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

32 references found.

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

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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, ^{29,30,31,32,33}Al, ^{31,32,33,34,35,36}Si, ^{33,34,35,36,37,38}P, ^{36,37,38,39,40}S, ^{37,38,39,40,41,42}Cl, ^{39,40,41,42,43,44}Ar.

doi: 10.1016/0375-9474(71)90270-3

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.

1986DU07

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 T_1/2. 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.

1986FI06

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

1986HUZW

CENBG-8605 (1986)

F.Hubert, J.P.Dufour, R.del Moral, H.Emmermann, D.Jean, C.Poinot, M.S.Pravikoff, A.Fleury, H.Delagrange, H.Geissel, K.-H.Schmidt

Studies of New Radioactive Nuclei at GANIL Energies

NUCLEAR REACTIONS Be(⁴⁰Ar, X), E=60 MeV/nucleon; measured βγ-coin for fragment decay for X=¹⁷C to ⁴⁰S.

RADIOACTIVITY ⁴⁰S, ^38,37P, ^36,35Si, ³⁴Al, ²⁶Ne, ²⁴F, ¹⁹N [from Be(⁴⁰Ar, X), E=60 MeV/nucleon]; measured βγ-coin, T_1/2.

1986SM05

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.

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 T_1/2. ^40,41Cl, ^38,39S, ^36,37P, ^35,36Si; calculated levels. Shell model.

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

1987DUZU

Contrib.Proc. 5th Int.Conf.Nuclei Far from Stability, Rosseau Lake, Canada, D1 (1987)

J.P.Dufour, R.Del Moral, F.Hubert, D.Jean, M.S.Pravikoff, A.Fleury, H.Delagrange, A.Mueller, K.-H.Schmidt, E.Hanelt, K.Summerer

Spectroscopic Measurements with a New Method: The projectile-fragments isotopic separation

RADIOACTIVITY ⁴⁰S, ^36,37,38P, ^35,36,37Si, ^32,34,35Al, ²⁶Ne, ²⁴F, ²²O, ^19,20N, ¹⁷C; measured T_1/2; deduced decay schemes. ¹⁷B; measured β-delayed 4n activity. ¹⁹C, ¹⁴Be; measured β-delayed neutron multiplicities. Projectile fragment isotopic separation.

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 T_1/2, 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

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, T_1/2, 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, T_1/2 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

1994MO37

Nuovo Cim. 107A, 1565 (1994)

G.Mouze

On Some Properties of the Valence Bosons

NUCLEAR STRUCTURE ^16,22O, ^22,28,34Si, ⁴⁰Ca; calculated proton, neutron pairing energies. ^{23,25,27,29,31,33,35,37}Si, ^{42,44,46,48,41,43,45,47,49}Ca; calculated from-core detachment energies variations; deduced valence bosons characteristics.

1994PO05

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

1995REZZ

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 T_1/2 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 T_1/2. ^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.

1997FO01

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, T_1/2. ³²Al deduced levels, possible J, π.

doi: 10.1103/PhysRevC.55.762

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, ^{32,33,34,35,36}Si, ^{34,35,36,37,38,39}P, ^{36,37,38,39,40,41}S, ^{39,40,41,42,43,44}Cl, ^{41,42,43,44,45,46}Ar, ^{44,45,46,47,48}K, ^{46,47,48,49,50}Ca, ^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, ^{27,29,33,35,41,43}Si, ^33,41Al, ^35,43P, ^{55,57,67,69,77,79}Ni, ^67,77Co, ^69,79Cu, ^79,81,89,91Zr, ⁸⁹Y, ⁹¹Nb, ^{99,101,131,133}Sn, 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

1999YOZW

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, ^{32,33,34,35,36,37}Mg, ^{34,35,36,37,38,39}Al, ^{37,38,39,40,41,42}Si, ^41,42,43P(β^-n) [from ⁹Be, ¹⁸¹Ta(⁴⁸Ca, X), E=70 MeV/nucleon]; measured T_1/2, β-delayed n emission probabilities. Projectile fragmentation separator.

