References quoted in the ENSDF dataset: 35MG ADOPTED LEVELS, GAMMAS
40 references found.
Clicking on a keynumber will list datasets that reference the given article.
Z.Phys. A332, 189 (1989)
D.Guillemaud-Mueller, Yu.E.Penionzhkevich, R.Anne, A.G.Artukh, D.Bazin, V.Borrel, C.Detraz, D.Guerreau, B.A.Gvozdev, J.C.Jacmart, D.X.Jiang, A.M.Kalinin, V.V.Kamanin, V.B.Kutner, M.Lewitowicz, S.M.Lukyanov, A.C.Mueller, Nguyen Hoai Chau, F.Pougheon, A.Richard, M.G.Saint-Laurent, W.D.Schmidt-Ott
Observation of New Neutron Rich Nuclei 26F, 35,36Mg, 38,39Al, 40,41Si, 43,44P, 45-47S, 46-49Cl, and 49-51Ar from the Interactions of 55 MeV/u 48Ca + Ta
NUCLEAR REACTIONS Ta(48Ca, X), E=55 MeV/nucleon; measured fragment spectra; deduced evidence for 29F, 35,36Mg, 38,39Al, 40,41Si, 43,44P, 45,46,47S, 46,47,48,49Cl, 49,50,51Ar.
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. 273B, 13 (1991)
S.K.Patra, C.R.Praharaj
Relativistic Mean Field Study of ' Island of Inversion ' in Neutron-Rich Ne, Na, Mg Nuclei
NUCLEAR STRUCTURE N=18-24; Z=10-20; calculated binding energies. Compared with data, other models. 26,27,28,29,30,31,32,33,34,35Ne, 29,30,31,32,33,34,35Na, 30,31,32,34,35,36Mg; calculated binding energy. Relativistic mean field model.
doi: 10.1016/0370-2693(91)90545-2
Pramana 37, L445 (1991)
S.K.Patra, C.R.Praharaj
Deformed Relativistic Mean Field Study of Binding Energy Anomaly in Neutron-Rich Ne, Na, Mg Nuclei
NUCLEAR STRUCTURE 29,30,31,32,33,34,35Ne, 29,30,31,32,33,34,35Na, 30,31,32,33,34,35,36Mg; calculated binding energy. 29Na; calculated nucleon single particle energies; deduced level J. 31Na; deduced level J. Relativistic mean field model.
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.Lett. 380B, 241 (1996)
Z.Ren, Z.Y.Zhu, Y.H.Cai, G.Xu
Relativistic Mean-Field Study of Mg Isotopes
NUCLEAR STRUCTURE 20,21,22,23,24,25,26,27,28,29,30,31,32,33,34,35,36,37,38,39,40Mg; calculated binding energy, nucleon matter radii, deformation, quadrupole moments.
doi: 10.1016/0370-2693(96)00462-5
At.Data Nucl.Data Tables 66, 131 (1997)
P.Moller, J.R.Nix, K.-L.Kratz
Nuclear Properties for Astrophysical and Radioactive-Ion-Beam Applications
NUCLEAR STRUCTURE Z=8-136; A=16-339; calculated, compiled total binding energy, one-, two-neutron, proton separation energies, pairing gaps, odd-nucleon parity, spin projection. Folded-Yukawa single particle potential, Lipkin-Nogami approximation.
RADIOACTIVITY Z=8-136; A=16-339; calculated, compiled β-, α-decay Q, T1/2. Folded-Yukawa single particle potential, Lipkin-Nogami approximation.
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.
Phys.Rev.Lett. 84, 5062 (2000)
F.Sarazin, H.Savajols, W.Mittig, F.Nowacki, N.A.Orr, Z.Ren, P.Roussel-Chomaz, G.Auger, D.Baiborodin, A.V.Belozyorov, C.Borcea, E.Caurier, Z.Dlouhy, A.Gillibert, A.S.Lalleman, M.Lewitowicz, S.M.Lukyanov, F.De Oliveira, Y.E.Penionzhkevich, D.Ridikas, H.Sakurai, O.Tarasov, A.de Vismes
Shape Coexistence and the N = 28 Shell Closure Far from Stability
ATOMIC MASSES 29,30Ne, 32,33Na, 34,35,36Mg, 36,37,38,39Al, 38,39,40,41Si, 38,39,40,41,42,43P, 40,41,42,43,44,45S, 43,44,45,46Cl, 47Ar; measured masses, two-neutron separation energies; deduced shell and deformation effects. Time-of-flight technique. Comparison with model predictions.
