ADOPTED LEVELS, GAMMAS for 191Ir

Author: V.R. Vanin Et Al. |  Citation: Nucl. Data Sheets 108, 2393 (2007) |  Cutoff date: 1-Dec-2006 

 Full ENSDF file | Adopted Levels (PDF version) 


Q(β-)=-1009 keV 4S(n)= 8026.5 keV 4S(p)= 5290.4 keV 12Q(α)= 2082.8 keV 13
Reference: 2012WA38

References:
  A  191Pt ε decay  B  191Os β- decay (15.4 d)
  C  191Ir IT decay (4.899 S)  D  Coulomb Excitation
  E  192Os(p,2nγ),(d,3nγ)  F  191Ir(γ,γ): MOSSBAUER
  G  190Os(3He,d),(α,t)  H  191Ir(d,d’)
  I  191Ir(p,p’) E=50 MeV  J  193Ir(p,t)
  K  191Ir(γ,γ’)  L  191Ir(n,n’γ)

General Comments:

Calculations:

Magnetic properties of selected levels: 2002St11.

Levels and properties in rotor + 1 quasiparticle model: 2001Ro23.

Levels and properties in triaxial rotor and supersymmetry model: 2000Be07.

Levels, B(E2), with IBM, in 185Ir-195Ir: 1994He24, 1986Ar03.

Supersymmetry model: 1985Hu07.

Compilation, review: NMR in oriented nuclei: 1996Ha09.

Isotope shift and hyperfine structure measurements: 1989Sa31.

Levels: The rotational bands of 191Ir with axially asymmetric core are discussed in 1979Vi06, 1987Pr10, and 2001Ro23. The band assignments are based on assignments in 191Ir(n,n’γ) (1987Pr10) and 192Os(3He,d) (1971Pr13). Spin(6) symmetry and U(6/4), U(6/20) supersymmetry are used to describe 191Ir (1984Mu19, 1986Mc01, 2000Be07).

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
     0.0ABCDEFGHIJ L 3/2+ STABLE      
    82.423 12 ABCDEFGHIJ L 1/2+ 4.08 ns 7     82.413 15 
    100
M1+E2
     0.0
3/2+
   129.413 13 ABCDEFGHIJ L 5/2+ 89.9 ps 9     47.05 3 
  129.416 16 
      0.0094 11 
    100.00 15 
E2
M1+E2
    82.423
     0.0
1/2+
3/2+
   171.29 4 ABCDE GH J L 11/2- 4.899 s 23 
% IT = 100
   41.89 4 
    100
E3
   129.413
5/2+
   178.950 12 A  DE GHIJ L 3/2+ 43 ps 4     49.59 3 
   96.517 9 
  178.96 3 
      1.11 13 
    100 4 
     31.6 10 
M1+E2
M1+E2
M1+E2
   129.413
    82.423
     0.0
5/2+
1/2+
3/2+
   300.4 4     E            121.5 5 
  300.4 5 
 
    100 8 


   178.950
     0.0
3/2+
3/2+
   343.23 5 A  DE GHIJ L (7/2)+ 20.4 ps 8    213.76 7 
  343.32 8 
     63.7 17 
    100.0 17 
M1+E2
(E2)
   129.413
     0.0
5/2+
3/2+
   351.154 17 A  DE G IJ L (5/2)+ 18.8 ps 25    172.19 2 
  221.74 8 
  268.71 8 
  351.17 3 
    100 3 
      3.6 3 
     48 5 
     99 3 
M1+E2
(M1)
E2
M1+E2
   178.950
   129.413
    82.423
     0.0
3/2+
5/2+
1/2+
3/2+
   390.94 6 A  DE G    L 7/2- 240 ps 20    219.65 5 
    100
E2
   171.29
11/2-
   502.61 5    DE  H J L (9/2)+ 13.4 ps 19    159.38 3 
  373.20 9 
      8.9 5 
    100.0 23 
[M1,E2]
E2
   343.23
   129.413
(7/2)+
5/2+
   504.13 11    DE  HI  L (7/2+)     152.9 3 
  161.2 5 
  325.2 5 
  374.83 15 
     58 5 
    200 80 
    100 5 
     52 11 
(D(+Q))



   351.154
   343.23
   178.950
   129.413
(5/2)+
(7/2)+
3/2+
5/2+
   538.854 17 A  DE  H JKL 3/2+ 9.8 ps 8    187.69 4 
  196 1 
  359.88 3 
  409.44 2 
  456.47 5 
  538.87 5 
      2.83 12 
      0.022 6 
     40.3 9 
     55 3 
     23.2 11 
    100 3 
M1+E2

M1+E2
M1+E2
M1+E2
M1+E2
   351.154
   343.23
   178.950
   129.413
    82.423
     0.0
(5/2)+
(7/2)+
3/2+
5/2+
1/2+
3/2+
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   556.64 11     E      L (13/2-)     385.33 10 
    100
(D+Q)
   171.29
11/2-
   587.95 7 A  DE G  JKL 3/2+,5/2+ ≈ 0.3 ps   244.6 2 
  458.59 15 
  587.95 8 
     69 7 
     38 3 
    100 5 

[M1,E2]
(M1)
   343.23
   129.413
     0.0
(7/2)+
5/2+
3/2+
   591.13 16     E      L (15/2-)     419.89 16 
    100
(Q)
   171.29
11/2-
   614 4        H            
   624.07 4 A  D     JKL (1/2+) > 5 ps    85.15 8 
  445.13 8 
  494.69 7 
  541.64 10 
  624.06 6 
      4.1 5 
      4.00 27 
      4.11 22 
     25 3 
    100 3 
[M1,E2]
[M1,E2]
(E2)
(M1)
(M1+E2)
   538.854
   178.950
   129.413
    82.423
     0.0
3/2+
3/2+
5/2+
1/2+
3/2+
   653.99 9    DE  H   L (9/2-)     263.08 7 
  482.5 5 
     79 17 
    100 13 


   390.94
   171.29
7/2-
11/2-
   658.90 5 A  DE  H  K  (3/2-) < 0.12 ns   267.92 8 
  479.95 7 
  576.46 8 
  658.75 15 
    100 10 
      7.2 4 
     16.4 5 
      2.01 15 
E2
[E1]
E1
[E1]
   390.94
   178.950
    82.423
     0.0
7/2-
3/2+
1/2+
3/2+
   686.10 10 A  DE GHIJ L 7/2+ 2.7 ps 3    556.79 15 
  686.02 17 
    100 3 
     76 3 
M1+E2
E2
   129.413
     0.0
5/2+
3/2+
   747.77 6 A  DE      L (5/2)+     208.96 15 
  396.7 2 
  404.1 3 
  568.81 8 
  618.7 4 
  747.75 13 
    100 6 
      8.0 25 
      9 4 
     41.7 18 
      6.7 25 
      2.76 25 
M1(+E2)
[M1,E2]

(M1)
[M1,E2]
[M1,E2]
   538.854
   351.154
   343.23
   178.950
   129.413
     0.0
3/2+
(5/2)+
(7/2)+
3/2+
5/2+
3/2+
   762.54 5 A  DE    J L 3/2+     138.2 2 
  223.67 8 
  411.3 3 
  583.61 8 
  633.18 10 
  680.0 2 
  762.60 15 
     22 15 
    100 9 
      8.8 22 
     69 5 
     26.4 11 
      7.2 6 
     11.8 9 
[M1,E2]
M1+E2
[M1,E2]
(M1)
E2(+M1)
[M1,E2]
[M1,E2]
   624.07
   538.854
   351.154
   178.950
   129.413
    82.423
     0.0
(1/2+)
3/2+
(5/2)+
3/2+
5/2+
1/2+
3/2+
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   799.79 5 A  DE      L (5/2)-     140.884 15 
  409.26 19 
     78 12 
    100 17 
M1(+E2)

   658.90
   390.94
(3/2-)
7/2-
   811.88 12    DE    J L (9/2+)     308.03 21 
  460.43 15 
  468.9 5 
     78 6 
    100 8 
     46 6 
(D)


   504.13
   351.154
   343.23
(7/2+)
(5/2)+
(7/2)+
   816.59 18            L     645.30 17 
    100

   171.29
11/2-
   825.10 17     E      L (7/2+,9/2+)     482.5 5 
  695.60 18 
   <220
    100 11 


   343.23
   129.413
(7/2)+
5/2+
   831.97 17    DE  H J L (11/2+) 3.15 ps 19    329.4 5 
  488.85 18 
     35.4 18 
    100 3 
(D(+Q))

   502.61
   343.23
(9/2)+
(7/2)+
   877.65 12     E G    L (9/2-,11/2+)     374.83 15 
  534.59 15 
    100 15 
     78 13 


   502.61
   343.23
(9/2)+
(7/2)+
   919.08 17     E      L (11/2-)     264.8 5 
  527.9 5 
  748.0 2 
    100 10 
     18 5 
     21 15 
(Q)


   653.99
   390.94
   171.29
(9/2-)
7/2-
11/2-
   927.80 25     E      L (7/2+)     389.1 5 
  425.5 10 
  798.3 3 
 
 
 



   538.854
   502.61
   129.413
3/2+
(9/2)+
5/2+
   935.46 13 A          L (1/2+,3/2,5/2+)     756.4 5 
  806.4 3 
  853.4 4 
  935.33 15 
     13 3 
     34.2 21 
      9.0 7 
    100 5 




   178.950
   129.413
    82.423
     0.0
3/2+
5/2+
1/2+
3/2+
   945.4 4    DE    J L (5/2+,7/2+,9/2+)     259.0 5 
  443
  603
  816.0 5 
     79 7 
     95 5 
    100 17 
     71 5 




   686.10
   502.61
   343.23
   129.413
7/2+
(9/2)+
(7/2)+
5/2+
   963.2 4     E        (15/2-)     372.1 5 
  406.5 5 
 
 


   591.13
   556.64
(15/2-)
(13/2-)
   977.04 8     E G    L (7/2-)     177.25 6 
  318.4 10 
  586.2 3 
    100 15 
 
     43 16 



   799.79
   658.90
   390.94
(5/2)-
(3/2-)
7/2-
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   991.28 16     E      L (11/2+)     178.7 5 
  487.1 5 
  489.0 5 
 
      9.4 18 
    100 3 



   811.88
   504.13
   502.61
(9/2+)
(7/2+)
(9/2)+
  1003.6 3    DE    J L (13/2+)     172.0
  500.9 3 
 
 


   831.97
   502.61
(11/2+)
(9/2)+
  1034 3       G    L 1/2+        
  1036.59 21     E      L (17/2-)     445.50 15 
  480 1 
    100 10 
    <25
(D+Q)

   591.13
   556.64
(15/2-)
(13/2-)
  1052.63 14     E      L     366.56 11 
  549.8 3 
  709.4 5 
    100 16 
     23 5 
      9 3 



   686.10
   502.61
   343.23
7/2+
(9/2)+
(7/2)+
  1070      G  J   3/2+        
  1127.1 6     E        (19/2-)     536.0 5 
    100
(Q)
   591.13
(15/2-)
  1130         J          
  1135.23 24     E      L (7/2-,9/2,11/2-)     216.8 5 
  482.5 5 
  743.6 3 
    100 14 
   <166
     41 4 



   919.08
   653.99
   390.94
(11/2-)
(9/2-)
7/2-
  1138      GH J          
  1206.57 18    DE      L (7/2+,9/2+,11/2+)     375.2 5 
  520.5 3 
  703.81 23 
   <180
    100 13 
     67 12 



   831.97
   686.10
   502.61
(11/2+)
7/2+
(9/2)+
  1206.89 20     E      L (9/2-)     229.85 18 
    100

   977.04
(7/2-)
  1210.5 4     E    J L (9/2,11/2)     332.5 5 
  556.8 5 
    100 20 
    <85


   877.65
   653.99
(9/2-,11/2+)
(9/2-)
  1244      G  J          
  1253.5 4     E        (13/2-)     334.6 5 
  599.4 5 
     38 6 
    100 10 


   919.08
   653.99
(11/2-)
(9/2-)
  1297.19 22            L     793.0 3 
  946.1 3 
     43 14 
    100 14 


   504.13
   351.154
(7/2+)
(5/2)+
  1359      G             
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
  1393       H            
  1397.7 3    DE      L (13/2+)     406.7 3 
  585.2 5 
    100 48 
      9 4 


   991.28
   811.88
(11/2+)
(9/2+)
  1400.9 4     E        (5/2+,7/2-)     715 1 
  741.4 5 
  898.9 5 
 
 
 



   686.10
   658.90
   502.61
7/2+
(3/2-)
(9/2)+
  1418.1 3    DE      L (15/2+)     414.3 5 
  586.2 3 
    100 18 
   <300


  1003.6
   831.97
(13/2+)
(11/2+)
  1421.7 4     E        (17/2-)     385.6 5 
  458.6 5 
  864.6 5 
  <1350
   <262
    100 12 



  1036.59
   963.2
   556.64
(17/2-)
(15/2-)
(13/2-)
  1433      G             
  1449      G      1/2-,3/2-        
  1461         J   3/2+        
  1507       H            
  1520      G      5/2-,7/2-        
  1596         J   3/2+        
  1600.1 6    DE        (17/2+)     596.5 5 
    100

  1003.6
(13/2+)
  1613      G             
  1642      G             
  1645.9 8     E        (21/2-)     518.8 5 
    100

  1127.1
(19/2-)
  1651.6 8     E            524.5 5 
    100

  1127.1
(19/2-)
  1660      G             
  1680.6 8     E        (23/2-)     553.5 5 
    100
(Q)
  1127.1
(19/2-)
  1711      G             
  2046.7 9     E            395.1 5 
 

  1651.6

  2046.7+X    E        5.5 s 7 
% IT = 100
     
  2112.1 11    D         (19/2+)     694
    100

  1418.1
(15/2+)
  2312.1 12    D         (21/2+)     712
    100

  1600.1
(17/2+)

E(level): Level energies from a least-squares fit to adopted γ-ray energies, using ΔEγ=0.5 keV when uncertainty not given.

Jπ(level): Assignments are based on rotational structure, on γ-ray multipolarities and decay patterns, and on L-transfers and spectroscopic factors of particle transfer reactions. Assignments for levels populated in 191Ir(n,n’γ) are based on comparisons between experimental and theoretical population rates. Specific arguments are given with individual levels, and bases for Nilsson orbital assignments are presented for rotational bandheads.

E(γ): From 191Pt ε decay unless noted, when the most accurate value between 192Os(p,2nγ),(d,3nγ), Coulomb excitation, and 191Ir(n,n’γ) rescaled value (0.055% smaller with increased uncertainties in respect of unevaluated values, see note on Eγ in 191Ir(n,n’γ)) was adopted, except for a few cases where the unweighted average from the discrepant values of 191Os β- decay and 191Pt ε decay were adopted

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Band Transitions:

E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 1 - 3/2(402)
     0.0 3/2+ STABLE      
   129.413 13  5/2+ 89.9 ps 9     47.05 3 
  129.416 16 
      0.0094 11 
    100.00 15 
E2
M1+E2
    82.423
     0.0
1/2+
3/2+
   343.23 5  (7/2)+ 20.4 ps 8    213.76 7 
  343.32 8 
     63.7 17 
    100.0 17 
M1+E2
(E2)
   129.413
     0.0
5/2+
3/2+
   502.61 5  (9/2)+ 13.4 ps 19    159.38 3 
  373.20 9 
      8.9 5 
    100.0 23 
[M1,E2]
E2
   343.23
   129.413
(7/2)+
5/2+
   831.97 17  (11/2+) 3.15 ps 19    329.4 5 
  488.85 18 
     35.4 18 
    100 3 
(D(+Q))

   502.61
   343.23
(9/2)+
(7/2)+
  1003.6 3  (13/2+)     172.0
  500.9 3 
 
 


   831.97
   502.61
(11/2+)
(9/2)+
  1418.1 3  (15/2+)     414.3 5 
  586.2 3 
    100 18 
   <300


  1003.6
   831.97
(13/2+)
(11/2+)
  1600.1 6  (17/2+)     596.5 5 
    100

  1003.6
(13/2+)
  2112.1 11  (19/2+)     694
    100

  1418.1
(15/2+)
  2312.1 12  (21/2+)     712
    100

  1600.1
(17/2+)
E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 2 - 1/2(400)
    82.423 12  1/2+ 4.08 ns 7       
   178.950 12  3/2+ 43 ps 4     49.59 3 
   96.517 9 
  178.96 3 
      1.11 13 
    100 4 
     31.6 10 
M1+E2
M1+E2
M1+E2
   129.413
    82.423
     0.0
5/2+
1/2+
3/2+
   351.154 17  (5/2)+ 18.8 ps 25    172.19 2 
  221.74 8 
  268.71 8 
  351.17 3 
    100 3 
      3.6 3 
     48 5 
     99 3 
M1+E2
(M1)
E2
M1+E2
   178.950
   129.413
    82.423
     0.0
3/2+
5/2+
1/2+
3/2+
   504.13 11  (7/2+)     152.9 3 
  161.2 5 
  325.2 5 
  374.83 15 
     58 5 
    200 80 
    100 5 
     52 11 
(D(+Q))



   351.154
   343.23
   178.950
   129.413
(5/2)+
(7/2)+
3/2+
5/2+
   811.88 12  (9/2+)     308.03 21 
  460.43 15 
  468.9 5 
     78 6 
    100 8 
     46 6 
(D)


   504.13
   351.154
   343.23
(7/2+)
(5/2)+
(7/2)+
   991.28 16  (11/2+)     178.7 5 
  487.1 5 
  489.0 5 
 
      9.4 18 
    100 3 



   811.88
   504.13
   502.61
(9/2+)
(7/2+)
(9/2)+
  1397.7 3  (13/2+)     406.7 3 
  585.2 5 
    100 48 
      9 4 


   991.28
   811.88
(11/2+)
(9/2+)
E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 3 - 1/2(411)
   538.854 17  3/2+ 9.8 ps 8       
   624.07 4  (1/2+) > 5 ps    85.15 8 
  445.13 8 
  494.69 7 
  541.64 10 
  624.06 6 
      4.1 5 
      4.00 27 
      4.11 22 
     25 3 
    100 3 
[M1,E2]
[M1,E2]
(E2)
(M1)
(M1+E2)
   538.854
   178.950
   129.413
    82.423
     0.0
3/2+
3/2+
5/2+
1/2+
3/2+
   747.77 6  (5/2)+     208.96 15 
  396.7 2 
  404.1 3 
  568.81 8 
  618.7 4 
  747.75 13 
    100 6 
      8.0 25 
      9 4 
     41.7 18 
      6.7 25 
      2.76 25 
M1(+E2)
[M1,E2]

(M1)
[M1,E2]
[M1,E2]
   538.854
   351.154
   343.23
   178.950
   129.413
     0.0
3/2+
(5/2)+
(7/2)+
3/2+
5/2+
3/2+
   927.80 25  (7/2+)     389.1 5 
  425.5 10 
  798.3 3 
 
 
 



   538.854
   502.61
   129.413
3/2+
(9/2)+
5/2+
E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 4 - Kπ=(7/2-)
   390.94 6  7/2- 240 ps 20       
   653.99 9  (9/2-)     263.08 7 
  482.5 5 
     79 17 
    100 13 


   390.94
   171.29
7/2-
11/2-
   919.08 17  (11/2-)     264.8 5 
  527.9 5 
  748.0 2 
    100 10 
     18 5 
     21 15 
(Q)


   653.99
   390.94
   171.29
(9/2-)
7/2-
11/2-
  1253.5 4  (13/2-)     334.6 5 
  599.4 5 
     38 6 
    100 10 


   919.08
   653.99
(11/2-)
(9/2-)
E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 5 - 11/2(505)
   171.29 4  11/2- 4.899 s 23 
% IT = 100
     
   556.64 11  (13/2-)     385.33 10 
    100
(D+Q)
   171.29
11/2-
   591.13 16  (15/2-)     419.89 16 
    100
(Q)
   171.29
11/2-
  1036.59 21  (17/2-)     445.50 15 
  480 1 
    100 10 
    <25
(D+Q)

   591.13
   556.64
(15/2-)
(13/2-)
E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 6 - Kπ=(3/2-)
   658.90 5  (3/2-) < 0.12 ns      
   799.79 5  (5/2)-     140.884 15 
  409.26 19 
     78 12 
    100 17 
M1(+E2)

   658.90
   390.94
(3/2-)
7/2-
   977.04 8  (7/2-)     177.25 6 
  318.4 10 
  586.2 3 
    100 15 
 
     43 16 



   799.79
   658.90
   390.94
(5/2)-
(3/2-)
7/2-
  1206.89 20  (9/2-)     229.85 18 
    100

   977.04
(7/2-)

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Additional Gamma Data:















E(level)
(keV)
Jπ(level)T1/2(level)E(γ)
(keV)
MultipolarityMixing
Ratio
Conversion
Coefficient
Additional Data
    82.423 1/2+ 4.08 ns 7     82.413 15 M1+E2-0.873 2010.54B(E2)(W.u.)=20.9 7, B(M1)(W.u.)=0.000474 14, α=10.54, α(K)=5.32 12, α(L)=3.95 9, α(M)=0.994 23, α(N)=0.241 6, α(O)=0.0378 8, α(P)=0.000687 15, α(N+)=0.279 7
   129.413 5/2+ 89.9 ps 9     47.05 3 E2 143.5B(E2)(W.u.)=10.4 13, α=143.5, α(L)=108.1 16, α(M)=27.7 4, α(N)=6.67 10, α(O)=1.010 15, α(P)=0.000955 14, α(N+)=7.69 11
5/2+ 89.9 ps 9    129.416 16 M1+E2-0.398 32.76B(E2)(W.u.)=96.2 24, B(M1)(W.u.)=0.0259 6, α=2.76, α(K)=2.15 3, α(L)=0.463 7, α(M)=0.1098 16, α(N)=0.0269 4, α(O)=0.00458 7, α(P)=0.000265 4, α(N+)=0.0317 5
   171.29 11/2- 4.899 s 23 
% IT = 100
   41.89 4 E3 1.69×104B(E3)(W.u.)=0.0299 5, α=1.69E4, α(L)=1.212E4 19, α(M)=3.71E3 6, α(N)=919 14, α(O)=135.6 21, α(P)=0.1446 22, α(N+)=1055 16
   178.950 3/2+ 43 ps 4     49.59 3 M1+E20.177 2511.5B(E2)(W.u.)=27 9, B(M1)(W.u.)=0.0053 11, α=11.5 10, α(L)=8.8 7, α(M)=2.09 18, α(N)=0.51 5, α(O)=0.086 7, α(P)=0.00472 8, α(N+)=0.60 5
3/2+ 43 ps 4     96.517 9 M1+E2+0.145 76.75B(E2)(W.u.)=58 9, B(M1)(W.u.)=0.066 8, α=6.75, α(K)=5.48 8, α(L)=0.972 15, α(M)=0.226 4, α(N)=0.0554 9, α(O)=0.00971 15, α(P)=0.000682 10, α(N+)=0.0658 10
3/2+ 43 ps 4    178.96 3 M1+E2-0.79 40.916B(E2)(W.u.)=15.7 20, B(M1)(W.u.)=0.00205 24, α=0.916 21, α(K)=0.682 21, α(L)=0.179 3, α(M)=0.0431 8, α(N)=0.01052 18, α(O)=0.00175 3, α(P)=8.2E-5 3, α(N+)=0.01235 21
   343.23 (7/2)+ 20.4 ps 8    213.76 7 M1+E2-0.342 70.667B(E2)(W.u.)=29.8 19, B(M1)(W.u.)=0.0296 15, α=0.667, α(K)=0.542 8, α(L)=0.0962 14, α(M)=0.0224 4, α(N)=0.00549 8, α(O)=0.000960 14, α(P)=6.64E-5 10, α(N+)=0.00652 10
(7/2)+ 20.4 ps 8    343.32 8 (E2) 0.0641B(E2)(W.u.)=41.9 20, α=0.0641, α(K)=0.0429 6, α(L)=0.01607 23, α(M)=0.00397 6, α(N)=0.000966 14, α(O)=0.0001560 22, α(P)=4.69E-6 7, α(N+)=0.001127 16
   351.154 (5/2)+ 18.8 ps 25    172.19 2 M1+E2+0.072 61.301B(E2)(W.u.)=3.9 9, B(M1)(W.u.)=0.056 8, α=1.301, α(K)=1.072 15, α(L)=0.1761 25, α(M)=0.0406 6, α(N)=0.00998 14, α(O)=0.001765 25, α(P)=0.0001322 19, α(N+)=0.01187 17
(5/2)+ 18.8 ps 25    221.74 8 (M1) 0.644B(M1)(W.u.)=0.00095 16, α=0.644, α(K)=0.532 8, α(L)=0.0864 13, α(M)=0.0199 3, α(N)=0.00489 7, α(O)=0.000866 13, α(P)=6.54×10-5 10, α(N+)=0.00582 9
(5/2)+ 18.8 ps 25    268.71 8 E2 0.1324B(E2)(W.u.)=39 7, α=0.1324, α(K)=0.0795 12, α(L)=0.0401 6, α(M)=0.01004 15, α(N)=0.00244 4, α(O)=0.000387 6, α(P)=8.40E-6 12, α(N+)=0.00283 4
(5/2)+ 18.8 ps 25    351.17 3 M1+E2-0.30 20.173B(E2)(W.u.)=1.7 4, B(M1)(W.u.)=0.0060 9, α=0.173 3, α(K)=0.1427 23, α(L)=0.0236 4, α(M)=0.00545 8, α(N)=0.001340 20, α(O)=0.000236 4, α(P)=1.74E-5 3, α(N+)=0.001593 24
   390.94 7/2- 240 ps 20    219.65 5 E2 0.252B(E2)(W.u.)=56 5, α=0.252, α(K)=0.1335 19, α(L)=0.0897 13, α(M)=0.0227 4, α(N)=0.00550 8, α(O)=0.000862 12, α(P)=1.367E-5 20, α(N+)=0.00637 9
   502.61 (9/2)+ 13.4 ps 19    159.38 3 [M1,E2] 1.2α=1.2 5, α(K)=0.8 6, α(L)=0.28 7, α(M)=0.070 20, α(N)=0.017 5, α(O)=0.0028 6, α(P)=0.00010 7, α(N+)=0.020 6
(9/2)+ 13.4 ps 19    373.20 9 E2 0.0508B(E2)(W.u.)=72 11, α=0.0508, α(K)=0.0350 5, α(L)=0.01198 17, α(M)=0.00295 5, α(N)=0.000717 10, α(O)=0.0001165 17, α(P)=3.86E-6 6, α(N+)=0.000838 12
   538.854 3/2+ 9.8 ps 8    187.69 4 M1+E20.54 110.89B(E2)(W.u.)=10 4, B(M1)(W.u.)=0.0031 5, α=0.89 5, α(K)=0.70 5, α(L)=0.146 4, α(M)=0.0345 10, α(N)=0.00845 24, α(O)=0.00144 3, α(P)=8.5E-5 7, α(N+)=0.0100 3
3/2+ 9.8 ps 8    359.88 3 M1+E2+0.023 90.1719B(E2)(W.u.)=0.013 10, B(M1)(W.u.)=0.0080 7, α=0.1719, α(K)=0.1422 20, α(L)=0.0228 4, α(M)=0.00525 8, α(N)=0.001291 18, α(O)=0.000229 4, α(P)=1.734E-5 25, α(N+)=0.001537 22
3/2+ 9.8 ps 8    409.44 2 M1+E2+0.19 10.1189B(E2)(W.u.)=0.60 9, B(M1)(W.u.)=0.0071 8, α=0.1189, α(K)=0.0983 14, α(L)=0.01589 23, α(M)=0.00365 6, α(N)=0.000898 13, α(O)=0.0001590 23, α(P)=1.195E-5 17, α(N+)=0.001069 15
3/2+ 9.8 ps 8    456.47 5 M1+E2-0.32 40.0856B(E2)(W.u.)=0.39 10, B(M1)(W.u.)=0.00204 21, α=0.0856 18, α(K)=0.0707 16, α(L)=0.01152 21, α(M)=0.00265 5, α(N)=0.000652 12, α(O)=0.0001152 21, α(P)=8.56E-6 19, α(N+)=0.000776 14
3/2+ 9.8 ps 8    538.87 5 M1+E2-0.68 20.0467B(E2)(W.u.)=2.52 25, B(M1)(W.u.)=0.0040 4, α=0.0467 9, α(K)=0.0383 7, α(L)=0.00649 11, α(M)=0.001501 24, α(N)=0.000369 6, α(O)=6.47E-5 11, α(P)=4.59E-6 9, α(N+)=0.000438 7
   587.95 3/2+,5/2+ ≈ 0.3 ps   458.59 15 [M1,E2] 0.06α=0.06 3, α(K)=0.05 3, α(L)=0.009 3, α(M)=0.0021 7, α(N)=0.00052 16, α(O)=9.E-5 3, α(P)=6.E-6 4, α(N+)=0.00061 20
3/2+,5/2+ ≈ 0.3 ps   587.95 8 (M1) 0.0471B(M1)(W.u.)≈0.17, α=0.0471, α(K)=0.0391 6, α(L)=0.00619 9, α(M)=0.001419 20, α(N)=0.000349 5, α(O)=6.19×10-5 9, α(P)=4.72E-6 7, α(N+)=0.000415 6
   624.07 (1/2+) > 5 ps    85.15 8 [M1,E2] 9.4α=9.4 4, α(K)=4 4, α(L)=3.8 25, α(M)=0.9 7, α(N)=0.23 16, α(O)=0.036 23, α(P)=0.0006 5, α(N+)=0.27 18
(1/2+) > 5 ps   445.13 8 [M1,E2] 0.06α=0.06 4, α(K)=0.05 3, α(L)=0.010 4, α(M)=0.0023 7, α(N)=0.00056 17, α(O)=0.00010 4, α(P)=6.E-6 4, α(N+)=0.00067 21
(1/2+) > 5 ps   494.69 7 (E2) 0.0244B(E2)(W.u.)<1.3, α=0.0244, α(K)=0.0181 3, α(L)=0.00478 7, α(M)=0.001154 17, α(N)=0.000281 4, α(O)=4.67E-5 7, α(P)=2.05E-6 3, α(N+)=0.000330 5
(1/2+) > 5 ps   541.64 10 (M1) 0.0583B(M1)(W.u.)<0.0038, α=0.0583, α(K)=0.0484 7, α(L)=0.00767 11, α(M)=0.001761 25, α(N)=0.000433 6, α(O)=7.68×10-5 11, α(P)=5.85E-6 9, α(N+)=0.000516 8
(1/2+) > 5 ps   624.06 6 (M1+E2)0.40 220.037B(E2)(W.u.)<2.7, B(M1)(W.u.)<0.0100, α=0.037 4, α(K)=0.030 4, α(L)=0.0049 4, α(M)=0.00113 9, α(N)=0.000277 23, α(O)=4.9E-5 5, α(P)=3.7E-6 4, α(N+)=0.00033 3
E(level)
(keV)
Jπ(level)T1/2(level)E(γ)
(keV)
MultipolarityMixing
Ratio
Conversion
Coefficient
Additional Data
   658.90 (3/2-) < 0.12 ns   267.92 8 E2 0.1337B(E2)(W.u.)>38, α=0.1337, α(K)=0.0801 12, α(L)=0.0406 6, α(M)=0.01016 15, α(N)=0.00247 4, α(O)=0.000391 6, α(P)=8.46E-6 12, α(N+)=0.00287 4
(3/2-) < 0.12 ns   479.95 7 [E1] 0.00869α=0.00869, α(K)=0.00725 11, α(L)=0.001111 16, α(M)=0.000254 4, α(N)=6.19×10-5 9, α(O)=1.079E-5 16, α(P)=7.47E-7 11, α(N+)=7.35E-5 11
(3/2-) < 0.12 ns   576.46 8 E1 0.00591B(E1)(W.u.)>1.0E-6, α=0.00591, α(K)=0.00494 7, α(L)=0.000746 11, α(M)=0.0001700 24, α(N)=4.16E-5 6, α(O)=7.27E-6 11, α(P)=5.14E-7 8, α(N+)=4.93E-5 7
(3/2-) < 0.12 ns   658.75 15 [E1] 0.00450α=0.00450, α(K)=0.00377 6, α(L)=0.000564 8, α(M)=0.0001285 18, α(N)=3.14×10-5 5, α(O)=5.51E-6 8, α(P)=3.95E-7 6, α(N+)=3.73E-5 6
   686.10 7/2+ 2.7 ps 3    556.79 15 M1+E2-1.11 100.0344B(E2)(W.u.)=18 3, B(M1)(W.u.)=0.0117 18, α=0.0344 18, α(K)=0.0279 16, α(L)=0.00505 20, α(M)=0.00118 5, α(N)=0.000289 11, α(O)=5.02E-5 20, α(P)=3.31E-6 19, α(N+)=0.000342 13
7/2+ 2.7 ps 3    686.02 17 E2 0.01141B(E2)(W.u.)=8.9 11, α=0.01141, α(K)=0.00896 13, α(L)=0.00188 3, α(M)=0.000446 7, α(N)=0.0001090 16, α(O)=1.85E-5 3, α(P)=1.020E-6 15, α(N+)=0.0001285 18
   747.77 (5/2)+     208.96 15 M1(+E2)0.5 40.67α=0.67 12, α(K)=0.53 12, α(L)=0.104 3, α(M)=0.0244 12, α(N)=0.0060 3, α(O)=0.001030 17, α(P)=6.5×10-5 16, α(N+)=0.0071 3
(5/2)+     396.7 2 [M1,E2] 0.09α=0.09 5, α(K)=0.07 4, α(L)=0.014 4, α(M)=0.0032 9, α(N)=0.00079 21, α(O)=0.00014 4, α(P)=8.E-6 5, α(N+)=0.0009 3
(5/2)+     568.81 8 (M1) 0.0513α=0.0513, α(K)=0.0426 6, α(L)=0.00675 10, α(M)=0.001548 22, α(N)=0.000381 6, α(O)=6.75×10-5 10, α(P)=5.14E-6 8, α(N+)=0.000453 7
(5/2)+     618.7 4 [M1,E2] 0.028α=0.028 14, α(K)=0.023 12, α(L)=0.0040 15, α(M)=0.0009 4, α(N)=0.00023 8, α(O)=3.9×10-5 15, α(P)=2.7E-6 15, α(N+)=0.00027 10
(5/2)+     747.75 13 [M1,E2] 0.017α=0.017 8, α(K)=0.014 7, α(L)=0.0024 9, α(M)=0.00056 21, α(N)=0.00014 5, α(O)=2.4×10-5 10, α(P)=1.7E-6 9, α(N+)=0.00016 6
   762.54 3/2+     138.2 2 [M1,E2] 1.9α=1.9 6, α(K)=1.2 8, α(L)=0.49 17, α(M)=0.12 5, α(N)=0.030 12, α(O)=0.0048 15, α(P)=0.00014 11, α(N+)=0.035 13
3/2+     223.67 8 M1+E20.39 250.58α=0.58 7, α(K)=0.47 7, α(L)=0.0842 12, α(M)=0.0196 4, α(N)=0.00482 9, α(O)=0.000840 14, α(P)=5.7×10-5 8, α(N+)=0.00571 9
3/2+     411.3 3 [M1,E2] 0.08α=0.08 4, α(K)=0.06 4, α(L)=0.012 4, α(M)=0.0029 8, α(N)=0.00071 20, α(O)=0.00012 4, α(P)=8.E-6 5, α(N+)=0.00084 24
3/2+     583.61 8 (M1) 0.0480α=0.0480, α(K)=0.0398 6, α(L)=0.00631 9, α(M)=0.001447 21, α(N)=0.000356 5, α(O)=6.31×10-5 9, α(P)=4.81E-6 7, α(N+)=0.000424 6
3/2+     633.18 10 E2(+M1)1.5 GT0.018α=0.018 4, α(K)=0.014 4, α(L)=0.0028 5, α(M)=0.00065 10, α(N)=0.000159 24, α(O)=2.7×10-5 5, α(P)=1.6E-6 5, α(N+)=0.00019 3
3/2+     680.0 2 [M1,E2] 0.022α=0.022 11, α(K)=0.018 9, α(L)=0.0031 12, α(M)=0.0007 3, α(N)=0.00018 7, α(O)=3.1×10-5 12, α(P)=2.1E-6 11, α(N+)=0.00021 8
3/2+     762.60 15 [M1,E2] 0.017α=0.017 8, α(K)=0.014 7, α(L)=0.0023 9, α(M)=0.00053 20, α(N)=0.00013 5, α(O)=2.3×10-5 9, α(P)=1.6E-6 8, α(N+)=0.00015 6
   799.79 (5/2)-     140.884 15 M1(+E2)0.5 52.1α=2.1 4, α(K)=1.6 5, α(L)=0.37 9, α(M)=0.09 3, α(N)=0.022 6, α(O)=0.0036 8, α(P)=0.00020 6, α(N+)=0.025 7
   831.97 (11/2+) 3.15 ps 19    488.85 18   0.0253B(E2)(W.u.)=70 4, α=0.0253

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Additional Level Data and Comments:

E(level)Jπ(level)T1/2(level)Comments
     0.03/2+ STABLE Q=+0.816 9, μ=+0.1507 6
Nuclear charge radius: <r2>1/2=5.40 11 fm (2004An14).
E(level): 3/2(402). Unweighted average from 191Os β- decay and 191Pt ε decay.
    82.4231/2+ 4.08 ns 7  μ=+0.600 6
E(level): 1/2(400). From 192Os(p,2nγ),(d,3nγ).
   129.4135/2+ 89.9 ps 9  μ=+0.81 6
E(level): 3/2(402). Unweighted average from 191Os β- decay and 191Pt ε decay.
   171.2911/2- 4.899 s 23 
% IT = 100
μ=+6.03 4
E(level): 11/2(505).
   178.9503/2+ 43 ps 4  μ=+1.4 4
E(level): 1/2(400). From 192Os(p,2nγ),(d,3nγ).
   343.23(7/2)+ 20.4 ps 8  μ=+1.40 6
E(level): 3/2(402). Unweighted average from 191Os β- decay and 191Pt ε decay.
   351.154(5/2)+ 18.8 ps 25  E(level): 1/2(400). From 192Os(p,2nγ),(d,3nγ).
   390.947/2- 240 ps 20  E(level): Kπ=(7/2-). From 191Os β- decay.
   502.61(9/2)+ 13.4 ps 19  μ=+2.38 23
E(level): 3/2(402). Unweighted average from 191Os β- decay and 191Pt ε decay.
   504.13(7/2+)   E(level): 1/2(400). From 192Os(p,2nγ),(d,3nγ).
   538.8543/2+ 9.8 ps 8  E(level): 1/2(411). From Coulomb excitation.
   556.64(13/2-)   E(level): 11/2(505).
   587.953/2+,5/2+ ≈ 0.3 ps XREF: γ(591).
   591.13(15/2-)   E(level): 11/2(505).
   624.07(1/2+) > 5 ps E(level): 1/2(411). From Coulomb excitation.
   653.99(9/2-)   E(level): Kπ=(7/2-). From 191Os β- decay.
   658.90(3/2-) < 0.12 ns E(level): Kπ=(3/2-).
   747.77(5/2)+   E(level): 1/2(411). From Coulomb excitation.
   799.79(5/2)-   E(level): Kπ=(3/2-).
   811.88(9/2+)   E(level): 1/2(400). From 192Os(p,2nγ),(d,3nγ).
   831.97(11/2+) 3.15 ps 19  E(level): 3/2(402). Unweighted average from 191Os β- decay and 191Pt ε decay.
   919.08(11/2-)   E(level): Kπ=(7/2-). From 191Os β- decay.
   927.80(7/2+)   E(level): 1/2(411). From Coulomb excitation.
   977.04(7/2-)   E(level): Kπ=(3/2-).
   991.28(11/2+)   E(level): 1/2(400). From 192Os(p,2nγ),(d,3nγ).
E(level)Jπ(level)T1/2(level)Comments
  1003.6(13/2+)   E(level): 3/2(402). Unweighted average from 191Os β- decay and 191Pt ε decay.
  1036.59(17/2-)   E(level): 11/2(505).
  1052.63   1987Pr10 from 191Ir(n,n’γ) and 1979Lu01 from 192Ir(p,2nγ) suggest Jπ=(9/2+); γ-branching ratios in (n,n’γ) and (p,2nγ) do not match.
E(level): 1987Pr10 from 191Ir(n,n’γ) and 1979Lu01 from 192Ir(p,2nγ) suggest Jπ=(9/2+); γ-branching ratios in (n,n’γ) and (p,2nγ) do not match.
  1138   L=1 or 2 in (3He,d) and (α,t).
E(level): L=1 or 2 in (3He,d) and (α,t).
  1206.57(7/2+,9/2+,11/2+)   XREF: E(1207.3).
  1206.89(9/2-)   XREF: E(1206.0)L(1207.7).
E(level): Kπ=(3/2-).
  1253.5(13/2-)   E(level): Kπ=(7/2-). From 191Os β- decay.
  1359   L=4 or 5 in (3He,d) and (α,t).
E(level): L=4 or 5 in (3He,d) and (α,t).
  1397.7(13/2+)   E(level): 1/2(400). From 192Os(p,2nγ),(d,3nγ).
  1418.1(15/2+)   E(level): 3/2(402). Unweighted average from 191Os β- decay and 191Pt ε decay.
  1433   L=3 or 4 (3He,d) and (α,t).
E(level): L=3 or 4 (3He,d) and (α,t).
  1600.1(17/2+)   E(level): 3/2(402). Unweighted average from 191Os β- decay and 191Pt ε decay.
  2112.1(19/2+)   E(level): 3/2(402). Unweighted average from 191Os β- decay and 191Pt ε decay.
  2312.1(21/2+)   E(level): 3/2(402). Unweighted average from 191Os β- decay and 191Pt ε decay.

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Additional Gamma Comments:

E(level)E(gamma)Comments
    82.423    82.413E(γ): Unweighted average from 191Os β- decay and 191Pt ε decay.
   129.413    47.05E(γ): From 191Os β- decay.
I(γ): From 191Os β- decay.
M(γ): from ce data in 191Os β- decay.
   129.416E(γ): Unweighted average from 191Os β- decay and 191Pt ε decay.
I(γ): From 191Os β- decay.
M(γ): from ce data in 191Os β- decay and 191Pt ε decay.
   171.29    41.89E(γ): Unweighted average from 191Os β- decay and 191Pt ε decay.
I(γ): From 191Os β- decay.
M(γ): from ce data in 191Os β- decay.
   300.4   121.5E(γ): From 192Os(p,2nγ),(d,3nγ).
   300.4E(γ): From 192Os(p,2nγ),(d,3nγ).
I(γ): From 192Os(p,2nγ).
   343.23   213.76E(γ): From 191Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in 191Ir(n,n’γ) dataset.
I(γ): From Coulomb excitation.
M(γ): from δ and RUL.
   343.32E(γ): From 191Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in 191Ir(n,n’γ) dataset.
I(γ): From Coulomb excitation.
M(γ): From Coulomb excitation.
   351.154   268.71M(γ): Mult=E2(+M1) with δ>3.6 from 191Pt ε decay, restricted by adopted spins.
   390.94   219.65M(γ): Mult=E2+(M1) with δ>3 in 191Pt ε decay; other level properties require multipolarity >1.
   502.61   159.38E(γ): From 191Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in 191Ir(n,n’γ) dataset.
I(γ): Weighted average of Coulomb excitation, 192Os(p,2nγ) and 191Ir(n,n’γ).
   373.20E(γ): From 191Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in 191Ir(n,n’γ) dataset.
I(γ): Weighted average of Coulomb excitation, 192Os(p,2nγ) and 191Ir(n,n’γ).
M(γ): From Coulomb excitation.
   504.13   152.9E(γ): From 191Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in 191Ir(n,n’γ) dataset.
I(γ): See also comment on 161.2γ Iγ.. Weighted average of Coulomb excitation, 192Os(p,2nγ) and 191Ir(n,n’γ).
M(γ): From 192Os(p,2nγ),(d,3nγ).
   161.2E(γ): From 192Os(p,2nγ),(d,3nγ).
I(γ): Unweighted average of Iγ(161.2)/Iγ(325.2)=1.21 17 in 192Os(p,2nγ) and 2.8 5 in 191Ir(n,n’γ); 161.2γ not seen in Coulomb excitation. Iγ(152.9γ)/Iγ(325.2γ) observed in all reactions in good agreement.
   325.2E(γ): From 192Os(p,2nγ),(d,3nγ).
I(γ): See also comment on 161.2γ Iγ.. Weighted average of Coulomb excitation, 192Os(p,2nγ) and 191Ir(n,n’γ).
   374.83E(γ): Multiply placed with intensity suitably divided. From 191Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in 191Ir(n,n’γ) dataset.
I(γ): γ multiply placed in 192Os(p,2nγ) and 191Ir(n,n’γ) but likely not in Coulomb excitation; see also comment on 161.2γ Iγ.. Multiply placed with intensity suitably divided. From Coulomb excitation.
   556.64   385.33E(γ): From 191Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in 191Ir(n,n’γ) dataset.
M(γ): From 192Os(p,2nγ),(d,3nγ).
   587.95   244.6E(γ): From Coulomb excitation.
I(γ): Other: 2.4(6) in 191Pt ε decay.. From Coulomb excitation.
   458.59I(γ): weighted average from 191Pt ε decay, 191Ir(n,n’γ), and Coulomb excitation.
   587.95I(γ): weighted average from 191Pt ε decay, 191Ir(n,n’γ), and Coulomb excitation.
   591.13   419.89E(γ): From 191Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in 191Ir(n,n’γ) dataset.
M(γ): From 192Os(p,2nγ),(d,3nγ).
   624.07   494.69M(γ): (M1,E2) from ce data. Decay scheme requires E2.
   653.99   263.08E(γ): From 191Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in 191Ir(n,n’γ) dataset.
I(γ): Other: Iγ>150 in 192Os(p,2nγ).. From Coulomb excitation.
   482.5E(γ): From 192Os(p,2nγ),(d,3nγ).
I(γ): This transition seems not to be a multiplet in Coulomb excitation; placed also from levels 825.4 and 1135.1 keV in other reactions.. From Coulomb excitation.
   658.90   267.92M(γ): Mult=E2(+M1) with δ>3 from 191Pt ε decay; see comment on 659 keV level Jπ for adopted multipolarity.
   576.46M(γ): RUL - see comment on 659 keV level Jπ.
E(level)E(gamma)Comments
   686.10   556.79E(γ): From 191Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in 191Ir(n,n’γ) dataset.
I(γ): From Coulomb excitation.
M(γ): From Coulomb excitation.
   686.02E(γ): From 191Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in 191Ir(n,n’γ) dataset.
I(γ): From Coulomb excitation.
M(γ): From Coulomb excitation.
   762.54   411.3I(γ): Other: 70(30) from 191Ir(n,n’γ).
   583.61I(γ): Other: 37(12) from 191Ir(n,n’γ).
   799.79   409.26E(γ): From 191Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in 191Ir(n,n’γ) dataset.
   811.88   308.03E(γ): From 191Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in 191Ir(n,n’γ) dataset.
I(γ): weighted average from 192Os(p,2nγ) and 192Os(d,3nγ).
M(γ): From 192Os(p,2nγ),(d,3nγ).
   460.43E(γ): From 191Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in 191Ir(n,n’γ) dataset.
I(γ): weighted average from 192Os(p,2nγ) and 192Os(d,3nγ).
   468.9E(γ): From 192Os(p,2nγ),(d,3nγ).
I(γ): weighted average from 192Os(p,2nγ) and 192Os(d,3nγ).
   816.59   645.30E(γ): From 191Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in 191Ir(n,n’γ) dataset.
   825.10   482.5E(γ): Multiply placed with undivided intensity. From 192Os(p,2nγ),(d,3nγ).
I(γ): Multiply placed with undivided intensity. From 192Os(p,2nγ).
   695.60E(γ): From 191Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in 191Ir(n,n’γ) dataset.
I(γ): From 192Os(p,2nγ).
   831.97   329.4E(γ): From 192Os(p,2nγ),(d,3nγ).
I(γ): From Coulomb excitation.
M(γ): From 192Os(p,2nγ),(d,3nγ).
   488.85E(γ): From 191Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in 191Ir(n,n’γ) dataset.
I(γ): From Coulomb excitation.
   877.65   374.83E(γ): Multiply placed with intensity suitably divided. From 191Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in 191Ir(n,n’γ) dataset.
I(γ): Multiply placed with intensity suitably divided. From 191Ir(n,n’γ).
   534.59E(γ): From 191Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in 191Ir(n,n’γ) dataset.
I(γ): From 191Ir(n,n’γ).
   919.08   264.8E(γ): From 192Os(p,2nγ),(d,3nγ).
I(γ): From 192Os(p,2nγ).
M(γ): From 192Os(p,2nγ),(d,3nγ).
   527.9E(γ): From 192Os(p,2nγ),(d,3nγ).
I(γ): From 192Os(p,2nγ).
   748.0E(γ): Other: 747.20 20, corrected value from 191Ir(n,n’γ).
I(γ): Corrected for Iγ(747.8γ) from 747.8 keV level using Iγ(747.8γ)/Iγ(209.0γ) from 191Pt ε decay and Iγ(209.0γ) from 192Os(p,2nγ).. From 192Os(p,2nγ).
   927.80   389.1E(γ): From 192Os(p,2nγ),(d,3nγ).
   425.5E(γ): From 192Os(p,2nγ),(d,3nγ).
   798.3E(γ): From 191Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in 191Ir(n,n’γ) dataset.
   945.4   259.0E(γ): From 192Os(p,2nγ),(d,3nγ).
I(γ): Weighted average of 192Os(p,2nγ) and 192Os(d,3nγ). See also comment on 816.0γ.
   443E(γ): From Coulomb excitation.
I(γ): Weighted average of Coulomb excitation and 191Ir(n,n’γ). See also comment on 816.0γ.
   603E(γ): From Coulomb excitation.
I(γ): See also comment on 816.0γ.. From Coulomb excitation.
   816.0E(γ): From 192Os(p,2nγ),(d,3nγ).
I(γ): Weighted average of Coulomb excitation, 192Os(p,2nγ), 192Os(d,3nγ), and 191Ir(n,n’γ). α different set of γ-ray transitions was seen decaying from 945.4 level in each reaction, this being the only common transition; all available data embodied in the adopted branching-ratios.
E(level)E(gamma)Comments
   963.2   372.1E(γ): From 192Os(p,2nγ),(d,3nγ).
   406.5E(γ): From 192Os(p,2nγ),(d,3nγ).
   977.04   177.25E(γ): From 191Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in 191Ir(n,n’γ) dataset.
I(γ): From 191Ir(n,n’γ).
   318.4E(γ): From 192Os(p,2nγ),(d,3nγ).
   586.2E(γ): Multiply placed with intensity suitably divided. From 191Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in 191Ir(n,n’γ) dataset.
I(γ): In 191Ir(n,n’γ), 586.2γ is a multiplet whose intensity could be properly divided.. Multiply placed with intensity suitably divided. From 191Ir(n,n’γ).
   991.28   178.7E(γ): From 192Os(p,2nγ),(d,3nγ).
   487.1E(γ): From 192Os(p,2nγ),(d,3nγ).
I(γ): From Coulomb excitation.
   489.0E(γ): From 192Os(p,2nγ),(d,3nγ).
I(γ): From Coulomb excitation.
  1003.6   172.0E(γ): From 192Os(p,2nγ),(d,3nγ).
   500.9E(γ): From 191Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in 191Ir(n,n’γ) dataset.
  1036.59   445.50E(γ): From 192Os(p,2nγ),(d,3nγ).
I(γ): from 192Os(d,3nγ), where it is a singlet (seen as a doublet in 191Ir(n,n’γ))
M(γ): From 192Os(p,2nγ),(d,3nγ).
   480E(γ): From 192Os(p,2nγ),(d,3nγ).
I(γ): from 192Os(d,3nγ), where it is multiply placed.
  1052.63   366.56E(γ): From 191Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in 191Ir(n,n’γ) dataset.
I(γ): From 191Ir(n,n’γ).
   549.8E(γ): From 191Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in 191Ir(n,n’γ) dataset.
I(γ): From 191Ir(n,n’γ).
   709.4E(γ): From 192Os(p,2nγ),(d,3nγ).
I(γ): Not seen in 191Ir(n,n’γ); deduced from Iγ(709γ):Iγ(550γ) =38 11:100 11 in (p,2nγ), where Iγ(367γ) was not given.. From 192Os(p,2nγ).
  1127.1   536.0E(γ): From 192Os(p,2nγ),(d,3nγ).
M(γ): From 192Os(p,2nγ),(d,3nγ).
  1135.23   216.8E(γ): From 192Os(p,2nγ),(d,3nγ).
I(γ): From 192Os(p,2nγ).
   482.5E(γ): Multiply placed with undivided intensity. From 192Os(p,2nγ),(d,3nγ).
I(γ): Multiply placed with undivided intensity. From 192Os(p,2nγ).
   743.6E(γ): From 191Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in 191Ir(n,n’γ) dataset.
I(γ): From 192Os(p,2nγ).
  1206.57   375.2E(γ): Multiply placed with undivided intensity. From 192Os(p,2nγ),(d,3nγ).
I(γ): Multiply placed with undivided intensity. From 192Os(p,2nγ).
   520.5E(γ): From 191Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in 191Ir(n,n’γ) dataset.
I(γ): Weighted average of Coulomb excitation and 191Ir(n,n’γ).
   703.81E(γ): From 191Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in 191Ir(n,n’γ) dataset.
I(γ): Weighted average of Coulomb excitation and 191Ir(n,n’γ).
  1206.89   229.85E(γ): Other: Eγ=228.6 5 in (p,2nγ).. From 191Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in 191Ir(n,n’γ) dataset.
  1210.5   332.5E(γ): From 192Os(p,2nγ),(d,3nγ).
I(γ): From 192Os(p,2nγ).
   556.8E(γ): From 192Os(p,2nγ),(d,3nγ).
I(γ): From 192Os(p,2nγ).
E(level)E(gamma)Comments
  1253.5   334.6E(γ): From 192Os(p,2nγ),(d,3nγ).
I(γ): From 192Os(d,3nγ).
   599.4E(γ): From 192Os(p,2nγ),(d,3nγ).
I(γ): From 192Os(d,3nγ).
  1297.19   793.0E(γ): From 191Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in 191Ir(n,n’γ) dataset.
I(γ): From 191Ir(n,n’γ).
   946.1E(γ): From 191Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in 191Ir(n,n’γ) dataset.
I(γ): From 191Ir(n,n’γ).
  1397.7   406.7E(γ): From 191Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in 191Ir(n,n’γ) dataset.
I(γ): From 191Ir(n,n’γ).
   585.2E(γ): From 192Os(p,2nγ),(d,3nγ).
I(γ): From 191Ir(n,n’γ).
  1400.9   715E(γ): From 192Os(p,2nγ),(d,3nγ).
   741.4E(γ): From 192Os(p,2nγ),(d,3nγ).
   898.9E(γ): From 192Os(p,2nγ),(d,3nγ).
  1418.1   414.3E(γ): From 192Os(p,2nγ),(d,3nγ).
I(γ): From Coulomb excitation.
   586.2E(γ): Multiply placed with undivided intensity. From 191Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in 191Ir(n,n’γ) dataset.
I(γ): In Coulomb excitation, 586.2γ is a doublet and the intensity could not be divided; 414.3γ was not seen in 191Ir(n,n’γ), where 586.2γ intensity could be divided.. Multiply placed with undivided intensity. From Coulomb excitation.
  1421.7   385.6E(γ): From 192Os(p,2nγ),(d,3nγ).
I(γ): From 192Os(p,2nγ).
   458.6E(γ): From 192Os(p,2nγ),(d,3nγ).
I(γ): From 192Os(p,2nγ).
   864.6E(γ): From 192Os(p,2nγ),(d,3nγ).
I(γ): From 192Os(p,2nγ).
  1600.1   596.5E(γ): From 192Os(p,2nγ),(d,3nγ).
  1645.9   518.8E(γ): From 192Os(p,2nγ),(d,3nγ).
  1651.6   524.5E(γ): From 192Os(p,2nγ),(d,3nγ).
  1680.6   553.5E(γ): From 192Os(p,2nγ),(d,3nγ).
M(γ): From 192Os(p,2nγ),(d,3nγ).
  2046.7   395.1E(γ): From 192Os(p,2nγ),(d,3nγ).
  2112.1   694E(γ): From Coulomb excitation.
  2312.1   712E(γ): From Coulomb excitation.

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