References quoted in the ENSDF dataset: 35AL ADOPTED LEVELS, GAMMAS
44 references found.
Clicking on a keynumber will list datasets that reference the given article.
Phys.Rev.Lett. 42, 40 (1979)
T.J.M.Symons, Y.P.Viyogi, G.D.Westfall, P.Doll, D.E.Greiner, H.Faraggi, P.J.Lindstrom, D.K.Scott, H.J.Crawford, C.McParland
Observation of New Neutron-Rich Isotopes by Fragmentation of 205-MeV/Nucleon 40Ar Ions
NUCLEAR REACTIONS 12C(40Ar, X), E=205 MeV/nucleon; measured σ; deduced production σ for 26,27,28,29,30Na. 30,31Na, 27,28Ne, 31,32,33Mg deduced evidence for particle stability.
doi: 10.1103/PhysRevLett.42.40
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 T1/2; deduced decay schemes. 17B; measured β-delayed 4n activity. 19C, 14Be; measured β-delayed neutron multiplicities. Projectile fragment isotopic separation.
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.722 (1988), AIP Conf.Proc. 164 (1987)
D.Bazin, R.Anne, D.Guerreau, D.Guillemaud-Mueller, A.C.Mueller, M.G.Saint-Laurent, W.D.Schmidt-Ott, V.Borrel, J.C.Jacmart, F.Pougheon, A.Richard
On the Production Mechanisms of Nuclei Far from Stability at GANIL Energies and Their Application to New β-Delayed Neutron Emitters
RADIOACTIVITY 15B, 18C, 19,20N, 34,35Al, 39P(β-n); measured T1/2, neutron emission probability. 17C, 36,37Si, 38P; measured neutron emission probability upper limit.
doi: 10.1063/1.36948
Program and Theses, Proc.38th Ann.Conf.Nucl.Spectrosc.Struct.At.Nuclei, Baku, p.177 (1988)
E.B.Balbutsev, J.Piperova
Giant Quadrupole and Monopole Resonances
NUCLEAR STRUCTURE A=40-240; calculated isovector, isoscalar GQR, GMR.
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
Z.Phys. A330, 63 (1988)
A.C.Mueller, D.Bazin, W.D.Schmidt-Ott, R.Anne, D.Guerreau, D.Guillemaud-Mueller, M.G.Saint-Laurent, V.Borrel, J.C.Jacmart, F.Pougheon, A.Richard
β-Delayed Neutron Emission of 15B, 18C, 19,20N, 34,35Al and 39P
RADIOACTIVITY 15B, 18C, 19,20N, 34,35Al, 39P(β-n) [from 181Ta(86Kr, X), E=45 MeV/nucleon]; measured T1/2, neutron emission probabilities.
Univ.Paris, Inst.Phys.Nucl., 1987 Ann.Rept., p.E7 (1988)
A.C.Mueller, D.Bazin, W.D.Schmidt-Ott, R.Anne, D.Guerreau, D.Guillemaud-Mueller, M.G.Saint-Laurent, V.Borrel, J.C.Jacmart, F.Pougheon, A.Richard
New Light Beta-Delayed Neutron Emitters
RADIOACTIVITY 18C, 20N, 35Al(β-n) [from Kr bombardment of Ta]; measured T1/2, neutron emission probability.
Nucl.Phys. A496, 477 (1989)
M.Lewitowicz, Yu.E.Penionzhkevich, A.G.Artukh, A.M.Kalinin, V.V.Kamanin, S.M.Lukyanov, Nguyen Hoai Chau, A.C.Mueller, D.Guillemaud-Mueller, R.Anne, D.Bazin, C.Detraz, D.Guerreau, M.G.Saint-Laurent, V.Borrel, J.C.Jacmart, F.Pougheon, A.Richard, W.D.Schmidt-Ott
β-Delayed Neutron Emission of the Isotopes 20C, 40,41,42P, 43,44S
RADIOACTIVITY 15,17B, 18,20C, 35Al, 40,41,42P, 43,44S [from 181Ta(48Ca, X)]; measured T1/2, delayed n emission probabilities.
