ADOPTED LEVELS, GAMMAS for 256Rf
Author: Balraj Singh | Citation: Nucl. Data Sheets 141, 327 (2017) | Cutoff date: 22-Mar-2017
Full ENSDF file | Adopted Levels (PDF version)
Q(β-)=-6280 keV SY | S(n)= 8180 keV SY | S(p)= 3014 keV 25 | Q(α)= 8926 keV 15 | ||
Reference: 2017WA10 |
References: | |||
A | 260Sg α decay (4.95 MS) | B | 208Pb(50Ti,2nγ) |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
0.0 | AB | 0+ | 6.67 ms 10 % α = 0.32 17 % SF = 99.68 17 | |||||
44 1 | AB | (2+) | 44 1 S | 100 | [E2] | 0.0 | 0+ | |
148 2 | B | (4+) | 104 1 S | 100 | [E2] | 44 | (2+) | |
309 2 | B | (6+) | 161 1 | 100 | [E2] | 148 | (4+) | |
527 2 | B | (8+) | 218 1 | 100 | [E2] | 309 | (6+) | |
799 2 | B | (10+) | 272 1 | 100 | [E2] | 527 | (8+) | |
≈946 | B | (3-) | 900 1 | | 44 | (2+) | ||
≈1120 | B | (5-) | 25 µs 2 % IT = ? % SF = ? | |||||
1122 3 | B | (12+) | 323 1 | 100 | [E2] | 799 | (10+) | |
≈1400 | B | (8-) | 17 µs 2 % IT = ? % SF = ? | |||||
1493 3 | B | (14+) | 371 1 | 100 | [E2] | 1122 | (12+) | |
1910 4 | B | (16+) | 417 2 | 100 | 1493 | (14+) | ||
>2200 | B | 27 µs 5 % IT = ? % SF = ? | ||||||
2369 4 | B | (18+) | 459 2 | 100 | 1910 | (16+) | ||
2868 5 | B | (20+) | 499 2 | 100 | 2369 | (18+) |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 1 - Kπ=0+ band. | |||||||
0.0 | 0+ | 6.67 ms 10 % α = 0.32 17 % SF = 99.68 17 | |||||
44 1 | (2+) | 44 1 S | 100 | [E2] | 0.0 | 0+ | |
148 2 | (4+) | 104 1 S | 100 | [E2] | 44 | (2+) | |
309 2 | (6+) | 161 1 | 100 | [E2] | 148 | (4+) | |
527 2 | (8+) | 218 1 | 100 | [E2] | 309 | (6+) | |
799 2 | (10+) | 272 1 | 100 | [E2] | 527 | (8+) | |
1122 3 | (12+) | 323 1 | 100 | [E2] | 799 | (10+) | |
1493 3 | (14+) | ||||||
1910 4 | (16+) | 417 2 | 100 | 1493 | (14+) | ||
2369 4 | (18+) | ||||||
2868 5 | (20+) | 499 2 | 100 | 2369 | (18+) |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Conversion Coefficient | Additional Data |
44 | (2+) | 44 1 | [E2] | 1.83×103 | α=1.83×103 22, α(L)=1.30E3 16, α(M)=3.8E2 5, α(N)=111 14, α(O)=29 4, α(P)=4.9 6, α(Q)=0.0157 16 | |
148 | (4+) | 104 1 | [E2] | 31.5 | α=31.5 15, α(L)=22.4 11, α(M)=6.6 4, α(N)=1.91 9, α(O)=0.502 24, α(P)=0.086 4, α(Q)=0.000476 20 | |
309 | (6+) | 161 1 | [E2] | 4.51 | α=4.51 14, α(K)=0.093 3, α(L)=3.15 10, α(M)=0.92 3, α(N)=0.266 9, α(O)=0.0701 22, α(P)=0.0121 4, α(Q)=9.78×10-5 25 | |
527 | (8+) | 218 1 | [E2] | 1.33 | α=1.33 3, α(K)=0.1204 17, α(L)=0.861 21, α(M)=0.249 6, α(N)=0.0721 18, α(O)=0.0190 5, α(P)=0.00334 8, α(Q)=3.68×10-5 8 | |
799 | (10+) | 272 1 | [E2] | 0.589 | α=0.589 12, α(K)=0.1016 15, α(L)=0.349 8, α(M)=0.1003 21, α(N)=0.0290 6, α(O)=0.00767 16, α(P)=0.00136 3, α(Q)=1.93×10-5 4 | |
1122 | (12+) | 323 1 | [E2] | 0.333 | α=0.333 6, α(K)=0.0832 12, α(L)=0.179 4, α(M)=0.0510 10, α(N)=0.0147 3, α(O)=0.00390 8, α(P)=0.000701 13, α(Q)=1.213×10-5 20 | |
1493 | (14+) | 371 1 | [E2] | 0.218 | α=0.218 4, α(K)=0.0692 10, α(L)=0.1069 19, α(M)=0.0302 6, α(N)=0.00870 15, α(O)=0.00231 4, α(P)=0.000419 8, α(Q)=8.51×10-6 14 |
Additional Level Data and Comments:
E(level) | Jπ(level) | T1/2(level) | Comments |
0.0 | 0+ | 6.67 ms 10 % α = 0.32 17 % SF = 99.68 17 | The α branching was determined by 1997He29 as (0.32|+0.17)%. Authors’ earlier measurement: (2.2 +7.3-1.8)% (1985He06). E(level): The α branching was determined by 1997He29 as (0.32|+0.17)%. Authors’ earlier measurement: (2.2 +7.3-1.8)% (1985He06). Kπ=0+ band. |
44 | (2+) | E(level): Kπ=0+ band. | |
148 | (4+) | E(level): Kπ=0+ band. | |
309 | (6+) | E(level): Kπ=0+ band. | |
527 | (8+) | E(level): Kπ=0+ band. | |
799 | (10+) | E(level): Kπ=0+ band. | |
1120 | (5-) | 25 µs 2 % IT = ? % SF = ? | E(level): From 2009Je01. Level energy deduced from (electron)(900γ) coin. Half-life from recoil-electron-electron-electron-fission(t). Isomers at ≈1120 and ≈1400 keV interpreted by 2009Je01 as possible 2-qp states, while the one at >2000 keV is interpreted as possible 4-qp state. See also 2011Ro20 where only one isomer of 17 μs 5 was seen and interpreted as possible 4-qp state. T1/2(level): From 2009Je01. Level energy deduced from (electron)(900γ) coin. Half-life from recoil-electron-electron-electron-fission(t). Isomers at ≈1120 and ≈1400 keV interpreted by 2009Je01 as possible 2-qp states, while the one at >2000 keV is interpreted as possible 4-qp state. See also 2011Ro20 where only one isomer of 17 μs 5 was seen and interpreted as possible 4-qp state. |
1122 | (12+) | E(level): Kπ=0+ band. | |
1400 | (8-) | 17 µs 2 % IT = ? % SF = ? | E(level): From 2009Je01. Level energy deduced from (electron)(900γ) coin. Half-life from recoil-electron-electron-electron-fission(t). Isomers at ≈1120 and ≈1400 keV interpreted by 2009Je01 as possible 2-qp states, while the one at >2000 keV is interpreted as possible 4-qp state. See also 2011Ro20 where only one isomer of 17 μs 5 was seen and interpreted as possible 4-qp state. T1/2(level): From 2009Je01. Level energy deduced from (electron)(900γ) coin. Half-life from recoil-electron-electron-electron-fission(t). Isomers at ≈1120 and ≈1400 keV interpreted by 2009Je01 as possible 2-qp states, while the one at >2000 keV is interpreted as possible 4-qp state. See also 2011Ro20 where only one isomer of 17 μs 5 was seen and interpreted as possible 4-qp state. |
1493 | (14+) | E(level): Kπ=0+ band. | |
1910 | (16+) | E(level): Kπ=0+ band. | |
2200 | 27 µs 5 % IT = ? % SF = ? | Possible 4-qp state (2009Je01,2013Ri07). E(level): From 2009Je01. Level energy deduced from (electron)(900γ) coin. Half-life from recoil-electron-electron-electron-fission(t). Isomers at ≈1120 and ≈1400 keV interpreted by 2009Je01 as possible 2-qp states, while the one at >2000 keV is interpreted as possible 4-qp state. See also 2011Ro20 where only one isomer of 17 μs 5 was seen and interpreted as possible 4-qp state. T1/2(level): From 2009Je01. Level energy deduced from (electron)(900γ) coin. Half-life from recoil-electron-electron-electron-fission(t). Isomers at ≈1120 and ≈1400 keV interpreted by 2009Je01 as possible 2-qp states, while the one at >2000 keV is interpreted as possible 4-qp state. See also 2011Ro20 where only one isomer of 17 μs 5 was seen and interpreted as possible 4-qp state. | |
2369 | (18+) | E(level): Kπ=0+ band. | |
2868 | (20+) | E(level): Kπ=0+ band. |
E(level) | E(gamma) | Comments |
44 | 44 | E(γ): Calculated value from Harris fit in a rotational band |
148 | 104 | E(γ): Calculated value from Harris fit in a rotational band |
946 | 900 | E(γ): from 2009Je01 |
Isotopic identification and assignment:
1975Og01: 208Pb(50Ti,2n) excitation function
1984Og02: 208Pb(50Ti,2n); 208Pb(49Ti,n) SF observed
1984Og02, 1985Mu11: daughter of 260Sg
1985He06: 208Pb(50Ti,2n),E=4.75-5.15 MeV/nucleon; 207Pb(50Ti,n),E=4.85 MeV/nucleon; parent of 252No (8410α)
1985So03: 249Cf(12C,5n),E=85 MeV, SF observed
Theoretical calculations: consult the Nuclear Science References (NSR) database for about 125 theory references.
2014Li15, 2012Jo05: nuclear structure theory references
Q-value: Estimated ΔQ(β-)=240, ΔS(n)=120 (2017Wa10)
Q-value: S(2n)=15120 280 (syst), S(2p)=5079 20, Q(εp)=126 23 (2017Wa10)