References quoted in the ENSDF dataset: 32AL ADOPTED LEVELS, GAMMAS
37 references found.
Clicking on a keynumber will list datasets that reference the given article.
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
Phys.Rev.Lett. 49, 455 (1982)
M.J.Murphy, T.J.M.Symons, G.D.Westfall, H.J.Crawford
Beta-Decay Half-Lives of Isotopes Produced in Projectile Fragmentation
RADIOACTIVITY 22O, 25Ne, 27,28Na, 29,30Mg, 31,32Al [from 9Be(40Ar, X), E=11.4 GeV]; measured β-decay T1/2.
NUCLEAR REACTIONS 9Be(40Ar, X)22O/25Ne/27Na/28Na/29Mg/30Mg/31Al/32Al, E=11.4 GeV; measured σ(fragment) vs mass, Z; deduced projectile fragmentation evidence.
doi: 10.1103/PhysRevLett.49.455
Nucl.Phys. A426, 37 (1984)
D.Guillemaud-Mueller, C.Detraz, M.Langevin, F.Naulin, M.De Saint-Simon, C.Thibault, F.Touchard, M.Epherre
β-Decay Schemes of very Neutron-Rich Sodium Isotopes and Their Descendants
RADIOACTIVITY 27,28,29,30,31,32,33,34Na, 29,30,31,32,33Mg, 32Al(β-) [from In(p, X), E=10 GeV]; measured Eγ, Iγ, βγγ-coin; deduced Iβ, log ft. 27,28,29,30,31,32Mg, 29,30,31Al, 32S deduced levels, γ-branching. 29,30,31,32Mg, 31Al deduced neutron emission probabilities.
doi: 10.1016/0375-9474(84)90064-2
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 T1/2. 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.
Phys.Rev.Lett. 57, 3253 (1986)
D.J.Vieira, J.M.Wouters, K.Vaziri, R.H.Kraus, Jr., H.Wollnik, G.W.Butler, F.K.Wohn, A.H.Wapstra
Direct Mass Measurements of Neutron-Rich Light Nuclei near N = 20
NUCLEAR REACTIONS 232Th(p, X), E=800 MeV; measured fragment mass to charge spectra. 19C, 20,21N, 23O, 23,24,25,26F, 27,28Ne, 28,29,30Na, 30,31,32Mg, 32,33,34Al, 36Si, 37P deduced mass excess, two-neutron separation energy vs neutron number. Recoil spectrometer.
doi: 10.1103/PhysRevLett.57.3253
Phys.Lett. 192B, 39 (1987)
A.Gillibert, W.Mittig, L.Bianchi, A.Cunsolo, B.Fernandez, A.Foti, J.Gastebois, C.Gregoire, Y.Schutz, C.Stephan
New Mass Measurements Far From Stability
NUCLEAR REACTIONS Ta(40Ar, X), E=60 MeV/nucleon; measured fragment rigidity, tof. 17B, 19,20C, 20,21,22N, 23,24O, 24,25,26F, 27,28Ne, 30,31,32Na, 31,32,33Mg, 32,33,34,35Al, 36,37Si, 37,38P deduced mass excess.
doi: 10.1016/0370-2693(87)91138-5
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
Phys.Lett. 258B, 29 (1991)
N.A.Orr, W.Mittig, L.K.Fifield, M.Lewitowicz, E.Plagnol, Y.Schutz, Z.W.Long, L.Bianchi, A.Gillibert, A.V.Belozyorov, S.M.Lukyanov, Yu.E.Penionzhkevich, A.C.C.Villari, A.Cunsolo, A.Foti, G.Audi, C.Stephan, L.Tassan-Got
New Mass Measurements of Neutron-Rich Nuclei Near N = 20
NUCLEAR REACTIONS Ta(48Ca, X), E=55 MeV/nucleon; measured projectile like fragment spectra. 17,19B, 20C, 20,21,22N, 22,23,24O, 24,25,26,27F, 26,27,28,29,30Ne, 28,29,30,31,32,33Na, 30,31,32,33,34,35Mg, 32,33,34,35,36,37Al, 36,37Si, 37P deduced mass excess.
doi: 10.1016/0370-2693(91)91203-8
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
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 T1/2 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 T1/2. 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.