doi: 10.1016/0375-9474(89)90072-9
Univ.Paris, Inst.Phys.Nucl., 1988 Ann.Rept., p.25 (1989)
A.C.Mueller, M.Lewitowicz, R.Anne, A.G.Artukh, D.Bazin, V.Borrel, C.Detraz, D.Guerreau, D.Guillemaud-Mueller, J.C.Jacmart, D.X.Jiang, A.M.Kalinin, V.V.Kamanin, S.M.Lukyanov, H.C.Nguyen, Yu.E.Penionzhkevich, F.Pougheon, A.Richard, M.G.Saint-Laurent, W.D.Schmidt-Ott
Etude de l'Emission de Neutrons Retardes par des Isotopes Legers tres Riches en Neutrons
RADIOACTIVITY 18,20C, 40,41,42P, 43,44S, 15,17B, 35Al(β-n) [from Ta(48Ca, X), E=55 MeV/nucleon]; measured T1/2, β-delayed neutron emission probabilities.
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
Phys.Lett. 260B, 285 (1991)
X.G.Zhou, X.L.Tu, J.M.Wouters, D.J.Vieira, K.E.G.Lobner, H.L.Seifert, Z.Y.Zhou, G.W.Butler
Direct Mass Measurements of the Neutron-Rich Isotopes of Fluorine Through Chlorine
NUCLEAR REACTIONS Th(p, X), E=800 MeV; measured fragment mass, charge state ratio, velocity histograms. 24,25,26,27F, 27,28,29Ne, 30,31,32Na, 30,31,32,33,34Mg, 33,34,35,36Al, 36,37,38Si, 38,39,40,41P, 40,41,42,43S, 41,42,43,44Cl deduced mass excess.
doi: 10.1016/0370-2693(91)91613-Z
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. C59, 642 (1999)
R.W.Ibbotson, T.Glasmacher, P.F.Mantica, H.Scheit
Coulomb Excitation of Odd-A Neutron-Rich π(s-d) and ν(f-p) Shell Nuclei
NUCLEAR REACTIONS 197Au(35Al, 35Al'), (37Si, 37Si'), (39P, 39P'), (41S, 41S'), (43S, 43S'), (45Cl, 45Cl'), E=42-47.4 MeV/nucleon; measured Eγ, Iγ following Coulomb excitation. 35Al, 37Si, 39P, 41,43S, 45Cl; deduced levels, J, π, excitation B(E2). Secondary beams from 48Ca fragmentation.
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, 32,33,34,35,36,37Mg, 34,35,36,37,38,39Al, 37,38,39,40,41,42Si, 41,42,43P(β-n) [from 9Be, 181Ta(48Ca, X), E=70 MeV/nucleon]; measured T1/2, β-delayed n emission probabilities. Projectile fragmentation separator.
Thesis, Michigan State University (2000)
B.V.Pritychenko
Intermediate-Energy Coulomb Excitation of the Neutron-Rich Radioactive Isotopes 26, 28Ne, 28-31Na, 30-34Mg, 34, 35Al, 33Si and 34P
NUCLEAR REACTIONS 197Au(26Ne, 26Ne'), (28Ne, 28Ne'), (30Mg, 30Mg'), (32Mg, 32Mg'), (34Mg, 34Mg'), (36Ar, 36Ar'), E ≈ 50 MeV/nucleon; 197Au(31Mg, 31Mg'), E=62.08 MeV/nucleon; 197Au(33Mg, 33Mg'), E=61.8 MeV/nucleon; 197Au(33Si, 33Si'), E=50.5 MeV/nucleon; 197Au(34P, 34P'), E=54.5 MeV/nucleon; 197Au(34Al, 34Al'), E=59.7 MeV/nucleon; 197Au(35Al, 35Al'), E=55.83 MeV/nucleon; 197Au(28Na, 28Na'), E=43.1 MeV/nucleon;197Au(29Na, 29Na'), E=59.97 MeV/nucleon; 197Au(30Na, 30Na'), E=55.6 MeV/nucleon; 197Au(31Na, 31Na'), E=58.9 MeV/nucleon; measured Eγ, Iγ, (particle)γ-coin following projectile Coulomb excitation. 26,28Ne, 30,32Mg, 36Ar, 197Au deduced levels energies, excitation B(E2), configurations. 28,29,30,31Na, 31,33Mg, 34,35Al, 33Si, 34P deduced excitation levels, σ. Secondary beams from 48Ca, 40Ar fragmentation, comparison with shell model, Nilsson diagrams and nuclear systematics for deformed 'island of inversion' nuclei.
