ADOPTED LEVELS, GAMMAS for 60V
Authors: E. Browne, J. K. Tuli | Citation: Nucl. Data Sheets 114, 1849 (2013) | Cutoff date: 31-Dec-2012
Full ENSDF file | Adopted Levels (PDF version)
| Q(β-)=13.26×103 keV 31 | S(n)= 3.48×103 keV 27 | S(p)= 14887 keV SY | Q(α)= -10936 keV SY | ||
| Reference: 2012WA38 |
| References: | |||
| A | 60Ti β- decay | B | 60V IT decay (0.32 μs) |
| E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
| 0.0+X | AB | 122 ms 18 % β- = 100 % β-n = ? % β-2n = ? | ||||||
| 0.0+Y | A | 40 ms 15 % β- = 100 % β-n = ? % β-2n = ? | ||||||
| 103.2+X | B | (2+) | 13 ns 3 | 103.2 5 ? | 100 | (M1+E2) | 0.0+X | |
| 202.1+X | B | (4+) | 0.32 µs 9 % IT = 100 | 98.9 5 ? | 100 | (E2) | 103.2+X | (2+) |
| E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Conversion Coefficient | Additional Data |
| 103.2+X | (2+) | 13 ns 3 | 103.2 5 | (M1+E2) | 0.18 | α=0.18 16, α(K)=0.16 15, α(L)=0.016 14, α(M)=0.0020 18, α(N)=9.E-5 9, α(N+)=9.E-5 9 |
| 202.1+X | (4+) | 0.32 µs 9 % IT = 100 | 98.9 5 | (E2) | 0.395 | α=0.395 10, α(K)=0.356 9, α(L)=0.0350 9, α(M)=0.00453 12, α(N)=0.000208 5, α(N+)=0.000208 5 |
Additional Level Data and Comments:
| E(level) | Jπ(level) | T1/2(level) | Comments |
| E(level) | E(gamma) | Comments |
| 103.2+X | 103.2 | E(γ): 104.0 (2012Ka36) M(γ): From 1999DaZQ based on level T1/2 and RUL |
| 202.1+X | 98.9 | E(γ): 99.7 (2012Ka06). M(γ): From 1999DaZQ based on level T1/2 and RUL |
2003So02: 70Ge30+ beam on 58Ni, E=61.8 MeV/α, measured β-. Deduced T1/2=68 ms 5 which authors consider for a composite of two isomers.
1999Le67,1999So20: 86Kr34+ beam on 58Ni, E=60.4 MeV/α, measured β-.
1999DaZQ: 86Kr34+ beam on 58Ni, E=60.3 MeV/α, measured γ, γ(t)
Mass measurements: 2011Es06.
Discovery of vanadium isotopes: 2010Sh05.
Levels: From finite-range droplet model 2000So02 expect 60V g.s. to be oblate, with β2=-0.011. α prolate configuration, β2=+0.11, is expected to lie about 115 keV higher. α configuration=((ν,[404]9/2+)(π,[303]5/2-)) is possible to yield π=-,J=2 to 7 for the oblate shape. For prolate shape states with π=+,J=1 to 4 are expected. Authors expect many close lying levels with possibly large spin differences.
Q-value: ΔS(p)=457 syst, ΔQ(α)=457 syst (2012Wa38)