NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = C.Wagemans Found 88 matches. 2017AN16 Phys.Rev. C 96, 054327 (2017) B.Andel, A.N.Andreyev, S.Antalic, A.Barzakh, N.Bree, T.E.Cocolios, V.F.Comas, J.Diriken, J.Elseviers, D.V.Fedorov, V.N.Fedosseev, S.Franchoo, L.Ghys, J.A.Heredia, M.Huyse, O.Ivanov, U.Koster, V.Liberati, B.A.Marsh, K.Nishio, R.D.Page, N.Patronis, M.D.Seliverstov, I.Tsekhanovich, P.Van den Bergh, J.Van De Walle, P.Van Duppen, M.Venhart, S.Vermote, M.Veselsky, C.Wagemans Detailed α-decay study of 180Tl RADIOACTIVITY 180Tl(α)[from U(p, X), E=1.4 GeV using Resonance Ionization Laser Ion Source (RILIS) and HRS separator at ISOLDE-CERN facility]; measured Eα, Iα, Eγ, Iγ, E(x ray), I(x ray), αγ- and αγγ-coin. 176Au; deduced levels, α-decay branching ratios, reduced α-widths, total and K-conversion coefficients, multipolarities, configurations, population of only the low-spin activity in 176Au from 180Tl α decay. Comparison with previous experimental data. Systematics of α-reduced widths in α-decays of 178,180,182,184Tl. 180Hg(α)[from 180Tl ϵ decay]; 176Au(α)[from 180Tl α decay]; 176Pt(α)[from 180Hg α decay]; measured Eα, Eγ, αγ-coin. 172Ir; deduced level, low-spin activity in 172Ir populated by 176Au α decay.
doi: 10.1103/PhysRevC.96.054327
2013EL08 Phys.Rev. C 88, 044321 (2013); Erratum Phys.Rev. C 102, 019908 (2020) J.Elseviers, A.N.Andreyev, M.Huyse, P.Van Duppen, S.Antalic, A.Barzakh, N.Bree, T.E.Cocolios, V.F.Comas, J.Diriken, D.Fedorov, V.N.Fedosseev, S.Franchoo, L.Ghys, J.A.Heredia, O.Ivanov, U.Koster, B.A.Marsh, K.Nishio, R.D.Page, N.Patronis, M.D.Seliverstov, I.Tsekhanovich, P.Van den Bergh, J.Van De Walle, M.Venhart, S.Vermote, M.Veselsky, C.Wagemans β-delayed fission of 180Tl RADIOACTIVITY 180Tl(EC), (β+), (SF)[from U(p, X), E=1.4 GeV]; measured Eα, Eβ, Eγ, fission fragment spectra, (fission fragment)(fission fragment)-coin, (fission fragment)γ-coin, mass and energy distribution of fission fragments, total kinetic energy of fission events, β-delayed fission probability, fission yield, half-life of 180Tl using RILIS source and HRS separator at ISOLDE-CERN facility. 180Hg; deduced asymmetric fission of excited states populated in decay of 180Tl. Viola systematics of total kinetic energies vs fissility parameter for 180Hg and heavier actinides.
doi: 10.1103/PhysRevC.88.044321
2012PO08 Nucl.Sci.Eng. 171, 204 (2012) L.Popescu, J.Heyse, J.Wagemans, C.Wagemans Cross-Section Measurement of Thermal Neutron-Induced Fission on 243Cm NUCLEAR REACTIONS 243Cm(n, F), E thermal; measured reaction products, Eα, Iα; deduced σ, Westcott g-factors. Comparison with available data.
doi: 10.13182/NSE11-65
2012VE01 Phys.Rev. C 85, 015803 (2012) S.Vermote, C.Wagemans, L.De Smet, C.Lampoudis, J.Van Gils Experimental determination of the 41Ca(n, α)38Ar reaction cross section up to 80 keV, and calculation of the Maxwellian averaged cross section at stellar temperatures NUCLEAR REACTIONS 41Ca(n, α), E<80 keV; measured E(α), I(α), σ. deduced resonances, J, π, widths, resonance strengths, Γn/Γp ratios, Maxwellian averaged cross section.
