NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = M.M.Aleonard Found 41 matches. 2012PL01 Eur.Phys.J. A 48, 68 (2012) C.Plaisir, F.Hannachi, F.Gobet, M.Tarisien, M.M.Aleonard, V.Meot, G.Gosselin, P.Morel, B.Morillon Measurement of the 85Rb(γ, n)84mRb cross-section in the energy range 10-19 MeV with bremsstrahlung photons NUCLEAR REACTIONS 85Rb(γ, n)84mRb, E=10-19 MeV; measured activation Eγ, Iγ from bremsstrahlung γ; deduced yields, σ, GDR parameters using GEANT4 and relative to 197Au(γ, n) and 63Cu(γ, n). Compared with other data.
doi: 10.1140/epja/i2012-12068-7
2004CL05 Phys.Rev. C 70, 044303 (2004) G.Claverie, M.M.Aleonard, J.F.Chemin, F.Gobet, F.Hannachi, M.R.Harston, G.Malka, J.N.Scheurer, P.Morel, V.Meot Search for nuclear excitation by electronic transition in 235U NUCLEAR REACTIONS 235U(γ, γ'), E=low; measured isomer excitation rate upper limit. Nuclear excitation by electronic transition, laser-induced plasma.
doi: 10.1103/PhysRevC.70.044303
2003AI07 Nucl.Instrum.Methods Phys.Res. A508, 367 (2003) M.Aiche, M.M.Aleonard, G.Barreau, D.Boivin, F.Bourgine, D.Cabaussel, J.F.Chemin, M.Harston, J.N.Scheurer, G.La Rana, R.Moro, A.Brondi, E.Vardaci, D.Curien, F.Hannachi Correction method for Doppler broadened γ-ray lines using the linear momentum of the evaporated charged particles in heavy-ion induced fusion-evaporation reactions NUCLEAR REACTIONS 58Ni(32S, 3p), (32S, 4p), (32S, pα), (32S, 2pα), (32S, 3pα), (32S, 2α), E=120 MeV; measured Eγ, Iγ, (particle)γ-coin. Eurogam II, Diamant arrays, Doppler correction method.
doi: 10.1016/S0168-9002(03)01475-X
2001NI13 Phys.Rev. C64, 034313 (2001) N.Nica, G.Duchene, V.E.Iacob, J.Dudek, F.A.Beck, Th.Byrski, D.Curien, G.de France, B.Haas, B.Kharraja, D.Prevost, C.Petrache, H.Savajols, J.P.Vivien, L.Han, K.Zuber, M.Aiche, M.M.Aleonard, J.F.Chemin, C.W.Beausang, S.Clarke, P.J.Dagnall, M.Smith, P.J.Twin, J.Simpson, M.A.Bentley High-Spin States in 155Er NUCLEAR REACTIONS 123Sb(37Cl, 5n), E=193 MeV; measured Eγ, Iγ, γγ-coin, γ-ray polarization. 155Er deduced high-spin levels, J, π, δ, configurations, deformation. Eurogam II array. Tilted-Fermi-surface analysis.
doi: 10.1103/PhysRevC.64.034313
2001VI13 Phys.Lett. 521B, 165 (2001) G.Viesti, V.Rizzi, D.Fabris, M.Lunardon, G.Nebbia, M.Cinausero, E.Fioretto, G.Prete, A.Brondi, G.La Rana, R.Moro, E.Vardaci, M.Aiche, M.M.Aleonard, G.Barreau, D.Boivin, J.N.Scheurer, J.F.Chemin, K.Hagel, J.B.Natowitz, R.Wada, S.Courtin, F.Haas, N.Rowley, B.M.Nyako, J.Gal, J.Molnar Exploring the Emission Barriers in Hot Nuclei NUCLEAR REACTIONS 170Er(30Si, 5nα), E=165 MeV; 170Er(29Si, 4nα), E=147 MeV; measured Eγ, Iγ, Eα, (charged particle)γ-coin. 200Pb deduced α-emission barrier distribution. Euroball IV, Diamant arrays, comparisons with model predictions.
doi: 10.1016/S0370-2693(01)01221-7
2000SC43 Acta Phys.Hung.N.S. 12, 195 (2000) J.N.Scheurer, M.Aiche, M.M.Aleonard, G.Barreau, D.Boivin, F.Bourgine, J.F.Chemin, T.P.Doan, A.Brondi, G.La Rana, R.Moro, A.Principe, E.Vardaci, D.Curien, G.Duchene, G.de France, F.A.Beck, B.Haas, J.P.Vivien, F.Hannachi Feeding of ND and SD Bands in 151, 152Dy Nuclei NUCLEAR REACTIONS 123Sb(37Cl, αX)150Dy/151Dy/152Dy/153Dy, E=191 MeV; measured Eα, αγ-, γγ-coin; deduced entry regions for normal-deformed, superdeformed bands. Euroball II, Diamant arrays.
