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NSR database version of April 11, 2024.

Search: Author = A.Gallmann

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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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1973HE09      Phys.Rev. C7, 1810 (1973)

B.Heusch, A.Gallmann

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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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1970FR10      Nucl.Phys. A156, 305 (1970)

R.M.Freeman, A.Gallmann

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
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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
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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
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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
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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
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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
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1969GA01      Nucl.Phys. A123, 27(1969)

A.Gallmann, F.Hibou, P.Fintz

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1967GA12      Phys.Rev. 164, 1257 (1967)

A.Gallmann, F.Haas, B.Heusch

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0276.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF1191.


1966GA19      Phys.Rev. 151, 735 (1966)

A.Gallmann, F.Haas, N.Balaux

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0274.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0309.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF1046.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0495.


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
Citations: PlumX Metrics


1960GA01      Bull.Am.Phys.Soc. 5, No.1, 19, E11 (1960)

A.Gallmann, J.Kane, R.Pixley

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0377.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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