References quoted in the ENSDF dataset: 32S ADOPTED LEVELS, GAMMAS
47 references found.
Clicking on a keynumber will list datasets that reference the given article.
Phys.Rev. 37, 490 (1931)
S.M.Naude, A.Christy
The Rotational Analysis of the S2 Bands
ATOMIC PHYSICS 32S; measured frequencies; deduced emission spectrum, internal angular momentum.
Z.Physik 100, 656 (1936)
E.Olsson
Das Bandenspektrum des Schwefels
doi: 10.1007/BF01336723
J.Phys.Soc.Japan 25, 950 (1968); Priv.Comm. 1968
H.Matsuda, T.Matsuo
Atomic Masses of 1H, 16O and 32S
ATOMIC MASSES 1H, 16O, 32S; measured masses.
Phys.Rev. 181, 1555 (1969)
C.J.Piluso, G.C.Salzman, D.K.McDaniels
Lifetime and Angular Distribution Measurements from the 31P(p, γ)32S Reaction
NUCLEAR REACTIONS 31P(p, γ), E = 1.248-1.583 MeV; measured σ(E;Eγ, θ), Doppler shift attenuation. 32S deduced levels, J, T1/2, γ-branching, γ-mixing. Ge(Li) detector.
Nucl.Phys. A135, 281 (1969)
J.P.Thibaud, M.M.Aleonard, D.Castera, P.Hubert, F.Leccia, P.Mennrath
Mesures des Vies Moyennes des Premiers Etats Excites du Noyau 32S
NUCLEAR REACTIONS 31P(p, γ), E = 0.811-1.555 MeV; measured Doppler shift attenuation. 32S levels deduced T1/2.
doi: 10.1016/0375-9474(69)90163-8
Phys.Rev.Lett. 24, 903 (1970)
K.Nakai, J.L.Quebert, F.S.Stephens, R.M.Diamond
Quadrupole Moments of First Excited States in 28Si, 32S, and 40Ar
NUCLEAR REACTIONS 206Pb(28Si, 28Si'γ), E=100-120 MeV; 206Pb(32S, 32S'γ), E=130-150 MeV; 130Te(40Ar, 40Ar'γ), E=110-125 MeV; measured σ(E(28Si'), Eγ, θ(γ)), σ(E(32S'), Eγ, θ(γ)), σ(E(40Ar'), Eγ, θ(γ)). 28Si, 32S, 40Ar levels deduced quadrupole moment.
doi: 10.1103/PhysRevLett.24.903
Can.J.Phys. 48, 47 (1970)
R.W.Ollerhead, T.K.Alexander, O.Hausser
Lifetimes in 32S
NUCLEAR REACTIONS 32S(p, p'γ), E=6.15-7.2 MeV; measured σ(E;Eγ), Doppler shift attenuation. 32S levels deduced T1/2, π, branching ratios, transition strengths.
Nucl.Phys. A175, 593 (1971)
O.Hausser, T.K.Alexander, A.B.McDonald, W.T.Diamond
Coulomb Reorientation of 2+ States in 32S and 112Cd
NUCLEAR REACTIONS 112Cd(32S, 32S'γ), E=90, 100 MeV; measured σ(Eγ, θ(S)). 32S, 112Cd levels deduced B(E2), q2. Enriched target.
doi: 10.1016/0375-9474(71)90452-0
Nucl.Phys. A161, 433 (1971)
F.Ingebretsen, B.W.Sargent, A.J.Ferguson, J.R.Leslie, A.Henrikson, J.H.Montague
Evidence for Vibrational Excited States in 32S
NUCLEAR REACTIONS 32S(p, p'γ), E=9.275 MeV; measured σ(Ep', Eγ, θ(p'γ)), Doppler-shift attenuation. 31P(p, γ), E=1.555 MeV; measured σ(Eγ, θ(γ)). 32S deduced levels, J, γ-mixing, T1/2, B(E2). Natural targets.
doi: 10.1016/0375-9474(71)90379-4
Nucl.Phys. A185, 644 (1972)
W.F.Coetzee, M.A.Meyer, D.Reitmann
A Study of the 31P(p, γ)32S Reaction and the Excited States of 32S
NUCLEAR REACTIONS 31P(p, γ), E=0.35-2.03 MeV; measured Q, σ(E;Eγ, θ(γ)), DSA. 32S deduced levels, resonance strengths, γ-ray branching ratios, T1/2, J, π, quadrupole moment, B(E2). Natural targets, Ge(Li) detector.
