References quoted in the ENSDF dataset: 35 REFERENCES
347 references found.
Clicking on a keynumber will list datasets that reference the given article.
Phys.Rev. 60, 537 (1941)
M.D.Kamen
Production and Isotopic Assignment of Long-Lived Radioactive Sulfur
Phys.Rev. 72, 646 (1947)
D.J.Hughes, D.Hall, C.Eggler, E.Goldfarb
Formation and Properties of Radioactive Lithium
Phys.Rev. 74, 1113 (1948); See Also 47To16 (N, Br), 49To17 (Cl)
C.H.Townes, A.N.Holden, F.R.Merritt
Microwave Spectra of Some Linear X Y Z Molecules
Phys.Rev. 76, 703 (1949)
V.W.Cohen, W.S.Koski, T.Wentink, Jr.
Nuclear Spin and Quadrupole Coupling of S35
Phys.Rev. 76, 1076 (1949)
L.Davis, Jr., B.T.Feld, C.W.Zabel, J.R.Zacharias
The Hyperfine Structure and Nuclear Moments of the Stable Chlorine Isotopes
Phys.Rev. 81, 948 (1951); See Also 49Co12
T.Wentink, Jr., W.S.Koski, V.W.Cohen
The Mass of S35 from Microwave Spectroscopy
Phys.Rev. 94, 1203 (1954); Calculated Using Data of 51We11
G.R.Bird, C.H.Townes
Sulfur Bonds and the Quadrupole Moments of O, S, and Se Isotopes
Phys.Rev. 93, 193 (1954)
B.F.Burke, M.W.P.Strandberg, V.W.Cohen, W.S.Koski
The Nuclear Magnetic Moment of S35 by Microwave Spectroscopy
Rev.Mod.Phys. 26, 95 (1954)
P.M.Endt, J.C.Kluyver
Energy Levels of Light Nuclei (Z = 11 to Z = 20)
Phys.Rev. 100, 1317 (1955)
C.H.Paris, W.W.Buechner, P.M.Endt
Energy Levels of S33, S35, Cl36, Cl38, and Ba139
NUCLEAR REACTIONS 35,37S(d, α), E=3.0-7.5 MeV; measured Eα, σ(E). 33,35S; deduced levels, Q-values. Enriched targets. Broad-range magnetic spectrograph.
Phys.Rev. 99, 620 (1955)
L.A.Toller, J.R.Patterson, H.W.Newson
Neutron Resonances in the Kilovolt Region: Cl35, Cl37, K39, and K41
NUCLEAR REACTIONS 35,37Cl, 39,41K(n, n'), E=2-200 keV; measured σ; deduced resonance features. Transmission method.
Phys.Rev. 104, 154 (1956)
O.C.Kistner, A.Schwarzschild, B.M.Rustad
Decay of A35
Rev.Mod.Phys. 29, 683 (1957)
P.M.Endt, C.M.Braams
Energy Levels of Light Nuclei (Z = 11 to Z = 20). II.
doi: 10.1103/RevModPhys.29.683
Phys.Rev. 110, 89 (1958)
P.M.Endt, C.H.Paris
Nuclear Levels in P30, S33, and S35
J.Research Natl.Bur.Standards 60, 447 (1958)
H.H.Seliger, W.B.Mann, L.M.Cavallo
Average Energy of Sulfur-35 Beta Decay
Phys.Rev. 116, 134 (1959)
J.S.Allen, R.L.Burman, W.B.Herrmannsfeldt, P.Stahelm, T.H.Braid
Determination of the Beta-Decay Interaction from Electron-Neutrino Angular Correlation Measurements
Nucleonics 17, No.10, 86 (1959)
J.P.Cali, L.F.Lowe
Direct Determination of the Half-Lives of Nine Nuclides
Science 129, 1360 (1959)
R.D.Cooper, E.S.Cotton
Half-Life of Sulfur-35
Progress in Nuclear Physics, Vol.7, p.54, Pergamon Press, New York (1959)
F.R.Metzger
Resonance fluorescence in nuclei
COMPILATION 7Li, 11B, 12C, 14N, 16O, 24Mg, 28Si, 31P, 48Ti, 51V, 56Fe, 60Ni, 63Cu, 72,74Ge, 74Se, 75As, 76Se, 96,97Mo, 141Pr, 152Sm, 196Pt, 198,199,202Hg, 203Tl; compiled experimental T1/2 of nuclear resonance fluorescence and other methods.
Izvest.Akad.Nauk SSSR, Ser.Fiz. 24, 877 (1960); Columbia Tech.Transl. 24, 878 (1961)
Yu.P.Antufev, A.K.Valter, V.Yu.Gonchar, E.G.Kopanets, A.N.Lvov, S.P.Tsytko
NUCLEAR STRUCTURE 35Cl; measured not abstracted; deduced nuclear properties.
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.
Phys.Rev. 117, 1297 (1960)
R.Wallace, J.A.Welch, Jr.
Beta Spectra of the Mirror Nuclei
NUCLEAR STRUCTURE 27Si, 25Al, 23Mg, 19Ne, 21Na, 33Cl, 35Ar, 31S, 29P, 39Ca, 41Sc, 37K; measured not abstracted; deduced nuclear properties.
Compt.rend. 253, 2944 (1961)
Y.Ozias, H.Roux, P.Boivinet, E.Calvet
Determination Microcalorimetrique des Caracteristiques d'un Element Radioactif
NUCLEAR STRUCTURE 32P, 35S; measured not abstracted; deduced nuclear properties.
Can.J.Phys. 39, 917 (1961)
R.S.Storey, L.W.Oleksiuk
Low-Lying Energy Levels in Cl-35
NUCLEAR STRUCTURE 35Cl; measured not abstracted; deduced nuclear properties.
Nucl.Sci.Eng. 11, 74 (1961)
E.I.Wyatt, S.A.Reynolds, T.H.Handley, W.S.Lyon, H.A.Parker
Half-Lives of Radionuclides. II
NUCLEAR STRUCTURE 153Sm, 147Pm, 142Pr, 22Na, 115Cd, 133Ba, 134Cs, 125Sb, 204Tl, 192Ir, 88Y, 82Br, 72Ga, 91Y, 24Na, 106Ru, 95Nb, 54Mn, 47Ca, 45Ca, 35S; 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
Arkiv Fysik 22, 400 (1962)
J.Dubois
(p, γ) Reactions on Nuclei in the Mass Region A = 30-50
NUCLEAR STRUCTURE 42Ca, 41Sc, 40Ca, 52Cr, 48V, 50V, 51V, 49V, 46Ti, 45Sc, 47V, 35Cl, 33Cl; measured not abstracted; deduced nuclear properties.
Nucl.Phys. 34, 1 (1962)
P.M.Endt, C.van der Leun
Energy Levels of Light Nuclei. III Z = 11 to Z = 20
doi: 10.1016/0029-5582(62)90806-4
Trans. Chalmars Univ.Technol., Gothenburg, No. 266 (1963)
J.Dubois
An Investigation of the S34(p, γ)Cl35 Reaction
NUCLEAR STRUCTURE 35Cl; measured not abstracted; deduced nuclear properties.
Physica 29, 681 (1963)
N.Hazewindus, W.Lourens, A.Scheepmaker, A.H.Wapstra
Gamma Ray Transitions in Cl35
NUCLEAR STRUCTURE 35Cl; measured not abstracted; deduced nuclear properties.
Phys.Rev. 129, 1723 (1963)
J.W.Nelson, E.B.Carter, G.E.Mitchell, R.H.Davis
Thresholds Observed in the C12(α, n)O15, Si28(α, n)S31, S32(α, n)Ar35, S34(α, n)Ar37, and Cl35(p, n)Ar35 Reactions
NUCLEAR STRUCTURE 12C, 15O, 31S, 35Ar, 37Ar; measured not abstracted; deduced nuclear properties.
Bull.Am.Phys.Soc. 9, No.4, 440, FA11 (1964)
A.K.Hyder, Jr., W.A.Anderson, G.I.Harris
Resonances in the 32,33,34S(p, γ)33,34,35Cl Reactions
NUCLEAR STRUCTURE 33Cl, 34Cl, 35Cl; measured not abstracted; deduced nuclear properties.
Physica 30, 899 (1964)
J.Kuperus
Protons from the alpha-particle bombardment of 31P
NUCLEAR REACTIONS 31P(α, p), E=1.7-3.3 MeV; measured Ep, Ip, σ(E, θ), resonance yield, enriched targets. 35Cl; deduced levels, J, π, resonance widths.
doi: 10.1016/0031-8914(64)90132-6
Phys.Rev. 137, B1453 (1965)
F.P.Calaprice, E.D.Commins, D.A.Dobson
Beta-Decay Asymmetry and Nuclear Magnetic Moment of Argon-35
NUCLEAR STRUCTURE 35Ar; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.137.B1453
Nucl.Sci.Eng. 22, 416 (1965)
K.F.Flynn, L.E.Glendenin, E.P.Steinberg
Half-Life Determinations by Direct Decay
NUCLEAR STRUCTURE 134Cs, 147Pm, 144Ce, 125Sb, 121Sn, 113Cd, 89Sr, 93Nb, 106Ru, 103Ru, 95Nb, 95Zr, 242Cm, 204Tl, 170Tm, 171Tm, 151Sm, 35S; measured not abstracted; deduced nuclear properties.
Phys.Rev.Letters 17, 659 (1966)
R.E.Azuma, L.W.Oleksiuk, J.D.Prentice, P.Taras
Properties of the 3.16-MeV Level of Cl35
NUCLEAR STRUCTURE 35Cl; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.17.659
Phys.Rev. 149, 791 (1966)
R.H.Bassel
Normalization of and Finite-Range Effects in (3He, d) and (t, d) Reactions
Nucl.Phys. 88, 12(1966)
G.A.P.Engelbertink, P.M.Endt
Measurements of (p, γ) Resonance Strengths in the s-d Shell
NUCLEAR REACTIONS 23Na, 24,25,26Mg, 27Al, 28,29,30Si, 31P, 32,34S, 35,37Cl, 39,41K, 40Ca(p, γ), E = 0.3-2.1 MeV; measured σ(Ep); deduced resonance strengths. Natural targets of different chemical compounds.
doi: 10.1016/0029-5582(66)90448-2
Nucl.Phys. 84, 241(1966)
F.C.Erne
Gamma-Ray Angular Correlation and Polarization Measurements in the Reaction 35Cl(p, γ)36Ar
NUCLEAR REACTIONS 35Cl(p, γ), 35Cl(p, p'γ), E = 0.733-2.595 MeV; measured p'γγ(θ, phi), γ polarization. 36Ar deduced levels, J, π, isospin, L(p), multipolarity mixings. Enriched target.
doi: 10.1016/0029-5582(66)90370-1
Nucl.Phys. 76, 248(1966)
J.H.Hough, W.L.Mouton
Nuclear Resonant Scattering of Bremsstrahlung from Low-Lying Levels in 27Al, 31P and 35Cl
NUCLEAR REACTIONS 27Al, 31P, 35Cl(γ, γ), Eγ = 1.0 to 1.3 MeV; measured σ. 27Al, 31P, 35Cl deduced level-width. Natural targets.
doi: 10.1016/0029-5582(66)90021-6
Ukr.Fiz.Zh. 11, 929 (1966)
E.G.Kopanets, Y.S.Korda, A.A.Koval, L.N.Sukhotin, S.P.Tsytko
Investigation of the 34S(p, gamma)35Cl Reaction
NUCLEAR STRUCTURE 35Cl; measured not abstracted; deduced nuclear properties.
Izv.Akad.Nauk SSSR, Ser.Fiz. 30, 407 (1966); Bull.Acad.Sci.USSR, Phys.Ser. 30, 414 (1967)
E.G.Kopanets, A.A.Koval, Y.S.Korda, L.N.Sukhotin, S.P.Tsytko
Investigation of the S34(p, γ)Cl35 Reaction at the 1904 and 2008 keV Proton Resonance Energies
NUCLEAR STRUCTURE 35Cl; measured not abstracted; deduced nuclear properties.
Phys.Rev. 151, 879 (1966)
D.B.Nichols, B.D.Kern, M.T.McEllistrem
Cross Sections of 35,37Cl(n, n'γ) Reactions
NUCLEAR STRUCTURE 37Cl, 35Cl; measured not abstracted; deduced nuclear properties.
Phys.Rev. 147, 829 (1966)
J.P.Schiffer, L.L.Lee, Jr., A.Marinov, C.Mayer-Boricke
Dependence of the Angular Distribution of the (d, p) Reaction on the Total Angular-Momentum Transfer. II
NUCLEAR STRUCTURE 35S, 33S, 29Si, 12C, 16O, 13C, 17O, 19F, 20F, 95Zr, 91Zr, 93Zr; measured not abstracted; deduced nuclear properties.
Phys.Letters 22, 183 (1966)
D.D.Watson
Spin and Parity of the 3.16 MeV and 7.54 MeV Levels in 35Cl
NUCLEAR STRUCTURE 35Cl; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(66)90567-1
Z.Physik 205, 8 (1967)
D.A.E.Darwish, S.A.El-Kateb, L.M.El-Nadi, O.E.Badawy, A.N.Lvov
The S34(p, γ)Cl35 Reaction and Energy Levels of the Cl35 Nucleus
NUCLEAR STRUCTURE 35Cl; measured not abstracted; deduced nuclear properties.
Nucl.Phys. A105, 1 (1967); Erratum Nucl.Phys. A115, 697 (1968)
P.M.Endt, C.Van der Leun
Energy Levels of Z=11-21 Nuclei (IV)
doi: 10.1016/0375-9474(67)90916-5
Izv.Akad.Nauk SSSR, Ser.Fiz. 31, 626 (1967); Bull.Acad.Sci.USSR, Phys.Ser. 31, 621 (1968)
E.G.Kopanets, A.A.Koval, Y.S.Korda, L.N.Sukhotin, S.P.Tsytko
Investigation of the Gamma Rays from Inelastic Scattering of Protons on 34S
NUCLEAR STRUCTURE 35Cl; measured not abstracted; deduced nuclear properties.
Izv.Akad.Nauk SSSR, Ser.Fiz. 31, 631 (1967); Bull.Acad.Sci.USSR, Phys.Ser. 31, 626 (1968)
E.G.Kopanets, A.A.Koval, L.N.Sukhotin, S.P.Tsytko
Spin and Parity Assignments for the 3.01 and 2.65 MeV Levels of 35Cl
NUCLEAR REACTIONS 34S(p, γ), E=2.079 MeV; measured σ(Eγ, θ(γ), θ(pγ), θ(γγ)). 35Cl deduced levels, J, π, level-width, γ-multipolarity.
Yadern.Fiz. 6, 233 (1967); Soviet J.Nucl.Phys. 6, 170 (1968)
E.G.Kopanets, Y.S.Korda, A.A.Koval, L.N.Sukhotin, S.P.Tsytko
p-γ-γ Triple Angular Correlations from the Reactions S34(p, γ)Cl35
NUCLEAR STRUCTURE 35Cl; measured not abstracted; deduced nuclear properties.
Nucl.Sci.Appl. 3, No.2, 44 (1967)
J.C.Manthuruthil, F.D.Lee, D.D.Watson
Analog States Through the S34(p, γ)Cl35 Reaction
NUCLEAR STRUCTURE 35Cl; measured not abstracted; deduced nuclear properties.
Phys.Rev. 164, 1386 (1967)
P.Taras, L.W.Oleksiuk, R.E.Azuma, J.D.Prentice
Properties of Some Levels of Cl35
NUCLEAR STRUCTURE 35Cl; measured not abstracted; deduced nuclear properties.
Phys.Rev. 164, 1399 (1967)
D.D.Watson, J.C.Manthuruthil, F.D.Lee
Isobaric Analog States in Cl35
NUCLEAR STRUCTURE 35Cl; measured not abstracted; deduced nuclear properties.
Nucl.Phys. A109, 577(1968)
R.E.Azuma, N.Anyas-Weiss, A.M.Charlesworth
Lifetime of the 3.163 MeV Level of 35Cl
NUCLEAR REACTIONS 34S(p, γ), E=1.214, 1.513 MeV; measured Doppler-shift attenuation, γγ-delay. 35Cl level deduced T1/2. Enriched target.
doi: 10.1016/0375-9474(68)90028-6
Nucl.Phys. A108, 113(1968)
R.R.Johnson, R.J.Griffiths
The 40Ar(p, d)39Ar and 36Ar(p, d)35Ar Reactions at 27.5 MeV
NUCLEAR REACTIONS 36,40Ar(p, d), E = 27.5 MeV; measured σ(Ed, θ). 35,39Ar deduced levels, L(n), , S. Enriched 36Ar target.
doi: 10.1016/0375-9474(68)90148-6
Phys.Rev. 172, 1078 (1968)
R.L.Kozub
(p, d) Reaction on N = Z Nuclei in the 2s-1d shell
NUCLEAR REACTIONS 24Mg, 28Si, 32S, 36Ar, 40Ca(p, d), E=33.6 MeV; measured σ(Ed, θ). 23Mg, 27Si, 31S, 35Ar, 39Ca deduced levels, J, π.
Phys.Rev. 173, 1101 (1968)
L.K.ter Veld, T.W.van der Mark
First Excited State of 35S
NUCLEAR STRUCTURE 35S; measured not abstracted; deduced nuclear properties.
J.Inorg.Nucl.Chem. 30, 1373 (1968)
E.J.Woodhouse, T.H.Norris
Half-Life of Sulphur-35
NUCLEAR STRUCTURE 35S; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0022-1902(68)80275-1
Arkiv Fysik 38, 585 (1969)
H.Ahlgren, J.Dubois, H.Linusson
A Study of the 34S(p, γ)35Cl Reaction
NUCLEAR REACTIONS 34S(p, γ), E = 1.019-1.267 MeV; measured σ(E;Eγ). 35Cl deduced resonances, J, level-width. 35Cl deduced levels. Ge(Li) detector.
Izv.Akad.Nauk SSSR, Ser.Fiz. 33, 1721 (1969); Bull.Acad.Sci.USSR, Phys.Ser. 33, 1576 (1970)
A.E.Antropov, P.P.Zarubin, P.D.Ioannu, B.N.Orlov, A.V.Plavko, V.F.Pomytkin, V.S.Romanov, A.I.Sorokin
Elastic and Inelastic Proton Scattering on 33S, 34S and 35Cl
NUCLEAR REACTIONS 33,34S, 35Cl(p, p), (p, p'), E=6 MeV; measured σ(Ep', θ). 33S, 35Cl deduced levels, L, J. Enriched targets.
Phys.Rev. 182, 1168 (1969)
N.E.Davison, J.T.Sample, W.J.McDonald, W.J.Wiesehahn, R.E.Azuma, J.D.Prentice
Levels in 35Cl Populated by 34S(d, n)35Cl
NUCLEAR REACTIONS 34S(d, n), E=4.95 MeV; measured σ(En, θ). 35Cl levels deduced J, π, L(p).
Phys.Rev. 185, 1515 (1969)
D.D.Duncan, K.H.Buerger, R.L.Place, B.D.Kern
Low-Lying Levels of 35Cl and 37Cl
NUCLEAR REACTIONS 35,37Cl(p, p'γ), E = 4.6-6.2 MeV; measured σ(E;Ep', Eγ, θ(γ), θ(p'γ)), Doppler shift attenuation. 35,37Cl levels deduced J, π, level-width, T1/2, γ-branching, γ-mixing.
Phys.Letters 30B, 240 (1969)
J.M.Freeman, D.C.Robinson, G.L.Wick
Magnitude of the Vector Coupling Constant Deduced from Recent Beta Decay Measurements
RADIOACTIVITY 10C, 35Ar; measured Eγ, Iγ; deduced log ft, vector coupling constant.
doi: 10.1016/0370-2693(69)90427-4
Nucl.Phys. A136, 577 (1969)
A.Graue, L.H.Herland, J.R.Lien, G.E.Sandvik, E.R.Cosman, W.H.Moore
A Study of the 35Cl Levels by Means of the 34S(3He, d)35Cl Reaction
NUCLEAR REACTIONS 34S(3He, d), E = 11.0 MeV; measured σ(Ed, θ), Q; deduced transition strengths. 35Cl deduced levels, S, L(p), isospin, analog states.
doi: 10.1016/0375-9474(69)90129-8
Can.J.Phys. 47, 1065 (1969)
O.Hausser, D.Pelte, T.K.Alexander, H.C.Evans
Coulomb Excitation of 35Cl Projectiles
NUCLEAR REACTIONS 12C, 24Mg(35Cl, 35Cl'γ), E = 51-61 MeV; measured Eγ, Iγ(θ), Doppler-shift attenuation. 35Cl deduced levels, T1/2, γ-mixing, γ-branching, transition strengths. Ge(Li) detector.
Can.J.Phys. 47, 1295(1969)
F.Ingebretsen, T.K.Alexander, O.Hausser, D.Pelte
Lifetime Measurements of the Six Lowest Lying Levels in 35Cl
NUCLEAR REACTIONS 32S(α, pγ), E = 7-9 MeV; measured Eγ, Doppler shift attenuation. 35Cl deduced levels, T1/2, γ-branching, J. Ge(Li) detectors.
