References quoted in the ENSDF dataset: 32S 31P(P,G) E=RES
55 references found.
Clicking on a keynumber will list datasets that reference the given article.
Phys.Rev. 99, 1339 (1955)
E.B.Paul, H.E.Gove, A.E.Litherland, G.A.Bartholomew
Proton Capture Gamma Rays from the Reaction 31P(p, γ)32S Leading to the Ground and First Excited States of 32S
NUCLEAR REACTIONS 31P(p, γ), (p, x), E=-1.0 eV-2.3 MeV; measured products, 32S, Eγ, Iγ; deduced σ(θ), resonance parameters. Data were imported from EXFOR entry C0873.
Nucl.Phys. 22, 245 (1961)
S.L.Andersen, O.Dorum, E.Gautvik, T.Holtebekk
Resonance Energies and Half-Widths for Proton Capture in Sodium and Phosphorus
NUCLEAR STRUCTURE 32S; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(61)90456-4
Proc.Rutherford Jubilee Intern.Conf., Manchester, England, J.B.Birks, Ed. Academic Press, New York, p.261 (1961)
S.L.Andersen
Gamma-Transitions in 32S
NUCLEAR STRUCTURE 32S; measured not abstracted; deduced nuclear properties.
J.Phys.Radium 22, 541 (1961)
G.R.Bishop, G.A.Proca
Contribution to the study of the S32 nucleus
NUCLEAR STRUCTURE 32S; measured not abstracted; deduced nuclear properties.
doi: 10.1051/jphysrad:019610022010054100
Nuclear Phys. 39, 631 (1962)
I.Berkes, I.Dezsi, I.Fodor, L.Keszthelyi
The Low Energy Resonances in the P31(p, γ)S32 Nuclear Reaction
NUCLEAR STRUCTURE 32S; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(62)90420-0
Bull.Am.Phys.Soc. 7, No.4, 301, JB8 (1962)
P.R.Chagnon, P.A.Treado
Low-Energy Resonances in P31(p, γ)S32
NUCLEAR STRUCTURE 32S; measured not abstracted; deduced nuclear properties.
Nuclear Phys. 31, 65 (1962)
E.B.Nelson, R.R.Carlson, L.D.Schlenker
The P31(p, γ) S32 Reaction at 355 keV and 440 keV Proton Energy
NUCLEAR STRUCTURE 32S; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(62)90729-0
Nucl.Phys. 40, 195 (1963)
P.R.Chagnon, P.A.Treado
Gamma Ray Transitions in 32S following Proton Capture by 31P
NUCLEAR STRUCTURE 32S; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(63)90265-7
Soc.Sci.Fennica, Commentationes Phys.Math 28, No.6 (1963)
E.Spring
An Investigation of the P31(p, γ)S32 Reaction at the Proton Energies 642 Kev, 812 Kev, 1116 Kev, and 1147 keV
NUCLEAR STRUCTURE 32S, 28Si; measured not abstracted; deduced nuclear properties.
Nucl.Phys. 40, 438 (1963)
L.K.Ter Veld, H.Brinkman
The 355 and 439 keV Resonances in the Reaction 31P(p, γ)32S
NUCLEAR STRUCTURE 32S; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(63)90286-4
Physica 30, 1197 (1964)
P.J.M.Smulders
Levels of 32S Excited in the 28Si(α, γ)32S and 31P(p, γ)32S Reactions
NUCLEAR STRUCTURE 32S; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-8914(64)90108-9
Phys.Norvegica 1, 247 (1965)
S.L.Andersen
Energy Levels in 32S from the Reaction 31P(p, γ)32S
NUCLEAR STRUCTURE 32S; measured not abstracted; deduced nuclear properties.