1999AI04 Eur.Phys.J. A 6, 121 (1999) M.Aiche, M.M.Aleonard, G.Barreau, D.Boivin, F.Bourgine, J.F.Chemin, J.N.Scheurer, T.P.Doan, A.Brondi, G.La Rana, R.Moro, A.Principe, E.Vardaci, D.Curien, G.Duchene, G.de France, F.A.Beck, B.Haas, J.P.Vivien, F.Hannachi Alpha Energy Distribution as a Probe for the Feeding of ND and SD Bands in 151, 152Dy Nuclei NUCLEAR REACTIONS 123Sb(37Cl, 4nα), (37Cl, 5nα), E=191 MeV; measured Eγ, Iγ, Eα, γγ-, αγ-coin. 151,152Dy deduced superdeformed, normal-deformed bands associated α spectra, band-feeding features, transitions from possible hyperdeformed band. Eurogam II, Diamant arrays.
doi: 10.1007/s100500050326
1999HO25 Eur.Phys.J. A 6, 43 (1999) M.Houry, R.Lucas, M.-G.Porquet, Ch.Theisen, M.Girod, M.Aiche, M.M.Aleonard, A.Astier, G.Barreau, F.Becker, J.F.Chemin, I.Deloncle, T.P.Doan, J.L.Durell, K.Hauschild, W.Korten, Y.Le Coz, M.J.Leddy, S.Perries, N.Redon, A.A.Roach, J.N.Scheurer, A.G.Smith, B.J.Varley Structure of Neutron Rich Palladium Isotopes Produced in Heavy Ion Induced Fission NUCLEAR REACTIONS 238U(12C, F), E=90 MeV; measured Eγ, Iγ, γγ-coin. 109,110,111,112,113,114,115,116,118Pd deduced high-spin levels, J, π, rotational bands, configurations, deformation, no shape transition. Euroball III array.
doi: 10.1007/s100500050315
1997AI03 Z.Phys. A358, 175 (1997) M.Aiche, M.M.Aleonard, G.Barreau, F.Bourgine, A.Brondi, D.Cabaussel-Sellam, D.Curien, J.F.Chemin, J.P.Goudour, M.Harston, G.La Rana, R.Moro, J.N.Scheurer, E.Vardaci First Results with DIAMANT and EUROGAM NUCLEAR REACTIONS 58Ni(32S, X), (32S, 2α), E=120 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-coin; deduced charged particle selectivity, Doppler correction features. 82Zr deduced transitions.
doi: 10.1007/s002180050297
1997AZ05 Acta Phys.Hung.N.S. 6, 289 (1997) F.Azaiez, S.Bouneau, J.Duprat, I.Deloncle, M.-G.Porquet, U.J.van Severen, T.Nakatsukasa, M.M.Aleonard, A.Astier, G.Baldsiefen, C.W.Beausang, F.A.Beck, C.Bourgeois, D.Curien, N.Dozie, L.Ducroux, B.Gall, H.Hubel, M.Kaci, W.Korten, M.Meyer, N.Redon, H.Sergolle, J.F.Sharpey-Schafer Octupole Vibrations of the Superdeformed 196Pb Nucleus NUCLEAR REACTIONS 186W(16O, 6n), E=110 MeV; measured Eγ, Iγ, γγ-coin. 196Pb deduced superdeformed bands, possible octupole vibrations.
