ADOPTED LEVELS, GAMMAS for 113Ag
Author: Jean Blachot | Citation: Nucl. Data Sheets 111, 1471 (2010) | Cutoff date: 1-May-2009
Full ENSDF file | Adopted Levels (PDF version)
Q(β-)=2016 keV 17 | S(n)= 8514 keV 17 | S(p)= 7994 keV 18 | Q(α)= -4452 keV 18 | ||
Reference: 2012WA38 |
References: | |||
A | 113Pd β- decay | B | 113Ag IT decay |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
0 | A | 1/2- | 5.37 h 5 % β- = 100 | |||||
43.5 1 | AB | 7/2+ | 68.7 s 16 % IT = 64 7 % β- = 36 7 | 43.6 2 | 100 | E3 | 0 | 1/2- |
139.30 15 | A | 9/2+ | 95.74 20 | 100 | M1 | 43.5 | 7/2+ | |
222.08 13 | A | 3/2+ | 23 ns 2 | 222.06 20 | 100 | E1 | 0 | 1/2- |
270.82 14 | A | (3/2-) | 270.81 20 | 100 | 0 | 1/2- | ||
273.59 16 | A | (1/2) | ≈ 30 ns | 51.5 2 273.6 2 | 25 100 | 222.08 0 | 3/2+ 1/2- | |
280.0 2 | A | 1/2+ | 57.9 3 280.0 2 | 1.2 6 100 4 | 222.08 0 | 3/2+ 1/2- | ||
366.84 20 | A | (5/2-) | 96.0 3 366.8 3 | 76 100 | 270.82 0 | (3/2-) 1/2- | ||
369.80 17 | A | 7/2+ | < 0.8 ns | 147.73 20 230.49 20 326.28 20 | 100 77 60 | E2 | 222.08 139.30 43.5 | 3/2+ 9/2+ 7/2+ |
476.70 14 | A | 5/2+ | < 0.5 ns | 205.87 20 254.61 20 337.32 20 433.4 2 | 19 100 9 26 | 270.82 222.08 139.30 43.5 | (3/2-) 3/2+ 9/2+ 7/2+ | |
526.16 16 | A | 49.6 2 386.9 2 482.4 3 | 2.3 16 100 | 476.70 139.30 43.5 | 5/2+ 9/2+ 7/2+ | |||
607.06 23 | A | 336.3 3 607.0 3 | 48 100 | 270.82 0 | (3/2-) 1/2- | |||
611.31 25 | A | (3/2-) | 472.1 3 567.7 3 | 7 100 | 139.30 43.5 | 9/2+ 7/2+ | ||
673.35 23 | A | 534.2 3 673.2 3 | 100 39 | 139.30 0 | 9/2+ 1/2- | |||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
781.79 20 | A | (5/2-) | 414.9 3 510.9 3 781.9 3 | 67 100 33 | 366.84 270.82 0 | (5/2-) (3/2-) 1/2- | ||
783.16 14 | A | (3/2,5/2,7/2) | 257.1 3 643.7 3 739.63 3 | 4.5 100 80 | 526.16 139.30 43.5 | 9/2+ 7/2+ |
E(level): From least-squares fit to γ energies.
M(γ): From α(K)exp in 113Pd β- decay and 113Ag IT decay
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 1 - INTRUDER-ROTATIONAL band (1990Ro16) | |||||||
222.08 13 | 3/2+ | 23 ns 2 | |||||
280.0 2 | 1/2+ | 57.9 3 280.0 2 | 1.2 6 100 4 | 222.08 0 | 3/2+ 1/2- | ||
369.80 17 | 7/2+ | < 0.8 ns | 147.73 20 230.49 20 326.28 20 | 100 77 60 | E2 | 222.08 139.30 43.5 | 3/2+ 9/2+ 7/2+ |
476.70 14 | 5/2+ | < 0.5 ns | 205.87 20 254.61 20 337.32 20 433.4 2 | 19 100 9 26 | 270.82 222.08 139.30 43.5 | (3/2-) 3/2+ 9/2+ 7/2+ |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Conversion Coefficient | Additional Data |
43.5 | 7/2+ | 68.7 s 16 % IT = 64 7 % β- = 36 7 | 43.6 2 | E3 | 1047 | B(E3)(W.u.)=0.048 6, α=1047 |
139.30 | 9/2+ | 95.74 20 | M1 | 0.478 | α=0.478 | |
222.08 | 3/2+ | 23 ns 2 | 222.06 20 | E1 | 0.01660 | B(E1)(W.u.)=1.13E-6 10, α=0.01660 |
369.80 | 7/2+ | < 0.8 ns | 147.73 20 | E2 | 0.362 | B(E2)(W.u.)>1.1×102, α=0.362 |
Additional Level Data and Comments:
E(level) | Jπ(level) | T1/2(level) | Comments |
222.08 | 3/2+ | 23 ns 2 | E(level): INTRUDER-ROTATIONAL band (1990Ro16). |
270.82 | (3/2-) | Jπ(level): 1988KaZE have derived low-lying negative parity states in odd-mass Ag: α=107,109,111,113,115Ag. | |
280.0 | 1/2+ | E(level): INTRUDER-ROTATIONAL band (1990Ro16). | |
366.84 | (5/2-) | Jπ(level): 1988KaZE have derived low-lying negative parity states in odd-mass Ag: α=107,109,111,113,115Ag. | |
369.80 | 7/2+ | < 0.8 ns | E(level): INTRUDER-ROTATIONAL band (1990Ro16). |
476.70 | 5/2+ | < 0.5 ns | E(level): INTRUDER-ROTATIONAL band (1990Ro16). |
611.31 | (3/2-) | Jπ(level): 1988KaZE have derived low-lying negative parity states in odd-mass Ag: α=107,109,111,113,115Ag. | |
781.79 | (5/2-) | Jπ(level): 1988KaZE have derived low-lying negative parity states in odd-mass Ag: α=107,109,111,113,115Ag. |
1988KaZE suggest that the 222, 369, 476 levels could be intruder states and have tried to derive parameter sets for this collective rotational-like band with K=1/2
Q-value: Note: Current evaluation has used the following Q record 2017 168520 177970 28-4444 20 2003Au03,2009AuZZ