ADOPTED LEVELS, GAMMAS for 169Tm

Author: Coral M. Baglin |  Citation: Nucl. Data Sheets 109, 2033 (2008) |  Cutoff date: 15-Jun-2008 

 Full ENSDF file | Adopted Levels (PDF version) 


Q(β-)=-898.5 keV 12S(n)= 8033.6 keV 15S(p)= 5573.9 keV 12Q(α)= 1197.7 keV 13
Reference: 2012WA38

References:
  A  169Er β- decay  B  169Yb ε decay (32.018 d)
  C  168Er(p,p) IAR  D  168Er(3He,d), (α,t)
  E  169Tm(γ,γ):MOSSBAUER EFFECT  F  169Tm(E,E’p) IAR
  G  Coulomb Excitation  H  170Er(p,2nγ), (d,3nγ)
  I  169Tm(γ,γ’)  J  169Tm(n,n’γ), (pol n,n)
  K  169Tm(3He,3He’)  L  muonic atom

General Comments:

For hfs and/or isotope-shift data see, e.g., 1985Pf01, 1986Al32, 1986Pf03, 1987Mi31, 1988Al04, 1993Ji03, 1995Kr23, 1997Kr16.

For muonic isomer shift data, see 1974Ba77.

For discussion of anapole moment of 169Tm, see 1999KaZU.

Levels: band(c) 1/2[541], α=-1/2 band. See comment on signature partner band.

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
      0.0AB DE GH J   1/2+ STABLE      
      8.41017 11 AB DE GH J   3/2+ 4.09 ns 5       8.41017 15 
   100
M1+E2
      0.0
1/2+
    118.18945 11 AB D  GH J   5/2+ 62 ps 3     109.77924 3 
   118.18940 14 
   100.0 4 
    10.78 4 
M1+E2
E2
      8.41017
      0.0
3/2+
1/2+
    138.93315 12  B D  GH J   7/2+ 302 ps 2      20.752 9 
   130.52293 6 
     1.73 2 
   100.0 3 
M1+E2
E2
    118.18945
      8.41017
5/2+
3/2+
    316.14633 11  B D   H J   7/2+ 659.9 ns 23     177.21307 6 
   197.95675 7 
   307.73586 10 
    62.01 21 
   100
    27.96 9 
M1+E2
M1+E2
E2
    138.93315
    118.18945
      8.41017
7/2+
5/2+
3/2+
    332.116 11  B    GH J   9/2+ 18.8 ps 5     193.15 5 
   213.935 17 
   100.0
    45.9 10 
M1+E2
E2
    138.93315
    118.18945
7/2+
5/2+
    341.94 4    D   H J   (1/2-)      333.53 5 
   341.95 5 
   100 50 
    55 28 


      8.41017
      0.0
3/2+
1/2+
    345.028 3  B D   H J   5/2-      205.99 6 
   226.3 7 
   336.618 3 
    36 9 
     2.7 19 
   100 3 
E1

E1(+M2)
    138.93315
    118.18945
      8.41017
7/2+
5/2+
3/2+
    367.67 5  B    GH J   11/2+ 41.6 ps 21     228.71 5 
   100
E2
    138.93315
7/2+
    379.26678 12  B     H     7/2- 52.2 ns 8      63.12044 4 
   240.331 3 
   261.07712 9 
   370.854 8 
   379.284 18 
   100.0 4 
     0.261 14 
     3.850 16 
     0.00202 21 
     0.00068 26 
E1
E1(+M2)
E1+M2
[M2]
[E3]
    316.14633
    138.93315
    118.18945
      8.41017
      0.0
7/2+
7/2+
5/2+
3/2+
1/2+
    430.122 11  B D   H J   (9/2)-       84.9 5 ?
   291.188 11 
    20 11 
   100 9 

E1
    345.028
    138.93315
5/2-
7/2+
    433.521 18  B     H     (9/2)+      101.41?
   117.376 19 
   294.54 11 
   <18
   100 6 
     2.4 6 

[M1,E2]
M1
    332.116
    316.14633
    138.93315
9/2+
7/2+
7/2+
    472.88128 14  B     H     9/2- 0.14 ns 7      93.61447 8 
   105.19 10 
   156.724 11 
   333.963 13 
   100.0 6 
     0.10 3 
     0.383 10 
     0.0675 24 
M1+E2
E1
E1
[E1]
    379.26678
    367.67
    316.14633
    138.93315
7/2-
11/2+
7/2+
7/2+
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
    474.968 9  B D   H J   (3/2)-      356.74 5 
   466.2 2 
   474.970 9 
    72 3 
    10.0 11 
   100.0 22 



    118.18945
      8.41017
      0.0
5/2+
3/2+
1/2+
    570.830 11  B D  GH J   3/2+ 10 ps 7     452.62 8 
   562.410 12 
   570.89 3 
    15 5 
   100.0 21 
    94 6 
M1+E2
M1+E2
M1+E2
    118.18945
      8.41017
      0.0
5/2+
3/2+
1/2+
    575.38 4        H     (11/2+)      141.85 5 
   259.23 5 
   100 10 
    96 48 


    433.521
    316.14633
(9/2)+
7/2+
    588.20 5    D   H     11/2-      115.32 5 
   208.8 5 
   100 10 
    10 5 
(M1+E2)

    472.88128
    379.26678
9/2-
7/2-
    602.82 19        H     (13/2-)      172.7 5 
   235.1 2 
    16 8 
   100 10 

(E1(+M2))
    430.122
    367.67
(9/2)-
11/2+
    633.292 3  B D  GH J   5/2+ 0.27 ps    494.357 8 
   515.101 6 
   624.881 4 
   633.32 10 
    29.8 5 
    84.5 12 
   100.0 25 
     0.140 9 
M1
M1
M1
[E2]
    138.93315
    118.18945
      8.41017
      0.0
7/2+
5/2+
3/2+
1/2+
    637.08 13       GH     13/2+ 5.4 ps 4     269.4 2 
   305.2 2 
    98.4 24 
   100
M1+E2
E2
    367.67
    332.116
11/2+
9/2+
    646.758 10  B D   H J   (7/2-)      171.6 5 
   216.4 2 
   301.6 2 
   314.6 2 
   507.8 3 
   528.569 10 
    10 5 
     5.0
     5.6
    22
     1.2 7 
   100.0 24 






    474.968
    430.122
    345.028
    332.116
    138.93315
    118.18945
(3/2)-
(9/2)-
5/2-
9/2+
7/2+
5/2+
    691.24 16       GH     15/2+ 8.1 ps 4     323.4 2 
   100
E2
    367.67
11/2+
    718.786 4  B    GH J   (7/2+)       72.028?
   386.671 13 
   579.851 5 
   600.603 8 
   710.354 15 
  <186
    17.4 4 
   100.0 17 
    59.1 9 
     1.77 9 

[M1,E2]
(M1)
(M1)

    646.758
    332.116
    138.93315
    118.18945
      8.41017
(7/2-)
9/2+
7/2+
5/2+
3/2+
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
    725.44 7        H     13/2-      137.26 5 
   252.5 2 
   100 10 
    29 3 
(M1+E2)

    588.20
    472.88128
11/2-
9/2-
    741.25 6        H     (13/2+)      165.8 2 
   307.74 5 
   100 9 
   <57


    575.38
    433.521
(11/2+)
(9/2)+
    781.796 6  B D   H J   (5/2)+      210.94 5 
   465.65
   642.873 9 
   663.599 7 
   773.386 14 
   781.64 8 
    53
    91.2 10 
    36.5 9 
    92.3 26 
   100.0 15 
     1.44 12 






    570.830
    316.14633
    138.93315
    118.18945
      8.41017
      0.0
3/2+
7/2+
7/2+
5/2+
3/2+
1/2+
    832.42 7  B     H J   (9/2+)      464.7
   500.35 10 
   693.46 8 
    41 24 
   100 9 
    98 5 



    367.67
    332.116
    138.93315
11/2+
9/2+
7/2+
    865.9 4        H     (17/2-)      175.0 5 
   262.7 5 
    41 22 
   100 16 


    691.24
    602.82
15/2+
(13/2-)
    878.35 10  B       J   (7/2+)      546.16 22 
   739.42 11 
   760.24 24 
    80 22 
   100 12 
    45 12 



    332.116
    138.93315
    118.18945
9/2+
7/2+
5/2+
    883.75 14        H     15/2-      158.3 2 
   295.4 2 
   100 10 
   <78
(M1(+E2))

    725.44
    588.20
13/2-
11/2-
    884.62 20    D   H     (11/2-)      281.7 2 ?
   454.5 2 
   552.0 2 ?
    36
    21
   100



    602.82
    430.122
    332.116
(13/2-)
(9/2)-
9/2+
   ≈900?      G          ≈900?
   100

      0.0
1/2+
    929.37 19        H     (15/2+)      188.7 5 
   353.9 2 
    37 21 
   100 10 


    741.25
    575.38
(13/2+)
(11/2+)
    938 2    D                
    964.0 4        H     (11/2+)      595.9 5 
   632.3 5 
   100
    72 38 


    367.67
    332.116
11/2+
9/2+
   1027.85 16       GH     17/2+ 1.91 ps 18     336.60 5 
   391.0 2 
    58.7 7 
   100
M1+E2
E2
    691.24
    637.08
15/2+
13/2+
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   1039.95 15        H          565.2 2 
   694.7 2 
    37
   100


