NSR Query Results
Output year order : Descending NSR database version of May 3, 2024. Search: Author = A.Gallmann Found 110 matches. Showing 1 to 100. [Next]1982TH01 Phys.Rev. C25, 331 (1982) C.E.Thorn, W.F.Piel, Jr., M.J.LeVine, P.D.Bond, A.Gallman Masses of 98Pd, 99Pd, and 100Pd NUCLEAR REACTIONS 96Ru(16O, 14C), (16O, 13C), (16O, 12C), 104Pd(16O, 14C), E=70 MeV; measured σ(E(12C)), σ(E(13C)), σ(E(14C)). 98,99,100Pd deduced level, Q, mass excess. 106Cd deduced mass excess. Q3D magnetic spectrometer.
doi: 10.1103/PhysRevC.25.331
1981HE08 Phys.Rev. C23, 1527 (1981) B.Heusch, C.Beck, J.P.Coffin, R.M.Freeman, A.Gallmann, F.Haas, F.Rami, P.Wagner, D.E.Alburger Systematics of Carbon + Carbon Fusion-Evaporation Reactions NUCLEAR REACTIONS 13C(13C, X), E=30-60 MeV; 12C, 13C, 14C(12C, X), E=40 MeV; measured σ(fragment θ, Z, mass), fusion-evaporation yields for 16,17,18O, 20,21,22Ne, 24,25Mg, 22,23,24Na, 19,20,21F. Enriched targets, tof fragment charge identification. Statistical particle evaporation calculations.
doi: 10.1103/PhysRevC.23.1527
1980HE11 J.Phys.(Paris), Colloq.C-10, 229 (1980) B.Heusch, C.Beck, J.P.Coffin, R.M.Freeman, A.Gallmann, F.Haas, F.Rami, P.Wagner, D.E.Alburger The 18O + 12C Fusion-Evaporation Reaction NUCLEAR REACTIONS 12C(18O, X), E=32-100 MeV; 14C(16O, X), E=50 MeV; 12C(16O, X), E not given; measured σ(fragment mass, E); deduced production σ for Si, Al, Mg, Na, Ne. 30Si deduced no resonance structure in fusion channels. Statistical Hauser-Feshach calculations, Monte Carlo technique. Tof.
1980KO02 Phys.Rev. C21, 579 (1980) J.J.Kolata, R.M.Freeman, F.Hass, B.Heusch, A.Gallmann Reaction Cross Sections for 12C + 12C NUCLEAR REACTIONS 12C(12C, X), E(cm)=14-31 MeV; measured production σ(E) for 22,23Na, 19,20,21,22Ne, 18,19F, 16O, 12C; deduced fusion σ, inelastic σ, 3α evaporation σ. 24Mg deduced fusion L trajectory.
doi: 10.1103/PhysRevC.21.579
1979FI08 J.Phys.(Paris) 40, 511 (1979) P.Fintz, I.Riedinger-Ordonez, G.Guillaume, F. Jundt, A.Gallmann Vies Moyennes de Niveaux de 53Mn Excites par la Reaction 50Cr(α, pγ)53Mn NUCLEAR REACTIONS 50Cr(α, p), E=45 MeV; measured γp-coin, DSA. 53Mn levels deduced T1/2, B(λ), branching ratios. Shell model.
doi: 10.1051/jphys:01979004006051100
1979GU10 Nucl.Phys. A322, 189 (1979) G.Guillaume, P.Fintz, A.Gallmann, F.Jundt, I.Riedinger-Ordonez, P.Sioshansi Etats de Haut Spin dans 53Mn NUCLEAR REACTIONS 40Ca(16O, 3pγ), E=45 MeV; measured σ(E, Eγ), σ(Eγ, θ), γγ-coin, γ-ray linear polarization. 53Mn deduced levels, J, π, δ. Natural target. Compton-suppression spectrometer, three-crystal Ge(Li) polarimeter.
doi: 10.1016/0375-9474(79)90341-5
1979KO03 Phys.Rev. C19, 408 (1979) J.J.Kolata, R.M.Freeman, F.Haas, B.Heusch, A.Gallmann Reaction Cross Sections for 16O + 12C NUCLEAR REACTIONS 12C(16O, X), E(cm)=17-28 MeV; measured σ(E, production). Evaporation model analysis of nuclide distributions. Correlation analysis of fluctuations.
doi: 10.1103/PhysRevC.19.408
1979KO15 Phys.Rev. C19, 2237 (1979) J.J.Kolata, R.M.Freeman, F.Haas, B.Heusch, A.Gallmann Gross and Intermediate-Width Structure in the Interaction of 16O with 16O NUCLEAR REACTIONS 16O(16O, X), E(cm)=12-40 MeV; measured production σ for 20Ne, 23Na, 27,28,29,30Si, 30,31P, 26,27Al, 24,26Mg; deduced total σ(fusion), barrier height, critical parameters, normalizations. Evaporation model, optical model analysis.
doi: 10.1103/PhysRevC.19.2237
1978CO07 Phys.Rev. C17, 1607 (1978) J.P.Coffin, P.Engelstein, A.Gallmann, B.Heusch, P.Wagner, H.E.Wegner 18O + 12C and 18O + 13C Fusion-Evaporation Reactions NUCLEAR REACTIONS 12,13C(18O, X), E=100 MeV; measured fusion σ(A, Z).