Nucl.Phys. 64, 177 (1965)
G.Dearnaley, D.S.Gemmell, B.W.Hooton, G.A.Jones
Fine Structure of the Giant Resonance in the Reaction P31(p, γ0)S32
NUCLEAR REACTIONS 31P(p, γ0), E=2-11.5 MeV; measured σ(E, θ). 32S deduced levels, J, π.
doi: 10.1016/0029-5582(65)90350-0
Soc.Sci.Fennica, Commentationes Phys.Math. 31, No.7 (1965)
P.Holmberg
The 31P(p, γ)32S Reaction in the Proton Energy Region 800-1160 keV
NUCLEAR STRUCTURE 32S; measured not abstracted; deduced nuclear properties.
Soc.Sci.Fennica, Commentationes Phy.Math. 31, No.1 (1965)
E.Spring, P.Holmberg, H.Jungner
The 31P(p, γ)32S Reaction at Proton Energies 1550 - 2050 keV
NUCLEAR STRUCTURE 32S; measured not abstracted; deduced nuclear properties.
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. 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
Phys.Norvegica 3, 31(1968)
O.Dorum
Polarization Measurements on Gamma Rays from Transitions in 32S
NUCLEAR REACTIONS 31P(p, γ), E = 1436 keV; measured γ linear polarization, σ(Eγ), asymmetry. 32S deduced levels, J, π, γ-mixing. Compton polarimeter.
Nucl.Phys. A138, 253 (1969)
W.M.Mason, N.W.Tanner, G.Kernel
Mechanism of the 31P(p, γ)32S Reaction in the Giant Dipole Resonance Region
NUCLEAR REACTIONS 31P(p, γ), E=9.5-11.5 MeV; measured σ(E;Eγ, θ); deduced channel spin components, direct reaction contribution. 32S deduced resonances, level-width, autocorrelations.
doi: 10.1016/0375-9474(69)90335-2
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
Comment.Phys.-Math. 40, 1 (1970)
I.Forsblom, P.Paukku, S.Penttinen
The 31P(p, γ)32S Reaction in the Proton Energy Range 2000-2400 keV
NUCLEAR REACTIONS 31P(p, γ), E=2.0-2.4 MeV; measured σ(E;Eγ, θ(γ)), Iγ. 32S deduced resonances, J, π, γ-branching. 32S deduced levels, γ-branching.
C.R.Acad.Sci., Ser.B, 271, 970 (1970)
S.Gales, M.Langevin, J.-M.Maison, J.Vernotte
Recherche du Premier Etat T = 2 du Noyau Soufre-32 au Moyen de la Reaction 31P(p, γ)32S
NUCLEAR REACTIONS 31P(p, γ), E=3.10-3.35 MeV; measured σ(E;Eγ, θ(γ)). 32S deduced resonances, levels, J, π, T, γ-branching.
Phys.Scr. 1, 159 (1970)
P.Holmberg, M.Viitasalo
The E = 1146 keV and 1151 keV Resonances in the 31P(p, γ)32S Reaction
NUCLEAR REACTIONS 31P(p, γ), E=1146, 1151 keV; measured σ(Eγ, θ(γ)). 32S deduced resonances, J, π.
Comment.Phys.-Math. 40, 149 (1970)
M.Viitasalo, I.Forsblom
The Spin and Parity of the 4458 keV State in 32S
NUCLEAR REACTIONS 31P(p, γ), E=1949 keV; measured σ(Eγ, θ(γ)). 32S deduced levels, resonances, J, π.
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
Nuovo Cimento 3A, 347 (1971)
M.J.Renan, R.J.Keddy
Lifetimes of Low-Lying Excited States in 32S
NUCLEAR REACTIONS 31P(p, γ), E=439, 541, 642 keV; measured Doppler-shift attenuation. 32S levels deduced T1/2.
Nucl.Instrum.Methods 97, 475 (1971)
B.P.Singh, H.C.Evans
Relative Efficiency of Ge(Li) Gamma Ray Detectors from 0.5 to 12 MeV
RADIOACTIVITY 56Co; measured Iγ. Ge(Li) detectors.
NUCLEAR REACTIONS 27Al(p, γ), 31P(p, γ), E=992 keV, 1248 keV; measured σ(Eγ, θ(γ)). 23Na, 39K, (p, γ), E=resonance; measured σ(Eγ, θ(γ)). 32S deduced levels, γ-branching. 24Mg, 28Si, 40Ca deduced branching ratios.