Phys.Rev. C53, R1465 (1996)
M.Robinson, P.Halse, W.Trinder, R.Anne, C.Borcea, M.Lewitowicz, S.Lukyanov, M.Mirea, Yu.Oganessian, N.A.Orr, Yu.Penionzhkevich, M.G.Saint-Laurent, O.Tarasov
New Isomer 32mAl
NUCLEAR REACTIONS 9Be(36S, X), E=75 MeV/nucleon; 9Be(40Ar, X), E=61 MeV/nucleon; measured (fragment)γ-coin, fragment mass distribution, γγ-coin; deduced evidence for 32mAl. 32Al deduced isomer T1/2, J, π, decay characteristics. Shell model comparison.
doi: 10.1103/PhysRevC.53.R1465
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, T1/2. 32Al deduced levels, possible J, π.
RIKEN-96, p.50 (1997)
H.Iwasaki, N.Aoi, D.Beaumel, N.Fukuda, M.Hirai, E.Ideguchi, M.Ishihara, T.Kishida, T.Kubo, H.Kumagai, S.M.Lukyanov, T.Nakamura, M.Notani, Y.T.Oganessian, Y.E.Penionzhkevich, H.Sakurai, T.Teranishi, Ya.Watanabe, Yu.Watanabe, K.Yoneda, A.Yoshida
Isomer Production in Fragmentation Reactions Induced by a 70A MeV 48Ca Beam
NUCLEAR REACTIONS 64Ni, 181Ta(48Ca, X), E=70 MeV/nucleon; measured (fragment)γ-coin. 26mNa, 32mAl deduced T1/2, isomer ratios. Projectile fragmentation technique.
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
Nucl.Phys. A734, 369 (2004)
S.Grevy, S.Pietri, L.Achouri, J.C.Angelique, P.Baumann, C.Borcea, A.Buta, W.Catford, S.Courtin, J.M.Daugas, F.De Oliveira, P.Dessagne, Z.Dlouhy, D.Guillemaud-Mueller, R.Hadeler, A.Knipper, F.R.Lecolley, J.L.Lecouey, M.Lewitowicz, E.Lienard, C.Miehe, J.Mrazek, F.Negoita, N.A.Orr, Y.Penionzhkevich, J.Peter, E.Poirier, M.Stanoiu, O.Tarasov, C.Timis, G.Walter
Spectroscopy at the N = 20 shell closure: the β-decay of 32Mg
RADIOACTIVITY 32Mg(β-), (β-n) [from Be(36S, X)]; measured Eγ, Iγ, γγ-coin, T1/2, β-delayed neutron spectra; deduced neutron emission probability. 32Al deduced levels, J, π, β-feeding intensities.
doi: 10.1016/j.nuclphysa.2004.01.068
Phys.Lett. B 615, 186 (2005)
H.Ueno, D.Kameda, G.Kijima, K.Asahi, A.Yoshimi, H.Miyoshi, K.Shimada, G.Kato, D.Nagae, S.Emori, T.Haseyama, H.Watanabe, M.Tsukui
Magnetic moments of 3013Al17 and 3213Al19
RADIOACTIVITY 30,32Al(β-) [from 40Ar fragmentation]; measured β-NMR spectra, T1/2; deduced μ.
NUCLEAR MOMENTS 30,32Al; measured β-NMR spectra; deduced μ.
doi: 10.1016/j.physletb.2005.04.037
Phys.Lett. B 643, 257 (2006)
P.Himpe, G.Neyens, D.L.Balabanski, G.Belier, D.Borremans, J.M.Daugas, F.de Oliveira Santos, M.De Rydt, K.Flanagan, G.Georgiev, M.Kowalska, S.Mallion, I.Matea, P.Morel, Yu.E.Penionzhkevich, N.A.Smirnova, C.Stodel, K.Turzo, N.Vermeulen, D.Yordanov
g factors of 31, 32, 33Al: Indication for intruder configurations in the 33Al ground state
NUCLEAR MOMENTS 31,32,33Al [from 9Be(36S, X), E=77.5 MeV/nucleon]; measured J, π of ground states, magnetic moments, hyperfine structure using laser and β-NMR spectroscopy; deduced g factors, magnetic dipole moments. Compared with shell-model calculations.