    474.968
    345.028
(3/2)-
5/2-
   1058.54 21        H          716.6 2 
   100

    341.94
(1/2-)
   1063.57 16        H     17/2-      179.6 2 
   338.3 2 
    90 9 
   100 10 


    883.75
    725.44
15/2-
13/2-
   1104.18 25       GH     19/2+ 1.94 ps 21     413.0 2 
   100
E2
    691.24
15/2+
   1112.6 5 ?       H          682.5 5 ?
   100

    430.122
(9/2)-
   1135.93 20        H          790.9 2 
   100

    345.028
5/2-
   1140.85 21        H     (17/2+)      210.94 5 
   399.6 2 
   <39
   100


    929.37
    741.25
(15/2+)
(13/2+)
   1152 2    D         (11/2-)        
   1188.7 3        H     (15/2-)      552.0 2 ?
   585.9 2 
  <189
   100 10 


    637.08
    602.82
13/2+
(13/2-)
   1190 20       G      +     1190 20 
   100

      0.0
1/2+
   1218.1 5        H     (21/2-)      352.2 2 
   100

    865.9
(17/2-)
   1223.04 15        H          877.9 2 
   881.2 2 
   100
    75


    345.028
    341.94
5/2-
(1/2-)
   1243 2    D                
   1262.40 21        H     19/2-      198.3 5 
   378.7 2 
  <185
   100


   1063.57
    883.75
17/2-
15/2-
   1300.8 6        H     (15/2+)      609.6 5 
   100

    691.24
15/2+
   1372 2    D         1/2+        
   1372.1 6        H     (19/2+)      442.7 5 
   100

    929.37
(15/2+)
   1400 2    D                
   1482.94 22        H     21/2-      220.5 2 
   419.4 2 
   100 10 
    77 8 


   1262.40
   1063.57
19/2-
17/2-
   1497.8 4       GH     21/2+ 0.87 ps 9     394.0 5 
   469.6 5 
    34 13 
   100 50 

E2
   1104.18
   1027.85
19/2+
17/2+
   1510.6 10         I    (1/2,3/2)+     1510.6
   100

      0.0
1/2+
   1515 2    D                
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   1527.5 10         I    (1/2,3/2)+     1527.5
   100

      0.0
1/2+
   1548.4 7 ?       H     (19/2-)      682.5 5 ?
   100

    865.9
(17/2-)
   1598.4 4 ?      GH     (23/2+)      494.2 2 ?
   100

   1104.18
19/2+
   1625.3 6        H     (21/2+)      484.4 5 
   100

   1140.85
(17/2+)
   1658.1 5        H     (25/2-)      440.0 2 
   100

   1218.1
(21/2-)
   1716.9 3        H     23/2-      233?
   454.5 2 
 
 


   1482.94
   1262.40
21/2-
19/2-
   1864.6 7         I    (1/2,3/2)+     1856.2
  1864.6
   100 26 
    47


      8.41017
      0.0
3/2+
1/2+
   1910.5 6         I    (1/2,3/2)+     1792.3
  1902.1
  1910.5
   100 10 
    46 5 
    98



    118.18945
      8.41017
      0.0
5/2+
3/2+
1/2+
   1922.3 7         I    (1/2,3/2)+     1804.1
  1922.3
   100 46 
    79


    118.18945
      0.0
5/2+
1/2+
   1963.7 10         I    (1/2,3/2)     1963.7
   100

      0.0
1/2+
   1978.4 10         I    (1/2,3/2)     1978.4
   100

      0.0
1/2+
   1991.7 7         I    (1/2,3/2)+     1983.3
  1991.7
    79 36 
   100


      8.41017
      0.0
3/2+
1/2+
   2075.5 7         I    (1/2,3/2)+     2067.1
  2075.5
   100 74 
    89


      8.41017
      0.0
3/2+
1/2+
   2168.7 7         I    (1/2,3/2)+     2160.3
  2168.7
   100 38 
    72


      8.41017
      0.0
3/2+
1/2+
   2190.6 10         I    (1/2,3/2)     2190.6
   100

      0.0
1/2+
   2215.3 10         I    (1/2,3/2)     2215.3
   100

      0.0
1/2+
   2236.1 7         I    (1/2,3/2)+     2117.9
  2236.1
    56 16 
   100


    118.18945
      0.0
5/2+
1/2+
   2262.5 7         I    (1/2,3/2)+     2144.3
  2262.5
   100 31 
    72


    118.18945
      0.0
5/2+
1/2+
   2293.8 10         I    (1/2,3/2)     2293.8
   100

      0.0
1/2+
   2306.3 10         I    (1/2,3/2)     2306.3
   100

      0.0
1/2+
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   2312.2 7         I    (1/2,3/2)+     2194.0
  2312.2
   100 37 
    92


    118.18945
      0.0
5/2+
1/2+
   2386.6 10         I    (1/2,3/2)     2386.6
   100

      0.0
1/2+
   2455.8 7         I    (1/2,3/2)     2447.4
  2455.8
    43 27 
   100


      8.41017
      0.0
3/2+
1/2+
   2466.0 10         I    (1/2,3/2)     2466.0
   100

      0.0
1/2+
   2492.0 7         I    (1/2,3/2)+     2373.8
  2492.0
    47 13 
   100


    118.18945
      0.0
5/2+
1/2+
   2553.4 7         I    (1/2,3/2)     2435.2
  2553.4
   100 43 
    64


    118.18945
      0.0
5/2+
1/2+
   2571.4 10         I    (1/2,3/2)     2571.4
   100

      0.0
1/2+
   2598.6 10         I    (1/2,3/2)+     2598.6
   100

      0.0
1/2+
   2602.8 10         I    (1/2,3/2)     2602.8
   100

      0.0
1/2+
   2687.0 10         I    (1/2,3/2)     2687.0
   100

      0.0
1/2+
   2749.4 7         I    (1/2,3/2)+     2741.0
  2749.4
    96 41 
   100


      8.41017
      0.0
3/2+
1/2+
   2756.4 10         I    (1/2,3/2)     2756.4
   100

      0.0
1/2+
   2769.1 7         I    (1/2,3/2)+     2760.7
  2769.1
    41 11 
   100


      8.41017
      0.0
3/2+
1/2+
   2786.5 10         I    (1/2,3/2)     2786.5
   100

      0.0
1/2+
   2814.2 7         I    (1/2,3/2)     2805.8
  2814.2
    89 79 
   100


      8.41017
      0.0
3/2+
1/2+
   2818.6 10         I    (1/2,3/2)     2818.6
   100

      0.0
1/2+
   2843.1 10         I    (1/2,3/2)     2843.1
   100

      0.0
1/2+
   2861.1 10         I    (1/2,3/2)+     2861.1
   100

      0.0
1/2+
   2943.3 6         I    (1/2,3/2)+     2825.1
  2934.9
  2943.3
    63 56 
   100 70 
    70



    118.18945
      8.41017
      0.0
5/2+
3/2+
1/2+
   2996.2 7         I    (1/2,3/2)+     2878.0
  2996.2
   100 26 
    89


    118.18945
      0.0
5/2+
1/2+
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   3127.6 10         I    (1/2,3/2)     3127.6
   100

      0.0
1/2+
   3175.6 10         I    (1/2,3/2)     3175.6
   100

      0.0
1/2+
   3185.0 10         I    (1/2,3/2)     3185.0
   100

      0.0
1/2+
   3187.5 10         I    (1/2,3/2)     3187.5
   100

      0.0
1/2+
   3191.3 7         I    (1/2,3/2)+     3182.9
  3191.3
    82 33 
   100


      8.41017
      0.0
3/2+
1/2+
   3199.7 10         I    (1/2,3/2)+     3199.7
   100

      0.0
1/2+
   3204.8 7         I    (1/2,3/2)+     3086.6
  3204.8
    56 19 
   100


    118.18945
      0.0
5/2+
1/2+
   3254.6 7         I    (1/2,3/2)     3246.2
  3254.6
   100 53 
    69


      8.41017
      0.0
3/2+
1/2+
   3274.5 10         I    (1/2,3/2)+     3274.5
   100

      0.0
1/2+
   3286.5 10         I    (1/2,3/2)+     3286.5
   100

      0.0
1/2+
   3299.6 7         I    (1/2,3/2)+     3291.2
  3299.6
   100 75 
    96


      8.41017
      0.0
3/2+
1/2+
   3308.4 10         I    (1/2,3/2)     3308.4
   100

      0.0
1/2+
   3341.2 7         I    (1/2,3/2)+     3332.8
  3341.2
    47 18 
   100


      8.41017
      0.0
3/2+
1/2+
   3376.4 7         I    (1/2,3/2)+     3368.0
  3376.4
   100 33 
    96


      8.41017
      0.0
3/2+
1/2+
   3383.9 10         I    (1/2,3/2)     3383.9
   100

      0.0
1/2+
   3419.2 10         I    (1/2,3/2)     3419.2
   100

      0.0
1/2+
   3436.3 7         I    (1/2,3/2)     3318.1
  3436.3
    67 43 
   100


    118.18945
      0.0
5/2+
1/2+
   3442.0 10         I    (1/2,3/2)     3442.0
   100

      0.0
1/2+
   3458.6 10         I    (1/2,3/2)     3458.6
   100

      0.0
1/2+
   3475.7 7         I    (1/2,3/2)+     3467.3
  3475.7
   100 41 
    47


      8.41017
      0.0
3/2+
1/2+
   3480.3 10         I    (1/2,3/2)     3480.3
   100

      0.0
1/2+
   3497.0 10         I    (1/2,3/2)     3497.0
   100

      0.0
1/2+
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   3527.0 7         I    (1/2,3/2)     3518.6
  3527.0
   100 72 
    72