doi: 10.1103/PhysRevC.85.015803
2011EL07 Phys.Rev. C 84, 034307 (2011) J.Elseviers, A.N.Andreyev, S.Antalic, A.Barzakh, N.Bree, T.E.Cocolios, V.F.Comas, J.Diriken, D.Fedorov, V.N.Fedosseyev, S.Franchoo, J.A.Heredia, M.Huyse, O.Ivanov, U.Koster, B.A.Marsh, R.D.Page, N.Patronis, M.Seliverstov, I.Tsekhanovich, P.Van den Bergh, J.Van De Walle, P.Van Duppen, M.Venhart, S.Vermote, M.Veselsky, C.Wagemans Shape coexistence in 180Hg studied through the β decay of 180Tl RADIOACTIVITY 180Tl(β+), (EC)[from U(p, X), E=1.4 GeV; measured electron-, positron-, α-, and fission-fragment spectra, Eγ, Iγ, γγ-, γ(ce)-coin, half-life at CERN-ISOLDE facility, resonant laser-ionization technique for source extraction. 180Tl; measured half-life of g.s.; deduced branching ratios, J, π of g.s. 180Hg; deduced levels, J, π, E0 transitions, multipolarity. Comparison with level schemes of 182,184,196Hg. Systematics of level energies of even A=174-206 Hg nuclei up to 12+.
doi: 10.1103/PhysRevC.84.034307
2011SE14 J.Korean Phys.Soc. 59, 1896s (2011) O.Serot, C.Wagemans, S.Vermote, J.Van Gils Measurement of the Neutron Induced Fission of 245Cm in the Resolved Resonance Region and Its Resonance Analysis NUCLEAR REACTIONS 245Cm(n, F), E=0.5-1000 eV; measured fission fragments; deduced fission σ, resonance integral; calculated σ using CONRAD code; deduced resonance parameters. Compared with other data, JEFF-3.1.1. Preliminary.
doi: 10.3938/jkps.59.1896
2010AN13 Phys.Rev.Lett. 105, 252502 (2010) A.N.Andreyev, J.Elseviers, M.Huyse, P.Van Duppen, S.Antalic, A.Barzakh, N.Bree, T.E.Cocolios, V.F.Comas, J.Diriken, D.Fedorov, V.Fedosseev, S.Franchoo, J.A.Heredia, O.Ivanov, U.Koster, B.A.Marsh, P.Van den Bergh, J.Van De Walle, K.Nishio, R.D.Page, N.Patronis, M.Seliverstov, I.Tsekhanovich, M.Venhart, S.Vermote, M.Veselsky, C.Wagemans, T.Ichikawa, A.Iwamoto, P.Moller, A.J.Sierk New Type of Asymmetric Fission in Proton-Rich Nuclei RADIOACTIVITY 180Tl(α), (β+), (EC) [from U(p, X), E=1.4 GeV]; measured fission fragments, Eα, Iα, X-rays. 180Hg; deduced asymetric fission fragment distribution, branching ratio for β-delayed fission.
doi: 10.1103/PhysRevLett.105.252502
2010VE03 Nucl.Phys. A837, 176 (2010) S.Vermote, C.Wagemans, O.Serot, J.Heyse, J.Van Gils, T.Soldner, P.Geltenbort, I.Al Mahamid, G.Tian, L.Rao Ternary particle emission in spontaneous fission of 250Cf and 252Cf and in neutron induced fission of 249Cf and 251Cf NUCLEAR REACTIONS 249,251Cf(n, F), E=5.4 meV; measured ternary α, triton and 6He emission probabilities, fission spectra, α-spectra, triton-spectra and 6He-spectra using energy loss telescope detectors. Comparison with other data and systematics. RADIOACTIVITY 250,252Cf(SF); measured ternary α, triton and 6He emission probabilities, fission spectra, α-spectra, triton-spectra and 6He-spectra using energy loss telescope detectors. Comparison with other data and systematics.
doi: 10.1016/j.nuclphysa.2010.03.001
2008VE05 Nucl.Phys. A806, 1 (2008) S.Vermote, C.Wagemans, O.Serot, J.Heyse, J.Van Gils, T.Soldner, P.Geltenbort Ternary α and triton emission in the spontaneous fission of 244Cm, 246Cm and 248Cm and in the neutron induced fission of 243Cm, 245Cm and 247Cm NUCLEAR REACTIONS 243,245,247Cm(n, F), E=5.4 meV; measured ternary fission α and triton emission probabilities and energy distributions. RADIOACTIVITY 244,246,248Cm(SF); measured ternary fission α and triton emission probabilities and energy distributions.
doi: 10.1016/j.nuclphysa.2008.03.006
2008WA14 Nucl.Sci.Eng. 160, 200 (2008) C.Wagemans, L.De Smet, S.Vermote, J.Heyse, J.Van Gils, O.Serot Measurement of the 236U(n, f) Cross Section in the Neutron Energy Range from 0.5 eV up to 25 keV NUCLEAR REACTIONS 236U(n, f), E=0.0005-25.0 keV; measured fission fragment spectra, cross sections.