RADIOACTIVITY 43S(IT) [from 48Ca fragmentation]; measured Eγ, Iγ, T1/2. Comparison with shell model.
doi: 10.1103/PhysRevLett.84.5062
Hyperfine Interactions 132, 147 (2001)
F.Sarazin, H.Savajols, W.Mittig, F.Nowacki, N.A.Orr, Z.Ren, P.Roussel-Chomaz, G.Auger, D.Baiborodin, A.V.Belozyorov, C.Borcea, E.Caurier, Z.Dlouhy, A.Gillibert, A.S.Lalleman, M.Lewitowicz, S.M.Lukyanov, F.de Oliveira, Y.E.Penionzhkevich, D.Ridikas, O.Tarasov, H.Sakurai, A.De Vismes
Shape Coexistence and the N = 28 Shell Closure Far from Stability
ATOMIC MASSES 29,30Ne, 32,33Na, 34,35,36Mg, 36,37,38,39Al, 38,39,40,41Si, 38,39,40,41,42,43P, 40,41,42,43,44,45S, 43,44,45,46Cl; measured masses, two-neutron separation energies; deduced shell effects. Time of flight method.
RADIOACTIVITY 43S(IT); measured Eγ, T1/2. Comparison with shell model prediction.
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
Chinese Physics 14, 2444 (2005)
J.-G.Chen, X.-Z.Cai, T.-T.Wang, Yu.-G.Ma, Z.-Z.Ren, D.-Q.Fang, C.Zhong, Yi.-B.Wei, W.Guo, X.-F.Zhou, K.Wang, G.-L.Ma, W.-D.Tian, J.-H.Chen, T.-Z.Yan, J.-X.Zuo, C.-W.Ma, W.-Q.Shen
Investigation on the deformation of Ne and Mg isotope chains within relativistic mean-field model
NUCLEAR STRUCTURE 18,19,20,21,22,23,24,25,26,27,28,29,30,31,32,33,34,35,36Ne, 20,21,22,23,24,25,26,27,28,29,30,31,32,33,34,35,36,37,38,39,40,41,42,43,44Mg; calculated deformations, binding energies, shape coexistence features. Relativistic mean-field model, comparison with data.
doi: 10.1088/1009-1963/14/12/013
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 638, 166 (2006)
Q.Zhi, Z.Ren
Systematic calculations on the ground state properties of Mg isotopes by the macroscopic-microscopic model
NUCLEAR STRUCTURE 20,21,22,23,24,25,26,27,28,29,30,31,32,33,34,35,36,37,38,39,40Mg; calculated binding energies, deformation parameters, B(E2), single- and two-neutron separation energies, quadrupole moments. Macroscopic-microscopic model, isospin-dependent Nilsson potential, comparison with data.
doi: 10.1016/j.physletb.2006.05.057
Phys.Rev. C 76, 054319 (2007)
I.Hamamoto
Nilsson diagrams for light neutron-rich nuclei with weakly-bound neutrons
NUCLEAR STRUCTURE 15,17,19C, 31,33,35,37Mg; calculated one-particle bound and resonant level energies. Deduced Nilsson diagrams using Woods-Saxon potential.