doi: 10.1016/0375-9474(72)90038-3
Aust.J.Phys. 26, 17 (1973)
C.E.Moss, R.H.Spear, F.Ahmad, A.M.Baxter, L.E.Carlson, P.R.Gardner
Gamma Ray Decay Schemes of Levels at Intermediate Energies in 32S
NUCLEAR REACTIONS 32S(p, p'γ), E=8.03-9.17 MeV; measured pγ-coin. 32S levels deduced branching ratios.
Nucl.Phys. A212, 493 (1973)
J.Vernotte, S.Gales, M.Langevin, J.M.Maison
Recherche de Resonances Isobariques Analogues dans 32S au Moyen des Reactions 31P(p, γ)32S, 31P(p, p)31P et 31P(p, α0)28Si
NUCLEAR REACTIONS 31P(p, γ), E=1.24-1.60 MeV; measured Q, σ(Ep;Eγ, θ(γ)); 31P(p, α0), E=1.24-1.60 MeV; measured σ(E); 31P(p, p), E=1.24-1.60 MeV; measured σ(E). 32S deduced resonances, resonance strengths, γ-ray branching ratios, mixing ratios, transition strengths, L, J, π, T, p-width, α-width, level-width, quadrupole moment. Ge(Li) detector.
doi: 10.1016/0375-9474(73)90820-8
Phys.Rev. C9, 1192 (1974)
Y.T.Cheng, A.Goswami, M.J.Throop, D.K.McDaniels
Status of Nuclear Coexistence for 32S
NUCLEAR REACTIONS 31P(p, γ), E=0.811, 1.117, 1.583 MeV; measured DSAM. 32S level deduced T1/2.
Phys.Rev. C17, 1961 (1978)
J.Kalifa, J.Vernotte, Y.Deschamps, F.Pougheon, G.Rotbard, M.Vergnes, B.H.Wildenthal
31P(3He, d)32S Reaction at 25 MeV
NUCLEAR REACTIONS 31P(3He, 3He), E=25 MeV; measured σ(θ); deduced optical model parameters. 31P(3He, d), E=25 MeV; measured σ(Ed, θ). 32S deduced levels, L, T, J, π, S. DWBA analysis.
Nucl.Phys. A315, 133 (1979)
P.C.Zalm, A.Holthuizen, J.A.G.De Raedt, G.van Middelkoop
Transient Field g-Factor Measurements on the 21+ States of 32S and 34S
NUCLEAR REACTIONS 32S(α, α'γ), E=8.25 MeV; 34S(α, α'γ), E=8.90 MeV; measured αγ(θ, B) in polarized Fe. 32,34S levels deduced g for first 2+ states. 34S enriched target. IMPAC.
doi: 10.1016/0375-9474(79)90638-9
Nucl.Phys. A349, 271 (1980)
G.C.Ball, O.Hausser, T.K.Alexander, W.G.Davies, J.S.Foster, I.V.Mitchell, J.R.Beene, D.Horn, W.McLatchie
Electric Quadrupole Moments of the First Excited States of 28Si, 32S and 34S
NUCLEAR REACTIONS 4He(32S, α), (34S, α), E=70 MeV; measured Doppler-broadened line shapes, αγ(t). 32,34S levels deduced T1/2. 208Pb(28Si, 28Si'), E=105 MeV; 208Pb(32S, 32S'), (34S, 34S'), E=122 MeV; measured σ(θ, E(28Si)), σ(θ, E(32S)), σ(θ, E(34S)), Coulomb excitation. 32,34S, 28Si level deduced static quadrupole moment, B(E2). Enriched targets.
doi: 10.1016/0375-9474(80)90454-6
Z.Phys. A300, 71 (1981)
G.Dannhauser, J.de Boer, R.Lutter, F.Riess, H.Bohn
The Quadrupole Moment Q2+ of 32S
NUCLEAR REACTIONS 60Ni(32S, 32S'), E=70-73 MeV; measured 32Sγ-coin, Coulomb excitation. 32S level deduced quadrupole moment.