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
J.Phys.(Paris) 33, 451 (1972)
F.Leccia, M.M.Aleonard, D.Castera, P.Hubert, P.Mennrath
Etude des Resonances de la Reaction 31P(p, γ)32S dans le Domaine d'Energie E = 1 100-1 600 keV
NUCLEAR REACTIONS 31P(p, γ), E=1.1-1.6 MeV; measured σ(E), Eγ, Iγ. 32S deduced resonances, J, π, level-width, γ-branching.
Comment.Phys.-Math. 42, 263 (1972)
M.Viitasalo, I.Forsblom
On the Gamma Decay of 32S
NUCLEAR REACTIONS 31P(p, γ), E=0.3-1.13 MeV; measured σ(E, Eγ). 32S levels deduced γ-branching.
Izv.Akad.Nauk SSSR, Ser.Fiz. 37, 1895 (1973); Bull.Acad.Sci.USSR, Phys.Ser. 37, No.9, 84 (1974)
V.Y.Kostin, E.G.Kopanets, A.A.Koval, A.N.Lvov, V.Y.Migalenya, S.P.Tsytko
Isospin Structure of 32S Levels from the Radiative Proton Capture Reaction
NUCLEAR REACTIONS 31P(p, γ), E=1.8-2.7 MeV; measured Eγ, Iγ. 32S deduced levels, resonances, J, π, T, T-mixing, γ-branching.
Phys.Rev. C8, 178 (1973)
J.Vernotte, S.Gales, M.Langevin, J.M.Maison
Investigation of the Lowest T = 2 State of 32S in the 31P + p Reactions
NUCLEAR REACTIONS 31P(p, γ), (p, p'γ), (p, αγ), E=3.27-3.3 MeV; measured σ(Eγ), σ(E). 32S deduced resonances, T, J, π, γ-branching.
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.
Can.J.Phys. 52, 950 (1974)
H.Grawe, J.E.Cairns, M.W.Greene, J.A.Kuehner
An Investigation of Odd Parity States in 32S
NUCLEAR REACTIONS 31P(p, γ), E=0.8-2.0 MeV; 32,34S(α, α'), E=16-18 MeV; measured DSA, σ(θ), σ(Eα'), P(γ). 32S deduced levels, J, π, T1/2, γ-branching ratios, γ-mixing.
Z.Phys. 269, 173 (1974)
M.Viitasalo, I.Forsblom
An Investigation of Excited States in 32S by the 31P(p, γ)32S Reaction
NUCLEAR REACTIONS 31P(p, γ), E=300-1420 keV; measured σ(E, Eγ, θ); deduced Q. 32S deduced resonances, J, π, γ-branching ratios, γ-mixing.
Aust.J.Phys. 28, 383 (1975)
S.G.Boydell, D.G.Sargood
Accurate Branching Ratio Measurements in 31P(p, γ)32S
NUCLEAR REACTIONS 31P(p, γ), E=0.4-1.75 MeV; measured σ(E, Eγ). 32S resonances deduced γ-branching.
Aust.J.Phys. 28, 155 (1975)
R.O'Brien, Z.E.Switkowski, A.K.Smith, D.G.Sargood
Total Yield Measurements in 31P(p, γ)32S
NUCLEAR REACTIONS 31P(p, γ), E=0.33-1.75 MeV; measured σ(E, Eγ). 32S deduced resonances, Γ.
Phys.Rev. C13, 984 (1976)
J.Vernotte, J.M.Maison, A.Chevallier, A.Huck, C.Miehe, G.Walter
Electromagnetic Properties of the 6621- and 7950-keV Levels in 32S
NUCLEAR REACTIONS 31P(p, γ), E=1.25-1.58 MeV; measured Iγ(θ), DSA. 32S deduced resonances, J, π, T1/2, δ, γ-branching, transition strengths.
