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 17S(n)= 8514 keV 17S(p)= 7994 keV 18Q(α)= -4452 keV 18
Reference: 2012WA38

References:
  A  113Pd β- decay  B  113Ag IT decay

General Comments:

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










E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
    0A  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)
XREFJπ(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

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Band Transitions:

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+

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Additional Gamma Data:













E(level)
(keV)
Jπ(level)T1/2(level)E(γ)
(keV)
MultipolarityConversion
Coefficient
Additional Data
   43.5 7/2+ 68.7 s 16 
% IT = 64 7
% β- = 36 7
   43.6 2 E31047B(E3)(W.u.)=0.048 6, α=1047
  139.30 9/2+      95.74 20 M10.478α=0.478
  222.08 3/2+ 23 ns 2    222.06 20 E10.01660B(E1)(W.u.)=1.13E-6 10, α=0.01660
  369.80 7/2+ < 0.8 ns   147.73 20 E20.362B(E2)(W.u.)>1.1×102, α=0.362

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Additional Level Data and Comments:

E(level)Jπ(level)T1/2(level)Comments
  222.083/2+ 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.
  280.01/2+   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.
  369.807/2+ < 0.8 ns E(level): INTRUDER-ROTATIONAL band (1990Ro16).
  476.705/2+ < 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.

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