1997BO28 Z.Phys. A358, 179 (1997) S.Bouneau, F.Azaiez, J.Duprat, I.Deloncle, M.-G.Porquet, U.J.van Severen, T.Nakatsukasa, M.-M.Aleonard, A.Astier, G.Baldsiefen, C.W.Beausang, F.A.Beck, C.Bourgeois, D.Curien, N.Dozie, L.Ducroux, B.J.P.Gall, H.Hubel, M.Kaci, W.Korten, M.Meyer, N.Redon, H.Sergolle, J.F.Sharpey-Schafer New Results on the Superdeformed 196Pb Nucleus: Decay of the excited bands to the yrast band NUCLEAR REACTIONS 186W(16O, 6n), E=110 MeV; measured Eγ, Iγ, γγγ-coin. 196Pb deduced superdeformed bands, dynamical moments of inertia. RPA model comparisons.
doi: 10.1007/s002180050299
1997BO37 Phys.Rev. C56, 3180 (1997) F.Bourgine, D.Cabaussel, D.Boivin, M.Aiche, M.-M.Aleonard, G.Barreau, J.-F.Chemin, T.P.Doan, J.P.Goudour, M.Harston, J.-N.Scheurer, A.Brondi, G.La Rana, R.Moro, A.Principe, E.Vardaci, D.Curien Energy Sharing in the Deexcitation of the 90Ru Compound Nucleus Via the pα Channel NUCLEAR REACTIONS 58Ni(32S, pα), E=120 MeV; measured Eγ, Iγ, (particle)γ-coin, p-, α-spectra, p-α angular correlations; deduced p, α energy sharing vs compound nucleus excitation energy. Statistical model calculations.
doi: 10.1103/PhysRevC.56.3180
1997KA34 Phys.Rev. C56, R600 (1997) M.Kaci, E.Gueorguieva, M.G.Porquet, F.Azaiez, I.Deloncle, S.Bouneau, J.Duprat, M.M.Aleonard, A.Astier, G.Baldsiefen, C.W.Beausang, F.A.Beck, Ch.Bourgeois, D.Curien, N.Dozie, L.Ducroux, B.J.P.Gall, W.Korten, M.Meyer, N.Redon, D.Prevost, H.Sergolle, J.Sharpey-Schafer, U.J.van Severen First Indication of Population of Superdeformed States by Incomplete Fusion Reactions NUCLEAR REACTIONS, ICPND 186W(16O, X)195Pb/196Pb/197Pb/196Tl/197Tl/193Hg/194Hg/190Pt/186Os/188Os, E=110 MeV; measured residual production yield, Eγ, Iγ, γγ-coin; deduced recoil v/c, evidence for incomplete fusion process. 194Hg deduced superdeformed band. EUROGAM II.
doi: 10.1103/PhysRevC.56.R600
1997SC43 Nucl.Instrum.Methods Phys.Res. A385, 501 (1997) J.N.Scheurer, M.Aiche, M.M.Aleonard, G.Barreau, F.Bourgine, D.Boivin, D.Cabaussel, J.F.Chemin, T.P.Doan, J.P.Goudour, M.Harston, A.Brondi, G.La Rana, R.Moro, E.Vardaci, D.Curien Improvements in the In-Beam γ-Ray Spectroscopy Provided by an Ancillary Detector Coupled to a Ge γ-Spectrometer: The DIAMANT-EUROGAM II example NUCLEAR REACTIONS, ICPND 58Ni(32S, xnypzα), E=120 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-coin; deduced residuals relative yields.
doi: 10.1016/S0168-9002(96)01038-8
1993HA20 Nucl.Phys. A557, 75c (1993) F.Hannachi, C.Schuck, G.Bastin, I.Deloncle, B.Gall, M.G.Porquet, A.G.Smith, F.Azaiez, C.Bourgeois, J.Duprat, A.Korichi, N.Perrin, N.Poffe, H.Sergolle, A.Astier, Y.Le Coz, M.Meyer, N.Redon, M.Bentley, J.Simpson, J.F.Sharpey-Schafer, M.J.Joyce, C.W.Beausang, P.Fallon, E.S.Paul, P.J.Dagnall, S.A.Forbes, S.Gale, P.M.Jones, R.Wadsworth, R.M.Clark, M.M.Aleonard, D.Curien, G.De France, M.Carpenter, R.Henry, T.Lauritsen, P.Willsau Study of the Superdeformed Band in 194Pb and 192Hg with EUROGAM NUCLEAR REACTIONS 162Dy(36S, 4n), E=162 MeV; measured Eγ, Iγ, γγ-coin, DSA. 160Gd(36S, 4n), E=159 MeV; measured γγ-coin. 194Pb deduced decay out of superdeformed band.
doi: 10.1016/0375-9474(93)90532-3
1990AZ04 Phys.Rev.Lett. 65, 305 (1990) F.Azaiez, M.M.Aleonard, S.Andriamonje, J.F.Chemin, J.N.Scheurer, D.W.Spooner, J.P.Thibaud, J.F.Bruandet, E.Liatard, F.Beck, G.Costa Observation of Characteristic X Rays Emitted During Sequential Proton Evaporation by the 112Xe Compound Nucleus NUCLEAR REACTIONS 54Fe(58Ni, X), E=4.1 MeV/nucleon; measured Doppler shifted (X-ray)(evaporation residue)-coin; deduced mean proton width. Evaporation of 3p from compound nucleus.