Nucl.Phys. A389, 185 (1982)
W.J.Vermeer, M.T.Esat, R.H.Spear
Quadrupole Moment of the First Excited State of 32S
NUCLEAR REACTIONS 208Pb(32S, 32S'), E=122-160 MeV; measured Coulomb excitation probabilities. 32S level deduced quadrupole moment, B(E2). Enriched target.
doi: 10.1016/0375-9474(82)90297-4
Phys.Rev. C37, 28 (1988)
D.F.Fang, E.G.Bilpuch, C.R.Westerfeldt, G.E.Mitchell
Proton Resonances in 32S from E(x) = 9.83 to 12.74 MeV
NUCLEAR REACTIONS 31P(p, p), (p, p'), (p, α), E=1.00-4.01 MeV; measured σ(θ) vs E; deduced 28Si(α, p0) reaction rates. 32S deduced levels, J, π, analog states, Γp, proton resonance strengths.
Z.Phys. A330, 361 (1988)
H.-J.Simonis, F.Hagelberg, K.-H.Speidel, M.Knopp, W.Karle, U.Kilgus, J.Gerber
Measurements of Lifetime and g-Factor of the 32S(41+) State at 4.459 MeV
NUCLEAR REACTIONS 4He(32S, 32S'), E=tandem; measured recoil αγ-coin, anisotropies. 32S level deduced g. Transient field technique.
Phys.Rev. C39, 311 (1989)
G.M.Crawley, C.Djalali, N.Marty, M.Morlet, A.Willis, N.Anantaraman, B.A.Brown, A.Galonsky
Isovector and Isoscalar Spin-Flip Excitations in Even-Even s-d Shell Nuclei Excited by Inelastic Proton Scattering
NUCLEAR REACTIONS 24,26Mg, 28Si, 32S(p, p'), E=201 MeV; measured σ(θ). 24,26Mg, 28Si, 32S deduced 1+ states, B(M1). Enriched targets. DWBA analysis, shell model calculations.
Phys.Rev. C52, 1681 (1995)
J.G.Ross, J.Gorres, C.Iliadis, S.Vouzoukas, M.Wiescher, R.B.Vogelaar, S.Utku, N.P.T.Bateman, P.D.Parker
Indirect Study of Low-Energy Resonances in 31P(p, α)28Si and 35Cl(p, α)32S
NUCLEAR REACTIONS 31P, 35Cl(3He, d), E=25 MeV; measured particle spectra, γd-, (particle)d-coin; deduced (p, γ), (p, α) reaction rates for 31P, 35Cl. 36Ar deduced levels Γ, J, π, T. 32S deduced levels Γ, J, π, T, resonance strength.
Z.Phys. A357, 157 (1997)
J.Brenneisen, B.Erhardt, F.Glatz, Th.Kern, R.Ott, H.Ropke, J.Schmalzlin, P.Siedle, B.H.Wildenthal
The Structure of 32S I. Spectroscopy of the Highly-Excited States
NUCLEAR REACTIONS 29Si(α, n), E=14.4 MeV; measured neutron spectra, γn-coin, γn(θ). 31P(p, γ), E=2-3.3 MeV; measured Eγ, Iγ, γ(θ). 32S deduced high-spin levels, J, π, T, γ-branching ratios, T1/2, δ, B(M1). Other data input.
Phys.Rev. C58, 699 (1998)
A.Kangasmaki, P.Tikkanen, J.Keinonen, W.E.Ormand, S.Raman, Zs.Fulop, A.Z.Kiss, E.Somorjai
Lifetimes of 32S Levels
NUCLEAR REACTIONS 2H(31P, n), E=24, 29 MeV; 28Si(6Li, np), E=8, 12 MeV; 31P(p, γ), E=1.0-1.6 MeV; measured Doppler-broadened Eγ, Iγ. 32S levels deduced T1/2, branching ratios, δ, B(E2), B(M1). DSA analysis, Monte Carlo simulations.
NUCLEAR STRUCTURE 32S; calculated levels, T1/2, δ. Shell model.