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, 35Si by β Decay: sd-fp Shell gap and single-particle states
RADIOACTIVITY 34,35Al(β-) [from U(p, X)]; measured Eγ, Iγ, T1/2, 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
Nucl.Phys. A701, 410c (2002)
S.Nummela, P.Baumann, E.Caurier, S.Courtin, P.Dessagne, O.Holmlund, A.Jokinen, A.Knipper, G.Le Scornet, C.Mieh, F.Nowacki, L.G.Lyapin, M.Oinonen, E.Poirier, Z.Radivojevic, M.Ramdhane, W.H.Trzaska, G.Walter, J.Aysto, and the ISOLDE Collaboration
Study of the Neutron-Rich Nuclei with N = 21, 35Si and 33Mg, by Beta Decay of 35Al and 33Na
RADIOACTIVITY 35Al, 33Na(β-), (β-n); measured Eγ, Iγ, β-delayed neutron spectra, T1/2. 35Si, 33Mg deduced levels, J, π.
doi: 10.1016/S0375-9474(01)01619-0
Phys.Rev. C 67, 055802 (2003)
P.Moller, B.Pfeiffer, K.-L.Kratz
New calculations of gross b-decay properties for astrophysical applications: Speeding-up the classical r process
RADIOACTIVITY 92,99Rb, 137I(β-), (β-n); calculated strength functions, T1/2, delayed-neutron emission probabilities. Z=8-76; 76Fe, 77Co, 78Ni, 79Cu, 80Zn, 81Ga, 125Tc, 126Ru, 127Rh, 128Pd, 129Ag, 130Cd, 131In, 190Gd, 191Tb, 192Dy, 193Ho, 194Er, 195Tm, 196Yb; calculated β-decay T1/2. Implications for astrophysical r-process discussed.
doi: 10.1103/PhysRevC.67.055802
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
J.Phys.(London) G31, S1965 (2005)
C.Timis, J.C.Angelique, A.Buta, N.L.Achouri, D.Baiborodin, P.Baumann, C.Borcea, S.Courtin, P.Dessagne, Z.Dlouhy, J.M.Daugas, S.Grevy, D.Guillemaud-Mueller, A.Knipper, F.R.Lecolley, J.L.Lecouey, M.Lewitowicz, E.Lienard, S.M.Lukyanov, F.M.Marques, C.Miehe, J.Mrazek, F.Negoita, F.Nowacki, F.de Oliveira, N.A.Orr, J.Peter, S.Pietri, Yu.E.Penionzhkevich, E.Poirier, M.Stanoiu, G.Walter
Spectroscopy around N = 20 shell closure: β-n decay study of 35Al
RADIOACTIVITY 35Al(β-), (β-n) [from 36S fragmentation]; measured β-delayed Eγ, En, T1/2, neutron emission probability; deduced log ft. 34,35Si deduced levels, J, π, feeding intensities.