doi: 10.1103/PhysRevLett.65.305
1990BU15 Nucl.Phys. A513, 291 (1990) J.Busto, D.Dassie, O.Helene, Ph.Hubert, P.Larrieu, F.Leccia, P.Mennrath, M.M.Aleonard, J.Chevallier The 0+ → 2+ Neutrinoless Double Beta Decay of 76Ge: Results of the Frejus experiment RADIOACTIVITY 76Ge(2β); measured βγ-coin; deduced neutrinoless decay T1/2. Ge, NaI detectors.
doi: 10.1016/0375-9474(90)90100-Z
1989AZ01 Nucl.Instrum.Methods Phys.Res. A281, 133 (1989) F.Azaiez, M.M.Aleonard, S.Andriamonje, J.F.Chemin, G.Claverie, J.N.Scheurer, F.Beck, G.Costa A 4π Light Charged Particle Multidetector for Reaction Channel Identification and Discrimination NUCLEAR REACTIONS 54Fe(58Ni, X), E=238 MeV; measured fusion-evaporation particle spectra. 4π light charged particle detector.
doi: 10.1016/0168-9002(89)91224-2
1989AZ02 Nucl.Phys. A501, 401 (1989) F.Azaiez, S.Andriamonje, J.F.Chemin, M.Fidah, J.N.Scheurer, M.M.Aleonard, G.Bastin, J.P.Thibaud, G.Costa, F.Beck, J.F.Bruandet, E.Liatard High-Spin States in Neutron Deficient 106Sn and 108Sn Isotopes NUCLEAR REACTIONS 54Fe(58Ni, 4p), (58Ni, 2pα), E=268 MeV; measured Eγ, Iγ, γγ-coin, linear polarization. 108Sn, 106Sn deduced levels J, π. Enriched target, Ge(Li) detectors.
doi: 10.1016/0375-9474(89)90299-6
1989BU18 Nuovo Cim. 102A, 937 (1989) J.Busto, D.Dassie, Ph.Hubert, P.Larrieu, F.Leccia, P.Mennrath, M.M.Aleonard, J.Chevallier Comments on ' Results of a Search on the Neutrinoless Double Beta Decay of the 76Ge to the Excited States of 76Se '
1980AL23 Nucl.Phys. A350, 190 (1980) M.M.Aleonard, Y.El Masri, I.Y.Lee, F.S.Stephens, M.A.Deleplanque, R.M.Diamond Experimental Study of 136Nd at High Angular Momentum NUCLEAR REACTIONS 100Mo(40Ar, xnγ), E=170 MeV; measured γ-multiplicities vs Eγ. 136Nd deduced effective moment of inertia. Enriched targets.
doi: 10.1016/0375-9474(80)90396-6
1979WA12 Nucl.Phys. A332, 433 (1979) D.Ward, H.R.Andrews, O.Hausser, Y.El Masri, M.M.Aleonard, I.Yang-Lee, R.M.Diamond, F.S.Stephens, P.A.Butler Measurements of Lifetimes and Feeding Times for High Spin States in 156Dy NUCLEAR REACTIONS 24Mg(136Xe, 4n), E=595 MeV; measured recoil distance decay curves, γγ-coin. 156Dy levels deduced Q0, B(E2) values, feeding times. NaI(Tl) multiplicity array, Ge(Li) detectors.
doi: 10.1016/0375-9474(79)90012-5
1978AL02 Phys.Rev.Lett. 40, 622 (1978) M.M.Aleonard, G.J.Wozniak, P.Glassel, M.A.Deleplanque, R.M.Diamond, L.G.Moretto, R.P.Schmitt, F.S.Stephens Evidence for Angular Momentum Fractionation in 86Kr-Induced Reactions On 107,109Ag, 165Ho, and 197Au NUCLEAR REACTIONS 107,109Ag, 165Ho, 197Au(86Kr, X), E=618 MeV; measured γ-multiplicities as function of fragment (Z).