doi: 10.1016/j.physletb.2006.10.26
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. 17,18,19,20,21,22N, 19,20,21,22,23,24O, 21,22,23,24,25,26,27F, 23,24,25,26,27,28,29,30Ne, 26,27,28,29,30,31,32,33Na, 28,29,30,31,32,33,34,35Mg, 31,32,33,34,35,36,37,38Al, 33,34,35,36,37,38,39,40Si, 36,37,38,39,40,41,42P, 39,40,41,42,43,44S, 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
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
Phys.Lett. B 647, 93 (2007)
D.Kameda, H.Ueno, K.Asahi, M.Takemura, A.Yoshimi, T.Haseyama, M.Uchida, K.Shimada, D.Nagae, G.Kijima, T.Arai, K.Takase, S.Suda, T.Inoue, J.Murata, H.Kawamura, Y.Kobayashi, H.Watanabe, M.Ishihara
Measurement of the electric quadrupole moment of 32Al
RADIOACTIVITY 32Al(β-) [from 40Ar fragmentation]; measured β-NMR spectra. 32Al deduced quadrupole moment.
doi: 10.1016/j.physletb.2007.01.063
Hyperfine Interactions 180, 61 (2007)
D.Kameda, H.Ueno, K.Asahi, D.Nagae, M.Takemura, K.Shimada, A.Yoshimi, T.Nagatomo, T.Sugimoto, M.Uchida, T.Arai, K.Takase, S.Suda, T.Inoue, J.Murata, H.Kawamura, H.Watanabe, Y.Kobayashi, M.Ishihara
Electric quadrupole moments of neutron-rich nuclei 32Al and 31Al
NUCLEAR MOMENTS 32,31Al(β-); measured ground state electric quadrupole moments using the β-NQR method.
doi: 10.1007/s10751-008-9685-x
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
RIKEN Accelerator Progress Report 2006, p.13 (2007)
K.Takase, D.Kameda, H.Ueno, Y.Kobayashi, A.Yoshimi, T.Sugimoto, T.Nagatomo, K.Shimada, D.Nagae, M.Takemura, T.Inoue, T.Arai, M.Uchida, H.Watanabe, K.Asahi
Test experiment on 32mAl isomeric moment
RADIOACTIVITY 32Al(β-); measured isomer decay, Eγ, Iγ, γγ-coin. using time differential perturbed angular distribution method; deduced T1/2, g-factor.
Eur.Phys.J. Special Topics 150, 185 (2007)
H.Ueno, D.Kameda, D.Nagae, M.Takemura, K.Asahi, K.Shimada, K.Takase, T.Sugimoto, T.Nagatomo, M.Uchida, T.Arai, T.Inoue, A.Yoshimi, T.Kawamura, K.Narita
Nuclear moments of neutron-rich aluminum isotopes
RADIOACTIVITY 30,31,32Al(β-); measured magnetic dipole and electric quadrupole moments using the β-NMR method.
doi: 10.1140/epjst/e2007-00299-y
Phys.Rev. C 77, 034305 (2008)
T.A.Hinners, V.Tripathi, S.L.Tabor, A.Volya, P.C.Bender, C.R.Hoffman, S.Lee, M.Perry, P.F.Mantica, A.D.Davies, S.N.Liddick, W.F.Mueller, A.Stolz, B.E.Tomlin
Complementary studies of T = 2 30Al and the systematics of intruder states
RADIOACTIVITY 30Mg(β-), (β-n), (2β-) [from 9Be(48Ca, X), E=140 MeV/nucleon]; measured Eγ, Iγ, βγ-coin, βγγ-coin, half-lives. 30Al; deduced levels, J, π.