doi: 10.1088/0954-3899/31/10/111
Proc.Frontiers in Nuclear Structure, Astrophysics, and Reactions, Isle of Kos, Greece, 12-17 Sept. 2005, S.V Harissopulos, P.Demetriou, R.Julin, Eds., p. 134 (2006); AIP Conf.Proc. 831 (2006)
J.C.Angelique, C.Timis, S.Pietri, N.L.Achouri, P.Baumann, C.Borcea, A.Buta, W.Catford, S.Courtin, J.M.Daugas, P.Dessagne, F.De Oliveira, Z.Dlouhy, S.Grevy, D.Guillemaud-Mueller, R.Hadeler, A.Knipper, F.R.Lecolley, J.L.Lecouey, M.Lewitowicz, E.Lienard, C.Miehe, J.Mrazek, F.Negoita, F.Nowacki, N.A.Orr, Y.Penionzhkevich, J.Peter, E.Poirier, M.Stanoiu, O.Tarasov, G.Walter
Spectroscopy Near the N=20 Shell Closure: β-n Decay Studies of 33Mg and 35Al
RADIOACTIVITY 33Mg, 35Al(β-), (β-n) [from 36S fragmentation]; measured Eγ, En, βγ-, βn-coin; deduced log ft. 34,35Si, 32,33Al deduced levels, J, π.
doi: 10.1063/1.2200913
CNS-REP-69, p.19 (2006)
T.Fukui, S.Ota, S.Shimoura, N.Aoi, E.Takeshita, S.Takeuchi, H.Suzuki, H.Baba, T.Fukuchi, Y.Hashimoto, E.Ideguchi, K.Ieki, N.Iwasa, H.Iwasaki, S.Kanno, Y.Kondo, T.Kubo, K.Kurita, T.Minemura, S.Michimasa, T.Motobayashi, T.Murakami, T.Nakabayashi, T.Nakamura, M.Niikura, T.Okumura, T.K.Onishi, H.Sakurai, M.Shinohara, D.Suzuki, M.K.Suzuki, M.Tamaki, K.Tanaka, Y.Togano, Y.Wakabayashi, K.Yamada
High Resolution In-beam Gamma Spectroscopy of N ∼ 20 Neutron-rich Nuclei
NUCLEAR REACTIONS He(28Na, X), (29Na, X), (30Na, X), (31Na, X), (30Mg, X), (31Mg, X), (32Mg, X), (33Mg, X), (32Al, X), (33Al, X), (34Al, X), (35Al, X), (34Si, X), (35Si, X), (36Si, X), (36P, X), (37P, X), E ≈ 40 MeV/nucleon; measured Eγ, Iγ, (particle)γ-coin. 28,29,30,31Na, 30,31,32,33Mg, 32,33,34,35Al deduced transitions.
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.Lett. B 649, 43 (2007)
B.Jurado, H.Savjols, W.Mittig, N.A.Orr, P.Roussel-Chomaz, D.Baiborodin, W.N.Catford, M.Chartier, C.E.Demonchy, Z.Dlouhy, A.Gillibert, L.Giot, A.Khouaja, A.Lepine-Szily, S.Lukyanov, J.Mrazek, Y.E.Penionzhkevich, S.Pita, M.Rousseau, A.C.Villari
Mass measurements of neutron-rich nuclei near the N = 20 and 28 shell closures
ATOMIC MASSES 23N, 23,24O, 25,26,27F, 27,28,29,30,31Ne, 31,32,33Na, 34,35,36Mg, 34,35,36,37,38,39Al, 36,37,38,39,40,41,42Si, 40,41,42,43,44P, 40,43,44,45S, 43,45,46,47Cl; measured masses; analysed neutron separation energy. Cyclotron-based mass spectrometry.
doi: 10.1016/j.physletb.2007.04.006
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
Priv.Com. (2008)
P.L.Reeder
Phys.Rev. C 79, 054303 (2009)
K.Yoshida
Core polarization for the electric quadrupole moment of neutron-rich aluminum isotopes
NUCLEAR STRUCTURE 32,34,36Si, 32Mg; calculated B(E2), response functions for isoscalar, isovector, and proton quadrupole excitations. Microscopic particle-vibration coupling model with Skyrme HFB and QRPA equations. Implications for quadrupole moments of 31,33,35Al.