Izv.Akad.Nauk SSSR, Ser.Fiz. 41, 151 (1977); Bull.Acad.Sci.USSR, Phys.Ser. 41, No.1, 124 (1977)
V.Y.Kostin, E.G.Kopanets, A.A.Koval, A.N.Lvov, V.Y.Migalenya, S.P.Tsytko
Angular Distributions of γ-Rays from the 31P(p, γ)32S Reaction
NUCLEAR REACTIONS 31P(p, γ), E=1121, 1151, 1557, 1953 keV; measured σ(Eγ, θ). 32S deduced γ-branching, δ for transitions from IAS.
Phys.Rev. C17, 1550 (1978)
B.M.Paine, S.R.Kennett, D.G.Sargood
(p, γ) Resonance Strengths in the s-d Shell
NUCLEAR REACTIONS 23Na, 27Al, 31P, 35Cl(p, γ), E=0.5-0.9 MeV; measured σ(E, Eγ). 24Mg, 28Si, 32S, 36Ar deduced resonance strengths.
At.Data Nucl.Data Tables 23, 3 (1979)
P.M.Endt
Strengths of Gamma-Ray Transitions in A = 6-44 Nuclei (III)
COMPILATION A=6-44; compiled Eγ, B(λ), γ-mixing, γ-branching ratios, level T1/2.
doi: 10.1016/0092-640X(79)90020-2
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
Phys.Rev. C23, 1900 (1981)
R.Hentela
Analog of the 3.00-MeV State of 32P in 32S
NUCLEAR REACTIONS 31P(p, γ), E=1149.5-1151.5 keV; measured σ(E, Eγ), γ(θ). 32S levels deduced resonance strengths, transition strengths, γ-branching ratio, J, π, δ. Ge(Li) detectors, natural targets.
Nucl.Phys. A460, 181 (1986)
F.Zijderhand, C.van der Leun
Strong M2 Transitions
NUCLEAR REACTIONS, ICPND 13C(p, γ), E ≈ 1460 keV; 15N(p, γ), E ≈ 430, 900 keV; 20Ne(p, γ), E ≈ 380 keV; 31P(p, γ), E ≈ 1250 keV; measured σ(E, Eγ), γ yield vs E, σ(E). 14N, 16O, 21Na, 32S deduced resonance strengths, γ-branching ratios, B(M2), Γγ, Γp, Γα, Γ, T. Enriched, implanted targets.
doi: 10.1016/0375-9474(86)90123-5
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.
Nucl.Phys. A533, 153 (1991)
C.Iliadis, U.Giesen, J.Gorres, S.Graff, M.Wiescher, R.E.Azuma, J.King, M.Buckby, C.A.Barnes, T.R.Wang
The Reaction Branching 31P(p, γ)/31P(p, α) in the rp-Process
NUCLEAR REACTIONS, ICPND 31P(p, γ), E=0.28-0.62 MeV; 31P(p, α), E=0.28-0.45 MeV; measured σ(E), relative yield. 32S, 28Si deduced resonances, J, π, resonance strengths. Hauser-Feshbach calculations.
doi: 10.1016/0375-9474(91)90824-P
Nucl.Phys. A559, 83 (1993)
C.Iliadis, J.Gorres, J.G.Ross, K.W.Scheller, M.Wiescher, C.Grama, Th.Schange, H.P.Trautvetter, H.C.Evans
Explosive Hydrogen Burning of 31P
NUCLEAR REACTIONS, ICPND 31P(p, γ), (p, α), E=160-370 keV; 28Si(α, γ), E=2.4-2.6 MeV; measured γ yield vs E; deduced stellar reaction rates, temperature dependence. 32S deduced proton thershold state features.
doi: 10.1016/0375-9474(93)90181-V
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.Korean Phys.Soc. 37, 512 (2000)
T.K.Yang, S.T.Park, B.K.Seo, H.C.Kim, D.W.Lee, G.D.Kim, S.Y.Lee, M.Igashira
Lifetimes of Excited Levels in 32S from the Doppler Shift Attenuation Method
NUCLEAR REACTIONS 31P(p, γ), E=1.557, 1.583 MeV; measured Eγ, Iγ, DSA. 32S levels deduced T1/2.
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
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.