J.Phys.(London) G31, S1869 (2005)
M.B.Gomez Hornillos, M.Chartier, W.Mittig, B.Blank, F.Chautard, C.E.Demonchy, A.Gillibert, B.Jacquot, B.Jurado, N.Lecesne, A.Lepine-Szily, N.A.Orr, P.Roussel-Chomaz, H.Savajols, A.C.C.Villari
Mass measurements with the CIME cyclotron at GANIL
ATOMIC MASSES 12C, 16O, 20Ne, 32S, 36,40Ar; measured masses. Cyclotron-based mass spectrometry.
doi: 10.1088/0954-3899/31/10/090
Nature(London) 438, 1096 (2005)
S.Rainville, J.K.Thompson, E.G.Myers, J.M.Brown, M.S.Dewey, E.G.Kessler, R.D.Deslattes, H.G.Borner, M.Jentschel, P.Mutti, D.E.Pritchard
A direct test of E=mc2
ATOMIC MASSES 28,29Si, 32,33S; measured mass ratios. Penning trap.
doi: 10.1038/4381096a
Phys.Rev. A 72, 022510 (2005)
W.Shi, M.Redshaw, E.G.Myers
Atomic masses of 32, 33S, 84, 86Kr, and 129, 132Xe with uncertainties ≤ 0.1 ppb
ATOMIC MASSES 32,33S, 84,86Kr, 129,132Xe; measured masses. Penning trap.
doi: 10.1103/PhysRevA.72.022510
Phys.Lett. B 632, 207 (2006)
K.-H.Speidel, S.Schielke, J.Leske, J.Gerber, P.Maier-Komor, S.J.Q.Robinson, Y.Y.Sharon, L.Zamick
Experimental g factors and B(E2) values in Ar isotopes: Crossing the N = 20 semi-magic divide
NUCLEAR REACTIONS 12C(32S, 8Be), (34S, 8Be), (32S, 32S'), E=65-67 MeV; measured Eγ, Iγ(θ, H, t), (particle)γ-coin, DSA. 36,38Ar, 32S levels deduced g factors, T1/2, B(E2). Transient field technique.
doi: 10.1016/j.physletb.2005.10.052
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
Nucl.Instrum.Methods Phys.Res. A589, 202 (2008)
T.Kibedi, T.W.Burrows, M.B.Trzhaskovskaya, P.M.Davidson, C.W.Nestor, Jr.
Evaluation of theoretical conversion coefficients using BrIcc
COMPILATION Z=5-110; compiled and evaluated ICC data. BrICC database.
doi: 10.1016/j.nima.2008.02.051
Phys.Rev. C 80, 051302 (2009)
A.A.Kwiatkowski, B.R.Barquest, G.Bollen, C.M.Campbell, D.L.Lincoln, D.J.Morrissey, G.K.Pang, A.M.Prinke, J.Savory, S.Schwarz, C.M.Folden III, D.Melconian, S.K.L.Sjue, M.Block
Precision test of the isobaric multiplet mass equation for the A=32, T=2 quintet
ATOMIC MASSES 32,33Si, 32S, 31,34P; measured masses using LEBIT Penning-trap spectrometer; deduced mass excesses. Discussed validity of quadratic form of isobaric multiplet mass equation (IMME).
doi: 10.1103/PhysRevC.80.051302
Phys.Rev. C 85, 025501 (2012)
D.Melconian, S.Triambak, C.Bordeanu, A.Garcia, J.C.Hardy, V.E.Iacob, N.Nica, H.I.Park, G.Tabacaru, L.Trache, I.S.Towner, R.E.Tribble, Y.Zhai
β decay of 32Cl: Precision γ-ray spectroscopy and a measurement of isospin-symmetry breaking
RADIOACTIVITY 32Cl(β+), (EC)[20 MeV/nucleon 32Cl secondary beam from 1H(32S, n), E AP 24.8 MeV/nucleon primary reaction using MARS facility]; measured particle spectra, Eγ, Iγ, β, βγ-coin, half-life; deduced mass excess, Q(EC). 32S; deduced levels, J, π, isospin, β branches, logft, Gamow-Teller matrix elements, isospin-symmetry-breaking correction for superallowed transition. Comparison with earlier studies and shell-model calculation. 30S, 32Cl(β+); measured half-lives from γ-decay curves.
doi: 10.1103/PhysRevC.85.025501
At.Data Nucl.Data Tables 99, 69 (2013)
I.Angeli, K.P.Marinova
Table of experimental nuclear ground state charge radii: An update
COMPILATION Z=0-96; compiled nuclear radii, rms nuclear charge radii.