NUCLEAR MOMENTS 31,33,35Al; calculated polarization charges and electric quadrupole moments. Comparison with experimental data.
doi: 10.1103/PhysRevC.79.054303
Int.J.Mod.Phys. E20, 893 (2011)
M.Kimura
Systematic study of the many-particle and many-hole states in and around the island of inversion
NUCLEAR STRUCTURE 33,35Al, 32,34Mg, 30,32Ne, 33Mg; calculated single-particle energies and quadrupole deformation, 33Mg low-lying state energies, J, π. AMD calculations, comparison with experimental data.
doi: 10.1142/S0218301311018915
Phys.Rev. C 86, 014612 (2012)
E.Kwan, D.J.Morrissey, D.A.Davies, M.Steiner, C.S.Sumithrarachchi, L.Weissman
Systematic studies of light neutron-rich nuclei produced via the fragmentation of 40Ar
NUCLEAR REACTIONS 9Be, Ni, 181Ta(40Ar, X)10Be/11Be/12Be/12B/13B/14B/15B/14C/15C/16C/17C/18C/19C/16N/17N/18N/19N/20N/21N/22N/19O/20O/21O/22O/23O/24O/21F/22F/23F/24F/25F/26F/27F/24Ne/25Ne/26Ne/27Ne/28Ne/29Ne/30Ne/26Na/27Na/28Na/29Na/30Na/31Na/32Na/33Na/28Mg/29Mg/30Mg/31Mg/32Mg/33Mg/34Mg/35Mg/31Al/32Al/33Al/34Al/35Al/36Al/33Si/34Si/35Si/36Si/37Si/38Si/35P/36P/37P/38P, E=140 MeV/nucleon; measured fission fragment spectra by energy loss from time-of-flight measurements, average isobaric velocities, parallel momentum transfers, widths, fragment σ. Comparison with empirical formula EPAX, and predictions from internuclear cascade and deep inelastic models using Monte Carlo ISABEL-GEMINI and DIT-GEMINI computer codes.
doi: 10.1103/PhysRevC.86.014612
Phys.Rev. C 85, 024621 (2012)
X.H.Zhang, Z.Y.Sun, R.F.Chen, Z.Q.Chen, Z.Y.Guo, J.L.Han, Z.G.Hu, T.H.Huang, R.S.Mao, Z.G.Xu, M.Wang, J.S.Wang, Y.Wang, G.Q.Xiao, H.S.Xu, X.H.Yuan, H.B.Zhang, X.Y.Zhang, T.C.Zhao
Projectile fragmentation reactions of 40Ar at 57 MeV/nucleon
NUCLEAR REACTIONS 9Be(40Ar, X)17F/18F/19F/20F/21F/22F/23F/24F/25F/19Ne/20Ne/21Ne/22Ne/23Ne/24Ne/25Ne/26Ne/27Ne/21Na/22Na/23Na/24Na/25Na/26Na/27Na/28Na/29Na/30Na/22Mg/23Mg/24Mg/25Mg/26Mg/27Mg/28Mg/29Mg/30Mg/31Mg/32Mg/24Al/25Al/26Al/27Al/28Al/29Al/30Al/31Al/32Al/33Al/34Al/35Al/26Si/27Si/28Si/29Si/30Si/31Si/32Si/33Si/34Si/35Si/36Si/37Si/28P/29P/30P/31P/32P/33P/34P/35P/36P/37P/38P/39P/30S/31S/32S/33S/34S/35S/36S/37S/38S/39S/40S/32Cl/33Cl/34Cl/35Cl/36Cl/37Cl/38Cl/39Cl/40Cl/41Cl/34Ar/35Ar/36Ar/37Ar/38Ar/39Ar/40Ar/41Ar/41Ar/37K/38K/39K/40K/39Ca/40Ca/41Ca/42Ca, E=57 MeV/nucleon; 181Ta(40Ar, X)17F/18F/19F/20F/21F/22F/23F/24F/25F/19Ne/20Ne/21Ne/22Ne/23Ne/24Ne/25Ne/26Ne/27Ne, 21Na/22Na/23Na/24Na/25Na/26Na/27Na/28Na/29Na/30Na/23Mg/24Mg/25Mg/26Mg/27Mg/28Mg/29Mg/30Mg/31Mg/32Mg/25Al/26Al/27Al/28Al/29Al/30Al/31Al/32Al/33Al/34Al/, 