doi: 10.1103/PhysRevLett.40.622
1978DE04 Phys.Rev.Lett. 40, 629 (1978) M.A.Deleplanque, I.Y.Lee, F.S.Stephens, R.M.Diamond, M.M.Aleonard Nuclear Shapes at High Angular Momentum NUCLEAR REACTIONS 124Sn, 82Se(40Ar, X), 100Mo(48Ca, X), E=158, 170, 185 MeV; measured γ-multiplicity.
doi: 10.1103/PhysRevLett.40.629
1977BU14 Phys.Lett. 68B, 122 (1977) P.A.Butler, I.Y.Lee, J.O.Newton, Y.El-Masri, M.M.Aleonard, P.Colombani, R.M.Diamond, F.S.Stephens, R.W.Lougheed, E.K.Hulet Fission of 232Th, 238U, 244Pu, 248Cm Induced by Xe and Kr Ions at Coulomb Barrier Energies NUCLEAR REACTIONS 232Th, 238U, 244Pu, 248Cm(86Kr, F), (136Xe, F), E ≈ Coulomb barrier; measured σ(θ).
doi: 10.1016/0370-2693(77)90181-2
1977LE10 Phys.Rev.Lett. 38, 1454 (1977) I.Y.Lee, M.M.Aleonard, M.A.Deleplanque, Y.El-Masri, J.O.Newton, R.S.Simon, R.M.Diamond, F.S.Stephens Second Discontinuity in the Yrast Levels of 158Er NUCLEAR REACTIONS 122Sn(40Ar, 4nγ); measured Eγ, Iγ, γγ-coin. 158Er deduced yrast levels, backbending.
doi: 10.1103/PhysRevLett.38.1454
1977NE02 Phys.Rev.Lett. 38, 810 (1977) J.O.Newton, I.Y.Lee, R.S.Simon, M.M.Aleonard, Y.El Masri, F.S.Stephens, R.M.Diamond Energy-Dependent Multiplicities of Continuum γ Rays NUCLEAR REACTIONS 12C, 27Al, K, Cl, Ti, Fe, 68Zn, 82Se, 126,130Te(40Ar, X), E=119-185 MeV; measured γ-multiplicities. KCl target.
doi: 10.1103/PhysRevLett.38.810
1976AL01 Nucl.Phys. A257, 490 (1976) M.M.Aleonard, P.Hubert, L.Sarger, P.Mennrath Etude des Etats Excites du 33Cl a l'Aide de la Reaction 32S(p, γ)33Cl NUCLEAR REACTIONS 32S(p, γ), E=0.4-2.6 MeV; measured σ(E, Eγ, θ); deduced Q. 33Cl deduced levels, resonance strengths, γ-ray branchings, T1/2, J, π, δ. Enriched targets.
doi: 10.1016/0375-9474(76)90587-X
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
1975AL24 J.Phys.(Paris) 36, 913 (1975) M.M.Aleonard, P.Hubert, L.Sarger, P.Mennrath Proprietes des Etats E(x) = 3447 et 4642 keV du 29P NUCLEAR REACTIONS 28Si(p, γ), E= < 2 MeV; measured σ(E, Eγ, θ), γγ(θ), γ(t). 29P deduced resonances, J, π, Γ, δ, M(λ), T1/2.
1974AL04 Phys.Lett. 49B, 40 (1974) M.M.Aleonard, C.Boursiquot, P.Hubert, P.Mennrath Strengths of (p, γ) Resonances in 33Cl, 35Cl and 28Si NUCLEAR REACTIONS 27Al(p, γ), E=633, 744 keV; 34S(p, γ), E=1214 keV; 32S(p, γ), E=580, 588 keV; measured σ(Eγ). 28Si, 33,35Cl deduced absolute resonance strength.
doi: 10.1016/0370-2693(74)90575-9
1974DA15 Phys.Rev. C9, 2200 (1974) J.Dalmas, F.Leccia, M.M.Aleonard E = 1.118 MeV Resonance in the 27Al(p, γ)28Si Reaction NUCLEAR REACTIONS 27Al(p, γ), E=1.118, 1.724, 2.876 MeV; measured Eγ, Iγ, γ(θ), DSA. 28Si deduced levels, T1/2, J, π, γ-mixing, γ-branching.
doi: 10.1103/PhysRevC.9.2200
1973LE15 J.Phys.(Paris) 34, 147 (1973) F.Leccia, M.M.Aleonard, D.Castera, P.Hubert, P.Mennrath Rapports d'Embranchement, Vies Moyennes et Melanges Multipolaires dans Le Noyau 24Mg NUCLEAR REACTIONS 23Na(p, γ), E=600-1500 keV; measured DSA, γ(θ). 24Mg levels deduced T1/2, γ-branching, γ-mixing, B(E2).
