References quoted in the ENSDF dataset: 29 REFERENCES
225 references found.
Clicking on a keynumber will list datasets that reference the given article.
Phys.Rev. 76, 861 (1949)
L.Seidlitz, E.Bleuler, D.J.Tendam
The Disintegration Energy of Al29
Phys.Rev. 92, 1256 (1953)
R.L.White, C.H.Townes
The Spin of Si29 and Mass Ratios of the Stable Si Isotopes
Phys.Rev. 93, 1428 (1954)
G.A.Williams, D.W.McCall, H.S.Gutowsky
The Nuclear Spin of Si29
Phys.Rev. 116, 1563 (1959)
J.Vorona, J.W.Olness, W.Haeberli, H.W.Lewis
Levels of P29 from Si28(p, p)Si28 and Si28(p, p')Si28
Z.Naturforsch. 15a, 593 (1960)
J.Janecke
The Half Lives of Some Positron Emitters with Superpermitted Transitions
NUCLEAR STRUCTURE 17F, 19Ne, 29P, 35Ar, 31S, 34Cl, 33Cl, 42Sc, 41Sc, 38K, 43Ti, 15O, 13N, 26Al, 25Al, 8Li; measured not abstracted; deduced nuclear properties.
Proc.Phys.Soc.(London) 76, 914 (1960)
A.A.Jaffe, F.de S.Barros, P.D.Forsyth, J.Muto, I.J.Taylor, S.Ramavataram
Some (t, p) Reactions in Light Nuclei
NUCLEAR STRUCTURE 29Al, 12B, 18O, 14C; measured not abstracted; deduced nuclear properties.
doi: 10.1088/0370-1328/76/6/311
Can.J.Phys. 38, 927 (1960)
A.E.Litherland, G.J.McCallum
An Illustration of a Type of Triple Correlation Measurement Which Can Be Easily Interpreted
NUCLEAR STRUCTURE 29Si; measured not abstracted; deduced nuclear properties.
J.Phys.Soc.Japan 15, 760 (1960)
Y.Oda, M.Takeda, N.Takano, T.Yamazaki, C.Hu, K.Kikuchi, S.Kobayashi, K.Matsuda, Y.Nagahara
Elastic and Inelastic Scattering of Protons from N, Ne, Mg, Si, S and A in the Energy Range from 7.6 MeV to 14.2 MeV
NUCLEAR STRUCTURE 24Mg, 32S, 28Si, 40Ar, 20Ne, 14N; measured not abstracted; deduced nuclear properties.
J.Phys.Soc.Japan 15, 1556 (1960)
K.Okano, T.Tabata, K.Fukuda
Lower Excited States in P29 from the Si28(p, γ)P29 Reaction
NUCLEAR STRUCTURE 29P; measured not abstracted; deduced nuclear properties.
Phys.Rev. 122, 920 (1961)
T.A.Belote, E.Kashy, J.R.Risser
Excited States in P29 from the Scattering of Protons by Si28
NUCLEAR STRUCTURE 29P; measured not abstracted; deduced nuclear properties.
Phys.Rev. 123, 568 (1961)
G.J.McCallum
Determination of M1-E2 Mixing Amplitudes in Mg25, Al27, Si29, and P31
NUCLEAR STRUCTURE 25Mg, 27Al, 29Si, 31P; measured not abstracted; deduced nuclear properties.
Nuclear Phys. 35, 472 (1962)
E.C.Booth, K.A.Wright
Nuclear Resonance Scattering of Bremsstrahlung
doi: 10.1016/0029-5582(62)90138-4
Phys.Rev. 127, 947 (1962)
M.W.Brenner, A.M.Hoogenboom, E.Kashy
Nuclear Energy Levels in P29
NUCLEAR STRUCTURE 29P; measured not abstracted; deduced nuclear properties.
Nucl.Phys. 52, 561 (1964)
H.Ejiri, H.Ohmura, Y.Nakajima, K.Horie, Y.Hashimoto, K.Etoh, S.Matsumoto, Y.Nogami
Excited States in 29P by the Reaction 28Si(p, γ)29P
NUCLEAR STRUCTURE 29P; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(64)90716-3
Phys.Letters 13, 148 (1964)
J.C.Hardy, R.I.Verrall
Delayed Protons Following the Decay of S29
NUCLEAR STRUCTURE 29S; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.13.764
Phys.Letters 16, 280 (1965)
T.W.Retz-Schmidt, S.J.Skorka, J.Morgenstern, H.Schmidt
The Width of the 6.379 MeV State in 29Si
NUCLEAR STRUCTURE 29Si; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(65)90851-6
Nucl.Phys. 68, 177(1965)
S.J.Skorka, T.W.Retz-Schmidt, H.Schmidt, J.Morgenstern, D.Evers
Width of the 4.931 MeV Level in Si29
NUCLEAR REACTIONS 29Si(γ, γ) [from 28Si(d, pγ)], E approx 4.9, 6.4 MeV; measured σ. 29Si deduced level-width, T1/2. Natural target.
doi: 10.1016/0029-5582(65)90378-0
Z.Naturforsch. 21a, 980 (1966)
M.Betigeri, R.Bock, H.H.Duhm, S.Martin, R.Stock
Die Reaktionen 30Si(d, p)31Si und 30Si(3He, D)31P
NUCLEAR STRUCTURE 29Si, 31P, 31Si; measured not abstracted; deduced nuclear properties.
Nucl.Phys. 86, 353(1966)
S.G.Buccino, D.S.Gemmell, L.L.Lee, Jr., J.P.Schiffer, A.B.Smith
The (d, n) Reaction on 24Mg and 28Si
NUCLEAR REACTIONS 24Mg, 28Si(d, n), E = 7.0, 9.0, 10.0 MeV; measured σ(En, θ). 25Al, 29P deduced levels, L, J, π, S. Natural targets.
doi: 10.1016/0029-5582(66)90543-8
Yadern.Fiz. 6, 219 (1967); Soviet J.Nucl.Phys. 6, 160 (1968)
O.F.Afonin, A.P.Grinberg, I.K.Lemberg, I.N.Chugunov
Coulomb Excitation of Light and Medium Nuclei at Supra-Barrier Energies
NUCLEAR STRUCTURE 23Na, 27Al, 29Si, 35Cl, 31P, 37Cl, 53Cr, 54Fe, 52Cr, 51V, 45Sc, 50Ti, 49Ti, 48Ti, 47Ti; measured not abstracted; deduced nuclear properties.
Phys.Rev. 157, 967 (1967)
J.A.Becker, L.F.Chase, Jr., R.E.McDonald
Levels of Si29 below 4.1-MeV Excitation Energy
NUCLEAR STRUCTURE 29Si; measured not abstracted; deduced nuclear properties.
Phys.Rev. 163, 1198 (1967)
D.Dehnhard, J.L.Yntema
Neutron Pickup Reactions on Si30
NUCLEAR STRUCTURE 29Si; measured not abstracted; deduced nuclear properties.
Arkiv Fysik 36, 471 (1967)
R.W.Fink, T.H.Braid, A.W.Friedman
Delayed Protons Following He3 Reactions with Oxygen, Silicon, and Sulfur Targets
Phys.Rev. 170, 1046(1968)
S.I.Baker, R.E.Segel
Lifetimes of the First Four Excited States in Si29
NUCLEAR REACTIONS 28Si(d, pγ), E=3 MeV; measured σ(Ep, Eγ), Doppler shift attenuation. 29Si levels deduced T1/2.
Phys.Rev. 167, 1043 (1968)
R.C.Bearse, D.H.Youngblood, J.L.Yntema
Proton Hole States in 29Al, 31P, and 33P
NUCLEAR STRUCTURE 29Al, 33P, 31P; measured not abstracted; deduced nuclear properties.
Phys.Letters 30B, 94 (1969)
P.G.Bizzeti, A.M.Bizzeti-Sona, A.Cambi, P.R.Maurenzig, C.Signorini
Lifetime of the First Excited State in 29P and 29Si
NUCLEAR REACTIONS 28Si(p, γ), E =1.65 MeV; 29Si(p, p'γ), E = 1.748 MeV; measured Doppler shift attenuation. 29P, 29Si levels deduced T1/2.
doi: 10.1016/0370-2693(69)90406-7
Phys.Rev. 187, 1445 (1969)
W.R.Harris, K.Nagatani, D.E.Alburger
Beta Decay of Al29
RADIOACTIVITY 29Al[from 27Al(t, p)]; measured Eγ, Iγ, γγ-coin; deduced β-branching, log ft. 29Si deduced levels, γ-branching.
Phys.Rev. 180, 997 (1969)
A.D.W.Jones
Study of the Low-Lying Excited States of Al29. I. Si30(t, α)Al29 Direct-Reaction Investigation
NUCLEAR REACTIONS 30Si(t, α), E=11.8 MeV; measured σ(Eα, θ). 29Al deduced levels, J, π, L(p), S.
Phys.Rev. 187, 1388 (1969)
A.D.W.Jones, J.A.Becker, R.E.McDonald
Study of the Low-Lying Excited States of Al29 II: Al27(t, pγ)Al29 and Si30(t, αγ)Al29 Angular Correlation Investigation
NUCLEAR REACTIONS 27Al(t, pγ), E=2.8 MeV; 30Si(t, αγ), E=2.5 MeV; measured σ(Ep, Eγ, θ(pγ)), σ(Eα, Eγ, θ(αγ)). 29Al deduced levels, J, π, γ-mixing, γ-branching.
Nucl.Phys. A132, 241 (1969)
D.C.Kean, K.W.Carter, C.J.Piluso, R.H.Spear
Angular Correlation Studies of the Low-Lying Levels of 29Al
NUCLEAR REACTIONS 26Mg(α, pγ), E=10.6, 11.3 MeV; measured σ(Ep, Eγ, θ), Eγ, Iγ. 29Al levels deduced γ-branching, J, delta. Enriched target.
doi: 10.1016/0375-9474(69)90481-3
Phys.Letters 30B, 470 (1969)
B.T.Lawergren, G.C.Neilson, J.L.Honsaker
K = 1/2 and K = 5/2 Components in the Ground State of 27Al
NUCLEAR REACTIONS 25Mg, 27Al(3He, n), E = 5.51, 5.66, 5.95 MeV; measured σ(E;En, θ). 27Al deduced ground-state K-mixing.
doi: 10.1016/0370-2693(69)90174-9
Phys.Rev. 187, 1210 (1969)
L.Meyer-Schutzmeister, D.S.Gemmell, R.E.Holland, F.T.Kuchnir, H.Ohnuma, N.G.Puttaswamy
Study of the Al27(He3, p)Si29 and Al27(He3, pγ)Si29 Reactions
NUCLEAR REACTIONS 27Al(3He, pγ), E=12 MeV; measured σ(Ep, Eγ, θ(p)). 29Si deduced levels, J, π, L, isobaric analog, anti-analog state.
Phys.Rev. 177, 1656(1969)
B.Teitelman, G.M.Temmer
Isospin-Forbidden Compound Nuclear Resonances in 25Al and 29P
NUCLEAR REACTIONS 28Si, 24Mg(p, p), (p, p'), E=5.6-7.4 MeV; measured σ(Ep; Ep', θ). 25Al, 29P deduced resonances, level-width, L(p), isobaric analog, Coulomb energy difference. Enriched 24Mg target.
Phys.Rev. 181, 1580 (1969)
M.J.Wozniak, Jr., R.L.Hershberger, D.J.Donahue
Mean Lives of States in Si29 below 5 MeV
NUCLEAR REACTIONS 28Si(d, pγ), E = 2 MeV; measured σ(Ep, Eγ), Doppler shift attenuation. 29Si levels deduced T1/2 B(E2), quadrupole moment.
Nucl.Phys. A157, 273 (1970)
A.Adams, J.M.Calvert
Proton-Gamma Angular Correlations in the Reactions 26Mg(d, p)27Mg and 28Si(d, p)29Si
NUCLEAR REACTIONS 26Mg(d, pγ), E=4.37, 5.34 MeV; measured σ(E;Ep, Eγ, θ(p), phi(γ)). Enriched target. 27Mg deduced levels. 28Si(d, pγ), E=4.37, 5.26 MeV; measured σ(E;Ep, Eγ, θ(p), phi(γ)). Natural target. 29Si deduced levels, branching ratios.
doi: 10.1016/0375-9474(70)90113-2
Nucl.Phys. A141, 33 (1970)
J.M.Calvert, T.Joy
Some Neutron-Gamma Ray Angular Correlation Studies of 29P
NUCLEAR REACTIONS 28Si(d, nγ), E=3-4 MeV; measured σ(E;En, Eγ, θ(nγ)). 29P levels deduced J, π, branching ratios. Natural target.
doi: 10.1016/0375-9474(70)90294-0
Phys.Rev. C2, 1570 (1970)
J.E.Cummings, D.J.Donahue
Mean Life Measurements in 29P
NUCLEAR REACTIONS 28Si(d, nγ), E=2.93, 3.50 MeV; measured σ(En, Eγ), Doppler shift attenuation. 29P levels deduced T1/2, B(λ), quadrupole moment.
Nucl.Phys. A140, 190 (1970)
P.R.de Kock, J.W.Koen, W.L.Mouton
Lifetime Measurements on 26Mg and 29Si by Doppler Shift Attenuation
NUCLEAR REACTIONS 26Mg, 29Si(p, p'γ), E=2.8-5.5 MeV; measured σ(E;Eγ), Doppler shift attenuation. 26Mg, 29Si deduced levels T1/2.
doi: 10.1016/0375-9474(70)90895-X
Phys.Rev. C2, 1390 (1970)
D.Dehnhard, J.L.Yntema
Study of Energy Levels of 29Si
NUCLEAR REACTIONS 30Si(3He, α), E=12 MeV; measured σ(Eα, θ). 29Si deduced levels, L(n), S.
Nucl.Phys. A158, 393 (1970)
C.Detraz, R.Richter
Study of the T = 3/2 States of 25Mg and 29Si
NUCLEAR REACTIONS 26Mg, 30Si(3He, α), E=15.4 MeV; measured σ(Eα, θ). 25Mg, 29Si T=3/2 deduced levels, L(n), J, π, S. Enriched targets.
doi: 10.1016/0375-9474(70)90191-0
Phys.Rev. C2, 990 (1970)
J.K.Dickens
28-30si(n, xγ) Reactions for 5.3 < E < 9.0 MeV
NUCLEAR REACTIONS 28,29,30Si(n, Xγ), E=5.3-9.0 MeV; measured σ(E;Eγ, θ(γ)). 25Mg, 28Al, 28,29,30Si deduced levels.
Phys.Rev. C1, 1000 (1970)
A.D.W.Jones, J.A.Becker, R.E.McDonald, A.R.Poletti
Beta Decay of Na25 and Al29
RADIOACTIVITY 25Na, 29Al[from 23Na, 27Al(t, p)]; measured Eγ, Iγ; deduced log ft. 25Mg, 29Si deduced γ-branching.
Phys.Rev. C2, 724 (1970)
K.S.Krane, R.M.Steffen
Determination of the E2/M1 Multipole Mixing Ratios of the Gamma Transitions in Cd110
RADIOACTIVITY 110mAg; measured γγ-coin, γγ(θ), Eγ. 110Cd transitions deduced γ-mixing ratios. Ge(Li) detectors.
Nucl.Phys. A158, 43 (1970)
G.P.Lamaze, C.R.Gould, C.E.Moss, N.R.Roberson, D.R.Tilley
An Angular Correlation Study of the Low-Lying Levels of 29P
NUCLEAR REACTIONS 32S(p, αγ), E=12.12, 12.89 MeV; measured σ(Eα, Eγ, θ(αγ)). 29P deduced levels, J, π, γ-branching ratios, γ-mixing ratios. Natural targets.
doi: 10.1016/0375-9474(70)90048-5
Nucl.Phys. A158, 364 (1970)
I.G.Main, N.Dawson, C.K.Davis, G.D.Jones, P.J.Mulhern, V.E.Storizhko, R.D.Symes, M.F.Thomas, P.J.Twin
Rotational Structure in 29Si
NUCLEAR REACTIONS 29Si(p, p'γ), E=6.5, 8.7 MeV; measured σ(Ep', Eγ, θ(p'γ)); 29Si(α, α'γ), E=15.4 MeV; measured σ(Eα', Eγ, θ(α'γ)); 26Mg(α, nγ), E=5.8, 6.3 MeV; measured σ(Eγ, θ(γ)); 29Si levels deduced J, γ-branching ratios, multipole mixing ratios. Enriched targets.
doi: 10.1016/0375-9474(70)90188-0
Nucl.Phys. A147, 81 (1970)
J.E.McQueen, Jr., J.M.Joyce, E.J.Ludwig
The 30Si(3He, α)29Si Reaction at 8.0 and 7.0 MeV
NUCLEAR REACTIONS 30Si(3He, 3He), E = 8.0, 7.0 MeV; measured σ(θ). 30Si(3He, α), E = 6.8 to 8.2 MeV; measured σ(E;Eα, θ). 29Si levels deduced L, S. Enriched target.
doi: 10.1016/0375-9474(70)90511-7
Can.J.Phys. 48, 2683 (1970)
C.F.Monahan, H.C.Evans, J.H.Montague, W.R.Paulson, W.M.Zuk
Transition Rates in 29P
NUCLEAR REACTIONS 28Si(p, γ), E=1-5 MeV; measured Doppler shift attenuation, σ(E;Eγ, θ(γ)). 29P deduced resonances, J, π, γ-branching, γ-mixing. 29P levels deduced T1/2.