doi: 10.1016/j.adt.2011.12.006
Phys.Rev. C 88, 064313 (2013)
M.Itoh, S.Kishi, H.Sakaguchi, H.Akimune, M.Fujiwara, U.Garg, K.Hara, H.Hashimoto, J.Hoffman, T.Kawabata, K.Kawase, T.Murakami, K.Nakanishi, B.K.Nayak, S.Terashima, M.Uchida, Y.Yasuda, M.Yosoi
Isoscalar giant resonance strengths 32S and possible excitation of superdeformed and 28Si + α cluster bandheads
NUCLEAR REACTIONS 32S(α, α'), E=386 MeV; measured Eα, Iα, σ(θ), isoscalar giant resonance strengths using Grand Raiden spectrometer at RCNP, Osaka cyclotron facility. 32S; deduced levels, J, π, L-transfers, E0, E1, E2, E3, E4 strengths, superdeformed bandheads, parity-doublet 28S+α cluster bands. Comparison with the assumption of point masses for 16O+16O and 28Si+α cluster structures. Multipole decomposition analysis (MDA) and DWBA analysis.
doi: 10.1103/PhysRevC.88.064313
Few-Body Systems 58, 58 (2017)
M.Bouhelal, M.Labidi, F.Haas
Shell Model Description of the 32, 34, 36S Isotopes
NUCLEAR STRUCTURE 32,34,36S; calculated levels, J, π, γ E2, E3 transition strengths using shell model with PSDPF interaction. Compared with data.
doi: 10.1007/s00601-017-1225-2
Eur.Phys.J. A 53, 26 (2017)
E.Ha, M.-K.Cheoun
A study of Gamow-Teller transitions for N = Z nuclei, 24Mg, 28Si, and 32S, by a deformed QRPA
NUCLEAR STRUCTURE 24Mg, 28Si, 32S; calculated single-neutron levels, J, π vs deformation, s-d shell β-decay GT transitions strength distribution, B(GT) using DQRPA (Deformed QRPA).
doi: 10.1140/epja/i2017-12216-7
Phys.Rev. C 98, 024309 (2018)
E.Aboud, M.B.Bennett, C.Wrede, M.Friedman, S.N.Liddick, D.Perez-Loureiro, D.W.Bardayan, B.A.Brown, A.A.Chen, K.A.Chipps, C.Fry, B.E.Glassman, C.Langer, E.I.McNeice, Z.Meisel, W.-J.Ong, P.D.O'Malley, S.D.Pain, C.J.Prokop, H.Schatz, S.B.Schwartz, S.Suchyta, P.Thompson, M.Walters, X.Xu
Toward complete spectroscopy using β decay: The example of 32Cl (βγ)32S
RADIOACTIVITY 32Cl(β+), (EC)[from 9Be(36Ar, X), E=150 MeV/nucleon followed by beam separation and purification using A1900 fragment separator and time-of-flight separation method using Radio Frequency Fragment Separator (RFFS) at NSCL-MSU]; measured Eγ, Iγ, βγ- and βγγ-coin using the Clovershare array of HPGe detectors, 32Cl implants and β by a plastic scintillator at NSCL-MSU. 32S; deduced levels, J, π, β feedings, logft, Gamow-Teller strengths, half-lives, proton, γ and α widths of 8861- and 9650-keV resonances. Comparison with sd USDA and USDB shell model calculations, and with previous experimental values and ENSDF evaluations. 31P(p, α)28Si, E=9650 keV; deduced resonance strength.
doi: 10.1103/PhysRevC.98.024309
Phys.Rev. C 98, 044301 (2018)
L.Huth, V.Durant, J.Simonis, A.Schwenk
Shell-model interactions from chiral effective field theory
NUCLEAR STRUCTURE 18,19,20O, 19,21,22F, 21,23,24Ne, 24,26,28Mg, 26,28,29Al, 29,30,31Si, 32,33,35P, 32,33,35S, 34,35,37Cl, 36,37Ar, 38K; calculated levels, J, π for the chiral shell-model interactions at LO, NLO, and NLOvs, and compared to experimental, and USDA/USDB shell-model results.