      8.41017
      0.0
3/2+
1/2+
   3538.7 10         I    (1/2,3/2)     3538.7
   100

      0.0
1/2+
   3541.9 7         I    (1/2,3/2)+     3423.7
  3541.9
   100 42 
   100


    118.18945
      0.0
5/2+
1/2+
   3573.3 10         I    (1/2,3/2)     3573.3
   100

      0.0
1/2+
   3613.0 10         I    (1/2,3/2)     3613.0
   100

      0.0
1/2+
   3624.8 6         I    (1/2,3/2)+     3506.6
  3616.4
  3624.8
   100 26 
    86 23 
   100



    118.18945
      8.41017
      0.0
5/2+
3/2+
1/2+
   3724.7 7         I    (1/2,3/2)+     3606.5
  3724.7
   100 26 
   100


    118.18945
      0.0
5/2+
1/2+
   3736.2 10         I    (1/2,3/2)     3736.2
   100

      0.0
1/2+
   3741.7 10         I    (1/2,3/2)     3741.7
   100

      0.0
1/2+
   3766.3 10         I    (1/2,3/2)     3766.3
   100

      0.0
1/2+
   3795.8 7         I    (1/2,3/2)     3787.3
  3795.7
     1.0E2 13 
    61


      8.41017
      0.0
3/2+
1/2+
   3806.7 10         I    (1/2,3/2)     3806.7
   100

      0.0
1/2+
   3862.5 10         I    (1/2,3/2)     3862.5
   100

      0.0
1/2+
   3875.3 10         I    (1/2,3/2)     3875.3
   100

      0.0
1/2+
   3916.8 10         I    (1/2,3/2)     3916.8
   100

      0.0
1/2+
   3950.2 10         I    (1/2,3/2)     3950.2
   100

      0.0
1/2+
   4103.6 10         I    (1/2,3/2)     4103.5
   100

      0.0
1/2+
   4190.2 7         I    (1/2,3/2)     4181.7
  4190.1
     1.0E2 10 
    56


      8.41017
      0.0
3/2+
1/2+
   4279.7 10         I    (1/2,3/2)     4279.6
   100

      0.0
1/2+
   4764.5 10         I    (1/2,3/2)     4764.4
   100

      0.0
1/2+
   4789.8 10         I    (1/2,3/2)     4789.7
   100

      0.0
1/2+
   4853.0 10         I    (1/2,3/2)     4852.9
   100

      0.0
1/2+
   4865.5 7         I    (1/2,3/2)     4857.0
  4865.4
     1.0E2 11 
    69


      8.41017
      0.0
3/2+
1/2+
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   4954.0 10         I    (1/2,3/2)     4953.9
   100

      0.0
1/2+
   5211.5 10         I    (1/2,3/2)+     5211.4
   100

      0.0
1/2+
   5507.1 10         I    (1/2,3/2)     5507
   100

      0.0
1/2+
   5529.9 10         I    (1/2,3/2)+     5529.8
   100

      0.0
1/2+
   5593.3 7         I    (1/2,3/2)     5584.8
  5593.2
    69 81 
   100


      8.41017
      0.0
3/2+
1/2+
   5598.3 10         I    (1/2,3/2)     5598.2
   100

      0.0
1/2+
      1.47E+4 3           K         
      1.576E+4 13      F              
  16102  C          1/2-        
      1.634E+4 14      F       (1/2)-        

E(level): Least-squares adjusted values based on adopted Eγ, with E(8.4 level) held fixed at 8.41017 15, the difference between E(118γ) and E(110γ), except where noted or where cross references clearly indicate a different source.

Jπ(level): Based on coincidence data, rotational structure, and γ-ray angular distributions in 170Er(p,2nγ), (d,3nγ), except where noted. Definite Jπ is assigned to members of bands defined by a cascade of transitions having regularly changing energies provided the Jπ of at least one member and the multipolarity of at least one intraband transition have been independently determined.

I(γ): Relative photon branching from each level; values are from 169Yb ε decay (32.018 d), except where noted; upper limits are given for photon branchings affected by multiple placement or by presence of contaminant.

Back to top

Band Transitions:

E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 1 - 1/2[411] band.
      0.0 1/2+ STABLE      
      8.41017 11  3/2+ 4.09 ns 5       8.41017 15 
   100
M1+E2
      0.0
1/2+
    118.18945 11  5/2+ 62 ps 3     109.77924 3 
   118.18940 14 
   100.0 4 
    10.78 4 
M1+E2
E2
      8.41017
      0.0
3/2+
1/2+
    138.93315 12  7/2+ 302 ps 2      20.752 9 
   130.52293 6 
     1.73 2 
   100.0 3 
M1+E2
E2
    118.18945
      8.41017
5/2+
3/2+
    332.116 11  9/2+ 18.8 ps 5     193.15 5 
   213.935 17 
   100.0
    45.9 10 
M1+E2
E2
    138.93315
    118.18945
7/2+
5/2+
    367.67 5  11/2+ 41.6 ps 21     228.71 5 
   100
E2
    138.93315
7/2+
    637.08 13  13/2+ 5.4 ps 4     269.4 2 
   305.2 2 
    98.4 24 
   100
M1+E2
E2
    367.67
    332.116
11/2+
9/2+
    691.24 16  15/2+ 8.1 ps 4     323.4 2 
   100
E2
    367.67
11/2+
   1027.85 16  17/2+ 1.91 ps 18     336.60 5 
   391.0 2 
    58.7 7 
   100
M1+E2
E2
    691.24
    637.08
15/2+
13/2+
   1104.18 25  19/2+ 1.94 ps 21     413.0 2 
   100
E2
    691.24
15/2+
   1497.8 4  21/2+ 0.87 ps 9     394.0 5 
   469.6 5 
    34 13 
   100 50 

E2
   1104.18
   1027.85
19/2+
17/2+
   1598.4 4  (23/2+)      494.2 2 ?
   100

   1104.18
19/2+
E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 2 - 7/2[404] band.
    316.14633 11  7/2+ 659.9 ns 23       
    433.521 18  (9/2)+      101.41?
   117.376 19 
   294.54 11 
   <18
   100 6 
     2.4 6 

[M1,E2]
M1
    332.116
    316.14633
    138.93315
9/2+
7/2+
7/2+
    575.38 4  (11/2+)      141.85 5 
   259.23 5 
   100 10 
    96 48 


    433.521
    316.14633
(9/2)+
7/2+
    741.25 6  (13/2+)      165.8 2 
   307.74 5 
   100 9 
   <57


    575.38
    433.521
(11/2+)
(9/2)+
    929.37 19  (15/2+)      188.7 5 
   353.9 2 
    37 21 
   100 10 


    741.25
    575.38
(13/2+)
(11/2+)
   1140.85 21  (17/2+)      210.94 5 
   399.6 2 
   <39
   100


    929.37
    741.25
(15/2+)
(13/2+)
   1372.1 6  (19/2+)      442.7 5 
   100

    929.37
(15/2+)
   1625.3 6  (21/2+)      484.4 5 
   100

   1140.85
(17/2+)
E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 3 - 1/2[541], α=+1/2 band.
    341.94 4  (1/2-)        
    345.028 3  5/2-      205.99 6 
   226.3 7 
   336.618 3 
    36 9 
     2.7 19 
   100 3 
E1

E1(+M2)
    138.93315
    118.18945
      8.41017
7/2+
5/2+
3/2+
    430.122 11  (9/2)-       84.9 5 ?
   291.188 11 
    20 11 
   100 9 

E1
    345.028
    138.93315
5/2-
7/2+
    602.82 19  (13/2-)      172.7 5 
   235.1 2 
    16 8 
   100 10 

(E1(+M2))
    430.122
    367.67
(9/2)-
11/2+
    865.9 4  (17/2-)      175.0 5 
   262.7 5 
    41 22 
   100 16 


    691.24
    602.82
15/2+
(13/2-)
   1218.1 5  (21/2-)      352.2 2 
   100

    865.9
(17/2-)
   1658.1 5  (25/2-)      440.0 2 
   100

   1218.1
(21/2-)
E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 4 - 7/2[523] band.
    379.26678 12  7/2- 52.2 ns 8       
    472.88128 14  9/2- 0.14 ns 7      93.61447 8 
   105.19 10 
   156.724 11 
   333.963 13 
   100.0 6 
     0.10 3 
     0.383 10 
     0.0675 24 
M1+E2
E1
E1
[E1]
    379.26678
    367.67
    316.14633
    138.93315
7/2-
11/2+
7/2+
7/2+
    588.20 5  11/2-      115.32 5 
   208.8 5 
   100 10 
    10 5 
(M1+E2)

    472.88128
    379.26678
9/2-
7/2-
    725.44 7  13/2-      137.26 5 
   252.5 2 
   100 10 
    29 3 
(M1+E2)

    588.20
    472.88128
11/2-
9/2-
    883.75 14  15/2-      158.3 2 
   295.4 2 
   100 10 
   <78
(M1(+E2))

    725.44
    588.20
13/2-
11/2-
   1063.57 16  17/2-      179.6 2 
   338.3 2 
    90 9 
   100 10 


    883.75
    725.44
15/2-
13/2-
   1262.40 21  19/2-      198.3 5 
   378.7 2 
  <185
   100


   1063.57
    883.75
17/2-
15/2-
   1482.94 22  21/2-      220.5 2 
   419.4 2 
   100 10 
    77 8 


   1262.40
   1063.57
19/2-
17/2-
   1716.9 3  23/2-      233?
   454.5 2 
 
 