2001NU01

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, 35}Si by β Decay: sd-fp Shell gap and single-particle states

RADIOACTIVITY ^34,35Al(β^-) [from U(p, X)]; measured Eγ, Iγ, T_1/2, 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

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 ^{28,29,30,31,32}Ne, ^{29,30,31,32,33,34}Na, ^{30,31,32,33,34,35}Mg, ^{31,32,33,34,35,36}Al, ^{32,33,34,35,36,37}Si, ^{33,34,35,36,37,38}P, ^{34,35,36,37,38,39}S, ^{35,36,37,38,39,40}Cl, ^{36,37,38,39,40,41}Ar; calculated binding energies. Weak-coupling model, comparison with data.

doi: 10.1140/epja/i2004-10021-1

2006KH08

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. ^{17,18,19,20,21,22}N, ^{19,20,21,22,23,24}O, ^{21,22,23,24,25,26,27}F, ^{23,24,25,26,27,28,29,30}Ne, ^{26,27,28,29,30,31,32,33}Na, ^{28,29,30,31,32,33,34,35}Mg, ^{31,32,33,34,35,36,37,38}Al, ^{33,34,35,36,37,38,39,40}Si, ^{36,37,38,39,40,41,42}P, ^{39,40,41,42,43,44}S, ^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

2006RO34

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

2007CH82

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

2007NE14

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

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

2008KI07

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

2008WI11

Phys.Rev. C 78, 054311 (2008)

M.T.Win, K.Hagino

Deformation of Λ hypernuclei

NUCLEAR STRUCTURE ¹²C, ^{18,20,22,24,26,28,30,32,34,36,38}Ne, ^{22,24,26,28,30,32,34,36,38,40,42}Si; calculated quadrupole deformation parameter, potential surfaces. ¹³C, ^{19,21,23,25,27,29,31,33,35,37,39}Ne, ^{23,25,27,29,31,33,35,37,39,41,43}Si; calculated quadrupole deformation parameter, potential surfaces for hypernuclei. Relativistic Mean Field model.

doi: 10.1103/PhysRevC.78.054311

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. ^{36,38,40,42,44}Si, ^34,36,38,40Mg; calculated B(E2), quadrupole moments, energy of 2⁺ state. ^{39,41,43,45,47,49,51}K, ^{35,37,39,41,43,45,47}P, ^{37,39,41,43,45,47,49}Cl; 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

2011KA03

Phys.Rev. C 83, 014320 (2011)

K.Kaneko, Y.Sun, T.Mizusaki, M.Hasegawa

Shell-model study for neutron-rich sd-shell nuclei

NUCLEAR STRUCTURE ³⁵Si, ^{36,37,38,40,42,43,44,46}S, ^{38,39,40,42,43,44,45,46,47,48}Ar, ^41,49Ca, ⁴⁷K; calculated levels, J, π. ⁴⁰Mg, ^{34,36,38,40,42,44,46,48,50,52}Si, ^{36,38,40,42,44,46,48,50,52,54}S, ^{38,40,42,44,46,48,50,52,54,56}Ar, ^{40,42,44,46,48,50,52,54,56,58}Ca; calculated energies of first 2+ states. Z=20, N=20-40; calculated effective proton single-particle energies. Z=8-20, N=20; calculated effective neutron single-particle energies. ^36,38,40,42Si, ^{36,38,40,42,44}S, ^{38,40,42,44,46}Ar; calculated B(E2) values for first 2+ states. ⁴⁰Mg, ⁴²Si, ⁴⁴S, ^44,46Ar, ⁴⁸Ca; calculated spectroscopic quadrupole moments of first 2+ states. ^{35,37,39,41,43}P, ^{37,39,41,43,45}Cl, ^{39,41,43,45,47,49}K; calculated 3/2+ to 1/2+ splittings. ⁴¹Si, ⁴³S, ⁴⁵Ar, ⁴⁷Ca; calculated 7/2- to 3/2- splittings. Spherical shell model in the sd-pf valence space with the extended pairing plus quadrupole-quadrupole forces accompanied by the monopole interaction (EPQQM). Comparison with experimental data for sd-shell nuclei.