Can.J.Phys. 48, 1578 (1970)
P.J.Scanlon, D.Crabtree
Half-Life Measurements on 29P and 33Cl
RADIOACTIVITY 29P, 33Cl; measured T1/2.
Nucl.Phys. A145, 449 (1970)
A.M.J.Spits, A.M.F. Op den Kamp, H.Gruppelaar
Gamma Rays from Thermal-Neutron Capture in Natural and 28Si Enriched Silicon
NUCLEAR REACTIONS 28,29,30Si, 6Li, 14N, 19F, 27Al, 54,56Fe, 207Pb(n, γ), E=thermal; 28Si(n, n'γ), E=fast; measured Eγ, Iγ; deduced Q. 29,30,31Si deduced levels, γ-branching. Natural, 28Si enriched targets, Ge(Li) detector.
doi: 10.1016/0375-9474(70)90435-5
Nucl.Phys. A151, 504 (1970)
R.P.Williams, S.G.Buccino, C.C.Wellborn
Gamma-Ray Transitions in 29P
NUCLEAR REACTIONS 28Si(p, γ), Ep=1.38 MeV; measured σ(Eγ, θ(γ)), Doppler shift attenuation. 29P deduced levels, γ-branching, γ-mixing, J, T1/2, level-width, B(λ).
doi: 10.1016/0375-9474(70)90393-3
Can.J.Phys. 49, 971 (1971)
R.D.Barton, J.S.Wadden, A.L.Carter, H.L.Pai
Lifetime of the 3.163 MeV Level of 35Cl
NUCLEAR REACTIONS 34S(p, γ), E=1.214 MeV; measured γγ-delay. 35Cl level deduced T1/2.
Phys.Rev. C4, 1625 (1971)
T.T.Bardin, J.A.Becker, T.R.Fisher, A.D.W.Jones
Levels of Si29 with Excitation Energy below 6.4 MeV
NUCLEAR REACTIONS 26Mg(α, nγ), E=5-8 MeV; measured σ(E;Eγ, θ(γ)), Doppler shift attenuation. 29Si deduced levels, J, π, T1/2, γ-branching, γ-mixing.
Nucl.Phys. A161, 375 (1971)
J.S.Forster, C.Broude, W.G.Davies
Angular Correlation Measurements of the First Three Excited States in 29P
NUCLEAR REACTIONS 32S(p, αγ), E=14.0 MeV; measured σ(Eα, Eγ, θ(γ), θ(αγ)). 29P deduced levels, γ-branching ratios, J, γ-mixing ratios. Natural target.
doi: 10.1016/0375-9474(71)90375-7
Particles and Nuclei 1, 372 (1971)
R.G.Hirko, R.A.Lindgren, A.J.Howard, J.G.Pronko, M.W.Sachs, D.A.Bromley
Nuclear Structure Studies on 29Al
NUCLEAR REACTIONS 27Al(t, p), E=3.34 MeV; measured σ(Ep, θ). 26Mg(α, pγ), E=13.82, 14 MeV; measured σ(Ep, Eγ, θ(γ), θ(pγ)). 29Al deduced levels, J, π, γ-mixing, γ-branching.
Phys.Rev. C3, 724 (1971)
A.D.W.Jones, J.A.Becker, R.E.McDonald
Study of the Low-Lying Excited States of 29Al. III. Mean Lifetimes and Interpretation
NUCLEAR REACTIONS 27Al(t, pγ), E=2.54 MeV; measured σ(Ep, Eγ), Doppler shift attenuation. 29Al levels deduced J, π, T1/2.
Nucl.Phys. A172, 663 (1971)
D.C.Kocher, P.J.Bjorkholm, W.Haeberli
The Reactions 16O(d, p)17O and 28Si(d, p)29Si Initiated by Vector-Polarized Deuterons
NUCLEAR REACTIONS 16O(polarized d, d); measured polarization parameter iT11(Ed, θ); 16O(polarized d, p)17O, Ed=8 MeV; 28Si(polarized d, p)29Si, Ed=9 MeV; measured polarization parameters iT11(Ed;Ep, θ), cross sections σ(Ed;Ep, θ); deduced J-dependence. 17O, 29Si deduced S. Natural targets.
doi: 10.1016/0375-9474(71)90053-4
Can.J.Phys. 49, 2886 (1971)
A.B.McDonald, T.K.Alexander, O.Hausser, G.T.Ewan
Lifetimes of States in 29Si, 27Al, and 26Mg
NUCLEAR REACTIONS 12C(19F, npγ), E=25 MeV; 12C(19F, αpγ), E=25 MeV; 27Al(35Cl, 35Cl'γ), E=67 MeV; measured recoil distance. 27Al(35Cl, 35Cl'γ), E=67 MeV; measured Doppler shift attenuation. 29Si, 27Al, 26Mg levels deduced T1/2.
Phys.Rev. C4, 1778 (1971)
M.C.Mermaz, C.A.Whitten, Jr., J.W.Champlin, A.J.Howard, D.A.Bromley
Study of the (d, p) Reaction on 28Si, 32S, and 36Ar at E = 18.00 MeV
NUCLEAR REACTIONS 28Si, 32S, 36Ar(d, p), E=18 MeV; measured σ(Ep, θ). 29Si, 33S, 37Ar deduced levels, J, π, L(n), S.
Can.J.Phys. 49, 355 (1971)
R.H.Spear, J.E.Cairns, R.V.Elliott, J.A.Kuehner, A.A.Pilt
Concerning a Possible K = 7/2 Negative Parity Band in 29Si
NUCLEAR REACTIONS 26Mg(α, nγ), E=5.54, 6.30 MeV; measured σ(Eγ;θ(γ)), γ-linear polarization. 29Si levels deduced J, π, γ-mixing.
Nucl.Phys. A173, 286 (1971)
D.M.Stupin, R.A.Ristinen, P.Schwandt
The 28Si(3He, 2p) and 12C(3He, 2p) Reactions at 40 MeV
NUCLEAR REACTIONS 28Si, 12C(3He, 2p), E=40 MeV; measured σ(E(p1), θ(p1), θ(2)), σ(θ); deduced p-p final-state interaction contribution. Natural targets.
doi: 10.1016/0375-9474(71)90346-0
OULNS-71-2, p.24 (1971)
K.Sugimoto, A.Mizobuchi, T.Minamisono, I.Tanihata
Precision Measurement of β-Decay Lifetime of 25Al
RADIOACTIVITY 25Al; measured T1/2.
Aust.J.Phys. 24, 37 (1971)
W.M.Zuk, J.L.Black, W.F.Davidson
A Search for the 3446 keV Level in 29P via the 28Si(p, γ)29P Reaction
NUCLEAR REACTIONS 28Si(p, γ), E=350-1450 keV; measured σ(E;Eγ), γγ-coin. 29P resonances deduced level-width.
Phys.Rev. C5, 1351 (1972)
T.T.Bardin, J.A.Becker, T.R.Fisher
Radiative Decay of the P29 8.38-MeV Level
NUCLEAR REACTIONS 28Si(p, γ), E=5.83 MeV; measured σ(Eγ, θ(γ)). 29P deduced levels, J, π, γ-mixing, γ-branching. Ge(Li) detectors.
J.Phys.(London) A5, 596 (1972)
D.C.Bailey, P.E.Carr, J.L.Durell, L.L.Green, M.W.Greene, A.N.James, J.F.Sharpey-Schafer, D.A.Viggars
A Study of the Principal Decay Modes and Lifetimes of Levels in 29Si below 7.2 MeV
NUCLEAR REACTIONS 26Mg(α, nγ), E=5.0, 6.75, 8.0, 9.25 MeV; measured DSA, Eγ, Iγ. 29Si deduced levels, T1/2, γ-branching.
doi: 10.1088/0305-4470/5/4/016
J.Phys.(London), A5, 1624 (1972)
F.El-Bedewi, M.Shalaby
Study of Energy Levels of 29Si via Deuteron Stripping
NUCLEAR REACTIONS 28Si(d, p), E=10 MeV; measured σ(Ep, θ), Q. 29Si deduced levels, J, π, S.
J.Phys.(London) A6, 1011 (1973)
D.G.Barnes, J.M.Calvert, T.Joy
Studies of Levels in 29P up to 4.76 MeV Using the 28Si(p, γ)29P Reaction
NUCLEAR REACTIONS 28Si(p, γ), E=0.72, 1.381, 1.652, 2.086 MeV; measured DSA, γ(θ). 29P levels, resonances deduced J, π, T1/2, level-width, γ-branching, γ-mixing.
doi: 10.1088/0305-4470/6/7/021
Z.Phys. 261, 351 (1973)
P.Betz, H.Ropke
Search for High-Spin States in 29Si Using a Neutron Time-of-Flight Spectrometer
NUCLEAR REACTIONS 26Mg(α, nγ), E=11, 12, 13, 14 MeV; measured nγ-coin, Eγ, Iγ, DSA. 29Si deduced levels, J, π, T1/2.
Phys.Rev. C8, 1331 (1973)
D.R.Goosman, C.N.Davids, D.E.Alburger
Mass and β Decay of the New Isotope 29Mg; Systematics of Masses of T(z) = 5/2 Nuclides in the 2s-1d Shell
RADIOACTIVITY 29Mg; measured T1/2, Eγ, Iγ, Eβ, βγ-coin. Deduced log ft, Q, J, π. 29Al deduced levels, γ-branching.
NUCLEAR REACTIONS 27Al(t, pγ), E=3 MeV; measured Eγ. 29Al deduced levels.
J.Phys.Soc.Jap. 34, 848 (1973)
I.Tanihata, T.Minamisono, A.Mizobuchi, K.Sugimoto
Precision Lifetimes of Positron Emitters, 25Al, 29P, 33Cl and 41Sc, and ft Values of Mirror β Decays
RADIOACTIVITY 25Al, 29P, 33Cl, 41Sc; measured T1/2. Deduced log ft.
J.Phys.(London) A6, L67 (1973)
D.A.Viggars, P.A.Butler, P.E.Carr, L.L.Gadeken, A.N.James, P.J.Nolan, J.F.Sharpey-Schafer
High Spin Negative Parity States in 29Si Associated with Oblate Deformation
NUCLEAR REACTIONS 26Mg(α, nγ), E=8.5, 10.0, 10.5, 11 MeV; measured DSA, γ(θ), polarization(γ). 29Si levels deduced J, π, T1/2.
doi: 10.1088/0305-4470/6/6/001
Phys.Rev.Lett. 33, 846 (1974)
N.Anantaraman, J.P.Draayer, H.E.Gove, J.P.Trentelman
Shapes of (6Li, d) Angular Distributions as Signatures of Rotational Bands in 29Si
NUCLEAR REACTIONS 24,25Mg(6Li, d), E=36 MeV; measured σ(Ed, θ). 29,28Si levels deduced L.
doi: 10.1103/PhysRevLett.33.846
Nucl.Phys. A218, 213 (1974)
F.A.Beck, T.Byrski, G.Costa, P.Engelstein
Lifetime Measurements in 29Al
NUCLEAR REACTIONS 26Mg(α, p), E=7-11 MeV; 27Al(t, p), E=2.5, 2.8 MeV; measured DSA, recoil distance. 29Al levels deduced T1/2. Isotopic, natural targets.
doi: 10.1016/0375-9474(74)90032-3
Nucl.Phys. A223, 125 (1974)
T.Byrski, F.A.Beck, P.Engelstein, M.Forterre, A.Knipper
Etude de la Structure du Noyau 29P
NUCLEAR REACTIONS 28Si(p, γ), E=0.35-2.65 MeV; 28Si(d, nγ), E=2.8, 5.1 MeV; measured Eγ, Iγ, dσ(θ(γ)), γγ(θ), Doppler shift attenuation. 29P levels, deduced E(X), J, γ-branching, γ-mixing, T1/2. Enriched target.
doi: 10.1016/0375-9474(74)90281-4
Phys.Rev. C10, 991 (1974)
N.A.Detorie, J.D.Goss, A.A.Rollefson, C.P.Browne
States in 29P via the 32S(p, α)29P Reaction
NUCLEAR REACTIONS 32S(p, α), E=15, 16 MeV; measured σ(Eα, θ). 29P deduced levels, level-width.
Nucl.Phys. A230, 285 (1974)
P.Ekstrom, J.Tillman
Study of 29Al with the 26Mg(α, pγ)29Al Reaction
NUCLEAR REACTIONS 26Mg(α, pγ), E=14.2, 16.5, 18.0 MeV; measured pγ(θ), γγ-coin, DSA, σ(Ep, Eγ). 29Al levels deduced E(X), T1/2, J, π, γ-branchings, mixing ratios, S. Enriched target.
doi: 10.1016/0375-9474(74)90308-X
Phys.Rev. C10, 1739 (1974)
N.L.Gearhart, H.J.Hausman, J.F.Morgan, G.A.Norton, N.Tsoupas
Spectroscopy of 29P via the 28Si(p, p'γ) Reaction
NUCLEAR REACTIONS 28Si(p, p), (p, p'γ), E=3.1-5.7 MeV; measured σ(E), p'γ(θ). 29P levels deduced J, π.
Nucl.Phys. A234, 167 (1974)
K.D.Hildenbrand, R.Bock, H.G.Bohlen, P.Braun-Munzinger, D.Fick, C.K.Gelbke, U.Weiss, W.Weiss
Elastic Neutron Transfer in the Scattering of Si Isotopes
NUCLEAR REACTIONS 29,30Si(28Si, 28Si), E=65, 70 MeV; 30Si(28Si, 29Si), E=70 MeV; measured σ(θ). 29,30Si levels deduced S. Enriched targets.
doi: 10.1016/0375-9474(74)90385-6
Z.Phys. 271, 139 (1974)
P.Leleux, P.C.Macq, J.P.Meulders, C.Pirart
The (τ, d), (d, p) and (d, n) Reactions on 28Si
NUCLEAR REACTIONS 28Si(3He, 3He), (3He, d), E=35.3 MeV; measured σ(θ), σ(Ed, θ). 29P levels deduced S. 28Si(d, n), (d, p), (d, d), E=13.5 MeV; measured σ(En, θ), σ(Ep, θ), σ(θ). 29Si deduced analog states, S.
Z.Phys. 269, 353 (1974)
H.Mackh, G.Mairle, G.J.Wagner
Proton Shell Structure of Mass 28-32 Nuclei
NUCLEAR REACTIONS 28,29,30Si, 31P, 32S(d, 3He), E=52 MeV; measured σ(E(3He), θ). 27,28,29Al, 30Si, 31P levels deduced L, S.
Bull.Am.Phys.Soc. 19, AD12 (1974)
W.S.McEver, L.Dries, J.Regner, T.R.Donoghue
The Elastic Scattering of Polarized Protons by 28Si from 2.0 to 3.8 MeV
NUCLEAR REACTIONS 28Si(p, p), E=2-3.8 MeV; measured proton spectra. 29P; deduced energies, J, π, resonance parameters.
Phys.Rev. C9, 1851 (1974)
L.R.Medsker, H.E.Jackson, J.L.Yntema
Unbound States in 29Si with the 28Si(d, p) Reaction
NUCLEAR REACTIONS 28Si(d, p), E=16 MeV; measured σ(Ep, θ); 29Si deduced levels, n-width, L(n).