   1482.94
   1262.40
21/2-
19/2-
E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 5 - 3/2[411] band + 1/2[411] γ vibration.
    570.830 11  3/2+ 10 ps 7       
    633.292 3  5/2+ 0.27 ps    494.357 8 
   515.101 6 
   624.881 4 
   633.32 10 
    29.8 5 
    84.5 12 
   100.0 25 
     0.140 9 
M1
M1
M1
[E2]
    138.93315
    118.18945
      8.41017
      0.0
7/2+
5/2+
3/2+
1/2+
    718.786 4  (7/2+)       72.028?
   386.671 13 
   579.851 5 
   600.603 8 
   710.354 15 
  <186
    17.4 4 
   100.0 17 
    59.1 9 
     1.77 9 

[M1,E2]
(M1)
(M1)

    646.758
    332.116
    138.93315
    118.18945
      8.41017
(7/2-)
9/2+
7/2+
5/2+
3/2+
    832.42 7  (9/2+)      464.7
   500.35 10 
   693.46 8 
    41 24 
   100 9 
    98 5 



    367.67
    332.116
    138.93315
11/2+
9/2+
7/2+
    964.0 4  (11/2+)      595.9 5 
   632.3 5 
   100
    72 38 


    367.67
    332.116
11/2+
9/2+
   1300.8 6  (15/2+)      609.6 5 
   100

    691.24
15/2+
E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 6 - 5/2[402] band.
    781.796 6  (5/2)+        
    878.35 10  (7/2+)      546.16 22 
   739.42 11 
   760.24 24 
    80 22 
   100 12 
    45 12 



    332.116
    138.93315
    118.18945
9/2+
7/2+
5/2+
E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 7 - 9/2[514] band
   1152 2  (11/2-)        

Back to top

Additional Gamma Data:















E(level)
(keV)
Jπ(level)T1/2(level)E(γ)
(keV)
MultipolarityMixing
Ratio
Conversion
Coefficient
Additional Data
      8.41017 3/2+ 4.09 ns 5       8.41017 15 M1+E20.0328 5263B(E2)(W.u.)=241 10, B(M1)(W.u.)=0.0342 8, α=263 5
    118.18945 5/2+ 62 ps 3     109.77924 3 M1+E2-0.139 102.37B(E2)(W.u.)=53 8, B(M1)(W.u.)=0.072 4, α=2.37
5/2+ 62 ps 3     118.18940 14 E2 1.642B(E2)(W.u.)=210 11, α=1.642
    138.93315 7/2+ 302 ps 2      20.752 9 M1+E20.0292 1654.9B(E2)(W.u.)=42 5, B(M1)(W.u.)=0.0454 13, α=54.9 9
7/2+ 302 ps 2     130.52293 6 E2 1.143B(E2)(W.u.)=287 5, α=1.143
    316.14633 7/2+ 659.9 ns 23     177.21307 6 M1+E2-0.30 130.594B(E2)(W.u.)=0.0017 14, B(M1)(W.u.)=1.25E-6 10, α=0.594 19
7/2+ 659.9 ns 23     197.95675 7 M1+E2-0.326 60.433B(E2)(W.u.)=0.00180 7, B(M1)(W.u.)=1.430E-6 14, α=0.433
7/2+ 659.9 ns 23     307.73586 10 E2 0.0662B(E2)(W.u.)=0.000576 4, α=0.0662
    332.116 9/2+ 18.8 ps 5     193.15 5 M1+E2-0.126 210.479B(E2)(W.u.)=16 6, B(M1)(W.u.)=0.0787 22, α=0.479 1
9/2+ 18.8 ps 5     213.935 17 E2 0.208B(E2)(W.u.)=273 10, α=0.208
    345.028 5/2-      205.99 6 E1 0.0497α=0.0497
5/2-      336.618 3 E1(+M2)0.66 LE0.07α=0.07 6
    367.67 11/2+ 41.6 ps 21     228.71 5 E2 0.1673B(E2)(W.u.)=336 17, α=0.1673
    379.26678 7/2- 52.2 ns 8      63.12044 4 E1 1.098B(E1)(W.u.)=7.88E-6 17, α=1.098
7/2- 52.2 ns 8     240.331 3 E1(+M2)+0.12 LT0.042B(E1)(W.u.)>3.5E-10, B(M2)(W.u.)<0.00044, α=0.042 9
7/2- 52.2 ns 8     261.07712 9 E1+M2-0.07 30.032B(E1)(W.u.)=4.26E-9 9, B(M2)(W.u.)=0.0014 12, α=0.032 5
7/2- 52.2 ns 8     370.854 8 [M2] 0.300B(M2)(W.u.)=2.6×10-5 3, α=0.300
7/2- 52.2 ns 8     379.284 18 [E3] 0.1270B(E3)(W.u.)=0.039 15, α=0.1270
    430.122 (9/2)-      291.188 11 E1 0.0207α=0.0207
    433.521 (9/2)+      117.376 19 [M1,E2] 1.82α=1.82 14
(9/2)+      294.54 11 M1 0.1522α=0.1522
    472.88128 9/2- 0.14 ns 7      93.61447 8 M1+E2+0.183 33.75B(E2)(W.u.)=70 40, B(M1)(W.u.)=0.039 20, α=3.75
9/2- 0.14 ns 7     105.19 10 E1 0.292B(E1)(W.u.)=2.9E-7 17, α=0.292
9/2- 0.14 ns 7     156.724 11 E1 0.1016B(E1)(W.u.)=3.3E-7 17, α=0.1016
9/2- 0.14 ns 7     333.963 13 [E1] 0.01480B(E1)(W.u.)=6E-9 3, α=0.01480
E(level)
(keV)
Jπ(level)T1/2(level)E(γ)
(keV)
MultipolarityMixing
Ratio
Conversion
Coefficient
Additional Data
    570.830 3/2+ 10 ps 7     452.62 8 M1+E21.5 +9-40.030B(E2)(W.u.)=2.6 23, B(M1)(W.u.)=0.0005 5, α=0.030 5
3/2+ 10 ps 7     562.410 12 M1+E20.8 +5-40.022B(E2)(W.u.)=3 +4-3, B(M1)(W.u.)=0.004 3, α=0.022 4
3/2+ 10 ps 7     570.89 3 M1+E20.8 +5-40.021B(E2)(W.u.)=3 3, B(M1)(W.u.)=0.003 3, α=0.021 4
    588.20 11/2-      115.32 5 (M1+E2) 1.93α=1.93 14
    602.82 (13/2-)      235.1 2 (E1(+M2)) 0.7α=0.7 7
    633.292 5/2+ 0.27 ps    494.357 8 M1 0.0389B(M1)(W.u.)=0.091, α=0.0389
5/2+ 0.27 ps    515.101 6 M1 0.0350B(M1)(W.u.)=0.23, α=0.0350
5/2+ 0.27 ps    624.881 4 M1 0.0214B(M1)(W.u.)=0.15, α=0.0214
5/2+ 0.27 ps    633.32 10 [E2] 0.00959B(E2)(W.u.)=0.24, α=0.00959
    637.08 13/2+ 5.4 ps 4     269.4 2 M1+E2-0.149 260.192B(E2)(W.u.)=13 5, B(M1)(W.u.)=0.090 8, α=0.192
13/2+ 5.4 ps 4     305.2 2 E2 0.0678B(E2)(W.u.)=318 24, α=0.0678
    691.24 15/2+ 8.1 ps 4     323.4 2 E2 0.0571B(E2)(W.u.)=337 17, α=0.0571
    718.786 (7/2+)      386.671 13 [M1,E2] 0.054α=0.054 20
(7/2+)      579.851 5 (M1) 0.0259α=0.0259
(7/2+)      600.603 8 (M1) 0.0237α=0.0237
    725.44 13/2-      137.26 5 (M1+E2) 1.11α=1.11 16
    883.75 15/2-      158.3 2 (M1(+E2)) 0.71α=0.71 14
   1027.85 17/2+ 1.91 ps 18     336.60 5 M1+E2-0.18 30.1048B(E2)(W.u.)=14 5, B(M1)(W.u.)=0.102 10, α=0.1048 16
17/2+ 1.91 ps 18     391.0 2 E2 0.0331B(E2)(W.u.)=350 40, α=0.0331
   1104.18 19/2+ 1.94 ps 21     413.0 2 E2 0.0284B(E2)(W.u.)=430 50, α=0.0284
   1497.8 21/2+ 0.87 ps 9     469.6 5 E2 0.0201B(E2)(W.u.)=340 220, α=0.0201

Back to top

Additional Level Data and Comments:

E(level)Jπ(level)T1/2(level)Comments
      0.01/2+ STABLE μ=-0.2316 15
No α decay observed (T1/2(α)>5×1016 y if 1.5|<E(α)|<3.7, 1956Po16).
E(level): No α decay observed (T1/2(α)>5×1016 y if 1.5|<E(α)|<3.7, 1956Po16). From 170Er(p,2nγ), (d,3nγ). 1/2[411] band.
      8.410173/2+ 4.09 ns 5  Q=-1.2 1, μ=+0.5148 48
E(level): From 170Er(p,2nγ), (d,3nγ). 1/2[411] band.
    118.189455/2+ 62 ps 3  μ=+0.761 45
E(level): 1/2[411] band.
Jπ(level): Definite Jπ for g.s. band established through J=21/2 based on band structure and independently established Jπ(8-keV level)=3/2+, and intraband M1+E2 110γ and E2 118γ from 118 level.
    138.933157/2+ 302 ps 2  μ=+1.39 5
E(level): 1/2[411] band.
Jπ(level): Definite Jπ for g.s. band established through J=21/2 based on band structure and independently established Jπ(8-keV level)=3/2+, and intraband M1+E2 110γ and E2 118γ from 118 level.
    316.146337/2+ 659.9 ns 23  μ=+0.156 8
E(level): 7/2[404] band.
    332.1169/2+ 18.8 ps 5  μ=1.56 9 (1999Ro03)
E(level): 1/2[411] band.
Jπ(level): Definite Jπ for g.s. band established through J=21/2 based on band structure and independently established Jπ(8-keV level)=3/2+, and intraband M1+E2 110γ and E2 118γ from 118 level.
    341.94(1/2-)   E(level): 1/2[541], α=+1/2 band.
    345.0285/2-   E(level): 1/2[541], α=+1/2 band.
    367.6711/2+ 41.6 ps 21  μ=2.28 14 (1999Ro03)
E(level): 1/2[411] band.
Jπ(level): Definite Jπ for g.s. band established through J=21/2 based on band structure and independently established Jπ(8-keV level)=3/2+, and intraband M1+E2 110γ and E2 118γ from 118 level.
    379.266787/2- 52.2 ns 8  μ=+3.04 14 (1997De02)
E(level): 7/2[523] band.
    430.122(9/2)-   E(level): 1/2[541], α=+1/2 band.
    433.521(9/2)+   E(level): 7/2[404] band.
    472.881289/2- 0.14 ns 7  E(level): 7/2[523] band.
    570.8303/2+ 10 ps 7  E(level): 3/2[411] band + 1/2[411] γ vibration.
    575.38(11/2+)   E(level): 7/2[404] band.
    588.2011/2-   E(level): 7/2[523] band.
    602.82(13/2-)   E(level): 1/2[541], α=+1/2 band.
    633.2925/2+ 0.27 ps E(level): 3/2[411] band + 1/2[411] γ vibration.
    637.0813/2+ 5.4 ps 4  μ=2.37 14 (1999Ro03)
E(level): 1/2[411] band.
Jπ(level): Definite Jπ for g.s. band established through J=21/2 based on band structure and independently established Jπ(8-keV level)=3/2+, and intraband M1+E2 110γ and E2 118γ from 118 level.
    691.2415/2+ 8.1 ps 4  μ=3.2 3 (1999Ro03)
E(level): 1/2[411] band.
Jπ(level): Definite Jπ for g.s. band established through J=21/2 based on band structure and independently established Jπ(8-keV level)=3/2+, and intraband M1+E2 110γ and E2 118γ from 118 level.
    718.786(7/2+)   E(level): 3/2[411] band + 1/2[411] γ vibration.
    725.4413/2-   E(level): 7/2[523] band.
    741.25(13/2+)   E(level): 7/2[404] band.
    781.796(5/2)+   XREF: d(785).
E(level): From 170Er(p,2nγ), (d,3nγ). 5/2[402] band.
    832.42(9/2+)   E(level): 3/2[411] band + 1/2[411] γ vibration.
E(level)Jπ(level)T1/2(level)Comments
    865.9(17/2-)   E(level): 1/2[541], α=+1/2 band.
    878.35(7/2+)   E(level): From 170Er(p,2nγ), (d,3nγ). 5/2[402] band.
    883.7515/2-   E(level): 7/2[523] band.
    929.37(15/2+)   E(level): 7/2[404] band.
    964.0(11/2+)   E(level): 3/2[411] band + 1/2[411] γ vibration.
   1027.8517/2+ 1.91 ps 18  μ=3.1 3 (1999Ro03)
E(level): 1/2[411] band.
Jπ(level): Definite Jπ for g.s. band established through J=21/2 based on band structure and independently established Jπ(8-keV level)=3/2+, and intraband M1+E2 110γ and E2 118γ from 118 level.
   1063.5717/2-   E(level): 7/2[523] band.
   1104.1819/2+ 1.94 ps 21  μ=4.2 8 (1999Ro03)
E(level): 1/2[411] band.
Jπ(level): Definite Jπ for g.s. band established through J=21/2 based on band structure and independently established Jπ(8-keV level)=3/2+, and intraband M1+E2 110γ and E2 118γ from 118 level.
   1140.85(17/2+)   E(level): 7/2[404] band.
   1152(11/2-)   E(level): From 170Er(p,2nγ), (d,3nγ). 9/2[514] band.
   1190+   B(E2)=0.040 9
B(E2)|^ from Coulomb excitation.
E(level): B(E2)|^ from Coulomb excitation.
   1218.1(21/2-)   E(level): 1/2[541], α=+1/2 band.
   1262.4019/2-   E(level): 7/2[523] band.
   1300.8(15/2+)   E(level): 3/2[411] band + 1/2[411] γ vibration.
   1372.1(19/2+)   E(level): 7/2[404] band.
   1482.9421/2-   E(level): 7/2[523] band.
   1497.821/2+ 0.87 ps 9  E(level): 1/2[411] band.
Jπ(level): Definite Jπ for g.s. band established through J=21/2 based on band structure and independently established Jπ(8-keV level)=3/2+, and intraband M1+E2 110γ and E2 118γ from 118 level.
   1510.6(1/2,3/2)+   B(M1,E1)|^(W.u.)=0.078 18.
E(level): B(M1,E1)|^(W.u.)=0.078 18. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   1527.5(1/2,3/2)+   B(M1,E1)|^(W.u.)=0.050 17.
E(level): B(M1,E1)|^(W.u.)=0.050 17. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   1598.4(23/2+)   E(level): From 170Er(p,2nγ), (d,3nγ). 1/2[411] band.
   1625.3(21/2+)   E(level): 7/2[404] band.
   1658.1(25/2-)   E(level): 1/2[541], α=+1/2 band.
   1716.923/2-   E(level): 7/2[523] band.
   1864.6(1/2,3/2)+   B(M1,E1)|^(W.u.)=0.19 3.
E(level): B(M1,E1)|^(W.u.)=0.19 3. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   1910.5(1/2,3/2)+   B(M1,E1)|^(W.u.)=0.61 4.
E(level): B(M1,E1)|^(W.u.)=0.61 4. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
E(level)Jπ(level)T1/2(level)Comments
   1922.3(1/2,3/2)+   B(M1,E1)|^(W.u.)=0.037 11.
E(level): B(M1,E1)|^(W.u.)=0.037 11. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   1963.7(1/2,3/2)   B(M1,E1)|^(W.u.)=0.019 6.
E(level): B(M1,E1)|^(W.u.)=0.019 6. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   1978.4(1/2,3/2)   B(M1,E1)|^(W.u.)=0.020 6.
E(level): B(M1,E1)|^(W.u.)=0.020 6. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   1991.7(1/2,3/2)+   B(M1,E1)|^(W.u.)=0.061 13.
E(level): B(M1,E1)|^(W.u.)=0.061 13. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   2075.5(1/2,3/2)+   B(M1,E1)|^(W.u.)=0.039 17.
E(level): B(M1,E1)|^(W.u.)=0.039 17. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   2168.7(1/2,3/2)+   B(M1,E1)|^(W.u.)=0.035 11.
E(level): B(M1,E1)|^(W.u.)=0.035 11. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   2190.6(1/2,3/2)   B(M1,E1)|^(W.u.)=0.022 4.
E(level): B(M1,E1)|^(W.u.)=0.022 4. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   2215.3(1/2,3/2)   B(M1,E1)|^(W.u.)=0.018 12.
E(level): B(M1,E1)|^(W.u.)=0.018 12. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   2236.1(1/2,3/2)+   B(M1,E1)|^(W.u.)=0.050 6.
E(level): B(M1,E1)|^(W.u.)=0.050 6. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   2262.5(1/2,3/2)+   B(M1,E1)|^(W.u.)=0.043 11.
E(level): B(M1,E1)|^(W.u.)=0.043 11. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   2293.8(1/2,3/2)   B(M1,E1)|^(W.u.)=0.018 4.
E(level): B(M1,E1)|^(W.u.)=0.018 4. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   2306.3(1/2,3/2)   B(M1,E1)|^(W.u.)=0.013 4.
E(level): B(M1,E1)|^(W.u.)=0.013 4. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   2312.2(1/2,3/2)+   B(M1,E1)|^(W.u.)=0.032 9.
E(level): B(M1,E1)|^(W.u.)=0.032 9. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   2386.6(1/2,3/2)   B(M1,E1)|^(W.u.)=0.020 8.
E(level): B(M1,E1)|^(W.u.)=0.020 8. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   2455.8(1/2,3/2)   B(M1,E1)|^(W.u.)=0.022 7.
E(level): B(M1,E1)|^(W.u.)=0.022 7. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   2466.0(1/2,3/2)   B(M1,E1)|^(W.u.)=0.010 3.
E(level): B(M1,E1)|^(W.u.)=0.010 3. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   2492.0(1/2,3/2)+   B(M1,E1)|^(W.u.)=0.051 5.
E(level): B(M1,E1)|^(W.u.)=0.051 5. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   2553.4(1/2,3/2)   B(M1,E1)|^(W.u.)=0.025 8.
E(level): B(M1,E1)|^(W.u.)=0.025 8. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   2571.4(1/2,3/2)   B(M1,E1)|^(W.u.)=0.010 3.
E(level): B(M1,E1)|^(W.u.)=0.010 3. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   2598.6(1/2,3/2)+   B(M1,E1)|^(W.u.)=0.035 10.
E(level): B(M1,E1)|^(W.u.)=0.035 10. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   2602.8(1/2,3/2)   B(M1,E1)|^(W.u.)=0.017 3.
E(level): B(M1,E1)|^(W.u.)=0.017 3. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   2687.0(1/2,3/2)   B(M1,E1)|^(W.u.)=0.011 3.
E(level): B(M1,E1)|^(W.u.)=0.011 3. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   2749.4(1/2,3/2)+   B(M1,E1)|^(W.u.)=0.031 7.
E(level): B(M1,E1)|^(W.u.)=0.031 7. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   2756.4(1/2,3/2)   B(M1,E1)|^(W.u.)=0.017 3.
E(level): B(M1,E1)|^(W.u.)=0.017 3. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   2769.1(1/2,3/2)+   B(M1,E1)|^(W.u.)=0.043 6.
E(level): B(M1,E1)|^(W.u.)=0.043 6. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
E(level)Jπ(level)T1/2(level)Comments
   2786.5(1/2,3/2)   B(M1,E1)|^(W.u.)=0.021 4.
E(level): B(M1,E1)|^(W.u.)=0.021 4. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   2814.2(1/2,3/2)   B(M1,E1)|^(W.u.)=0.032 21.
E(level): B(M1,E1)|^(W.u.)=0.032 21. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   2818.6(1/2,3/2)   B(M1,E1)|^(W.u.)=0.015 6.
E(level): B(M1,E1)|^(W.u.)=0.015 6. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   2843.1(1/2,3/2)   B(M1,E1)|^(W.u.)=0.011 3.
E(level): B(M1,E1)|^(W.u.)=0.011 3. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   2861.1(1/2,3/2)+   B(M1,E1)|^(W.u.)=0.033 12.
E(level): B(M1,E1)|^(W.u.)=0.033 12. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   2943.3(1/2,3/2)+   B(M1,E1)|^(W.u.)=0.043 16.
E(level): B(M1,E1)|^(W.u.)=0.043 16. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   2996.2(1/2,3/2)+   B(M1,E1)|^(W.u.)=0.033 6.
E(level): B(M1,E1)|^(W.u.)=0.033 6. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   3127.6(1/2,3/2)   B(M1,E1)|^(W.u.)=0.020 3.
E(level): B(M1,E1)|^(W.u.)=0.020 3. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   3175.6(1/2,3/2)   B(M1,E1)|^(W.u.)=0.010 3.
E(level): B(M1,E1)|^(W.u.)=0.010 3. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   3185.0(1/2,3/2)   B(M1,E1)|^(W.u.)=0.030 12.
E(level): B(M1,E1)|^(W.u.)=0.030 12. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   3187.5(1/2,3/2)   B(M1,E1)|^(W.u.)=0.009 5.
E(level): B(M1,E1)|^(W.u.)=0.009 5. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   3191.3(1/2,3/2)+   B(M1,E1)|^(W.u.)=0.030 7.
E(level): B(M1,E1)|^(W.u.)=0.030 7. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   3199.7(1/2,3/2)+   B(M1,E1)|^(W.u.)=0.033 9.
E(level): B(M1,E1)|^(W.u.)=0.033 9. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   3204.8(1/2,3/2)+   B(M1,E1)|^(W.u.)=0.046 12.
E(level): B(M1,E1)|^(W.u.)=0.046 12. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   3254.6(1/2,3/2)   B(M1,E1)|^(W.u.)=0.025 7.
E(level): B(M1,E1)|^(W.u.)=0.025 7. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   3274.5(1/2,3/2)+   B(M1,E1)|^(W.u.)=0.029 7.
E(level): B(M1,E1)|^(W.u.)=0.029 7. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   3286.5(1/2,3/2)+   B(M1,E1)|^(W.u.)=0.028 4.
E(level): B(M1,E1)|^(W.u.)=0.028 4. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   3299.6(1/2,3/2)+   B(M1,E1)|^(W.u.)=0.037 15.
E(level): B(M1,E1)|^(W.u.)=0.037 15. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   3308.4(1/2,3/2)   B(M1,E1)|^(W.u.)=0.012 4.
E(level): B(M1,E1)|^(W.u.)=0.012 4. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   3341.2(1/2,3/2)+   B(M1,E1)|^(W.u.)=0.037 9.
E(level): B(M1,E1)|^(W.u.)=0.037 9. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   3376.4(1/2,3/2)+   B(M1,E1)|^(W.u.)=0.030 6.
E(level): B(M1,E1)|^(W.u.)=0.030 6. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   3383.9(1/2,3/2)   B(M1,E1)|^(W.u.)=0.020 3.
E(level): B(M1,E1)|^(W.u.)=0.020 3. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   3419.2(1/2,3/2)   B(M1,E1)|^(W.u.)=0.020 4.
E(level): B(M1,E1)|^(W.u.)=0.020 4. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   3436.3(1/2,3/2)   B(M1,E1)|^(W.u.)=0.027 12.
E(level): B(M1,E1)|^(W.u.)=0.027 12. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   3442.0(1/2,3/2)   B(M1,E1)|^(W.u.)=0.012 7.
E(level): B(M1,E1)|^(W.u.)=0.012 7. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
E(level)Jπ(level)T1/2(level)Comments
   3458.6(1/2,3/2)   B(M1,E1)|^(W.u.)=0.013 7.
E(level): B(M1,E1)|^(W.u.)=0.013 7. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   3475.7(1/2,3/2)+   B(M1,E1)|^(W.u.)=0.055 13.
E(level): B(M1,E1)|^(W.u.)=0.055 13. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   3480.3(1/2,3/2)   B(M1,E1)|^(W.u.)=0.020 3.
E(level): B(M1,E1)|^(W.u.)=0.020 3. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   3497.0(1/2,3/2)   B(M1,E1)|^(W.u.)=0.008 3.
E(level): B(M1,E1)|^(W.u.)=0.008 3. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   3527.0(1/2,3/2)   B(M1,E1)|^(W.u.)=0.017 7.
E(level): B(M1,E1)|^(W.u.)=0.017 7. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   3538.7(1/2,3/2)   B(M1,E1)|^(W.u.)=0.011 3.
E(level): B(M1,E1)|^(W.u.)=0.011 3. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   3541.9(1/2,3/2)+   B(M1,E1)|^(W.u.)=0.026 7.
E(level): B(M1,E1)|^(W.u.)=0.026 7. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   3573.3(1/2,3/2)   B(M1,E1)|^(W.u.)=0.015 9.
E(level): B(M1,E1)|^(W.u.)=0.015 9. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   3613.0(1/2,3/2)   B(M1,E1)|^(W.u.)=0.013 4.
E(level): B(M1,E1)|^(W.u.)=0.013 4. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   3624.8(1/2,3/2)+   B(M1,E1)|^(W.u.)=0.057 9.
E(level): B(M1,E1)|^(W.u.)=0.057 9. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   3724.7(1/2,3/2)+   B(M1,E1)|^(W.u.)=0.034 6.
E(level): B(M1,E1)|^(W.u.)=0.034 6. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   3736.2(1/2,3/2)   B(M1,E1)|^(W.u.)=0.010 4.
E(level): B(M1,E1)|^(W.u.)=0.010 4. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   3741.7(1/2,3/2)   B(M1,E1)|^(W.u.)=0.014 4.
E(level): B(M1,E1)|^(W.u.)=0.014 4. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   3766.3(1/2,3/2)   B(M1,E1)|^(W.u.)=0.012 3.
E(level): B(M1,E1)|^(W.u.)=0.012 3. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   3795.8(1/2,3/2)   B(M1,E1)|^(W.u.)=0.014 11.
E(level): B(M1,E1)|^(W.u.)=0.014 11. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   3806.7(1/2,3/2)   B(M1,E1)|^(W.u.)=0.008 3.
E(level): B(M1,E1)|^(W.u.)=0.008 3. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   3862.5(1/2,3/2)   B(M1,E1)|^(W.u.)=0.012 4.
E(level): B(M1,E1)|^(W.u.)=0.012 4. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   3875.3(1/2,3/2)   B(M1,E1)|^(W.u.)=0.016 4.
E(level): B(M1,E1)|^(W.u.)=0.016 4. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   3916.8(1/2,3/2)   B(M1,E1)|^(W.u.)=0.014 4.
E(level): B(M1,E1)|^(W.u.)=0.014 4. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   3950.2(1/2,3/2)   B(M1,E1)|^(W.u.)=0.015 3.
E(level): B(M1,E1)|^(W.u.)=0.015 3. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   4103.6(1/2,3/2)   B(M1,E1)|^(W.u.)=0.0056 22.
E(level): B(M1,E1)|^(W.u.)=0.0056 22. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   4190.2(1/2,3/2)   B(M1,E1)|^(W.u.)=0.021 13.
E(level): B(M1,E1)|^(W.u.)=0.021 13. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   4279.7(1/2,3/2)   B(M1,E1)|^(W.u.)=0.008 3.
E(level): B(M1,E1)|^(W.u.)=0.008 3. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   4764.5(1/2,3/2)   B(M1,E1)|^(W.u.)=0.006 3.
E(level): B(M1,E1)|^(W.u.)=0.006 3. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   4789.8(1/2,3/2)   B(M1,E1)|^(W.u.)=0.008 4.
E(level): B(M1,E1)|^(W.u.)=0.008 4. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
E(level)Jπ(level)T1/2(level)Comments
   4853.0(1/2,3/2)   B(M1,E1)|^(W.u.)=0.007 4.
E(level): B(M1,E1)|^(W.u.)=0.007 4. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   4865.5(1/2,3/2)   B(M1,E1)|^(W.u.)=0.015 9.
E(level): B(M1,E1)|^(W.u.)=0.015 9. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   4954.0(1/2,3/2)   B(M1,E1)|^(W.u.)=0.023 6.
E(level): B(M1,E1)|^(W.u.)=0.023 6. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   5211.5(1/2,3/2)+   B(M1,E1)|^(W.u.)=0.030 6.
E(level): B(M1,E1)|^(W.u.)=0.030 6. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   5507.1(1/2,3/2)   B(M1,E1)|^(W.u.)=0.023 26.
E(level): B(M1,E1)|^(W.u.)=0.023 26. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   5529.9(1/2,3/2)+   B(M1,E1)|^(W.u.)=0.059 21.
E(level): B(M1,E1)|^(W.u.)=0.059 21. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   5593.3(1/2,3/2)   B(M1,E1)|^(W.u.)=0.05 4.
E(level): B(M1,E1)|^(W.u.)=0.05 4. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
   5598.3(1/2,3/2)   B(M1,E1)|^(W.u.)=0.031 17.
E(level): B(M1,E1)|^(W.u.)=0.031 17. From 169Tm(γ,γ’). From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
Jπ(level): From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.

Back to top

Additional Gamma Comments:

E(level)E(gamma)Comments
      8.41017      8.41017E(γ): from recoil-corrected level-energy difference.
    118.18945    109.77924E(γ): From the evaluation by 2000He14 (with energy scale based on Eγ=411.80205 keV 17 for the "Gold standard " (2+ to g.s. transition in 198Hg)). ΔE quoted here includes the 0.3 ppm uncertainty arising from the energy-wavelength conversion. See 169Yb ε decay (32.018 d) for uncertainties that do not have that systematic uncertainty included.
    118.18940E(γ): From the evaluation by 2000He14 (with energy scale based on Eγ=411.80205 keV 17 for the "Gold standard " (2+ to g.s. transition in 198Hg)). ΔE quoted here includes the 0.3 ppm uncertainty arising from the energy-wavelength conversion. See 169Yb ε decay (32.018 d) for uncertainties that do not have that systematic uncertainty included.
I(γ): from ε decay. However, Iγ=10.21 5 (1999Ro03) in Coulomb excitation is not consistent with this. Other I(118γ)/I(110γ): 11 2 (1967Se09) and 11.0 10 (1977Ta10) in Coulomb excitation; 11 3 in β- decay.
    138.93315    130.52293E(γ): From the evaluation by 2000He14 (with energy scale based on Eγ=411.80205 keV 17 for the "Gold standard " (2+ to g.s. transition in 198Hg)). ΔE quoted here includes the 0.3 ppm uncertainty arising from the energy-wavelength conversion. See 169Yb ε decay (32.018 d) for uncertainties that do not have that systematic uncertainty included.
    316.14633    177.21307E(γ): From the evaluation by 2000He14 (with energy scale based on Eγ=411.80205 keV 17 for the "Gold standard " (2+ to g.s. transition in 198Hg)). ΔE quoted here includes the 0.3 ppm uncertainty arising from the energy-wavelength conversion. See 169Yb ε decay (32.018 d) for uncertainties that do not have that systematic uncertainty included.
    197.95675E(γ): From the evaluation by 2000He14 (with energy scale based on Eγ=411.80205 keV 17 for the "Gold standard " (2+ to g.s. transition in 198Hg)). ΔE quoted here includes the 0.3 ppm uncertainty arising from the energy-wavelength conversion. See 169Yb ε decay (32.018 d) for uncertainties that do not have that systematic uncertainty included.
    307.73586E(γ): From the evaluation by 2000He14 (with energy scale based on Eγ=411.80205 keV 17 for the "Gold standard " (2+ to g.s. transition in 198Hg)). ΔE quoted here includes the 0.3 ppm uncertainty arising from the energy-wavelength conversion. See 169Yb ε decay (32.018 d) for uncertainties that do not have that systematic uncertainty included.
    332.116    193.15I(γ): From Coulomb excitation.
M(γ): From Coulomb excitation.
    213.935I(γ): weighted average of 39 6 in ε decay, 43 9 in (p,2nγ), 45.2 5 (1999Ro03), 49.1 11 (1977Ta10), 56 5 (1967Se09) in Coulomb excitation.
M(γ): from Coulomb excitation.
    341.94    333.53E(γ): From 170Er(p,2nγ), (d,3nγ).
I(γ): From 170Er(p,2nγ), (d,3nγ).
    341.95E(γ): From 170Er(p,2nγ), (d,3nγ).
I(γ): From 170Er(p,2nγ), (d,3nγ).
    367.67    228.71E(γ): From 170Er(p,2nγ), (d,3nγ).
M(γ): from γ(θ) and RUL in Coulomb excitation.. From Coulomb excitation.
    379.26678     63.12044E(γ): From the evaluation by 2000He14 (with energy scale based on Eγ=411.80205 keV 17 for the "Gold standard " (2+ to g.s. transition in 198Hg)). ΔE quoted here includes the 0.3 ppm uncertainty arising from the energy-wavelength conversion. See 169Yb ε decay (32.018 d) for uncertainties that do not have that systematic uncertainty included.
    261.07712E(γ): From the evaluation by 2000He14 (with energy scale based on Eγ=411.80205 keV 17 for the "Gold standard " (2+ to g.s. transition in 198Hg)). ΔE quoted here includes the 0.3 ppm uncertainty arising from the energy-wavelength conversion. See 169Yb ε decay (32.018 d) for uncertainties that do not have that systematic uncertainty included.
    430.122     84.9E(γ): From 170Er(p,2nγ), (d,3nγ).
I(γ): From 170Er(p,2nγ), (d,3nγ).
    291.188E(γ): From 170Er(p,2nγ), (d,3nγ).
I(γ): From 170Er(p,2nγ), (d,3nγ).
    472.88128     93.61447E(γ): From the evaluation by 2000He14 (with energy scale based on Eγ=411.80205 keV 17 for the "Gold standard " (2+ to g.s. transition in 198Hg)). ΔE quoted here includes the 0.3 ppm uncertainty arising from the energy-wavelength conversion. See 169Yb ε decay (32.018 d) for uncertainties that do not have that systematic uncertainty included.
    474.968    466.2E(γ): from (p,2nγ).
    570.830    452.62M(γ): From Coulomb excitation.
    562.410M(γ): From Coulomb excitation.
    570.89M(γ): From Coulomb excitation.
    575.38    141.85E(γ): From 170Er(p,2nγ), (d,3nγ).
I(γ): From 170Er(p,2nγ), (d,3nγ).
    259.23E(γ): From 170Er(p,2nγ), (d,3nγ).
I(γ): From 170Er(p,2nγ), (d,3nγ).
    588.20    115.32E(γ): From 170Er(p,2nγ), (d,3nγ).
I(γ): From 170Er(p,2nγ), (d,3nγ).
M(γ): D+Q from (p,2nγ), Δπ=no from level scheme.
    208.8E(γ): From 170Er(p,2nγ), (d,3nγ).
I(γ): From 170Er(p,2nγ), (d,3nγ).
E(level)E(gamma)Comments
    602.82    172.7E(γ): From 170Er(p,2nγ), (d,3nγ).
I(γ): From 170Er(p,2nγ), (d,3nγ).
    235.1E(γ): From 170Er(p,2nγ), (d,3nγ).
I(γ): From 170Er(p,2nγ), (d,3nγ).
M(γ): d(+Q) from (p,2nγ), Δπ=yes from level scheme.
    637.08    269.4E(γ): From 170Er(p,2nγ), (d,3nγ).
I(γ): weighted average of 99.6 12 (1999Ro03) and 93.7 24 (1977Ta10) in Coulomb excitation. Other Iγ: 101 14 in (p,2nγ); 79 8 (1967Se09) in Coulomb excitation.. From Coulomb excitation.
M(γ): From Coulomb excitation.
    305.2E(γ): From 170Er(p,2nγ), (d,3nγ).
I(γ): From Coulomb excitation.
M(γ): From Coulomb excitation.
    646.758    171.6E(γ): From 170Er(p,2nγ), (d,3nγ).
I(γ): From 170Er(p,2nγ), (d,3nγ).
    216.4E(γ): From 170Er(p,2nγ), (d,3nγ).
I(γ): From 170Er(p,2nγ), (d,3nγ).
    301.6E(γ): From 170Er(p,2nγ), (d,3nγ).
I(γ): From 170Er(p,2nγ), (d,3nγ).
    314.6E(γ): From 170Er(p,2nγ), (d,3nγ).
I(γ): From 170Er(p,2nγ), (d,3nγ).
    528.569I(γ): From 170Er(p,2nγ), (d,3nγ).
    691.24    323.4E(γ): From 170Er(p,2nγ), (d,3nγ).
M(γ): From Coulomb excitation.
    725.44    137.26E(γ): From 170Er(p,2nγ), (d,3nγ).
I(γ): From 170Er(p,2nγ), (d,3nγ).
M(γ): D+Q from (p,2nγ), Δπ=no from level scheme.
    252.5E(γ): From 170Er(p,2nγ), (d,3nγ).
I(γ): From 170Er(p,2nγ), (d,3nγ).
    741.25    165.8E(γ): From 170Er(p,2nγ), (d,3nγ).
I(γ): From 170Er(p,2nγ), (d,3nγ).
    307.74E(γ): for multiplet in (p,2nγ).. From 170Er(p,2nγ), (d,3nγ).
I(γ): From 170Er(p,2nγ), (d,3nγ).
    781.796    210.94E(γ): Multiply placed. From 170Er(p,2nγ), (d,3nγ).
I(γ): From 170Er(p,2nγ), (d,3nγ).
    865.9    175.0E(γ): From 170Er(p,2nγ), (d,3nγ).
I(γ): From 170Er(p,2nγ), (d,3nγ).
    262.7E(γ): From 170Er(p,2nγ), (d,3nγ).
I(γ): From 170Er(p,2nγ), (d,3nγ).
    883.75    158.3E(γ): From 170Er(p,2nγ), (d,3nγ).
I(γ): From 170Er(p,2nγ), (d,3nγ).
M(γ): d(+Q) from (p,2nγ), Δπ=no from level scheme.
    295.4E(γ): From 170Er(p,2nγ), (d,3nγ).
I(γ): From 170Er(p,2nγ), (d,3nγ).
    884.62    281.7E(γ): From 170Er(p,2nγ), (d,3nγ).
I(γ): From 170Er(p,2nγ), (d,3nγ).
    454.5E(γ): Multiply placed. From 170Er(p,2nγ), (d,3nγ).
I(γ): From 170Er(p,2nγ), (d,3nγ).
    552.0E(γ): Multiply placed. From 170Er(p,2nγ), (d,3nγ).
I(γ): From 170Er(p,2nγ), (d,3nγ).
    900    900E(γ): From Coulomb excitation.
    929.37    188.7E(γ): From 170Er(p,2nγ), (d,3nγ).
I(γ): From 170Er(p,2nγ), (d,3nγ).
    353.9E(γ): From 170Er(p,2nγ), (d,3nγ).
I(γ): From 170Er(p,2nγ), (d,3nγ).
E(level)E(gamma)Comments
    964.0    595.9E(γ): From 170Er(p,2nγ), (d,3nγ).
I(γ): From 170Er(p,2nγ), (d,3nγ).
    632.3E(γ): From 170Er(p,2nγ), (d,3nγ).
I(γ): From 170Er(p,2nγ), (d,3nγ).
   1027.85    336.60E(γ): From 170Er(p,2nγ), (d,3nγ).
I(γ): from 1999Ro03 in Coulomb excitation. Other Iγ: 52 5 (1977Ta10) in Coulomb excitation; 336 in (p,2nγ); 114 (1974Ba66) in (d,3nγ).. From Coulomb excitation.
M(γ): From Coulomb excitation.
    391.0E(γ): From 170Er(p,2nγ), (d,3nγ).
I(γ): From Coulomb excitation.
M(γ): From Coulomb excitation.
   1039.95    565.2E(γ): From 170Er(p,2nγ), (d,3nγ).
I(γ): From 170Er(p,2nγ), (d,3nγ).
    694.7E(γ): From 170Er(p,2nγ), (d,3nγ).
I(γ): From 170Er(p,2nγ), (d,3nγ).
   1058.54    716.6E(γ): From 170Er(p,2nγ), (d,3nγ).
   1063.57    179.6E(γ): From 170Er(p,2nγ), (d,3nγ).
I(γ): From 170Er(p,2nγ), (d,3nγ).
    338.3E(γ): From 170Er(p,2nγ), (d,3nγ).
I(γ): From 170Er(p,2nγ), (d,3nγ).
   1104.18    413.0E(γ): From 170Er(p,2nγ), (d,3nγ).
M(γ): From Coulomb excitation.
   1112.6    682.5E(γ): Multiply placed. From 170Er(p,2nγ), (d,3nγ).
   1135.93    790.9E(γ): From 170Er(p,2nγ), (d,3nγ).
   1140.85    210.94E(γ): Multiply placed. From 170Er(p,2nγ), (d,3nγ).
I(γ): From 170Er(p,2nγ), (d,3nγ).
    399.6E(γ): From 170Er(p,2nγ), (d,3nγ).
I(γ): From 170Er(p,2nγ), (d,3nγ).
   1188.7    552.0E(γ): Multiply placed. From 170Er(p,2nγ), (d,3nγ).
I(γ): From 170Er(p,2nγ), (d,3nγ).
    585.9E(γ): From 170Er(p,2nγ), (d,3nγ).
I(γ): From 170Er(p,2nγ), (d,3nγ).
   1190   1190E(γ): From Coulomb excitation.
   1218.1    352.2E(γ): From 170Er(p,2nγ), (d,3nγ).
   1223.04    877.9E(γ): From 170Er(p,2nγ), (d,3nγ).
I(γ): From 170Er(p,2nγ), (d,3nγ).
    881.2E(γ): From 170Er(p,2nγ), (d,3nγ).
I(γ): From 170Er(p,2nγ), (d,3nγ).
   1262.40    198.3E(γ): From 170Er(p,2nγ), (d,3nγ).
I(γ): From 170Er(p,2nγ), (d,3nγ).
    378.7E(γ): From 170Er(p,2nγ), (d,3nγ).
I(γ): From 170Er(p,2nγ), (d,3nγ).
   1300.8    609.6E(γ): From 170Er(p,2nγ), (d,3nγ).
   1372.1    442.7E(γ): From 170Er(p,2nγ), (d,3nγ).
   1482.94    220.5E(γ): From 170Er(p,2nγ), (d,3nγ).
I(γ): From 170Er(p,2nγ), (d,3nγ).
    419.4E(γ): From 170Er(p,2nγ), (d,3nγ).
I(γ): From 170Er(p,2nγ), (d,3nγ).
E(level)E(gamma)Comments
   1497.8    394.0E(γ): From 170Er(p,2nγ), (d,3nγ).
I(γ): weighted average of 29 15 from Coulomb excitation and 50 26 from (p,2nγ).. From 170Er(p,2nγ), (d,3nγ).
    469.6E(γ): From 170Er(p,2nγ), (d,3nγ).
I(γ): From 170Er(p,2nγ), (d,3nγ).
M(γ): From Coulomb excitation.
   1510.6   1510.6E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   1527.5   1527.5E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   1548.4    682.5E(γ): Multiply placed. From 170Er(p,2nγ), (d,3nγ).
   1598.4    494.2E(γ): Multiply placed. From 170Er(p,2nγ), (d,3nγ).
   1625.3    484.4E(γ): From 170Er(p,2nγ), (d,3nγ).
   1658.1    440.0E(γ): From 170Er(p,2nγ), (d,3nγ).
   1716.9    233E(γ): From 170Er(p,2nγ), (d,3nγ).
    454.5E(γ): Multiply placed. From 170Er(p,2nγ), (d,3nγ).
   1864.6   1856.2E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   1864.6E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   1910.5   1792.3E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   1902.1E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   1910.5E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   1922.3   1804.1E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   1922.3E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   1963.7   1963.7E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   1978.4   1978.4E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   1991.7   1983.3E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   1991.7E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   2075.5   2067.1E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   2075.5E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   2168.7   2160.3E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   2168.7E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
E(level)E(gamma)Comments
   2190.6   2190.6E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   2215.3   2215.3E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   2236.1   2117.9E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   2236.1E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   2262.5   2144.3E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   2262.5E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   2293.8   2293.8E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   2306.3   2306.3E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   2312.2   2194.0E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   2312.2E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   2386.6   2386.6E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   2455.8   2447.4E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   2455.8E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   2466.0   2466.0E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   2492.0   2373.8E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   2492.0E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   2553.4   2435.2E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   2553.4E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   2571.4   2571.4E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   2598.6   2598.6E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   2602.8   2602.8E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   2687.0   2687.0E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   2749.4   2741.0E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   2749.4E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   2756.4   2756.4E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
E(level)E(gamma)Comments
   2769.1   2760.7E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   2769.1E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   2786.5   2786.5E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   2814.2   2805.8E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   2814.2E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   2818.6   2818.6E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   2843.1   2843.1E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   2861.1   2861.1E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   2943.3   2825.1E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   2934.9E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   2943.3E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   2996.2   2878.0E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   2996.2E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   3127.6   3127.6E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   3175.6   3175.6E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   3185.0   3185.0E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   3187.5   3187.5E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   3191.3   3182.9E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   3191.3E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   3199.7   3199.7E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   3204.8   3086.6E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   3204.8E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   3254.6   3246.2E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   3254.6E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   3274.5   3274.5E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
E(level)E(gamma)Comments
   3286.5   3286.5E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   3299.6   3291.2E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   3299.6E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   3308.4   3308.4E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   3341.2   3332.8E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   3341.2E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   3376.4   3376.4E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   3383.9   3383.9E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   3419.2   3419.2E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   3436.3   3318.1E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   3436.3E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   3442.0   3442.0E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   3458.6   3458.6E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   3475.7   3467.3E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   3475.7E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   3480.3   3480.3E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   3497.0   3497.0E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   3527.0   3518.6E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   3527.0E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   3538.7   3538.7E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   3541.9   3423.7E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   3541.9E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   3573.3   3573.3E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   3613.0   3613.0E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   3624.8   3506.6E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   3616.4E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   3624.8E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
E(level)E(gamma)Comments
   3724.7   3606.5E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   3724.7E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   3736.2   3736.2E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   3741.7   3741.7E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   3766.3   3766.3E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   3795.8   3787.3E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   3795.7E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   3806.7   3806.7E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   3862.5   3862.5E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   3875.3   3875.3E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   3916.8   3916.8E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   3950.2   3950.2E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   4103.6   4103.5E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   4190.2   4181.7E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   4190.1E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   4279.7   4279.6E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   4764.5   4764.4E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   4789.8   4789.7E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   4853.0   4852.9E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   4865.5   4857.0E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   4865.4E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   4954.0   4953.9E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   5211.5   5211.4E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   5507.1   5507E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   5529.9   5529.8E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
E(level)E(gamma)Comments
   5593.3   5584.8E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   5593.2E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).
   5598.3   5598.2E(γ): From 169Tm(γ,γ’).. From 169Tm(γ,γ’). d excitation from 1/2+ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
I(γ): From 169Tm(γ,γ’).

Back to top