doi: 10.13182/NSE160-200
2007DE15 Phys.Rev. C 75, 034617 (2007) L.De Smet, C.Wagemans, G.Goeminne, J.Heyse, J.Van Gils Experimental determination of the 36Cl(n, p)36S and 36Cl(n, α)33P reaction cross sections and the consequences on the origin of 36S NUCLEAR REACTIONS 36Cl(n, p), (n, α), E=0.5-250 keV; measured σ; deduced resonance parameters, Maxwellian-averaged cross section. Astrophysical implications discussed.
doi: 10.1103/PhysRevC.75.034617
2007DE55 Phys.Rev. C 76, 045804 (2007) L.De Smet, C.Wagemans, J.Wagemans, J.Heyse, J.Van Gils Experimental determination of the 26Al(n, α)23Na reaction cross section and calculation of the Maxwellian averaged cross section at stellar temperatures NUCLEAR REACTIONS 26Al(n, α), E<100 keV; measured cross-sections. 27Al deduced resonance energies, widths, areas and spins.26Al deduced galactic abundance.
doi: 10.1103/PhysRevC.76.045804
2007HE09 Nucl.Sci.Eng. 156, 211 (2007) J.Heyse, C.Wagemans, L.De Smet, O.Serot, J.Wagemans, J.Van Gils High Resolution Measurement of the 234U(n, f) Cross Section in the Neutron Energy Range from 0.5 eV to 100 keV NUCLEAR REACTIONS 234U(n, F), E=0.5 eV to 100 keV; measured fission cross sections; deduced resonance integral. Special attention to the resonance at 5.16 eV.
doi: 10.13182/NSE07-A2697
2006HU15 Phys.Rev. C 74, 054311 (2006) M.Hult, J.Gasparro, G.Marissens, P.Lindahl, U.Watjen, P.N.Johnston, C.Wagemans, M.Kohler Underground search for the decay of 180Tam RADIOACTIVITY 180mTa(β-), (EC); measured lower limits for T1/2, log ft.
doi: 10.1103/PhysRevC.74.054311
2005DE42 Nucl.Phys. A758, 80c (2005) L.De Smet, C.Wagemans, G.Goeminne, J.Wagemans, J.Heyse, J.Van Gils Investigation of the (n, p) and (n, α) reactions on 26Al and 36Cl and their astrophysical relevance NUCLEAR REACTIONS 26Al(n, α), (n, p), E < 140 keV; measured σ; deduced resonance features. 36Cl(n, p), 26Al(n, α), E=stellar; analyzed astrophysical reaction rates.
doi: 10.1016/j.nuclphysa.2005.05.020
2004WA27 Nucl.Phys. A742, 291 (2004) C.Wagemans, J.Heyse, P.Janssens, O.Serot, P.Geltenbort Energy distribution of the ternary alpha's emitted in 235U(nth, f) and 252Cf(SF) NUCLEAR REACTIONS 235U(n, F), E=thermal; measured α spectra; deduced ternary fission yields. RADIOACTIVITY 252Cf(SF); measured α spectra; deduced ternary fission yields.
doi: 10.1016/j.nuclphysa.2004.06.029
2003WA23 Nucl.Phys. A719, 127c (2003) C.Wagemans, G.Goeminne, L.De Smet, J.Wagemans High resolution measurement of the 36Cl(n, p)36S and 36Cl(n, α)33P reactions NUCLEAR REACTIONS 36Cl(n, p), (n, α), E=0.1-350 keV; measured σ; deduced resonance energies.
doi: 10.1016/S0375-9474(03)00981-3
2002GO28 Nucl.Instrum.Methods Phys.Res. A489, 577 (2002) G.Goeminne, C.Wagemans, J.Wagemans, U.Koster, P.Geltenbort, B.Denecke, L.Johansson, S.Pomme Preparation and Characterisation of an 39Ar Sample and Study of the 39Ar(nth, α)36S Reaction NUCLEAR REACTIONS 39Ar(n, α), E=thermal; measured σ upper limit. Target nuclei produced via proton spallation of titanium. RADIOACTIVITY 39Ar(β-) [from Ti(p, X)]; measured Eβ.
doi: 10.1016/S0168-9002(02)00803-3
2002WA05 Phys.Rev. C65, 034614 (2002) J.Wagemans, C.Wagemans, G.Goeminne, O.Serot, M.Loiselet, M.Gaelens The 17O(n, α)14C Reaction from Subthermal up to Approximately 350 keV Neutron Energy NUCLEAR REACTIONS 17O(n, α), E < 350 keV; measured σ; deduced resonance features, astrophysical reaction rate.