Izv.Akad.Nauk SSSR, Ser.Fiz. 33, 711 (1969); Bull.Acad.Sci.USSR, Phys.Ser. 33, 655 (1970)
E.G.Kopanets
Analog States in 35Cl
NUCLEAR REACTIONS 34S(p, γ), E < 2.8 MeV; measured nothing, reanalyzed data. 35Cl deduced resonances, anti-analog state, γ-branching. Summarizes previous work.
Bull.Am.Phys.Soc. 14, No.12, 1222, CC12 (1969)
M.Kregar, P.Kump, V.Ramsak, M.Vakselj, M.Zupan, D.Brajnik, U.Miklavzic
Properties of Some Excited States in 35Cl
Intern.J.Appl.Radiation Isotopes 20, 868 (1969)
F.Lagoutine, J.Legrand, Y.Le Gallic
Periodes de Quelques Radionucleides
RADIOACTIVITY 32P, 35S, 110mAg, 170Tm, 199Au; measured T1/2.
doi: 10.1016/0020-708X(69)90113-6
Ukr.Fiz.Zh. 14, 1198 (1969)
V.Y.Migalenya, E.G.Kopanets, A.M.Lvov, A.P.Gaidamaka, A.O.Koval, V.Y.Kostin, S.P.Tsitko
The 3.95 MeV Level and Decay Scheme of the 8.38 MeV Isobar-Analog State in Cl35
NUCLEAR REACTIONS 34S(p, γ), E=2.079 MeV; measured Eγ, Iγ. 35Cl deduced levels, analogstate, γ-branching.
Nucl.Phys. A131, 235 (1969)
G.E.Moss
Excitation Energies of Levels in 35S
NUCLEAR REACTIONS 34S(d, p), E=6.495 MeV; measured σ(Ep). 35S deduced levels. Enriched target.
doi: 10.1016/0375-9474(69)90821-5
Can.J.Phys. 47, 1605 (1969)
P.Taras, J.Matas
Properties of the 1.763 MeV Level in 35Cl
NUCLEAR REACTIONS 35Cl(p, p'γ), E = 3.05-3.37 MeV; measured σ(E;Eγ, θ(γ)), γ linear polarization. 35Cl level deduced J, π, γ-mixing.
Nucl.Phys. A138, 209 (1969)
G.L.Wick, D.C.Robinson, J.M.Freeman
A New Measurement of the ft Value for the Mirror Decay 35Ar(β+)35Cl and a Calculation of the Vector Coupling Constant
RADIOACTIVITY 35Ar; measured Eγ, Iγ, T1/2; deduced Eβ, log ft, β-branching, vector coupling constant. Natural targets, Ge(Li) detector.
NUCLEAR REACTIONS 35Cl(p, n), E approx 6.9 MeV; measured threshold; deduced Q.
doi: 10.1016/0375-9474(69)90393-5
Nucl.Phys. A154, 551 (1970)
K.S.Burton, L.C.McIntyre, Jr.
Mean Lives and Angular Correlations in 35S with the 34S(d, pγ)35S Reaction
NUCLEAR REACTIONS 34S(d, pγ), E=2.00-3.25 MeV; measured Doppler-shift attenuation, σ(E;Ep, Eγ, θ(pγ)). 35S deduced levels, T1/2, J, γ-branching, γ-mixing. Enriched target.
doi: 10.1016/0375-9474(70)90126-0
Can.J.Phys. 48, 1259 (1970)
B.W.Hooton, O.Hausser, F.Ingebretsen, T.K.Alexander
Level Structure of 35Cl from the 32S(α, pγ)35Cl Reaction
NUCLEAR REACTIONS 32S(α, pγ), E=10.975, 11.960, 12.120 MeV; measured σ(Ep, Eγ, θ(pγ)). 35Cl deduced levels, J, π, γ-branching, γ-mixing.
Phys.Lett. 31B, 297 (1970)
F.Ingebretsen, C.Broude, J.S.Forster
Properties of the 3942 keV Level in 35Cl and Evidence for a Ground State Rotational Band
NUCLEAR REACTIONS 32S(α, pγ), E=10 MeV; measured Doppler shift attenuation, Eγ. 35Cl deduced levels, T1/2, π, ground-state rotational band, branching ratios, γ-mixing.
doi: 10.1016/0370-2693(70)90176-0
Izv.Akad.Nauk SSSR, Ser.Fiz. 34, 2101 (1970); Bull.Acad.Sci. USSR, Phys.Ser. 34, 1873 (1971)
E.G.Kopanets, V.Y.Migalenya, A.N.Lvov, A.A.Koval, V.Y.Kostin, A.P.Gaidamaka, S.P.Tsytko
Search for a 2p1/2 Analog State in 35Cl
NUCLEAR REACTIONS 34S(p, γ), E=2317, 2223, 2336 keV; measured Eγ, Iγ, pγ(θ). 35Cl analog resonances deduced J, levels, γ-branching. Ge(Li) detector.
Nucl.Phys. A140, 97 (1970)
R.A.Morrison
A Study of Nuclei with Masses Near 32 with the (3He, d) Reaction
NUCLEAR REACTIONS 30Si, 31P, 32S(3He, d), 30Si, 31P(3He, 3He), E =15 MeV; 34S(3He, d), E=13 MeV; measured σ(θ). 31P, 32S, 33,35Cl deduced levels, J, π, L(p), S.
doi: 10.1016/0375-9474(70)90887-0
Can.J.Phys. 48, 603 (1970)
P.Taras, J.Matas
Properties of the 2.645, 2.693, 3.001, and 3.162 MeV Levels in 35Cl
NUCLEAR REACTIONS 35Cl(p, p'γ), E=4.2-5.2 MeV; measured σ(E;Eγ, θ(γ)), γ-linear polarization. 35Cl deduced levels, branching ratios, J, π, γ-mixing, transition strengths.
Nucl.Instrum.Methods 77, 10 (1970)
P.Taras, J.Matas
Analysis of Linear Polarization Measurements of Unresolved Gamma Rays
NUCLEAR REACTIONS 35Cl(p, p'γ), E=5.11 MeV; measured γ-linear polarization. 35Cl transitions deduced γ-mixing.
Phys.Rev. C2, 1378 (1970)
C.J.Umbarger, K.W.Kemper, J.W.Nelson, H.S.Plendl
Excitation Functions for the Reactions 34S(p, n)34Cl and 31P(α, n)34Cl
NUCLEAR REACTIONS 34S(p, n), E=6.3-8.0 MeV; 31P(α, n), E=6.3-7.2 MeV; measured σ(E;θ); deduced thresholds. 35Cl deduced resonances, T.
Phys.Rev. C1, 1455 (1970)
C.A.Whitten, Jr., M.C.Mermaz, D.A.Bromley
Study of the (d, t) Reaction on Si28, S32, and Ar36
NUCLEAR REACTIONS 28Si, 32S, 36Ar(d, t), E=22, 21 MeV; measured σ(Et, θ). 27Si, 31S, 35Ar levels deduced L(n), S.
Nucl.Phys. A176, 284 (1971)
A.G.Artukh, V.V.Avdeichikov, G.F.Gridnev, V.L.Mikheev, V.V.Volkov, J.Wilczynski
New Isotopes 29,30Mg, 31,32,33Al, 33,34,35,36Si, 35,36,37,38P, 39,40S and 41,42Cl Produced in Bombardment of a 232Th Target with 290 MeV 40Ar Ions
NUCLEAR REACTIONS 232Th(40Ar, X), E=290 MeV; measured fragments isotopic yields; deduced evidence for 27,28,29,30Mg, 29,30,31,32,33Al, 31,32,33,34,35,36Si, 33,34,35,36,37,38P, 36,37,38,39,40S, 37,38,39,40,41,42Cl, 39,40,41,42,43,44Ar.
doi: 10.1016/0375-9474(71)90270-3
Phys.Rev. C4, 2291 (1971)
L.S.August, P.Shapiro, L.R.Cooper, C.D.Bond
J Dependence for L = 2 (α, p) Transitions in s-d Shell Nuclei
NUCLEAR REACTIONS 24Mg, 32S(α, p), E=28.8 MeV; measured σ(θ); deduced J-dependence for L=2 transitions.
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.
Drukkerij Elinkwijk-Utrecht (1971)
W.Bruynesteyn
Elastische Protonenverstrooiing aan 34S en 35Cl
NUCLEAR REACTIONS 34S(p, p), E=700-950 and 1500-2250 keV; 35Cl(p, p), E=600-3100 keV; 36Cl, 36Ar; measured proton spectra; deduced resonances.
Nucl.Phys. A176, 273 (1971)
J.M.G.Caraca, R.D.Gill, P.B.Johnson, H.J.Rose
Transition Strengths in 37Ar and 35Cl
NUCLEAR REACTIONS 37Cl(p, nγ), 35Cl(p, p'), E=4.15-6.15 MeV; measured Doppler-shift attenuation. 37Ar, 35Cl deduced T1/2. Natural target.
doi: 10.1016/0375-9474(71)90269-7
Phys.Lett. 34B, 128 (1971)
C.Detraz, C.E.Moss, C.S.Zaidins
Beta Decay of 23Mg, 27Si, 31S, 35Ar and 39Ca
RADIOACTIVITY 23Mg, 27Si, 31S, 35Ar, 39Ca; measured β-delayed γ-spectra; deduced log ft, branching ratios.
doi: 10.1016/0370-2693(71)90686-1
Amer.J.Phys. 39, 131 (1971)
W.R.French, Jr., W.M.Wehrbein, D.Goss, J.K.Gasper
Determination of Energy Levels in Stable Nuclei by Neutron Inelastic Scattering
NUCLEAR REACTIONS Na, Al, Mg, Cl, Cu, Zn, Pb, Fe(n, n'γ), E < 10 MeV; measured Eγ, Iγ. 23Na, 24,26Mg, 27Al, 35,37Cl, 63,65Cu, 64,66,68Zn, 54,56Fe, 206,207,208Pb deduced transitions.
Can.J.Phys. 49, 663 (1971)
J.S.Geiger, B.W.Hooton
Beta Decay of 35Ar
RADIOACTIVITY 35Ar; measured Eγ, Iγ, T1/2; deduced log ft.
Z.Naturforsch. 26a, 1933 (1971)
W.Grimm, W.Herzog
Phosphor-35 - ein neues Nuklik
RADIOACTIVITY 35P; measured T1/2, Eγ.
Izv.Akad.Nauk SSSR, Ser.Fiz. 35, 1676 (1971); Bull.Acad.Sci.USSR, Phys.Ser. 35, 1526 (1972)
E.G.Kopanets, A.N.Lvov, V.Y.Migalenya, V.Y.Kostin, A.A.Koval, S.P.Tsytko
Proton Radiative Capture and Isobaric-Analog States in 27Al, 35Cl, and 41K
NUCLEAR REACTIONS 26Mg, 34S, 40Ar(p, γ), E=0.8-3 MeV; measured pγγ-triple correlations, σ(E;Eγ, θ(γ)). 27Al, 35Cl, 41K deduced isobaric analog resonances, J, π, level-width, γ-branching.
Izv.Akad.Nauk SSSR, Ser.Fiz. 35, 1684 (1971); Bull.Acad.Sci.USSR, Phys.Ser. 35, 1533 (1972)
R.P.Kolalis, Y.A.Nemilov, V.S.Romanov, V.S.Sadkovskii, E.D.Teterin, K.A.Gridnev, A.E.Denisov
(d, p) and (d, α) Reactions on 34S for 6.6 MeV Deuterons
NUCLEAR REACTIONS 34S(d, p), (d, α), E=6.6 MeV; measured σ(Ep, θ), σ(Eα, θ). 32P, 35S deduced levels, J, π, S.
Izv.Akad.Nauk SSSR, Ser.Fiz. 35, 1682 (1971); Bull.Acad.Sci.USSR, Phys.Ser. 35, 1531 (1972)
E.G.Kopanets, V.Y.Migalenya, A.N.Lvov, A.A.Koval, V.Y.Kostin, S.P.Tsytko
Behavior of (p, γ)-Reaction Excitation Functions Near Isobaric Analog Resonances
NUCLEAR REACTIONS 26Mg, 34S, 40Ar(p, γ), E < 3 MeV; analyzed σ(E). 35Cl, 35S deduced isobaric analog states.
Z.Phys. 247, 453 (1971)
W.R.McMurray, D.M.Holz, I.J.van Heerden, G.Wiechers
Study of the Reactions 31P(α, p)34S and 29Si(α, n)32S
NUCLEAR REACTIONS 31P(α, pγ), 29Si(α, nγ), E=3-5.3 MeV; measured σ(E;θ). 35Cl, 33S deduced levels, resonances, level-width, J.
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.
Phys.Rev. C4, 1611 (1971)
F.W.Prosser, Jr., G.I.Harris
Gamma-Ray Transitions in A = 35 Nuclei
NUCLEAR REACTIONS 34S(p, γ), E approx 1.2 MeV; measured σ(E;Eγ, θ(γ)), Doppler shifts. 34S(d, pγ), E=4.48 MeV; measured pγ-delay. 35S level deduced T1/2. 35Cl deduced levels, J, π, γ-branching, γ-multipolarity.
Can.J.Phys. 49, 328 (1971)
P.Taras
Gamma-Ray Linear Polarization and Angular Distribution Formulas in Terms of Phase-Defined Reduced Matrix Elements
NUCLEAR REACTIONS 35Cl(p, p'γ), E=3.115 MeV; measured nothing; analyzed Iγ(θ), γ-linear polarization data. 35Cl level deduced J, γ-mixing.
Nucl.Phys. A170, 607 (1971)
J.G.van der Baan, H.G.Leighton
Investigation of the 34S(d, p)35S Reaction at E = 10 MeV
NUCLEAR REACTIONS 34S(d, p), E=10 MeV; measured Q , σ(θ). 35S deduced levels, L, J, π, S. Enriched target.
doi: 10.1016/0375-9474(71)90240-5
Nucl.Phys. A162, 82 (1971)
B.Vignon, J.F.Burandet, N.Longequeue, I.S.Towner
Analysis of the 35,37Cl(p, t) and (p, 3He) Reactions to Mirror and Analogue States
NUCLEAR REACTIONS 35,37Cl(p, t), 35,37Cl(p, 3He), E=40 MeV; measured σ(θ). 33Cl, 33S, 35Cl, 35S deduced levels, J, π, T, L, isobaric analogs. Natural gas target, isotopic AgCl target.
doi: 10.1016/0375-9474(71)90487-8
Can.J.Phys. 49, 2396 (1971)
W.J.Wiesehahn
Levels in 35Cl: Experimental
NUCLEAR REACTIONS 34S(p, γ), E approx 1-1.5 MeV; measured Doppler shift attenuation, σ(E;Eγ, θ(γ)), γ-linear polarization. 35Cl deduced resonances, level-width, levels, T1/2, J, π, γ-branching, γ-mixing.
Phys.Rev. C6, 842 (1972)
K.E.Apt, J.D.Knight
Decay of 35P
RADIOACTIVITY 35P; measured T1/2, Eγ, Iγ; deduced log ft, J, π.
Z.Naturforsch. 27a, 72 (1972)
J.Blaser, O.Lutz, W.Steinkilberg
Nuclear Magnetic Resonance Studies of 35Cl, 37Cl, 79Br, and 81Br in Aqueous Solution
NUCLEAR MOMENTS 2H, 35,37Cl, 79,81Br; measured ν ratios. 35,37Cl, 79,81Br deduced μ. NMR.
Nucl.Phys. A192, 291 (1972)
C.Broude, J.S.Forster, F.Ingebretsen
Electromagnetic Transition Strengths in 35Cl
NUCLEAR REACTIONS 32S(α, p), E=10 MeV; measured Eγ, Doppler-shift attenuation. 35Cl deduced levels, J, π, T1/2. Natural target.
doi: 10.1016/0375-9474(72)90260-6
Phys.Rev. C6, 1298 (1972)
J.E.Brock, I.A.Luketina, A.R.Poletti
Lifetime Measurements in 35Cl and 37Cl
NUCLEAR REACTIONS 35,37Cl(p, p'), (p, α), 37Cl(p, n), E=6 MeV; measured DSA, Eγ. 35,37Cl deduced levels, T1/2, level-width.
Yad.Fiz. 15, 1093 (1972); Sov.J.Nucl.Phys. 15, 605 (1972)
J.D.Jafar, A.A.Abdullah, N.K.Al-Kuraishi, M.S.Alvash, M.A.Khalil, A.M.Demidov
Spectra of γ Rays Produced in Si30 and S34 Capture of Thermal Neutrons
NUCLEAR REACTIONS 30Si, 34S(n, γ), E=thermal; measured Eγ, Iγ; deduced Q. 31Si, 35S deduced levels, J, π, γ-branching.
Nucl.Phys. A197, 529 (1972)
R.M.Freeman, R.Faerber, M.Toulemonde, A.Gallmann
Etude de Transitions γ dans le Noyau 35S
NUCLEAR REACTIONS 34S(d, pγ), E=3.50, 4.00 MeV; measured Eγ, DSA, σ(Ep, Eγ, θ(pγ)). 35S deduced levels, γ-branching ratios, J, γ-mixing, T1/2. Enriched target.
doi: 10.1016/0375-9474(72)91027-5
Phys.Rev. C6, 820 (1972)
D.R.Goosman, D.E.Alburger
Mass and Decay of a Highly Neutron-Rich Isotope of Phosphorus: 48-sec 35P
RADIOACTIVITY 35P; measured Eγ, βγ-coin, T1/2; deduced J, π, log ft, Q. 35S deduced levels.
Nucl.Phys. A195, 485 (1972)
P.Hubert, M.M.Aleonard, D.Castera, F.Leccia, P.Mennrath
Etude des Etats Excites du Noyau 35Cl (I). Courbe d'Excitation de la Reaction 34S(p, γ)35Cl, Energie et Rapports d'Embranchement des Niveaux du 35Cl
NUCLEAR REACTIONS 34S(p, γ), E=0.7-2.1 MeV; measured σ(E;Eγ), Q. 35Cl deduced resonances, levels, γ-branching.
doi: 10.1016/0375-9474(72)91071-8
Nucl.Phys. A195, 502 (1972)
P.Hubert, M.M.Aleonard, D.Castera, F.Leccia, P.Mennrath
Etude des Etats Excites du 35Cl (II). Vies Moyennes
NUCLEAR REACTIONS 34S(p, γ)35Cl, E=0.7-2.1 MeV; measured Doppler-shift attenuation. 35Cl levels deduced T1/2, J, π.
doi: 10.1016/0375-9474(72)91072-X
Bull.Amer.Phys.Soc. 17, No.10, 892, AB9 (1972)
F.D.Lee, D.D.Watson
Gamma Decay of Excited States of Cl35
NUCLEAR REACTIONS 34S(p, γ), E approx 1111 keV; measured σ(Eγ, θ(γγ)). 35Cl levels deduced J, γ-mixing, γ-branching.
Phys.Rev. C6, 196 (1972)
I.A.Luketina, J.E.Brock, A.R.Poletti
Lifetime Measurements in Ar37
NUCLEAR REACTIONS 37Cl(p, nγ), E=3.45-6.0 MeV; measured DSA, Eγ, Iγ. 35Cl(p, p'γ), E=3.45-6.0 MeV; measured Eγ. 37Ar deduced levels, J, π, γ-branching, T1/2. 35Cl deduced transition.
Nucl.Phys. A188, 461 (1972)
N.Shikazono, Y.Kawarasaki
Study of Odd-A Nuclei in the 2s-1d Shell by Means of the (γ, γ') Reaction
NUCLEAR REACTIONS 19F, 23Na, 27Al, 31P, 35Cl, 39K(γ, γ'), E(max)=14 MeV(γ from bremsstrahlung); measured Eγ, Iγ. 19F, 23Na, 27Al, 31P deduced levels, level-width. Natural target.
doi: 10.1016/0375-9474(72)90214-X
Phys.Rev. A6, 1702 (1972)
R.M.Sternheimer
Quadrupole Shielding and Antishielding Factors for Several Atomic Ground States
NUCLEAR MOMENTS 27Al, 35,36,37Cl, 63,65Cu, 67,68,69,71,72Ga; measured nothing. calculated Sternheimer correction. Deduced Q.
Nucl.Phys. A183, 651 (1972)
R.J.Van Reenen, W.J.Naude, W.L.Mouton
Lifetimes of the First Six Excited States of 35Cl
NUCLEAR REACTIONS 35Cl(p, p'γ), E=5.47 MeV to 5.61 MeV; measured Doppler-shift attenuation. 35Cl levels deduced T1/2. Enriched target.
doi: 10.1016/0375-9474(72)90362-4
Nucl.Phys. A181, 196 (1972)
T.W.van der Mark, L.K.ter Veld
Angular Correlations and Decay of Excited States in 35S
NUCLEAR REACTIONS 34S(d, pγ), E=4.72 MeV; 37Cl(d, αγ), E=4.25 MeV; measured σ(Eα, Ep, θ(pγ)). 35S deduced levels, J, γ-branching, multipole mixing. Enriched targets.
doi: 10.1016/0375-9474(72)90912-8
Phys.Scr. 8, 129 (1973)
N.G.Alenius, E.Wallander
High Spin States in 35Cl from the 32S(α, p)35Cl Reaction
NUCLEAR REACTIONS 32S(α, pγ), E=12-16 MeV; measured σ(E, Eγ, θ), γγ(θ). 35Cl deduced levels, J, π.