doi: 10.1103/PhysRevC.17.1607
1978OE01 Phys.Rev. C18, 239 (1978) H.Oeschler, J.P.Coffin, P.Engelstein, A.Gallmann, K.S.Sim, P.Wagner Heavy-Ion Transfer Reactions as a Diffusion Process NUCLEAR REACTIONS 130Te(28Si, X), E=140 MeV; measured < Q > , < ΔA > ; deduced drift, diffusion coefficients for energy dissipation, mass transport.
doi: 10.1103/PhysRevC.18.239
1978WI04 Phys.Rev. C18, 401 (1978) D.H.Wilkinson, A.Gallmann, D.E.Alburger Super-Allowed Fermi β Decay: Half-Lives of 14O and 38K-m RADIOACTIVITY 14O, 38mK; measured T1/2; deduced ft values. Compared with systematics.
doi: 10.1103/PhysRevC.18.401
1977HA11 Nucl.Phys. A279, 237 (1977) F.Haas, R.M.Freeman, B.Heusch, A.Gallmann Structure en Bande du Noyau 22Na: le Premier Niveau Jπ = 6+ NUCLEAR REACTIONS 19F(α, n), E=7.825, 8.225 MeV; measured n-γ(θ), Doppler shift attenuation. 22Na levels deduced J, π, branching ratios, δ, T1/2, transition strengths.
doi: 10.1016/0375-9474(77)90226-3
1977HE04 Phys.Rev. C15, 1196 (1977) B.Heusch, F.Haas, R.M.Freeman, A.Gallmann Experimental Study of the 12C(3He, p)14N Reaction Mechanism between 11 And 20 MeV Bombarding Energy NUCLEAR REACTIONS 12C(3He, pγ), E=11-20 MeV; measured pγ(θ); deduced reaction mechanism, nuclear alignments.
doi: 10.1103/PhysRevC.15.1196
1977KO16 Phys.Rev. C16, 891 (1977) J.J.Kolata, R.C.Fuller, R.M.Freeman, F.Haas, B.Heusch, A.Gallmann Reaction Cross Sections for 16O + 16O NUCLEAR REACTIONS 16O(16O, X), E(cm)=12.5-30.5 MeV; measured σ(A) for production of A=16-31 reaction products; deduced broad shape resonances.
doi: 10.1103/PhysRevC.16.891
1976CO26 Phys.Rev. C14, 861 (1976) J.P.Coffin, F.Jundt, A.Gallmann, E.K.Warburton Mean Lifetimes of the 44Sc 1648, 1652, 1681, and 1768 keV Levels NUCLEAR REACTIONS 41K(α, nγ), E=5.0-11 MeV; measured nγ-, γγ-coin, Eγ, DSA. 44Sc deduced levels, T1/2. Enriched target, Ge(Li) detectors.
doi: 10.1103/PhysRevC.14.861
1976FI03 Nucl.Phys. A259, 493 (1976) P.Fintz, G.Guillaume, F.Jundt, I.Ordonez, A.Gallmann, D.E.Alburger Etude de Neutrons Retardes de la Reaction 10Be + 11B RADIOACTIVITY 9Li, 16C, 17N [from 10Be+11Be, E=30-40 MeV]; measured T1/2, delayed γ, delayed neutrons. 19N; measured no activity. Radioactive target.
doi: 10.1016/0375-9474(76)90084-1
1976FR09 Nucl.Phys. A261, 471 (1976) R.M.Freeman, F.Haas, B.Heusch, A.Gallmann Largeurs de Transitions Gamma du Niveau a 2788 keV de 21Ne NUCLEAR REACTIONS 18O(α, n), E=4.7 MeV; measured Iγ, γγ(θ), recoil distance. 21Ne deduced branching ratios, δ, T1/2, transition strengths.
doi: 10.1016/0375-9474(76)90160-3
1976FR19 Phys.Rev. C14, 2006 (1976) R.M.Freeman, F.Haas, B.Heusch, A.Gallmann Strong Isoscalar M2 Transition in 22Na NUCLEAR REACTIONS 19F(α, nγ), E=5.5 MeV; measured n, γ spectra. 22Na level deduced γ-branching.
doi: 10.1103/PhysRevC.14.2006
1976GU14 Nucl.Phys. A272, 338 (1976) G.Guillaume, B.Rastegar, P.Fintz, A.Gallmann Etude de 17N par la Reaction 18O(t, αγ)17N NUCLEAR REACTIONS 18O(t, αγ), E=3.5 MeV; measured Eα, Eγ, σ(Eα, Eγ, θαγ). 17N deduced levels, γ-branching ratios, J, π, δ. Enriched target.
doi: 10.1016/0375-9474(76)90336-5
1976KO24 Phys.Lett. 65B, 333 (1976) J.J.Kolata, R.M.Freeman, F.Haas, B.Heusch, A.Gallmann On the Fusion Cross Section for 16O + 12C NUCLEAR REACTIONS 12C(16O, X), E=40-65 MeV; measured total fusion σ(E).
doi: 10.1016/0370-2693(76)90235-5
1975WA06 Phys.Rev. C11, 1459 (1975) P.Wagner, R.M.Freeman, A.Gallman, E.K.Warburton Decay of the 10Be 0+ 6.18-MeV Level NUCLEAR REACTIONS 11B(t, αγ); measured σ(Eγ), αγ-coin. 10Be deduced transitions, γ-branching ratios.
