References quoted in the ENSDF dataset: 32CL ADOPTED LEVELS, GAMMAS
23 references found.
Clicking on a keynumber will list datasets that reference the given article.
Phys.Rev. 90, 320 (1953)
N.W.Glass, L.K.Jensen, J.R.Richardson
The Short-Lived Radioisotopes P28 and Cl32
RADIOACTIVITY 28P, 32Cl(EC), 24Al(EC), (β+) [from 28Si, 32S, 24Mg(p, n), E=20 MeV]; measured decay products, Eγ, Iγ. 28P, 32Cl; deduced γ-ray energies, T1/2, masses. Comparison with available data. UCLA cyclotron.
Can.J.Phys. 32, 223 (1954)
S.W.Breckon, A.Henrikson, W.M.Martin, J.S.Foster
The Radioactive Isotopes Al24, P28, Cl32
doi: 10.1139/p54-020
Phys.Rev. 96, 773 (1954)
H.Tyren, P.A.Tove
Short-Lived Radio-Nuclides Produced by a Synchrocyclotron
Nucl.Phys. 77, 401(1966)
W.C.Anderson, L.T.Dillman, J.J.Kraushaar
The Decay of 32Cl and 40Sc and the T=1 Isobaric Analogue States in 32S And 40Ca
RADIOACTIVITY 32Cl, 40Sc[from 32S(p, n), 40Ca(p, n)]; measured Eβ+, Eγ, Iγ, γγ-coin. 32S, 40Ca deduced levels, isospin. Natural targets.
doi: 10.1016/0029-5582(66)90184-2
Phys.Rev.Letters 17, 705 (1966)
D.A.Bromley, J.C.Overley, P.D.Parker
Masses of N12, Al24, P28, Cl32, and Sc40
NUCLEAR STRUCTURE 24Al, 12C, 12N, 40Sc, 28P, 32Cl; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.17.705
Phys.Rev. 165, 1194 (1968)
A.J.Armini, J.W.Sunier, J.R.Richardson
Masses and Decay of Al24, P28, Cl32, Sc40, and Their Tz = 0 Analog States
NUCLEAR STRUCTURE 28P, 32Cl, 40Sc, 24Al; measured not abstracted; deduced nuclear properties.
Nucl.Phys. A137, 585 (1969)
J.E.Steigerwalt, J.W.Sunier, J.R.Richardson
Delayed Heavy-Particle Emission from 24Al and 32Cl
RADIOACTIVITY 24Al, 32Cl [from 24Mg, 32S(p, n)]; measured T1/2; delayed Ep, Ip, Eα, Iα; deduced Eβ, Iβ, log ft. 24Mg, 32S deduced levels, J, π.
doi: 10.1016/0375-9474(69)90095-5
Phys.Rev. C4, 1800 (1971)
D.R.Goosman, K.W.Jones, E.K.Warburton, D.E.Alburger
Masses and Half-Lives of 20Na, 24Al, 28P, 32Cl, and 36K from the (p, n) Reaction
RADIOACTIVITY 20Na, 24Al, 28P, 32Cl, 36K; measured T1/2. 20Ne, 24Mg, 28Si, 32S, 36Ar(p, n), E approx threshold; measured Q, threshold. 20Na, 24Al, 28P, 32Cl, 36K deduced mass excess.
Phys.Rev.Lett. 39, 792 (1977)
E.Hagberg, P.G.Hansen, J.C.Hardy, A.Huck, B.Jonson, S.Mattsson, H.L.Ravn, P.Tidemand-Petersson, G.Walter
Decay of a T(z) = -2 Nucleus: Argon-32
RADIOACTIVITY 32Ar; measured β delayed protons, T1/2; deduced log ft. 32Cl deduced level, T, mass excess.
doi: 10.1103/PhysRevLett.39.792
Nucl.Phys. A330, 429 (1979)
J.Honkanen, M.Kortelahti, K.Valli, K.Eskola, A.Hautojarvi, K.Vierinen
Delayed Particle Emission Following the β+ Decay of 28P and 32Cl
RADIOACTIVITY 28P [from 28Si(p, n)];32Cl [from 32S(p, n)]; measured β-delayed Ep, Eα, Ip, Iα; deduced maximum log ft. 28Si, 32S deduced levels, Γα/Γp, J, π. Natural targets.
doi: 10.1016/0375-9474(79)90064-2
Nucl.Phys. A503, 77 (1989)
C.Jeanperrin, L.H.Rosier, B.Ramstein, E.I.Obiajunwa
Spectroscopy of 32Cl Nucleus via the 32S(3He, t)32Cl reaction at 34.5 MeV
NUCLEAR REACTIONS 32S(3He, t), E=34.5 MeV; measured σ(θ). 32Cl deduced levels, J, π, T. Coulomb displacement energy calculation comparison, magnetic spectrometer.
doi: 10.1016/0375-9474(89)90255-8
Z.Phys. A345, 265 (1993)
D.Schardt, K.Riisager
Beta-Neutrino Recoil Broadening in β-Delayed Proton Emission of 32Ar and 33Ar
RADIOACTIVITY 32,33Ar(β+p) [from Ca(p, X), E=600 MeV]; measured β-delayed Ep, Ip. 32Cl deduced level width. 33Cl deduced level width, Gamow-Teller transition strength to IAS.