27Si/28Si/29Si/30Si/31Si/32Si/33Si/34Si/35Si/36Si/29P/30P/31P/32P/33P/34P/35P/36P/37P/38P/31S/32S/33S/34S/35S/36S/37S/38S/39S/40S/33Cl/34Cl/35Cl/36Cl/37Cl/38Cl/39Cl/40Cl/35Ar/36Ar/37Ar/38Ar/39Ar/38K/39K/40K/40Ca/41Ca, E=57 MeV/nucleon; measured particle spectra, energy loss, time of flight, fragment yields, momentum distributions, cross sections; deduced fragment excitation energies, mass yield ratios. RIBLL, HIRFL facilities. Comparison with empirical parameterization of fragmentation cross section (EPAX), abrasion-ablation (AA) model, and heavy-ion phase-space exploration (HIPSE) model. Discussed target dependence of fragment cross sections.
doi: 10.1103/PhysRevC.85.024621
J.Phys.(London) G40, 105110 (2013)
H.Li, Z.Ren
Shell model calculations for the β--decays of Z = 9-13 nuclei
RADIOACTIVITY 27,29F, 28,29,30,31,32,33,34Ne, 29,30,31,32,33,34,35,36,37Na, 30,31,32,33,34,35,36,37,38,39,40Mg, 31,32,33,34,35,36,37,38,39,40,41,42,43Al(β-), (β-n); calculated T1/2, beta-delayed neutron emission probabilities, log ft, branching ratios. Shell model, WBMB interaction, comparison with available data.
doi: 10.1088/0954-3899/40/10/105110
Int.J.Mod.Phys. E22, 1350005 (2013)
M.K.Sharma, M.S.Mehta, S.K.Patra
Nuclear reaction cross-section for drip-line nuclei in the framework of Glauber model using relativistic and nonrelativistic densities
NUCLEAR STRUCTURE 12,19,20,21,22C, 21,22,23N, 20,21,22,23,24O, 23,24,25,26,27,28,29F, 28,29,30,31,32Ne, 27,28,29,30,31,32,33,34,35Na, 30,31,32,33,34,35,36,37,38,39,40,41,42Mg, 33,34,35,36,37,38,39,40,41,42,43,44Al; calculated binding energy, charge radii, deformation parameter. Relativistic mean field, Skyrme HF, comparison with available data.
doi: 10.1142/S0218301313500055
Phys.Rev. C 90, 014302 (2014)
E.Caurier, F.Nowacki, A.Poves
Merging of the islands of inversion at N = 20 and N = 28
NUCLEAR STRUCTURE 28O, 29F, 30Ne, 31Na, 32Mg, 33Al, 34Si, 35P, 36S, 37Cl, 38Ar; calculated correlation energies and gaps of the 0p-0h and 2p-2h configurations. 24,26,28,30,32,34,36,38,40,42,44Mg, 18,20,22,24,26,28,30,32,34,36,38,40,42Ne, 28,30,32,34,36,38,40,42,44,46Si; calculated energies and B(E2) of first 2+ states. 29,31F, 30,31,32Ne, 31,33Na, 30,31,32,33Mg, 35,35Al, 34Si; calculated low-lying levels, J, π, magnetic dipole moments. Nuclei near islands of inversion at N=20 and N=28, and their merging in Magnesium chain of nuclei. Large-scale shell-model calculations with the effective interaction SDPF-U-MIX. Comparison with experimental results.