doi: 10.1103/PhysRevC.98.044301
Phys.Rev. C 100, 054329 (2019)
N.A.Smirnova, B.R.Barrett, Y.Kim, I.J.Shin, A.M.Shirokov, E.Dikmen, P.Maris, J.P.Vary
Effective interactions in the sd shell
NUCLEAR STRUCTURE 18,19,21,23,25,26,27F, 21,22,23,24O, 22Na, 24Mg, 28,29Si, 32S, 39K; calculated levels, J, π, effective single-particle energies (ESPEs), B(E2) and Q(first 2+) for 24Mg, 28Si, 32S. 16,17,18,19,20,21,22,23,24,25,26,27,28O; calculated ground state energies relative to that of 16O, sub-shell gap and neutron spin-orbit splitting for even-A nuclei. No-core shell-model calculations with Okubo-Lee-Suzuki transformation, and microscopic effective shell-model interactions in the valence sd shell, obtained from chiral N3LO, JISP16, and Daejeon16 nucleon-nucleon potentials. Comparison with experimental data. Discussed possible role of the three-nucleon forces.
doi: 10.1103/PhysRevC.100.054329
Can.J.Phys. 98, 148 (2020)
S.Aslanzadeh, M.R.Shojaei, A.A.Mowlavi
Calculation of the energy levels and charge radius of 24Mg and 32S isotopes in the cluster model
NUCLEAR STRUCTURE 24Mg, 32S; calculated energy levels, J, π, charge radii using cluster model. Comparison with available data.
Phys.Rev. C 101, 054308 (2020)
J.M.R.Fox, C.W.Johnson, R.N.Perez
Uncertainty quantification of an empirical shell-model interaction using principal component analysis
NUCLEAR STRUCTURE 18F, 26Al, 26Mg; calculated B(E2) and B(M1) for several transitions; deduced median values and uncertainty intervals from comparison with experimental values. 17,18,19,20,21,22,23,24O, 18,19,20,21,22,23,24,25,26,27F, 20,21,22,23,24,25,26,27,28Ne, 22,23,24,25,26,27,28,29Na, 24,25,26,27,28,29,30Mg, 26,27,28,29,30,31,32,33Al, 28,29,30,31,32,33,34Si, 30,31,32,33,34,35P, 32,33,34,35,36S, 34,35,36,37Cl, 36,37,38Ar, 38,39K; calculated level energies, J, π; deduced uncertainties from comparison with experimental energies. Uncertainty quantification (UQ) in level energies, B(E2), B(M1) and B(GT) of a "gold-standard" empirical interaction for nuclear configuration-interaction shell model calculations in the sd-shell valence, investigating sensitivity of observables to perturbations in the 66 parameters.
RADIOACTIVITY 26Ne, 32Si(β-); calculated B(GT), dark matter scattering on 36Ar coupling parameter; deduced uncertainty intervals for B(GT) from comparison with experimental values. Uncertainty quantification through shell-model calculations.
doi: 10.1103/PhysRevC.101.054308
INDC(NDS)-0816 (2020)
N.Stone
Table of Recommended Nuclear Magnetic Dipole Moments: Part II, Short-Lived States
COMPILATION Z=5-95; 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
INDC(NDS)-0833 (2021)
N.J.Stone
Table of Nuclear Electric Quadrupole Moments
COMPILATION Z=1-102; compiled experimental measurements of static electric quadrupole moments of ground states and excited states of atomic nuclei throughout the periodic table.
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.
Phys.Rev. C 105, 054314 (2022)
D.D.Dao, F.Nowacki
Nuclear structure within a discrete nonorthogonal shell model approach: New frontiers
NUCLEAR STRUCTURE 20,22,24,26,28Ne, 24,26,28,30Mg, 28,30,32Si, 32,34S, 36Ar; calculated ground state energy, levels, J, π, B(E2). 25Mg; calculated levels, J, π. 254No; calculated levels, J, π, proton and neutron orbital occupancies for the ground state, potential energy surface. Discrete nonorthogonal shell model (DNO-SM) formalism. Comparison to experimental data.
doi: 10.1103/PhysRevC.105.054314
Prog.Part.Nucl.Phys. 123, 103930 (2022)
T.Kibedi, A.B.Garnsworthy, J.L.Wood
Electric monopole transitions in nuclei
doi: 10.1016/j.ppnp.2021.103930