275 (1978) P.D'Hondt, A.De Clercq, A.J.Deruytter, C.Wagemans, M.Asghar, A.Emsallem Study of α-Particles Produced in Thermal Neutron Induced Reactions on 235U NUCLEAR REACTIONS 235U(n, F), 235U(n, α), E=thermal; measured fission α-distribution, σ(n, α).
doi: 10.1016/0375-9474(78)90358-5
1978WA15 Ann.Nucl.Energy 5, 267 (1978) C.Wagemans, M.Asghar, F.Caitucoli, P.Perrin, P.D'Hondt, A.J.Deruytter Measurement of the Thermal Neutron-Induced Fission Cross-Section of 231Pa NUCLEAR REACTIONS 231Pa(n, F), E=thermal; measured σ.
doi: 10.1016/0306-4549(78)90079-8
1977DE10 Phys.Rev. C15, 1440 (1977) D.De Frenne, H.Thierens, E.Jacobs, P.D'hondt, A.De Clercq, K.Heyde, A.J.Deruytter Excited States in 118Sn Populated by the β- Decay of 118In-g and 118Sb RADIOACTIVITY 118In; measured Eγ, Iγ; deduced log ft. 118Sn deduced levels, J, π. NUCLEAR REACTIONS 238U(γ, F), E=25, 50 MeV bremsstrahlung; measured yields for A=111-113, 115, 117, 123, 125.
doi: 10.1103/PhysRevC.15.1440
1977WA09 Nucl.Phys. A285, 32 (1977) C.Wagemans, M.Asghar, P.D'Hondt, A.J.Deruytter, A.Emsallem Study of Some Characteristics of the Thermal-Neutron-Induced Sub-Barrier Fission of 231Pa, 232Th and 237Np NUCLEAR REACTIONS 231Pa, 232Th, 237Np(n, F), E=th; measured σ, average kinetic energy, long range alphas/binary fission.
doi: 10.1016/0375-9474(77)90144-0
1976AS02 Nucl.Phys. A259, 429 (1976) M.Asghar, A.Emsallem, R.Chery, C.Wagemans, P.D'Hondt, A.J.Deruytter The 238U(n, α)235Th Reaction with Thermal Neutrons NUCLEAR REACTIONS 238U(n, α), E=thermal; measured σ(Eα); deduced Q. 235Th deduced mass, Qβ.
doi: 10.1016/0375-9474(76)90078-6
1976DE10 Phys.Rev. C13, 1536 (1976) A.De Clercq, E.Jacobs, D.De Frenne, H.Thierens, P.D'hondt, A.J.Deruytter Fragment Mass and Kinetic Energy Distribution for the Photofission of 235U and 238U with 25-MeV End-Point Bremsstrahlung NUCLEAR REACTIONS 235,238U(γ, F), E ≤ 25 MeV; measured fragment energy correlation; deduced fragment mass, energy yield.
doi: 10.1103/PhysRevC.13.1536
1976JA15 Phys.Rev. C14, 1874 (1976) E.Jacobs, H.Thierens, A.De Clercq, D.De Frenne, P.D'hondt, A.J.Deruytter Neutron Emission in the Photofission of 235U and 238U with 25-MeV Bremsstrahlung NUCLEAR REACTIONS 235,238U(γ, F), E(max)=25 MeV; calculated neutron emission curve from experimental provisional, post-neutron mass distributions.
doi: 10.1103/PhysRevC.14.1874
1976TH07 Nucl.Instrum.Methods 134, 299 (1976) H.Thierens, D.de Frenne, E.Jacobs, A.de Clercq, P.D'Hondt, A.J.Deruytter Study of the Catcherfoil Technique with the Aid of 252cfs.f. And 235U(n(th), f) RADIOACTIVITY, Fission 252Cf(SF); measured mass yield. Catcherfoil technique. NUCLEAR REACTIONS 235U(n, F), E=th; measured mass yield. Catcherfoil technique.
doi: 10.1016/0029-554X(76)90285-8
1976TH13 Phys.Rev. C14, 1058 (1976) H.Thierens, D.De Frenne, E.Jacobs, A.De Clercq, P.D'hondt, A.J.Deruytter Product Yields for the Photofission of 235U and 238U with 25-MeV Bremsstrahlung NUCLEAR REACTIONS 235,238U(γ, F), E(max)=25 MeV; measured fragment γ-spectra; deduced mass distributions, isomeric ratios, most probable charges.