doi: 10.1103/PhysRevC.90.014302
Eur.Phys.J. A 51, 38 (2015)
M.Bigdeli, S.Elyasi
LOCV approach and core-crust transition in neutron stars
doi: 10.1140/epja/i2015-15038-7
Phys.Rev. C 92, 024608 (2015)
S.Momota, I.Tanihata, A.Ozawa, M.Notani, K.Yoshida, K.Morimoto, T.Yamaguchi, T.Onishi, A.Yoshida, Y.X.Watanabe, Z.Liu, A.Ono
Velocity-dependent transverse momentum distribution of fragments produced from 40Ar+9Be at 95 MeV/nucleon
NUCLEAR REACTIONS 9Be(40Ar, X), E=95 MeV/nucleon; measured time-of-flight, energy loss and angular distribution of fragments using Rikagaku Kenkyusho (RIKEN) Projectile Fragment Separator at RIKEN. 10,11,12Be, 11,12,13,14,15B, 13,14,15,16,17,18C, 14,15,16,17,18,19,20,21N, 17,18,19,20,21,22,23,24O, 19,20,21,22,23,24,25,26F, 21,22,23,24,25,26,27,28,29Ne, 24,25,26,27,28,29,30,31Na, 26,27,28,29,30,31,32,33,34Mg, 28,29,30,31,32,33,34,35,36Al, 30,31,32,33,34,35,36,37Si; analyzed transverse momentum distributions for fragments; deduced formulation for the width of transverse momentum distribution. Comparison with antisymmetrized molecular-dynamics model calculations to investigate reaction mechanism.
doi: 10.1103/PhysRevC.92.024608
Phys.Rev. C 93, 025805 (2016)
T.Marketin, L.Huther, G.Martinez-Pinedo
Large-scale evaluation of β-decay rates of r-process nuclei with the inclusion of first-forbidden transitions
RADIOACTIVITY Z=8-110, N=11-236, A=19-339(β-); calculated decay rates for Gamow-Teller and first-forbidden transitions, total decay rates, P0n, P1n, P3n, P4n, P5n delayed-neutron emission probabilities, average energies of electrons antineutrinos and photons after decay. Z=47-48, A=114-154; calculated Q(β-). Z=36-43, A=93-117; Z=37-50, N=65-88; Z=24-32, N=50; Z=42-49, N=82; Z=6-73, N=126; 194,195,196Re, 199,200Os, 198,199,201,202Ir, 203,204Pt, 204Au, 211,212,213Tl, 218,219Bi(β-); calculated half-lives for β- decay. Fully self-consistent covariant density functional theory (CDFT) framework with the ground states calculated with relativistic Hartree-Bogoliubov (RHB) model, and excited states within the proton-neutron relativistic quasiparticle random phase approximation (pn-RQRPA). Comparison with experimental Q values and half-lives. Calculated abundances of heavy nuclei, and evolution of neutron-to-seed ratio resulting from hot and cold r-processes using half-lives from the FRDM and the current model. Supplementary file contains theoretical values of half-lives and Pxn for 5409 neutron-rich nuclei.
doi: 10.1103/PhysRevC.93.025805
Phys.Rev. C 94, 044311 (2016)
F.Sammarruca, Y.Nosyk
Impact of the neutron matter equation of state on neutron skins and neutron drip lines in chiral effective field theory
NUCLEAR STRUCTURE 20,21,22,23,24,25,26,27,28,29,30,31O, 28,29,30,31,32,33,34,35,36,37,38,39,40,41,42,43,44,45Mg, 32,33,34,35,36,37,38,39,40,41,42,43,44,45,46,47,48,49Al; calculated binding energies and neutron skins for neutron-rich isotopes. Microscopic equations of state for neutron matter obtained at LO, NLO, N2LO and N3LO orders of chiral EFT, with phenomenological model for the EoS of symmetric nuclear matter. Comparison with available experimental values.