doi: 10.1103/PhysRevC.11.1459
1975WA10 Phys.Rev. C11, 1622 (1975) P.Wagner, M.A.Ali, J.P.Coffin, A.Gallmann Electromagnetic Properties of Low-Lying 26Mg States NUCLEAR REACTIONS 26Mg(α, α'γ), E=16 MeV; measured Eγ, Iγ, DSA, Coulomb excitation. 26Mg levels deduced K, J, π, T1/2, B(λ), γ-mixing, γ-branching. Ge(Li) detectors.
doi: 10.1103/PhysRevC.11.1622
1974CL07 Nucl.Phys. A232, 311 (1974) T.P.Cleary, N.Stein, W.D.Callender, D.A.Bromley, J.P.Coffin, A.Gallmann The Structure of 209Bi (II). Macroscopic Structure from Direct Scattering NUCLEAR REACTIONS 209Bi, 208Pb(p, p'), E=16.10 MeV; measured σ(Ep', θ). 209Bi deduced levels, L, J, β. 209Bi(p, p'), E=14.95 MeV; measured σ(Ep', θ). 209Bi deduced levels. Enriched, natural targets.
doi: 10.1016/0375-9474(74)90624-1
1974CO01 Phys.Rev. C9, 38 (1974) J.P.Coffin, A.Gallmann, F.Haas, P.Wagner, J.W.Olness Lifetime of the 18O 4+1 State at 3.555-MeV Excitation NUCLEAR REACTIONS 16O(t, p), (t, n), E=3.1 MeV; measured σ(θ), recoil distance. 18O, 18F levels deduced T1/2, λ, γ-branching.
doi: 10.1103/PhysRevC.9.38
1974DA02 Phys.Rev. C9, 216 (1974) C.N.Davids, D.R.Goosman, D.E.Alburger, A.Gallmann, G.Guillaume, D.H.Wilkinson, W.A.Lanford β Decay of 22F RADIOACTIVITY 22F; measured T1/2, Eγ, Iγ, Eβ, γγ-coin, γβ-coin. Deduced log ft. 22Ne deduced levels, J, π.
doi: 10.1103/PhysRevC.9.216
1974DA06 Nucl.Phys. A220, 166 (1974) N.E.Davison, P.Fintz, A.Gallmann Study of the Reactions 12C(d, d)12C and 12C(d, p)13C Across the Resonance at E = 2.71 MeV NUCLEAR REACTIONS 12C(d, d), E=2.61-2.82 MeV; measured σ(E, θ(d)); 12C(d, p), E=2.61-2.82 MeV; measured σ(E, Ep, θ(p)); 14N deduced level. 13C deduced levels, L(n). Natural target.
doi: 10.1016/0375-9474(74)90759-3
1974GU11 Nucl.Phys. A227, 284 (1974) G.Guillaume, B.Rastegar, P.Fintz, A.Gallmann Transitions Electromagnetiques dans le Noyau 32Si Atteint par la Reaction 30Si(t, pγ)32Si NUCLEAR REACTIONS 30Si(t, pγ), E=2.5-3.3 MeV; measured Eγ, DSA, σ(Ep, Eγ, θ(pγ)). 32Si deduced levels, E(X), γ-branching ratios, J, π, γ-mixing, T1/2. Enriched target.
doi: 10.1016/0375-9474(74)90797-0
1974GU19 Nucl.Phys. A233, 357 (1974) G.Guillaume, P.Fintz, F.Jundt, I.Ordonez, A.Gallmann, D.E.Alburger, K.W.Jones Recherche de l'Isotope 19N par la Reaction 10Be(11B, 2p)19N RADIOACTIVITY 19N [from 10Be(11B, 2p)]; measured Eγ, Iγ, delayed neutrons, T1/2; deduced Iγ limits, log ft. 19O level deduced π. Radioactive target.
doi: 10.1016/0375-9474(74)90461-8
1974RA15 Nucl.Phys. A225, 80 (1974) B.Rastegar, G.Guillaume, P.Fintz, A.Gallmann Etude du Noyau 28Mg par la Reaction 26Mg(t, pγ)28Mg NUCLEAR REACTIONS 26Mg(t, pγ), E=2.54-3.20 MeV; measured Eγ, DSA, σ(Ep, Eγ, θ(pγ)). 28Mg deduced levels, γ-branching ratios, J, π, γ-mixing, T1/2. Enriched targets.
doi: 10.1016/0375-9474(74)90366-2
1973FR18 Phys.Rev. C8, 2182 (1973) R.M.Freeman, F.Haas, B.Heusch, J.Fernandez Castillo, J.W.Olness, A.Gallmann Rotational Band Structure of 22Na. II. Neutron-Gamma Coincidence Measurements NUCLEAR REACTIONS 19F(α, nγ), E=11 MeV; measured nγ(θ, t), DSA, γγ(θ). 22Na levels deduced T1/2, quadrupole moment.
doi: 10.1103/PhysRevC.8.2182
1973HA40 Nucl.Phys. A211, 289 (1973) F.Haas, R.M.Freeman, B.Heusch, S.Kohmoto, A.Gallmann Vies Moyennes dans 14N NUCLEAR REACTIONS 12C(3He, pγ), E=5.54 MeV; measured Eγ, DSA, σ(Ep, Eγ, θ(pγ)). 14N deduced levels, T1/2. Natural 12C targets self-supporting or on Ni backing.
doi: 10.1016/0375-9474(73)90720-3
1973HA55 Phys.Rev. C8, 2169 (1973) F.Haas, R.M.Freeman, J.Fernandez Castillo, A.Gallmann Rotational Band Structure of 22Na. I. Electromagnetic Transitions for Levels of E(ex) < 4.0 MeV NUCLEAR REACTIONS 19F(α, nγ), E=5-8 MeV; measured DSA, recoil distance, Eγ. 22Na levels deduced T1/2, π, γ-branching.
