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NSR database version of April 27, 2024.

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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 T_1/2, 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 T_1/2; 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, T_1/2, 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, T_1/2. 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 T_1/2, 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, T_1/2, 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, T_1/2, 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 T_1/2, 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 T_1/2, 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, T_1/2. 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, T_1/2; 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, T_1/2. 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 T_1/2, 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, T_1/2. 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 T_1/2, 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, T_1/2, 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, T_1/2. 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, T_1/2. 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 T_1/2, 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, T_1/2. 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, T_1/2; 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, T_1/2; 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, T_1/2; 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, T_1/2. 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 T_1/2.

doi: 10.1139/p70-201
Citations: PlumX Metrics

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 T_1/2.

doi: 10.1016/0375-9474(70)90149-1
Citations: PlumX Metrics

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 T_1/2, level-width, γ-branching. ¹²C(d, p), E = 3.25 MeV; measured Eγ. ¹³C deduced levels.

doi: 10.1103/PhysRev.185.1242
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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 T_1/2. 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 T_1/2, 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, T_1/2; 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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