NUCLEAR REACTIONS 18O(14C, np), E=22 MeV; measured Eγ, Iγ, (particle)γ-coin, γ(θ). 30Al; deduced levels, J, π, comparison with shell-model calculations. 26Na, 28,32Al, 30,32,34P; systematics.
doi: 10.1103/PhysRevC.77.034305
RIKEN Accelerator Progress Report 2007, p.17 (2008)
D.Kameda, K.Takase, H.Ueno, A.Yoshimi, T.Nagatomo, Y.Hasama, H.Watanabe, M.Uchida, N.Hatakeyama, T.Inoue, S.Kagami, K.Suzuki, C.Nakano, H.Kawamura, T.Toyoda, K.Narita, J.Murata, D.Nagae, K.Shimada, K.Asahi
g-Factor measurement of the isomeric state of 32Al
RADIOACTIVITY 32Al; measured Eγ, Iγ from spin aligned 32Al; deduced isomer decay ratio, T1/2. Time differential perturbed angular distribution method.
Priv.Com. (2008)
P.L.Reeder
Phys.Rev. C 92, 061301 (2015)
A.A.Kwiatkowski, C.Andreoiu, J.C.Bale, A.Chaudhuri, U.Chowdhury, S.Malbrunot-Ettenauer, A.T.Gallant, A.Grossheim, G.Gwinner, A.Lennarz, T.D.Macdonald, T.J.M.Rauch, B.E.Schultz, S.Seeraji, M.C.Simon, V.V.Simon, D.Lunney, A.Poves, J.Dilling
Observation of a crossover of S2n in the island of inversion from precision mass spectrometry
ATOMIC MASSES 27,29,30,31,32,33,34Al; measured TOF-ICR resonance, mass excess using Ion Trap for Atomic and Nuclear science (TITAN) Penning-trap facility at TRIUMF. Comparison with AME-2012, and previous experimental values. Systematics of S(2n) values for 28,29,30,31,32,33,34,35,36,37Mg, 29,30,31,32,33,34,35,36,37,38Al, comparison of experimental and theoretical values; deduced crossover at N=21 in the island of inversion. Large-scale shell-model calculations.
doi: 10.1103/PhysRevC.92.061301
Phys.Lett. B 772, 529 (2017)
R.Han, X.Q.Li, W.G.Jiang, Z.H.Li, H.Hua, S.Q.Zhang, C.X.Yuan, D.X.Jiang, Y.L.Ye, J.Li, Z.H.Li, F.R.Xu, Q.B.Chen, J.Meng, J.S.Wang, C.Xu, Y.L.Sun, C.G.Wang, H.Y.Wu, C.Y.Niu, C.G.Li, C.He, W.Jiang, P.J.Li, H.L.Zang, J.Feng, S.D.Chen, Q.Liu, X.C.Chen, H.S.Xu, Z.G.Hu, Y.Y.Yang, P.Ma, J.B.Ma, S.L.Jin, Z.Bai, M.R.Huang, Y.J.Zhou, W.H.Ma, Y.Li, X.H.Zhou, Y.H.Zhang, G.Q.Xiao, W.L.Zhan
Northern boundary of the "island of inversion" and triaxiality in 34Si
RADIOACTIVITY 34Al(β-) [from 9Be(40Ar, X), E=69.2 MeV/nucleon]; measured decay products, Eγ, Iγ; deduced γ-ray energies, J, π, isomer T1/2. Comparison with shell model calculations using Gogny D1S and SDPF-M interactions.