doi: 10.1103/PhysRevC.8.2169
1973HE09 Phys.Rev. C7, 1810 (1973) Study of the 12C(h, p)14N Reaction Mechanism by a Systematic Use of the p-γ Angular-Correlation Method NUCLEAR REACTIONS 12C(3He, pγ), E=3-11 MeV; measured σ(E, θ), pγ(θ). 14N levels deduced alignment.
doi: 10.1103/PhysRevC.7.1810
1973WA14 Phys.Rev. C7, 2418 (1973) P.Wagner, J.P.Coffin, M.A.Ali, D.E.Alburger, A.Gallman Lifetime Measurements of Low-Lying States of 33P NUCLEAR REACTIONS 31P(t, pγ), E=2.5, 3.1 MeV; measured σ(Ep), DSA, Iγ, pγ-coin, Eγ. 33P deduced levels, γ-branching, T1/2, γ-mixing, J.
doi: 10.1103/PhysRevC.7.2418
1972CL02 Phys.Rev.Lett. 28, 699 (1972) T.P.Cleary, W.D.Callender, N.Stein, C.H.King, D.A.Bromley, J.P.Coffin, A.Gallmann Alternate Models of Particle-Core Coupling in 209Bi NUCLEAR REACTIONS 209Bi(p, p'), E=16.10, 14.95 MeV; measured σ(Ep', θ). 209Bi deduced levels.
doi: 10.1103/PhysRevLett.28.699
1972FI22 Nucl.Phys. A197, 423 (1972) P.Fintz, B.Rastegar, N.E.Davison, F.Hibou, G.Guillaume, A.Gallmann Etude Experimentale de Transitions Electromagnetiques dans le Noyau 28Mg NUCLEAR REACTIONS 26Mg(t, pγ), E=2.5-3.2 MeV; measured σ(Ep, Eγ, θ(pγ)), Doppler-shift attenuation. 28Mg deduced levels, γ-branching ratios, J, γ-mixing, T1/2. Enriched target.
doi: 10.1016/0375-9474(72)91020-2
1972FR11 Nucl.Phys. A197, 529 (1972) R.M.Freeman, R.Faerber, M.Toulemonde, A.Gallmann Etude de Transitions γ dans le Noyau 35S NUCLEAR REACTIONS 34S(d, pγ), E=3.50, 4.00 MeV; measured Eγ, DSA, σ(Ep, Eγ, θ(pγ)). 35S deduced levels, γ-branching ratios, J, γ-mixing, T1/2. Enriched target.
doi: 10.1016/0375-9474(72)91027-5
1972GA05 Can.J.Phys. 50, 278 (1972) A.Gallmann, F.Haas, M.Toulemonde Mesures de Rapports d'Embranchement et de Vies Moyennes dans 30Si NUCLEAR REACTIONS 27Al(α, pγ), E=9-10 MeV; measured σ(E;Ep, Eγ), DSA. 30Si levels deduced T1/2, γ-branching.
doi: 10.1139/p72-043
1971GA08 Nucl.Phys. A166, 271 (1971) A.Gallmann, G.Guillaume, N.E.Davison, P.Wagner, G.Franck Polarisation Lineaire de Rayonnements γ Emis dans la Reaction 46Ti(p, p'γ) NUCLEAR REACTIONS 46Ti(p, p'γ), E=5.489, 5.508 MeV; measured γ-linear polarization pγ(E;θ(γ)=90°), σ(E;Eγ, θ(γ)). 46Ti levels deduced J, π, γ-mixing, branching ratios. Enriched target. Ge(Li) detectors.
doi: 10.1016/0375-9474(71)90430-1
1971HI06 Nucl.Phys. A171, 603 (1971) F.Hibou, P.Fintz, B.Rastegar, A.Gallmann Etude des Premiers Niveaux Excites du 19O par des Mesures de Correlations Angulaires et de Vies Moyennes NUCLEAR REACTIONS 18O(d, pγ), E=1.7, 5.0 MeV; 17O(t, pγ), E=2.95 MeV; measured σ(Ep, Eγ, θ(pγ)), Doppler-shift attenuation. 19O deduced levels J, π, γ-mixing, T1/2. Enriched targets.
doi: 10.1016/0375-9474(71)90606-3
1971JU02 Nucl.Phys. A166, 266 (1971) F.Jundt, E.Aslanides, A.Gallmann, D.E.Alburger Determination de la Parite du Niveau de 4.19 MeV de 36S NUCLEAR REACTIONS 34S(t, p), E=3.1 MeV; measured γ linear polarization. 36S levels deduced π. Enriched target.
doi: 10.1016/0375-9474(71)90429-5
1971JU03 Nucl.Phys. A170, 12 (1971) F.Jundt, E.Aslanides, B.Fride, A.Gallmann Desintegration β+ de 25Al RADIOACTIVITY 25Al[from 24Mg(d, n)]; measured Eγ, Iγ, T1/2; deduced Iβ, log ft. Enriched target.
doi: 10.1016/0375-9474(71)90679-8
1971JU04 Phys.Rev. C4, 498 (1971) F.Jundt, E.Aslanides, A.Gallmann, E.K.Warburton Studies of the Low-Lying States of 41K via the Reactions 41Ar(β-)41K And 41K(p, p'γ)41K RADIOACTIVITY 41Ar; measured Eγ, Iγ, T1/2; deduced log ft. 41K deduced levels, J, π. 41K(p, p'γ), E=5.3, 5.5, 5.8 MeV; measured σ(Ep', Eγ). 41K deduced levels, J, π, γ-branching.