doi: 10.1103/PhysRevC.14.1058
1976WA04 Nucl.Phys. A259, 423 (1976) C.Wagemans, P.D'Hondt, A.J.Deruytter, A.Emsallem, M.Asghar The Thermal Neutron Induced Fission Cross Section of 232Th NUCLEAR REACTIONS 232Th(n, F), E=thermal; measured, calculated σ(n, F).
doi: 10.1016/0375-9474(76)90077-4
1976WA05 Nucl.Sci.Eng. 60, 44 (1976) Measurement and Normalization of the Relative Plutonium-241 Fission Cross Section in the Thermal and Low-Resonance Energy Region NUCLEAR REACTIONS 241Pu(n, F), E=0.1-50 eV; measured σ(E).
doi: 10.13182/NSE76-A26856
1976WA17 Ann.Nucl.Energy 3, 437 (1976) The Neutron Induced Fission Cross Section of 235U in the Energy Region From 0.008 eV to 30 keV NUCLEAR REACTIONS 235U(n, F), E=0.008 eV-30 keV; measured σ(E).
doi: 10.1016/0306-4549(76)90028-1
1975WA13 Ann.Nucl.Energy 2, 25 (1975) The Wescott g(f)-Factor for 239Pu and its Temperature Dependence NUCLEAR REACTIONS 239Pu(n, F), E=0.008-10 eV; measured σ; deduced Westcott factor.
doi: 10.1016/0306-4549(75)90067-5
1975WA27 Ann.Nucl.Energy 2, 541 (1975) The Westcott g-Factor as a Function of the Temperature for 241Pu NUCLEAR STRUCTURE 241Pu; calculated Westcott g-factor.
doi: 10.1016/0306-4549(75)90052-3
1975WA32 Z.Phys. A275, 149 (1975) The Emission of Long-Range α-Particles in the Thermal Neutron Induced Fission of 233U, 235U, and 239Pu NUCLEAR REACTIONS 233,235U, 239Pu(n, F), E=thermal; measured long range α yields relative to binary fission.
doi: 10.1007/BF01409590
1975WA38 Z.Phys. A 275, 149 (1975) The emission of long range α-particles in the thermal neutron induced fission of 233U, 235U, and 239Pu NUCLEAR REACTIONS 233U(n, f), 235U(n, α), 235U(n, f), 239Pu(n, α), 239Pu(n, f), E=0.0253 eV; measured products, 2-HE-4, 232Th, 236U; deduced yields, σ, σ(E). Data were imported from EXFOR entry 21529.
doi: 10.1007/BF01409590
1974DE19 Phys.Rev. C10, 383 (1974) A.J.Deruytter, G.Wegener-Penning Redetermination of the Half-Life of 235U for α Emission RADIOACTIVITY 235U; measured Eα, Iα; deduced α-branching, T1/2.
doi: 10.1103/PhysRevC.10.383
1974DE43 Ann.Nucl.Sci.Eng. 1, 311 (1974) The Accurate Fission Cross-Section of 239Pu from 0.005 eV to 0.1 eV and its Reference Value at 2200 m/s NUCLEAR REACTIONS 239Pu(n, F), 10B(n, α), E=0.005-0.1 eV; measured σ(E, E(fragment mass)), σ(E, Eα).
doi: 10.1016/0302-2927(74)90011-7
1974DE44 Nucl.Sci.Eng. 54, 423 (1974) Measurement and Normalization of the Relative Uranium-233 Fission Cross Section in the Low Resonance Region NUCLEAR REACTIONS 233U(n, F), E=0.008-50 eV; measured fission σ, calculated fission, resonance integrals.
doi: 10.13182/NSE74-A23436
1974WA20 Nucl.Phys. A234, 285 (1974) Ratio of the Ternary-to-Binary Fission Cross Sections Induced by Thermal and Resonance Neutrons in 241Pu NUCLEAR REACTIONS 241Pu(n, F), E=0.01-50ev; measured ternary, binary fission; deduced J-dependence of T/B ratio. 242Pu deduced resonances, J.