Nucl.Phys. A201, 513 (1973)
N.Anyas-Weiss, R.Griffiths, N.A.Jelley, W.Randolph, J.Szucs, T.K.Alexander
Lifetimes in 22Ne, 22Na, 30Si, 30P and 35Cl Using the Recoil-Distance Method
NUCLEAR REACTIONS 19F(α, p), 19F(α, n), 27Al(α, p), 27Al(α, n), 32S(α, p), E=5.5, 8.6 MeV; measured recoil distance. 22Ne, 22Na, 30Si, 30P, 35Cl levels deduced T1/2. Natural targets.
doi: 10.1016/0375-9474(73)90317-5
Phys.Rev. C8, 660 (1973)
R.R.Betts, H.T.Fortune, R.Middleton
Neutron Pickup from 36Ar
NUCLEAR REACTIONS 36Ar(3He, α), E=18 MeV; measured σ(Eα, θ). 35Ar deduced levels, L(n), J, π, S.
Lett.Nuovo Cim. 8, 342 (1973)
F.Brandolini, M.De Poli, C.Rossi Alvarez
Lifetimes of the First 7/2- Levels in 35Cl and 37Cl
NUCLEAR REACTIONS 32,34S(α, pγ), E=11.2 MeV; measured recoil distance, γp-coin. 35,37Cl levels deduced T1/2.
Atomkernenergie 21, 203 (1973)
M.N.H.Comsan, M.A.Farouk, A.Z.El-Behay
Fluctuation Study of the 34S(d, p)35S Reaction
NUCLEAR REACTIONS 34S(d, p), E=1.8-2.5 MeV; measured σ(E;Ep, θ). 36Cl level deduced level-width, T1/2.
Nucl.Phys. A214, 1 (1973); Erratum Nucl.Phys. A248, 153 (1975)
P.M.Endt, C.Van der Leun
Energy Levels of A = 21-44 Nuclei (V)
COMPILATION A=21-44; compiled level schemes.
doi: 10.1016/0375-9474(73)91131-7
Z.Phys. 260, 185 (1973)
B.Fant, J.Keinonen, A.Anttila, M.Bister
Investigation of Gamma Ray Transitions and Lifetimes in 35Cl
NUCLEAR REACTIONS 34S(p, γ), E=1-2 MeV; measured Eγ, Iγ, DSA. Deduced Q. 35Cl deduced levels, T1/2, resonances, γ-branching.
Phys.Rev. C7, 1871 (1973)
J.D.Goss, H.Stocker, N.A.Detorie, C.P.Browne, A.A.Rollefson
States of 35Cl via the 32S(α, p)35Cl Reaction
NUCLEAR REACTIONS 32S(α, p), E=20.0, 20.28 MeV; measured σ(Ep, θ). 35Cl deduced levels.
Phys.Rev. C7, 1120 (1973)
E.K.Warburton, J.W.Olness, G.A.P.Engelbertink, T.K.Alexander
Doppler-Shift Attenuation Measurements of Lifetimes for (2s-1d)-Shell Nuclei Excited by Heavy-Ion Bombardment of 2H
NUCLEAR REACTIONS 2H(18O, pγ), E=26.2 MeV; 2H(19F, pγ), E=24.6 MeV; 2H(32S, pγ), (32S, nγ), E=54.6 MeV; 2H(34S, pγ), (34S, nγ), E=59.6 MeV; 2H(35Cl, pγ), (35Cl, nγ), E=57.4 MeV; 2H(37Cl, pγ), E=57.4 MeV; measured Eγ, Iγ, Doppler shift attenuation. 19O, 20F, 33S, 33Cl, 35S, 35Cl, 36Cl, 36Ar, 38Cl levels deduced T1/2.
Phys.Lett. 49B, 40 (1974)
M.M.Aleonard, C.Boursiquot, P.Hubert, P.Mennrath
Strengths of (p, γ) Resonances in 33Cl, 35Cl and 28Si
NUCLEAR REACTIONS 27Al(p, γ), E=633, 744 keV; 34S(p, γ), E=1214 keV; 32S(p, γ), E=580, 588 keV; measured σ(Eγ). 28Si, 33,35Cl deduced absolute resonance strength.
doi: 10.1016/0370-2693(74)90575-9
Phys.Fenn. 9, 23 (1974)
M.Bister, A.Anttila, J.Keinonen, B.Fant
Isobaric Analog Resonances in 35Cl
NUCLEAR REACTIONS 34S(p, p), (p, γ), E=1.21, 1.51, 1.90, 2.07 MeV; measured σ(E, θ), σ(E, Eγ, θ). 35Cl deduced analog resonances, p-width, J, π.
Nucl.Phys. A230, 329 (1974)
P.Doll, H.Mackh, G.Mairle, G.J.Wagner
Comparative Spectroscopy with the (d, τ) Reaction on Even Ar Isotopes
NUCLEAR REACTIONS 36,38Ar(d, 3He), E=52 MeV; measured σ(E(3He), θ). 35,37Cl deduced levels, S, J, π. Enriched targets.
doi: 10.1016/0375-9474(74)90311-X
Can.J.Phys. 52, 1090 (1974)
D.A.Hutcheon, D.C.S.White, W.J.McDonald, G.C.Neilson
Lifetimes of 7/2- States in 35Cl, 37Cl, and 39K
NUCLEAR REACTIONS 35,37Cl, 39K(p, p'γ), E=5.65 MeV; measured Eγ, Iγ, γ(t). 35,37Cl, 39K levels deduced T1/2.
Yad.Fiz. 19, 1181 (1974); Sov.J.Nucl.Phys. 19, 603 (1975)
L.V.Ilenko, E.A.Rudak
Gamma Decay of Resonance States from the Reaction 34S(p, γ)35Cl
NUCLEAR REACTIONS 34S(p, γ), E=0.7-2.4 MeV; measured nothing, analyzed published data. 35Cl resonances deduced J, π, configuration.
Nucl.Phys. A218, 333 (1974)
P.M.Johnson, M.A.Meyer, D.Reitmann
A Study of the 35Cl(p, γ)36Ar Reaction and the Energy Levels of 36Ar
NUCLEAR REACTIONS 35Cl(p, γ), (p, p), E=0.4-3.0 MeV; measured σ(E, Eγ), Eγ, Iγ, Doppler-shift attenuation. 36Ar deduced levels, resonance strengths, γ-decay branching ratios, T1/2, J, π, S, T1/2. Enriched targets.
doi: 10.1016/0375-9474(74)90008-6
J.Phys.(London) A7, 1977 (1974)
P.R.G.Lornie, E.M.Jayasinghe, G.D.Jones, H.G.Price, M.F.Thomas, P.J.Twin, P.J.Nolan
High Spin Negative Parity States in 35Cl
NUCLEAR REACTIONS 32S(α, pγ); measured pγ(θ), P(θ), DSA, recoil distance. 35Cl levels deduced J, π, γ-mixing, T1/2, γ-branching ratios, transition strengths.
doi: 10.1088/0305-4470/7/16/002
Phys.Rev. C10, 2138 (1974)
U.N.Singh, H.I.Liou, G.Hacken, M.Slagowitz, F.Rahn, J.Rainwater, W.Makofske, J.B.Garg
Neutron Resonance Spectroscopy: Chlorine
NUCLEAR REACTIONS 35,37Cl(n, n), (n, γ), E=20 eV-400 keV; measured total σ(E). 36,38Cl deduced resonances, J, L, S, n-width.
Nucl.Phys. A226, 326 (1974)
M.A.Van Driel, H.H.Eggenhuisen, J.A.J.Hermans, D.Bucurescu, H.A.van Rinsvelt, G.A.P.Engelbertink
Investigation of the 3.46 MeV Isomeric Level of 38K with the 24Mg(16O, pnγ)38K Reaction
NUCLEAR REACTIONS Mg(16O, Xγ), E=36, 38 MeV; measured γ(t), Eγ, Iγ, recoil distance. 38K levels deduced E(X), γ-branching, ICC, T1/2. 35Cl, 38Ar levels deduced T1/2. Natural targets.
doi: 10.1016/0375-9474(74)90409-6
Nucl.Phys. A250, 221 (1975)
J.M.Davidson, T.Taylor, D.A.Hutcheon, D.M.Sheppard, W.C.Olsen
Study of 35Ar from 33S(3He, n)35Ar and 33S(3He, nγ)35Ar
NUCLEAR REACTIONS 33S(3He, n), E=6.375, 6.660 MeV; 33S(3He, nγ), E=6.390 MeV; measured σ(En, θ), Eγ, nγ-coin; deduced Q. 35Ar deduced levels, L, J, π, T. Enriched target. Ge(Li) detector.
doi: 10.1016/0375-9474(75)90254-7
Radiochem.Radioanal.Lett. 20, 175 (1975)
G.Deconninck, G.Debras
Analysis of Chlorine by Prompt Gamma Rays Induced by Protons
NUCLEAR REACTIONS 35,37Cl(p, γ), (p, p'γ), (p, αγ), E=1-3 MeV; measured σ.
Phys.Rev. C12, 1109 (1975)
A.Guichard, H.Nann, B.H.Wildenthal
37Cl(p, 3He)35S Reaction
NUCLEAR REACTIONS 37Cl(p, 3He), E=40.2 MeV; measured σ(E(3He), θ). 35S deduced levels, L, S, J, π.
Phys.Scr. 12, 280 (1975)
J.Keinonen, M.Riihonen, A.Anttila
Strengths of Analogue Resonances in (p, γ) Reactions on Sulphur Isotopes
NUCLEAR REACTIONS 32S(p, γ), E=588 keV; 34S(p, γ), E=1214 keV; 33S(p, γ), E=1542 keV; 36S(p, γ), E=1887 keV; measured σ(E, Eγ). 33,34,35,37Cl resonances deduced strengths, Γ.
Phys.Lett. 60B, 32 (1975)
H.Nann, W.S.Chien, A.Saha, B.H.Wildenthal
The Strongest L=6 Transitions Observed in the (α, d) Reaction on Odd-Mass A=33-41 Target Nuclei
NUCLEAR REACTIONS 33S, 35,37Cl, 39,41K(α, α), (α, d), E=40 MeV; measured σ(Ed, θ). 35Cl, 37,39Ar, 41,43Ca levels deduced L.
doi: 10.1016/0370-2693(75)90519-5
Nucl.Phys. A254, 80 (1975)
W.A.Schier, B.K.Barnes, G.P.Couchell, J.J.Egan, P.Harihar, S.C.Mathur, A.Mittler, E.Sheldon
Spin and Parity Assignments for 35Cl Levels from the 31P(α, p)34S Reaction
NUCLEAR REACTIONS 31P(α, p), (α, α), E=3.25-5.50 MeV; measured absolute σ(E, En, θ); deduced optical potential. 35Cl deduced resonances J, π, L.
doi: 10.1016/0375-9474(75)90583-7
Phys.Lett. 56B, 212 (1975)
R.Sherr, I.Talmi
Systematic Effects of Charge Independence Breaking on Energies of Analog States
NUCLEAR STRUCTURE 33,34,35,36Cl, 34,35,36,37Ar, 35,36,37,38K, 36,37,38,39Ca; calculated IAS energy differences.
doi: 10.1016/0370-2693(75)90377-9
Thesis, Groningen Univ. Netherlands (1975)
T.W.van der Mark
Studies on the nuclei 33S, 33Cl and 35S
NUCLEAR REACTIONS 32,34S(d, p), E=4.25, 4.72 MeV; 32,34S(p, γ), E=1.8-1.9 MeV; 37Cl(d, α), E=4.25 MeV; measured σ(Ep), σ(Eα), Eγ, Iγ, (particle)γ(θ), γγ-coin. 33,35S, 33,35Cl; deduced levels, J, π, γ-branchings, mixing ratios, resonance strengths.
Phys.Lett. 57B, 413 (1975)
G.J.Wagner, P.Doll, K.T.Knopfle, G.Mairle
Lifetime of Nuclear Hole States Caused by Phonon-Hole Coupling
NUCLEAR REACTIONS 36,38,40Ar, 40,42,44,48Ca(d, 3He), E=52 MeV; measured σ(E(3He), θ). 35,37,39Cl, 39,41,43,47K levels deduced spreading width.
doi: 10.1016/0370-2693(75)90256-7
Phys.Rev. C13, 1479 (1976)
W.Benenson, A.Guichard, E.Kashy, D.Mueller, H.Nann
Mass of 35K
NUCLEAR REACTIONS 40Ca(3He, 8Li), E=75.8, 73.7 MeV; measured σ; deduced Q. 35K deduced mass excess, levels.
Phys.Rev. C14, 160 (1976)
J.Keinonen, R.Rascher, M.Uhrmacher, N.Wust, K.P.Lieb
M2 Transitions between the 1f7/2 and the 1d3/2 Orbit
NUCLEAR REACTIONS 25Mg, 27Al(16O, X), E=30-50 MeV; measured Eγ, recoil distance DSA. 36Cl levels deduced γ-branching. 35,36Cl, 40K, 41Ca levels deduced T1/2. M2 transition systematics 33 ≤ A ≤ 47.
Nucl.Phys. A264, 13 (1976)
M.A.Meyer, I.Venter, W.F.Coetzee, D.Reitmann
Energy Levels of 35Cl
NUCLEAR REACTIONS 34S(p, γ), E=0.7-2.01 MeV; measured σ(E, Eγ, θ), DSA. 35Cl deduced resonances, levels, J, π, T1/2, γ-branching, δ. Enriched targets.
doi: 10.1016/0375-9474(76)90141-X
Nucl.Phys. A265, 416 (1976)
R.J.Sparks
Investigation of the Reaction 34S(p, γ)35Cl (I). Resonances at Proton Energies Above 2 MeV
NUCLEAR REACTIONS 34S(p, γ), E=1.21, 1.95-2.91 MeV; measured σ(E, Eγ); deduced Q. 35Cl deduced resonances, J, π, γ-branching, strength.
doi: 10.1016/0375-9474(76)90552-2
Nucl.Phys. A265, 429 (1976)
R.J.Sparks
Investigation of the Reaction 34S(p, γ)35Cl (II). Angular Distributions and Resonant Absorption
NUCLEAR REACTIONS 34S(p, γ), E=2.33-2.79 MeV; measured σ(E, Eγ, θ). 35Cl deduced levels, J, π, δ, γ-ray branching ratios, transition strengths. 35Cl(γ, γ), E=9.08 MeV; measured σ(Eγ). 35Cl deduced level, Γ, Γγ, Γp, resonance strength. Natural scatterer. Enriched 34S target.
doi: 10.1016/0375-9474(76)90553-4
Nucl.Phys. A272, 466 (1976)
M.A.Van Driel, H.H.Eggenhuisen, G.A.P.Engelbertink, L.P.Ekstrom, J.A.J.Hermans
Model Independent Jπ Assignments in 38Ar from γ-Ray Experiments in Heavy-Ion Induced Reactions
NUCLEAR REACTIONS 24Mg(16O, 2pγ), (16O, pαγ), E=38, 45 MeV; measured σ(E, Eγ), σ(Eγ, θ), γγ-coin, γ-ray linear polarization. 38Ar deduced levels, branching ratio, J, π, δ, alignment parameters. 35Cl deduced levels, δ, alignment parameters. Enriched targets. Compton-suppression spectrometer, three-Ge(Li) polarimeter.
doi: 10.1016/0375-9474(76)90343-2
Phys.Rev. C14, 996 (1976)
E.K.Warburton, J.W.Olness, A.R.Poletti, J.J.Kolata
Decay Schemes for High-Spin States in 35,36,37Cl and 37Ar from Heavy-Ion Fusion-Evaporation
NUCLEAR REACTIONS 25,24,26Mg, 27Al, 18O, 10Be(18O, X), 24,26Mg, 27Al, 28Si(19F, X), 26Mg, 27Al(14N, X), 27Al, 18O(16O, X), 26Mg, 18,16O, 10Be(13C, X), 25,26Mg, 19F, 18O(12C, X), 12C(11B, X), E=20-60 MeV; measured fusion evaporation, γγ-coin, polarization, recoil distance. 35,36,37Cl, 37Ar deduced levels, J, π, T1/2. Ge(Li) detectors, natural, enriched targets.
Acta Phys.Pol. B7, 633 (1976)
E.A.Wesolowski, M.Kicinska
Shell and Excitation Energy Effects in the Potential Radii Deduced from (d, p) Reactions on s-d Shell Nuclei at Low Deuteron Energy
NUCLEAR REACTIONS 23Na, 24,26Mg, 27Al, 28Si, 31P, 32,34S, 35Cl(d, p), E=2.4, 2.5, 2.6 MeV; measured σ(Ep, θ). 25Mg, 27Mg, 29Si levels deduced β.
Nucl.Phys. A287, 94 (1977)
R.Abegg, S.K.Datta
Study of the Reaction 34S(d, p)35S with Vector-Polarized Deuterons
NUCLEAR REACTIONS 34S(polarized d, p), E=11.8 MeV; measured vector analyzing power, iT11(Ed, Ep, θ), σ(Ed, Ep, θ). 35S levels deduced J, π, L, S. Enriched target.
doi: 10.1016/0375-9474(77)90565-6
Phys.Rev. C15, 1847 (1977)
G.Azuelos, J.E.Kitching, K.Ramavataram
Half-Lives and Branching Ratios of Some T = 1/2 Nuclei
RADIOACTIVITY 13N, 15O, 17F, 33Cl; measured T1/2. 21Na, 25Al, 27Si, 29P; measured absolute Iβ. 23Mg, 31S, 35Ar, 37K, 39Ca; measured T1/2, absolute Iβ.
Z.Phys. A282, 371 (1977)
L.Koester, K.Knopf, W.Waschkowski
Scattering of Slow Neutrons by the Isotopes of Chlorine
NUCLEAR REACTIONS Cl, 35,37Cl(n, n), E=slow; measured scattering lengths.
Izv.Akad.Nauk SSSR, Ser.Fiz. 41, 1688 (1977); Bull.Acad.Sci.USSR, Phys.Ser. 41, No.8, 128 (1977)
E.G.Kopanets, A.A.Koval, V.Y.Kostin, L.P.Korda, P.M.Tutakin, S.P.Tsytko
Angular Distributions of γ-Rays Emitted in the 34S(p, γ)35Cl Reaction
NUCLEAR REACTIONS 34S(p, γ), E=1.0-1.4 MeV; measured σ(E;Eγ, θ). 35Cl deduced resonances, J, π, γ-branching, δ.
Izv.Akad.Nauk SSSR, Ser.Fiz. 41, 1658 (1977); Bull.Acad.Sci.USSR, Phys.Ser. 41, No.8, 104 (1977)
A.A.Koval, E.G.Kopanets, V.Y.Kostin, L.P.Korda, P.M.Tutakin, S.P.Tsytko
The Fine Structure of the 7/2- Isobar-Analog States of the 35Cl Nucleus
NUCLEAR REACTIONS 34S(p, γ), E=1.0-1.4 MeV; measured σ(E;Eγ, θ). 35Cl deduced fine structure of isobar analog resonance, γ-branching, δ, B(λ).
Phys.Rev. C15, 1959 (1977)
H.Nann, W.S.Chien, A.Saha, B.H.Wildenthal
High-Spin States of (fp)2 Character in 34,35,36Cl and 37,39Ar
NUCLEAR REACTIONS 32,33,34S, 35,37Cl(α, d), E=40 MeV; measured σ(Ed, θ). 34,35,36Cl, 37,39Ar levels deduced L, J, π.
Nucl.Phys. A284, 1 (1977)
D.A.Outlaw, G.E.Mitchell, E.G.Bilpuch
High Resolution Study of the 34S(p, p) Reaction
NUCLEAR REACTIONS 34S(p, p), E=1.45-2.82 MeV; measured σ(E). 35Cl deduced IAS, J, π, Γp.
doi: 10.1016/0375-9474(77)90681-9
J.Phys.(London) G3, 1363 (1977)
D.C.Palmer, D.R.Maxson, J.R.Bading
35Cl, 37Cl and 36Ar(n, d) Reactions at 14.1 MeV
NUCLEAR REACTIONS 35,37Cl, 36Ar(n, d), E=14.1 MeV; measured σ(Ed, θ). 34,36S, 35Cl levels deduced S. Enriched targets.
doi: 10.1088/0305-4616/3/10/010
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
Phys.Rev. C16, 1159 (1977)
R.Sherr
Charge-Dependent and A-Dependent Effects in Isotope Shifts of Coulomb Displacement Energies
NUCLEAR STRUCTURE 33,34,35,36Cl, 33,34,35,36S, 37Cl, 34,35,36,37,38Ar, 35,36,37,38,39K, 36,37,38,39,41,42,43,44,45,46,47,48Ca, 41,42,43,44,45,46,47,48,49Sc, 42,43,44,45,46,47,48,49,50Ti, 45,46,47,48,49,50,51V, 46,47,48,49,51,52,50Cr, 49,50,51,52,53Mn, 50,51,52,53,54Fe, 53,54,55Co, 54,55Ni, 17,18,19,20O, 17,18,19,20,21F, 18,19,20,21,22,23,24Ne, 19,20,21,22,23,24,25Na, 20,21,22,23,24,25,26Mg, 23,24,25,26,27Al, 24,25,26,27Si; calculated Coulomb displacement energies.