doi: 10.1103/PhysRevC.4.498
1971OL02 Phys.Rev. C3, 2323 (1971) J.W.Olness, W.R.Harris, A.Gallmann, F.Jundt, D.E.Alburger, D.H.Wilkinson Levels of S36 from S34(t, p)S36 NUCLEAR REACTIONS 34S(t, pγ), E=3.12 MeV; measured σ(Ep, Eγ, θ(pγ)), Eγ, Iγ, tγ-delay. 36S deduced levels, L, J, π.
doi: 10.1103/PhysRevC.3.2323
1970AS06 Nucl.Phys. A152, 251 (1970) E.Aslanides, F.Jundt, A.Gallmann Desintegration β+ de 18Ne RADIOACTIVITY 18Ne[from 16O(3He, n)]; measured Iγ, T1/2; deduced Iβ, log ft. Natural gas target.
doi: 10.1016/0375-9474(70)90827-4
1970FI08 Nucl.Phys. A150, 49 (1970) P.Fintz, F.Hibou, B.Rastegar, A.Gallman Etude de Transitions γ dans le Noyau 19O NUCLEAR REACTIONS 18O(d, pγ), E=5.0 MeV; measured σ(Ep, Eγ). 19O deduced levels, γ-branching ratios. Enriched target.
doi: 10.1016/0375-9474(70)90453-7
1970FR10 Nucl.Phys. A156, 305 (1970) Etude de Transitions γ dans les Noyaux 40K et 28Al NUCLEAR REACTIONS 27Al(d, p), 39,41K(d, p), E=3.5, 3.7 MeV; measured Eγ, pγ-coin. 28Al, 40K deduced levels, γ-branching ratios. 42K deduced transitions. Natural targets.
doi: 10.1016/0375-9474(70)90143-0
1970GA01 Nucl.Phys. A143, 326 (1970) A.Gallmann, G.Frick, B.Heusch, F.Haas, E.K.Warburton Mesures de Vies Moyennes dans 13C et 10B par la Methode du Parcours de Recul NUCLEAR REACTIONS 10B(α, pγ), E = 1.96 MeV; 7Li(α, nγ), E = 8.95 MeV; measured Eγ(θ(γ) = 0°), Doppler shift, recoil distance. 13C, 10B deduced levels, T1/2. Enriched 10B, natural Li targets.
doi: 10.1016/0375-9474(70)90567-1
1970GA09 Can.J.Phys. 48, 1595 (1970) A.Gallman, F.Haas, N.Balaux, B.Heusch, M.Toulemonde Mesures de Vies Moyennes dans 12B, 14N et 16O NUCLEAR REACTIONS 11B(d, pγ), E=2.1 MeV; 19F(p, αγ), E=4.1 MeV; 12C(3He, pγ), E=4 MeV; measured Doppler-shift attenuation. 12B, 14N, 16O levels deduced T1/2.
doi: 10.1139/p70-201
1970HA52 Nucl.Phys. A156, 385 (1970) F.Haas, B.Heusch, G.Frick, A.Gallmann, D.E.Alburger Vies Moyennes des Niveaux de 3.79 MeV de 30Si et 0.709 MeV de 30P NUCLEAR REACTIONS 27Al(α, pγ), E=4.60 MeV; 27Al(α, nγ), E=8.50 MeV; measured Eγ, recoil distance. 30Si, 30P levels deduced T1/2.
doi: 10.1016/0375-9474(70)90149-1
1969AL17 Phys.Rev. 185, 1242 (1969) D.E.Alburger, E.K.Warburton, A.Gallmann, D.H.Wilkinson Decay of the 6.18-MeV J(π) = 0+ Level of Be10 NUCLEAR REACTIONS 9Be(d, pγ), E = 3.25 MeV; measured σ(Ep), γγ-coin, Doppler shift attenuation. 10Be level deduced T1/2, level-width, γ-branching. 12C(d, p), E = 3.25 MeV; measured Eγ. 13C deduced levels.
doi: 10.1103/PhysRev.185.1242
1969FI07 Nucl.Phys. A132, 265 (1969) P.Fintz, F.Hibou, B.Rastegar, A.Gallmann Niveaux Excites de 19O Etudies par la Reaction 18O(d, p)19O NUCLEAR REACTIONS 18O(d, p), E=3, 5 MeV; measured σ(Ep, θ), σ(Eγ), pγ-, γγ-coin. 19O deduced levels, L, π, γ-branching ratio. Enriched target.
doi: 10.1016/0375-9474(69)90483-7
1969GA01 Nucl.Phys. A123, 27(1969) Resonances dans la Reaction 10B+α par l'Etude des Rayonnements γ Detectes avec un Semi-Conducteur Ge(Li) NUCLEAR REACTIONS 10B(α, p), (α, α'), E=1.0-3.5 MeV; measured σ(E; Eγ). 14N deduced levels, level-width. Enriched 10B target, Ge(Li) detector.
doi: 10.1016/0375-9474(69)90887-2
1969GA05 Phys.Rev. 179, 921 (1969) A.Gallmann, F.Jundt, E.Aslanides, D.E.Alburger Beta Decays of C15, F17, and F20 RADIOACTIVITY 15C, 17F, 20F; measured Iγ; deduced log ft, β-branching. 15N, 17O, 20Ne deduced levels. Ge(Li) detector.