doi: 10.1016/0375-9474(74)90563-6
1973DE48 J.Nucl.Energy 27, 645 (1973) A.J.Deruytter, J.Spaepen, P.Pelfer The Accurate Fission Cross-Section of 235U from 0.002 to 0.15 eV and its Reference Value at 2200m/s NUCLEAR REACTIONS 10B(n, α), 235U(n, F), E=0.002-0.15 eV; measured σ(E).
doi: 10.1016/0022-3107(73)90024-5
1973WA27 Nucl.Phys. A212, 556 (1973) Ratio of the Ternary to Binary Fission Induced by Thermal and Resonance Neutrons in 239Pu NUCLEAR REACTIONS, Fission 239Pu(n, F), E=0.02-50 eV, measured ternary, binary fission; deduced J-dependence of ternary/binary ratio. 240Pu deduced resonances, J.
doi: 10.1016/0375-9474(73)90823-3
1972DE51 J.Nucl.Energy 26, 293 (1972) Measurement and Normalization of the Relative 239Pu Fission Cross-Section in the Low Resonance Region NUCLEAR REACTIONS 239Pu(n, F), E < 30 eV; measured reaction products; deduced σ(E), fission resonance integrals. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset20132. 1972WA26 Nucl.Phys. A194, 657 (1972) Ratio of the Ternary to Binary Fission Cross Sections Induced by Resonance Neutrons in 235U NUCLEAR REACTIONS, Fission 235U(n, F), En=5-40 eV; measured lra fission(t), normal binary fission(b); deduced correlation of t/b with J.
doi: 10.1016/0375-9474(72)91011-1
1971DE61 J.Nucl.Energy 25, 263 (1971) Measurement and Normalization of the Relative 235U Fission Cross-Section in the Low Resonance Region NUCLEAR REACTIONS 235U(n, F), E < =th; measured σ(E) in low resonance region.
doi: 10.1016/0022-3107(71)90001-3
1967DE15 J.Nucl.Energy 21, 833 (1967) Precise Determination of the Branching Ratio and Q-Value of the 10B(n, α)7Li Reaction and of the Q-Value of the 6Li(n, α)3H Reaction NUCLEAR STRUCTURE 6Li, 7Li, 10B; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0022-3107(67)90094-9
1966PO07 Nucl.Phys. 82, 331(1966) F.Poortmans, H.Ceulemans, A.J.Deruytter, M.N.De Mevergnies The 149Sm(n, α)146Nd Reaction with Low Energy Neutrons NUCLEAR REACTIONS 149Sm(n, α), E = 0.004 eV-0.1 eV; measured σ(E, Eα). 150Sm deduced resonance parameters, J. Enriched target.
doi: 10.1016/0029-5582(66)90007-1
1965DE06 Nucl.Sci.Eng. 21, 325 (1965) A.J.Deruytter, I.G.Schroder, J.A.Moore Measurement of the Half-Life of U235 for Alpha Emission NUCLEAR STRUCTURE 235U; measured not abstracted; deduced nuclear properties.
doi: 10.13182/NSE65-A20036
1965SC27 Phys.Rev. 137, B519 (1965) I.G.Schroder, A.J.Deruytter, J.A.Moore Relative Probability of Ternary Fission with Emission of Long-Range Alpha Particles in the Thermal-Neutron Fission of U235 NUCLEAR REACTIONS 233U(n, F), E thermal; measured reaction products; deduced the ratio of binary to ternary fission.
doi: 10.1103/physrev.137.b519
1963DE34 J.Phys. 24, 939 (1963) A.J.Deruytter, I.G.Schroder, J.A.Moore Une Mesure Precise de la Demie-Vie de 235U pour l'Emission α NUCLEAR STRUCTURE 235U; measured not abstracted; deduced nuclear properties.
doi: 10.1051/jphys:019630024011093900
1963PR11 J.Nucl.Energy:Pt.A 17, 83 (1963) A Precise Determination of the Thermal Neutron Absorption Cross Sectionof B10 and Natural Boron by Time of Flight NUCLEAR STRUCTURE B, 10B; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0368-3230(63)90027-2
1962DE15 Cu(Pnpl) - 219, p.11 (1962) A.J.Deruytter, J.A.Moore, I.G.Schroder Measurement of the Half-Life of U235 NUCLEAR STRUCTURE 235U; measured not abstracted; deduced nuclear properties.
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