Phys.Rev. C50, 1185 (1994)
S.Vouzoukas, C.P.Browne, U.Giesen, J.Gorres, S.M.Graff, H.Herndl, C.Iliadis, L.O.Lamm, J.Meissner, J.G.Ross, K.Scheller, L.van Wormer, M.Wiescher, A.A.Rollefson
Reaction Rate for 31S(p, γ)32Cl and Its Influence on the SiP Cycle in Hot Stellar Hydrogen Burning
NUCLEAR REACTIONS 32S(3He, t), E=22.5-25 MeV; measured σ(Et), σ(θ); deduced 31S(p, γ) reaction rate, hot stellar hydrogen burning implications. 32Cl deduced level, J, π, C2S, Γγ.
Phys.Rev. C62, 044312 (2000)
W.F.Rogers, G.Georgiev, G.Neyens, D.Borremans, N.Coulier, R.Coussement, A.D.Davies, J.L.Mitchell, S.Teughels, B.A.Brown, P.F.Mantica
Ground-State Magnetic Moment of the T = 1 Nucleus 32Cl using On-Line β-NMR Spectroscopy
RADIOACTIVITY 31S, 32Cl(β+) [from 36Ar fragmentation]; measured β asymmetry vs NMR frequency. 31S, 32Cl deduced μ. Comparisons with neighboring nuclides. β-NMR technique.
doi: 10.1103/PhysRevC.62.044312
Phys.Rev. C 73, 054313 (2006)
S.Triambak, A.Garcia, E.G.Adelberger, G.J.P.Hodges, D.Melconian, H.E.Swanson, S.A.Hoedl, S.K.L.Sjue, A.L.Sallaska, H.Iwamoto
Mass of the lowest T = 2 state in 32S: A test of the isobaric multiplet mass equation
NUCLEAR REACTIONS 31P(p, γ), E=3.285 MeV; measured Eγ, Iγ. 32S deduced excited states energies.
ATOMIC MASSES 32Si, 32P, 32S, 32Cl, 32Ar; analyzed mass excesses for T=2 quintet. Isospin-multiplet mass equation.
doi: 10.1103/PhysRevC.73.054313
Phys.Rev. C 77, 065503 (2008)
M.Bhattacharya, D.Melconian, A.Komives, S.Triambak, A.Garcia, E.G.Adelberger, B.A.Brown, M.W.Cooper, T.Glasmacher, V.Guimaraes, P.F.Mantica, A.M.Oros-Peusquens, J.I.Prisciandaro, M.Steiner, H.E.Swanson, S.L.Tabor, M.Wiedeking
ft value of the 0+ → 0+ β+ decay of 32Ar: A measurement of isospin symmetry breaking in a superallowed decay
RADIOACTIVITY 32Ar(β+) [from 9Be(36Ar, X), E=100 MeV/nucleon]; measured Eγ, Iγ, Ep, Ip, pγ-coin. 32Ar; deduced superallowed decay branching ratio, ft value, isospin symmetry breaking correction. 32Cl; deduced levels, J, π. 31S; deduced levels, π. Comparison with theoretical data.
ATOMIC MASSES 32Cl; measured masses. Q-value method.
doi: 10.1103/PhysRevC.77.065503
Phys.Rev. C 82, 052501 (2010)
A.Kankainen, T.Eronen, D.Gorelov, J.Hakala, A.Jokinen, V.S.Kolhinen, M.Reponen, J.Rissanen, A.Saastamoinen, V.Sonnenschein, J.Aysto
High-precision mass measurement of 31S with the double Penning trap JYFLTRAP improves the mass value for 32Cl
ATOMIC MASSES 31S; measured mass by time-of-flight (TOF) ion-cyclotron resonance method using JYFLTRAP double Penning trap mass spectrometer using 31P as reference; deduced mass excess and Q value for EC decay. 32Cl; analyzed mass excess from S(p); deduced improved Q(ϵ) value and logft. 32Si, 32P, 32S, 32Cl, 32Ar; analyzed isobaric mass multiplet equation (IMME) for A=32, T=2 quintet. Comparison of masses with previous measurements and evaluations.