doi: 10.1103/PhysRev.179.921
1969GA16 Rev.Phys.Appl. 4, 216 (1969) A.Gallmann, F.Haas, B.Heusch, M.Toulemonde Mesures de Vies Moyennes par Effet Doppler NUCLEAR REACTIONS 11B(d, p), E=2.1 MeV; 12C(3He, p), E=4 MeV; measured Doppler shift attenuation. 12B, 14N levels deduced T1/2. Ge(Li) detector.
doi: 10.1051/rphysap:0196900402021601
1969GA27 Phys.Rev. 186, 1160 (1969) A.Gallmann, E.Aslanides, F.Jundt, E.Jacobs Positron Decays of 42Ti and 38Ca RADIOACTIVITY 38Ca[from 36Ar(3He, n)], 42Ti[from 40Ca(3He, n)]; measured T1/2, Eγ, Iγ; deduced log ft. 38K, 42Sc levels deduced J, π, branching ratios.
doi: 10.1103/PhysRev.186.1160
1969HA49 Phys.Rev. 188, 1625 (1969) F.Haas, B.Heusch, A.Gallmann, D.A.Bromley Experimental Investigations of the C12(h, p)N14 Reaction Mechanism NUCLEAR REACTIONS 12C(3He, pγ), E=4.6-11 MeV; measured σ(E;θ(p), θ(pγ)); deduced heavy-particle direct stripping. 15O deduced resonances. 14N deduced level population.
doi: 10.1103/PhysRev.188.1625
1968GA10 Nucl.Phys. A118, 515(1968) A.Gallmann, F.Jundt, E.Aslanides, D.A.Bromley Etude de la Region de 3 MeV d'Excitation de 27Al NUCLEAR REACTIONS 27Al(p, p'); E=4.32-4.43; 4.81-4.90; 5.70-5.80 MeV; measured σ(E;Ep'), γγ-coin. 27Al levels deduced γ-branching ratios, J. Natural target.
doi: 10.1016/0375-9474(68)90436-3
1968GO05 Nucl.Phys. A109, 417(1968) S.Gorodetzky, E.Aslanides, A.Gallmann, G.Frick Radioactivite β de 18Ne, 23Mg, 26Si et 27Mg RADIOACTIVITY 18Ne [from 16O(3He, n)], 23Mg [from 23Na (p, n)], 26Si [from 24Mg (3He, n)]; measured Eγ, Iγ; deduced Iβ, log ft. Natural target. 27Mg [from 26Mg(d, p)]; measured Eγ, Iγ, T1/2; deduced Iβ, log ft. Enriched target. 18F, 23Na, 26,27Al deduced levels, branching ratios.
doi: 10.1016/0375-9474(68)90607-6
1968KA15 Phys.Rev. 175, 1426 (1968) R.W.Kavanagh, A.Gallmann, E.Aslanides, F.Jundt, E.Jacobs Positron Decay of 38Ca and 38K NUCLEAR STRUCTURE 14O, 38K, 38Ca, 37K, 35Ar, 34Cl; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.175.1426
1967GA10 Phys.Rev. 163, 1190 (1967) A.Gallmann, G.Frick, E.K.Warburton, D.E.Alburger, S.Hechtl Positron Decay of Mg22 NUCLEAR STRUCTURE 22Mg; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.163.1190
1967GA12 Phys.Rev. 164, 1257 (1967) Study of Unbound Levels in N14 by the C12(He3, pγ)N14 Reaction NUCLEAR STRUCTURE 12C, 14N; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.164.1257
1967GO07 Phys.Rev. 155, 1119 (1967) S.Gorodetzky, R.M.Freeman, A.Gallmann, F.Haas, B.Heusch Angular-Correlation Studies of the Reactions O16(He3, Pγ)F18 and O16(He3, αγ)O15 NUCLEAR STRUCTURE 18F, 16O, 15O; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.155.1119
1967GO10 Nucl.Phys. A97, 475(1967) S.Gorodetzky, J.P.Coffin, G.Frick, A.Gallmann, F.Jundt, E.Aslanides Contribution a l'Etude du Doublet de Niveaux a 6.88 MeV de 28Si NUCLEAR REACTIONS 25Mg(α, nγ), E = 6 MeV; measured σ(Eγ). 27Al(d, nγ), E = 4.6 MeV; measured E+E-(θ). 28Si deduced levels, J, π. Enriched 25Mg target, Ge(Li) detector.
doi: 10.1016/0375-9474(67)90502-7
1966AL06 Phys.Rev. 143, 692 (1966) D.E.Alburger, P.D.Parker, D.J.Bredin, D.H.Wilkinson, P.F.Donovan, A.Gallmann, R.E.Pixley, L.F.Chase, Jr., R.E.McDonald Properties of the 4.77- and 5.16-MeV States of B10 NUCLEAR STRUCTURE 6Li, 11B, 10B; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.143.692
1966AL10 Phys.Rev. 148, 1050 (1966) D.E.Alburger, A.Gallmann, J.B.Nelson, J.T.Sample, E.K.Warburton Properties of Excited States in C14 NUCLEAR STRUCTURE 14C, 13C; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.148.1050
1966GA08 Phys.Rev. 147, 753 (1966) A.Gallman, P.Fintz, J.B.Nelson, D.E.Alburger Study of Excited States in N15 and N16 NUCLEAR STRUCTURE 14N, 13C, 15N, 16N, 14C; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.147.753
1966GA09 Nucl.Phys. 82, 161(1966) A.Gallman, P.Fintz, P.E.Hodgson Reactions (d, p) sur 11B, 12C, 14N et 16O a E < 5.5 MeV NUCLEAR REACTIONS 12C, 16O(d, d), E = 4 MeV; measured σ(θ). 11B(d, p), E = 5.5 MeV; 12C(d, p), E = 1.2-4.5 MeV; 14N(d, p), E = 1.3-5.5 MeV; 16O(d, p), E = 1.3, 4 MeV; measured σ(Ep, θ). 12B, 13C, 15N, 17O deduced S.