RADIOACTIVITY 27,28Ne, 28,29,30,31Na, 30,31,32,33Mg, 32,33,34,35Al, 36,37Si(β-); measured decay products; deduced T1/2. Comparison with ENSDF values.
doi: 10.1016/j.physletb.2017.07.007
Phys.Rev. C 96, 024316 (2017)
A.Saxena, P.C.Srivastava
First-principles results for electromagnetic properties of sd shell nuclei
NUCLEAR MOMENTS 17,18,19,20O, 17,18,19,20,21,22F, 19,20,21,22,23,25Ne, 20,21,22,23,25,26,27,28,29,30,31Na, 21,23,24,25,26,27,29,31Mg, 23,24,25,26,27,28,30,31,32,33Al, 27,28,29,30,33Si, 28,29,31,32P, 31,32S; calculated magnetic-dipole and electric quadrupole moments for ground states, occupancies of d3/2, d5/2, and s1/2 proton and neutron orbitals. 28Na, 25Mg, 27,28,32Al, 27,29,30Si, 28,29,31P, 32,33S; calculated dominant configuration of the wave functions. First-principles ab initio shell-model calculations using valence-space Hamiltonians derived with in-medium similarity renormalization group (IM-SRG) and the coupled-cluster effective interaction (CCEI) approaches. Comparison with experimental values, and with results from the phenomenological USDB effective interaction.
doi: 10.1103/PhysRevC.96.024316
Can.J.Phys. 96, 774 (2018)
M.Bouhelal, N.Saidane, S.Belaid, F.Haas
Shell model description of the O+ and O- excited states in sd shell nuclei
NUCLEAR STRUCTURE 16,18,20,22O, 18,20,22,24F, 20,22,24,26Ne, 22,24,26,28Na, 24,26,28,30Mg, 26,28,30,32Al, 28,30,32,34Si, 30,32,34P, 32,34,36S, 34,36Cl, 36,38Ar, 38K, 40Ca; calculated O+ and O- excited states. Shell model calculations using the PSDPF interaction, comparison with available data.
Phys.Lett. B 782, 619 (2018)
Z.Y.Xu, H.Heylen, K.Asahi, F.Boulay, J.M.Daugas, R.P.de Groote, W.Gins, O.Kamalou, A.Koszorus, M.Lykiardopoulou, T.J.Mertzimekis, G.Neyens, H.Nishibata, T.Otsuka, R.Orset, A.Poves, T.Sato, C.Stodel, J.C.Thomas, N.Tsunoda, Y.Utsuno, M.Vandebrouck, X.F.Yang
Nuclear moments of the low-lying isomeric 1+ state of 34Al: Investigation on the neutron 1p1h excitation across N=20 in the island of inversion
NUCLEAR MOMENTS 32,34Al; measured transition frequencies using β-NMR/NQR techniques; deduced nuclear g factor and quadrupole moments. Comparison with large-scale shell-model calculations using several effective interactions.
doi: 10.1016/j.physletb.2018.06.009
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 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
Phys.Rev. C 103, 014318 (2021)
H.Heylen, C.S.Devlin, W.Gins, M.L.Bissell, K.Blaum, B.Cheal, L.Filippin, R.F.Garcia Ruiz, M.Godefroid, C.Gorges, J.D.Holt, A.Kanellakopoulos, S.Kaufmann, A.Koszorus, K.Konig, S.Malbrunot-Ettenauer, T.Miyagi, R.Neugart, G.Neyens, W.Nortershauser, R.Sanchez, F.Sommer, L.V.RodrIguez, L.Xie, Z.Y.Xu, X.F.Yang, D.T.Yordanov
High-resolution laser spectroscopy of 27-32Al
NUCLEAR MOMENTS 27,28,29,30,31,32Al; measured hyperfine structure spectra of the 3s23p2P3/20 to 3s24s2S1/2 atomic transition using collinear laser spectroscopy at the COLLAPS-ISOLDE-CERN facility; deduced hyperfine parameters, magnetic dipole moments and spectroscopic quadrupole moments with reference to those for 27Al, isotope shifts and mean-square charge radii relative to 27Al. Comparison with theoretical calculations using ab initio valence space in-medium similarity renormalization group method (VS-IMSRG) with multiple sets of two- and three-nucleon forces from chiral effective field theory, and with previous available experimental results. Neutral atoms of 27,28,29,30,31,32Al produced in U(p, X), E=1.4-GeV, using uranium carbide target, followed by extraction from the target, ionized by a resonance ionization laser ion source (RILIS), accelerated to 30 keV, and finally mass separated.
doi: 10.1103/PhysRevC.103.014318
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.