doi: 10.1103/PhysRevC.76.054319
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, 041302 (2007)
M.B.Tsang, W.G.Lynch, W.A.Friedman, M.Mocko, Z.Y.Sun, N.Aoi, J.M.Cook, F.Delaunay, M.A.Famiano, H.Hui, N.Imai, H.Iwasaki, T.Motobayashi, M.Niikura, T.Onishi, A.M.Rogers, H.Sakurai, H.Suzuki, E.Takeshita, S.Takeuchi, M.S.Wallace
Fragmentation cross sections and binding energies of neutron-rich nuclei
NUCLEAR REACTIONS 9Be(86Kr, X)69Cu/71Cu/73Cu/75Cu/76Cu/77Cu/78Cu/79Cu, E=64 MeV/A; analyzed cross sections, binding energies. 9Be, 181Ta(48Ca, X)23Na/24Na/25Na/26Na/27Na/28Na/29Na/30Na/31Na/26Mg/27Mg/28Mg/29Mg/30Mg/31Mg/32Mg/33Mg/34Mg/35Mg, E=140 MeV/nucleon; analyzed cross sections.
doi: 10.1103/PhysRevC.76.041302
Priv.Com. (2008)
P.L.Reeder
RIKEN Accelerator Progress Report 2010, p.17 (2011)
N.Fukuda, T.Kubo, T.Ohnishi, N.Inabe, H.Takeda, D.Kameda
Production cross sections of neutron-rich isotopes produced by the fragmentation of a 48Ca beam at 345 MeV/nucleon
NUCLEAR REACTIONS 9Be(48Ca, X), E=345 MeV/nucleon; measured thick target fragmentation. 19,20,22C, 22,24O, 21,23,26,28,29,30,31,32Ne, 25,27,29,32,33,34,35,36,37,38Mg, 34,41Al, 39,40Si, 41,42Si, 40,42,44S deduced production σ. Compared with EPAX-2.15 systematics.
Phys.Rev. C 83, 044305 (2011)
A.Gade, D.Bazin, B.A.Brown, C.M.Campbell, J.M.Cook, S.Ettenauer, T.Glasmacher, K.W.Kemper, S.McDaniel, A.Obertelli, T.Otsuka, A.Ratkiewicz, J.R.Terry, Y.Utsuno, D.Weisshaar
In-beam γ -ray spectroscopy of 35Mg and 33Na
NUCLEAR REACTIONS 9Be(38Si, X)33Na/35Mg/36Mg/38Si, E=83 MeV/nucleon, [secondary 38Si beam from 9Be(48Ca, X), E=140 MeV/nucleon primary reaction]; measured Eγ, production σ, (33Na)γ-, (35Mg)γ-coin using SeGA array. 33Na, 35Mg; deduced levels, J, π, rotational band in 33Na. Comparison with large-scale Monte-Carlo shell model (MCSM) calculations with SDPF-M interaction, and with large-scale shell-model calculations with SDPF-U interaction. Calculated composition of 35Mg wave functions, quadrupole moments and B(E2) values. Systematics of S(n) for A=30-35 Mg nuclei. Relevance to Island of Inversion.
doi: 10.1103/PhysRevC.83.044305
Phys.Rev. C 83, 021302 (2011)
R.Kanungo, A.Prochazka, W.Horiuchi, C.Nociforo, T.Aumann, D.Boutin, D.Cortina-Gil, B.Davids, M.Diakaki, F.Farinon, H.Geissel, R.Gernhauser, J.Gerl, R.Janik, B.Jonson, B.Kindler, R.Knobel, R.Krucken, M.Lantz, H.Lenske, Y.Litvinov, B.Lommel, K.Mahata, P.Maierbeck, A.Musumarra, T.Nilsson, C.Perro, C.Scheidenberger, B.Sitar, P.Strmen, B.Sun, Y.Suzuki, I.Szarka, I.Tanihata, Y.Utsuno, H.Weick, M.Winkler
Matter radii of 32-35Mg
NUCLEAR REACTIONS C, H(32Mg, X), (33Mg, X)(34Mg, X)(35Mg, X), E=900 MeV/nucleon, [secondary Mg beams from Be(48Ca, X) primary reaction]; measured interaction cross sections by detecting unreacted Mg particles by Bρ-ΔE-TOF method. 32,33,34,35Mg; deduced matter radii by Glauber model analysis. Comparison with HF and RMF predictions. Neutron skin thickness.
doi: 10.1103/PhysRevC.83.021302
Phys.Rev. C 86, 064322 (2012)
H.T.Fortune, R.Sherr
Matter radii of 29-35Mg
NUCLEAR STRUCTURE 29,30,31,32,33,34,35Mg; calculated matter radii for ground states for different configurations. Comparison with experimental data.
doi: 10.1103/PhysRevC.86.064322
Phys.Rev. C 86, 024614 (2012)
W.Horiuchi, T.Inakura, T.Nakatsukasa, Y.Suzuki
Glauber-model analysis of total reaction cross sections for Ne, Mg, Si, and S isotopes with Skyrme-Hartree-Fock densities
NUCLEAR REACTIONS 12C(17Ne, X), (18Ne, X), (19Ne, X), (20Ne, X), (21Ne, X), (22Ne, X), (23Ne, X), (24Ne, X), (25Ne, X), (26Ne, X), (27Ne, X), (28Ne, X), (29Ne, X), (30Ne, X), (31Ne, X), (32Ne, X), (33Ne, X), (34Ne, X), (20Mg, X), (21Mg, X), (22Mg, X), (23Mg, X), (24Mg, X), (25Mg, X), (26Mg, X), (27Mg, X), (28Mg, X), (29Mg, X), (30Mg, X), (31Mg, X), (32Mg, X), (33Mg, X), (34Mg, X), (35Mg, X), (36Mg, X), (37Mg, X), (38Mg, X), (24Si, X), (25Si, X), (26Si, X), (27Si, X), (28Si, X), (29Si, X), (30Si, X), (31Si, X), (32Si, X), (33Si, X), (34Si, X), (35Si, X), (36Si, X), (37Si, X), (38Si, X), (39Si, X), (40Si, X), (41Si, X), (42Si, X), (43Si, X), (44Si, X), (45Si, X), (46Si, X), (26S, X), (27S, X), (28S, X), (29S, X), (30S, X), (31S, X), (32S, X), (33S, X), (34S, X), (35S, X), (36S, X), (37S, X), (38S, X), (39S, X), (40S, X), (41S, X), (42S, X), (43S, X), (44S, X), (45S, X), (46S, X), (47S, X), (48S, X), (49S, X), (50S, X), E=240 MeV/nucleon; 12C(13O, X), (14O, X), (15O, X), (16O, X), (17O, X), (18O, X), (19O, X), (20O, X), (21O, X), (22O, X), (23O, X), (24O, X), (17Ne, X), (18Ne, X), (19Ne, X), (20Ne, X), (21Ne, X), (22Ne, X), (23Ne, X), (24Ne, X), (25Ne, X), (26Ne, X), (27Ne, X), (28Ne, X), (29Ne, X), (30Ne, X), (31Ne, X), (32Ne, X), (33Ne, X), (34Ne, X), (20Mg, X), (21Mg, X), (22Mg, X), (23Mg, X), (24Mg, X), (25Mg, X), (26Mg, X), (27Mg, X), (28Mg, X), (29Mg, X), (30Mg, X), (31Mg, X), (32Mg, X), (33Mg, X), (34Mg, X), (35Mg, X), (36Mg, X), (37Mg, X), (38Mg, X), E=1000 MeV/nucleon; calculated total reaction σ. Glauber model for high-energy nucleus-nucleus collisions with SkM* interaction. Comparison with experimental data. Role of nuclear deformation in determining the matter radius.
NUCLEAR STRUCTURE 20,21,22,23,24,25,26,27,28,29,30,31,32,33,34Ne, 22,23,24,25,26,27,28,29,30,31,32,33,34,35,36,37,38Mg, 24,25,26,27,28,29,30,31,32,33,34,35,36,37,38,39,40,41,42,43,44,45,46Si, 26,27,28,29,30,31,32,33,34,35,36,37,38,39,40,41,42,43,44,45,46,47,48,49,50S; calculated point matter, neutron and proton radii, neutron Fermi energy for Ne isotopes, quadrupole deformation parameter. Skyrme-Hartree-Fock calculation SkM* and SLy4 interactions.
doi: 10.1103/PhysRevC.86.024614
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
Nucl.Phys. A913, 116 (2013)
R.Chatterjee, R.Shyam, K.Tsushima, A.W.Thomas
Structure and Coulomb dissociation of 23O within the quark-meson coupling model
NUCLEAR REACTIONS Pb(23O, n22O), E=422 MeV/nucleon; calculated Coulomb dissociation σ(E), longitudinal momentum distribution using QMC (quark-meson coupling) model. Compared with available data.
NUCLEAR STRUCTURE 23N, 23O, 31Ne, 35Mg, 37Na, 45S, 49Ar; calculated valence neutron separation energy, 23O density distribution, neutron, proton radii using QMC (quark-meson coupling) model. Compared with available data.
doi: 10.1016/j.nuclphysa.2013.06.004
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
Fakultat fur Physik der Technischen Universitat Munchen (2013)
K.Steiger
Decay spectroscopy of neutron-rich nuclei around 37Al
RADIOACTIVITY 29F, 30Ne, 31,35Na, 35,36Mg, 37,38Al(β-)[from 9Be(48Ca, X), E=345 MeV/nucleon]; measured Eγ, Iγ, γγ-coin, (implants)βγ-correlations, half-lives, isotopic yields, using BigRIPS and ZeroDegree spectrometer at RIBF-RIKEN facility. 30Na, 37,38Si; deduced levels, J, π, β feedings, logft. Nuclei near "island of inversion". Comparison with shell-model calculations.
Phys.Rev. C 89, 064301 (2014)
M.K.Gaidarov, P.Sarriguren, A.N.Antonov, E.Moya de Guerra
Ground-state properties and symmetry energy of neutron-rich and neutron-deficient Mg isotopes
NUCLEAR STRUCTURE 20,21,22,23,24,25,26,27,28,29,30,31,32,33,34,35,36Mg; calculated potential energy curves, proton and neutron charge density distributions for even-even nuclei, nuclear symmetry energy, quadrupole deformation as function of mass, S(2n), proton, neutron, charge, and matter rms radii, neutron skin thickness, isotope shifts, charge radii in A=27-32 Mg isotopes in island of inversion. Self-consistent deformed Skyrme-Hartree-Fock plus BCS method. Comparison with experimental data.
doi: 10.1103/PhysRevC.89.064301
Phys.Rev. C 89, 044610 (2014)
S.Watanabe, K.Minomo, M.Shimada, S.Tagami, M.Kimura, M.Takechi, M.Fukuda, D.Nishimura, T.Suzuki, T.Matsumoto, Y.R.Shimizu, M.Yahiro
Ground-state properties of neutron-rich Mg isotopes
NUCLEAR REACTIONS 12C(24Mg, X), (25Mg, X), (26Mg, X), (27Mg, X), (28Mg, X), (29Mg, X), (30Mg, X), (31Mg, X), (32Mg, X), (33Mg, X), (34Mg, X), (35Mg, X), (36Mg, X), (37Mg, X), (38Mg, X), E=240 MeV/nucleon; calculated reaction σ; deduced rms matter radii from reaction cross sections. Antisymmetrized molecular dynamics (AMD) with folding model and deformed Woods-Saxon model. Comparison with experimental data, and with other theoretical calculations.
NUCLEAR STRUCTURE 24,25,26,27,28,29,30,31,32,33,34,35,36,37,38,39,40Mg; calculated ground state binding J, π, S(n), S(2n) for 40Mg, β and γ deformation parameters, proton, neutron and matter radii, neutron skin thickness. 37Mg; calculated levels, J, π, neutron single-particle energies. Antisymmetrized molecular dynamics (AMD) with folding model and deformed Woods-Saxon model. Comparison with experimental data.
doi: 10.1103/PhysRevC.89.044610
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
Chin.Phys.C 39, 064102 (2015)
M.K.Sharma, R.N.Panda, M.K.Sharma, S.K.Patra
Nuclear structure study of some bubble nuclei in the light mass region using mean field formalism
NUCLEAR STRUCTURE 9,10,11,12Be, 12,13,14,15B, 12,13,14,15,16,17,18,19,20C, 20,21,22,23N, 20,21,22,23,24O, 23,24,25,26,27F, 28,29,30,31,32Ne, 32,33,34,35Mg, 32,33,34,35Si, 34,35,36,37S, 34,36,38,40,42,44,46,48Ar; calculated binding energy, charge radius. RMF(NL3) and HF(SEI-I) formalisms.
doi: 10.1088/1674-1137/39/6/064102
Chin.Phys.C 40, 114101 (2016)
H.-B.Bai, Z.-H.Zhang, X.-W.Li
Investigation of the Mg isotopes using the shell-model-like approach in relativistic mean field theory
NUCLEAR STRUCTURE 19,20,21,22,23,24,25,26,27,28,29,30,31,32,33,34,35,36,37,38,39,40Mg; calculated binding energies, radii and quadrupole deformations. Comparison with available data.
doi: 10.1088/1674-1137/40/11/114101
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
Phys.Rev. C 93, 014322 (2016)
M.K.Sharma, R.N.Panda, M.K.Sharma, S.K.Patra
Search for halo structure in 37Mg using the Glauber model and microscopic relativistic mean-field densities
NUCLEAR STRUCTURE 24,25,26,27,28,29,30,31,32,33,34,35,36,37,38,39,40Mg; calculated binding energies, charge radii, density profiles as function of radial distance. 35,36,37,38,39,40Mg; comparison of RMF densities with spherical equivalent densities. Relativistic mean field formalism (RMF) formalism. Comparison with experimental data.
NUCLEAR REACTIONS 12C(24Mg, X), (25Mg, X), (26Mg, X), (27Mg, X), (28Mg, X), (29Mg, X), (30Mg, X), (31Mg, X), (32Mg, X), (33Mg, X), (34Mg, X), (35Mg, X), (36Mg, X), (37Mg, X), (38Mg, X), (39Mg, X), (40Mg, X), E=240 MeV/nucleon; calculated reaction σ, σ(θ) for 34,35,36,37,38Mg projectiles. 12C(37Mg, X), E=30-1000 MeV/nucleon; calculated rms radius and reaction cross section as a function of diffuseness parameter, one neutron removal cross sections including total, elastic and inelastic parts. 12C(37Mg, 36Mg), E=240 MeV/nucleon; calculated longitudinal momentum distribution. Glauber model in conjunction with densities from relativistic mean field formalism. Comparison with experimental data.
doi: 10.1103/PhysRevC.93.014322
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, 034328 (2017)
S.Momiyama, P.Doornenbal, H.Scheit, S.Takeuchi, M.Niikura, N.Aoi, K.Li, M.Matsushita, D.Steppenbeck, H.Wang, H.Baba, E.Ideguchi, M.Kimura, N.Kobayashi, Y.Kondo, J.Lee, S.Michimasa, T.Motobayashi, N.Shimizu, M.Takechi, Y.Togano, Y.Utsuno, K.Yoneda, H.Sakurai
In-beam γ-ray spectroscopy of 35Mg via knockout reactions at intermediate energies
NUCLEAR REACTIONS C(36Mg, 35Mg), E=235 MeV; C(37Al, 35Mg), E=246 MeV, [secondary 36Mg and 37Al beams from 9Be(48Ca, X), E=345 MeV/nucleon primary reaction, followed by separation using BigRIPS separator and Zero Degree spectrometer at RIBF-RIKEN facility]; measured reaction products, Eγ, Iγ, (35Mg)γ-coin, inclusive and γ-ray cross sections, parallel momentum distributions using DALI2 array of 186 large-volume NaI(Tl) crystals. 35Mg; deduced levels, J, π. Comparison with shell-model calculations using SDPF-M interaction, and with antisymmetrized molecular dynamics (AMD) model calculations using Gogny D1S force. C(36Mg, 34Mg), (36Mg, 33Mg), E=235 MeV; measured inclusive σ.
NUCLEAR STRUCTURE 35Mg; calculated levels, J, π, single-particle knockout cross sections, spectroscopic factors using shell-model with SDPF-M interaction, and antisymmetrized molecular dynamics (AMD) model with Gogny D1S force. Comparison with experimental data.
doi: 10.1103/PhysRevC.96.034328
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