doi: 10.1103/PhysRevC.94.044311
Chin.Phys.C 41, 030001 (2017)
G.Audi, F.G.Kondev, M.Wang, W.J.Huang, S.Naimi
The NUBASE2016 evaluation of nuclear properties
COMPILATION A=1-295; compiled, evaluated nuclear structure and decay data.
doi: 10.1088/1674-1137/41/3/030001
Phys.Rev. C 96, 034301 (2017)
S.Chakraborty, U.Datta, T.Aumann, S.Beceiro Novo, K.Boretzky, C.Caesar, B.V.Carlson, W.N.Catford, M.Chartier, D.Cortina-Gil, G.De Angelis, P.Diaz Fernandez, H.Emling, O.Ershova, L.M.Fraile, H.Geissel, D.Gonzalez-Diaz, H.Johansson, B.Jonson, N.Kalantar-Nayestanaki, T.Kroll, R.Krucken, C.Langer, T.Le Bleis, Y.Leifels, J.Marganiec, G.Munzenberg, M.A.Najafi, T.Nilsson, C.Nociforo, V.Panin, R.Plag, A.Rahaman, R.Reifarth, M.V.Ricciardi, C.Rigollet, D.Rossi, C.Scheidenberger, H.Scheit, H.Simon, J.T.Taylor, Y.Togano, S.Typel, Y.Utsuno, A.Wagner, F.Wamers, H.Weick, J.S.Winfield
Ground-state configuration of neutron-rich 35Al via Coulomb breakup
NUCLEAR REACTIONS C, Pb(35Al, 34Al), E=403 MeV/nucleon, [secondary 35Al beam from fragmentation of 531 MeV/nucleon 40Ar primary beam followed by separation of reaction products using FRS separator at GSI]; measured four-momenta of the projectile, fragments, and other decay products such as fragments, neutrons, and γ rays after secondary reaction using Large Area Neutron Detector for neutrons and Crystal Ball array of NaI(Tl) detectors for γ detection at GSI; deduced inclusive differential Coulomb dissociation (CD) cross section of 35Al breaking up into a neutron and 34Al fragment in its ground state and isomer. 34Al; deduced levels, Coulomb dissociation σ, spectroscopic factors. 35Al; deduced J, π, configurations, spectroscopic factor for the ground state.
doi: 10.1103/PhysRevC.96.034301
Phys.Rev. C 96, 024325 (2017)
A.T.Gallant, M.Alanssari, J.C.Bale, C.Andreoiu, B.R.Barquest, U.Chowdhury, J.Even, A.Finlay, D.Frekers, G.Gwinner, R.Klawitter, B.Kootte, A.A.Kwiatkowski, D.Lascar, K.G.Leach, E.Leistenschneider, A.Lennarz, A.J.Mayer, D.Short, R.Thompson, M.Wieser, D.Lunney, J.Dilling
Mass determination near N=20 for Al and Na isotopes
ATOMIC MASSES 31,32Na, 29,34,35Al; measured cyclotron frequencies and mass excesses by time-of-flight ion-cyclotron-resonance (TOF-ICR) technique using the TITAN Penning trap mass spectrometer at ISAC-TRIUMF; deduced S(2n). Radioactive isotopes produced via the isotope separator on-line (ISOL) technique by a 480-MeV proton beam impinging on a UCx target, followed by the separation of sodium isotopes by surface ionization, and aluminum isotopes by the TRIUMF Resonant Ionization Laser Ion Source (TRILIS). Comparison with previous experimental values and mass evaluations. Systematics of S(2n) values for N=18-25 Na, Mg, and Al isotopic chains.
doi: 10.1103/PhysRevC.96.024325
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
Chin.Phys.C 41, 030003 (2017)
M.Wang, G.Audi, F.G.Kondev, W.J.Huang, S.Naimi, X.Xu
The AME2016 atomic mass evaluation (II). Tables, graphs and references
ATOMIC MASSES A=1-295; compiled, evaluated atomic masses data.
doi: 10.1088/1674-1137/41/3/030003