doi: 10.1103/PhysRevC.83.014320

2012IM01

Phys.Rev. C 85, 034313 (2012)

N.Imai, Y.Hirayama, Y.X.Watanabe, T.Teranishi, T.Hashimoto, S.Hayakawa, Y.Ichikawa, H.Ishiyama, S.C.Jeong, D.Kahl, S.Kubono, H.Miyatake, H.Ueno, H.Yamaguchi, K.Yoneda, A.Yoshimi

Isobaric analog resonances of the N=21 nucleus ³⁵Si

NUCLEAR REACTIONS ¹H(³⁴Si, p), [secondary ³⁴Si from fragmentation of 63 MeV/nucleon ⁴⁰Ar beam], E=5 MeV/nucleon; measured particle spectra, energy loss, cross sections of the proton elastic scattering at E(p)(cm)=2.5-5.5 MeV. ³⁵P; deduced resonances, proton widths, total widths, spectroscopic factors; IAR of ³⁵Si states. R-matrix analysis. ³⁵Si; deduced levels, J, π from IAR assignment. Thick target inverse kinematics (TTIK) experiments at RIKEN facility. Comparison of ³⁵Si levels with those in N=21 nuclei of ³³Mg, ³⁷S, ³⁹Ar, ⁴¹Ca. Comparison with previous studies.

doi: 10.1103/PhysRevC.85.034313

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.

2014ST18

Phys.Rev. C 90, 034301 (2014)

S.R.Stroberg, A.Gade, J.A.Tostevin, V.M.Bader, T.Baugher, D.Bazin, J.S.Berryman, B.A.Brown, C.M.Campbell, K.W.Kemper, C.Langer, E.Lunderberg, A.Lemasson, S.Noji, F.Recchia, C.Walz, D.Weisshaar, S.J.Williams

Single-particle structure of silicon isotopes approaching ⁴²Si

NUCLEAR REACTIONS ⁹Be(³⁶Si, ³⁵Si), (³⁶Si, ³⁵Al), E=97.7 MeV/nucleon; ⁹Be(³⁸Si, ³⁷Si), (³⁸Si, ³⁷Al), E=86 MeV/nucleon; ⁹Be(⁴⁰Si, ³⁹Si), (⁴⁰Si, ³⁹Al), E=79 MeV/nucleon, [secondary beams of ^36,38,40Si produced in ⁹Be(⁴⁸Ca, X), E=140 MeV/nucleon primary reaction]; measured Doppler-shifted γ-ray spectra, Eγ, Iγ, γγ-, (residue)γ-coin, (³⁶Si)γ-coin using GRETINA array for γ detection and ionization chamber and plastic scintillators in the focal plane of S800 spectrograph at NSCL-MSU facility. ^35,37,39Al, ^35,37,39Si; deduced levels, J, π, parallel momentum distributions, l-values. ^36,38,40Si; one-neutron and one-proton total and partial knockout σ, single-particle structure, and enhanced collectivity in the region of ⁴²Si. Eikonal model analysis of parallel momentum distributions. Comparison with large-scale shell model calculations.

NUCLEAR STRUCTURE ^35,37,39Al, ^35,37,39Si; calculated levels, J, π using large-scale shell model with SDPF-U and SDPF-MU interactions. Comparison with experimental data.

doi: 10.1103/PhysRevC.90.034301

2014STZZ

REPT INDC(NDS)-0658 (2014)

N.J.Stone

Table of nuclear magnetic dipole and electric quadrupole moments

COMPILATION Z=0-99; A=1-254; compiled μ, electric quadrupole moments, J, π, T_1/2, experimental methods.