References quoted in the ENSDF dataset: 35P ADOPTED LEVELS, GAMMAS

26 references found.

Clicking on a keynumber will list datasets that reference the given article.


1971AR32

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


1971GR53

Z.Naturforsch. 26a, 1933 (1971)

W.Grimm, W.Herzog

Phosphor-35 - ein neues Nuklik

RADIOACTIVITY 35P; measured T1/2, Eγ.


1972AP01

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.

doi: 10.1103/PhysRevC.6.842


1972GO31

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.

doi: 10.1103/PhysRevC.6.820


1975JEZX

REPT LBL-4000, P93

ATOMIC MASSES 8,9,10He, 10,11,12Li, 12,13,14Be, 14,15,16B, 17,18C, 19,20N, 21,22,23O, 23,24F, 25,26Ne, 26,27,28,29,30,31,32,33Na, 29,30Mg, 31,32Al, 33,34Si, 35,36P, 39,40S, 41,42Cl; calculated mass excess, proton, neutron binding energy.


1983WI08

Phys.Rev. C28, 1343 (1983)

B.H.Wildenthal, M.S.Curtin, B.A.Brown

Predicted Features of the Beta Decay of Neutron-Rich sd-Shell Nuclei

RADIOACTIVITY 21,22,23,24,25,26,27,28O, 23,24,25,26,27,28,29F, 25,26,27,28,29,30Ne, 27,28,29,30,31Na, 29,30,31,32Mg, 31,32,33Al, 33,34Si, 35P(β-); calculated Q, T1/2, log ft, Gamow-Teller transition strength, branching to daughter residual states. Shell model.

doi: 10.1103/PhysRevC.28.1343


1984MA49

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.


1985DR06

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


1985KH04

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


1986WO02

Nucl.Phys. A451, 413 (1986)

C.L.Woods

Shell-Model Calculations for Neutron-Rich Nuclei with A = 35-41

NUCLEAR STRUCTURE 36,37S, 35P, 38Ar; calculated levels, single nucleon transfer spectroscopic factors. 39Ar; calculated levels, single nucleon spectroscopic factors, δ. 41,40Ar, 38,37Cl; calculated levels, single nucleon spectroscopic factors, average T1/2. 40,41Cl, 38,39S, 36,37P, 35,36Si; calculated levels. Shell model.

doi: 10.1016/0375-9474(86)90068-0


1987WA10

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.

doi: 10.1103/PhysRevC.35.1851


1988DUZS

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.


1988DUZT

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


1988OR01

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


1988WA04

Phys.Rev. C37, 754 (1988)

E.K.Warburton, J.A.Becker

Shell-Model Description of the β- Decay of the N = 21 and 22 Isotones 34Al, 36Si, and 37P

NUCLEAR STRUCTURE 34Al, 34,35,36Si, 35,36,37P, 37S; calculated levels, branching ratios, log ft, B(λ), β-decay T1/2. Shell model.

doi: 10.1103/PhysRevC.37.754


1997VO03

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.

doi: 10.1103/PhysRevC.55.2458


1999AI02

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


1999DU05

Phys.Rev. C59, R2347 (1999)

J.Duflo, A.P.Zuker

The Nuclear Monopole Hamiltonian

NUCLEAR STRUCTURE 39,41,47,49Ca, 47K, 49Sc, 15,17,21,23O, 21N, 23F, 27,29,33,35,41,43Si, 33,41Al, 35,43P, 55,57,67,69,77,79Ni, 67,77Co, 69,79Cu, 79,81,89,91Zr, 89Y, 91Nb, 99,101,131,133Sn, 131In, 133Sb, 207Tl, 207,209Pb, 209Bi; calculated single-particle orbits. 12,14C, 16,22,28O, 18,34,42Si, 40,48Ca, 56,68,78Ni, 80,90Zr, 100,132Sn, 208Pb; calculated shell gaps. Monopole Hamiltonian.

doi: 10.1103/PhysRevC.59.R2347


2003AU03

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


2003SM02

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


2004KH16

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


2007HO08

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


2007NO13

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


2009NO01

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


2011AUZZ

Priv.Comm. (2011)

G.Audi, W.Meng

Atomic Mass Evaluation 2011


2012WA38

Chin.Phys.C 36, 1603 (2012)

M.Wang, G.Audi, A.H.Wapstra, F.G.Kondev, M.MacCormick, X.Xu, B.Pfeiffer

The AME2012 atomic mass evaluation (II). Tables, graphs and references

COMPILATION A=1-295; compiled, evaluated atomic mass data.