Nucl.Phys. A307, 65 (1978)
M.Cenja, M.Duma, C.Hategan, M.Tanase
The (p, n) Threshold Anomaly in Proton Elastic Scattering on 23Na, 27Al, 31P, 35Cl and 34S
NUCLEAR REACTIONS 23Na, 27Al, 31P, 35Cl, 34S(p, p), E=3.5-8.5 MeV; measured excitation functions at backward angles; deduced (p, n) threshold anomalies.
doi: 10.1016/0375-9474(78)90426-8
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
J.Phys.Soc.Jpn. 44, 353 (1978)
K.Gul
Mass Excesses of Some Proton Rich Light Nuclides
ATOMIC MASSES 14N, 12,13O, 14,15F, 16,17Ne, 18,19Na, 20,21Mg, 22,23Al, 24,25Si, 26,27P, 28,29S, 30,31Cl, 32,33Ar, 34,35K, 36,37Ca; calculated mass excess.
Phys.Lett. B 85, 212 (1979)
L.C.Carraz, G.T.Ewan, E.Hagberg, J.C.Hardy, B.Jonson, S.Mattsson, H.L.Ravn, P.Tidemand-Petersson, for the ISOLDE Collaboration
A precise determination of the excitation energy of the lowest T=3/2 state in 35Ar
RADIOACTIVITY 35K(EC), (β+)[from 45Sc(p, X)]; measured Eγ, Iγ, chemical, mass separation. 35Ar; deduced levels, J, π.
doi: 10.1016/0370-2693(79)90581-1
Nucl.Phys. A325, 269 (1979)
M.A.Eswaran, H.E.Gove, R.Cook, B.Sikora
The α-Transfer Reactions 27Al(6Li, d)31P, 29Si(6Li, d)33S and 31P(6Li, d)35Cl at 36 MeV
NUCLEAR REACTIONS 27Al, 29Si, 31P(6Li, d), E=36 MeV; measured σ(Ed, θ). 31P, 33S, 35Cl deduced Sα. Exact finite-range DWBA analysis.
doi: 10.1016/0375-9474(79)90163-5
Nucl.Phys. A313, 276 (1979)
E.Hagberg, J.C.Hardy, B.Jonson, S.Mattsson, P.Tidemand-Petersson, The ISOLDE Collaboration
The Superallowed Decay of 35Ar: A Persistent Anomaly
RADIOACTIVITY 35Ar [from V(p, 6p11n)]; measured Iγ; deduced ft value. Cabibbo angle. Natural target, Ge(Li) detector. Chem mass separation.
doi: 10.1016/0375-9474(79)90500-1
Nucl.Phys. A331, 389 (1979)
B.M.Paine, D.G.Sargood
(p, γ) Resonance Strengths in the s-d Shell
NUCLEAR REACTIONS 26Mg, 27Al, 30Si, 34S, 37Cl, 39K, 40Ca(p, γ), E=0.5-2.0 MeV; measured σ(E). 27Al, 28Si, 31P, 35Cl, 38Ar, 40Ca, 41Sc deduced resonance strengths. Natural, enriched targets.
doi: 10.1016/0375-9474(79)90349-X
Yad.Fiz. 29, 289 (1979); Sov.J.Nucl.Phys. 29, 143 (1979)
L.M.Solin, Y.A.Nemilov, V.N.Kuzmin, K.I.Zherebtsova
New Levels of 37S
NUCLEAR REACTIONS 36S(d, p), E=3.55 MeV; measured σ(Ep). 37S deduced levels. 13C, 18O, 35S deduced levels.
Phys.Rev.Lett. 42, 40 (1979)
T.J.M.Symons, Y.P.Viyogi, G.D.Westfall, P.Doll, D.E.Greiner, H.Faraggi, P.J.Lindstrom, D.K.Scott, H.J.Crawford, C.McParland
Observation of New Neutron-Rich Isotopes by Fragmentation of 205-MeV/Nucleon 40Ar Ions
NUCLEAR REACTIONS 12C(40Ar, X), E=205 MeV/nucleon; measured σ; deduced production σ for 26,27,28,29,30Na. 30,31Na, 27,28Ne, 31,32,33Mg deduced evidence for particle stability.
doi: 10.1103/PhysRevLett.42.40
Nucl.Phys. A316, 189 (1979)
Tai Kuang-Hsi, T.Dossing, C.Gaarde, J.S.Larsen
Angular Correlations in Compound Nucleus Decay Following the Reactions 16O + 27Al, 40Ca and 58Ni
NUCLEAR REACTIONS 27Al(16O, 2α), (16O, αp), (16O, 2p), E=50, 60 MeV; 40Ca, 58Ni(16O, 2α), (16O, αp), (16O, 2p), E=70 MeV; measured αα(θ), αp(θ), pp(θ). Model calculation of αα(θ). Enriched 58Ni target.
doi: 10.1016/0375-9474(79)90679-1
Nucl.Phys. A341, 365 (1980)
K.Eskola, M.Riihonen, K.Vierinen, J.Honkanen, M.Kortelahti, K.Valli
Beta-Delayed Particle Emission of 36K
RADIOACTIVITY 36K [from 36Ar(p, n)]; measured β-delayed Ep, Eα, Ip, Iα; deduced maximum log ft. 36Ar deduced levels, Γγ, Γp, Γα, J, π. Implanted 36Ar target.
doi: 10.1016/0375-9474(80)90370-X
Nucl.Phys. A343, 109 (1980)
G.T.Ewan, E.Hagberg, J.C.Hardy, B.Jonson, S.Mattsson, P.Tidemand-Petersson, I.S.Towner
The Decay of 35K
RADIOACTIVITY 35K [from 45Sc(p, 8n3p), chemical, mass separation]; measured Eγ, Iγ, β-delayed Ep, Ip; deduced logft. 35Ar deduced levels. Ge(Li), surface barrier Si detectors.
doi: 10.1016/0375-9474(80)90643-0
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.
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.
Nucl.Phys. A359, 149 (1981)
W.Biesiot, Ph.B.Smith, J.L.Stavast, P.B.Goldhoorn, S.Van der Hoek
Parameters of Selected Levels in 35Cl
NUCLEAR REACTIONS 34S(p, γ), (p, p), E=1.4-2.8 MeV; measured σ(E, Eγ, θ). 35Cl deduced levels J, π, Γ, resonance strength. Enriched targets.
doi: 10.1016/0375-9474(81)90217-7
Phys.Lett. B98, 26 (1981)
C.van der Leun, G.J.L.Nooren
Spin J=1/2 Assignments to Proton-Capture Resonances
NUCLEAR REACTIONS 36S(p, γ), E=699, 924, 1219 keV; 34S(p, γ), E=832 keV; 54Fe(p, γ), E=107, 1370 keV; analyzed γ(θ) data. 37,35Cl, 55Co resonance deduced unique J, π assignments.
doi: 10.1016/0370-2693(81)90359-2
Phys.Rev. C25, 872 (1982)
K.T.Lesko, D.-K.Lock, A.Lazzarini, R.Vandenbosch, V.Metag, H.Doubre
Energy Dependence of Fusion Cross Section for 28Si + 12C by Evaporation Residue Measurements
NUCLEAR REACTIONS, ICPND 28Si(12C, X)35Cl/38K/37Ar/34Cl/32S/34S/35Ar/35Cl/38Ar/31P, E(cm)=18.4-35 MeV; measured Eγ, Iγ, σ(evaporation residue) vs θ; deduced evaporation residual σ, fusion σ(E). Entrance channel, level density limitation models.
Phys.Rev. C26, 2022 (1982)
R.A.Racca, F.W.Prosser, C.N.Davids, D.G.Kovar
Search for Structure in the Fusion of 16O + 24Mg
NUCLEAR REACTIONS, ICPND 24Mg(16O, 2p), (16O, np), (16O, pα), (16O, 2α), (16O, 2pα), (16O, p2α), E=40-51 MeV; measured residuals production σ(E); deduced no structure in fusion σ vs E. Activation technique.
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.
J.Phys.(Paris) 44, 957 (1983)
H.Glattli, J.Coustham
Spin-Dependent Scattering and Absorption of Thermal Neutrons on Dynamically Polarized Nuclei
NUCLEAR REACTIONS 13C, 35,37Cl, 79,81Br, 31P, 41K(n, n), (n, X), E=thermal; measured neutron phase shift, precession angle vs target polarization, σ(absorption). 13C, 35Cl, 79,81Br deduced spin-dependent part of scattering length. 31P, 37Cl, 41K deduced spin-dependent scattering length part upper limit. Dynamic target polarization, KCI, KBr, Ca3(PO4)2, BaCO3 samples.
Phys.Lett. 125B, 116 (1983)
M.Langevin, C.Detraz, D.Guillemaud-Mueller, A.C.Mueller, C.Thibault, F.Touchard, M.Epherre
35Na: A new neutron-rich Sodium isotope
NUCLEAR REACTIONS Ir(p, X), E=10 GeV; measured βn-coin; deduced evidence for 35Na.
RADIOACTIVITY 35Na(β-) [from Ir(p, X), E=10 GeV, on-line separation]; measured βn-coin, T1/2.
doi: 10.1016/0370-2693(83)91248-0
Phys.Rev. C27, 1188 (1983)
S.Raman, E.T.Jurney, D.A.Outlaw, I.S.Towner
34Cl Superallowed β Decay
RADIOACTIVITY 34Cl(β+) [from 33S(p, γ)]; 35S(β-); analyzed data. 34Cl deduced Q(β++EC), T1/2, ft. 35S deduced Q(β-).
NUCLEAR REACTIONS 32,33,34S(n, γ), E=thermal; measured Eγ. 33,34,35S deduced neutron separation energy. 33,34S(p, γ), E=0.9-1.4 MeV; measured Eγ. 34Cl, 35Cl deduced resonances, proton separation energy.
Nucl.Phys. A417, 269 (1984)
E.G.Adelberger, J.L.Osborne, H.E.Swanson, B.A.Brown
The l-Forbidden Gamow-Teller Decay of 39Ca
RADIOACTIVITY 35Ar, 39Ca(β+); measured Iγ, Eγ; deduced ft, empirical single-particle operator normalizations. 35Cl levels deduced Iβ, γ-branching ratios, Gamow-Teller transition strengths. 39K levels deduced Iβ, Gamow-Teller transition strengths. Shell model.
doi: 10.1016/0375-9474(84)90508-6
Phys.Rev. C29, 1980 (1984)
R.F.Carlton, W.M.Good, J.A.Harvey, R.L.Macklin, B.Castel
Determination of Unbound States in 35S from Neutron Total and Capture Cross-Section Measurements on 34S
NUCLEAR STRUCTURE 35S; calculated levels, neutron strength function. Shell model, R-matrix methods.
NUCLEAR REACTIONS 34S(n, n), E=90-1500 keV; measured σ(E). 34S(n, γ), E=30-1100 keV; measured capture σ. 35S deduced resonances, average parameters, J, π, (gΓn), (gΓnΓγ/Γ), level spacings, densities, neutron strength function.
Nucl.Instrum.Methods 228, 62 (1984)
D.Elenkov, D.Lefterov, G.Toumbev
Two-Target DSAM following the (n, n'γ) Reaction with Fast Reactor Neutrons
NUCLEAR REACTIONS 11B, 24Mg, 27Al, 32S, 35Cl, 39K, 40Ca, 45Sc, 51V(n, n'γ), E=fast; measured DSA. 11B, 24Mg, 27Al, 32S, 35Cl, 39K, 40Ca, 45Sc, 51V levels deduced T1/2. Two-target system.
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. A319, 287 (1984)
W.A.Mayer, W.Henning, R.Holzwarth, H.J.Korner, G.Korschinek, W.U.Mayer, G.Rosner, H.J.Scheerer
Mass Excess and Excited States of Neutron-Rich Silicon, Phosphorus and Sulphur Isotopes
NUCLEAR REACTIONS 36S(14C, 17O), (14C, 16O), (14C, 15O), (14C, 15N), (14C, 14N), (14C, 13C), (14C, 12C), E=71 MeV; measured ejectile spectra. 36S(18O, 17O), (18O, 16O), E=80 MeV; measured γ(ejectile)-coin; deduced Q. 33,34Si, 35,36P deduced mass excess, levels. 35Si deduced mass. 37,38S deduced mass excess, levels, γ-decay. Ge(Li) detector, Q3D magnetic spectrograph.
Nucl.Phys. A414, 219 (1984)
S.Piskor, P.Franc, J.Kremenek, W.Schaferlingova
Spectroscopic Information on 35S and 37S from the (d, p) Reaction
NUCLEAR REACTIONS 34,36S(d, p), E=12.3 MeV; measured Q, σ(θ). 35,37S deduced levels, L, π, spectroscopic factors. Enriched target.
doi: 10.1016/0375-9474(84)90641-9
Phys.Rev. C30, 1442 (1984)
C.E.Thorn, J.W.Olness, E.K.Warburton, S.Raman
36S(d, p)37S and 34,36S(d, 3He)33,35P Reactions
NUCLEAR REACTIONS 36S(d, p), E=25 MeV; 34,36S(d, 3He), E=30 MeV; measured σ(θ), σ(Ep), σ(E(3He)). 37S deduced levels, thermal neutron capture σ, J, π, (2J+1)S. 33,35P deduced levels, L, J, π, C2S.
Phys.Rev.Lett. 55, 799 (1985)
T.Altzitzoglou, F.Calaprice, M.Dewey, M.Lowry, L.Piilonen, J.Brorson, S.Hagen, F.Loeser
Experimental Search for a Heavy Neutrino in the Beta Spectrum of 35S
RADIOACTIVITY 35S(β-); measured Eβ, Iβ; deduced no heavy neutrino evidence.
doi: 10.1103/PhysRevLett.55.799
Pisma Zh.Eksp.Teor.Fiz. 42, 233 (1985); JETP Lett.(USSR) 42, 289 (1985)
A.M.Apalikov, S.D.Boris, A.I.Golutvin, L.P.Laptin, V.A.Lyubimov, N.F.Myasoedov, V.V.Nagovitsyn, E.G.Novikov, V.Z.Nozik, V.A.Soloshchenko, I.N.Tikhomirov, E.F.Tretyakov
Search for Heavy Neutrinos in β Decay
RADIOACTIVITY 35S(β-); measured Eβ, Iβ; deduced mixing ratios over heavy neutrino mass interval.
Phys.Rev.Lett. 55, 1384 (1985)
J.Aysto, D.M.Moltz, X.J.Xu, J.E.Reiff, J.Cerny
Observation of the First T(z) = -5/2 Nuclide, 35Ca via Its β-Delayed Two-Proton Emission
NUCLEAR REACTIONS 40Ca(3He, 4nα), E=135 MeV; measured β-delayed two-proton spectra, Ep, Ip. 35Ca deduced mass excess. Natural Ca target.
RADIOACTIVITY 35Ca(β+2p) [from 40Ca(3He, 4nα), E=135 MeV]; measured β-delayed two-proton sum spectra, pp-coin, Ep, Ip; deduced T=1/2, (5/2)+ level decay characteristics, approximate T1/2. 35K level deduced proton decay characteristics. 34Ar, 33Cl levels deduced proton branching characteristics.
doi: 10.1103/PhysRevLett.55.1384
Phys.Rev. C31, 1499 (1985)
W.W.Daehnick, R.D.Rosa
Weak Branches in 42Sc, 35Ar, and 27Si β+ Decay
RADIOACTIVITY 42Ca, 35Ar, 27Si(β+); measured Eγ, Iγ, γ(t). 35Cl, 27Al levels deduced relative β-branching.
Nucl.Phys. A441, 95 (1985)
P.V.Drumm, L.K.Fifield, R.A.Bark, M.A.C.Hotchkis, C.L.Woods, P.Maier-Komor
Ground-State Mass Excesses and Low-Lying Levels of the Neutron-Rich Nuclei 36P, 35P and 34P
NUCLEAR REACTIONS 36,34S(7Li, 7Be), 36S(6Li, 7Be), E=52 MeV; 36,34S(11B, 11C), E=83 MeV; measured σ(E(7Be)), σ(E(11C)). 36,35,34P deduced mass excess, levels. Enriched targets.
doi: 10.1016/0375-9474(85)90169-1
Z.Phys. A322, 121 (1985)
T.J.Kennett, W.V.Prestwich, J.S.Tsai
Radiative Thermal Neutron Capture by Natural Sulfur
NUCLEAR REACTIONS S(n, γ), E=thermal; measured Eγ, Iγ. 33S deduced levels, J, π, neutron separation energies. 35S deduced levels, neutron separation energies.
Phys.Lett. 156B, 155 (1985)
S.Khan, Th.Kihm, K.T.Knopfle, G.Mairle, V.Bechtold, L.Friedrich
The Mass of 35P and Spin-Parity Assignments for Excited 35P States
NUCLEAR REACTIONS 36S(d, 3He), (polarized d, 3He), E=52 MeV; measured σ(E(3He)), σ(θ), iT11(θ). 35P deduced mass excess, levels, J, π, C2S.
doi: 10.1016/0370-2693(85)91499-6
J.Radioanal.Nucl.Chem. 89, 123 (1985)
A.Z.Kiss, E.Koltay, B.Nyako, E.Somorjai, A.Anttila, J.Raisanen
Measurements of Relative Thick Target Yields for PIGE Analysis on Light Elements in the Proton Energy Interval 2.4-4.2 MeV
NUCLEAR REACTIONS, ICPND 7Li, 37Cl, 41,39K, 48Ca(p, nγ), 7Li, 14N, 17,18O, 23Na, 13C, 26,25Mg, 27Al, 29,28Si, 31P, 32,34,33S, 35,37Cl, 41K, 42,43Ca, 45Sc(p, p'γ), 9Be, 12,13C, 14N, 16O, 23Na, 24,25,26Mg, 28,29,30Si, 31P, 32,34S, 35,37Cl, 39,41K, 23Na, 44Ca, 45Sc(p, γ), 9Be, 10B, 15N, 19F, 23Na, 31P, 37Cl, 41K(p, αγ), E=2.4-4.2 MeV; measured thick target relative γ yields, Eγ, Iγ. Particle induced prompt gamma emission analysis.
Nucl.Phys. A447, 577c (1985)
P.Kristiansson, J.P.Bondorf, L.Carlen, H.-A.Gustafsson, B.Jakobsson, A.Kristiansson, G.Lovhoiden, H.Nifenecker, O.-B.Nielsen, A.Oskarsson, H.Ryde, T.-F.Thorsteinsen, M.Westenius
Large-Angle Correlations Observed in Intermediate Energy Heavy Ion Collisions
NUCLEAR REACTIONS 12C, 27Al, 64Cu, 197Au(12C, 2p), (12C, 2d), (12C, 2t), (12C, 2α), E=85 MeV/nucleon; measured (particle)(particle)(θ), large angle; deduced reaction mechanism.
doi: 10.1016/0375-9474(86)90633-0
Phys.Rev. C32, 2215 (1985)
J.Markey, F.Boehm
Search for Admixture of Heavy Neutrinos with Masses between 5 and 55 keV
RADIOACTIVITY 35S(β-); measured β-spectrum, shape; deduced heavy neutrino admixture upper limit. Magnetic spectrometer.
Phys.Lett. 160B, 322 (1985)
T.Ohi, M.Nakajima, H.Tamura, T.Matsuzaki, T.Yamazaki, O.Hashimoto, R.S.Hayano
Search for Heavy Neutrinos in the Beta Decay of 35S. Evidence Against the 17 keV Heavy Neutrino
RADIOACTIVITY 35S(β-); measured Eβ, Iβ; deduced heavy neutrino admixture upper limit.
doi: 10.1016/0370-2693(85)91336-X
Phys.Rev. C32, 18 (1985)
S.Raman, R.F.Carlton, J.C.Wells, E.T.Jurney, J.E.Lynn
Thermal Neutron Capture Gamma Rays from Sulfur Isotopes: Experiment and theory
NUCLEAR REACTIONS 34,33,32,36S(n, γ), E=thermal; measured Eγ, Iγ; deduced model dependent effects. 33,34,35,37S deduced levels, γ-branching, J, π, E1 transition. Potential capture theory.