doi: 10.1016/0029-5582(66)90529-3
1966GA16 Nucl.Phys. 88, 602(1966) A.Gallmann, G.Frick, D.E.Alburger, E.Aslanides, P.Siffert Radioactivite β+ de 30S RADIOACTIVITY 30S [from 28Si(3He, n)]; measured Eγ, Iγ; deduced Iβ, log ft. Natural target.
doi: 10.1016/0029-5582(66)90418-4
1966GA17 Nucl.Phys. 88, 654(1966); Erratum Nucl.Phys. A99, 696(1967) A.Gallmann, P.Wagner, G.Franck, D.Wilmore, P.E.Hodgson Analyse des Reactions 25Mg(p, p)25Mg et 24Mg(d, p)25Mg a 5 et a 6 MeV NUCLEAR REACTIONS 25Mg(p, p'), E = 5, 6 MeV; 24Mg(d, p), E = 5, 6 MeV; measured σ(Ep', θ). Enriched target.
doi: 10.1016/0029-5582(66)90422-6
1966GA18 Nucl.Phys. 88, 675(1966) A.Gallmann, P.Wagner, P.E.Hodgson Fluctuations des Sections Efficaces des Reactions 25Mg(p, p)25Mg et 24Mg(d, p)25Mg NUCLEAR REACTIONS 25Mg(p, p), E = 4.5-6.1 MeV; 24Mg(d, p), E = 2.8-6.1 MeV; measured σ(E;Ep, θ). Fluctuation analysis. Enriched targets.
doi: 10.1016/0029-5582(66)90423-8
1966GA19 Phys.Rev. 151, 735 (1966) Angular-Correlation Studies of the Reaction C12(He3, α)C11 and O16(He3, α)O15 NUCLEAR STRUCTURE 15O, 16O, 11C, 12C; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.151.735
1966GO12 Nucl.Phys. 82, 113(1966) S.Gorodetzky, J.P.Coffin, A.Gallmann, G.Frick, F.Jundt Etude de la Transition de 8.92 MeV A 0 dans 11Be et de la Transition de 6.49 MeV A 0 dans 11C NUCLEAR REACTIONS 10B(d, pγ), (d, nγ), E = 4.2 MeV; measured E+E- coincidences (θ). 11B, 11C levels deduced J, π.
doi: 10.1016/0029-5582(66)90526-8
1966GO15 Phys.Rev. 149, 801 (1966) S.Gorodetzky, R.M.Freeman, A.Gallman, F.Hass Angular-Correlation Studies of the Reactions O16(He3, αγ)O15, C12(He3, pγ)N14, and C12(d, pγ)C13 NUCLEAR STRUCTURE 12C, 15O, 13C, 16O, 14N; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.149.801
1965GA02 Phys.Rev. 138, B560 (1965) A.Gallman, F.Hibou, P.Fintz, P.E.Hodgson, E.K.Warburton B10(d, p)B12 Angular Distributions at E = 5.5 MeV for the B12 2.62- and 2.72-MeV Levels NUCLEAR STRUCTURE 11B; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.138.B560
1965GO04 Nucl.Phys. 62, 575 (1965) S.Gorodetzky, G.Bassompierre, A.Gallmann Etude de la Reaction 27Al(3He, p)29Si a 5 MeV NUCLEAR REACTIONS 27Al(3He, p), E=5 MeV; measured σ(Ep, θ).
doi: 10.1016/0029-5582(65)90582-1
1965GO05 Phys.Rev. 137, B1466 (1965) S.Gorodetzky, A.Gallmann, R.Rebmeister Study of the Excited States of B10 from 5 to 8 MeV by the B11(He3, α)B10 Reaction and a Note on the B11(He3, t0)C11 Reaction NUCLEAR STRUCTURE 11B; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.137.B1466
1965GO11 Nucl.Phys. 73, 74 (1965) S.Gorodetzky, A.Gallmann, J.P.Coffin, G.Frick, F.Jundt Transition Monopolaire dans 18O NUCLEAR REACTIONS 18O(p, p'), E=5.63 MeV; measured E+E--coincidences(θ). 18O transition deduced γ-multipolarity. Enriched target.
doi: 10.1016/0029-5582(65)90154-9
1964GO24 Compt.Rend.Congr.Intern.Phys.Nucl., Paris, P.Gugenberger, Ed., Centre National de la Recherche Scientifique, Paris, Vol.II, p.408(1964) S.Gorodetzky, A.Gallmann, G.Frick, J.P.Coffin, F.Jundt Etude des Embranchements Faibles de la Radioactivite β+ de 27Si NUCLEAR STRUCTURE 27Si; measured not abstracted; deduced nuclear properties.