Phys.Rev. C10, 1181 (1974)
E.Roeckl, P.F.Dittner, C.Detraz, R.Klapisch, C.Thibault, C.Rigaud
Decay Properties of the Neutron-Rich Isotopes, 11Li and 27-31Na
RADIOACTIVITY 9,11Li, 27,28,29,30,31Na, 29,30Mg; measured Eγ, Iγ, T1/2, delayed neutrons, βγ-coin, Eβ. 26Na measured Eβ. 26,27,28,29Na deduced Qβ. 28Na level deduced J, π. 27Mg; calculated β-branching ratio, log ft.
Phys.Rev.Lett. 33, 1343 (1974)
D.K.Scott, B.G.Harvey, D.L.Hendrie, L.Kraus, C.F.Maguire, J.Mahoney, Y.Terrien, K.Yagi
Spectroscopy of Exotic Nuclei Using Heavy-Ion Transfer Reactions
NUCLEAR REACTIONS 26Mg(11B, 11C), (11B, 13N), (11B, 8B), 28Si(11B, 8B), E=86 MeV; measured σ; deduced Q. 26Mg deduced mass excess.
doi: 10.1103/PhysRevLett.33.1343
J.Phys.(London) A7, 360 (1974)
D.A.Viggars, P.A.Butler, P.E.Carr, L.L.Gadeken, L.L.Green, A.N.James, P.J.Nolan, J.F.Sharpey-Schafer
Angular Correlation Measurements on Levels in 29Si Above 5 MeV Excitation
NUCLEAR REACTIONS 26Mg(α, nγ); measured σ(Eγ, θ), DSA, γ-polarization(linear). 29Si deduced levels, T1/2, γ-branching, γ-mixing, J, π.
doi: 10.1088/0305-4470/7/3/007
J.Phys.(Paris) 36, 913 (1975)
M.M.Aleonard, P.Hubert, L.Sarger, P.Mennrath
Proprietes des Etats E(x) = 3447 et 4642 keV du 29P
NUCLEAR REACTIONS 28Si(p, γ), E= < 2 MeV; measured σ(E, Eγ, θ), γγ(θ), γ(t). 29P deduced resonances, J, π, Γ, δ, M(λ), T1/2.
Phys.Rev.Lett. 35, 1131 (1975)
N.Anantaraman, C.L.Bennett, J.P.Draayer, H.W.Fulbright, H.E.Gove, J.Toke
Systematics of Ground-State α-Particle Spectroscopic Strengths for sd- and fp-Shell Nuclei
NUCLEAR REACTIONS 16,18O, 20,21,22Ne, 28Si, 32S, 36Ar, 40,42,44,48Ca, 50Ti(6Li, d), E=32 MeV; 24,25Mg(6Li, d), E=36 MeV; 36Ar, 50,52Cr, 54,56Fe, 58,60,62Ni(6Li, d), E=28 MeV; measured σ; deduced Sα.
doi: 10.1103/PhysRevLett.35.1131
Phys.Rev. C12, 563 (1975)
G.Azuelos, J.E.Kitching
Half-Lives of Some T = 1/2 Mirror Decays
RADIOACTIVITY 11C, 19Ne, 21Na, 23Mg, 25,26Al, 27Si, 29P; measured T1/2. 11C, 19Ne, 21Na, 23Mg, 25Al, 27Si, 29P; calculated log ft.
Z.Phys. A273, 251 (1975)
W.R.Coker
Comments on 'The (3He, d) Reaction on 28Si'
NUCLEAR REACTIONS 28Si(3He, d), E=18-40 MeV; analyzed data; deduced inconsistencies in previous analyses. 29P levels deduced S.
Nucl.Phys. A241, 285 (1975)
R.C.Haight, I.D.Proctor, H.F.Lutz, W.Bartolini
The 30Si(p, d)29Si and 30Si(p, t)28Si Reactions at 27 MeV
NUCLEAR REACTIONS 30Si(p, d), 30Si(p, t), E=27 MeV; measured σ(Ed, θ), σ(Et, θ). 29Si deduced levels, J, π, S. 28Si deduced levels, L, π, enhancement ratios. Enriched target.
doi: 10.1016/0375-9474(75)90318-8
Yad.Fiz. 22, 886 (1975); Sov.J.Nucl.Phys. 22, 460 (1975)
K.V.Karadzhev, I.B.Mazurov, V.I.Manko, A.N.Nersesyan
Excited States of the 29P Nucleus
NUCLEAR REACTIONS 28Si(p, p'), (p, p'γ), (p, γ), E=4.97, 5.30 MeV; measured σ(E). 29P deduced resonances, Γ.
Nucl.Phys. A246, 402 (1975)
R.J.Peterson, R.A.Ristinen
The (3He, d) Reaction on 24Mg and 28Si at 38.5 MeV
NUCLEAR REACTIONS 24Mg, 28Si(3He, d), E=38.5 MeV; measured σ(Ed, θ). 25Al, 29P levels deduced S. DWBA, CCBA calculations. Enriched targets.
doi: 10.1016/0375-9474(75)90655-7
Phys.Lett. 59B, 333 (1975)
K.K.Seth, A.Saha, H.Nann, B.H.Wildenthal
Structure of Positive Parity States in 29P and Two-Step Processes in (p, t) Reactions
NUCLEAR REACTIONS 30Si, 31P(p, t), E=40 MeV; measured σ(Et, θ). 29P, 28Si deduced levels, L.
doi: 10.1016/0370-2693(75)90085-4
Nucl.Phys. A242, 345 (1975)
I.Tserruya, W.Bohne, P.Braun-Munzinger, C.K.Gelbke, W.Grochulski, H.L.Harney, J.Kuzminski
Transfer Reactions Induced by 16O on 29,30Si
NUCLEAR REACTIONS 28,29,30Si(16O, 16O), 29,30Si(16O, 15N), 29Si(16O, 15O), 29,30Si(16O, 17O), 30Si(16O, 14C), 30Si(16O, 18O), E(lab)=73.5 MeV; measured σ(θ). 28,29,30Si, 30,31P, 32S levels deduced S. Recoil DWBA analysis. Enriched targets.
doi: 10.1016/0375-9474(75)90054-8
Phys.Rev. C11, 1111 (1975)
J.R.Williams, R.O.Nelson, C.R.Gould, D.R.Tilley
Gamma Ray Linear Polarization Measurements for 29Al
NUCLEAR REACTIONS 26Mg(α, p), E=11.26 MeV; measured linear polarization, pγ-coin. 29Al levels deduced J, π. Enriched target.
Phys.Lett. 63B, 248 (1976)
G.Baur, H.H.Wolter
Sequential Transfer Mechanism in the Elastic Scattering of Nearly Identical Heavy Ions
NUCLEAR REACTIONS 30Si(28Si, 28Si), (28Si, 29Si), E=70 MeV; calculated σ(θ).
doi: 10.1016/0370-2693(76)90255-0
Phys.Rev. C13, 1792 (1976)
F.A.Beck, T.Byrski, A.Knipper, J.P.Vivien
Angular Correlation and Gamma Ray Linear Polarization Measurements in 29Al
NUCLEAR REACTIONS 26Mg(α, pγ), E=14.2 MeV; measured pγ(θ), Eγ, Iγ, linear polarization. 29Al deduced levels, J, π, δ, γ-branching. Enriched target. Ge(Li) Compton polarimeter.
Phys.Rev. C13, 80 (1976)
W.W.Dykoski, D.Dehnhard
Single Proton Transfer to 29,30P States
NUCLEAR REACTIONS 28,29,30Si(3He, 3He), E=25 MeV; measured σ(θ); deduced optical model parameters. 28,29Si(3He, d), E=25 MeV; measured σ(Ed, θ). 29,30P deduced levels, J, π, T, S, L. Enriched target.
Nucl.Phys. A274, 1 (1976); Erratum Nucl.Phys. A279, 532 (1977)
P.G.Ikossi, T.B.Clegg, W.W.Jacobs, E.J.Ludwig, W.J.Thompson
Isospin-Forbidden T=3/2 Resonances in 25Al, 29P and 33Cl, and the Systematics of Isospin Mixing
NUCLEAR REACTIONS 24Mg(p, p), E=5.65-6.25 MeV; 32S(polarized p, p), E=3-3.8 MeV; 28Si(polarized p, p), E=5.6-5.9 MeV; measured σ(E, θ), A(E, θ); deduced optical model parameters. 33Cl, 29P, 25Al, 21Na deduced resonance parameters, reduced widths. Enriched targts, polarized, unpolarized beams.
doi: 10.1016/0375-9474(76)90223-2
Nucl.Phys. A270, 164 (1976)
M.J.Kenny, B.J.Allen, J.W.Boldeman, A.M.R.Joye
Resonance Neutron Capture in Silicon
NUCLEAR REACTIONS 28,29Si(n, γ), E=31.7, 38.8, 55.9, 67.7 keV; measured σ(E, Eγ). 29,30Si deduced resonances, Γγ. Natural target.
doi: 10.1016/0375-9474(76)90132-9
Nucl.Phys. A265, 517 (1976)
W.R.McMurray, T.W.Conlon, B.W.Hooton, M.Ivanovich
The Transfer Reactions Induced by 38 MeV 19F Ions on 27Al
NUCLEAR REACTIONS 27Al(19F, 20Ne), (19F, 18O), (19F, 18F), (19F, 17O), 27Al(19F, 17F), (19F, 16O), (19F, 15N), E=38 MeV; measured σ(θ). Discussed optimum Q-values, yields, single-, multi-nucleon transfer, DWBA analysis. 28Si, 26,28Al levels deduced S.
doi: 10.1016/0375-9474(76)90559-5
Phys.Rev. C13, 1367 (1976)
L.Ray, W.R.Coker
Multistep Inelastic Processes in the Reaction 28Si(3He, d)29P Leading to Bound and Unbound States
NUCLEAR REACTIONS 28Si(3He, d), E=20, 35.3, 40 MeV; calculated σ(Ed, θ); deduced multistep inelastic contributions. 29P levels deduced S. DWBA, CCBA.
Phys.Rev. C14, 775 (1976)
C.M.Teodorescu, P.Viatte, S.Micek, R.Muller, J.Lang, J.Unternahrer, L.Jarczyk
Particle Unbound States in 29Si and 29P by the Reaction 28Si(d, pn)
NUCLEAR REACTIONS 28Si(d, np), E=11 MeV; measured σ(Ep, θ(p), θn). 29Si deduced resonances. 29P deduced resonances, J, π, Γ. DWBA analysis.
Phys.Rev. C13, 510 (1976)
N.Tsoupas, H.J.Hausman, N.L.Gearhart, G.H.Terry
Partial Decay Widths of Resonances in 29P
NUCLEAR REACTIONS 28Si(p, p'γ), E=3.0-5.2 MeV; measured σ(E, θ), pγ-coin. 29P deduced resonances, Γ, J, π.
J.Phys.(London), G3, 681 (1977)
S.W.Brain, A.Johnston, W.A.Gillespie, E.W.Lees, R.P.Singhal
Inelastic Electron Scattering from 29Si
NUCLEAR REACTIONS 29Si(e, e'), E=63-117 MeV; measured σ(E;θ). 29Si deduced levels, B(λ). Enriched target, resolution=0.16%, DWBA analysis.
J.Phys.Soc.Jap. 43, 755 (1977)
K.Koyama, N.Nakanishi, S.Takeda, S.Yamada, H.Sakaguchi, M.Nakamura, S.Takeuchi, H.Ohnuma
(3He, d) Stripping to Bound and Unbound States in 29P
NUCLEAR REACTIONS 28Si(3He, d), (3He, 3He), E=29.3 MeV; measured σ(θ). 29P levels deduced S. DWBA, CCBA analyses.
Nucl.Phys. A293, 425 (1977)
D.Schwalm, E.K.Warburton, J.W.Olness
Coulomb Excitation of sd Shell Nuclei: A Self-Contained Set of B(E2) Values and Lifetime Measurements
NUCLEAR REACTIONS 24,25,26Mg, 27Al(28Si, 28Si'), E=39.5-42 MeV; 24,25,26Mg(29Si, 29Si'), E=40.5 MeV; 24,25,26Mg, 27Al(31P, 31P'), E=44-46 MeV; 20,21,22Ne, 23Na, 24,25,26Mg, 28,29,30Si(32S, 32S'), E=41.3-51 MeV; 24,25,26Mg(33S, 33S'), E=49 MeV; 24,25,26Mg, 28,29,30Si(34S, 34S'), E=49-52.5 MeV; 23Na, 27Al(35Cl, 35Cl'), E=53-56 MeV; 24,25,26Mg, 27Al(37Cl, 37Cl'), E=53-65 MeV; measured σ(Eγ), DSA, Coulomb excitation. 20,21,22Ne, 23Na, 24,25,26Mg, 27Al, 28,29,30Si, 31P, 32,33,34S, 35,37Cl levels deduced B(E2), T1/2, quadrupole moment. Natural, enriched targets.
doi: 10.1016/0375-9474(77)90108-7
Atomkernenergie 31, 163 (1978)
A.T.Baranik, I.Bondouk, H.Sharaf
An Investigation of the Si28(d, p)Si29 Reaction in the Deuteron Energy Range 1.0 to 2.5 MeV
NUCLEAR REACTIONS 28Si(d, p), E=1.0-2.5 MeV; measured σ(E, θ). 29Si levels deduced L, S. Hauser-Feshbach, DWBA theory.
Nucl.Phys. A310, 1 (1978)
P.M.Endt, C.van der Leun
Energy Levels of A = 21-44
COMPILATION A=21-44; compiled, evaluated structure data.
doi: 10.1016/0375-9474(78)90611-5
Phys.Rev. C18, 1100 (1978)
S.M.Grimes, C.H.Poppe, C.Wong, B.J.Dalton
Spin Cutoff Parameters for 28Si, 29Si, and 30P: Comparison of Measurements with Spectral Distribution Calculations
NUCLEAR REACTIONS 25,26Mg, 27Al(α, n), E=10-18 MeV; measured σ(En, θ); deduced spin cutoff parameters for 28,29Si, 30P. Natural, enriched targets.
Phys.Rev. C18, 2342 (1978)
G.Huber, F.Touchard, S.Buttgenbach, C.Thibault, R.Klapisch, H.T.Duong, S.Liberman, J.Pinard, J.L.Vialle, P.Juncar, P.Jacquinot
Spins, Magnetic Moments, and Isotope Shifts of 21-31Na by High Resolution Laser Spectroscopy of the Atomic D1 Line
NUCLEAR MOMENTS 21,22,24,25,26,27,28,29,30,31Na [from U(p, X), E=20 GeV]; measured J, hfs, a, isotope shift.
Phys.Rev. C17, 1256 (1978)
A.Spadafora, H.T.Fortune
Analysis of 28Si(3He, d)29P
NUCLEAR REACTIONS 28Si(3He, d), E=25.0 MeV; measured nothing, reanalyzed data. 29P levels deduced S.
J.Phys.Soc.Jpn. 45, 367 (1978)
Y.Toba, H.Sakaguchi, A.Goto, F.Ohtani, N.Nakanishi, N.Kishida, M.Yasue, T.Hasegawa
Proton Inelastic Scattering on 28,29,30Si and Blocking Effect in the Core-Excitation of 29Si
NUCLEAR REACTIONS 28,29,30Si(p, p), (p, p'), E=51.9 MeV; measured σ(θ). 28,29,30Si deduced β2. Optical model, DWBA analyses.
Phys.Rev. C19, 164 (1979)
C.Detraz, D.Guillemaud, G.Huber, R.Klapisch, M.Langevin, F.Naulin, C.Thibault, L.C.Carraz, F.Touchard
Beta Decay of 27-32Na and their Descendants
RADIOACTIVITY 27,28,29,30,31,32Na, 29,30,31Mg, 31Al [from U(p, X), E=24 GeV]; measured T1/2, Eγ, βγ-coin; deduced Iγ, Iβ, delayed-neutron branching ratios. Mass-spectroscopy techniques.
Z.Phys. A289, 229 (1979)
A.Lindholm, L.Nilsson, I.Bergqvist, N.Olsson
Evidence for Neutron Capture Through Doorway States in 29Si
NUCLEAR REACTIONS 28Si(n, γ), E=2.7-6.2 MeV; measured σ(E); deduced possible evidence for doorway. Comparison with theory.