J.Phys.(London) G12, 391 (1986)
M.E.Brandan, A.Menchaca-Rocha, A.Szanto de Toledo, N.Carlin Filho, E.M.Szanto, M.M.Coimbra
Detection of 8Be Nuclei from the Reaction 16O + 27Al at 65 MeV
NUCLEAR REACTIONS 27Al(16O, 8Be), E=65 MeV; measured σ(E(8Be)), ejectile production σ. ΔE-E telescope. Two-body kinematic calculations.
doi: 10.1088/0305-4616/12/5/006
Z.Phys. A324, 487 (1986)
J.P.Dufour, R.Del Moral, A.Fleury, F.Hubert, D.Jean, M.S.Pravikoff, H.Delagrange, H.Geissel, K.-H.Schmidt
Beta Decay of 17C, 19N, 22O, 24F, 26Ne, 32Al, 34Al, 35-36Si, 36-37-38P, 40S
RADIOACTIVITY 17C, 19N, 22O, 24F, 26Ne, 32,34Al, 35,36Si, 36,37,38P, 40S(β-) [from 9Be(40Ar, X), E=60 MeV/nucleon]; measured βγ(t); deduced T1/2. 17N, 19O, 22F, 24Ne, 26Na, 32,33Si, 35,36P, 36,37,38S, 40Cl deduced levels, γ-branching.
NUCLEAR REACTIONS 9Be(40Ar, X)17C/19N/22O/24F/26Ne/32Al/34Al/35Si/36Si/36P/37P/38P/40S, E=60 MeV/nucleon; measured βγ(t); deduced evidence for residuals production.
Z.Naturforsch. 41a, 15 (1986)
M.Elbel, R.Quad
The Quadrupole Moments of the Stable Nuclei of Sulphur and Chlorine
NUCLEAR MOMENTS 33S, 35,37Cl; measured hfs; deduced quadrupole moments. Collinear laser spectroscopy.
Nucl.Phys. A453, 497 (1986)
L.K.Fifield, C.L.Woods, W.N.Catford, R.A.Bark, P.V.Drumm, K.T.Keoghan
The Mass of 35Si
NUCLEAR REACTIONS 34,36S(13C, 14O), E=91 MeV; measured σ(E(14O)). 35Si deduced mass excess. 33Si deduced energy levels. Enriched targets.
doi: 10.1016/0375-9474(86)90449-5
Nucl.Phys. A455, 149 (1986)
M.Langevin, A.C.Mueller, D.Guillemaud-Mueller, M.G.Saint-Laurent, R.Anne, M.Bernas, J.Galin, D.Guerreau, J.C.Jacmart, S.D.Hoath, F.Naulin, F.Pougheon, E.Quiniou, C.Detraz
Mapping of the Proton Drip-Line up to Z = 20: Observation of the T(z)=-(5/2) series 23Si, 27S, 31Ar and 35Ca
NUCLEAR REACTIONS Ni(40Ca, X)23Si/27S/31Ar/35Ca, E=3097 MeV; measured fragment spectra; deduced fragment mass, charge distributions, T(z)=-5/2 residuals production.
doi: 10.1016/0375-9474(86)90348-9
Z.Phys. A324, 283 (1986)
R.J.Smith, P.J.Woods, R.Chapman, J.L.Durell, J.N.Mo, B.R.Fulton, R.A.Cunningham
Use of the 64Ni(36S, 34,35Si)66,65Zn Reactions to Measure the Masses of 34Si and 35Si
NUCLEAR REACTIONS 64Ni(36S, 35Si), (36S, 34Si), E=198 MeV; measured σ(E(35Si)), σ(E(34Si)). 34,35Si deduced mass excess. Model prediction comparison. Gas filled focal plane detector, QMG/2 magnetic spectrometer.
Phys.Rev. C34, 1031 (1986)
E.K.Warburton, D.E.Alburger, J.A.Becker, B.A.Brown, S.Raman
Probe of the Shell Crossing at A = 40 via Beta Decay: Experiment and theory
RADIOACTIVITY 35P, 37,38S, 38Cl(β-) [from 36S(d, X), (t, X), E=3-3.4 MeV]; measured Eγ, Iγ; deduced log ft. 38,37Cl, 35S, 38Ar deduced levels, γ-branching ratios, Gamow-Teller transition strengths. Shell model calculations.
NUCLEAR STRUCTURE 35S, 37,38Cl, 38Ar; calculated levels, Gamow-Teller, unique first forbidden β-decay. Shell model.
Izv.Akad.Nauk SSSR, Ser.Fiz. 51, 134 (1987); Bull.Acad.Sci.USSR, Phys.Ser. 51, No.1, 124 (1987)
U.R.Arzibekov, A.S.Gabelko, M.Kh.Zhalilov, K.M.Irgashev, B.S.Ishkhanov, I.M.Kapitonov, I.M.Piskarev
Decay Characteristics of Dipole Giant Resonance in the Nucleus 39K
NUCLEAR REACTIONS 39K(γ, p), (γ, n), (γ, α), E ≤ 32 MeV; analyzed integrated, partial σ. 38Ar, 38K, 35Cl deduced levels, J, π.
Appl.Radiat.Isot. 38, 845 (1987)
T.Genka, K.Kobayashi, S.Hagiwara
A Calorimeter for the Measurement of the Activity of Tritium and Other Pure Beta Emitters
RADIOACTIVITY 3H, 14C, 35S, 32P(β-); measured maximum, average β- energies; deduced heating powers. Microcalorimeter.
Phys.Lett. 192B, 39 (1987)
A.Gillibert, W.Mittig, L.Bianchi, A.Cunsolo, B.Fernandez, A.Foti, J.Gastebois, C.Gregoire, Y.Schutz, C.Stephan
New Mass Measurements Far From Stability
NUCLEAR REACTIONS Ta(40Ar, X), E=60 MeV/nucleon; measured fragment rigidity, tof. 17B, 19,20C, 20,21,22N, 23,24O, 24,25,26F, 27,28Ne, 30,31,32Na, 31,32,33Mg, 32,33,34,35Al, 36,37Si, 37,38P deduced mass excess.
doi: 10.1016/0370-2693(87)91138-5
Indian J.Phys. 61A, 209 (1987)
R.Nathuram, G.Subrahmanian, S.R.Thontadarya
Range of Beta Particles in 4π Geometry
RADIOACTIVITY 35S, 45Ca, 60Co, 137Cs(β-); 170Tm, 204Tl(β-), (EC); 91,90Y(β-); 32P(β+); measured β-endpoint energies; deduced mass attenuation coefficient, β-range relation. 4 π geometry.
Phys.Rev. C35, 1851 (1987)
E.K.Warburton, J.A.Becker
Shell-Model Description of the Beta Decay of the N = 21 Isotones 35Si and 36P
NUCLEAR STRUCTURE 35Si, 35,36P, 36S; calculated binding energies. Shell model.
RADIOACTIVITY 36P, 35Si(β-); calculated T1/2, log ft, branching ratio, Gamow-Teller transition strengths, Eγ, Γγ. 35P, 36S deduced levels, B(λ), decay characteristics. Shell model.
Nucl.Instrum.Methods Phys.Res. A273, 748 (1988)
Y.Charon, J.C.Cuzon, H.Tricoire, L.Valentin
A High Resolution β- Detector
RADIOACTIVITY 3H, 32P, 35S(β-); measured β-detector efficiency. High resolution.
doi: 10.1016/0168-9002(88)90090-3
Nucl.Instrum.Methods Phys.Res. A265, 475 (1988)
F.Corvi, A.Prevignano, H.Liskien, P.B.Smith
An Experimental Method for Determining the Total Efficiency and the Response Function of a Gamma-Ray Detector in the Range 0.5-10 MeV
NUCLEAR REACTIONS 26Mg(p, γ), E=1.001, 2.22 MeV; 30Si(p, γ), E=1.398 MeV; 34S(p, γ), E=1.211 MeV; measured γγ-coin; deduced weighting function. 56Fe(n, γ), E=1.15 keV; analyzed capture reaction data. 57Fe resonance deduced (gΓnΓγ/γ).
doi: 10.1016/S0168-9002(98)90016-X
Priv.Comm. (1988)
J.P.Dufour
RADIOACTIVITY 35,36Si, 36P(β-) [from 9Be(40Ar, X), E=60 MeV/nucleon]; measured Eγ, Iγ. 35,36P, 36S; deduced levels, J, π, β-branching, logft.
Proc. 5th Int.Conf.Nuclei Far from Stability, Rosseau Lake, Canada 1987, Ed., I.S.Towner, p.344 (1988), AIP Conf.Proc. 164 (1987)
J.P.Dufour, R.Del Moral, F.Hubert, D.Jean, M.S.Pravikoff, A.Fleury, H.Delagrange, A.C.Mueller, K.-H.Schmidt, E.Hanelt, K.Summerer, J.Frehaut, M.Beau, G.Giraudet
Spectroscopic Measurements with a New Method: The projectile-fragments isotopic separation
RADIOACTIVITY 17C, 19,20N, 22O, 23,24F, 25,26Ne, 27Na, 30Mg, 32,33,34,35Al, 34,35,36,37Si, 36,37,38P, 40S(β-) [from 9Be(40Ar, X), E=60 MeV/nucleon]; measured Eγ, T1/2, production rates. 26Ne, 35Si, 36P(β-); measured Eγ, Iγ. 26Na, 35P, 36S; deduced levels, J, π, β-branching, logft. 17,18,19C, 17B, 14Be(β-n)[from Be, Ta(22Na, X), E=60 MeV/nucleon]; measured β--delayed 1n, 2n, 3n and 4n emission, associated multiplicity, T1/2 for 14Be, 17B and 19C; deduced evidence for beta-delayed 4n-decay mode. Comparison with shell model calculations. LISE spectrometer at GANIL.
doi: 10.1063/1.36999
Phys.Rev.Lett. 60, 499 (1988)
J.D.Garnett, E.D.Commins, K.T.Lesko, E.B.Norman
β-Decay Asymmetry Parameter for 35Ar: An anomaly resolved
RADIOACTIVITY 35Ar(β+), (EC) [from 35Cl(polarized p, n), E=10 MeV]; measured β-decay asymmetry parameter; deduced quark mixing angle.
doi: 10.1103/PhysRevLett.60.499
Z.Phys. A330, 63 (1988)
A.C.Mueller, D.Bazin, W.D.Schmidt-Ott, R.Anne, D.Guerreau, D.Guillemaud-Mueller, M.G.Saint-Laurent, V.Borrel, J.C.Jacmart, F.Pougheon, A.Richard
β-Delayed Neutron Emission of 15B, 18C, 19,20N, 34,35Al and 39P
RADIOACTIVITY 15B, 18C, 19,20N, 34,35Al, 39P(β-n) [from 181Ta(86Kr, X), E=45 MeV/nucleon]; measured T1/2, neutron emission probabilities.
Nucl.Phys. A477, 523 (1988); Erratum Nucl.Phys. A485, 734 (1988)
N.A.Orr, W.N.Catford, L.K.Fifield, T.R.Ophel, D.C.Weisser, C.L.Woods
Heavy-Ion Reaction Studies of 35,36P
NUCLEAR REACTIONS 37Cl(11B, 13N), 37Cl(13C, 14O), 34S(18O, 17F), E=81-108 MeV; measured σ(E(13N)), σ(E(14O)), σ(E(17F)). 35,36P deduced ground-state mass excess, levels. Enriched targets.
doi: 10.1016/0375-9474(88)90355-7
Nucl.Phys. A480, 77 (1988)
O.P.van Pruissen, G.J.L.Nooren, C.van der Leun
Primary Gamma-Ray Transitions of Mixed E1 + M2 Character
NUCLEAR REACTIONS 30Si(p, γ), E ≈ 1.94, 2.11 MeV; 34S(p, γ), E=0.4-0.7 MeV, E ≈ 1.47 MeV; measured σ(E(p)), σ(θ), I(γ). 31P, 35Cl deduced resonances, Γ, J, π, γ-branching, δ(M2/E1). Enriched targets.
doi: 10.1016/0375-9474(88)90385-5
Izv.Akad.Nauk SSSR, Ser.Fiz. 52, 923 (1988); Bull.Acad.Sci.USSR, Phys.Ser. 52, No.5, 86 (1988)
P.P.Zarubin, V.P.Gusev, A.E.Antropov
Compound-Nucleus Proton Elastic Scattering Cross Sections at E(p) ≈ 6 MeV
NUCLEAR REACTIONS 23Na, 24,25,26Mg, 27Al, 28,29,30Si, 31P, 32,33,34,36S, 35Cl, 46,48,50Ti, 51V, 50,52,53,54Cr, 55Mn, 54,56,57Fe(p, p), E=6 MeV; measured integral σ.
Phys.Rev. C39, 216 (1989)
N.M.Badiger, N.Umakantha
Internal Bremsstrahlung Spectrum of 35S in the Range from 10 to 100 keV
RADIOACTIVITY 35S(β-); measured inner bremsstrahlung spectrum.
Phys.Rev. C39, 128 (1989)
P.A.DeYoung, M.S.Gordon, Xiuqin Lu, R.L.McGrath, J.M.Alexander, D.M.de Castro Rizzo, L.C.Vaz
Emission Times in Low-Energy Heavy-Ion Reactions by Particle-Particle Correlations
NUCLEAR REACTIONS 27Al(16O, 2p), (16O, 2α), E=140 MeV; measured pp, αα correlations; deduced successive proton emission interval T1/2, (αα) correlations problematics.
Fiz.Elem.Chastits At.Yadra 20, 930 (1989); Sov.J.Part.Nucl. 20, 393 (1989)
M.K.Georgieva, D.V.Elenkov, D.P.Lefterov, G.H.Toumbev
Measurement of the Lifetimes of Excited Nuclear States by the Doppler Shift Attenuation Method Using the Reaction (n, n'γ) with Two Targets
NUCLEAR REACTIONS 11B, 23Na, 24Mg, 27Al, 28Si, 31P, 32S, 35,37Cl, 39K, 40Ca, 45Sc, 48Ti, 51V, 52Cr, 55Mn, 56Fe, 58,60,64Ni(n, n'γ), E=fast; measured γ-spectra, DSA. 11B, 23Na, 24Mg, 27Al, 28Si, 31P, 32S, 35,37Cl, 39K, 40Ca, 45Sc, 48Ti, 51V, 52Cr, 55Mn, 56Fe, 58,60,64Ni level deduced T1/2, B(λ).
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.
Nucl.Phys. A496, 477 (1989)
M.Lewitowicz, Yu.E.Penionzhkevich, A.G.Artukh, A.M.Kalinin, V.V.Kamanin, S.M.Lukyanov, Nguyen Hoai Chau, A.C.Mueller, D.Guillemaud-Mueller, R.Anne, D.Bazin, C.Detraz, D.Guerreau, M.G.Saint-Laurent, V.Borrel, J.C.Jacmart, F.Pougheon, A.Richard, W.D.Schmidt-Ott
β-Delayed Neutron Emission of the Isotopes 20C, 40,41,42P, 43,44S
RADIOACTIVITY 15,17B, 18,20C, 35Al, 40,41,42P, 43,44S [from 181Ta(48Ca, X)]; measured T1/2, delayed n emission probabilities.
doi: 10.1016/0375-9474(89)90072-9
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.Instrum.Methods Phys.Res. A274, 345 (1989)
M.Takiue, T.Natake, H.Fujii
Nuclide Identification of β-Emitter by a Double Ratio Technique Using a Liquid Scintillation Counter
RADIOACTIVITY 3H, 14C, 32P(β-); 36Cl(β-), (β+), (EC); 63Ni, 35S, 45Ca(β-); measured β-activity; deduced quenching correction role in nuclide identification. Computer aided quenching correction, liquid scintillation double ratio technique.
doi: 10.1016/0168-9002(89)90400-2
Nucl.Phys. A519, 529 (1990)
C.Detraz, R.Anne, P.Bricault, D.Guillemaud-Mueller, M.Lewitowicz, A.C.Mueller, Y.H.Zhang, V.Borrel, J.C.Jacmart, F.Pougheon, A.Richard, D.Bazin, J.P.Dufour, A.Fleury, F.Hubert, M.S.Pravikoff
Search for Direct Two-Proton Radioactivity from Ti Isotopes at the Proton Drip Line
RADIOACTIVITY 39,40Ti(β+p); [from 58Ni(58Ni, X), E=65 MeV/nucleon]; measured β-delayed charged particle spectra. 39,40Ti deduced T1/2. Magnetic analysis, tof, solid state detector telescope.
doi: 10.1016/0375-9474(90)90445-R
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
Phys.Rev. A42, 1160 (1990)
D.Sundholm, J.Olsen
Nuclear Quadrupole Moments of 33S and 35S
NUCLEAR MOMENTS 33,35S; calculated quadrupole moments. Multi-configurational Hartree-Fock.
Pramana 37, 269 (1991)
H.C.Jain, S.Chattopadhyay, Y.K.Agarwal, M.L.Jhingan, S.K.Mitra, H.V.Panchal, A.Roy
A Plunger Set-Up for Measuring Picosecond Nuclear Half-Lives
NUCLEAR REACTIONS 27Al(16O, xnypzα), E=60 MeV; measured Eγ, Iγ, recoil distance. 35Cl, 37,38Ar, 40K levels deduced T1/2. Plunger technique.
Nucl.Instrum.Methods Phys.Res. A300, 293 (1991)
S.Lindenstruth, A.Degener, R.D.Heil, A.Jung, U.Kneissl, J.Margraf, H.H.Pitz, H.Schacht, U.Seemann, R.Stock, C.Wesselborg
Measurements and Simulations of Low Energy, Thick Target Bremsstrahlung Spectra
NUCLEAR REACTIONS 13C, 23Na, 27Al, 31P, 35Cl, 48Ti(γ, γ'), E=4.1 MeV bremsstrahlung; measured Eγ, Iγ. Nuclear resonance fluorescence technique, Monte Carlo simulations.
doi: 10.1016/0168-9002(91)90439-W
Phys.Rev. C44, 1995 (1991)
M.A.Miller, P.A.Voytas, A.D.Roberts, P.A.Quin, W.Haeberli
Polarization Transfer in the 23Na(p(pol), 23Mg(pol))n, 31P(p(pol), 31S(pol))n, and 35Cl(p(pol), 35Ar(pol))n Reactions
NUCLEAR REACTIONS 31P(polarized p, n), E=6.38-9.1 MeV; 35Cl(polarized p, n), E=7.27-10.29 MeV; 23Na(polarized p, n), E ≈ 7 MeV; measured residual nucleus β+-decay parity violating asymmetry; deduced polarization transfer coefficient energy dependence. NaI, red phosphorous, Cl2, CCL4-(He) mixture targets.
RADIOACTIVITY 31S [from 31P(polarized p, n), E=6.38-9.1 MeV]; 35Ar [from 35Cl(polarized p, n), E=7.27-10.29 MeV]; 23Mg [from 23Na(polarized p, n), E ≈ 7 MeV]; measured β+-decay parity violating asymmetry.
J.Phys.(London) G17, 919 (1991)
O.Naviliat-Cuncic, T.A.Girard, J.Deutsch, N.Severijns
Left-Right Symmetry Breaking Sensitivity of β-Asymmetry Measurements
RADIOACTIVITY 13N, 17F, 35Ar, 29P, 31S; analyzed decay data; deduced β-asymmetry parameters limits, left-right symmetry breaking role. Other nuclei considered.
doi: 10.1088/0954-3899/17/6/013
Phys.Lett. 258B, 29 (1991)
N.A.Orr, W.Mittig, L.K.Fifield, M.Lewitowicz, E.Plagnol, Y.Schutz, Z.W.Long, L.Bianchi, A.Gillibert, A.V.Belozyorov, S.M.Lukyanov, Yu.E.Penionzhkevich, A.C.C.Villari, A.Cunsolo, A.Foti, G.Audi, C.Stephan, L.Tassan-Got
New Mass Measurements of Neutron-Rich Nuclei Near N = 20
NUCLEAR REACTIONS Ta(48Ca, X), E=55 MeV/nucleon; measured projectile like fragment spectra. 17,19B, 20C, 20,21,22N, 22,23,24O, 24,25,26,27F, 26,27,28,29,30Ne, 28,29,30,31,32,33Na, 30,31,32,33,34,35Mg, 32,33,34,35,36,37Al, 36,37Si, 37P deduced mass excess.
doi: 10.1016/0370-2693(91)91203-8
Phys.Rev. C44, 514 (1991)
A.Ray, D.Shapira, J.Gomez del Campo, H.J.Kim, C.Beck, B.Djerroud, B.Heusch, D.Blumenthal, B.Shivakumar
Compound Nucleus Origin of Back-Angle Yields in the 31P + 16O and 35Cl + 12C Reactions
NUCLEAR REACTIONS 16O(31P, 16O), 16O(31P, 12C), E=135.6 MeV; measured σ(E, θ); deduced entrance channel dependence, orbiting yield. Comparison with other data.
Phys.Lett. 260B, 285 (1991)
X.G.Zhou, X.L.Tu, J.M.Wouters, D.J.Vieira, K.E.G.Lobner, H.L.Seifert, Z.Y.Zhou, G.W.Butler
Direct Mass Measurements of the Neutron-Rich Isotopes of Fluorine Through Chlorine
NUCLEAR REACTIONS Th(p, X), E=800 MeV; measured fragment mass, charge state ratio, velocity histograms. 24,25,26,27F, 27,28,29Ne, 30,31,32Na, 30,31,32,33,34Mg, 33,34,35,36Al, 36,37,38Si, 38,39,40,41P, 40,41,42,43S, 41,42,43,44Cl deduced mass excess.
doi: 10.1016/0370-2693(91)91613-Z
J.Radioanal.Nucl.Chem. 166, 493 (1992)
M.Belgaid, M.Siad, M.Allab
Measurement of 14.7 MeV Neutron Cross Sections for Several Isotopes
NUCLEAR REACTIONS 24Mg, 27Al, 28,29,30Si, 35,37Cl, 45Sc, 46Ti, 56Fe, 58,61Ni, 92Mo, 107Ag, 113,115In, 197Au(n, p), (n, α), (n, 2n), (n, np), (n, n'γ), E=14.73 MeV; measured Eγ, Iγ; deduced reaction σ. Hyperpure Ge detector.