1964WA05 Phys.Rev. 133, B42 (1964) E.K.Warburton, D.E.Alburger, A.Gallmann, P.Wagner, L.F.Chase, Jr. Determination of the Multipolarity of Nuclear Electromagnetic Transitions Using a Magnetic Pair Spectrometer NUCLEAR STRUCTURE 13C, 9Be; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.133.B42
1963FR10 Phys.Rev. 132, 2169 (1963) G.Frick, A.Gallmann, D.E.Alburger, D.H.Wilkinson, J.P.Coffin Positron Radioactivities of O14, Ne18, Si26, S30 NUCLEAR STRUCTURE 26Si, 14O, 18Ne, 30S; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.132.2169
1963GA03 Phys.Rev. 129, 1765 (1963) A.Gallmann, D.E.Alburger, D.H.Wilkinson, F.Hibou He3 Reactions on B11 and N14 NUCLEAR STRUCTURE 14N, 11B; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.129.1765
1963GO09 Nucl.Phys. 43, 92 (1963) S.Gorodetzky, G.Bassompierre, C.St.Pierre, A.Gallmann, P.Wagner Etude de la Reaction N14(He3, p)O16 entre 2.5 et 5.5 MeV NUCLEAR STRUCTURE 14N; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(63)90331-6
1963GO32 J.Phys. 24, 892 (1963) S.Gorodetzky, R.E.Pixley, A.Gallman, G.Frick, J.P.Coffin, G.Sibille Emission de Paires Internes du Niveau de 3, 63 MeV dans 18O NUCLEAR STRUCTURE 18O; measured not abstracted; deduced nuclear properties.
doi: 10.1051/jphys:019630024011089201
1963WI05 Phys.Rev. 130, 1953 (1963) D.H.Wilkinson, D.E.Alburger, A.Gallmann, P.F.Donovan Alpha-Particle Emission in the Decays of B12 and N12 NUCLEAR STRUCTURE 12B, 12N; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.130.1953
1962GO21 Compt.rend. 255, 879 (1962) S.Gorodetzky, P.Fintz, A.Gallmann NUCLEAR STRUCTURE 14N; measured not abstracted; deduced nuclear properties.
1962GO24 Compt.rend. 255, 1505 (1962) S.Gorodetzky, P.Fintz, A.Gallmann NUCLEAR STRUCTURE 11B; measured not abstracted; deduced nuclear properties.
1962GO26 Nuclear Phys. 38, 177 (1962) S.Gorodetzky, J.Ullman, G.Bergdolt, A.Gallmann Polarisation des Protons dans la Diffusion Elastique sur O16 et C12 NUCLEAR STRUCTURE 12C, 16O; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(62)91026-X
1961GO03 Compt.Rend. 252, 713 (1961) S.Gorodetzky, P.Fintz, G.Bassompierre, A.Gallmann NUCLEAR STRUCTURE 15N; measured not abstracted; deduced nuclear properties.
1961GO26 J.Phys.Radium 22, 570 (1961) S.Gorodetzky, J.Ullman, G.Bergdolt, A.Gallmann NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
1961GO27 J.Phys.Radium 22, 573 (1961) S.Gorodetzky, A.Gallmann, P.Fintz, G.Bassompierre NUCLEAR STRUCTURE 11B; measured not abstracted; deduced nuclear properties.
1961GO28 J.Phys.Radium 22, 575 (1961) S.Gorodetzky, A.Gallmann, P.Fintz, G.Bassompierre NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
1961GO29 J.Phys.Radium 22, 578 (1961) S.Gorodetzky, G.Frick, A.Gallmann NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
doi: 10.1051/jphysrad:019610022010057800
1960GA01 Bull.Am.Phys.Soc. 5, No.1, 19, E11 (1960) Thermal Neutron Capture in He3 NUCLEAR STRUCTURE 4He; measured not abstracted; deduced nuclear properties. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset11009. 1960GO14 Compt.Rend. 250, 3153 (1960) S.Gorodetzky, M.Croissiaux, A.Gallmann, P.Fintz, J.Samuel, G.Bassompierre Study of the 6.76 and 7.30 MeV Levels of B11 by the B10(d, p)B11 Reaction NUCLEAR STRUCTURE 11B; measured not abstracted; deduced nuclear properties.
1960GO18 J.Phys.Radium 21, 349 (1960) S.Gorodetzky, J.Samuel, A.Gallmann Angular Correlation (d, pγ) in the Reaction Be9(d, p)Be10 NUCLEAR STRUCTURE 10Be; measured not abstracted; deduced nuclear properties.
doi: 10.1051/jphysrad:01960002105034900
1960GO19 J.Phys.Radium 21, 358 (1960) S.Gorodetzky, A.Gallmann, P.Fintz, J.Samuel Excitation Curves for Certain Gamma Rays in the Reaction C12(d, p)C13 NUCLEAR STRUCTURE 13C; measured not abstracted; deduced nuclear properties.
doi: 10.1051/jphysrad:01960002105035800
1960GO25 Nuclear Phys. 18, 286 (1960) S.Gorodetzky, M.Croissiaux, A.Gallmann, P.Fintz, J.Samuel, G.Bassompierre Etude de Quelques Nineaux Excites du 11B par la Reaction 10B(d, p)11B NUCLEAR STRUCTURE 11B; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(60)90405-3
1959AL06 Phys.Rev. 116, 939 (1959) D.E.Alburger, A.Gallmann, D.H.Wilkinson Decay Schemes of C15, N16, and O19
doi: 10.1103/PhysRev.116.939
1959AL83 Phys.Rev.Letters 2, 110 (1959) D.E.Alburger, A.Elwyn, A.Gallmann, J.V.Kane, S.Ofer, R.E.Pixley Search for an 80-msec Activity in Light Nuclei
doi: 10.1103/PhysRevLett.2.110
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