doi: 10.1103/PhysRevC.65.034614
2002WA09 Nucl.Sci.Eng. 141, 171 (2002) C.Wagemans, J.Wagemans, O.Serot The 234U(nth, f) Cross Section Revisited NUCLEAR REACTIONS 234U(n, F), E=thermal; measured fission σ. Revision of previous result.
doi: 10.13182/NSE02-A2276
2001GO29 Nucl.Phys. A688, 233c (2001) G.Goeminne, C.Wagemans, J.Wagemans, P.Geltenbort, M.Loiselet, M.Gaelens, B.Denecke, U.Koester Investigation of the 37Ar(n, p)37Cl, 37Ar(n, α)34S and 39Ar(n, α)36S Reactions at Various Stellar Temperatures NUCLEAR REACTIONS 37Ar(n, p), (n, α), 39Ar(n, α), E<100 keV; measured Ep, Eα, Eγ, σ, Maxwellian averaged σ. Comparison with statistical model calculations.
doi: 10.1016/S0375-9474(01)00705-9
2001WA28 Nucl.Phys. A688, 490c (2001) J.Wagemans, C.Wagemans, G.Goeminne, P.Geltenbort Detailed Investigation of the 14N(n, p)14C, 17O(n, α)14C, 26Al(n, p)26Mg and 26Al(n, α)23Na Reactions NUCLEAR REACTIONS 14N(n, p), 17O(n, α), 26Al(n, p), (n, α), E=thermal; measured σ. Comparison with earlier data.
doi: 10.1016/S0375-9474(01)00765-5
2001WA46 Nucl.Phys. A696, 31 (2001) J.Wagemans, C.Wagemans, G.Goeminne, P.Geltenbort, A.Moens Investigation of the Thermal 26Al(n, pi)26Mg and 26Al(n, αi)23Na Reactions NUCLEAR REACTIONS 26Al(n, p), (n, α), E=thermal; measured Eα, Ep, yields; deduced σ; calculated branching ratios.
doi: 10.1016/S0375-9474(01)01125-3
2001WA50 Hyperfine Interactions 132, 323 (2001) C.Wagemans, J.Wagemans, G.Goeminne Determination of Atomic Masses and Nuclear Binding Energies via Neutron Induced Reactions NUCLEAR REACTIONS 99Ru, 153Gd(n, α), E=thermal; 36Cl, 40K(n, p), E=thermal; 36S, 40Ar(p, n), E ≈ 2 MeV; analyzed particle spectra; deduced mass differences, binding energies.
doi: 10.1023/A:1011968519381
2000GO32 Nucl.Phys. A678, 11 (2000) G.Goeminne, C.Wagemans, J.Wagemans, O.Serot, M.Loiselet, M.Gaelens Investigation of the 37Ar(n, p)37Cl and 37Ar(n, α)34S Reactions in the Neutron Energy Range from 10 meV to 100 keV NUCLEAR REACTIONS 37Ar(n, α), E < 100 keV; measured σ; deduced resonance parameters. 37Ar(n, α), (n, p), E < 1000 keV; calculated Maxwellian averaged σ. Astrophysical implications discussed.
doi: 10.1016/S0375-9474(00)00312-2
2000SE09 Eur.Phys.J. A 8, 187 (2000) Description of Long-Range Alpha Emission using the Sudden Approximation RADIOACTIVITY 238,240,242,244Pu(SF); calculated long-range alpha emission probabilities, angular distributions. Comparison with data.
doi: 10.1007/s100500070105
2000WA15 Phys.Rev. C61, 064601 (2000) J.Wagemans, C.Wagemans, G.Goeminne, P.Geltenbort Experimental Determination of the 14N(n, p)14C Reaction Cross Section for Thermal Neutrons NUCLEAR REACTIONS 14N(n, p), E=thermal; measured σ. 17O(n, α), E=thermal; deduced renormalized σ. Astrophysical implications discussed.
doi: 10.1103/PhysRevC.61.064601
2000WA36 Nucl.Sci.Eng. 136, 415 (2000) C.Wagemans, O.Serot, P.Geltenbort, O.Zimmer Experimental Determination of the 236U(nth, f) Cross Section NUCLEAR REACTIONS 236U(n, F), E=thermal; measured fission σ. Comparison with previous results.
doi: 10.13182/NSE00-A2170
1999BI06 Nucl.Phys. A647, 3 (1999) R.Bieber, C.Wagemans, G.Goeminne, J.Wagemans, B.Denecke, M.Loiselet, M.Gaelens, P.Geltenbort, H.Oberhummer Thermal Neutron Induced (n, p) and (n, α) Reactions on 37Ar NUCLEAR REACTIONS 37Ar(n, α), (n, αγ), (n, p), E=thermal; measured α spectra, proton spectra; deduced reaction σ, (n, α0)/(n, α1) branching ratio. Comparison with previous data.