Phys.Rev.Lett. 69, 3151 (1992)
M.Chen, D.A.Imel, T.J.Radcliffe, H.Henrikson, F.Boehm
New Limits on the 17 keV Neutrino
RADIOACTIVITY 35S(β-); measured β-spectrum; deduced no heavy ν evidence, admixture upper limit.
doi: 10.1103/PhysRevLett.69.3151
Phys.Lett. 276B, 423 (1992)
K.H.Hicks, D.E.Alburger
Search for Light Neutral Boson Associated with Beta Decay
RADIOACTIVITY 35S(β-); measured γγ-coin; deduced no evidence for light neutral boson. High parity Ge low energy photon detectors.
doi: 10.1016/0370-2693(92)91661-R
Z.Phys. A342, 273 (1992)
D.M.Moltz, J.C.Batchelder, T.F.Lang, T.J.Ognibene, J.Cerny, P.E.Haustein, P.L.Reeder
Beta-Delayed Two-Proton Decay of 39Ti
RADIOACTIVITY 39Ti(β+p) [from Ca(3He, X), E=110 MeV]; measured two-proton energy sum spectra following β-decay; deduced decay scheme, energy available for two-proton emission. 39Sc deduced IAS.
Phys.Lett. 316B, 26 (1993)
H.Abele, G.Helm, U.Kania, C.Schmidt, J.Last, D.Dubbers
On the Origin of the 17 keV Neutrino Signals, and a Loss-Free Measurement of the 35S β-Spectrum
RADIOACTIVITY 35S(β-); measured β-spectra; deduced no 17 keV neutrino evidence. Virtually loss free β-spectroscopy method.
doi: 10.1016/0370-2693(93)90652-X
Phys.Rev. C48, R1 (1993)
G.E.Berman, M.L.Pitt, F.P.Calaprice, M.M.Lowry
New Evidence Against 17-keV Neutrino Emission in the β Decay Momentum Spectrum of 35S
RADIOACTIVITY 35S(β-); measured β-spectra; deduced no 17 keV neutrino emission evidence.
Nucl.Instrum.Methods Phys.Res. B79, 524 (1993)
I.Bogdanovic, S.Fazinic, M.Jaksic, T.Tadic, O.Valkovic, V.Valkovic
Proton Elastic Scattering from Fluorine, Chlorine, Zinc, Selenium and Bromine in the Energy Region from 2.5 to 4.8 MeV
NUCLEAR REACTIONS 19F, 37,35Cl, Zn, Se, Br(p, p), (p, p'), E=2.5-4.8 MeV; measured σ(θ) data.
doi: 10.1016/0168-583X(93)95405-T
Phys.Lett. 304B, 60 (1993)
A.Converse, M.Allet, W.Haeberli, W.Hajdas, J.Lang, J.Liechti, H.Luscher, M.A.Miller, R.Muller, O.Naviliat-Cuncic, P.A.Quin, J.Sromicki
Measurement of the Asymmetry Parameter for 35Ar β-Decay as a Test of the CVC Hypothesis
RADIOACTIVITY 35Ar(β+) [from 35Cl(polarized p, n)35Ar, E=9.2 MeV]; measured β-decay, βγ-coin, asymmetry parameter, Eβ, Iβ; deduced conserved vector current hypothesis implications. Polarized source.
doi: 10.1016/0370-2693(93)91400-H
Nucl.Instrum.Methods Phys.Res. A334, 645 (1993)
T.A.Girard, R.P.Henriques, J.I.Collar, M.Godinho, G.Bonfait, G.Waysand, D.Limagne, V.Jeudy, V.Pagesy
Response of a Metastable Superconducting Grains Suspension to Irradiation by 35S Decay Electrons
RADIOACTIVITY 35S(β-); measured electron energy loss spectrum. Prototype detector composed of a suspension.
doi: 10.1016/0168-9002(93)90834-5
Nucl.Instrum.Methods Phys.Res. A325, 234 (1993)
A.Grau Carles, L.Rodriguez Barquero, A.Grau Malonda
Standardization of 14C and 35S Mixtures
RADIOACTIVITY 14C(β-); 35S(β-); measured β-spectra unfolding, quench intensities; deduced mixed source standardization. Liquid scintillation spectrometry.
doi: 10.1016/0168-9002(93)91025-I
Nucl.Phys. A565, 543 (1993)
G.Mairle, M.Seeger, H.Reinhardt, T.Kihm, K.T.Knopfle, C.L.Wen
The Distribution of Proton-Hole Strengths in the (2s, 1d)-Shell of 35Cl, 37Cl and 39Cl
NUCLEAR REACTIONS 36,38,40Ar(polarized d, 3He), E=52 MeV; measured σ(θ), iT11(θ). 35,37,39Cl deduced levels, J, π, spectroscopic factors, proton occupancies, single-particle energies, spreading widths. 39Cl deduced mass excess. Enriched 36,38Ar gas targets. DWBA analysis.
doi: 10.1016/0375-9474(93)90044-X
Phys.Rev.Lett. 70, 394 (1993)
J.L.Mortara, I.Ahmad, K.P.Coulter, S.J.Freedman, B.K.Fujikawa, J.P.Greene, J.P.Schiffer, W.H.Trzaska, A.R.Zeuli
Evidence Against a 17 keV Neutrino from 35S Beta Decay
RADIOACTIVITY 35S(β-); measured β-spectrum; deduced evidence against 17 keV neutrino. Mixed 35S, 14C source.
doi: 10.1103/PhysRevLett.70.394
J.Chem.Phys. 98, 7152 (1993)
D.Sundholm, J.Olsen
Finite Element Multiconfiguration Hartree-Fock Determination of the Nuclear Quadrupole Moments of Chlorine, Potassium, and Calcium Isotopes
NUCLEAR MOMENTS 35,36,37Cl, 39,40,41K, 41,43,45,47Ca; calculated quadrupole moments.
Phys.Lett. 331B, 193 (1994)
M.G.Bowler, N.A.Jelley
The Origin of the Spurious 17 keV Neutrino Signal Observed in 35S Beta-Decay
RADIOACTIVITY 35S(β-); measured β-spectra; deduced spurious 17 keV ν signal origin. Different geometries, collimation, source thickness, clumping associated energy loss effects.
doi: 10.1016/0370-2693(94)90963-6
Phys.Rev. C49, 2413 (1994)
B.Fornal, R.H.Mayer, I.G.Bearden, Ph.Benet, R.Broda, P.J.Daly, Z.W.Grabowski, I.Ahmad, M.P.Carpenter, P.B.Fernandez, R.V.F.Janssens, T.L.Khoo, T.Lauritsen, E.F.Moore, M.Drigert
Gamma Ray Studies of Neutron-Rich sdf Shell Nuclei Produced in Heavy Ion Collisions
NUCLEAR REACTIONS 160Gd(34S, X), E=159 MeV; 160Gd(36S, X), E=159 MeV; 160Gd(37Cl, X), E=167 MeV; measured γγ-coin; deduced reaction mechanism. 38,36S, 37,39Cl, 34,35P, 34,33Si deduced level schemes.
Appl.Radiat.Isot. 45, 83 (1994)
A.Grau Carles
A New Linear Spectrum Unfolding Method Applied to Radionuclide Mixtures in Liquid Scintillation Spectrometry
RADIOACTIVITY 204Tl(β-), (EC); 45Ca(β-); 35S(β-); 36Cl(β+), (β-), (EC); 14C(β-); 3H(β-); measured β-counting rates, spectra; deduced new technique convenience. New linear spectrum unfolding method. Mixtures of 12C+3H, 45Ca+35Sc, 204Tl+36Cl sources.
doi: 10.1016/0969-8043(94)90152-X
J.Radioanal.Nucl.Chem. 187, 367 (1994)
Y.Homma, Y.Murase, K.Handa
Absolute Liquid Scintillation Counting of 35S and 45Ca using a Modified Integral Counting Method
RADIOACTIVITY 45Ca(β-); 35S(β-); measured β-disintegration rates. Modified integral counting method.
Z.Naturforsch. 49a, 874 (1994)
S.Muller, S.Chen, H.Daniel, O.Dragoun, N.Dragounova, H.Hagn, E.Hechtl, K.-H.Hiddemann, A.Spalek
Search for an Admixture of a 17 keV Neutrino in the β Decay of 35S
RADIOACTIVITY 35S(β-); measured β spectra; deduced 17 keV neutrino admixture upper limit, electron scattering neglect related uncertainities.
Nucl.Phys. A571, 221 (1994)
A.Poves, J.Retamosa
Theoretical Study of the Very Neutron-Rich Nuclei Around N = 20
NUCLEAR STRUCTURE 28O, 34Si, 30Ne, 32Mg; calculated intruder levels, B(λ), quadrupole moments. 27,28,29,30O, 28,29,30,31F, 29,30,31,32Ne, 30,31,32,33Na, 31,32,33,34Mg, 32,33,34,35Al, 33,34,35,36Si; calculated levels, binding energies. Shell model.
doi: 10.1016/0375-9474(94)90058-2
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
Z.Phys. C68, 391 (1995)
M.G.Bowler, N.A.Jelley
Investigations into the Origin of the Spurious 17 keV Neutrino Signal Observed in 35S Beta Decay
RADIOACTIVITY 35S(β-); measured β spectrum; deduced β-endpoint energy, 17 keV neutrino admixture upper limit.
Phys.Rev. C51, 3487 (1995)
A.Garcia, E.G.Adelberger, P.V.Magnus, H.E.Swanson, F.E.Wietfeldt, O.Tengblad, and the Isolde Collaboration
36Ca β Decay and the Isobaric Multiplet Mass Equation
RADIOACTIVITY 36Ca(β+p); measured β-delayed Ep, Ip. 36K deduced T=2 states mass. Precise test of the isobaric multiplet mass equation.
Phys.Lett. 347B, 152 (1995)
S.Moriyama, M.Minowa
The 17 keV Neutrino and the Search for Anomalous γ Rays in 35S Decay
RADIOACTIVITY 35S(β-); measured Eγ, Iγ; deduced external, internal bremsstrahlung role, proposed 17 keV neutrino hypothesis exclusion.
doi: 10.1016/0370-2693(95)00040-R
Proc.Intern.Conf on Exotic Nuclei and Atomic Masses, Arles, France, June 19-23, 1995, p.587 (1995)
P.L.Reeder, Y.Kim, W.K.Hensley, H.S.Miley, R.A.Warner, Z.Y.Zhou, D.J.Vieira, J.M.Wouters, H.L.Seifert
Beta Decay Half-Lives and Delayed Particle Emission from TOFI Measurements
NUCLEAR REACTIONS 232Th(p, X), E=800 MeV; measured β(fragment)-coin; deduced T1/2 for 8Li to 45Cl. Tof isochronous spectrometer.
RADIOACTIVITY 25,26F, 28Ne, 35Mg, 33,36Ar, 41S, 44Cl(β-n) [from 232Th(p, X), E=800 MeV]; measured T1/2. 31,35Mg, 14B, 17C, 18N, 32,33,34,35Al, 36,37Si, 38P, 45Cl(β-n) [from 232Th(p, X), E=800 MeV]; measured neutron emission probabilities. Tof isochronous spectrometer.
Phys.Lett. 348B, 331 (1995)
W.Trinder, E.G.Adelberger, B.A.Brown, Z.Janas, H.Keller, K.Krumbholz, V.Kunze, P.Magnus, F.Meissner, A.Piechaczek, M.Pfutzner, E.Roeckl, K.Rykaczewski, W.-D.Schmidt-Ott, M.Weber
Gamow-Teller Strength in the β-Decay of 36Ca
RADIOACTIVITY 36Ca(β+p); measured βγ-coin, β+-delayed proton spectra, T1/2; deduced log ft, Gamow-Teller transition strength.
doi: 10.1016/0370-2693(95)00130-D
Nucl.Instrum.Methods Phys.Res. A373, 65 (1996)
V.Jeudy, J.I.Collar, T.A.Girard, D.Limagne, G.Waysand
35S Beta Irradiation of a Tin Strip in a State of Superconducting Geometrical Metastability
RADIOACTIVITY 35S(β-); measured spectra; deduced thermal nucleation breaking geometric metastability. Irradiation of Sn strip in a state of superconducting geometrical metastability.
doi: 10.1016/0168-9002(95)01451-9
Yad.Fiz. 59, No 5, 775 (1996); Phys.Atomic Nuclei 59, 739 (1996)
A.S.Kachan, A.N.Vodin, V.M.Mishchenko, R.P.Slabospitsky
Fine Structure of the M1 Resonance in 35Cl
NUCLEAR REACTIONS 34S(p, γ), E=1-3 MeV; measured Eγ, Iγ, γ(θ). 35Cl deduced M1 resonance, fine structure, resonance strength.
Nucl.Phys. A607, 1 (1996)
A.Klein, B.A.Brown, U.Georg, M.Keim, P.Lievens, R.Neugart, M.Neuroth, R.E.Silverans, L.Vermeeren, and the ISOLDE Collaboration
Moments and Mean Square Charge Radii of Short-Lived Argon Isotopes
NUCLEAR MOMENTS 36,38,40Ar; measured isotope shifts, hfs; deduced hyperfine constants, spins I, μ, electric quadrupole moments, mean square charge radii. Collinear fast-beam laser spectroscopy, collisional ionization and β-detection. Shell model.
RADIOACTIVITY 32,33,34,35Ar(β+); 37Ar(EC); 39,46Ar(β-); measured isotope shifts, hfs; deduced hyperfine constants, spins I, μ, electric quadrupole moments, mean square charge radii. Collinear fast-beam laser spectroscopy, collisional ionization and β-detection. Shell model.
doi: 10.1016/0375-9474(96)00192-3
Bull.Rus.Acad.Sci.Phys. 60, 805 (1996)
A.N.Vodin, A.S.Kachan, V.M.Mishchenko, R.P.Slabospitsky
Isobar-Analogue d5/2 State in the 35Cl Nucleus
NUCLEAR REACTIONS 34S(p, γ), E ≤ 4 MeV; measured Eγ, Iγ. 35Cl deduced resonances, J, π, Γγ, d5/2 IAR.
Nucl.Phys. A621, 235c (1997)
H.Beer, C.Coceva, R.Hofinger, P.Mohr, H.Oberhummer, P.V.Sedyshev, Yu.P.Popov
Measurement of Direct Neutron Capture by Neutron-Rich Sulfur Isotopes
NUCLEAR REACTIONS 34,36S(n, γ), E=reactor; measured Eγ, Iγ; deduced capture σ. 35,37S deduced levels, J, π, spectroscopic factors. Direct capture model.
doi: 10.1016/S0375-9474(97)00244-3
Phys.Rev. C55, 762 (1997)
B.Fornal, R.Broda, W.Krolas, T.Pawlat, J.Wrzesinski, D.Bazzacco, D.Fabris, S.Lunardi, C.Rossi Alvarez, G.Viesti, G.de Angelis, M.Cinausero, D.R.Napoli, Z.W.Grabowski
γ-Ray Studies of Neutron-Rich N = 18, 19 Nuclei Produced in Deep-Inelastic Collisions
NUCLEAR REACTIONS, ICPND 208Pb(37Cl, X)38Cl/39Cl/40Cl/39S/40S/36P/37P/38P/32Si/33Si/34Si/35Si/36Si/30Al/31Al/32Al/34Al/28Mg/29Mg/30Mg/31Mg/28Na, E=230 MeV; measured γγ-coin; deduced residuals yields. 32Si deduced isomer, T1/2. 32Al deduced levels, possible J, π.
Nucl.Phys. A621, 211c (1997)
C.Iliadis, R.E.Azuma, J.Chow, J.D.King, A.C.Morton, L.Buchmann, M.Dombsky, K.P.Jackson, J.M.D'Auria, U.Giesen, J.G.Ross, H.Schatz, M.Wiescher
Decay Studies of Importance to Explosive Hydrogen Burning
RADIOACTIVITY 36K(β+p), (β+α) [from Ca(p, X), E=500 MeV]; measured α-, proton spectra; deduced log ft. 36Ar deduced α-emitting resonance.
doi: 10.1016/S0375-9474(97)00240-6
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. A620, 191 (1997)
W.Trinder, E.G.Adelberger, B.A.Brown, Z.Janas, H.Keller, K.Krumbholz, V.Kunze, P.Magnus, F.Meissner, A.Piechaczek, M.Pfutzner, E.Roeckl, K.Rykaczewski, W.-D.Schmidt-Ott, M.Weber
Study of the β Decays of 37Ca and 36Ca
RADIOACTIVITY 37,36Ca(β+p) [from 9Be(40Ca, X), E=300 MeV/nucleon]; measured β-delayed Ep, Ip, Eγ, Iγ, βγ-, βγp-coin, T1/2. 37K deduced levels isospin mixing. 36K levels deduced J, π assignment nonvalidity. Ge, Si detectors. sd-shell model.
doi: 10.1016/S0375-9474(97)00163-2
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.
Phys.Rev. C58, 2831 (1998)
B.J.Cole
Proton and Two-Proton Drip Lines in the sd Shell
NUCLEAR STRUCTURE 21,22Al, 22,23Si, 23,24,25,26P, 25,26,27,28S, 27,28,29,30Cl, 29,30,31Ar, 31,32,33,34K, 32,33,34,35Ca; calculated binding energies, one-, two-proton separation energies; deduced proton, diproton drip lines.
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
Nuovo Cim. 111A, 835 (1998)
M.Lewitowicz, W.Trinder, M.Bhattacharya, E.G.Adelberger, J.C.Angelique, R.Anne, J.Aysto, C.Borcea, J.M.Daugas, C.Donzaud, A.Garcia, S.Grevy, R.Grzywacz, D.Guillemaud-Mueller, A.Jokinen, N.I.Kaloskamis, S.Leenhardt, M.J.Lopez, A.C.Mueller, F.de Oliveira, A.Ostrowski, F.Pougheon, M.G.Saint-Laurent, T.Siiskonen, O.Sorlin, H.E.Swanson
Beta-Decay of Light Nuclei Close to the Proton Drip-Line: 40Ti and 35Ca
RADIOACTIVITY 40Ti, 35Ca(β+) [from Ni(50Cr, X), (40Ca, X)]; measured β-delayed proton spectra, Eγ, T1/2, B(F), B(GT). 35K deduced IAS. Implications for solar neutrino detector efficiency discussed.
Phys.Rev. C57, 2205 (1998)
M.Schafer, W.-D.Schmidt-Ott, T.Dorfler, T.Hild, T.Pfeiffer, R.Collatz, H.Geissel, M.Hellstrom, Z.Hu, H.Irnich, N.Iwasa, M.Pfutzner, E.Roeckl, M.Shibata, B.Pfeiffer, K.Asahi, H.Izumi, H.Ogawa, H.Sato, H.Ueno, H.Okuno
Polarization in Fragmentation, g Factor of 35K
NUCLEAR REACTIONS 9Be(40Ca, X)39Ca/35K/37K, E=500 MeV/nucleon; measured fragments beta asymmetry; deduced polarization. 35K deduced g factor. Projectile fragment separator.
RADIOACTIVITY 35K(β+) [from 9Be(40Ca, X)]; measured T1/2. Projectile fragment separator.
Phys.Rev. C60, 034614 (1999)
N.Aissaoui, N.Added, N.Carlin, G.M.Crawley, S.Danczyk, J.Finck, M.M.de Moura, D.Hirata, D.J.Morrissey, S.J.Sanders, J.Stasko, M.Steiner, A.A.P.Suaide, E.M.Szanto, A.Szanto de Toledo, M.Thoennessen, J.A.Winger
Strong Absorption Radii from Reaction Cross Section Measurements for Neutron-Rich Nuclei
NUCLEAR REACTIONS Si(30Al, X), (31Al, X), (32Al, X), (33Al, X), (32Si, X), (33Si, X), (34Si, X), (35Si, X), (36Si, X), (34P, X), (35P, X), (36P, X), (37P, X), (38P, X), (39P, X), (36S, X), (37S, X), (38S, X), (39S, X), (40S, X), (41S, X), (39Cl, X), (40Cl, X), (41Cl, X), (42Cl, X), (43Cl, X), (44Cl, X), (41Ar, X), (42Ar, X), (43Ar, X), (44Ar, X), (45Ar, X), (46Ar, X), (44K, X), (45K, X), (46K, X), (47K, X), (48K, X), (46Ca, X), (47Ca, X), (48Ca, X), (49Ca, X), (50Ca, X), (49Sc, X), (50Sc, X), (51Sc, X), (52Sc, X), (53Ti, X), (54Ti, X), E ≈ 38-80 MeV/nucleon; measured mean energy-integrated reaction σ. 30,31,32,33Al, 32,33,34,35,36Si, 34,35,36,37,38,39P, 36,37,38,39,40,41S, 39,40,41,42,43,44Cl, 41,42,43,44,45,46Ar, 44,45,46,47,48K, 46,47,48,49,50Ca, 49,50,51,52Sc, 53,54Ti deduced strong absorption radii. Secondary beams from 55Mn fragmentation.
doi: 10.1103/PhysRevC.60.034614
Phys.Rev. C59, 642 (1999)
R.W.Ibbotson, T.Glasmacher, P.F.Mantica, H.Scheit
Coulomb Excitation of Odd-A Neutron-Rich π(s-d) and ν(f-p) Shell Nuclei
NUCLEAR REACTIONS 197Au(35Al, 35Al'), (37Si, 37Si'), (39P, 39P'), (41S, 41S'), (43S, 43S'), (45Cl, 45Cl'), E=42-47.4 MeV/nucleon; measured Eγ, Iγ following Coulomb excitation. 35Al, 37Si, 39P, 41,43S, 45Cl; deduced levels, J, π, excitation B(E2). Secondary beams from 48Ca fragmentation.
