**References quoted in the ENSDF dataset: 59K ADOPTED LEVELS **

8 references found.

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

Yad.Fiz. 58, No 12, 2172 (1995); Phys.Atomic Nuclei 58, 2058 (1995)

M.V.Zverev, N.V.Klochkova, Yu.S.Lutostanski, E.K.Yudina

*Nucleosynthesis and the Properties of Nuclei from Oxygen to Nickel Near the Neutron-Stability Boundary*

NUCLEAR STRUCTURE ^{24}O, ^{29}F, ^{32}Ne, ^{37}Na, ^{42}Mg, ^{47}Al, ^{48}Si, ^{49}P, ^{50}S, ^{53}Cl, ^{56}Ar, ^{59}K, ^{62}Ca, ^{69}Sc, ^{72}Ti, ^{75}V, ^{80}Cr, ^{81}Mn, ^{84}Fe, ^{85}Co, ^{88}Ni; calculated one-, two-neutron separation energies. ^{42}Mg, ^{46}Si, ^{80}Cr, ^{88}Ni; calculated nucleon densities. ^{40}Mg, ^{41}Al, ^{42}Si, ^{43}P, ^{44}S, ^{45}Cl, ^{46}Ar, ^{47}K, ^{48}Ca; calculated Fermi surface characteristics. Self-consistent finite Fermi systems theory.

Phys.Rev. C 78, 024613 (2008)

G.G.Adamian, N.V.Antonenko, S.M.Lukyanov, Yu.E.Penionzhkevich

*Possibility of production of neutron-rich isotopes in transfer-type reactions at intermediate energies*

NUCLEAR REACTIONS ^{181}Ta(^{48}Ca, X)^{38}Si/^{40}Si/^{42}Si/^{44}Si/^{46}Si/^{36}Mg/^{38}Mg/^{40}Mg/^{41}Al/^{43}Al/^{45}Al/^{45}P/^{47}P/^{46}S/^{48}S/^{50}S/^{49}Cl/^{51}Cl/^{53}Cl/^{50}Ar/^{52}Ar/^{54}Ar/^{53}K/^{55}K/^{57}K/^{59}K/^{56}Ca/^{58}Ca/^{60}Ca/^{59}Sc/^{61}Sc/^{63}Sc/^{60}Ti/^{62}Ti/^{64}Ti/^{66}Ti, E=64, 140 MeV/nucleon; W(^{48}Ca, X)^{41}Si/^{42}Si/^{43}Si/^{44}Si/^{46}Si/^{36}Mg/^{37}Mg/^{38}Mg/^{40}Mg, E=142 MeV/nucleon; calculated production σ of neutron-rich isotopes of Mg, Al, Si, P, S, Cl, Ar, K, Ca, Sc, Ti. Comparison with experimental data.

doi: 10.1103/PhysRevC.78.024613

Phys.Rev. C 92, 024314 (2015)

G.Co, V.De Donno, M.Anguiano, R.N.Bernard, A.M.Lallena

*Electric quadrupole and magnetic dipole moments of odd nuclei near the magic ones in a self-consistent approach*

NUCLEAR STRUCTURE ^{16,22,24}O, ^{40,48,60}Ca, ^{90}Zr, ^{100,132}Sn, ^{208}Pb; calculated energies and B(E2) of first 2+ states, energies and B(M1) of low-lying 1+ states using D1M and D1S Gogny interactions, and comparison with experimental data. Hartree-Fock and random phase approximation (RPA) calculations.

NUCLEAR MOMENTS ^{15,21,23}N, ^{17,23,25}F, ^{15,17,21,23,25}O, ^{39,47,59}K, ^{41,49,61}Sc, ^{39,41,47,49,59,61}Ca, ^{89}Y, ^{91}Nb, ^{89,91}Zr, ^{99,131}In, ^{101,133}Sb, ^{99,101,131,133}Sn, ^{207}Tl, ^{209}Bi, ^{207,209}Pb; calculated magnetic dipole and electric quadrupole moments of ground states and in some cases excited states using D1M and D1S Gogny interactions and ^{16,22,24}O, ^{40,48,60}Ca, ^{90}Zr, ^{100,132}Sn, ^{208}Pb as core nuclei and associated single-particle states. Hartree-Fock random phase approximation (RPA), independent particle model (IPM) first-order perturbation theory, and finite Fermi systems (FFS) calculations.

doi: 10.1103/PhysRevC.92.024314

Phys.Rev.Lett. 121, 022501 (2018)

O.B.Tarasov, D.S.Ahn, D.Bazin, N.Fukuda, A.Gade, M.Hausmann, N.Inabe, S.Ishikawa, N.Iwasa, K.Kawata, T.Komatsubara, T.Kubo, K.Kusaka, D.J.Morrissey, M.Ohtake, H.Otsu, M.Portillo, T.Sakakibara, H.Sakurai, H.Sato, B.M.Sherrill, Y.Shimizu, A.Stolz, T.Sumikama, H.Suzuki, H.Takeda, M.Thoennessen, H.Ueno, Y.Yanagisawa, K.Yoshida

*Discovery of ^{60}Ca and Implications For the Stability of ^{70}Ca*

NUCLEAR REACTIONS ^{9}Be(^{70}Zn, X)^{47}P/^{49}S/^{52}Cl/^{54}Ar/^{57}K/^{59}Ca/^{60}Ca/^{62}Sc, E=345 MeV/nucleon; measured reaction products. ^{59}K; deduced new isotopes discovery. Comparison with the drip-line predictions of a wide variety of mass models.

doi: 10.1103/physrevlett.121.022501

At.Data Nucl.Data Tables 125, 1 (2019)

P.Moller, M.R.Mumpower, T.Kawano, W.D.Myers

*Nuclear properties for astrophysical and radioactive-ion-beam applications (II)*

NUCLEAR STRUCTURE Z=8-136; calculated the ground-state odd-proton and odd-neutron spins and parities, proton and neutron pairing gaps, one- and two-neutron separation energies, quantities related to β-delayed one- and two-neutron emission probabilities, average energy and average number of emitted neutrons, β-decay energy release and T_{1/2} with respect to Gamow-Teller decay with a phenomenological treatment of first-forbidden decays, one- and two-proton separation energies, and α-decay energy release and half-life.

doi: 10.1016/j.adt.2018.03.003

Chin.Phys.C 45, 030001 (2021)

F.G.Kondev, M.Wang, W.J.Huang, S.Naimi, G.Audi

*The NUBASE2020 evaluation of nuclear physics properties*

COMPILATION A=1-295; compiled, evaluated nuclear structure and decay data.

Phys.Rev. C 104, 044321 (2021)

F.Minato, T.Marketin, N.Paar

*β-delayed neutron-emission and fission calculations within relativistic quasiparticle random-phase approximation and a statistical model*

RADIOACTIVITY Z=8-110, N=11-209, A=19-318(β^{-}), (β^{-}n); calculated T_{1/2}, β^{-}-delayed neutron emission (BDNE) branching ratios (P_{0n}, P_{1n}, P_{2n}, P_{3n}, P_{4n}, P_{5n}, P_{6n}, P_{7n}, P_{8n}, P_{9n}, P_{10n}), mean number of delayed neutrons per beta-decay, and average delayed neutron kinetic energy, total beta-delayed fission and α emission branching ratios for four fission barrier height models (ETFSI, FRDM, SBM, HFB-14). Z=93-110, N=184-200, A=224-318; calculated T_{1/2}, β^{-}-delayed fission (BDF) branching ratios (P_{0f}, P_{1f}, P_{2f}, P_{3f}, P_{4f}, P_{5f}, P_{6f}, P_{7f}, P_{8f}, P_{9f}, P_{10f}), total beta-delayed fission and beta-delayed neutron emission branching ratios for four fission barrier height models ^{140,162}Sn; calculated β strength functions, β^{-}-delayed neutron branching ratios from P_{0n} to P_{10n} by pn-RQRPA+HFM and pn-RQRPA methods. ^{137,138,139,140,156,157,158,159,160,161,162}Sb; calculated isotope production ratios as a function of excitation energy. ^{123,124,125,126,127,128,129,130,131,132,133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155,156}Pd, ^{120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155,156,157,158,159}Ag, ^{200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,221,222,223,224,225,226,227,228,229,230,231,232,233,234,235,236,237,238,239,240,241,242,243,244,245,246,247,248,249,250}Os, ^{200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,221,222,223,224,225,226,227,228,229,230,231,232,233,234,235,236,237,238,239,240,241,242,243,244,245,246,247,248,249,250,251,252,253,254,255}Ir; calculated β-delayed one neutron branching ratio P_{1n} by pn-RQRPA+HFM, pn-RQRPA, and FRDM+QRPA+HFM methods, and compared with available experimental data. ^{89}Br, ^{138}I; calculated β-delayed neutron spectrum by pn-RQRPA+HFM method, and compared with experimental spectra. ^{260,261,262,263,264,265,266,267,268,269,270,271,272,273,274,275,276,277,278,279,280,281,282,283,284,285,286,287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316,317,318,319,320,321,322,323,324,325,326,327,328,329,330}Fm; calculated fission barrier heights for HFB-14, FRDM, ETFSI and SBM models, mean numbers and mean energies of emitted β-delayed neutrons by pn-RQRPA+HFM and pn-RQRPA methods. ^{63,64,65,66,67,68,69,70,71,72,73,74,75,76,77,78,79,80,81,82,83,84,85,86,87,88,89,90,91,92,93,94,95,96,97,98,99}Ni, ^{120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155,156,157,158,159,160,161,161,162,163,164,165,166,167,168,169,170}Sn; calculated mean numbers and mean energies of emitted β-delayed neutrons by pn-RQRPA+HFM and pn-RQRPA methods. Z=70-110, N=120-190; calculated β^{-}-delayed α branching ratios P_{α} (%) for FRDM fission barrier data. Fully self-consistent covariant density-functional theory (CDFT), with the ground states of all the nuclei calculated with the relativistic Hartree-Bogoliubov (RHB) model with the D3C^{*} interaction, and relativistic proton-neutron quasiparticle random-phase approximation (pn-RQRPA) for β strength functions, with particle evaporations and fission from highly excited nuclear states estimated by Hauser-Feshbach statistical model (pn-RQRPA+HFM) for four fission barrier height models (ETFSI, FRDM, SBM, HFB-14). Detailed tables of numerical data for β-delayed neutron emission (BDNE), β-delayed fission (BDF) and β-delayed α-particle emission branching ratios are given in the Supplemental Material of the paper.

doi: 10.1103/PhysRevC.104.044321

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.