doi: 10.1016/S0375-9474(99)00013-5
1998SE17 Nucl.Phys. A641, 34 (1998) Energy Distributions and Yields of Long Range Alpha Particles Emitted During Spontaneous Fission of 238, 240, 242, 244Pu Isotopes RADIOACTIVITY 238,240,242,244Pu(SF); measured α spectra, yields of long range alpha particles; deduced fission mode, excitation energy dependence.
doi: 10.1016/S0375-9474(98)00465-5
1998WA06 Phys.Rev. C57, 1766 (1998) C.Wagemans, R.Bieber, H.Weigmann, P.Geltenbort Determination of the Thermal Neutron Induced 41Ca(n, p)41K and 41Ca(n, α)38Ar Reaction Cross Sections NUCLEAR REACTIONS 41Ca(n, p), (n, α), E=thermal; measured σ, Eα. 42Ca deduced level, J, π, primary γ-transition multipolarity. Surface barrier detector.
doi: 10.1103/PhysRevC.57.1766
1998WA31 Phys.Rev. C58, 2840 (1998) J.Wagemans, C.Wagemans, R.Bieber, P.Geltenbort Determination of the Thermal Neutron Induced 17O(n, α)14C Reaction Cross Section NUCLEAR REACTIONS 17O(n, α), E=thermal; measured σ. Enriched gas target.
doi: 10.1103/PhysRevC.58.2840
1997DE11 Nucl.Phys. A617, 331 (1997) L.Dematte, C.Wagemans, R.Barthelemy, P.D'hondt, A.Deruytter Fragments' Mass and Energy Characteristics in the Spontaneous Fission of 236Pu, 238Pu, 240Pu, 242Pu, and 244Pu RADIOACTIVITY 236,238,240,242,242Pu(SF); measured fission fragment complementary kinetic energies; deduced energy, mass distributions, mass-energy correlations, cold fission events. Fission mode analysis.
doi: 10.1016/S0375-9474(97)00032-8
1996WA04 Nucl.Phys. A597, 188 (1996) C.Wagemans, L.Dematte, S.Pomme, P.Schillebeeckx Mass and Energy Distributions for 243Am(n(th), f) NUCLEAR REACTIONS 243Am(n, F), E=thermal; measured fission fragment mass-energy correlations; deduced mass, energy yields. Fission mode analysis.
doi: 10.1016/0375-9474(95)00439-4
1996WA15 Phys.Rev. C54, 389 (1996) C.Wagemans, R.Bieber, P.Geltenbort Determination of the Thermal Neutron Induced 36Cl(n, p)36S and 36Cl(n, α)33P Reaction Cross Sections NUCLEAR REACTIONS 36Cl(n, p), (n, α), E=thermal; measured σ(n, α), σ(n, p), reaction σ; deduced existence of negative resonance.
doi: 10.1103/PhysRevC.54.389
1995PO09 Nucl.Phys. A587, 1 (1995) Ternary-to-Binary Fission Ratios in the Resonances for 235U(n, f) NUCLEAR REACTIONS 235U(n, F), E=thermal-2500 eV; measured α-, triton-emission probability versus E in ternary fission; deduced correlation with fission modes and resonance spin.
doi: 10.1016/0375-9474(94)00814-4
1995PO18 Nucl.Instrum.Methods Phys.Res. A359, 587 (1995) S.Pomme, C.Wagemans, F.Verhaegen, L.Van Den Durpel, J.Van Gils, R.Barthelemy A Double ΔE-E Detection Set-Up for Ternary Fission NUCLEAR REACTIONS 235U(n, F), E not given; measured α-, triton spectra following ternary fission; deduced comparison with computer simulation. Double ΔE-E detection set up. RADIOACTIVITY 252Cf(SF); measured α-, triton total energy spectra following ternary fission; deduced comparison with computer simulation. Double ΔE-E detection set up.
doi: 10.1016/0168-9002(95)00070-4
1994DR06 Nucl.Phys. A573, 291 (1994) S.Druyts, C.Wagemans, P.Geltenbort Determination of the 35Cl(n, p)35S Reaction Cross Section and Its Astrophysical Implications NUCLEAR REACTIONS 35Cl(n, p), E=thermal-100 keV; measured proton yield vs E; deduced reaction, maxwellian averaged σ; calculated (n, p)/(n, γ) branching ratio.
doi: 10.1016/0375-9474(94)90172-4
1994SC33 Nucl.Phys. A580, 15 (1994) P.Schillebeeckx, C.Wagemans, P.Geltenbort, F.Gonnenwein, A.Oed Investigation of Mass, Charge and Energy of 241Pu(n(th), f) Fragments with the Cosi-Fan-Tutte Spectrometer NUCLEAR REACTIONS 241Pu(n, F), E=thermal; measured fission light-fragment mass-charge-energy correlations; deduced different mass, energy, charge yields, proton even-odd effect on yield, kinetic energy. Fission-mode analysis.
doi: 10.1016/0375-9474(94)90812-5
1994WA17 Phys.Rev. C50, 487 (1994) C.Wagemans, S.Druyts, P.Geltenbort Characteristics of the 50V(n(th), p)50Ti Reaction NUCLEAR REACTIONS 50V(n, p), E=thermal; measured σ, high precision. 50V, 50Ti deduced mass difference.
doi: 10.1103/PhysRevC.50.487
1993WA14 Nucl.Sci.Eng. 115, 173 (1993) C.Wagemans, P.Van Uffelen, A.Deruytter, R.Barthelemy, J.Van Gils Normalization of the 239Pu Fission Cross Section NUCLEAR REACTIONS 239Pu(n, F), E=0.01-1000 eV; measured fission σ(E); deduced normalization.
doi: 10.13182/NSE93-A28527
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
1991EY01 Nucl.Instrum.Methods Phys.Res. A303, 152 (1991) R.Eykens, A.Goetz, A.Lamberty, J.Van Gestel, J.Pauwels, C.Wagemans, S.Druyts, P.D'hondt Preparation and Characterization of 35Cl and 36Cl Samples for (n, p) Cross Section Measurements NUCLEAR REACTIONS 35,36Cl(n, p), E=thermal; measured particle spectra; deduced reaction σ.
doi: 10.1016/0168-9002(91)90779-P
1989WA02 Nucl.Sci.Eng. 101, 293 (1989) C.Wagemans, P.Schillebeeckx, J.P.Bocquet Measurement of the Thermal Neutron Induced Fission Cross Section of 243Am NUCLEAR REACTIONS 243Am(n, F), E=thermal; measured fission σ. Pure sample.
doi: 10.13182/NSE89-A23617
1989WA29 Nucl.Phys. A502, 287c (1989) C.Wagemans, P.Schillebeeckx, A.Deruytter Investigation of Neutron Shell Effects and Fission Channels in the Spontaneous Fission of the Pu-Isotopes RADIOACTIVITY 236,238,240,242,244Pu(SF); measured fission fragment energy, mass distribution. Model analyses.
doi: 10.1016/0375-9474(89)90669-6
1989WA31 Nucl.Instrum.Methods Phys.Res. A282, 4 (1989) On the Necessity of Alternative Methods to Determine Sample Thicknesses and Masses NUCLEAR REACTIONS 41Ca(n, α), E=thermal; measured σ(Eα). 237Np(n, F), E=thermal; measured fission fragment yield vs mass. Sample thickness, mass determination, alternative method necessity.
doi: 10.1016/0168-9002(89)90102-2
1988DE33 Phys.Rev. C38, 1270 (1988) A.D'Eer, C.Wagemans, M.Neve de Mevergnies, F.Gonnenwein, P.Geltenbort, M.S.Moore, J.Pauwels Neutron-Induced Fission of the 26 min 235U Isomer NUCLEAR REACTIONS 235,235mU(n, F), E=cold, thermal; measured isomer to ground state fission σ ratio. Target production from 239Pu decay.
doi: 10.1103/PhysRevC.38.1270
1987WA20 Nucl.Phys. A469, 497 (1987) C.Wagemans, H.Weigmann, R.Barthelemy Measurement and Resonance Analysis of the 33S(n, α) Cross Section NUCLEAR REACTIONS 33S(n, α), E=0.010-1 MeV; measured σ(E). 34S deduced resonaces, Γα, (gΓnΓα/Γ), J, π. R-matrix analysis.
doi: 10.1016/0375-9474(87)90035-2
1986WA05 Phys.Rev. C33, 943 (1986) C.Wagemans, P.D'hondt, P.Schillebeeckx, R.Brissot Triton and Alpha Emission in the Thermal-Neutron-Induced Ternary Fission of 233U, 235U, 239Pu, and 241Pu NUCLEAR REACTIONS 233,235U, 239,241Pu(n, αF), (n, tF), (n, α), E=thermal; measured ternary fission α-, triton yield, energy distributions; deduced σ(n, α0) upper-limit.
doi: 10.1103/PhysRevC.33.943
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
1985WA26 Nucl.Instrum.Methods 236, 429 (1985) Some Users' Comments on the Fabrication, assaying and Use of Samples for Nuclear Measurements NUCLEAR REACTIONS 235U, 237Np(n, F), E=thermal; measured fission fragment spectra, yield vs mass. Sample fabrication, assaying discussion. RADIOACTIVITY 210Po(α) [from 209Bi(n, γ)210Bi(β-decay)]; measured Eα, Iα. Sample fabrication, assaying discussion.
doi: 10.1016/0168-9002(85)90938-6
1984DH05 Ann.Nucl.Energy 11, 485 (1984) P.D'Hondt, C.Wagemans, A.Emsallem, R.Brissot Measurement of the Thermal-Neutron-Induced Fission Cross-Section of 238U NUCLEAR REACTIONS 238U(n, F), E=thermal; measured fission fragment spectra, fission σ relative to 235U. 239U deduced negative energy resonances.
doi: 10.1016/0306-4549(84)90073-2
1984EM01 Z.Phys. A315, 201 (1984) A.Emsallem, M.Asghar, P.D'Hondt, C.Wagemans Thermal Neutron Induced α-Particle Reaction on 64, 65, 67Zn and 77Se NUCLEAR REACTIONS 64,65,67Zn, 77Se(n, α), E=thermal; measured σ(Eα). 65,66,68Zn, 78Se deduced resonances contributing to α-decay. 61,62,64Ni, 74Ge levels deduced α-branching. Natural, enriched, radioactive targets.
doi: 10.1007/BF01419380
1984WA10 Phys.Rev. C30, 218 (1984) C.Wagemans, E.Allaert, A.Deruytter, R.Barthelemy, P.Schillebeeckx Comparison of the Energy and Mass Characteristics of the 239Pu(n(th), f) and the 240Pu(sf) Fragments RADIOACTIVITY 240Pu(SF); measured fission fragment mass, energy distributions, correlations; deduced fission characteristics. Comparison with thermal neutron induced fission on 239Pu. NUCLEAR REACTIONS 239Pu(n, F), E=thermal; measured fission fragment mass, energy distributions, correlations; deduced fission characteristics. Comparison with 240Pu spontaneous fission decay.
doi: 10.1103/PhysRevC.30.218
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
1981CA13 Nucl.Phys. A369, 15 (1981) F.Caitucoli, C.Wagemans, P.Perrin, E.Allaert, P.D'Hondt, M.Asghar Mass and Energy Characteristics of the 241Pu(n(th), f) Fragments NUCLEAR REACTIONS, Fission 241Pu(n, F), E=thermal; measured fragment kinetic energies; deduced energy, mass distributions, mass-energy correlations.
doi: 10.1016/0375-9474(81)90003-8
1981EM03 Nucl.Phys. A368, 108 (1981) A.Emsallem, M.Asghar, C.Wagemans, H.Weigmann Study of Neutron Induced Charged Particle Reactions on 40K. (I). Thermal Neutrons NUCLEAR REACTIONS 40K(n, α), (n, p), E=thermal; measured Eα, E(p), σ(Eα), σ(Ep); deduced Q(p), primary gamma-ray multipolarity.
doi: 10.1016/0375-9474(81)90733-8
1981WA11 Nucl.Phys. A362, 1 (1981) C.Wagemans, E.Allaert, A.De Clercq, P.D'Hondt, A.Deruytter, G.Barreau, A.Emsallem The (n(th), α) Reaction on 233U, 235U and 238U and Determination of the 238U(n(th), α)235Th Reaction Characteristics NUCLEAR REACTIONS 233,238U(n, α), E=thermal; measured σ(Eα). 235U(n, α), E=thermal; measured σ(Eα); deduced Qα. 235Th deduced mass, Qβ.
doi: 10.1016/0375-9474(81)90666-7
1981WA25 Nucl.Phys. A369, 1 (1981) C.Wagemans, E.Allaert, F.Caitucoli, P.D'Hondt, G.Barreau, P.Perrin Experimental Study of Some Important Characteristics of the Thermal Neutron Induced Fission of 237Np NUCLEAR REACTIONS, Fission 237Np(n, F), E=thermal; measured fragment kinetic energies, ternary α-particles; deduced energy, mass distribution, mass-energy correlations, fission neutron emission curve.
doi: 10.1016/0375-9474(81)90002-6
1981WA31 Nucl.Instrum.Methods 190, 167 (1981) C.Wagemans, E.Allaert, G.Barreau, A.Emsallem, P.D'Hondt Determination of Atomic Masses via (n(th), p) and (n(th), α) Reactions NUCLEAR REACTIONS 153Gd(n, α), 50V(n, p), E=thermal; measured σ(Eα), σ(Ep); deduced Q. 153Gd deduced mass. 50V, 50Ti, 153Gd, 150Sm deduced mass difference. 235Th deduced mass. Analyzed (n, α) data, 238U mass input.
doi: 10.1016/0029-554X(81)90217-2
1981WE12 Nucl.Phys. A368, 117 (1981) H.Weigmann, C.Wagemans, A.Emsallem, M.Asghar Study of Neutron Induced Charged Particle Reactions on 40K. (II). Resonance Neutrons NUCLEAR REACTIONS 40K(n, α), (n, p), E=0.00002-70 keV; measured σ(Eα), σ(Ep). 41K deduced resonances, L, J, π, < Γp >, < Γα >, level density spin cut-off parameter.
doi: 10.1016/0375-9474(81)90734-X
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
1980DH03 Nucl.Phys. A346, 461 (1980) P.D'Hondt, C.Wagemans, A.Declercq, G.Barreau, A.Deruytter Energy Distribution and Absolute Yields of the Charged Light Particles Emitted During the Thermal Neutron Induced Ternary Fission of 235U NUCLEAR REACTIONS, Fission 235U(n, F), E=thermal; measured ternary fission particle yield, energy distribution.
doi: 10.1016/0375-9474(80)90480-7
1980WA18 Ann.Nucl.Energy 7, 495 (1980) C.Wagemans, G.Coddens, H.Weigmann, R.Barthelemy Measurement of the 239Pu(n, F)Cross Section from Thermal up to 30 keV Neutron Energy NUCLEAR REACTIONS, Fission 239Pu(n, F), E=thermal-30 keV; measured σ(E).
doi: 10.1016/0306-4549(80)90095-X
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
1978AS08 Nucl.Phys. A311, 205 (1978) M.Asghar, F.Caitucoli, P.Perrin, C.Wagemans Fission Fragment Energy Correlation Measurements for the Thermal Neutron Fission of 239Pu and 235U NUCLEAR REACTIONS 239Pu, 235U(n, F), E=thermal; measured reaction products; deduced complementary fragment kinetic energies, fragment mass-versus energy correlations.
doi: 10.1016/0375-9474(78)90510-9
1978AS09 Nucl.Phys. A311, 413 (1978) M.Asghar, F.Caitucoli, P.Perrin, C.Guet, P.D'Hondt, C.Wagemans Fission Fragment Energy Correlation Measurements for the Thermal Neutron Sub-Barrier Fission of 231Pa NUCLEAR REACTIONS 235U, 231Pa(n, F), E=th; measured complementary fragment kinetic energies; deduced fragment mass-versus-energy correlations.
doi: 10.1016/0375-9474(78)90522-5
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
1978EM01 Z.Phys. A286, 411 (1978) A.Emsallem, M.Asghar, C.Wagemans, P.D'hondt Search for the (n(th), α) Reaction on 180Hf, 181Ta and 209Bi NUCLEAR REACTIONS 180Hf, 181Ta, 209Bi(n, α), E=th; measured σ(Eα).
doi: 10.1007/BF01408899
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
1977AS08 Nucl.Phys. A292, 225 (1977) M.Asghar, P.D'Hondt, C.Guet, P.Perrin, C.Wagemans Fission Fragment Energy Correlation Measurements for the Thermal Neutron Sub-Barrier Fission of 237Np and Above-the-Barrier Fission of 235U NUCLEAR REACTIONS 237Np, 235U(n, F), E=th; measured complementary fragment kinetic energies; deduced average kinetic energies, σ, fragment mass versus energy correlations.
doi: 10.1016/0375-9474(77)90370-0
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
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
1975WE18 Phys.Rev.Lett. 35, 1213 (1975) H.Weigmann, J.A.Wartena, C.Wagemans Are There Fission-Fragment Energy Variations in 235U Neutron Resonances (Question) NUCLEAR REACTIONS 235U(n, X), E < 25 eV; measured σ(E); deduced no resonance energy variations.
doi: 10.1103/PhysRevLett.35.1213
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
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
1970VA15 J.Phys. (Paris) 31, 149 (1970) Calcul de la Diffusion d'Electrons du Niveau a 3, 56 MeV du 6Li dans le Cadre de la Theorie de Hartree-Fock Generalisee NUCLEAR REACTIONS 6Li(e, e'), E not given; calculated form factor for 3.56-MeV excitation. Generalized Hartree-Fock theory.
doi: 10.1051/jphys:01970003102-3014900
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