Phys.Rev. C60, 044604 (1999)
D.Ohsawa, R.Katano, Y.Isozumi
K-Shell Internal Ionization and Excitation in β Decay of 35S
RADIOACTIVITY 35S(β-); measured X-ray spectra; deduced K-shell transition probability. Internal ionization.
ATOMIC PHYSICS 35S(β-); measured X-ray spectra; deduced K-shell transition probability. Internal ionization.
doi: 10.1103/PhysRevC.60.044604
Nucl.Instrum.Methods Phys.Res. A423, 337 (1999)
L.Palermo, E.Holzschuh, W.Kundig, P.Wenk, R.Alberto
Preparation of a 35S-Source for β-Spectroscopy
RADIOACTIVITY 35S(β-); measured Eβ, Iβ(t), T1/2. Source preparation for β spectroscopy.
doi: 10.1016/S0168-9002(98)01357-6
Phys.Lett. 459B, 67 (1999)
W.Trinder, J.C.Angelique, R.Anne, J.Aysto, C.Borcea, J.M.Daugas, D.Guillemaud-Mueller, S.Grevy, R.Grzywacz, A.Jokinen, M.Lewitowicz, M.J.Lopez, F.de Oliveira, A.N.Ostrowski, T.Siiskonen, M.G.Saint-Laurent
β-Decay of 35Ca
RADIOACTIVITY 35Ca(β+) [from Ni(40Ca, X)]; measured β-delayed proton spectra, pβ-coin, T1/2, B(GT). 35K deduced proton decay modes, no two-proton IAS decay. Shell model calculations.
doi: 10.1016/S0370-2693(99)00655-3
RIKEN-98, p.78 (1999)
K.Yoneda, H.Sakurai, N.Aoi, N.Fukuda, T.Gomi, E.Ideguchi, N.Imai, H.Iwasaki, T.Kubo, Z.Liu, S.M.Lukyanov, T.Nakamura, M.Notani, H.Ogawa, Y.E.Penionzhkevich, W.-D.Schmidt-Ott, S.Shimoura, E.Sokol, Y.X.Watanabe, A.Yoshida, X.Zhou, M.Ishihara
The First Measurements of Half Lives and Neutron Emission Probabilities of Very Neutron Rich Nuclides of Mg, Al, Si, and P
RADIOACTIVITY 31,32,33Na, 32,33,34,35,36,37Mg, 34,35,36,37,38,39Al, 37,38,39,40,41,42Si, 41,42,43P(β-n) [from 9Be, 181Ta(48Ca, X), E=70 MeV/nucleon]; measured T1/2, β-delayed n emission probabilities. Projectile fragmentation separator.
Phys.Rev. B61, 13588 (2000)
H.Haas, H.M.Petrilli
Quadrupole Moments of the Halogen Nuclei
NUCLEAR MOMENTS 35Cl, 79Br, 127I; analyzed molecular data; calculated electric field gradients; deduced nuclear quadrupole moments.
doi: 10.1103/PhysRevB.61.13588
Phys.Lett. 482B, 1 (2000)
E.Holzschuh, L.Palermo, H.Stussi, P.Wenk
The β-Spectrum of 35S and Search for the Admixture of Heavy Neutrinos
RADIOACTIVITY 35S(β-); measured β spectrum; deduced E0, neutrino mixing probability upper limit. Comparison with model predictions.
doi: 10.1016/S0370-2693(00)00476-7
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.
Phys.Rev.Lett. 84, 5062 (2000)
F.Sarazin, H.Savajols, W.Mittig, F.Nowacki, N.A.Orr, Z.Ren, P.Roussel-Chomaz, G.Auger, D.Baiborodin, A.V.Belozyorov, C.Borcea, E.Caurier, Z.Dlouhy, A.Gillibert, A.S.Lalleman, M.Lewitowicz, S.M.Lukyanov, F.De Oliveira, Y.E.Penionzhkevich, D.Ridikas, H.Sakurai, O.Tarasov, A.de Vismes
Shape Coexistence and the N = 28 Shell Closure Far from Stability
ATOMIC MASSES 29,30Ne, 32,33Na, 34,35,36Mg, 36,37,38,39Al, 38,39,40,41Si, 38,39,40,41,42,43P, 40,41,42,43,44,45S, 43,44,45,46Cl, 47Ar; measured masses, two-neutron separation energies; deduced shell and deformation effects. Time-of-flight technique. Comparison with model predictions.
RADIOACTIVITY 43S(IT) [from 48Ca fragmentation]; measured Eγ, Iγ, T1/2. Comparison with shell model.
doi: 10.1103/PhysRevLett.84.5062
Bull.Rus.Acad.Sci.Phys. 64, 327 (2000)
A.N.Vodin, A.S.Kachan
γ-Transitions between Compound States in 1d2s-Shell Nuclei
NUCLEAR STRUCTURE 21Na, 24Mg, 25,27Al, 29,31P, 33,35Cl, 39K; analyzed γ transitions at excitation energies higher than the proton binding energy; deduced γ width, B(M1), B(E1), B(E2).
Bull.Rus.Acad.Sci.Phys. 65, 725 (2001)
A.S.Kachan, A.N.Vodin, V.M.Mishchenko, R.P.Slabospitsky
M1 Resonance in Odd sd-Shell Nuclei
NUCLEAR REACTIONS 22Ne, 26Mg, 30Si, 34,36S(p, γ), E=0.8-3 MeV; measured Eγ, Iγ. 23Na, 27Al, 31P, 35,37Cl deduced transitions B(M1), resonance energy.
Eur.Phys.J. A 10, 119 (2001)
M.J.Lopez-Jimenez, M.G.Saint-Laurent, J.C.Angelique, R.Anne, J.Aysto, C.Borcea, J.M.Daugas, D.Guillemaud-Mueller, S.Grevy, R.Grzywacz, A.Jokinen, M.Lewitowicz, F.Nowacki, F.de Oliveira Santos, A.N.Ostrowski, T.Siiskonen, W.Trinder
New Transitions in the β-Decay of 36Ca
RADIOACTIVITY 36Ca(β+p); measured Eγ, Eβ, β-delayed proton spectra; deduced log ft, B(GT). 36K deduced IAS proton decay features. 35,36Ar deduced transitions. Comparison with shell model predictions.
Phys.Rev. C63, 044316 (2001)
S.Nummela, P.Baumann, E.Caurier, P.Dessagne, A.Jokinen, A.Knipper, G.Le Scornet, C.Miehe, F.Nowacki, M.Oinonen, Z.Radivojevic, M.Ramdhane, G.Walter, J.Aysto, and the ISOLDE Collaboration
Spectroscopy of 34, 35Si by β Decay: sd-fp Shell gap and single-particle states
RADIOACTIVITY 34,35Al(β-) [from U(p, X)]; measured Eγ, Iγ, T1/2, γγ-, βγ-coin, β-delayed neutrons; deduced log ft. 34,35Si deduced levels, J, π. Comparison with shell model calculations.
doi: 10.1103/PhysRevC.63.044316
Phys.Rev. C64, 024610 (2001)
S.Pirrone, G.Politi, G.Lanzalone, S.Aiello, N.Arena, Seb.Cavallaro, E.Geraci, F.Porto, S.Sambataro
Fusion and Competing Processes in the 32S + 12C Reaction at E(32S) = 19.5 MeV/nucleon
NUCLEAR REACTIONS 12C(32S, X)22Na/23Na/24Na/24Mg/25Mg/26Mg/26Al/27Al/28Al/28Si/29Si/30Si/30P/31P/32P/34Cl/35Cl/36Cl/Ar, E=19.5 MeV/nucleon; measured fusion residues isotopic yields, velocity and angular distributions, fusion and incomplete fusion σ. Comparison with model predictions.
doi: 10.1103/PhysRevC.64.024610
Hyperfine Interactions 132, 147 (2001)
F.Sarazin, H.Savajols, W.Mittig, F.Nowacki, N.A.Orr, Z.Ren, P.Roussel-Chomaz, G.Auger, D.Baiborodin, A.V.Belozyorov, C.Borcea, E.Caurier, Z.Dlouhy, A.Gillibert, A.S.Lalleman, M.Lewitowicz, S.M.Lukyanov, F.de Oliveira, Y.E.Penionzhkevich, D.Ridikas, O.Tarasov, H.Sakurai, A.De Vismes
Shape Coexistence and the N = 28 Shell Closure Far from Stability
ATOMIC MASSES 29,30Ne, 32,33Na, 34,35,36Mg, 36,37,38,39Al, 38,39,40,41Si, 38,39,40,41,42,43P, 40,41,42,43,44,45S, 43,44,45,46Cl; measured masses, two-neutron separation energies; deduced shell effects. Time of flight method.
RADIOACTIVITY 43S(IT); measured Eγ, T1/2. Comparison with shell model prediction.
Bull.Rus.Acad.Sci.Phys. 65, 746 (2001)
A.N.Vodin, A.S.Kachan, V.M.Mishchenko
Isobar-Analogue Resonances in the 35Cl Nucleus
NUCLEAR REACTIONS 34S(p, γ), E=1183-2820 keV; measured Eγ, excitation function. 35Cl deduced levels, J, π, B(M1), resonanace widths, analog states features.
JINR-E7-2002-237 (2002)
S.M.Lukyanov, Yu.E.Penionzhkevich
Peculiarities of O-Mg Isotopes at the Neutron Drip Line
NUCLEAR REACTIONS Ta(48Ca, X)19B/20C/22C/21N/23N/24O/27F/29F/31F/30Ne/32Ne/34Ne/33Na/35Na/37Na/38Mg, E=59.8 MeV; measured yields. Mass and level energy systematics in neighboring nuclides discussed.
Nucl.Phys. A701, 383c (2002)
K.Matsuta, T.Tsubota, C.Ha, T.Miyake, M.Sasaki, K.Sato, K.Minamisono, K.Tanaka, S.Kaminaka, A.Takemura, T.Sumikama, T.Nagatomo, K.Hashimoto, M.Mihara, M.Fukuda, T.Minamisono, T.Ohtsubo, Y.Nojiri, S.Momota, A.Kitagawa, M.Torikoshi, M.Kanazawa, S.Koda, T.Nishio, M.Suda, J.R.Alonso, G.F.Krebs, T.J.M.Symons
Precise Magnetic Moment of Short-Lived Beta Emitter 35Ar
RADIOACTIVITY 35Ar(β-); measured β-NMR spectra from oriented nuclei; deduced μ.
doi: 10.1016/S0375-9474(01)01615-3
Nucl.Phys. A701, 410c (2002)
S.Nummela, P.Baumann, E.Caurier, S.Courtin, P.Dessagne, O.Holmlund, A.Jokinen, A.Knipper, G.Le Scornet, C.Mieh, F.Nowacki, L.G.Lyapin, M.Oinonen, E.Poirier, Z.Radivojevic, M.Ramdhane, W.H.Trzaska, G.Walter, J.Aysto, and the ISOLDE Collaboration
Study of the Neutron-Rich Nuclei with N = 21, 35Si and 33Mg, by Beta Decay of 35Al and 33Na
RADIOACTIVITY 35Al, 33Na(β-), (β-n); measured Eγ, Iγ, β-delayed neutron spectra, T1/2. 35Si, 33Mg deduced levels, J, π.
doi: 10.1016/S0375-9474(01)01619-0
Phys.Rev. C65, 037301 (2002); Comment Phys.Rev. C 69, 049803 (2004)
C.Samanta, S.Adhikari
Extension of the Bethe-Weizsacker Mass Formula to Light Nuclei and Some New Shell Closures
NUCLEAR STRUCTURE C, Li, Bi; calculated binding energy per nucleon. Z=4-17; calculated one-neutron separation energies. 26O, 32Ne, 35Na, 38Mg, 41Al; calculated one- and two-neutron separation energies. New shell closures discussed.
doi: 10.1103/PhysRevC.65.037301
Bull.Rus.Acad.Sci.Phys. 66, 40 (2002)
A.N.Vodin, A.S.Kachan, V.M.Mishchenko
Isobar-Analogue f7/2 Resonances in Odd 1d2s-Shell Nuclei
NUCLEAR REACTIONS 26Mg(p, γ), E ≈ 2294, 2324 keV; 30Si(p, γ), E ≈ 2187 keV; 34S(p, γ), E ≈ 1212 keV; 36S(p, γ), E ≈ 1887 keV; measured Eγ, Iγ(θ); deduced resonance strengths, widths. 27Al, 31P, 35,37Cl deduced transitions δ, B(M1) for IAR decay, isospin quasiparticle interaction constant.
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
Nucl.Phys. A714, 441 (2003)
N.A.Smirnova, C.Volpe
On the asymmetry of Gamow-Teller β-decay rates in mirror nuclei in relation with second-class currents
RADIOACTIVITY 8,9Li, 12,13B, 17N, 20O, 20,21F, 25Na, 28,31Al, 35S, 35P(β-); 8B, 9C, 12,13N, 13O, 17Ne, 20Na, 20,21Mg, 25Si, 28P, 31Ar, 35K, 35Ca(β+); calculated Gamow-Teller decay rates. Comparison with data.
NUCLEAR MOMENTS 8,9Li, 9Be, 8,12,13B, 9,13C, 12,13N, 13O; calculated μ, quadrupole moments.
doi: 10.1016/S0375-9474(02)01392-1
Phys.Rev. B 69, 125101 (2004); Phys.Rev. B 70, 119901 (2004)
R.E.Alonso, A.Svane, C.O.Rodriguez, N.E.Christensen
Nuclear quadrupole moment determination of 35Cl, 79Br, and 127I
NUCLEAR MOMENTS 35Cl, 79Br, 127I; analyzed nuclear quadrupole resonance data; deduced quadrupole moments.
doi: 10.1103/PhysRevB.69.125101
At.Data Nucl.Data Tables 87, 185 (2004)
I.Angeli
A consistent set of nuclear rms charge radii: properties of the radius surface R(N, Z)
COMPILATION A=1-248; compiled, analyzed charge radii.
doi: 10.1016/j.adt.2004.04.002
Phys.Rev.Lett. 92, 132502 (2004)
J.Ekman, D.Rudolph, C.Fahlander, A.P.Zuker, M.A.Bentley, S.M.Lenzi, C.Andreoiu, M.Axiotis, G.de Angelis, E.Farnea, A.Gadea, Th.Kroll, N.Marginean, T.Martinez, M.N.Mineva, C.Rossi-Alvarez, C.A.Ur
Unusual Isospin-Breaking and Isospin-Mixing Effects in the A = 35 Mirror Nuclei
NUCLEAR REACTIONS 16O(24Mg, nα), (24Mg, pα), E=60 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-, (neutron)γ-coin. 35Ar deduced levels, J, π, isospin mixing. GASP, ISIS arrays.
doi: 10.1103/PhysRevLett.92.132502
Nucl.Phys. A730, 80 (2004)
L.S.Geng, H.Toki, A.Ozawa, J.Meng
Proton and neutron skins of light nuclei within the relativistic mean field theory
NUCLEAR STRUCTURE 16,17,18,19,20,21,22,23,24,25,26,27,28,29,30,31,32,33,34Ne, 18,19,20,21,22,23,24,25,26,27,28,29,30,31,32,33,34,35,36,37Na, 28,29,30,31,32,33,34,35,36,37,38,39,40,41Cl, 29,30,31,32,33,34,35,36,37,38,39,40,41Ar; calculated binding energies, radii, deformation parameters, neutron and proton separation energies. Deformed relativistic mean field.
doi: 10.1016/j.nuclphysa.2003.10.014
Eur.Phys.J. A 22, 17 (2004)
S.Khaled, M.Ramdhane, F.Benrachi
Application of the weak-coupling model for calculating the binding energies of neutron-rich A ∼ 32 nuclei
NUCLEAR STRUCTURE 28,29,30,31,32Ne, 29,30,31,32,33,34Na, 30,31,32,33,34,35Mg, 31,32,33,34,35,36Al, 32,33,34,35,36,37Si, 33,34,35,36,37,38P, 34,35,36,37,38,39S, 35,36,37,38,39,40Cl, 36,37,38,39,40,41Ar; calculated binding energies. Weak-coupling model, comparison with data.
doi: 10.1140/epja/i2004-10021-1
Nucl.Phys. A734, E69 (2004)
Yu.S.Lutostansky
Properties of nuclei near the neutron-drip line in O - Si region
NUCLEAR STRUCTURE Z=8-14; calculated neutron drip-line features. 37Na; calculated single-particle level energies. 29,30,31,32,34,36Ne, 31,32,33,34,35,37,39Na; calculated T1/2, deformation dependence. Comparisons with data.
doi: 10.1016/j.nuclphysa.2004.03.022
Proc.Nuclei at the Limits, Argonne, Illinois, D.Seweryniak and T.L.Khoo, eds., p.205 (2005); AIP Conf. Proc 764 (2005)
F.Della Vedova, S.M.Lenzi, M.Ionescu-Bujor, N.Marginean, E.Farnea, M.Nespolo, G.de Angelis, M.Axiotis, D.Bazzacco, A.Bizzeti-Sona, P.G.Bizzeti, F.Brandolini, D.Bucurescu, A.Iordachescu, S.Lunardi, R.Menegazzo, D.R.Napoli, C.Rossi Alvarez, C.A.Ur
Isospin Symmetry Along The N=Z Line In The sd Shell
NUCLEAR REACTIONS 24Mg(16O, n2α), (16O, p2α), (16O, nα), (16O, pα), E=70 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-, (neutron)γ-coin. 31S, 31P, 35Ar, 35Cl deduced levels, J, π, mirror energy differences. GASP, ISIS arrays.
doi: 10.1063/1.1905312
Eur.Phys.J. A 25, Supplement 1, 363 (2005)
J.Ekman, L.-L.Andersson, C.Fahlander, E.K.Johansson, R.du Rietz, D.Rudolph
News on mirror nuclei in the sd and fp shells
NUCLEAR REACTIONS 16O(24Mg, nα), (24Mg, pα), E=60 MeV; 28Si(32S, n2α), (32S, p2α), E=130 MeV; 24Mg(40Ca, 2np), (40Ca, n2p), E=104 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-, (neutron)γ-coin. 35Ar, 35Cl, 51Fe, 51Mn, 61Ga, 61Zn deduced levels, J, π, mirror energy difference. Discussed electromagnetic spin-orbit effect. Large-scale shell model calculations.
doi: 10.1140/epjad/i2005-06-016-2
J.Phys.(London) G31, S1965 (2005)
C.Timis, J.C.Angelique, A.Buta, N.L.Achouri, D.Baiborodin, P.Baumann, C.Borcea, S.Courtin, P.Dessagne, Z.Dlouhy, J.M.Daugas, S.Grevy, D.Guillemaud-Mueller, A.Knipper, F.R.Lecolley, J.L.Lecouey, M.Lewitowicz, E.Lienard, S.M.Lukyanov, F.M.Marques, C.Miehe, J.Mrazek, F.Negoita, F.Nowacki, F.de Oliveira, N.A.Orr, J.Peter, S.Pietri, Yu.E.Penionzhkevich, E.Poirier, M.Stanoiu, G.Walter
Spectroscopy around N = 20 shell closure: β-n decay study of 35Al
RADIOACTIVITY 35Al(β-), (β-n) [from 36S fragmentation]; measured β-delayed Eγ, En, T1/2, neutron emission probability; deduced log ft. 34,35Si deduced levels, J, π, feeding intensities.
doi: 10.1088/0954-3899/31/10/111
Proc.Frontiers in Nuclear Structure, Astrophysics, and Reactions, Isle of Kos, Greece, 12-17 Sept. 2005, S.V Harissopulos, P.Demetriou, R.Julin, Eds., p. 134 (2006); AIP Conf.Proc. 831 (2006)
J.C.Angelique, C.Timis, S.Pietri, N.L.Achouri, P.Baumann, C.Borcea, A.Buta, W.Catford, S.Courtin, J.M.Daugas, P.Dessagne, F.De Oliveira, Z.Dlouhy, S.Grevy, D.Guillemaud-Mueller, R.Hadeler, A.Knipper, F.R.Lecolley, J.L.Lecouey, M.Lewitowicz, E.Lienard, C.Miehe, J.Mrazek, F.Negoita, F.Nowacki, N.A.Orr, Y.Penionzhkevich, J.Peter, E.Poirier, M.Stanoiu, O.Tarasov, G.Walter
Spectroscopy Near the N=20 Shell Closure: β-n Decay Studies of 33Mg and 35Al
RADIOACTIVITY 33Mg, 35Al(β-), (β-n) [from 36S fragmentation]; measured Eγ, En, βγ-, βn-coin; deduced log ft. 34,35Si, 32,33Al deduced levels, J, π.
doi: 10.1063/1.2200913
Phys.Rev. C 74, 055502 (2006)
V.E.Iacob, J.C.Hardy, J.F.Brinkley, C.A.Gagliardi, V.E.Mayes, N.Nica, M.Sanchez-Vega, G.Tabacaru, L.Trache, R.E.Tribble
Precise half-life measurements for the superallowed β+ emitters 34Ar and 34Cl
RADIOACTIVITY 34,35Ar, 34Cl(β+) [from 1H(35Cl, xnyp)]; measured T1/2.
doi: 10.1103/PhysRevC.74.055502
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, 024318 (2006)
T.J.Mertzimekis, P.F.Mantica, A.D.Davies, S.N.Liddick, B.E.Tomlin
Ground state magnetic dipole moment of 35K
RADIOACTIVITY 35K(EC), (β+) [from 9Be(36Ar, X)]; measured β-NMR spectra from polarized source. 35K deduced μ. Systematics of magnetic moments in neighboring nuclides discussed.
doi: 10.1103/PhysRevC.73.024318
Phys.Rev. C 73, 045501 (2006)
D.F.Measday, T.J.Stocki
γ rays from muon capture in natural Ca, Fe, and Ni
NUCLEAR REACTIONS Ca(μ-, νxnypzα)43K/41K/40K/39K/38K/37K/39Ar/38Ar/38Cl/37Cl/36Cl/35Cl/34Cl, E at rest; Fe(μ-, νxnypzα)56Mn/55Mn/54Mn/53Mn/54Cr, E at rest; Ni(μ-, νxnypzα)58Fe/56Fe/59Co/57Co, E at rest; measured Eγ, Iγ, yields.
doi: 10.1103/PhysRevC.73.045501
Atlas of Neutron Resonances, 5ed., Resonance Parameters and Thermal Cross Sections, Z = 1-100, Elsevier, Amsterdam (2006)
S.F.Mughabghab
COMPILATION Z=1-100; compiled, evaluated thermal neutron induced σ, resonance parameter data.