RADIOACTIVITY 31S(EC)[from 32S(p, pn), E=40 MeV]; measured mass using IGISOL and JYFLTRAP facilities; deduced Q value, logft. 32S, 32Cl, 32Ar(EC); analyzed Q values, logft. Implication for superallowed β decay of 32Ar.
doi: 10.1103/PhysRevC.82.052501
Phys.Rev. C 81, 055503 (2010)
C.Wrede, J.A.Clark, C.M.Deibel, T.Faestermann, R.Hertenberger, A.Parikh, H.-F.Wirth, S.Bishop, A.A.Chen, K.Eppinger, A.Garcia, R.Krucken, O.Lepyoshkina, G.Rugel, K.Setoodehnia
Toward precise QEC values for the superallowed 0+ → 0+ β decays of T=2 nuclides: The masses of 20Na, 24Al, 28P, and 32Cl
NUCLEAR REACTIONS 20Ne, 24Mg, 28Si, 32S, 36Ar(3He, t), E=32 MeV; measured triton spectra using Q3D magnetic spectrograph; deduced levels, Q values, mass excesses.
ATOMIC MASSES 20Na, 24Al, 28P, 32Cl; measured mass excesses using (3He, t) reaction. 36Ar(3He, t)36K used for calibration. Comparison with AME-2003.
doi: 10.1103/PhysRevC.81.055503
Phys.Rev. C 84, 055806 (2011)
M.Matos, J.C.Blackmon, L.E.Linhardt, D.W.Bardayan, C.D.Nesaraja, J.A.Clark, C.M.Deibel, P.D.O'Malley, P.D.Parker
Unbound states of 32Cl and the 31S(p, γ)32Cl reaction rate
NUCLEAR REACTIONS 32S(3He, t), E=30 MeV; measured E(t), I(t), σ(θ), pt(θ). 32Cl; deduced levels, J, π, branching ratios for proton decay to 31S. 28Si(3He, t)28P, E=30 MeV; measured E(t), I(t); deduced levels. 31S(p, γ)32Cl; deduced reaction rates.
doi: 10.1103/PhysRevC.84.055806
Acta Phys.Pol. B45, 167 (2014)
W.Satula, J.Dobaczewski, M.Konieczka, W.Nazarewicz
Isospin Mixing Within the Symmetry Restored Density Functional Theory and Beyond
NUCLEAR STRUCTURE 32Cl, 32S, 10C, 14O, 22Mg, 34Ar, 34Cl, 18Ne, 26Si, 30S, 18F, 22Na, 30P; calculated energy levels, J, π, isospin breaking corrections. Density functional theory model, comparison with available data.
INDC(NDS)-0794 (2019)
N.J.Stone
Table of Recommended Nuclear Magnetic Dipole Moments: Part I - Long-lived States
COMPILATION Z=0-99; compiled experimental values of nuclear magnetic moments.
Phys.Rev. C 104, L061303 (2021)
M.Kamil, S.Triambak, A.Magilligan, A.Garcia, B.A.Brown, P.Adsley, V.Bildstein, C.Burbadge, A.Diaz Varela, T.Faestermann, P.E.Garrett, R.Hertenberger, N.Y.Kheswa, K.G.Leach, R.Lindsay, D.J.Marin-Lambarri, F.Ghazi Moradi, N.J.Mukwevho, R.Neveling, J.C.Nzobadila Ondze, P.Papka, L.Pellegri, V.Pesudo, B.M.Rebeiro, M.Scheck, F.D.Smit, H.-F.Wirth
Isospin mixing and the cubic isobaric multiplet mass equation in the lowest T=2, A=32 quintet
ATOMIC MASSES 32Ar, 32Cl, 32S, 32P, 32Si; analyzed experimental masses by a cubic fit to the isobaric multiplet mass equation (IMME) for the lowest isospin T=2 quintet in A=32 nuclei; investigated isospin mixing by combining high-resolution experimental data for proton spectrum from 32Ar β-delayed proton decay, and from triton spectrum in 32S(3He, t) reaction with the state-of-the-art shell-model calculations; evaluated isospin mixing matrix elements; extracted cubic and quartic coefficients of the IMME; deduced that isospin mixing with nonanalog T=1 states contributes to the IMME breakdown. 32Ar; analyzed experimental β-delayed proton spectrum by R-matrix fit; calculated proton emission amplitudes from states in 32Cl.
doi: 10.1103/PhysRevC.104.L061303
Chin.Phys.C 45, 030003 (2021)
M.Wang, W.J.Huang, F.G.Kondev, G.Audi, S.Naimi
The AME 2020 atomic mass evaluation (II). Tables, graphs and references
ATOMIC MASSES A=1-295; compiled, evaluated atomic masses, mass excess, β-, ββ and ββββ-decay, binding, neutron and proton separation energies, decay and reaction Q-value data.