ADOPTED LEVELS, GAMMAS for 146Tb

Authors: Yu. Khazov, A. Rodionov and G. Shulyak |  Citation: Nucl. Data Sheets 136, 163 (2016) |  Cutoff date: 14-Jul-2016 

 Full ENSDF file | Adopted Levels (PDF version) 


Q(β-)=-5210 keV 50S(n)= 9.53×103 keV 11S(p)= 2130 keV 50Q(α)= 1130 keV 50
Reference: 2012WA38

References:
  A  146Dy ε decay  B  146Tb IT decay
  C  115In(34S,3nγ)  D  118Sn(32S,p3nγ)
  E  144Sm(6Li,4nγ) 

General Comments:

Produced and identified: 1973NeZU, 1974Ne01. 141Pr target, irradiated by 118 MeV 12C beam.

146Tb level scheme was built on the basis of γγ(DCO), γ(X-ray), γγ(θ)(lin pol) coin, ce measurements. The level scheme consists of two unconnected parts: obtained from 146Dy ε decay, and from reaction study data. The latter includes two isomers: Jπ=5-, T1/2=24.1 s and Jπ=10+, T1/2=1.18 ms; placements of these states are not known exactly. There are supposed as 150 keV 100 and 930 keV 110 correspondingly higher g.s., 1+; (2012Au07; systematics).

In framework of shell model, nuclide 146Tb has one proton-particle and one neutron-hole with respect to doubly closed 146Gd. The ground state has πd-15/2νd-13/2 structure. The higher lying states should arise from coupling of the odd neutrons in s1/2, d3/2 or h11/2 and odd protons in the same orbitals, as well as in d5/2. Intense β+ feedings of the states between 1.7 and 2.2 MeV were observed, these states were populated through (πh211/2)0+|)(πh11/2νh9/2)1+ transitions.

In the second part of the scheme, the states higher than the isomer J=5- have two quasi-particles configuration, their mixture or many-quasi-particle excitations, also coupling to the excitations of 146Gd (detailed probable shell-model configurations for large number of levels are given in the table II of 2004Kr14). Three γ ray cascades were observed at 5-8 MeV, one of them was interpreted as ΔJ=1 magnetic transition sequence.

Levels: Detailed shell-model configurations for many levels are given in table II of 2004Kr14










E(level)
(keV)		XREFJπ(level) T1/2(level)E(γ)
(keV)		I(γ)M(γ)Final Levels
        0.0A     1+ 8 s 4 
% ε = 100
     
      241.09 10 A     1+      241.1 2 
   100
M1
        0.0
1+
      280.19 12 A     1+      280.2 2 
   100
M1
        0.0
1+
      338.15 13 A     1+      338.1 2 
   100
E2
        0.0
1+
      354.85 11 A     1+       74.7 2 
   113.7 2 
   354.9 2 
     5.9 7 
    ≈9
   100 4 
M1

M1
      280.19
      241.09
        0.0
1+
1+
1+
      384.65 12 A     1+      143.5 2 
   384.6 2 
    ≈3
   100 3 

M1
      241.09
        0.0
1+
1+
      397.99 23 A     (1+)      117.8 2 
   100

      280.19
1+
      565.91 13 A     (1+)      285.7 2 
   324.8 2 
   565.9 3 
   ≈14
   ≈51
  ≈100



      280.19
      241.09
        0.0
1+
1+
1+
      574.95 24 A     (1+)      236.8 2 
   100

      338.15
1+
      618.4 3 A     (1+)      618.4 3 
   100

        0.0
1+
      653.15 18 A     (0,1)+      268.4 2 
   100
M1
      384.65
1+
      660.31 13 A     1+      305.5 2 
   322.1 2 
   419.3 2 
   660.3 3 
   ≈29
   100 13 
   ≈65
   ≈76

M1


      354.85
      338.15
      241.09
        0.0
1+
1+
1+
1+
      664.83 23 A     (1+)      664.9 3 
   100

        0.0
1+
      682.14 17 A     (1+)      441.1 2 
   682.1 3 
   ≈81
  ≈100


      241.09
        0.0
1+
1+
      920.0 3 A     (1+)      920.0 3 
   100

        0.0
1+
     1162.3 4 A     (1+)      882.1 3 
   100

      280.19
1+
     1696.1 3 A     (1+)     1696.1 3 
   100

        0.0
1+
     1726.96 14 A     1+     1062.2 3 
  1066.8 3 
  1073.4 3 
  1161.2 3 
  1342.3 3 
  1372.2 3 
  1388.8 3 
  1446.7 3 
   ≈44
   ≈98
   ≈35
  ≈100
   ≈65
   ≈35
   ≈60
   ≈77








      664.83
      660.31
      653.15
      565.91
      384.65
      354.85
      338.15
      280.19
(1+)
1+
(0,1)+
(1+)
1+
1+
1+
1+
E(level)
(keV)		XREFJπ(level) T1/2(level)E(γ)
(keV)		I(γ)M(γ)Final Levels
     1737.40 15 A     1+     1084.4 3 
  1171.2 3 
  1352.8 3 
  1399.3 3 
  1496.3 3 
  1737.4 3 
   ≈20
   ≈15
   ≈78
   ≈22
   ≈20
  ≈100






      653.15
      565.91
      384.65
      338.15
      241.09
        0.0
(0,1)+
(1+)
1+
1+
1+
1+
     1923.8 3 A         1923.8 3 
   100

        0.0
1+
     2082.01 15 A     1+     1727.1 3 
  1743.8 3 
  1801.8 3 
  1841.0 3 
  2082.0 3 
   ≈12
   ≈24
  ≈100
   ≈24
   ≈45





      354.85
      338.15
      280.19
      241.09
        0.0
1+
1+
1+
1+
1+
     2156.80 14 A     1+     1474.7 3 
  1772.1 3 
  1801.8 3 
  1876.7 3 
  1915.7 3 
  2156.8 3 
   ≈13
   ≈12
    ≈8
   ≈18
   ≈21
  ≈100






      682.14
      384.65
      354.85
      280.19
      241.09
        0.0
(1+)
1+
1+
1+
1+
1+
        0.0+X B DE 5- 24.1 s 5 
% ε = 100
     
       18.73+X 13  B DE 6-       18.7 5 S
 

        0.0+X
5-
      156.70+X 10  B DE 6-      138.0 1 
   156.7 1 
    30 16 
   100 16 
M1
M1
       18.73+X
        0.0+X
6-
5-
      361.87+X 13  B DE 7-      205.2 1 
   343.1 1 
     8.4 10 
   100 4 
M1
M1+E2
      156.70+X
       18.73+X
6-
6-
      779.57+X 16  BCDE 10+ 1.20 ms 3 
% IT = 100
   417.7 1 
   100
E3
      361.87+X
7-
      804.57+X 24     E 8+      442.7 2 
   100
E1
      361.87+X
7-
     1370.17+X 18   CDE 11+      590.60 6 
   100
M1
      779.57+X
10+
     2147.40+X 18   CDE 11-      777.23 2 
   100
E1
     1370.17+X
11+
E(level)
(keV)		XREFJπ(level) T1/2(level)E(γ)
(keV)		I(γ)M(γ)Final Levels
     2170.64+X 18   CDE (11-)      800.47 3 
   100
E1
     1370.17+X
11+
     2188.31+X 18   CDE 12-       40.90 12 
   818.13 3 
     7.0 7 
   100 2 

E1
     2147.40+X
     1370.17+X
11-
11+
     2224.22+X 18   CD  (12+)       53.6 1 
    76.7 1 
   854.05 1 
    50 30 
   100 30 
    80 30 



     2170.64+X
     2147.40+X
     1370.17+X
(11-)
11-
11+
     2577.84+X 18   CDE 13-      389.53 3 
   100
M1
     2188.31+X
12-
     2760.31+X 23   C        572.00 15 
   100

     2188.31+X
12-
     2920.96+X 22   CD  (13+)      696.5 2 
   100

     2224.22+X
(12+)
     3085.18+X 18   CDE (13-)      896.87 3 
   100
(M1)
     2188.31+X
12-
     3149.64+X 21   CDE (13)-      571.8 1 
   100
(M1)
     2577.84+X
13-
     3264.44+X 18   CD  (14+)      343.35 15 
  1040.25 5 
    52 8 
   100 11 
M1
E2
     2920.96+X
     2224.22+X
(13+)
(12+)
     3284.34+X 19   CDE 14-      199.17 12 
   706.43 9 
     7.7 9 
   100 11 
D
M1
     3085.18+X
     2577.84+X
(13-)
13-
     3368.02+X 19   CDE 15-       83.67 3 
   100
M1
     3284.34+X
14-
     3461.7+X 5 ?    E (14)-      177.6 2 ?
 
M1
     3284.34+X
14-
     3487.86+X 19   CDE 16-      119.83 3 
   100
M1
     3368.02+X
15-
     3580.06+X 23   CD  (15+)      315.8 2 
   100
M1
     3264.44+X
(14+)
     3584.79+X 20   CDE 17-       96.93 3 
   100
M1
     3487.86+X
16-
     3691.73+X 20   CDE      203.80 6 
   323.77 9 
   100 14 
    80 9 


     3487.86+X
     3368.02+X
16-
15-
     3905.13+X 21   CD  15-      640.75 15 
   100
E1
     3264.44+X
(14+)
     3945.72+X 22   CD  (16+)      365.7 1 
   100
(M1+E2)
     3580.06+X
(15+)
     4115.10+X 21   CDE 18-      530.17 10 
   100
M1
     3584.79+X
17-
     4140.67+X 20   CDE 17-      652.80 6 
   100
M1
     3487.86+X
16-
     4217.50+X 20   CDE 17-      271.9 2 
   312.4 1 
   525.67 9 
   729.69 9 
    ≤8
    23 3 
    31 3 
   100 3 

E2

M1
     3945.72+X
     3905.13+X
     3691.73+X
     3487.86+X
(16+)
15-

16-
E(level)
(keV)		XREFJπ(level) T1/2(level)E(γ)
(keV)		I(γ)M(γ)Final Levels
     4464.75+X 21   CD  18+      247.3 1 
   100
E1
     4217.50+X
17-
     4506.33+X 22   CD  (17-)      560.65 15 
   100
E1
     3945.72+X
(16+)
     4579.91+X 21   CDE 19-      464.73 9 
   100
M1
     4115.10+X
18-
     4690.43+X 20   CDE 18+      549.75 9 
  1105.70 6 
    67 13 
   100 13 
E1
D
     4140.67+X
     3584.79+X
17-
17-
     4775.98+X 22   CD  (18-)      269.65 5 
   558.4 2 
   100 10 
    94 10 


     4506.33+X
     4217.50+X
(17-)
17-
     4867.31+X 23   CD  19+      177.0 2 
   100
M1
     4690.43+X
18+
     5075.15+X 21   CDE 19+      384.77 7 
   960.00 12 
   100 14 
    45 5 
D
E1
     4690.43+X
     4115.10+X
18+
18-
     5134.33+X 22   CD  19-      358.35 5 
   669.5 1 
   916.6 2 
   100 12 
    47 7 
    83 10 
M1


     4775.98+X
     4464.75+X
     4217.50+X
(18-)
18+
17-
     5277.56+X 23   CD  19     1162.45 15 
  1692.75 15 
    43 4 
   100 11 
D
Q
     4115.10+X
     3584.79+X
18-
17-
     5364.98+X 21   CD  20+      289.85 5 
   785.05 5 
   100 10 
    52 6 
M1

     5075.15+X
     4579.91+X
19+
19-
     5491.87+X 24   CD  20      214.3 1 
  1377.0 5 
   100 11 
    29 7 
D

     5277.56+X
     4115.10+X
19
18-
     5543.11+X 22   CD  20+      408.75 5 
  1078.5 1 
    68 7 
   100 11 
E1
E2
     5134.33+X
     4464.75+X
19-
18+
     5580.69+X 22   CD  20-      713.4 1 
  1000.7 1 
   100 10 
   ≤30
E1

     4867.31+X
     4579.91+X
19+
19-
     5741.5+X 3   C        666.40 15 
   100
D
     5075.15+X
19+
     5809.1+X 3   C       2229.00 15 
   100

     3580.06+X
(15+)
     5814.35+X 23   CD  21+      233.65 5 
   449.45 15 
    96 11 
   100 12 
D
M1
     5580.69+X
     5364.98+X
20-
20+
     5853.7+X 3   C       1273.80 15 
   100

     4579.91+X
19-
     5945.82+X 25   C   21      453.95 5 
   100
D
     5491.87+X
20
     6387.8+X 3   C   22+      573.45 14 
   100
M1
     5814.35+X
21+
E(level)
(keV)		XREFJπ(level) T1/2(level)E(γ)
(keV)		I(γ)M(γ)Final Levels
     6439.9+X 3   C       1860.00 15 
   100

     4579.91+X
19-
     6492.67+X 22   C   22+      949.55 3 
   100
E2
     5543.11+X
20+
     6495.6+X 3   C   23(+)      107.8 1 
   100
D
     6387.8+X
22+
     6533.2+X 3   C   22      587.4 1 
   100
D
     5945.82+X
21
     6682.3+X 4   C        149.1 3 
   100

     6533.2+X
22
     6836.0+X 4   C   (24+)      340.40 25 
   100
M1
     6495.6+X
23(+)
     7096.4+X 5   C        414.10 15 
   100

     6682.3+X

     7142.5+X 5   C        306.50 25 
   100

     6836.0+X
(24+)
     7563.42+X 23   C   24+     1070.75 5 
   100
E2
     6492.67+X
22+
     7737.0+X 3   C   (23+)     1244.35 15 
   100
D
     6492.67+X
22+
     8003.5+X 3   C   (24+)      266.50 15 
   100
D
     7737.0+X
(23+)
     8302.5+X 4   C        739.10 25 
   100

     7563.42+X
24+
   8370+X 3   C   (24+)      633.0 25 
   100
M1
     7737.0+X
(23+)
     8388.7+X 4   C   (25+)      385.20 15 
   100
D
     8003.5+X
(24+)
   8875+X 3   C   (26+)      486.0 25 
   870.60 15 ?
   100 25 
    ≤8
M1
E2
     8388.7+X
     8003.5+X
(25+)
(24+)
   9304+X 3   C   (27+)      429.30 15 
   100
M1
   8875+X
(26+)
   9717+X 3   C   (28+)      413.40 15 
   100
M1
   9304+X
(27+)
  10192+X 3   C   (29+)      474.60 15 
   100
M1
   9717+X
(28+)
  10655+X 3   C   (30+)      463.10 15 
   100
M1
  10192+X
(29+)

E(level): From a least-squares fit to Eγ’s; normalized χ2=0.5

Jπ(level): Assigned on the basis of the measured conversion electrons, DCO values, γ(θ), linear polarization in the 115In(34S,3nγ) (in the main) and 118Sn(32S,p3nγ), 144Sm(6Li,4nγ) reactions, except other marked. Possible configurations are from the ε decay and the reaction studies data

E(γ): Unweighted average data from IT decay and reaction except as noted. Evaluators assumed ