NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = J.M.Maison Found 71 matches. 2017BE31 Phys.Rev. C 96, 054601 (2017) A.Belhout, S.Ouichaoui, H.Beaumevieille, A.Bouchemha, G.Bogaert, S.Fortier, J.Kiener, A.Lefebvre-Schuhl, J.M.Maison, L.Rosier, J.Rotbard, V.Tatischeff, J.P.Thibaud, J.Vernotte New determination of proton spectroscopic factors and reduced widths for 8Be states in the 16.5-18.0 MeV excitation energy region via the study of the 7Li(3He, d)8Be transfer reaction at Elab=20 MeV: Implication for the 7Li(p, α)4He hydrogen burning reaction NUCLEAR REACTIONS 7Li(3He, d)8Be, E=20 MeV; measured E(d), I(d), σ, σ(θ) using split-pole magnetic spectrometer and a ΔE-E position-sensitive drift chamber at the Orsay 14.8-MV tandem accelerator facility. Nonlocal, finite-range (FR)-distorted-wave Born approximation (DWBA) analysis of cross section data. 8Be; deduced levels, J, π, isospin, absolute and partial spectroscopic factors. Comparison with previous experimental results, and with shell-model calculations. Relevance to 7Li(p, α)4He hydrogen burning in astrophysical applications.
doi: 10.1103/PhysRevC.96.054601
2007BE45 Nucl.Phys. A793, 178 (2007) A.Belhout, S.Ouichaoui, H.Beaumevieille, A.Boughrara, S.Fortier, J.Kiener, J.M.Maison, S.K.Mehdi, L.Rosier, J.P.Thibaud, A.Trabelsi, J.Vernotte Measurement and DWBA analysis of the 12C(6Li, d)16O α-transfer reaction cross sections at 48.2 MeV. R-matrix analysis of 12C(α, γ)16O direct capture reaction data NUCLEAR REACTIONS 12C(6Li, d), E=48.2 MeV; measured Ed, σ(θ) to first eleven states of 16O; deduced level energies, widths, spectroscopic factors. DWBA analysis. 12C(α, γ), E(cm)≈ 0-3 MeV; analyzed σ; deduced resonance parameters. R-Matrix calculations. Astrophysical implications discussed.
doi: 10.1016/j.nuclphysa.2007.06.008
2001BE45 Phys.Lett. 514B, 226 (2001) D.Beaumel, T.Kubo, T.Teranishi, H.Sakurai, S.Fortier, A.Mengoni, N.Aoi, N.Fukuda, M.Hirai, N.Imai, H.Iwasaki, H.Kumagai, H.Laurent, S.M.Lukyanov, J.M.Maison, T.Motobayashi, T.Nakamura, H.Ohnuma, S.Pita, K.Yoneda, M.Ishihara Determination of the Astrophysical S Factor of the 8B(p, γ)9C Capture Reaction from the d(8B, 9C)n Reaction NUCLEAR REACTIONS 2H(8B, 9C), E=14.4 MeV/nucleon; measured excitation energy spectra, σ(θ); deduced asymtotic normalization coefficients. 8B(p, γ), E(cm) ≈ 1-100 keV; deduced astrophysical S-factor.
doi: 10.1016/S0370-2693(01)00828-0
2001CA45 Phys.Lett. 516B, 21 (2001) F.Cappuzzello, A.Cunsolo, S.Fortier, A.Foti, M.Khaled, H.Laurent, H.Lenske, J.M.Maison, A.L.Melita, C.Nociforo, L.Rosier, C.Stephan, L.Tassan-Got, J.S.Winfield, H.H.Wolter Excited States of 11Be NUCLEAR REACTIONS 11B(7Li, 7Be), E=57 MeV; measured particle spectra. 11Be deduced levels, widths, core excitation. 7Be deduced excited state. Quasiparticle RPA calculations.
doi: 10.1016/S0370-2693(01)00940-6
2001KH17 Nucl.Phys. A694, 103 (2001) E.Khan, T.Suomijarvi, Y.Blumenfeld, V.G.Nguyen, N.Alamanos, F.Auger, E.Bauge, D.Beaumel, J.P.Delaroche, P.Delbourgo-Salvador, A.Drouart, S.Fortier, N.Frascaria, A.Gillibert, M.Girod, C.Jouanne, K.W.Kemper, A.Lagoyannis, V.Lapoux, A.Lepine-Szily, I.Lhenry, J.Libert, F.Marechal, J.M.Maison, A.Musumarra, S.Ottini-Hustache, P.Piattelli, S.Pita, E.C.Pollacco, P.Roussel-Chomaz, D.Santonocito, J.E.Sauvestre, J.A.Scarpaci, T.Zerguerras Proton Scattering from the Unstable Nuclei 30S and 34Ar: Structural evolution along the sulfur and argon isotopic chains NUCLEAR REACTIONS 1H(30S, 30S'), (32S, 32S'), E=53 MeV/nucleon; 1H(34Ar, 34Ar'), E=47 MeV/nucleon; measured recoil proton spectra, σ(E, θ). 30,32S, 34Ar deduced levels, J, π, deformation. Optical model analysis. NUCLEAR STRUCTURE 30,32,34,36,38,40,42,44S, 34,36,38,40,42,44,46Ar; calculated proton and neutron radii, density distributions. Quasiparticle RPA, Skyrme interaction.
doi: 10.1016/S0375-9474(01)00981-2
2001WI05 Nucl.Phys. A683, 48 (2001) J.S.Winfield, S.Fortier, W.N.Catford, S.Pita, N.A.Orr, J.Van de Wiele, Y.Blumenfeld, R.Chapman, S.P.G.Chappell, N.M.Clarke, N.Curtis, M.Freer, S.Gales, H.Langevin-Joliot, H.Laurent, I.Lhenry, J.M.Maison, P.Roussel-Chomaz, M.Shawcross, K.Spohr, T.Suomijarvi, A.de Vismes Single-Neutron Transfer from 11Begs via the (p, d) Reaction with a Radioactive Beam NUCLEAR REACTIONS 1H(11Be, 10Be), E=35.3 MeV/nucleon; 1H(15N, 14N), E=38.9 MeV/nucleon; measured σ(θ). 11Be levels deduced spectroscopic factors, configurations. Vibrational coupling model, radioactive beam.
doi: 10.1016/S0375-9474(00)00463-2
1999FO09 Phys.Lett. 461B, 22 (1999) S.Fortier, S.Pita, J.S.Winfield, W.N.Catford, N.A.Orr, J.Van de Wiele, Y.Blumenfeld, R.Chapman, S.P.G.Chappell, N.M.Clarke, N.Curtis, M.Freer, S.Gales, K.L.Jones, H.Langevin-Joliot, H.Laurent, I.Lhenry, J.M.Maison, P.Roussel-Chomaz, M.Shawcross, M.Smith, K.Spohr, T.Suomijarvi, A.de Vismes Core Excitation in 11Begs via the p(11Be, 10Be)d Reaction NUCLEAR REACTIONS 1H(11Be, 10Be), E=35.3 MeV/nucleon; measured particle spectra, (particle)d-coin, σ(E, θ). 11Be deduced core excitation, vibrational coupling. DWBA analysis. Secondary beam from 15N fragmentation.
doi: 10.1016/S0370-2693(99)00825-4
1999VE09 Nucl.Phys. A655, 415 (1999) J.Vernotte, G.Berrier-Ronsin, S.Fortier, E.Hourani, A.Khendriche, J.M.Maison, L.-H.Rosier, G.Rotbard, E.Caurier, F.Nowacki One-Nucleon Pickup Reactions on 32S: Experimental results and shell-model calculations NUCLEAR REACTIONS 32S(d, 3He), E=27 MeV; measured excitation energies. 32S(3He, α), E=25 MeV; measured excitation energies, σ(E, θ). 31P, 31S levels deduced spectroscopic factors. Comparison with shell-model predictions.
doi: 10.1016/S0375-9474(99)00301-2
1999WI04 J.Phys.(London) G25, 755 (1999) J.S.Winfield, S.Fortier, W.N.Catford, S.Pita, N.A.Orr, Y.Blumenfeld, R.Chapman, S.P.G.Chappell, N.M.Clarke, N.Curtis, M.Freer, S.Gales, K.L.Jones, H.Langevin-Joliot, H.Laurent, I.Lhenry, J.-M.Maison, P.Roussel-Chomaz, M.Shawcross, M.Smith, K.Spohr, T.Suomijarvi, A.de Vismes Structure of 11Be from the (d, p) Reaction in Inverse Kinematics NUCLEAR REACTIONS 1H(11Be, 10Be), E=35 MeV/nucleon; measured d, Be spectra, yield vs excitation energy. 11Be deduced halo features.
doi: 10.1088/0954-3899/25/4/029
1998VE01 Phys.Rev. C57, 1256 (1998) J.Vernotte, G.Berrier-Ronsin, S.Fortier, E.Hourani, J.Kalifa, J.M.Maison, L.-H.Rosier, G.Rotbard, B.H.Wildenthal 25Mg(d, 3He)24Na Reaction at 29 MeV and a Spectroscopic Analysis of the Levels of 24Na NUCLEAR REACTIONS 27Al, 29Si, 25Mg(d, 3He), E=29 MeV; measured σ(E(3He), θ). 24Na deduced levels, J, π, spectroscopic factors. DWBA analysis, shell model calculations.
doi: 10.1103/PhysRevC.57.1256
1997BE07 Phys.Rev. C55, 1200 (1997) G.Berrier-Ronsin, G.Rotbard, M.Vergnes, S.Fortier, J.M.Maison, L.-H.Rosier, J.Vernotte, P.Van Isacker, J.Jolie Transfer Results for Odd-Odd 198Au as a Test of Extended Supersymmetry NUCLEAR REACTIONS 197Au(d, p), E=22 MeV; measured σ(θ), spectra. 198Au deduced levels, spectroscopic strengths. DWBA analysis, interacting boson models, supersymmetry.
doi: 10.1103/PhysRevC.55.1200
1997DE14 Phys.Rev. C55, 3149 (1997) F.de Oliveira, A.Coc, P.Aguer, G.Bogaert, J.Kiener, A.Lefebvre, V.Tatischeff, J.-P.Thibaud, S.Fortier, J.M.Maison, L.Rosier, G.Rotbard, J.Vernotte, S.Wilmes, P.Mohr, V.Kolle, G.Staudt Comparison of Low-Energy Resonances in 15N(α, γ)19F and 15O(α, γ)19Ne and Related Uncertainties NUCLEAR REACTIONS 15O, 15N(α, γ), 15N(7Li, t), E not given; analyzed uncertainties in resonance strengths. 19Ne, 19F deduced resonance widths.
doi: 10.1103/PhysRevC.55.3149
1997LE14 Nucl.Phys. A621, 199c (1997); Erratum Nucl.Phys. A628, 686 (1998) A.Lefebvre, S.Vouzoukas, P.Aguer, G.Bogaert, A.Coc, A.Denker, F.de Oliveira, S.Fortier, J.Gorres, J.Kiener, J.M.Maison, M.G.Porquet, L.Rosier, V.Tatischeff, J.P.Thibaud, M.Wiescher 31S(p, γ)32Cl Reaction in Explosive Hydrogen Burning NUCLEAR REACTIONS 32S(3He, t), E=24 MeV; measured γt-coin; deduced reaction rates. 32Cl deduced levels, resonance strengths, widths.
doi: 10.1016/S0375-9474(97)00238-8
1996BE16 Nucl.Phys. A599, 265c (1996) D.Beaumel, S.Fortier, S.Gales, J.Guillot, H.Langevin-Joliot, H.Laurent, J.M.Maison, J.Vernotte, J.Bordewijk, S.Brandenburg, A.Krasznahorkay, G.M.Crawley, C.P.Massolo, M.Renteria, A.Khendriche Decay Properties of High-Lying Single-Particles Modes NUCLEAR REACTIONS 64Ni, 90Zr, 120Sn, 208Pb(α, n3He), E=120 MeV; measured neutron spectra, nn(θ). 91Zr, 209Pb deduced resonances, J, π, neutron decay features.
doi: 10.1016/0375-9474(96)00068-1
1996DE07 Nucl.Phys. A597, 231 (1996) F.de Oliveira, A.Coc, P.Aguer, C.Angulo, G.Bogaert, J.Kiener, A.Lefebvre, V.Tatischeff, J.-P.Thibaud, S.Fortier, J.M.Maison, L.Rosier, G.Rotbard, J.Vernotte, M.Arnould, A.Jorissen, N.Mowlavi Determination of α-Widths in 19F Relevant to Fluorine Nucleosynthesis NUCLEAR REACTIONS 15N(7Li, t), (7Li, 7Li), E=28 MeV; measured σ(θ); deduced astrophysical reaction rate. 19F levels deduced α-width, spectroscopic factors. Finite-range DWBA analysis, Hauser-Feshbach contribution, α-transfer reactions, cluster model. Enriched gas target.
doi: 10.1016/0375-9474(95)00455-6
1996WI05 Phys.Rev. C54, 125 (1996) J.S.Winfield, D.Beaumel, S.Gales, H.Laurent, I.Lhenry, J.M.Maison, G.M.Crawley, S.Danczyk, S.E.Hirzebruch, J.C.Stasko, T.Suomijarvi The (7Li, 7Beγ) Reaction and Isovector Spin Strength in 40Ca NUCLEAR REACTIONS 12C, 40Ca(7Li, 7Be), E=70 MeV/nucleon; measured (particle)γ-coin. 40Ca deduced continuum isovector spin strength. Spectrometer, CsI detectors.
doi: 10.1103/PhysRevC.54.125
1995FO19 Phys.Rev. C52, 2401 (1995) S.Fortier, D.Beaumel, S.Gales, J.Guillot, H.Langevin-Joliot, H.Laurent, J.M.Maison, J.Bordewijk, S.Brandenburg, A.Krasznahorkay, G.M.Crawley, C.P.Massolo, M.Renteria, A.Khendriche Damping of Unbound Single-Particle Modes NUCLEAR REACTIONS 64Ni, 90Zr, 120Sn(α, 3He), E=120 MeV; measured 3He-spectra, neutron spectra following residual decay, n(3He)-coin. 91Zr, 121Sn, 65Ni deduced non-statistical neutron branching ratios. Statistical analysis.
doi: 10.1103/PhysRevC.52.2401
1995LA22 Phys.Rev. C52, 3066 (1995) H.Laurent, J.A.Scarpaci, D.Beaumel, Y.Blumenfeld, S.Fortier, N.Frascaria, S.Gales, J.P.Garron, J.Guillot, I.Lhenry, J.C.Roynette, J.M.Maison, T.Suomijarvi, A.Gillibert, P.Roussel-Chomaz, A.Van der Woude Role of the Breakup Process in the 48Ca(20Ne, 19Ne n) Reaction at 48A MeV NUCLEAR REACTIONS 48Ca(20Ne, n19Ne), E=48 MeV/nucleon; measured E(19Ne), En, σ(En, θ); deduced neutron multiplicity, reaction mechanism. Breakup process model.
doi: 10.1103/PhysRevC.52.3066
1995LH02 Nucl.Phys. A583, 115c (1995) I.Lhenry, D.Beaumel, S.Fortier, S.Gales, H.Laurent, J.M.Maison, F.Azaiez, Y.Blumenfeld, J.Guillot, H.Langevin-Joliot, T.Suomijarvi, S.Brandenburg, G.M.Crawley, J.Finck, J.Stasko A Search for the Isovector Monopole Resonance in 208Pb NUCLEAR REACTIONS 208Pb(13C, 13N), E=60 MeV/nucleon; measured σ(θ), missing energy spectra. 208Tl deduced level, neutron decay features.
doi: 10.1016/0375-9474(94)00643-2
1994BE07 Phys.Rev. C49, 2444 (1994) D.Beaumel, S.Fortier, S.Gales, J.Guillot, H.Langevin-Joliot, H.Laurent, J.M.Maison, J.Vernotte, J.A.Bordewijk, S.Brandenburg, A.Krasznahorkay, G.M.Crawley, C.P.Massolo, M.Renteria Decay Modes of High-Lying Single-Particle States in 209Pb NUCLEAR REACTIONS 208Pb(α, n3He), E=122 MeV; measured E(3He), (3He)n-, γ(3He)-coin, neutron angular correlations. 209Pb deduced direct decay branching ratios, Γ(spreading)/Γ, Γn/Γ for structures at high excitation. Statistical model calculations.
doi: 10.1103/PhysRevC.49.2444
1994LA10 Nucl.Phys. A569, 297c (1994) H.Laurent, S.Gales, D.Beaumel, G.M.Crawley, J.E.Finck, S.Fortier, J.M.Maison, C.P.Massolo, D.J.Mercer, J.S.Winfield, G.H.Yoo Spin-Isospin Multipole Excitations by Means of the (6Li, 6He) Reaction at 100 A.MeV NUCLEAR REACTIONS 12,13C, 58Ni, 90Zr, 208Pb(6Li, 6He), E=100 MeV/nucleon; measured σ(θ, E(6He)). 13,12N, 58Cu, 90Nb, 208Bi deduced spin-isospin multipole excitation features.
doi: 10.1016/0375-9474(94)90120-1
1994VE02 Phys.Rev. C49, 1559 (1994) J.Vernotte, G.Berrier-Ronsin, S.Fortier, E.Hourani, J.Kalifa, A.Khendriche, J.M.Maison, L.H.Rosier, G.Rotbard 29Si(d, 3He)28Al Reaction at 29 MeV NUCLEAR REACTIONS 29Si(d, 3He), E=29 MeV; measured σ(θ). 28Al deduced levels, L, J, π, S. DWBA analyses, shell model calculations. Enriched target.
doi: 10.1103/PhysRevC.49.1559
1993RO12 Phys.Rev. C47, 1921 (1993) G.Rotbard, G.Berrier, M.Vergnes, S.Fortier, J.Kalifa, J.M.Maison, L.Rosier, J.Vernotte, P.Van Isacker, J.Jolie Transfer Results for Odd-Odd 196Au and the Extended Supersymmetry NUCLEAR REACTIONS 197Au(p, d), E=25 MeV; measured σ(θ), σ(Ed). 196Au deduced levels, L, possible J, π, spectroscopic factors.
doi: 10.1103/PhysRevC.47.1921
1993RO20 Phys.Rev. C48, R2148 (1993) G.Rotbard, G.Berrier-Ronsin, O.Constantinescu, S.Fortier, S.Gales, M.Hussonnois, J.B.Kim, J.M.Maison, L.-H.Rosier, J.Vernotte, Ch.Briancon, R.Kulessa, Yu.Ts.Oganessian, S.A.Karamian Blocking Effect in the 16+ → 16+ (p, t) Transition on the Isomeric 178m2Hf Target NUCLEAR REACTIONS 178Hf(p, t), E=19 MeV; measured σ(θ); deduced aligned quasineutron orbitals blocking effect. 178Hf deduced isomer to isomer, 0+ → 0+ transition σ ratio. Target in isomeric state.
doi: 10.1103/PhysRevC.48.R2148
1993VE03 Phys.Rev. C48, 205 (1993) J.Vernotte, G.Berrier-Ronsin, S.Fortier, E.Hourani, J.Kalifa, J.M.Maison, L.H.Rosier, G.Rotbard, B.H.Wildenthal 27Al(d, 3He)26Mg Reaction at 29 MeV NUCLEAR REACTIONS 27Al(d, 3He), E=29 MeV; measured σ(θ), σ(3He); deduced model parameters. 26Mg deduced levels, J, π, C2S. DWBA analysis. Model comparison.
doi: 10.1103/PhysRevC.48.205
1991MA06 Phys.Rev. C43, 1687 (1991) C.P.Massolo, S.Fortier, S.Gales, F.Azaiez, E.Gerlic, J.Guillot, E.Hourani, H.Langevin-Joliot, J.M.Maison, J.P.Schapira, G.M.Crawley Onset of Neutron Single-Particle Strengths in the Tin Isotopic Chain NUCLEAR REACTIONS 124,122,120,118,116,112Sn(α, 3He), E=183 MeV; measured σ(θ) vs excitation energy; deduced model parameters. 113,117,119,121,123,125Sn levels deduced L, C2S, neutron particle response function. Enriched targets. DWBA analysis.
doi: 10.1103/PhysRevC.43.1687
1989FO01 Phys.Rev. C39, 82 (1989) S.Fortier, S.Gales, E.Hourani, J.M.Maison, C.P.Massolo, J.P.Schapira Neutron-Hole Strengths and Core Coupling in 87Sr via the 88Sr(3He, α)87Sr Reaction NUCLEAR REACTIONS 88Sr(3He, α), E=36 MeV; measured σ(E(α)), σ(θ). 87Sr deduced levels, spectroscopic factors, L. DWBA, CRC analyses. Enriched target.
doi: 10.1103/PhysRevC.39.82
1989HO19 Z.Phys. A334, 277 (1989) E.Hourani, F.Azaiez, Ph.Dessagne, A.Elayi, S.Fortier, S.Gales, J.M.Maison, P.Massolo, Ch.Miehe, A.Richard Search for Proton Radioactivity in 65As, 69Br and 97Y RADIOACTIVITY 65As [from 40Ca(28Si, 2np)]; 69Br [from 40Ca(32S, 2np)]; 97Y [from 40Ca(40Ca, 2np)]; measured particle spectra, (particle)(particle)-coin spectra; deduced no proton activity evidence.
1989LA19 Phys.Rev. C40, 1972 (1989) V.Landre, P.Aguer, G.Bogaert, A.Lefebvre, J.P.Thibaud, S.Fortier, J.M.Maison, J.Vernotte 17O(3He, d)18F Reaction and Its Implication in the 17O Destruction in the CNO Cycle in Stars NUCLEAR REACTIONS 17O(3He, d), E=15 MeV; measured σ(Ed), σ(θ); deduced model parameters. 18F deduced levels, J, π, spectroscopic factors. 17O(p, α), (p, γ), E(cm) ≤ 150 keV; calculated astrophysical S-factor vs E; deduced reaction rate.
doi: 10.1103/PhysRevC.40.1972
1988DA01 Phys.Rev. C37, 250 (1988) V.M.Datar, S.Fortier, S.Gales, E.Hourani, H.Langevin, J.M.Maison, C.P.Massolo Search for Short Lived Neutral Particle in the 15.1 MeV Isovector Transition of 12C NUCLEAR REACTIONS 12C(p, p'), E=19 MeV; measured e+e--coin; deduced no neutral φ-particle evidence, Γ(φ)/Γγ upper limits.
doi: 10.1103/PhysRevC.37.250
1988DE28 Phys.Rev. C37, 2687 (1988); Erratum Phys.Rev. C41, 1319 (1990) Ph.Dessagne, Ch.Miehe, P.Baumann, A.Huck, G.Klotz, M.Ramdane, G.Walter, J.M.Maison β+-Electron-Capture Decay of 69Se RADIOACTIVITY 69Se(β+p) [from 40Ca(32S, n2p), E=100 MeV]; measured β-delayed E(p), I(p), E(γ), γγ-coin; deduced total proton branching ratios, log ft, β-strength function. 69As deduced levels, γ-branching. Natural target, Ge(Li), surface barrier Si(Au) detectors.
doi: 10.1103/PhysRevC.37.2687
1988HO03 Nucl.Instrum.Methods Phys.Res. A264, 357 (1988) E.Hourani, J.Kumpulainen, F.Azaiez, S.Fortier, S.Gales, J.M.Maison, P.Massolo, B.Ramstein, J.P.Schapira Mass Identification in Heavy Ion Collection with the Spectrometer SOLENO NUCLEAR REACTIONS 24Mg(16O, X), E=87.5 MeV; 12C(32S, X), E=121 MeV; 24Mg(32S, X), E=121 MeV; measured σ(fragment E), mass distribution. Mass spectrometer. RADIOACTIVITY 252Cf(SF); measured fission fragment distribution. Mass spectrometer.
doi: 10.1016/0168-9002(88)90924-2
1988LA18 Phys.Rev. C38, 1168 (1988) H.Langevin-Joliot, V.Datar, E.Gerlic, J.Van de Wiele, F.Azaiez, S.Fortier, S.Gales, J.Guillot, J.M.Maison, C.P.Massolo, G.Duhamel, G.Perrin Highest Spin n-p States in Heavy Nuclei via the (α, d) Reaction at 218 MeV NUCLEAR REACTIONS 90Zr, 120Sn, 144Sm, 208Pb(α, d), E=218 MeV; measured σ(θ). 92Nb, 122Sb, 146Eu, 210Bi deduced levels, J, π. DWBA analysis.
doi: 10.1103/PhysRevC.38.1168
1986MA49 Phys.Rev. C34, 1256 (1986) C.P.Massolo, F.Azaiez, S.Gales, S.Fortier, E.Gerlic, J.Guillot, E.Hourani, J.M.Maison Damping of High-Spin Single-Particle Strengths in 209Pb NUCLEAR REACTIONS 208Pb(α, 3He), E=183 MeV; measured σ(θ), σ(E(3He)); deduced model parameters. 209Pb deduced levels, J, π, L, strength functions. Enriched target, magnetic spectrometer. DWBA analysis.
doi: 10.1103/PhysRevC.34.1256
1985AZ03 Nucl.Phys. A444, 373 (1985) F.Azaiez, S.Fortier, S.Gales, E.Hourani, J.M.Maison, J.Kumpulainen, J.P.Schapira The γ-Decay of the 1g9/2 and 2p Inner-Hole States in 111Sn via the 112Sn(3He, αγ) Reaction at 32 MeV NUCLEAR REACTIONS 112Sn(3He, αγ), E=32 MeV; measured σ(Eα, Eγ). 111Sn levels deduced possible J, π, γ-decay of inner hole states, 1g9/2, 2p strength functions. Magnetic spectrometer, Ge(Li) detector, enriched target.
doi: 10.1016/0375-9474(85)90458-0
1985VE05 Phys.Rev. C31, 2071 (1985) M.Vergnes, S.Grafeuille, G.Rotbard, G.Berrier-Ronsin, J.Vernotte, J.M.Maison, S.Fortier, R.Tamisier, P.Van Isacker, J.Jolie Transfer in the Light Hg Isotopes and the U(6/12) Models NUCLEAR REACTIONS 200,198,196Hg(p, d), E=25 MeV; measured σ(Ed), σ(θ). 199,197,195Hg levels deduced S, symmetry characteristics.
doi: 10.1103/PhysRevC.31.2071
1984GA24 Phys.Lett. 144B, 323 (1984) S.Gales, C.P.Massolo, F.Azaiez, S.Fortier, E.Gerlic, J.Guillot, E.Hourani, J.M.Maison, J.P.Schapira, G.M.Crawley High-Lying Neutron Particle States Observed via the (α, 3He) Reaction at 183 MeV NUCLEAR REACTIONS 116,118,120Sn(α, 3He), E=183 MeV; measured σ(θ, E(3He)), σ(θ). 117,119Sn deduced high lying neutron states. 121Sn deduced high lying neutron states, possible J, π, C2S. DWBA analysis.
doi: 10.1016/0370-2693(84)91270-X
1984VE06 Phys.Rev. C30, 517 (1984) M.Vergnes, G.Berrier-Ronsin, G.Rotbard, J.Vernotte, J.M.Maison, R.Bijker Breaking of the Multi-j Supersymmetry Schemes in the 195Pt(d, p)196Pt Reaction NUCLEAR REACTIONS 195Pt(d, p), E=25.2 MeV; measured σ(θ), σ(Ep); deduced supersymmetry breaking evidence. 196Pt levels deduced spectroscopic strengths. DWBA analysis.
doi: 10.1103/PhysRevC.30.517
1982BE21 Phys.Rev. C25, 2848 (1982) G.Berrier-Ronsin, M.Vergnes, G.Rotbard, J.Vernotte, S.Fortier, J.M.Maison, R.Tamisier Mass of 197Hg NUCLEAR REACTIONS 199Hg(p, t), E=25 MeV; measured σ(Et), Q. 197Hg deduced mass excess.
doi: 10.1103/PhysRevC.25.2848
1982DE03 Phys.Rev. C25, 146 (1982) P.De Gelder, D.De Frenne, E.Jacobs, K.Heyde, S.Fortier, J.M.Maison, M.N.Rao, C.P.Massolo Excited States of 102Tc: A study of the proton-neutron interaction NUCLEAR REACTIONS 100Mo(3He, p), E=25 MeV; measured σ(Ep, θ); 104Ru(d, α), E=20 MeV; measured Eα. 102Tc deduced levels, L, J, π. Split-pole spectrograph, enriched target. DWBA analysis, shell model.
doi: 10.1103/PhysRevC.25.146
1982GA12 Phys.Rev.Lett. 48, 1593 (1982) G.Gales, C.P.Massolo, S.Fortier, E.Gerlic, J.Guillot, E.Hourani, J.M.Maison, J.P.Schapira, B.Zwieglinski, P.Martin, V.Comparat High-Lying Proton Strengths Observed in Stripping Reactions NUCLEAR REACTIONS 144Sm(α, t), E=80 MeV; 144Sm(3He, d), E=240 MeV; measured σ(θ), σ(Et), σ(Ed). 145Eu deduced broad structures, Γ, L, J, π, C2S, h9/2, i13/2 proton strength distribution. Zero-range DWBA analysis.
doi: 10.1103/PhysRevLett.48.1593
1982HO17 Nucl.Phys. A391, 432 (1982) E.Hourani, S.Fortier, J.M.Maison, S.Gales, J.P.Schapira Direct Transfer and Two-Step Processes in the 42Ca(α, 3He)43Ca Reaction NUCLEAR REACTIONS 42Ca(α, 3He), E=36 MeV; measured σ(E, θ). 43Ca deduced levels, L, S. DWBA, coupled-channel analyses. Enriched target.
doi: 10.1016/0375-9474(82)90618-2
1982MA07 J.Phys.(London) G8, 361 (1982) C.P.Massolo, S.Fortier, J.M.Maison, M.N.Rao The Fragmentation of the f-p Neutron-Hole Strength in 91Mo below 6 MeV Excitation Energy NUCLEAR REACTIONS 92Mo(3He, α), E=25 MeV; measured σ(Eα, θ). 91Mo deduced levels, L, C2S, configuration. Enriched target, magnetic spectrometer. DWBA analysis.
doi: 10.1088/0305-4616/8/3/007
1981FO09 Nucl.Phys. A370, 189 (1981) S.Fortier, J.M.Maison, P.Picot, S.Gales, E.Hourani, J.P.Schapira Two-Step Processes in the 40Ca(α, 3He)41Ca Reaction NUCLEAR REACTIONS 40Ca(α, 3He), E=36 MeV; measured σ(E(3He), θ). 41Ca deduced levels, L, S. DWBA, coupled-channels analyses. Enriched target.
doi: 10.1016/0375-9474(81)90072-5
1980FO11 Nucl.Phys. A346, 285 (1980) S.Fortier, E.Hourani, J.M.Maison Single-Particle and Core-Excited States in 49Sc (I). The 48Ca(3He, d)49Sc reaction NUCLEAR REACTIONS 48Ca(3He, d), E=25 MeV; measured σ(Ed, θ). 49Sc deduced levels, L, S, analog states. Enriched target. DWBA analysis.
doi: 10.1016/0375-9474(80)90470-4
1980FO12 Nucl.Phys. A346, 303 (1980) S.Fortier, I.Fodor-Lovas, E.Hourani, J.M.Maison, J.P.Schapira Single-Particle and Core-Excited States in 49Sc (II). The 48Ca(α, t)49Sc reaction NUCLEAR REACTIONS 48Ca(α, t), E=36 MeV; measured σ(Eα, θ). 49Sc deduced levels, L, S. Enriched targets. DWBA, coupled-channels analyses.
doi: 10.1016/0375-9474(80)90471-6
1980GA01 Phys.Rev. C21, 98 (1980) S.Gales, Y.El Hage, J.P.Schapira, S.Fortier, H.Laurent, J.M.Maison High-Spin Analog Resonances Near the N = 50 Neutron Shell NUCLEAR REACTIONS 92Mo(3He, d), E=28.5 MeV; 96Zr(3He, d), E=39 MeV; measured σ(Ed, θ). 92Mo(3He, pd), E=30 MeV; 96Zr(3He, pd), E=37.5 MeV; measured σ(Ed, Ep, θp). 93Tc, 97Nb deduced IAS, L, J, π, S, Γp, Γp'. DWBA, Gamow function form factors. Magnetic analysis, enriched targets.
doi: 10.1103/PhysRevC.21.98
1979CH32 Nucl.Phys. A331, 407 (1979) J.F.Chemin, S.Andriamonje, J.Roturier, B.Saboya, J.P.Thibaud, S.Joly, S.Plattard, J.Uzureau, H.Laurent, J.M.Maison, J.P.Schapira Measurement of Compound-Nucleus Lifetime by X-Ray Spectroscopy in the 106Cd(p, p')106Cd Reaction NUCLEAR REACTIONS 106Cd(p, p'), E=10, 12 MeV; measured Ep', E(X), P(X-ray)-coin, ionization probability; deduced reaction times, < Γ > . Enriched, natural targets.
doi: 10.1016/0375-9474(79)90351-8
1979RA16 Phys.Rev. C20, 139 (1979) M.N.Rao, C.P.Massolo, S.Fortier, J.M.Maison Nuclear Structure of 94Tc NUCLEAR REACTIONS 92Mo(3He, p), E=25 MeV; measured σ(Ep, θ). 94Tc deduced levels, J, π, transfer L. DWBA, coupled channels calculation. Enriched target, split-pole spectrograph.
doi: 10.1103/PhysRevC.20.139
1978GA06 Phys.Rev. C17, 1308 (1978) S.Gales, Y.El Hage, S.Fortier, H.Laurent, J.M.Maison, J.P.Schapira Proton Decay of T > Hole States in Heavy Nuclei by Means of the (3He, αp) Reaction on 96Zr and 144Sm NUCLEAR REACTIONS 96Zr, 144Sm(3He, pα), E=39 MeV; measured σ(Ep, Eα, θ(p)). 95Zr, 143Sm deduced IAS, proton branching. 94Y deduced levels, J, π, Γp, S. Enriched targets.
doi: 10.1103/PhysRevC.17.1308
1978SC07 Phys.Rev. C17, 1588 (1978) J.P.Schapira, J.M.Maison, M.N.Rao, S.Fortier, S.Gales, H.Laurent γ Decay and Splitting of the First Analog State in 53Mn, 55Co, and 59Cu NUCLEAR REACTIONS 52Cr, 54Fe, 58Ni(3He, dγ), E=18 MeV; measured σ(Ed, Eγ). 53Mn, 55Co, 59Cu deduced levels, γ-branching, δ. Natural, enriched targets, Ge(Li) detectors.
doi: 10.1103/PhysRevC.17.1588
1977FO06 Nucl.Phys. A288, 82 (1977) S.Fortier, J.M.Maison, S.Gales, H.Laurent, J.P.Schapira Spectroscopic Study of 55Co via the 54Fe(τ, d)55Co and 54Fe(τ, dp)54Fe Reactions NUCLEAR REACTIONS 54Fe(3He, d), E=25 MeV; measured σ(Ed, θ). 54Fe(3He, dp), E=24 MeV; measured σ(Ed), dp(θ, t). 55Co deduced levels, J, π, L, S, IAS, population parameters, Γp, Γp'. 55Fe, 55Co deduced Coulomb energy difference. Enriched target.
doi: 10.1016/0375-9474(77)90082-3
1977GA17 Nucl.Phys. A288, 201 (1977) S.Gales, E.Hourani, S.Fortier, H.Laurent, J.M.Maison, J.P.Schapira Neutron-Hole Strengths and Isobaric Analog States in 95Zr NUCLEAR REACTIONS 91,92,94,96Zr(3He, α), E=39 MeV; measured σ(Eα, θ). 90,91,93,95Zr deduced levels, L, J, π, S. 95Y-95Zr analog pairs deduced Coulomb displacement energies, Γ, L, J, π, S. Enriched target, magnetic spectrometer.
doi: 10.1016/0375-9474(77)90130-0
1977GA18 Nucl.Phys. A288, 221 (1977) S.Gales, E.Hourani, S.Fortier, H.Laurent, J.M.Maison, J.P.Schapira Deeply Bound Hole States and Isobaric Analog States in 89Zr NUCLEAR REACTIONS 90Zr(3He, α), E=39 MeV; measured σ(Eα, θ). 89Zr deduced levels, L, J, π, S. Enriched target, magnetic spectrometer.
doi: 10.1016/0375-9474(77)90131-2
1977LA07 Nucl.Phys. A284, 501 (1977) H.Laurent, C.P.Massolo, J.P.Schapira, S.Fortier, S.Gales, J.M.Maison A Time-Integrated Perturbed Angular Correlation Measurement on the First 2+ of 24Mg, Using Charge State Separation NUCLEAR REACTIONS 24Mg(32S, 32S), E=67 MeV; measured γ(θ) on recoil into vacuum in the 12+, 11+, 10+, 9+ charge states. 24Mg deduced ionic electron configurations. Natural target.
doi: 10.1016/0375-9474(77)90399-2
1976GA04 Nucl.Phys. A259, 189 (1976) S.Gales, S.Fortier, H.Laurent, J.M.Maison, J.P.Schapira Spectroscopic Studies of Unbound Isobaric Analog States in 49V and 51V Via the 48,50Ti(τ, d) and the 48,50Ti(τ, dp) Reactions NUCLEAR REACTIONS 48,50Ti(3He, d), E=25.0 MeV; measured σ(Ed, θ). 48,50Ti(3He, pd), E=25.5 MeV; measured σ(Ed, Ep, θ). 49,51V deduced IAS, L, J, π, S, Γp, proton branching. 49,51V, 49,51Ti analog pairs deduced Coulomb displacement energies. DWBA analysis using Gamov functions as form factors. Enriched, natural targets.
doi: 10.1016/0375-9474(76)90062-2
1976GA15 Nucl.Phys. A265, 213 (1976) S.Gales, S.Fortier, H.Laurent, J.M.Maison, J.P.Schapira Population and Proton Decay of the g9/2 Isobaric Analog State in 53Mn via the 52Cr(τ, dp)52Cr Reaction NUCLEAR REACTIONS 52Cr(3He, pd), E=24 MeV; measured σ(Ed, Ep, θ(p)). 53Mn deduced IAS, J, Γp, S.
doi: 10.1016/0375-9474(76)90350-X
1976GA19 Nucl.Phys. A268, 257 (1976); Erratum Nucl.Phys. A280, 499 (1977) S.Gales, S.Fortier, H.Laurent, J.M.Maison, J.P.Schapira Proton States in 59Cu and Structure of the 59Cu-59Ni Analog Pair NUCLEAR REACTIONS 58Ni(3He, d), E=25 MeV; measured σ(E, θ). 58Ni(3He, pd), E=24 MeV; measured σ(Ed, Ep, θ(p)). 59Cu deduced levels, L, J, π, S, isobaric analog states, population parameters, Γp, Γp'. 59Ni-59Cu isotopes deduced Coulomb energy differences. Enriched target.
doi: 10.1016/0375-9474(76)90462-0
1976GA20 Phys.Rev. C14, 842 (1976) S.Gales, S.Fortier, H.Laurent, J.M.Maison, J.P.Schapira Unbound Isobaric Analog States in 53Mn: The Reactions 52Cr(3He, d)53Mn and 52Cr(3He, dp)52Cr NUCLEAR REACTIONS 52Cr(3He, d), E=25 MeV; measured σ(Ed, θ). 52Cr(3He, pd), E=24 MeV; measured σ(Ed, Ep, θ(p)). 53Mn deduced IAS, L, J, π, S, Γp, proton branching. 53Cr, 53Mn analog pairs deduced Coulomb displacement energies. DWBA analysis using Gamov functions as form factors. Natural targets.
doi: 10.1103/PhysRevC.14.842
1976HU01 Phys.Rev. C13, 1786 (1976) A.Huck, G.J.Costa, G.Walter, M.M.Aleonard, J.Dalmas, P.Hubert, F.Leccia, P.Mennrath, J.Vernotte, M.Langevin, J.M.Maison Lowest T = 2 State of 36Ar via the 35Cl(p, γ)36Ar Reaction NUCLEAR REACTIONS 35Cl(p, γ), E=2.36-2.42 MeV; measured σ(E, Eγ). 36Ar deduced resonances, J, π, T, δ, B(M1).
doi: 10.1103/PhysRevC.13.1786
1976VE01 Phys.Rev. C13, 461 (1976) J.Vernotte, S.Fortier, M.Langevin, J.M.Maison, M.Vergnes, B.H.Wildenthal 37Cl(3He, αγ)36Cl Reaction: γ Decay of the Two Lowest Lying T = 2 States NUCLEAR REACTIONS 40Ca, 37Cl(3He, αγ), E=18 MeV; measured σ(Eγ), αγ-coin. 36Cl deduced levels, J, π, B(λ), γ-branching. 39Ca deduced levels.
doi: 10.1103/PhysRevC.13.461
1976VE03 Phys.Rev. C13, 984 (1976) J.Vernotte, J.M.Maison, A.Chevallier, A.Huck, C.Miehe, G.Walter Electromagnetic Properties of the 6621- and 7950-keV Levels in 32S NUCLEAR REACTIONS 31P(p, γ), E=1.25-1.58 MeV; measured Iγ(θ), DSA. 32S deduced resonances, J, π, T1/2, δ, γ-branching, transition strengths.
doi: 10.1103/PhysRevC.13.984
1975FO15 Nucl.Phys. A254, 189 (1975) S.Fortier, S.Gales, H.Laurent, J.M.Maison, J.P.Schapira Gamma Decay of Analog States in 41Ca NUCLEAR REACTIONS 42Ca(3He, αγ), E=18 MeV; measured σ(Eα, Eγ, theta(γ)), Doppler shift. 41Ca levels deduced J, δ, γ-branching, T1/2. Enriched target.
doi: 10.1016/0375-9474(75)90591-6
1975GA10 Phys.Lett. 56B, 449 (1975) S.Gales, S.Fortier, H.Laurent, J.M.Maison, J.P.Schapira Angular Correlation Studies of Isobaric Analog States in 49Sc via the 48Ca(τ, dp)48Sc Reaction NUCLEAR REACTIONS 48Ca(3He, pd), E=25.5 MeV; measured dp-coin. 49Sc deduced IAS, L, J, π, S, p-width.
doi: 10.1016/0370-2693(75)90409-8
1974LA14 Nucl.Instrum.Methods 117, 17 (1974) H.Laurent, J.P.Schapira, S.Fortier, S.Gales, J.M.Maison Un Systeme de Detection a 0° du Faisceau, Utilisant un Triplet de Lentilles Quadrupolaires Magnetiques NUCLEAR REACTIONS 42Ca(3He, α), (3He, d), E=15, 18 MeV; measured Eα, Iα, Ed, Id. 41Ca deduced levels, analog resonance.
doi: 10.1016/0029-554X(74)90378-4
1973VE06 Phys.Rev. C8, 178 (1973) J.Vernotte, S.Gales, M.Langevin, J.M.Maison Investigation of the Lowest T = 2 State of 32S in the 31P + p Reactions NUCLEAR REACTIONS 31P(p, γ), (p, p'γ), (p, αγ), E=3.27-3.3 MeV; measured σ(Eγ), σ(E). 32S deduced resonances, T, J, π, γ-branching.
doi: 10.1103/PhysRevC.8.178
1973VE08 Nucl.Phys. A212, 493 (1973) J.Vernotte, S.Gales, M.Langevin, J.M.Maison Recherche de Resonances Isobariques Analogues dans 32S au Moyen des Reactions 31P(p, γ)32S, 31P(p, p)31P et 31P(p, α0)28Si NUCLEAR REACTIONS 31P(p, γ), E=1.24-1.60 MeV; measured Q, σ(Ep;Eγ, θ(γ)); 31P(p, α0), E=1.24-1.60 MeV; measured σ(E); 31P(p, p), E=1.24-1.60 MeV; measured σ(E). 32S deduced resonances, resonance strengths, γ-ray branching ratios, mixing ratios, transition strengths, L, J, π, T, p-width, α-width, level-width, quadrupole moment. Ge(Li) detector.
doi: 10.1016/0375-9474(73)90820-8
1972FO12 Phys.Rev. C6, 378 (1972) S.Fortier, H.Laurent, J.M.Maison, J.P.Schapira, J.Vernotte, W.Weisz First T = 2 Level in 32P NUCLEAR REACTIONS 30Si(3He, pγ), E=8.02 MeV; measured σ(Ep, Eγ, θ(p)), pγ-coin. 32P deduced levels, J, π, γ-branching.
doi: 10.1103/PhysRevC.6.378
1970AR08 Nucl.Phys. A147, 305 (1970) Study of the Giant Resonance by Photon Scattering in Medium Spherical Nuclei NUCLEAR REACTIONS Ti, 51V, Cr, 75As, Se, 89Y, Cd, In, Sn(γ, γ'), Eγ = 12-30 MeV; measured σ(E, θ); deduced σ(γγ'). Ti, 51V, Cr, 75As, Se, 89Y, Cd, In, Sn deduced giant dipole resonance width, isobaric spin splitting. Natural targets, NaI(Tl) crystal.
doi: 10.1016/0375-9474(70)90270-8
1970GA26 C.R.Acad.Sci., Ser.B, 271, 970 (1970) S.Gales, M.Langevin, J.-M.Maison, J.Vernotte Recherche du Premier Etat T = 2 du Noyau Soufre-32 au Moyen de la Reaction 31P(p, γ)32S NUCLEAR REACTIONS 31P(p, γ), E=3.10-3.35 MeV; measured σ(E;Eγ, θ(γ)). 32S deduced resonances, levels, J, π, T, γ-branching.
1965MA45 Phys.Letters 19, 308 (1965) J.M.Maison, M.Langevin, J.M.Loiseaux Observation de la Decroissance des Etats de la Resonance Geante Dipolaire de 16O Vers les Niveaux Excites de Parite Negative et Positive de 15O et 16N NUCLEAR STRUCTURE 15O, 16O, 15N; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(65)91000-0
Back to query form |