Phys.Rev. C 74, 034602 (2006)
B.T.Roeder, K.W.Kemper, N.Aoi, D.Bazin, M.Bowen, C.M.Campbell, J.M.Cook, D.-C.Dinca, A.Gade, T.Glasmacher, H.Iwasaki, S.Kanno, T.Motobayashi, W.F.Mueller, T.Nakamura, H.Sakurai, H.Suzuki, S.Takeuchi, J.R.Terry, K.Yoneda, H.Zwahlen
Production cross sections for heavy-ion fragmentation reactions on a liquid deuterium target at intermediate energies
NUCLEAR REACTIONS 2H(48Ca, X)48Sc/47Ca/46Ca/48K/47K/46K/45K/44K/45Ar/44Ar/42Ar/42Cl/40Cl/39Cl, E=102 MeV/nucleon; 2H(40S, X)40Cl/39S/38S/37P/36P/34Si/33Si/32Al/31Al, E=99.3 MeV/nucleon; 2H(42S, X)42Cl/42S/40S/39P/38P/37P/36Si/35Si/33Al/32Al, E=99.8 MeV/nucleon; measured production σ. Comparison with model predictions, fragmentation from Be and Ta targets.
doi: 10.1103/PhysRevC.74.034602
Phys.Lett. B 638, 166 (2006)
Q.Zhi, Z.Ren
Systematic calculations on the ground state properties of Mg isotopes by the macroscopic-microscopic model
NUCLEAR STRUCTURE 20,21,22,23,24,25,26,27,28,29,30,31,32,33,34,35,36,37,38,39,40Mg; calculated binding energies, deformation parameters, B(E2), single- and two-neutron separation energies, quadrupole moments. Macroscopic-microscopic model, isospin-dependent Nilsson potential, comparison with data.
doi: 10.1016/j.physletb.2006.05.057
Phys.Rev. C 76, 067601 (2007)
G.Chaudhuri, S.Das Gupta, W.G.Lynch, M.Mocko, M.B.Tsang
Cross sections of neutron-rich nuclei from projectile fragmentation: Canonical thermodynamic model estimates
NUCLEAR REACTIONS 9Be(48Ca, X)25Si/26Si/27Si/28Si/29Si/30Si/32Si/33Si/34Si/35Si/36Si/37Si/38Si/39Si/40Si/41Si, E=140 MeV; 9Be(86Kr, X)59Cu/60Cu/61Cu/62Cu/63Cu/64Cu/65Cu/66Cu/67Cu/68Cu/69Cu/70Cu/71Cu/72Cu/73Cu/74Cu/75Cu/76Cu/77Cu/78Cu/79Cu/80Cu, E=64 MeV; calculated cross sections, binding energies. Comparison with experimental data.
doi: 10.1103/PhysRevC.76.067601
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 75, 034317 (2007)
F.Della Vedova, S.M.Lenzi, M.Ionescu-Bujor, N.Marginean, M.Axiotis, D.Bazzacco, A.M.Bizzeti-Sona, P.G.Bizzeti, A.Bracco, F.Brandolini, D.Bucurescu, E.Farnea, A.Iordachescu, S.Lunardi, T.Martinez, P.Mason, R.Menegazzo, B.Million, D.R.Napoli, M.Nespolo, P.Pavan, C.Rossi Alvarez, C.A.Ur, R.Venturelli, A.P.Zuker
Isospin symmetry breaking at high spin in the mirror nuclei 35Ar and 35Cl
NUCLEAR REACTIONS 24Mg(16O, nα), (16O, pα), E=70 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-coin. 35Ar, 35Cl deduced high-spin levels, J, π, configurations, analog states, spin-orbit interaction effects, isospin symmetry features. GASP, ISIS arrays.
doi: 10.1103/PhysRevC.75.034317
Phys.Rev. C 76, 054319 (2007)
I.Hamamoto
Nilsson diagrams for light neutron-rich nuclei with weakly-bound neutrons
NUCLEAR STRUCTURE 15,17,19C, 31,33,35,37Mg; calculated one-particle bound and resonant level energies. Deduced Nilsson diagrams using Woods-Saxon potential.
doi: 10.1103/PhysRevC.76.054319
Phys.Rev. C 75, 034313 (2007)
A.Hodsdon, R.Chapman, X.Liang, F.Haas, J.Ollier, E.Caurier, F.Nowacki, M.-D.Salsac, F.Azaiez, S.Beghini, B.Behera, M.Burns, L.Corradi, D.Curien, A.N.Deacon, Zs.Dombradi, E.Farnea, E.Fioretto, A.Gadea, A.Jungclaus, K.L.Keyes, A.Latina, N.Marginean, G.Montagnoli, D.Napoli, D.O'Donnell, A.Papenberg, F.Scarlassara, J.F.Smith, K.-M.Spohr, M.Stanoiu, A.Stefanini, S.Szilner, M.Trotta, C.Ur, D.Verney, Z.Wang
Spectroscopy of neutron-rich 37P
NUCLEAR REACTIONS 208Pb(36S, X)32P/33P/34P/35P/36P/37P, E=215 MeV; measured particle yields, Eγ, Iγ, (particle)γ-coin. 37P deduced levels, J, π, configurations. Clara array.
doi: 10.1103/PhysRevC.75.034313
Phys.Lett. B 649, 43 (2007)
B.Jurado, H.Savjols, W.Mittig, N.A.Orr, P.Roussel-Chomaz, D.Baiborodin, W.N.Catford, M.Chartier, C.E.Demonchy, Z.Dlouhy, A.Gillibert, L.Giot, A.Khouaja, A.Lepine-Szily, S.Lukyanov, J.Mrazek, Y.E.Penionzhkevich, S.Pita, M.Rousseau, A.C.Villari
Mass measurements of neutron-rich nuclei near the N = 20 and 28 shell closures
ATOMIC MASSES 23N, 23,24O, 25,26,27F, 27,28,29,30,31Ne, 31,32,33Na, 34,35,36Mg, 34,35,36,37,38,39Al, 36,37,38,39,40,41,42Si, 40,41,42,43,44P, 40,43,44,45S, 43,45,46,47Cl; measured masses; analysed neutron separation energy. Cyclotron-based mass spectrometry.
doi: 10.1016/j.physletb.2007.04.006
Nucl.Phys. A781, 277 (2007)
R.Kshetri, M.S.Sarkar, I.Ray, P.Banerjee, S.Sarkar, R.Raut, A.Goswami, J.M.Chatterjee, S.Chattopadhyay, U.Datta Pramanik, A.Mukherjee, C.C.Dey, S.Bhattacharya, B.Dasmahapatra, S.Bhowal, G.Gangopadhyay, P.Datta, H.C.Jain, R.K.Bhowmik, S.Muralithar R.P.Singh, R.Kumar
High spin structure of 35Cl and the sd-fp shell gap
NUCLEAR REACTIONS 12C(28Si, pα), E=70, 88 MeV; measured Eγ, Iγ, γγ-coin, DSA. 35Cl deduced levels J, π, δ, T1/2. INGA array, shell model calculations.
doi: 10.1016/j.nuclphysa.2006.10.084
Eur.Phys.J. Special Topics 150, 149 (2007)
G.Neyens, P.Himpe, D.L.Balabanski, P.Morel, L.Perrot, M.De Rydt, I.Stefan, C.Stodel, J.C.Thomas, N.Vermeulen, D.T.Yordanov
The "island of inversion" from a nuclear moments perspective and the g factor of 35Si
RADIOACTIVITY 35Si(β-); measured ground state g-factor using the β-NMR method.
doi: 10.1140/epjst/e2007-00291-7
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
Phys.Rev. C 76, 041302 (2007)
M.B.Tsang, W.G.Lynch, W.A.Friedman, M.Mocko, Z.Y.Sun, N.Aoi, J.M.Cook, F.Delaunay, M.A.Famiano, H.Hui, N.Imai, H.Iwasaki, T.Motobayashi, M.Niikura, T.Onishi, A.M.Rogers, H.Sakurai, H.Suzuki, E.Takeshita, S.Takeuchi, M.S.Wallace
Fragmentation cross sections and binding energies of neutron-rich nuclei
NUCLEAR REACTIONS 9Be(86Kr, X)69Cu/71Cu/73Cu/75Cu/76Cu/77Cu/78Cu/79Cu, E=64 MeV/A; analyzed cross sections, binding energies. 9Be, 181Ta(48Ca, X)23Na/24Na/25Na/26Na/27Na/28Na/29Na/30Na/31Na/26Mg/27Mg/28Mg/29Mg/30Mg/31Mg/32Mg/33Mg/34Mg/35Mg, E=140 MeV/nucleon; analyzed cross sections.
doi: 10.1103/PhysRevC.76.041302
Phys.Rev. C 76, 024308 (2007)
C.Yazidjian, G.Audi, D.Beck, K.Blaum, S.George, C.Guenaut, F.Herfurth, A.Herlert, A.Kellerbauer, H.-J.Kluge, D.Lunney, L.Schweikhard
Evidence for a breakdown of the isobaric multiplet mass equation: A study of the A = 35, T = 3/2 isospin quartet
ATOMIC MASSES 35,36,37,38,43,44,45,46K; measured masses using ISOLTRAP. Discussed implications on IMME.
doi: 10.1103/PhysRevC.76.024308
Bull.Rus.Acad.Sci.Phys. 72, 1556 (2008); Izv.Akad.Nauk RAS, Ser.Fiz. 72, 1642 (2008)
A.N.Aleinikov, V.A.Rabotkin, A.P.Shumeyko
Study of the 35S internal bremsstrahlung spectra by the threshold detector method
RADIOACTIVITY 35S(β-); measured internal bremsstrahlung spectrum.
doi: 10.3103/S1062873808110257
Phys.Lett. B 662, 389 (2008)
K.Minamisono, P.F.Mantica, H.L.Crawford, J.S.Pinter, J.B.Stoker, Y.Utsuno, R.R.Weerasiri
Quadrupole moment of 37K
RADIOACTIVITY 37K(β+); measured electric quadrupole moment using the β-NQR technique. 35S, 37Ar, 35,37,39K, 39Ca; analyzed electric quadrupole moment using shell model and effective charge dependency.
doi: 10.1016/j.physletb.2008.03.049
Phys.Rev. C 78, 037302 (2008)
M.Wiedeking, E.Rodriguez-Vieitez, P.Fallon, M.P.Carpenter, R.M.Clark, D.Cline, M.Cromaz, M.Descovich, R.V.F.Janssens, I.-Y.Lee, M.-A.Deleplanque, A.O.Macchiavelli, F.S.Stephens, R.Teng, X.Wang, D.Ward, C.Y.Wu, S.Zhu, T.Otsuka, Y.Utsuno, A.Volya
Intruder excitations in 35P
NUCLEAR REACTIONS 208Pb(36S, X), E=230 MeV; measured Eγ, Iγ, γγ-, (particle)γ-coin. 34Si, 35P; deduced levels, J, π, B(E2). Comparison with shell model calculations.
doi: 10.1103/PhysRevC.78.037302
Phys.Rev. C 78, 054311 (2008)
M.T.Win, K.Hagino
Deformation of Λ hypernuclei
NUCLEAR STRUCTURE 12C, 18,20,22,24,26,28,30,32,34,36,38Ne, 22,24,26,28,30,32,34,36,38,40,42Si; calculated quadrupole deformation parameter, potential surfaces. 13C, 19,21,23,25,27,29,31,33,35,37,39Ne, 23,25,27,29,31,33,35,37,39,41,43Si; calculated quadrupole deformation parameter, potential surfaces for hypernuclei. Relativistic Mean Field model.
doi: 10.1103/PhysRevC.78.054311
Bull.Rus.Acad.Sci.Phys. 73, 176 (2009); Izv.Akad.Nauk RAS, Ser.Fiz. 73, 187 (2009)
Yu.S.Lyutostansky
Disturbance of the shell structure of neutron-rich nuclei in the oxygen-magnesium region
NUCLEAR STRUCTURE 28O, 37,39,43Na; calculated neutron single particle levels as a function of deformation; 31,33,35Na; calculated binding energies as a function of quadrupole moment, deformation.
doi: 10.3103/S1062873809020099
Phys.Rev. C 79, 014310 (2009)
F.Nowacki, A.Poves
New effective interaction for 0(h-bar)ω shell-model calculations in the sd-pf valence space
NUCLEAR STRUCTURE 35Si, 35P, 37S, 39,47Ar, 41,49Ca, 47,49K; calculated levels, J, π, single-particle energies. 36,38,40,42,44Si, 34,36,38,40Mg; calculated B(E2), quadrupole moments, energy of 2+ state. 39,41,43,45,47,49,51K, 35,37,39,41,43,45,47P, 37,39,41,43,45,47,49Cl; calculated energy splitting between 1/2+ and 3/2+ states. Shell-model calculations in sd-pf valence space. Comparison with experimental data.
doi: 10.1103/PhysRevC.79.014310
Phys.Rev. C 79, 054303 (2009)
K.Yoshida
Core polarization for the electric quadrupole moment of neutron-rich aluminum isotopes
NUCLEAR STRUCTURE 32,34,36Si, 32Mg; calculated B(E2), response functions for isoscalar, isovector, and proton quadrupole excitations. Microscopic particle-vibration coupling model with Skyrme HFB and QRPA equations. Implications for quadrupole moments of 31,33,35Al.
NUCLEAR MOMENTS 31,33,35Al; calculated polarization charges and electric quadrupole moments. Comparison with experimental data.
doi: 10.1103/PhysRevC.79.054303
Phys.Rev.Lett. 104, 112701 (2010)
J.Lee, M.B.Tsang, D.Bazin, D.Coupland, V.Henzl, D.Henzlova, M.Kilburn, W.G.Lynch, A.M.Rogers, A.Sanetullaev, A.Signoracci, Z.Y.Sun, M.Youngs, K.Y.Chae, R.J.Charity, H.K.Cheung, M.Famiano, S.Hudan, P.O'Malley, W.A.Peters, K.Schmitt, D.Shapira, L.G.Sobotka
Neutron-Proton Asymmetry Dependence of Spectroscopic Factors in Ar Isotopes
NUCLEAR REACTIONS 1H(34Ar, d), (36Ar, d), (46Ar, d), E=33 MeV/nucleon; measured Eδ, Iδ; 34,36,46Ar; deduced neutron ground state spectroscopic factors. Comparison with shell model calculations.
doi: 10.1103/PhysRevLett.104.112701
Priv.Comm. (2010)
M.Wiedeking
Priv.Comm. (2011)
G.Audi
NUBASE-2011
Priv.Comm. (2011)
G.Audi, W.Meng
Atomic Mass Evaluation 2011
Phys.Rev. C 83, 044305 (2011)
A.Gade, D.Bazin, B.A.Brown, C.M.Campbell, J.M.Cook, S.Ettenauer, T.Glasmacher, K.W.Kemper, S.McDaniel, A.Obertelli, T.Otsuka, A.Ratkiewicz, J.R.Terry, Y.Utsuno, D.Weisshaar
In-beam γ -ray spectroscopy of 35Mg and 33Na
NUCLEAR REACTIONS 9Be(38Si, X)33Na/35Mg/36Mg/38Si, E=83 MeV/nucleon, [secondary 38Si beam from 9Be(48Ca, X), E=140 MeV/nucleon primary reaction]; measured Eγ, production σ, (33Na)γ-, (35Mg)γ-coin using SeGA array. 33Na, 35Mg; deduced levels, J, π, rotational band in 33Na. Comparison with large-scale Monte-Carlo shell model (MCSM) calculations with SDPF-M interaction, and with large-scale shell-model calculations with SDPF-U interaction. Calculated composition of 35Mg wave functions, quadrupole moments and B(E2) values. Systematics of S(n) for A=30-35 Mg nuclei. Relevance to Island of Inversion.
doi: 10.1103/PhysRevC.83.044305
Phys.Rev. C 83, 021302 (2011)
R.Kanungo, A.Prochazka, W.Horiuchi, C.Nociforo, T.Aumann, D.Boutin, D.Cortina-Gil, B.Davids, M.Diakaki, F.Farinon, H.Geissel, R.Gernhauser, J.Gerl, R.Janik, B.Jonson, B.Kindler, R.Knobel, R.Krucken, M.Lantz, H.Lenske, Y.Litvinov, B.Lommel, K.Mahata, P.Maierbeck, A.Musumarra, T.Nilsson, C.Perro, C.Scheidenberger, B.Sitar, P.Strmen, B.Sun, Y.Suzuki, I.Szarka, I.Tanihata, Y.Utsuno, H.Weick, M.Winkler
Matter radii of 32-35Mg
NUCLEAR REACTIONS C, H(32Mg, X), (33Mg, X)(34Mg, X)(35Mg, X), E=900 MeV/nucleon, [secondary Mg beams from Be(48Ca, X) primary reaction]; measured interaction cross sections by detecting unreacted Mg particles by Bρ-ΔE-TOF method. 32,33,34,35Mg; deduced matter radii by Glauber model analysis. Comparison with HF and RMF predictions. Neutron skin thickness.
doi: 10.1103/PhysRevC.83.021302
Phys.Rev. C 83, 014606 (2011)
J.Lee, M.B.Tsang, D.Bazin, D.Coupland, V.Henzl, D.Henzlova, M.Kilburn, W.G.Lynch, A.M.Rogers, A.Sanetullaev, Z.Y.Sun, M.Youngs, R.J.Charity, L.G.Sobotka, M.Famiano, S.Hudan, D.Shapira, P.O'Malley, W.A.Peters, K.Y.Chae, K.Schmitt
Neutron spectroscopic factors of 34Ar and 46Ar from (p, d) transfer reactions
NUCLEAR REACTIONS 1H(34Ar, d), (36Ar, d), (46Ar, d), E=33 MeV/nucleon, [34,46Ar secondary beams from 9Be(36Ar, X), E=150 MeV/nucleon and 9Be(48Ca, X), E=140 MeV/nucleon primary reactions]; measured Ed, Id, σ(θ); 34,36,46Ar; deduced neutron ground-state spectroscopic factors. Comparison with shell model calculations.
doi: 10.1103/PhysRevC.83.014606
Phys.Rev. C 83, 034610 (2011)
F.M.Nunes, A.Deltuva, J.Hong
Improved description of 34, 36, 46Ar( p, d) transfer reactions
NUCLEAR REACTIONS 1H(34Ar, d), (36Ar, d), (46Ar, d), E=33 MeV/nucleon; analyzed σ(θ), spectroscopic factors using finite range adiabatic wave approximation (ADWA) and Full three-body Faddeev calculations. Neutron-proton asymmetry dependence from knockout measurements.
doi: 10.1103/PhysRevC.83.034610
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.