doi: 10.1051/jphys:01973003402-3014700
1972HU10 Nucl.Phys. A195, 485 (1972) P.Hubert, M.M.Aleonard, D.Castera, F.Leccia, P.Mennrath Etude des Etats Excites du Noyau 35Cl (I). Courbe d'Excitation de la Reaction 34S(p, γ)35Cl, Energie et Rapports d'Embranchement des Niveaux du 35Cl NUCLEAR REACTIONS 34S(p, γ), E=0.7-2.1 MeV; measured σ(E;Eγ), Q. 35Cl deduced resonances, levels, γ-branching.
doi: 10.1016/0375-9474(72)91071-8
1972HU11 Nucl.Phys. A195, 502 (1972) P.Hubert, M.M.Aleonard, D.Castera, F.Leccia, P.Mennrath Etude des Etats Excites du 35Cl (II). Vies Moyennes NUCLEAR REACTIONS 34S(p, γ)35Cl, E=0.7-2.1 MeV; measured Doppler-shift attenuation. 35Cl levels deduced T1/2, J, π.
doi: 10.1016/0375-9474(72)91072-X
1972LE29 J.Phys.(Paris) 33, 451 (1972) F.Leccia, M.M.Aleonard, D.Castera, P.Hubert, P.Mennrath Etude des Resonances de la Reaction 31P(p, γ)32S dans le Domaine d'Energie E = 1 100-1 600 keV NUCLEAR REACTIONS 31P(p, γ), E=1.1-1.6 MeV; measured σ(E), Eγ, Iγ. 32S deduced resonances, J, π, level-width, γ-branching.
doi: 10.1051/jphys:01972003305-6045100
1970AL05 Nucl.Phys. A146, 90 (1970) M.M.Aleonard, D.Castera, P.Hubert, F.Leccia, P.Mennrath, J.P.Thibaud Mesures des Vies Moyennes des Premiers Etats Excites du Noyau 28Si NUCLEAR REACTIONS 27Al(p, γ), E=774-2054 keV; measured Doppler shift attenuation. 28Si levels deduced T1/2.
doi: 10.1016/0375-9474(70)91089-4
1970TH03 C.R.Acad.Sci., Ser.B, 270, 115 (1970) J.-P.Thibaud, M.-M.Aleonard, D.Castera, P.Hubert, F.Leccia, P. Mennrath Mesure par Effet Doppler de Vies Moyennes d'Etats Excites dans le Noyau de l'Argon-36 NUCLEAR REACTIONS 35Cl(p, γ), E=0.859, 1.097, 1.129 MeV; measured σ(E;Eγ), Doppler shift attenuation. 36Ar levels deduced T1/2, J, π, γ-branching.
1970TH04 J.Phys. (Paris) 31, 131 (1970) J.P.Thibaud, M.M.Aleonard, D.Castera, P.Hubert, F.Leccia, P.Mennrath Mesures des Vies Moyennes des Premiers Etats Excites du Noyau 36Ar NUCLEAR REACTIONS 35Cl(p, γ), E=1.7-2.6 MeV; measured Doppler shift attenuation, σ(E;Eγ). 36Ar levels deduced T1/2, B(EL), level-width.
doi: 10.1051/jphys:01970003102-3013100
1969AL06 Compt.Rend. 268B, 1272 (1969) M.-M.Aleonard, D.Castera, P.Hubert, F.Leccia, P.Mennrath, J.-P.Thibaud Contribution a la Mesure par Effet Doppler des Vies Moyennes des Etats Nuclearires Excites. Application Aux Etats d'Energie de 1, 778, 4, 617 et 6, 272 MeV du Noyau du Silicium-28 NUCLEAR REACTIONS 27Al(p, γ), E=992, 1317, 2482 keV; measured Doppler shift attenuation. 28Si levels deduced T1/2. Ge(Li) detector.
1969TH03 Nucl.Phys. A135, 281 (1969) J.P.Thibaud, M.M.Aleonard, D.Castera, P.Hubert, F.Leccia, P.Mennrath Mesures des Vies Moyennes des Premiers Etats Excites du Noyau 32S NUCLEAR REACTIONS 31P(p, γ), E = 0.811-1.555 MeV; measured Doppler shift attenuation. 32S levels deduced T1/2.
doi: 10.1016/0375-9474(69)90163-8
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