Nucl.Phys. A324, 1 (1979)
F.Terrasi, A.Brondi, P.Cuzzocrea, R.Moro, M.Romano
Proton Resonant and Direct Capture on 28Si
NUCLEAR REACTIONS 28Si(p, γ), E=1.3-2.3 MeV; measured σ(E), Iγ, Iγ(θ). 29P levels deduced γ branchings, strengths, S. Enriched, natural targets.
doi: 10.1016/0375-9474(79)90072-1
Phys.Rev. C19, 177 (1979)
D.J.Vieira, R.A.Gough, J.Cerny
β-Delayed Proton Decay of 29S
RADIOACTIVITY 29S [from 28Si(3He, 2n), E=32 MeV]; measured β-delayed protons, T1/2. 29P deduced levels, IAS-proton decay, log ft. Comparison with shell model.
Univ.Wash.Nucl.Phys.Lab.Ann.Rept., p.64 (1980)
E.G.Adelberger, C.D.Hoyle, P.G.Ikossi
Higher T=3/2 States in 29P and 25Al
NUCLEAR REACTIONS 24Mg, 28Si(p, p), (p, p'), E<8 MeV; measured reaction products. 25Al, 29P; deduced level energy, J, π.
Univ.Wash.Nucl.Phys.Lab.Ann.Rept., p.40 (1980)
E.G.Adelberger, C.D.Hoyle, P.G.Ikossi, K.A.Snover
Spectroscopy of 29P and the Giant Gamow-Teller Resonance in the β+ Decay of 29S
NUCLEAR REACTIONS 28Si(p, p), E=2.6, 7.9 MeV; measured reaction products. 29P; deduced σ, energy levels, J, π.
RADIOACTIVITY 29S(β+); measured decay products; deduced energy distribution of of Gamow-Teller strength, energy levels, J, π.
Phys.Rev. C21, 2227 (1980)
L.C.Bland, H.T.Fortune, O.K.Gorpinich, Y.S.Stryuk, V.N.Shcherbin, V.V.Tokarevski
Reaction 27Al(α, d)29Si at 27.2 MeV
NUCLEAR REACTIONS 27Al(α, d), E=27.2 MeV; measured σ(Ed, θ). 29Si levels deduced L. DWBA analysis, microscopic, macroscopic form factors.
Nucl.Phys. A339, 285 (1980)
H.Clement, R.N.Boyd, C.R.Gould, T.B.Clegg
Study of the Structure of the Low-Lying Levels of 29Si via the 28Si(d, pγ) Reaction and Multi-Step Reaction Calculations
NUCLEAR REACTIONS 28Si(polarized d, pγ), E=7.6 MeV; measured pγ(θ). DWBA, CCBA calculations.
doi: 10.1016/0375-9474(80)90094-9
Phys.Rev. C21, 844 (1980)
E.Fabrici, S.Micheletti, M.Pignanelli, F.G.Resmini, R.De Leo, G.D'Erasmo, A.Pantaleo
Proton Elastic Scattering on Light Nuclei. II. Nuclear Structure Effects
NUCLEAR REACTIONS 9Be, 10,11B, 12,13C, 14,15N, 16,17,18O, 19F, 20,22Ne, 23Na, 24,25,26Mg, 27Al, 28,29,30Si, 31P, 32,34S, 35,37Cl, 40Ar, 39,41K, 40,42,43,44,48Ca, 45Sc, 46,47,48,50Ti, 51V, 50,52,53,54Cr, 55Mn, 54,56,58Fe, 59Co, 58,60,61,62,64Ni, 63,65Cu, 64,66,67,68,70Zn(p, p), (p, p'), E=35.2 MeV; 23Na, 31P, 39K, 45Sc, 51V, 50,53,54Cr, 62,64Ni(p, p), (p, p'), E=29.7 MeV; measured σ(θ); deduced optical-model parameters. 9Be, 10,11B, 12C, 14,15N, 16,17,18O, 19F, 20,22Ne, 23Na, 24,25,26Mg, 27Al, 28,29,30Si, 31P, 32,34S, 35,37Cl, 40Ar, 39,41K, 40,42,43,44,48Ca, 45Sc, 46,47,48,50Ti, 51V, 50,52,53,54Cr, 55Mn, 54,56,58Fe, 59Co, 58,60,61,62,64Ni, 63,65Cu, 64,66,67,68,70Zn level deduced β2. Optical-model, coupled-channel analyses.
Izv.Akad.Nauk SSSR, Ser.Fiz. 44, 2402 (1980)
O.K.Gorpinich, Yu.S.Stryuk, V.V.Tokarevsky, V.N.Scherin, L.Blend, T.Fortune
Comparison of Cluster and Microscopic Description of the (α, d) Reaction on 27Al
NUCLEAR REACTIONS 27Al(α, d), E=27.2 MeV; measured σ(θ). 29Si levels deduced L, S. Microscopic, macroscopic DWBA analysis.
Phys.Lett. B94, 319 (1980)
W.W.Jacobs, A.G.Drentje, P.H.Pile, P.P.Singh, T.P.Sjoreen, S.E.Vigdor
Comparison of (d, p) and (p, π+) Reactions on 28Si at Similar Momentum Transfer
NUCLEAR REACTIONS 28Si(d, p), E=76 MeV; 28Si(p, π+), E=191 MeV; measured σ(θ, Ep), σ(θ, E(π+)); deduced differences in reaction processes. 12,13C levels deduced single neutron wave function components.
doi: 10.1016/0370-2693(80)90887-4
Acta Phys.Pol. B11, 641 (1980)
L.Jarczyk, B.Kamys, K.Seliger, Z.Wrobel, J.Lang, R.Muller, C.M.Schweizer-Teodorescu
Investigation of Nucleon-Unbound States in 29Si and 29P by the Reaction 28Si(d, pn)
NUCLEAR REACTIONS 28Si(d, p), (d, n), E=11 MeV; measured σ(θp, θn, En), σ(θn, θp, Ep), σ(θp, θn). 29Si, 29P deduced resonances, J, π, Γ. DWBA analysis, stripping to unbound states.
Nucl.Phys. A334, 269 (1980)
S.Joly, G.Grenier, J.Voignier, J.W.Boldeman
Resonance Neutron Capture Spectroscopy in 28Si
NUCLEAR REACTIONS 28Si(n, γ), E=565, 813 keV; measured σ(E, Eγ). 29Si resonances deduced Γγ. Natural target. Valence, shell models.
doi: 10.1016/0375-9474(80)90068-8
Proc.Intern.Conf.Atomic Masses and Fundamental Constants, 6th, East Lansing (1979), J.A.Nolen, Jr., W.Benenson, Eds., Plenum Press, New York, p.25 (1980)
R.C.Pardo
Masses of Medium Weight Nuclei by Transfer Reactions
NUCLEAR REACTIONS 92Mo, 106Cd, 112Sn, 144Sm, 70Ge, 90Zr, 24Mg, 32S, 40Ca(3He, 6He), E=70 MeV; 144Sm(12C, 9Be), (12C, 10Be), 23Na, 31P(p, t), (p, 3He), E=45 MeV; E not given; measured spectra. 21Mg, 21Na, 29Si, 37Ca deduced levels. 67Ge, 87Zr, 89Mo, 103Cd, 109Sn, 144Sm deduced mass excess, Q-value.
Nucl.Phys. A349, 513 (1980)
D.E.C.Scherpenzeel, G.A.P.Engelbertink, H.J.M.Aarts, C.J.Van Der Poel, H.F.R.Arciszewski
Coincident High-Velocity DSA Lifetime Measurements on Excited States of Si Isotopes and Stopping Power Investigations
NUCLEAR REACTIONS 4He(28Si, αγ), E=53 MeV; 2H(28Si, pγ), E=29, 33 MeV; 3H(28Si, pγ), E=33 MeV; measured αγ-, pγ-coin, DSA; deduced electronic stopping power for Si in Mg. 28,29,30Si levels deduced T1/2.
doi: 10.1016/0375-9474(80)90304-8
Nucl.Phys. A342, 1 (1980)
J.van Driel, R.Kamermans, R.J.de Meijer, A.E.L.Dieperink
Investigation of the (3He, 2He) Reaction; Reaction Mechanism and Application to the Reaction on 28Si
NUCLEAR REACTIONS 28Si(3He, 2p), E=52 MeV; measured σ(Ep1, Ep2, θ). 29Si deduced levels, J, π, L, S. DWBA analysis, normalization constant, optical model. Natural target.
doi: 10.1016/0375-9474(80)90503-5
Phys.Rev. C22, 374 (1980)
K.E.Whitner, C.F.Williamson, B.E.Norum, S.Kowalski
Inelastic Electron Scattering from 29Si
NUCLEAR REACTIONS 28,29Si(e, e'), E=126-293 MeV; measured form factors. 29Si levels deduced configurations. PWBA analysis, particle-phonon coupling.
Phys.Rev. C22, 1696 (1980)
H.S.Wilson, R.W.Kavanagh, F.M.Mann
Gamow-Teller Transitions in Some Intermediate-Mass Nuclei
RADIOACTIVITY 14O, 21Na, 25Al, 26Si, 29,30P, 30,31S, 33,34mCl, 35Ar, 38Ca, 41Sc measured Iγ; deduced log ft. 26Si, 29P, 30,31S, 34mCl, 38Ca; measured T1/2. Shell model calculations, allowed Gamow-Teller transitions.
Yad.Fiz. 33, 294 (1981)
T.L.Belyaeva, N.S.Zelenskaya, L.Z.Ismail, V.M.Lebedev, A.V.Spassky, I.B.Teplov
A Possible Description of the Angular and Energy Dependences of Reactions with α Particles on 12C and 27Al Nuclei in the l-Dependent Potential Model
NUCLEAR REACTIONS 12C(α, α), (α, p), E=15-25 MeV; 27Al(α, α), (α, p), (α, d), (α, t), E=18-25 MeV; measured σ(θ, E). Exchange processes, l-dependent optical model analysis.
Nucl.Phys. A366, 449 (1981)
M.Langevin, C.Detraz, D.Guillemaud, F.Naulin, M.Epherre, R.Klapisch, S.K.T.Mark, M.De Saint Simon, C.Thibault, F.Touchard
β-Delayed Charged Particles from 9Li and 11Li
RADIOACTIVITY 9,11Li; measured β-delayed Eα, βα-coin. 11Li; measured β-delayed E(6He), β(6He)-coin; deduced log ft. 9Li deduced single neutron emission probability, β-delayed I(n). 11Li deduced three neutron emission probability, β-delayed I(n). 9,11Be levels deduced anti-analog character.
doi: 10.1016/0375-9474(81)90521-2
Z.Phys. A302, 117 (1981)
A.D.Panagiotou, P.K.Kakanis, E.N.Gazis, M.Bernas, C.Detraz, M.Langevin, D.Guillemaud, E.Plagnol
A New Mass Measurement of 29Mg. Observation of Excited States via the 13C(18O, 2p)29Mg Reaction
NUCLEAR REACTIONS 13C(18O, 2p), E=32 MeV; measured pp-coin, σ(Ep1, Ep2, θ). 29Mg deduced mass excess, levels. Silicon surface barrier detectors.
Nucl.Phys. A371, 288 (1981)
I.Skwirczynska, E.Kozik, A.Budzanowski, J.Ploskonka, A.Strzalkowski
On the Mechanism of the 27Al(α, d)29Si Reaction
NUCLEAR REACTIONS 27Al(α, d), E=26.2, 26.45, 26.7 MeV; measured σ(Ed, θ). 29Si levels deduced two-nucleon spectroscopic amplitudes. Microscopic, macroscopic DWBA, Hauser-Feshbach analyses, shell model.
doi: 10.1016/0375-9474(81)90068-3
Nucl.Phys. A385, 474 (1982)
D.E.Alburger, E.K.Warburton
Beta Decays of 25Na, 25Al and 29Al
RADIOACTIVITY 25Na(β-), 29Al(β-), 25Al(β+) [from 23Na, 27Al(t, p), 24Mg(d, n)]; measured Eγ, Iγ; deduced log ft, Iβ. 25Mg, 29Si deduced γ-branching.
doi: 10.1016/0375-9474(82)90098-7
Z.Phys. A309, 163 (1982)
P.Betz, E.Bitterwolf, A.Burkard, F.Glatz, F.Heidinger, Th.Kern, R.Lehmann, S.Norbert, H.Ropke, C.Schneider, J.Siefert
Spectroscopy of Highly Excited States in 29Si
NUCLEAR REACTIONS 28Si(d, pγ), E=6.5, 7 MeV; 26Mg(α, nγ), E=12, 14, 15 MeV; 27Al(3He, pγ), E=9 MeV; measured σ(Ep), σ(En), γp(θ), γp-coin. 29Si deduced levels, J, π, K, deformation, rotational band structure. Shell model.
Yad.Fiz. 36, 19 (1982)
N.T.Burtebaev, A.D.Duisebaev, G.N.Ivanov, V.I.Kanashevich, E.I.Kebin, V.A.Lichman, Yu.I.Nechaev, V.G.Sukharevsky, V.A.Khaimin
Study of Reactions Induced by Accelerated 3He Ions of 34.8-MeV Energy on 27Al, 59Co, and 112Sn Nuclei with Protons, Deuterons, Tritons, and α-Particles in the Final State
NUCLEAR REACTIONS 27Al, 59Co, 112Sn(3He, p), (3He, d), (3He, t), (3He, α), E=34.8 MeV; measured σ(θ), angle integrated σ. Exciton model analysis.
Phys.Rev. C25, 2756 (1982)
F.Touchard, J.M.Serre, S.Buttgenbach, P.Guimbal, R.Klapisch, M.de Saint Simon, C.Thibault, H.T.Duong, P.Juncar, S.Liberman, J.Pinard, J.L.Vialle
Electric Quadrupole Moments and Isotope Shifts of Radioactive Sodium Isotopes
NUCLEAR MOMENTS 20,21,22,24,31Na; measured isotope shifts, hyperfine constant (A). 20,21,22,24,31Na deduced μ. 21Na, 25,26,27,28,29Na measured hyperfine constants; deduced spectroscopic quadrupole moment.
Izv.Akad.Nauk SSSR, Ser.Fiz. 47, 2143 (1983)
M.Chenzha, M.Duma, C.Hategan, M.Tanase, A.S.Deineko, I.Ya.Malakhov, V.E.Storizhko, N.A.Shlyakhov
Experimental Study of Threshold Anomalies in the Elastic Scattering of Protons by Nuclei with A ≈ 30
NUCLEAR REACTIONS 27Al(p, p), E ≈ 4.6-7.1 MeV; 29Si(p, p), E ≈ 4.9-7.5 MeV; 23Na, 31P, 35Cl, 34S(p, p), E=1-10 MeV; measured σ(θ); deduced threshold anomaly characteristics.
Nucl.Phys. A408, 221 (1983)
R.J.Peterson, C.A.Fields, R.S.Raymond, J.R.Thieke, J.L.Ullmann
A Study of the 28Si(d, p)29Si Reaction
NUCLEAR REACTIONS 28Si(d, p), E=17.85 MeV; measured σ(E(p), θ). 29Si deduced spectroscopic factors for bound, unbound states. DWBA, CCBA analyses.
doi: 10.1016/0375-9474(83)90582-1
Nucl.Phys. A431, 237 (1984)
L.C.Bland, H.T.Fortune, D.L.Watson, M.A.Abouzeid, B.H.Wildenthal
The 27Al(t, p)29Al Reaction at E(t) = 15 MeV
NUCLEAR REACTIONS 27Al(t, p), E=15 MeV; measured σ(θ). 29Al deduced levels L, J, π. DWBA analysis, shell model comparison.
doi: 10.1016/0375-9474(84)90173-8
Nucl.Phys. A425, 141 (1984)
J.S.Eck, K.W.Kemper, T.R.Ophel
The (7Li, 6Li) Reaction on 28Si and 40Ca at E(7Li) = 45 MeV
NUCLEAR REACTIONS 28Si, 40Ca(7Li, 6Li), E=45 MeV; measured σ(θ); deduced potential parameters. 41Ca, 29Si levels deduced absolute C2S spectroscopic factors. DWBA analysis, Woods-Saxon, double folding potentials.
doi: 10.1016/0375-9474(84)90220-3
Nucl.Phys. A426, 37 (1984)
D.Guillemaud-Mueller, C.Detraz, M.Langevin, F.Naulin, M.De Saint-Simon, C.Thibault, F.Touchard, M.Epherre
β-Decay Schemes of very Neutron-Rich Sodium Isotopes and Their Descendants
RADIOACTIVITY 27,28,29,30,31,32,33,34Na, 29,30,31,32,33Mg, 32Al(β-) [from In(p, X), E=10 GeV]; measured Eγ, Iγ, βγγ-coin; deduced Iβ, log ft. 27,28,29,30,31,32Mg, 29,30,31Al, 32S deduced levels, γ-branching. 29,30,31,32Mg, 31Al deduced neutron emission probabilities.
doi: 10.1016/0375-9474(84)90064-2
Nucl.Phys. A414, 151 (1984)
M.Langevin, C.Detraz, D.Guillemaud-Mueller, A.C.Mueller, C.Thibault, F.Touchard, M.Epherre
β-Delayed Neutrons from very Neutron-Rich Sodium and Magnesium Isotopes
RADIOACTIVITY 29,30,31,32,34Na, 31,32,33,34Mg(β-n); measured β-delayed neutron emission, T1/2, βn-coin; deduced neutron emission probability. On-line mass spectrometer, 4π liquid scintillator β-coincident neutron detector.
doi: 10.1016/0375-9474(84)90502-5
Z.Phys. A317, 149 (1984)
A.Lindholm, L.Nilsson, I.Bergqvist, R.Zorro, N.Olsson, B.Castel, A.Likar
Fast Neutron Radiative Capture in Silicon
NUCLEAR REACTIONS 28Si(n, γ), E=3-14 MeV; measured σ(θ=90°) vs E; deduced reaction mechanism. 29Si deduced GDR, GQR interference channel dependence. Compound nucleus, direct-semidirect, continuum shell model analyses.
Nucl.Phys. A431, 344 (1984)
R.A.McCulloch, N.M.Clarke, R.J.Griffiths, J.S.Hanspal, S.Roman, J.M.Barnwell
The Interaction of 33 MeV Polarised Helions with 30Si
NUCLEAR REACTIONS 30Si(polarized 3He, 3He), (polarized 3He, α), (polarized 3He, d), E=33.4 MeV; measured σ(θ), A(θ); deduced optical model potentials. 29,30Si, 31P levels deduced β2, β3, j-dependence, spectroscopic factors.
doi: 10.1016/0375-9474(84)90179-9
Nucl.Phys. A430, 189 (1984)
H.Miessen, H.Rothhaas, G.Luhrs, G.A.Peterson, R.S.Hicks, R.A.Lindgren, B.L.Berman, S.Kowalski, C.F.Williamson
Elastic Magnetic Electron Scattering from 29Si and 31P
NUCLEAR REACTIONS 29Si, 31P(e, e), E=90-280 MeV; measured transverse electric σ(θ) vs E, form factors. 29Si, 31P deduced radial current densities, occupation probabilities, 2s1/2 neutron, proton orbitals. Enriched 29Si, natural 31P targets. Particle-core coupling, shell model interpretations.
doi: 10.1016/0375-9474(84)90200-8
Nucl.Phys. A437, 141 (1985)
L.K.Fifield, P.V.Drumm, M.A.C.Hotchkis, T.R.Ophel, C.L.Woods
The 26Mg(18O, 17F)27Na and 26Mg(18O, 15O)29Mg Reactions and the Level Schemes of 27Na and 29Mg
NUCLEAR REACTIONS 26Mg(18O, 17F), (18O, 15O), E=100-117 MeV; measured σ(E(17F)), σ(E(15O)). 27Na, 29Mg deduced levels, ground state mass excesses. Enriched targets.
doi: 10.1016/0375-9474(85)90230-1
Phys.Rev. C31, 1941 (1985)
Z.Y.Zhou, E.C.Schloemer, M.D.Cable, M.Ahmed, J.E.Reiff, J.Cerny
Additional Beta-Delayed Protons form the T(z) = -(3/2) Nuclei 21Mg, 25Si, 29S, and 41Ti
RADIOACTIVITY 21Mg, 25Si, 29S, 41Ti(β+p) [from 20Ne, 24Mg, 28Si, 40Ca(3He, 2n), E=31.5-41.5 MeV]; measured β-delayed Ep, Ip; deduced log ft. 21Na, 25Al, 29P, 41Sc levels deduced relative Ip.
ECN FYS/RASA-85/19 (1985)
W.L.Zijp
On the Statistical Evaluation of Inconsistent Measurement Results
Phys.Rev. C33, 1294 (1986)
K.S.Dhuga, H.T.Fortune, M.Burlein, M.Carchidi, M.Dwyer, G.Gilfoyle, J.W.Sweet
Direct and Compound Components of the 27Al(6Li, α)29Si Reaction at 32 MeV
NUCLEAR REACTIONS, ICPND 27Al(6Li, α), E=32 MeV; measured σ(Eα), σ(θ); deduced σ, direct, compound components, potential, level density prameters. 29Si levels deduced spectroscopic factors. DWBA, statistical model analyses.
Phys.Rev. C33, 1971 (1986)
M.A.G.Fernandes, B.l.Burks, D.J.Horen, G.R.Satchler, R.L.Auble, F.E.Bertrand, J.L.Blankenship, J.L.C.Ford, Jr., E.E.Gross, D.C.Hensley, R.O.Sayer, D.Shapira, T.P.Sjoreen
One-Nucleon-Transfer Reactions Induced by 352-MeV 18O on 28Si
NUCLEAR REACTIONS 28Si(18O, 17O), (18O, 19F), E=352 MeV; measured σ(θ); deduced model parameters. 29Si, 27Al levels deduced single-nucleon transfer spectroscopic factors. DWBA analysis.
Nuovo Cim. 91A, 370 (1986)
E.Frota-Pessoa, S.Joffily
Resolution of the 95Zr Ground State into a Doublet
NUCLEAR REACTIONS 28Si, 94Zr(d, p), E=15.5 MeV; measured σ(Ep), σ(θ). 29Si, 95Zr deduced levels.
Nucl.Phys. A455, 494 (1986)
J.S.Hanspal, K.I.Pearce, N.M.Clarke, R.J.Griffiths, R.E.Brown, R.A.Hardekopf, W.Gruebler
The Interaction of 17 MeV Polarised Tritons with 30Si
NUCLEAR REACTIONS 30Si(polarized t, t), (polarized t, t'), (polarized t, d), (polarized t, α), E=17 MeV; measured σ(θ), A(θ). 30Si deduced deformation parameters. 31Si, 29Al levels deduced spectroscopic factors. Optical model, CCBA, DWBA analyses.
doi: 10.1016/0375-9474(86)90319-2
Phys.Rev. C36, 765 (1987)
P.Baumann, Ph.Dessagne, A.Huck, G.Klotz, A.Knipper, G.Marguier, C.Miehe, M.Ramdane, C.Richard-Serre, G.Walter, B.H.Wildenthal
Gamow-Teller Beta Decay of 29Na and Comparison with Shell-Model Predictions
RADIOACTIVITY 29Na(β-n) [from U(p, X), E=600 MeV]; measured Eγ, Iγ, β-delayed En, I(n), γγ-, nγ-coin, T1/2; deduced log ft, Gamow-Teller transition strength. 29Mg deduced levels, J, π, T1/2, β-branching ratios. Ge(Li), BaF2, plastic detectors. Shell model.
Nucl.Phys. A462, 290 (1987)
K.I.Pearce, N.M.Clarke, R.J.Griffiths, J.S.Hanspal, R.A.McCulloch
CCBA Description of One-Nucleon Pickup by Polarized Helions and Polarized Tritons on 30Si
NUCLEAR REACTIONS 30Si(polarized 3He, α), E=33 MeV; 30Si(polarized t, α), E=17 MeV; analyzed σ(θ), analyzing power vs θ; deduced reaction mechanism. 29Si, 29Al levels deduced spectroscopic amplitudes.
doi: 10.1016/0375-9474(87)90549-5
Nucl.Phys. A467, 215 (1987)
K.I.Pearce, N.M.Clarke, R.J.Griffiths, P.J.Simmonds, D.Barker, J.B.A.England, M.C.Mannion, C.A.Ogilvie
36 MeV Triton Inelastic Scattering and One-Nucleon Transfer Reaction
NUCLEAR REACTIONS 26Mg, 28,30Si(t, t), (t, t'), (t, d), (t, α), E=36 MeV; measured σ(θ). 26Mg, 28,30Si deduced deformation parameters. 27Mg, 29,31Si, 25Na, 27,29Al levels deduced spectroscopic factors. Optical model, CCBA and DWBA analyses.
doi: 10.1016/0375-9474(87)90527-6
Nucl.Phys. A480, 125 (1988)
O.Karban, L.Potvin, I.M.Turkiewicz
The 28Si(3He, pp)29Si Reaction Induced by 33 MeV Polarized 3He
NUCLEAR REACTIONS 28Si(polarized 3He, 2p), E=33 MeV; measured σ(θ(2p), E), A(E1, E2, θ1, θ2); deduced j-dependence, normalisation factor. 29Si levels deduced J, π, spectroscopic factors. Sequential breakup, statistical model analysis.
doi: 10.1016/0375-9474(88)90388-0
J.Phys.(London) G14, Supplement S215 (1988)
H.Kitazawa, M.Igashira
Mechanism of s-Wave and p-Wave Neutron Resonance Capture in Light and Medium-Weight Nuclei
NUCLEAR REACTIONS 16O, 28Si, 32S(n, γ), E ≈ resonance; measured Eγ, Iγ. 17O, 29Si, 33S deduced resonance Γγ. Valence capture model.
doi: 10.1088/0305-4616/14/S/023
Nucl.Phys. A476, 392 (1988)
C.L.Woods, W.N.Catford, L.K.Fifield, N.A.Orr, R.J.Sadleir
Studies of the T(z) = (5/2) Nuclei 31Al and 29Mg
NUCLEAR REACTIONS 30Si(18O, 17F), E=100 MeV; 30Si(13C, 14O), E=93 MeV; measured σ(E(17F)), σ(E(14O)). 31Al deduced ground state mass excess. 31Al, 29Mg deduced levels, L. Enriched targets.
doi: 10.1016/0375-9474(88)90490-3
Phys.Rev. C39, 626 (1989)
P.Baumann, Ph.Dessagne, A.Huck, G.Klotz, A.Knipper, Ch.Miehe, M.Ramdane, G.Walter, G.Marguier, H.Gabelmann, C.Richard-Serre, K.Schlosser, A.Poves
Beta Decay of 30Na: Experiment and theory
RADIOACTIVITY 30Na(β-n); measured E(γ), I(γ), E(n), I(n), γγ-, γn-coin; deduced log ft, B(GT). 30Mg deduced levels, J, π, I(β). 28,29Mg deduced levels, J, π. Ge(Li), scintillation detectors.
Z.Phys. A332, 189 (1989)
D.Guillemaud-Mueller, Yu.E.Penionzhkevich, R.Anne, A.G.Artukh, D.Bazin, V.Borrel, C.Detraz, D.Guerreau, B.A.Gvozdev, J.C.Jacmart, D.X.Jiang, A.M.Kalinin, V.V.Kamanin, V.B.Kutner, M.Lewitowicz, S.M.Lukyanov, A.C.Mueller, Nguyen Hoai Chau, F.Pougheon, A.Richard, M.G.Saint-Laurent, W.D.Schmidt-Ott
Observation of New Neutron Rich Nuclei 26F, 35,36Mg, 38,39Al, 40,41Si, 43,44P, 45-47S, 46-49Cl, and 49-51Ar from the Interactions of 55 MeV/u 48Ca + Ta
NUCLEAR REACTIONS Ta(48Ca, X), E=55 MeV/nucleon; measured fragment spectra; deduced evidence for 29F, 35,36Mg, 38,39Al, 40,41Si, 43,44P, 45,46,47S, 46,47,48,49Cl, 49,50,51Ar.
At.Data Nucl.Data Tables 42, 189 (1989)
P.Raghavan
Table of Nuclear Moments
COMPILATION Z=1-99; compiled μ, electric quadrupole moments.
doi: 10.1016/0092-640X(89)90008-9
Nucl.Phys. A496, 15 (1989)
B.von Przewoski, P.D.Eversheim, F.Hinterberger, L.Doberitz, J.Campbell, M.Hammans, R.Henneck, W.Lorenzon, M.A.Pickar, I.Sick
A Measurement of dσ/d(Omega) and A(y) in Elastic Proton Scattering from 12,13C, 29Si and 31P at 72 MeV
NUCLEAR REACTIONS 12,13C, 29Si, 31P(polarized p, p), E=72 MeV; measured σ(θ), A(y)(θ); deduced optical model potential.
doi: 10.1016/0375-9474(89)90213-3
Nucl.Phys. A521, 1 (1990); Errata and Addenda Nucl.Phys. A529, 763 (1991); Errata Nucl.Phys. A564, 609 (1993)
P.M.Endt
Energy Levels of A = 21-44 Nuclei (VII)
COMPILATION A=21-44; compiled, evaluated structure data.
doi: 10.1016/0375-9474(90)90598-G
Nucl.Phys. A510, 346 (1990)
S.Graff, J.Gorres, M.Wiescher, R.E.Azuma, J.King, J.Vise, G.Hardie T.R.Wang
Proton Capture on 28Si and Its Astrophysical Implications
NUCLEAR REACTIONS, ICPND 28Si(p, γ), E=0.37-2.95 MeV; measured σ(E); deduced astrophysical S-factor, total reaction rate. 29P deduced resonances, resonance strengths, Γ, spectroscopic factors.
doi: 10.1016/0375-9474(90)90244-G
Phys.Rev. C41, 1272 (1990)
M.A.Islam, T.J.Kennett, W.V.Prestwich
Thermal neutron capture in silicon
NUCLEAR REACTIONS 28,29,30Si(n, γ), E=thermal; measured Eγ, Iγ, σ. 29,30,31Si deduced levels, neutron separation energy. Pair spectrometer, hyperpure Ge detector.
Phys.Rev. C42, 1110 (1990)
G.S.Masson, P.A.Quin
Measurement of the Asymmetry Parameter for 29P β Decay
RADIOACTIVITY 29P [from 28Si(polarized d, p)]; measured asymmetry parameter; deduced decay theory validity.
Nucl.Phys. A510, 301 (1990)
S.Piskor, W.Schaferlingova
Spectroscopic Information on 13,14C, 15N, 17O, 29-31Si, 33S, 38Cl and 111,113,115,117Cd from the (d, p) Reaction
NUCLEAR REACTIONS 12,13C, 14N, 16O, 28,29,30Si, 32S, 37Cl, 110,112,114,116Cd(d, p), E=12.3 MeV; measured Q, σ(θ). 13,14C, 15N, 17O, 29,30,31Si, 33S deduced levels. 38Cl deduced levels, L, J, π, spectroscopic factors. Natural targets.
doi: 10.1016/0375-9474(90)90241-D
Nucl.Phys. A517, 176 (1990)
P.Tikkanen, J.Keinonen, A.Kuronen, A.Z.Kiss, E.Koltay, E.Pintye, B.H.Wildenthal
Short Lifetimes in 29Si-29P for the Test of Shell-Model Wave Functions
NUCLEAR REACTIONS 15N(16O, np), E=17, 20, 22 MeV; 28Si(p, γ), E=1.38, 1.65, 2.08, 2.29 MeV; measured DSA. 29Si, 29P levels deduced T1/2, δ, γ-branching. Implanted, enriched 15N, 28Si targets. Shell model comparison.
doi: 10.1016/0375-9474(90)90267-P
Nucl.Phys. A531, 353 (1991)
V.Borrel, J.C.Jacmart, F.Pougheon, R.Anne, C.Detraz, D.Guillemaud-Mueller, A.C.Mueller, D.Bazin, R.Del Moral, J.P.Dufour, F.Hubert, M.S.Pravikoff, E.Roeckl
31Ar and 27S: Beta-delayed two-proton emission and mass excess
RADIOACTIVITY 31Ar, 27S(β+p), (β+2p); [from 36Ar fragmentation reaction]; measured β-delayed Ep, T1/2, branching ratios; deduced ground state masses. Magnetic, energy-loss and time-of-flight analysis, solid-state detector telescope.
doi: 10.1016/0375-9474(91)90616-E
Phys.Rev. C45, 69 (1992)
D.Bazin, R.Del Moral, J.P.Dufour, A.Fleury, F.Hubert, M.S.Pravikoff, R.Anne, P.Bricault, C.Detraz, M.Lewitowicz, Y.Zheng, D.Guillemaud-Mueller, J.C.Jacmart, A.C.Mueller, F.Pougheon, A.Richard
Decay Modes of 31Ar and First Observation of β-Delayed Three-Proton Radioactivity
RADIOACTIVITY 31Ar; measured T1/2, β(multi-proton)coin, Ep. 31Cl deduced levels. 31Ar deduced mass excess, p-xp branching ratios. Silicon detectors. Calculated coin rates, Monte-Carlo, β-p branching ratio, shell model.
Phys.Rev. C46, 2364 (1992)
H.Kitazawa, M.Igashira, M.Shimizu, K.Muto, T.Oda, Y.Achiha, Y.-H.Lee, N.Mukai
Electric and Magnetic Dipole Transitions from Broad s-Wave Neutron Resonance in Even-Even sd-Shell Nuclei
NUCLEAR REACTIONS 24Mg(n, γ), E=658 keV; 28Si(n, γ), E=180 keV; 32S(n, γ), E=103 keV; measured Eγ, Iγ, σ(E, Eγ) at 125°. 25Mg, 29Si, 33S levels deduced transition γ-multipolarity, partial radiative widths. Valence capture shell models, configuration mixing.
Phys.Rev. C46, 972 (1992)
S.Raman, E.T.Jurney, J.W.Starner, J.E.Lynn
Thermal-Neutron Capture by Silicon Isotopes
NUCLEAR REACTIONS 28,29,30Si(n, γ), E=thermal; measured Eγ, Iγ following capture; deduced σ. 29,30,31Si deduced neutron separation energies, transition γ-multipolarity. Direct capture interpretation.
Z.Phys. A342, 303 (1992)
O.Tengblad, M.J.G.Borge, L.Johannsen, B.Jonson, M.Lindroos, T.Nilsson, G.Nyman, A.Poves, H.L.Ravn, J.Retamosa, K.Riisager, P.Sona, K.Wilhelmsen, and the ISOLDE Collaboration
Study of Neutron Rich Neon Isotopes
RADIOACTIVITY 26,27,28,29Ne(β-n) [from Th(3He, X), E=910 MeV]; measured Iβ, T1/2, neutron emission probabilities. Shell model analysis.
Nucl.Phys. A549, 223 (1992)
J.F.Wilkerson, T.M.Mooney, R.E.Fauber, T.B.Clegg, H.J.Karwowski, E.J.Ludwig, W.J.Thompson
Isospin-Nonconserving Particle Decays in Light Nuclei
NUCLEAR REACTIONS 12C, 16O, 20Ne, 24Mg, 28Si, 32S, 36Ar(polarized p, p), E ≈ resonance; 23Na, 31P(polarized p, p), (polarized p, α), 24Mg, 28Si(α, α), 20Ne(polarized p, p), E=6.4-7.7 MeV; measured σ(θ, E), analyzing power vs E, θ; deduced σ(E). 13N, 17F, 24Na, 25Al, 29P, 33S, 37K, 24Mg, 32S, 28Si deduced resonance parameters, isospin-nonconservation probabilities. Enriched targets, ion-implanted targets, polarized and unpolarized beams.
doi: 10.1016/0375-9474(92)90041-H
Phys.Rev. C47, 2502 (1993)
G.Klotz, P.Baumann, M.Bounajma, A.Huck, A.Knipper, G.Walter, G.Marguier, C.Richard-Serre, A.Poves, J.Retamosa
Beta Decay of 31,32Na and 31Mg: Study of the N = 20 shell closure
RADIOACTIVITY 31,32Na, 31Mg(β-n) [from U(p, X), E=600 MeV]; measured Eγ, Iγ, γγ-, nγ-coin, Iβ; deduced log ft. 31,32Mg, 31Al deduced levels, J, π. 32Al deduced γ-cascade evidence.
Nucl.Phys. A571, 1 (1994)
J.Vernotte, G.Berrier-Ronsin, J.Kalifa, R.Tamisier, B.H.Wildenthal
Spectroscopic Factors from One-Proton Stripping Reactions on sd-Shell Nuclei: Experimental Measurements and Shell-Model Calculations
NUCLEAR REACTIONS 16,18O, 19F, 23Na, 24,25,26Mg, 27Al, 28,29,30Si, 31P, 32,34S, 35,37Cl, 39K(3He, d), E=25 MeV; measured σ(θ); deduced bound proton optical potential parametrization. 17,19F, 20Ne, 24Mg, 25,26,27Al, 28Si, 29,30,31P, 32S, 33,35Cl, 36,38Ar, 40Ca levels deduced spectroscopic factors.
doi: 10.1016/0375-9474(94)90339-5
Priv.Comm. (1996)
F.Pougheon
NUCLEAR STRUCTURE 19Na; analyzed measured not given; deduced T1/2 estimate.
At.Data Nucl.Data Tables 66, 131 (1997)
P.Moller, J.R.Nix, K.-L.Kratz
Nuclear Properties for Astrophysical and Radioactive-Ion-Beam Applications
NUCLEAR STRUCTURE Z=8-136; A=16-339; calculated, compiled total binding energy, one-, two-neutron, proton separation energies, pairing gaps, odd-nucleon parity, spin projection. Folded-Yukawa single particle potential, Lipkin-Nogami approximation.
RADIOACTIVITY Z=8-136; A=16-339; calculated, compiled β-, α-decay Q, T1/2. Folded-Yukawa single particle potential, Lipkin-Nogami approximation.
Nucl.Phys. A616, 286c (1997)
T.Suzuki, H.Geissel, O.Bochkarev, L.Chulkov, M.Golovkov, D.Hirata, H.Irnich, Z.Janas, H.Keller, T.Kobayashi, G.Kraus, G.Munzenberg, S.Neumaier, F.Nickel, A.Ozawa, A.Piechaczek, E.Roeckl, W.Schwab, K.Summerer, K.Yoshida, I.Tanihata
Matter Radii of Na and Mg Isotopes
NUCLEAR REACTIONS C(20Na, X), (21Na, X), (22Na, X), (23Na, X), (25Na, X), (26Na, X), (27Na, X), (28Na, X), (29Na, X), (30Na, X), (31Na, X), (32Na, X), (20Mg, X), (22Mg, X), (23Mg, X), (24Mg, X), (25Mg, X), (27Mg, X), (29Mg, X), (30Mg, X), (31Mg, X), (32Mg, X), (33Mg, X), E=950 MeV/nucleon; measured interaction σ. 32,31,30,29,28,27,26,25,23,22,21,20Na, 20,22,23,24,27,29,30,31,32Mg deduced effective rms radii, nucleon skin thickness related features.
doi: 10.1016/S0375-9474(97)00099-7
Phys.Lett. 409B, 64 (1997)
O.Tarasov, R.Allatt, J.C.Angelique, R.Anne, C.Borcea, Z.Dlouhy, C.Donzaud, S.Grevy, D.Guillemaud-Mueller, M.Lewitowicz, S.Lukyanov, A.C.Mueller, F.Nowacki, Yu.Oganessian, N.A.Orr, A.N.Ostrowski, R.D.Page, Yu.Penionzhkevich, F.Pougheon, A.Reed, M.G.Saint-Laurent, W.Schwab, E.Sokol, O.Sorlin, W.Trinder, J.S.Winfield
Search for 28O and Study of Neutron-Rich Nuclei Near the N = 20 Shell Closure
NUCLEAR REACTIONS Ta(36S, X)24Si/33Al/32Mg/31Na/30Ne/29F, E=78 MeV/nucleon; measured fragment yields. 28O deduced evidence for particle instability. LISE spectrometer.
RADIOACTIVITY 27,29F, 28,29,30Ne, 30,31Na(β-) [from Ta(36S, X), E=78 MeV/nucleon]; measured T1/2.
doi: 10.1016/S0370-2693(97)00901-5
Phys.Rev. C55, 2458 (1997)
H.Vonach, A.Pavlik, A.Wallner, M.Drosg, R.C.Haight, D.M.Drake, S.Chiba
Spallation Reactions in 27Al and 56Fe Induced by 800 MeV Protons
NUCLEAR REACTIONS, ICPND 27Al(p, X)28Si/25Na/24Na/22Na/23Ne/18Ne/23F/22F/21F/20F/20O/19O/14O, E=800 MeV; 56Fe(p, X)56Co/53Fe/54Mn/52Mn/52mMn/50mMn/51Cr/49Cr/48Cr/53V/48V/51Ti/48Sc/47Sc/46Sc/44gSc/44mSc/43Sc/42mSc/42K/38mK/41Ar/39Cl/38Cl/34Cl/32Cl/38S/37S/35P/33Si/26Si/30Al/29Al/28Al/28Mg/27Mg/25Na/24Na/22Na/23Ne/20F, E=800 MeV; measured γ production σ, discrete γ lines; deduced nuclide production σ.
Nucl.Phys. A634, 475 (1998); Erratum Nucl.Phys. A641, 529 (1998)
L.Axelsson, J.Aysto, M.J.G.Borge, L.M.Fraile, H.O.U.Fynbo, A.Honkanen, P.Hornshoj, A.Jokinen, B.Jonson, P.O.Lipas, I.Martel, I.Mukha, T.Nilsson, G.Nyman, B.Petersen, K.Riisager, M.H.Smedberg, O.Tengblad, and the ISOLDE Collaboration
Beta Decay of 31Ar
RADIOACTIVITY 31Ar(β+p) [from 1 GeV p on CaO powder target]; measured βp-, βγ-coin, Ep, Ip. 31Cl deduced levels, branching, log ft, Gamow-Teller strength, IAS. OXBASH shell-model calculations, Gamow-Teller quenching, isospin mixing.
doi: 10.1016/S0375-9474(98)00172-9
Nucl.Phys. A633, 1 (1998)
P.M.Endt
Supplement to Energy Levels of A = 21-44 Nuclei (VII)
COMPILATION A=21-44; compiled, evaluated structure data.
doi: 10.1016/S0375-9474(97)00613-1
RIKEN-97, p.74 (1998)
M.Notani, N.Aoi, N.Fukuda, E.Ideguchi, M.Ishihara, H.Iwasaki, H.Ogawa, T.Kubo, S.M.Lukyanov, T.Nakamura, Yu.E.Penionzhkevich, H.Sakurai, T.Teranishi, Y.X.Watanabe, K.Yoneda, A.Yoshida
Lifetime Measurement of 31, 32Ne
RADIOACTIVITY 27,29F, 29,30,31,32Ne, 31,32,33Na(β-) [from Ta(40Ar, X), E=95 MeV/nucleon]; measured T1/2. ΔE-tof frag identification.
Nucl.Phys. A630, 661 (1998)
T.Suzuki, H.Geissel, O.Bochkarev, L.Chulkov, M.Golovkov, N.Fukunishi, D.Hirata, H.Irnich, Z.Janas, H.Keller, T.Kobayashi, G.Kraus, G.Munzenberg, S.Neumaier, F.Nickel, A.Ozawa, A.Piechaczeck, E.Roeckl, W.Schwab, K.Summerer, K.Yoshida, I.Tanihata
Nuclear Radii of Na and Mg Isotopes
NUCLEAR REACTIONS C(20Na, X), (21Na, X), (22Na, X), (23Na, X), (25Na, X), (26Na, X), (27Na, X), (28Na, X), (29Na, X), (30Na, X), (31Na, X), (32Na, X), (20Mg, X), (22Mg, X), (23Mg, X), (24Mg, X), (25Mg, X), (27Mg, X), (29Mg, X), (30Mg, X), (31Mg, X), (32Mg, X), (33Mg, X), E=950 MeV/nucleon; measured interaction σ. 20,21,22,23,25,26,27,28,29,30,31,32Na, 20,22,23,24,27,29,30,31,32Mg deduced rms radii, neutron, proton skin features. Shell model calculations.
doi: 10.1016/S0375-9474(97)00799-9
J.Phys.(London) G25, 859 (1999)
Z.Dlouhy, Yu.Penionzhkevich, R.Anne, D.Baiborodin, C.Borcea, A.Fomichev, D.Guillemaud-Mueller, R.Kalpakchieva, M.Lewitowicz, S.Lukyanov, A.C.Mueller, Yu.Oganessian, R.D.Page, A.Reed, M.G.Saint-Laurent, E.Sokol, N.Skobelev, O.Sorlin, O.Tarasov, V.Toneev, W.Trinder
Dripline Nuclei Produced by Quasi-Fragmentation of the 32, 34, 36S Primary Beams
NUCLEAR REACTIONS C, 181Ta(36S, X), E=75 MeV/nucleon; C, 197Au(32S, X), E=9.1, 16.1 MeV; measured Z=6-14 fragments isotopic production σ. 26,28O deduced particle instability.
RADIOACTIVITY 26,27,29F, 27,28,29,30Ne, 30,31Na(β-) [from 36S fragmentation]; measured T1/2. Comparison with shell-model predictions, previous measurements.
doi: 10.1088/0954-3899/25/4/055
Phys.Rev. C59, 2275 (1999)
H.O.U.Fynbo, L.Axelsson, J.Aysto, M.J.G.Borge, L.M.Fraile, A.Honkanen, P.Hornshoj, Y.Jading, A.Jokinen, B.Jonson, I.Martel, I.Mukha, T.Nilsson, G.Nyman, M.Oinonen, K.Riisager, T.Siiskonen, M.H.Smedberg, O.Tengblad, F.Wenander, and the ISOLDE Collaboration
31Ar Examined: New limit on the β-delayed three-proton branch
RADIOACTIVITY 31Ar(β+); measured Eβ, Ep, β-delayed multi-proton decay branching ratios; deduced three-proton branch upper limit.
Phys.Rev. C60, 024311 (1999)
A.T.Reed, O.Tarasov, R.D.Page, D.Guillemaud-Mueller, Yu.E.Penionzhkevich, R.G.Allatt, J.C.Angelique, R.Anne, C.Borcea, V.Burjan, W.N.Catford, Z.Dlouhy, C.Donzaud, S.Grevy, M.Lewitowicz, S.M.Lukyanov, F.M.Marques, G.Martinez, A.C.Mueller, P.J.Nolan, J.Novak, N.A.Orr, F.Pougheon, P.H.Regan, M.G.Saint-Laurent, T.Siiskonen, E.Sokol, O.Sorlin, J.Suhonen, W.Trinder, S.M.Vincent
Radioactivity of Neutron-Rich Oxygen, Fluorine, and Neon Isotopes
RADIOACTIVITY 19B, 24O, 25,26,27,29F, 28,29,30Ne(β-) [from 36S fragmentation]; measured Eγ, Iγ, βγ-, βn-coin, T1/2, neutron emission probabilities; deduced log ft. 24F, 25,26Ne, 28,30Na deduced levels, possible J, π. Comparison with shell model calculations.
doi: 10.1103/PhysRevC.60.024311
Nucl.Phys. A677, 38 (2000)
H.O.U.Fynbo, M.J.G.Borge, L.Axelsson, J.Aysto, U.C.Bergmann, L.M.Fraile, A.Honkanen, P.Hornshoj, Y.Jading, A.Jokinen, B.Jonson, I.Martel, I.Mukha, T.Nilsson, G.Nyman, M.Oinonen, I.Piqueras, K.Riisager, T.Siiskonen, M.H.Smedberg, O.Tengblad, J.Thaysen, F.Wenander, and the ISOLDE Collaboration
The β2p Decay Mechanism of 31Ar
RADIOACTIVITY 31Ar(β+p) [from Ca(p, 3pxn)]; measured β-delayed Ep, E(2p), pp energy and angular correlations. 31Ar deduced β1p and β2p decay channels, T1/2. 30S, 31Cl deduced levels, J, π, branching ratios. CaO target, on-line mass separation, double sided Si strip detectors, surface barrier Si detector.
doi: 10.1016/S0375-9474(00)00248-7
Eur.Phys.J. A 8, 31 (2000)
M.Keim, U.Georg, A.Klein, R.Neugart, M.Neuroth, S.Wilbert, P.Lievens, L.Vermeeren, B.A.Brown, and the ISOLDE Collaboration
Measurement of the Electric Quadrupole Moments of 26-29Na
NUCLEAR MOMENTS 26,27,28,29,30,31Na; measured β-NMR spectra; deduced μ. 26,27,28,29Na deduced quadrupole moments. Oriented nuclei, optical pumping.
RADIOACTIVITY 26,27,28,29,30,31Na(β-) [from U(p, X)]; measured β-NMR spectra; deduced μ. 26,27,28,29Na deduced quadrupole moments. Oriented nuclei, optical pumping.
Nucl.Phys. A673, 411 (2000)
A.Ozawa, O.Bochkarev, L.Chulkov, D.Cortina, H.Geissel, M.Hellstrom, M.Ivanov, R.Janik, K.Kimura, T.Kobayashi, A.A.Korsheninnikov, G.Munzenberg, F.Nickel, A.A.Ogloblin, M.Pfutzner, V.Pribora, H.Simon, B.Sitar, P.Strmen, K.Summerer, T.Suzuki, I.Tanihata, M.Winkler, K.Yoshida
Production Cross-Sections of Light Neutron-Rich Nuclei from 40Ar Fragmentation at About 1 GeV/nucleon
NUCLEAR REACTIONS 9Be(40Ar, X)11B/12B/14B/15B/17B/19B/13C/14C/17C/18C/19C/20C/22C/14N/15N/16N/17N/18N/19N/20N/21N/22N/23N/16O/17O/19O/21O/22O/23O/24O/18F/19F/21F/23F/24F/25F/26F/27F/29F, E ≈ 1 GeV/nucleon; measured production σ. 26O deduced particle instability. Fragment recoil separator. Comparisons with empirical parameterization.
doi: 10.1016/S0375-9474(00)00147-0
Thesis, Michigan State University (2000)
B.V.Pritychenko
Intermediate-Energy Coulomb Excitation of the Neutron-Rich Radioactive Isotopes 26, 28Ne, 28-31Na, 30-34Mg, 34, 35Al, 33Si and 34P
NUCLEAR REACTIONS 197Au(26Ne, 26Ne'), (28Ne, 28Ne'), (30Mg, 30Mg'), (32Mg, 32Mg'), (34Mg, 34Mg'), (36Ar, 36Ar'), E ≈ 50 MeV/nucleon; 197Au(31Mg, 31Mg'), E=62.08 MeV/nucleon; 197Au(33Mg, 33Mg'), E=61.8 MeV/nucleon; 197Au(33Si, 33Si'), E=50.5 MeV/nucleon; 197Au(34P, 34P'), E=54.5 MeV/nucleon; 197Au(34Al, 34Al'), E=59.7 MeV/nucleon; 197Au(35Al, 35Al'), E=55.83 MeV/nucleon; 197Au(28Na, 28Na'), E=43.1 MeV/nucleon;197Au(29Na, 29Na'), E=59.97 MeV/nucleon; 197Au(30Na, 30Na'), E=55.6 MeV/nucleon; 197Au(31Na, 31Na'), E=58.9 MeV/nucleon; measured Eγ, Iγ, (particle)γ-coin following projectile Coulomb excitation. 26,28Ne, 30,32Mg, 36Ar, 197Au deduced levels energies, excitation B(E2), configurations. 28,29,30,31Na, 31,33Mg, 34,35Al, 33Si, 34P deduced excitation levels, σ. Secondary beams from 48Ca, 40Ar fragmentation, comparison with shell model, Nilsson diagrams and nuclear systematics for deformed 'island of inversion' nuclei.
Yad.Fiz. 64, No 6, 1197 (2001); Phys.Atomic Nuclei 64, 1121 (2001)
Yu.E.Penionzhkevich
Research on Neutron-Rich Nuclei in the Region of the Nuclear Shells N = 20 and N = 28
NUCLEAR REACTIONS Be(36S, X)19B/22C/31F/32Mg, E=77 MeV/nucleon; measured Eγ, Iγ, yields.
RADIOACTIVITY 22N, 24O, 25,27,29F, 27,28,29,30Ne, 30,31Na(β-); measured T1/2, neutron-emission probability.
ATOMIC MASSES Z=12-20; A=28-50; measured two-neutron separation energies. Direct time-of-flight technique.
doi: 10.1134/1.1383628
Nucl.Phys. A729, 3 (2003)
G.Audi, O.Bersillon, J.Blachot, A.H.Wapstra
The NUBASE evaluation of nuclear and decay properties
COMPILATION A=1-293; compiled, evaluated ground- and isomeric-states mass excess, J, π, decay properties.
doi: 10.1016/j.nuclphysa.2003.11.001
Nucl.Phys. A729, 337 (2003)
G.Audi, A.H.Wapstra, C.Thibault
The AME2003 atomic mass Evaluation (II). Tables, graphs, and references
COMPILATION A=1-293; compiled, evaluated atomic mass data.
doi: 10.1016/j.nuclphysa.2003.11.003
Phys.Lett. B 566, 84 (2003)
Y.Yanagisawa, M.Notani, H.Sakurai, M.Kunibu, H.Akiyoshi, N.Aoi, H.Baba, K.Demichi, N.Fukuda, H.Hasegawa, Y.Higurashi, M.Ishihara, N.Iwasa, H.Iwasaki, T.Gomi, S.Kanno, M.Kurokawa, Y.U.Matsuyama, S.Michimasa, T.Minemura, T.Mizoi, T.Nakamura, A.Saito, M.Serata, S.Shimoura, T.Sugimoto, E.Takeshita, S.Takeuchi, K.Ue, K.Yamada, K.Yoneda, T.Motobayashi
The first excited state of 30Ne studied by proton inelastic scattering in reversed kinematics
NUCLEAR REACTIONS 1H(29Ne, 29Ne'), (30Ne, 30Ne'), E=48 MeV/nucleon; measured Eγ, Iγ, (particle)γ-coin. 30Ne deduced level energy. 29Ne deduced transitions.
doi: 10.1016/S0370-2693(03)00802-5
Radiochim.Acta 91, 689 (2003)
H.Yashima, Y.Uwamino, H.Iwase, H.Sugita, T.Nakamura, S.Ito, A.Fukumura
Measurement and calculation of radioactivities of spallation products by high-energy heavy ions
NUCLEAR REACTIONS Cu(p, X), (α, X), (12C, X), (20Ne, X), (40Ar, X)7Be/22Na/24Na/27Mg/28Mg/29Al/34mCl/38Cl/39Cl/41Ar/42K/43K/43Sc/44Sc/44mSc/46Sc/47Sc/48Sc/48Cr/49Cr/51Cr/54Mn/56Mn/52Fe/59Fe/55Co/56Co/57Co/58Co/60Co/61Co/62mCo/57Ni/65Ni/60Cu/61Cu/64Cu/62Zn/63Zn/65Zn, E=100, 230 MeV/nucleon; measured production σ. Activation technique.
doi: 10.1524/ract.91.12.689.23423
Nucl.Phys. A746, 96c (2004)
H.Scheit, and the REX and MINIBALL Collaboration
First results on in-beam γ spectroscopy of neutron-rich Na and Mg isotopes at REX-ISOLDE
NUCLEAR REACTIONS 2H(25Na, 26Na), (30Mg, 29Mg), (30Mg, 31Mg), E=2.2 MeV/nucleon; measured Eγ, Iγ, (particle)γ-coin. Ni(30Mg, 30Mg'), E=2.25 MeV/nucleon; measured Eγ, Iγ, (particle)γ-coin following projectile Coulomb excitation. 26Na, 29,30,31Mg deduced levels, transitions.
doi: 10.1016/j.nuclphysa.2004.09.126
Nucl.Phys. A734, 374 (2004)
Y.Yanagisawa, M.Notani, H.Sakurai, M.Kunibu, H.Akiyoshi, N.Aoi, H.Baba, K.Demichi, N.Fukuda, H.Hasegawa, Y.Higurashi, M.Ishihara, N.Iwasa, H.Iwasaki, T.Gomi, S.Kanno, M.Kurokawa, Y.U.Matsuyama, S.Michimasa, T.Minemura, T.Mizoi, T.Nakamura, A.Saito, M.Serata, S.Shimoura, T.Sugimoto, E.Takeshita, S.Takeuchi, K.Ue, K.Yamada, K.Yoneda, T.Motobayashi
The First Excited State of 30Ne Studied by Proton Inelastic Scattering in Reversed Kinematics
NUCLEAR REACTIONS 1H(30Ne, 30Ne'), (29Ne, 29Ne'), E not given; measured Eγ, Iγ, (particle)γ-coin. 30Ne deduced level energy, deformation. 29Ne deduced transitions.
doi: 10.1016/j.nuclphysa.2004.01.071
Phys.Rev. C 72, 054316 (2005)
M.Belleguic, F.Azaiez, Zs.Dombradi, D.Sohler, M.J.Lopez-Jimenez, T.Otsuka, M.G.Saint-Laurent, O.Sorlin, M.Stanoiu, Y.Utsuno, Yu.-E.Penionzhkevich, N.L.Achouri, J.C.Angelique, C.Borcea, C.Bourgeois, J.M.Daugas, F.De Oliveira-Santos, Z.Dlouhy, C.Donzaud, J.Duprat, Z.Elekes, S.Grevy, D.Guillemaud-Mueller, S.Leenhardt, M.Lewitowicz, S.M.Lukyanov, W.Mittig, M.G.Porquet, F.Pougheon, P.Roussel-Chomaz, H.Savajols, Y.Sobolev, C.Stodel, J.Timar
Search for neutron excitations across the N = 20 shell gap in 25-29Ne
NUCLEAR REACTIONS 9Be, C(36S, X)25Ne/26Ne/27Ne/28Ne, E=77.5 MeV/nucleon; measured Eγ, Iγ, γγ-coin. 26,28Ne deduced levels, J, π. 27,29Ne deduced excited states. Comparison with shell model predictions.
doi: 10.1103/PhysRevC.72.054316
Phys.Rev. C 72, 048201 (2005); Erratum Phys.Rev. C 72, 059901 (2005)
J.J.Kelly
Accuracy of traditional Legendre estimators of quadrupole ratios for the N → Δ transition
doi: 10.1103/PhysRevC.72.048201
At.Data Nucl.Data Tables 90, 75 (2005)
N.J.Stone
Table of nuclear magnetic dipole and electric quadrupole moments
NUCLEAR MOMENTS Z=0-99; A=1-255; compiled μ, electric quadrupole moments.
COMPILATION Z=0-99; A=1-255; compiled μ, electric quadrupole moments.
doi: 10.1016/j.adt.2005.04.001
Phys.Rev.Lett. 94, 162501 (2005)
V.Tripathi, S.L.Tabor, P.F.Mantica, C.R.Hoffman, M.Wiedeking, A.D.Davies, S.N.Liddick, W.F.Mueller, T.Otsuka, A.Stolz, B.E.Tomlin, Y.Utsuno, A.Volya
29Na: Defining the Edge of the Island of Inversion for Z = 11
RADIOACTIVITY 28,29Ne(β-) [from Be(48Ca, X)]; measured Eγ, Iγ, γγ-, βγ-coin; deduced log ft. 28,29Na deduced levels, J, π, β-feeding intensities, configurations, inverted shell structure.
doi: 10.1103/PhysRevLett.94.162501
Eur.Phys.J. A 25, Supplement 1, 101 (2005)
V.Tripathi, S.L.Tabor, P.F.Mantica, C.R.Hoffman, M.Wiedeking, A.D.Davies, S.N.Liddick, W.F.Mueller, A.Stolz, B.E.Tomlin, A.Volya
Voyage to the "Island of Inversion": 29Na
RADIOACTIVITY 29Ne(β-) [from Be(48Ca, X)]; measured Eγ, Eβ, γγ-, βγ-coin; deduced log ft. 29Na deduced levels, β-feeding intensities. Comparison with shell model calculations.
doi: 10.1140/epjad/i2005-06-124-y
Proc. Int.Sym.on Structure of Exotic Nuclei and Nuclear Forces, Tokyo, Japan, 9-12 March 2006, p.165 (2006)
P.Fallon, E.Rodriguez-Vieitez, D.Bazin, C.M.Campbell, J.M.Cook, R.M.Clark, D.-C.Dinca, A.Gade, T.Glasmacher, I.-Y.Lee, A.O.Macchiavelli, W.F.Mueller, S.G.Prussin, M.Wiedeking, K.Yoneda
Transition to the Island of Inversion: Study of Excited States in 28-30Ne
RADIOACTIVITY 28,29,30Ne; measured Eγ, Iγ, γγ-coinc. 28,29,30Ne deduced level, J, π.
CNS-REP-69, p.19 (2006)
T.Fukui, S.Ota, S.Shimoura, N.Aoi, E.Takeshita, S.Takeuchi, H.Suzuki, H.Baba, T.Fukuchi, Y.Hashimoto, E.Ideguchi, K.Ieki, N.Iwasa, H.Iwasaki, S.Kanno, Y.Kondo, T.Kubo, K.Kurita, T.Minemura, S.Michimasa, T.Motobayashi, T.Murakami, T.Nakabayashi, T.Nakamura, M.Niikura, T.Okumura, T.K.Onishi, H.Sakurai, M.Shinohara, D.Suzuki, M.K.Suzuki, M.Tamaki, K.Tanaka, Y.Togano, Y.Wakabayashi, K.Yamada
High Resolution In-beam Gamma Spectroscopy of N ∼ 20 Neutron-rich Nuclei
NUCLEAR REACTIONS He(28Na, X), (29Na, X), (30Na, X), (31Na, X), (30Mg, X), (31Mg, X), (32Mg, X), (33Mg, X), (32Al, X), (33Al, X), (34Al, X), (35Al, X), (34Si, X), (35Si, X), (36Si, X), (36P, X), (37P, X), E ≈ 40 MeV/nucleon; measured Eγ, Iγ, (particle)γ-coin. 28,29,30,31Na, 30,31,32,33Mg, 32,33,34,35Al deduced transitions.
Nucl.Phys. A780, 1 (2006)
A.Khouaja, A.C.C.Villari, M.Benjelloun, D.Hirata, G.Auger, H.Savajols, W.Mittig, P.Roussel-Chomaz, N.A.Orr, M.G.Saint-Laurent, S.Pita, A.Gillibert, M.Chartier, C.E.Demonchy, L.Giot, D.Baiborodin, Y.Penionzhkevich, W.N.Catford, A.Lepine-Szily, Z.Dlouhy
Reaction cross-section and reduced strong absorption radius measurements of neutron-rich nuclei in the vicinity of closed shells N = 20 and N = 28
NUCLEAR REACTIONS Si(17N, X), (18N, X), (19N, X), (20N, X), (21N, X), (22N, X), (19O, X), (20O, X), (21O, X), (22O, X), (23O, X), (24O, X), (21F, X), (22F, X), (23F, X), (24F, X), (25F, X), (26F, X), (27F, X), (23Ne, X), (24Ne, X), (25Ne, X), (26Ne, X), (27Ne, X), (28Ne, X), (29Ne, X), (30Ne, X), (26Na, X), (27Na, X), (28Na, X), (29Na, X), (30Na, X), (31Na, X), (32Na, X), (33Na, X), (28Mg, X), (29Mg, X), (30Mg, X), (31Mg, X), (32Mg, X), (33Mg, X), (34Mg, X), (35Mg, X), (31Al, X), (32Al, X), (33Al, X), (34Al, X), (35Al, X), (36Al, X), (37Al, X), (38Al, X), (33Si, X), (34Si, X), (35Si, X), (36Si, X), (37Si, X), (38Si, X), (39Si, X), (40Si, X), (36P, X), (37P, X), (38P, X), (39P, X), (40P, X), (41P, X), (42P, X), (39S, X), (40S, X), (41S, X), (42S, X), (43S, X), (44S, X), (42Cl, X), (43Cl, X), (44Cl, X), (45Cl, X), (45Ar, X), (46Ar, X), E=30-65 MeV/nucleon; measured energy-integrated reaction σ. 17,18,19,20,21,22N, 19,20,21,22,23,24O, 21,22,23,24,25,26,27F, 23,24,25,26,27,28,29,30Ne, 26,27,28,29,30,31,32,33Na, 28,29,30,31,32,33,34,35Mg, 31,32,33,34,35,36,37,38Al, 33,34,35,36,37,38,39,40Si, 36,37,38,39,40,41,42P, 39,40,41,42,43,44S, 42,43,44,45Cl, 45,46Ar; deduced radii, isospin dependence. 35Mg, 44S; deduced possible halo structure or large deformation.
doi: 10.1016/j.nuclphysa.2006.07.042
Phys.Rev. C 73, 054303 (2006)
V.Tripathi, S.L.Tabor, C.R.Hoffman, M.Wiedeking, A.Volya, P.F.Mantica, A.D.Davies, S.N.Liddick, W.F.Mueller, A.Stolz, B.E.Tomlin, T.Otsuka, Y.Utsuno
β-delayed γ spectroscopy of neutron rich 27, 28, 29Na
RADIOACTIVITY 27,28,29Ne(β-); 28,29Ne(β-n); 29Ne(β-2n) [from Be(48Ca, X)]; measured β-delayed Eγ, Iγ, T1/2; deduced log ft, branching ratios. 27,28,29Na deduced levels, J, π.
NUCLEAR REACTIONS Be(48Ca, X)27F/29Ne/30Na/31Na/32Mg, E=12.3 MeV/nucleon; measured yields.
doi: 10.1103/PhysRevC.73.054303
IAEA-STI/PUB/1263 (2007)
H.D.Choi, R.B.Firestone, R.M.Lindstrom, G.L.Molnar, S.F.Mughabghab, R.Paviotti Corcuera, Z.Revay, A.Trkov, V.Zerkin, C.Zhou
Database of Prompt Gamma Rays from Slow Neutron Capture for Elemental Analysis
COMPILATION Z=1-92; compiled Eγ, Iγ from neutron capture.
Phys.Rev. C 76, 064609 (2007)
P.Napolitani, K.-H.Schmidt, L.Tassan-Got, P.Armbruster, T.Enqvist, A.Heinz, V.Henzl, D.Henzlova, A.Kelic, R.Pleskac, M.V.Ricciardi, C.Schmitt, O.Yordanov, L.Audouin, M.Bernas, A.Lafriaskh, F.Rejmund, C.Stephan, J.Benlliure, E.Casarejos, M.Fernandez-Ordonez, J.Pereira, A.Boudard, B.Fernandez, S.Leray, C.Villagrasa, C.Volant
Measurement of the complete nuclide production and kinetic energies of the system 136Xe+hydrogen at 1 GeV per nucleon
NUCLEAR REACTIONS 136Xe(p, X), E=1 GeV/nucleon; measured isotopic cross sections, kinetic energies. 6,7,8Li, 9,10,11,12Be, 10,11,12,13B, 11,12,13,14,15C, 13,14,15,16,17N, 15,16,17,18,19O, 17,18,19,20,21F, 19,20,21,22,23Ne, 22,23,24,25Na, 23,24,25,26,27Mg, 25,26,27,28,29,30Al, 28,29,30,31,32Si, 30,31,32,33,34P, 32,33,34,35,36,37,38S, 34,35,36,37,38,39,40Cl, 36,37,38,39,40,41,42,43Ar, 39,40,41,42,43,44,45K, 41,42,43,44,45,46,47Ca, 43,44,45,46,47,48,49,50Sc, 45,46,47,48,49,50,51,52Ti, 46,47,48,49,50,51,52,53,54,55V, 49,50,51,52,53,54,55,56,57Cr, 50,51,52,53,54,55,56,57,58,59,60Mn, 55,56,57,58,59,60,61,62Fe, 57,58,59,60,61,62,63,64,65Co, 59,60,61,62,63,64,65,66,67Ni, 60,61,62,63,64,65,66,67,68,69,70Cu, 62,63,64,65,66,67,68,69,70,71,72Zn, 66,67,68,69,70,71,72,73,74,75Ga, 68,69,70,71,72,73,74,75,76,77Ge, 70,71,72,73,74,75,76,77,78,79,80,81As, 72,73,74,75,76,77,78,79,80,81,82,83Se, 74,75,76,77,78,79,80,81,82,83,84,85Br, 76,77,78,79,80,81,82,83,84,85,86,87,88Kr; measured cross sections.
NUCLEAR REACTIONS 136Xe(p, X), E=1 GeV/nucleon; measured isotopic cross sections, kinetic energies. 79,80,81,82,83,84,85,86,87,88,89,90Rb, 81,82,83,84,85,86,87,88,89,90,91,92,93Sr, 84,85,86,87,88,89,90,91,92,93,94,95,96Y, 86,87,88,89,90,91,92,93,94,95,96,97,98,99Zr, 87,88,89,90,91,92,93,94,95,96,97,98,99,100Nb, 90,91,92,93,94,95,96,97,98,99,100,101,102,103,104Mo, 92,93,94,95,96,97,98,99,100,101,102,103,104,105,106Tc, 95,96,97,98,99,100,101,102,103,104,105,106,107,108,109Ru, 97,98,99,100,101,102,103,104,105,106,107,108,109,110,111Rh, 99,100,101,102,103,104,105,106,107,108,109,110,111,112,113,114,115Pd, 101,102,103,104,105,106,107,108,109,110,111,112,113,114,115,116,117,118,119,120,121,122Ag, 104,105,106,107,108,109,110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125Cd, 105,106,107,108,109,110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125,126,127In, 108,109,110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130Sn, 110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132Sb, 111,112,113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134Te, 113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135I, 116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135Xe, 122,123,124,125,126,127,128,129,130,131,132,133,134,135,136Cs, 127,128,129,130,131,132Ba; measured cross sections.
doi: 10.1103/PhysRevC.76.064609
Phys.Rev. C 76, 044605 (2007)
M.Notani, H.Sakurai, N.Aoi, H.Iwasaki, N.Fukuda, Z.Liu, K.Yoneda, H.Ogawa, T.Teranishi, T.Nakamura, H.Okuno, A.Yoshida, Y.X.Watanabe, S.Momota, N.Inabe, T.Kubo, S.Ito, A.Ozawa, T.Suzuki, I.Tanihata, M.Ishihara
Projectile fragmentation reactions and production of nuclei near the neutron drip line
NUCLEAR REACTIONS 9Be(40Ar, X)6Li/7Li/8Li/9Li/7Be/8Be/9Be/10Be/11Be/12Be/10B/11B/12B/13B/14B/15B/11C/12C/13C/14C/15C/16C/17C/18C/13N/14N/15N/16N/17N/18N/19N/20N/21N/15O/16O/17O/18O/19O/20O/21O/22O/23O/24O/17F/18F/19F/20F/21F/22F/23F/24F/25F/26F/27F/19Ne/20Ne/21Ne/22Ne/23Ne/24Ne/25Ne/26Ne/27Ne/28Ne/29Ne/21Na/22Na/23Na/24Na/25Na/26Na/27Na/28Na/29Na/30Na/31Na/32Na/23Mg/24Mg/25Mg/26Mg/27Mg/28Mg/29Mg/30Mg/31Mg/32Mg/33Mg/34Mg/25Al/26Al/27Al/28Al/29Al/30Al/31Al/32Al/33Al/34Al/35Al/36Al/27Si/28Si/29Si/30Si/31Si/32Si/33Si/34Si/35Si/36Si/37Si/38Si/29P/30P/31P/32P/33P/34P/35P/36P/37P/38P/39P/33S/34S/35S/36S/37S/38S/36Cl/37Cl/38Cl/39Cl/39Ar, E=100 MeV/nucleon; 181Ta(40Ar, X)6Li/7Li/8Li/9Be/10Be/11Be/10B/11B/12B/13B/14B/11C/12C/13C/14C/15C/16C/17C/13N/14N/15N/16N/17N/18N/19N/15O/16O/17O/18O/19O/20O/21O/17F/18F/19F/20F/21F/22F/23F/24F/19Ne/20Ne/21Ne/22Ne/23Ne/24Ne/25Ne/26Ne/27Ne/21Na/22Na/23Na/24Na/25Na/26Na/27Na/28Na/29Na/23Mg/24Mg/25Mg/26Mg/27Mg/28Mg/29Mg/30Mg/31Mg/24/25Al/26Al/27Al/28Al/29Al/30Al/31Al/32Al/33Al/34Al/26Si/27Si/28Si/29Si/30Si/31Si/32Si/33Si/34Si/29P/30P/31P/32P/33P/34P/35P/36P/30S/31S/32S/33S/34S/35S/36S/37S/33Cl/34Cl/35Cl/36Cl/37Cl/35Ar/36Ar/37Ar/38Ar/39Ar/37K/38K/39K/40K, E=100 MeV/nucleon; measured momentum distribution, production cross sections. RIKEN.
doi: 10.1103/PhysRevC.76.044605
iThesis, University of California Berkeley (2007)
E.Rodriguez-Vieitez
Structure and Cross Section Data of Neutron-Rich N ∼ 20 Nuclei Produced in Fragmentation and Few-Nucleon Knockout Reactions
RADIOACTIVITY 28,29,30Ne; measured Eγ, Iγ, γγ-coinc. 28,29,30Ne; deduced levels, J, π.
Nucl.Instrum.Methods Phys.Res. A589, 202 (2008)
T.Kibedi, T.W.Burrows, M.B.Trzhaskovskaya, P.M.Davidson, C.W.Nestor, Jr.
Evaluation of theoretical conversion coefficients using BrIcc
COMPILATION Z=5-110; compiled and evaluated ICC data. BrICC database.
doi: 10.1016/j.nima.2008.02.051
Phys.Rev. C 77, 034307 (2008)
M.Kowalska, D.T.Yordanov, K.Blaum, P.Himpe, P.Lievens, S.Mallion, R.Neugart, G.Neyens, N.Vermeulen
Nuclear ground-state spins and magnetic moments of 27Mg, 29Mg, and 31Mg
NUCLEAR MOMENTS 25,27,29,31Mg [from 238U(p, X), E=1.4 GeV]; measured J, π of ground states, magnetic moments, hyperfine structure using laser and β-NMR spectroscopy. Compared with shell-model calculations.
doi: 10.1103/PhysRevC.77.034307
Phys.Rev. C 77, 014316 (2008)
J.R.Terry, B.A.Brown, C.M.Campbell, J.M.Cook, A.D.Davies, D.-C.Dinca, A.Gade, T.Glasmacher, P.G.Hansen, B.M.Sherrill, H.Zwahlen, D.Bazin, K.Yoneda, J.A.Tostevin, T.Otsuka, Y.Utsuno, B.Pritychenko
Single-neutron knockout from intermediate energy beams of 30, 32Mg: "Mapping the transition into the "island of inversion"
NUCLEAR REACTIONS 9Be(30Mg, 29Mg), E=85.8 MeV/nucleon; 9Be(32Mg, 31Mg), E=75.7 MeV/nucleon; measured Eγ, Iγ, (fragment)γ-coin, cross sections; deduced spectroscopic factors. 29,31Mg; deduced levels, angular momenta, half-lives. Single-particle knockout reaction.
doi: 10.1103/PhysRevC.77.014316
Phys.Rev. C 78, 034615 (2008)
Yu.E.Titarenko, V.F.Batyaev, A.Yu.Titarenko, M.A.Butko, K.V.Pavlov, S.N.Florya, R.S.Tikhonov, S.G.Mashnik, A.V.Ignatyuk, N.N.Titarenko, W.Gudowski, M.Tesinsky, C.-M.L.Persson, H.Ait Abderrahim, H.Kumawat, H.Duarte
Cross sections for nuclide production in a 56Fe target irradiated by 300, 500, 750, 1000, 1500, and 2600 MeV protons compared with data on a hydrogen target irradiated by 300, 500, 750, 1000, and 1500 MeV/nucleon 56Fe ions
NUCLEAR REACTIONS 56Fe(p, X)7Be/22Na/24Na/27Mg/28Mg/29Al/38S/34mCl/38Cl/39Cl/41Ar/42K/43K/44K/47Ca/43Sc/44Sc/44mSc/46Sc/47Sc/48Sc/48V/48Cr/49Cr/51Cr/52Mn/52mMn/54Mn/56Mn/52Fe/53Fe/55Co/56Co/57Co, E=300, 500, 750, 1000, 1500, 2600 MeV; measured Eγ, Iγ, σ, mass distributions. 1H(56Fe, X)E=300, 500, 750, 100, 1500 MeV/nucleon; systematics of σ. 27Al(p, x)22Na; analyzed excitation function.
doi: 10.1103/PhysRevC.78.034615
Phys.Lett. B 674, 168 (2009)
A.M.Hurst, C.Y.Wu, J.A.Becker, M.A.Stoyer, C.J.Pearson, G.Hackman, M.A.Schumaker, C.E.Svensson, R.A.E.Austin, G.C.Ball, D.Bandyopadhyay, C.J.Barton, A.J.Boston, H.C.Boston, R.Churchman, D.Cline, S.J.Colosimo, D.S.Cross, G.Demand, M.Djongolov, T.E.Drake, P.E.Garrett, C.Gray-Jones, K.L.Green, A.N.Grint, A.B.Hayes, K.G.Leach, W.D.Kulp, G.Lee, S.Lloyd, R.Maharaj, J.-P.Martin, B.A.Millar, S.Mythili, L.Nelson, P.J.Nolan, D.C.Oxley, E.Padilla-Rodal, A.A.Phillips, M.Porter-Peden, S.V.Rigby, F.Sarazin, C.S.Sumithrarachchi, S.Triambak, P.M.Walker, S.J.Williams, J.Wong, J.L.Wood
Narrowing of the neutron sd-pf shell gap in 29Na
NUCLEAR REACTIONS 110Pd(29Na, 29Na'), E=70 MeV; measured Eγ, Iγ, (particle)γ-coin, charged-particle spectra following Coulomb excitation; deduced σ. 29Na; deduced B(E2). Comparison with shell model.
doi: 10.1016/j.physletb.2009.03.017
Phys.Rev. C 80, 014310 (2009)
C.J.Lin, X.X.Xu, H.M.Jia, F.Yang, F.Jia, S.T.Zhang, Z.H.Liu, H.Q.Zhang, H.S.Xu, Z.Y.Sun, J.S.Wang, Z.G.Hu, M.Wang, R.F.Chen, X.Y.Zhang, C.Li, X.G.Lei, Z.G.Xu, G.Q.Xiao, W.L.Zhan
Experimental study of two-proton correlated emission from 29S excited states
NUCLEAR REACTIONS 197Au(29S, 29S'), E=49.2 MeV/nucleon; measured particle spectra by ΔE-tof, (29S)(p)(p)-coin. 29S; deduced excitation spectrum, two proton and 2He cluster decay branching ratios.
RADIOACTIVITY 29S(2p); measured (29S)(p)(p)-coin; deduced branching ratios of two proton and 2He cluster decay modes from excited states.
doi: 10.1103/PhysRevC.80.014310
Chin.Phys.C 33, Supplement 1, 218 (2009)
D.-M.Zhou, Y.-N.Zheng, X.-Z.Zhang, D.-Q.Yuan, Y.Zuo, P.Fan, Z.-Q.Wang, H.-L.Luo, G.-J.Xu, S.-Y.Zhu
Structure of β-emitting nuclei 29P
RADIOACTIVITY 29P(β+) [from 28Si(d, n)29P, E=3 MeV]; measured decay products, β-NMR spectra; deduced magnetic moment, density distribution of protons, neutrons and matter.
doi: 10.1088/1674-1137/33/S1/070
Phys.Rev. C 81, 067303 (2010)
R.R.Reynolds, P.D.Cottle, A.Gade, D.Bazin, C.M.Campbell, J.M.Cook, T.Glasmacher, P.G.Hansen, T.Hoagland, K.W.Kemper, W.F.Mueller, B.T.Roeder, J.R.Terry, J.A.Tostevin
25Si and 29S studied via single neutron knockout reactions
NUCLEAR REACTIONS 9Be(26Si, 25Si), E=109 MeV/nucleon; 9Be(30S, 29S), E=103 MeV/nucleon, [secondary beams of 26Si and 30S from primary 9Be(36Ar, X), E=150 MeV/nucleon]; measured Eγ, Iγ, (particle)γ-coin, σ using SeGA array. 25Si, 29S; deduced levels, J, π. Comparisons with previous experimental data, mirror nuclei 25Na and 29Al, and shell model calculations.
doi: 10.1103/PhysRevC.81.067303
Priv.Comm. (2011)
G.Audi, W.Meng
Atomic Mass Evaluation 2011
INDC(NDS)-0594 (2011)
N.J.Stone
Table of nuclear magnetic dipole and electric quadrupole moments
COMPILATION Z=1-99, N=1-254; compiled experimental data on nuclear magnetic and electrical quadrupole moments.
Phys.Rev.Lett. 108, 042504 (2012)
D.T.Yordanov, M.L.Bissell, K.Blaum, M.De Rydt, Ch.Geppert, M.Kowalska, J.Kramer, K.Kreim, A.Krieger, P.Lievens, T.Neff, R.Neugart, G.Neyens, W.Nortershauser, R.Sanchez, P.Vingerhoets
Nuclear Charge Radii of 21-32Mg
ATOMIC PHYSICS 21,22,23,24,25,26,27,28,29,30,31,32Mg; measured the atomic isotope shift representing the transition frequencies with respect to the fine structure levels; deduced rms charge radii, evolution of nuclear shape through deformation regions. Comparison with theory and differential mean square radii, application of laser-induced orientation for isotope shift measurements.
doi: 10.1103/PhysRevLett.108.042504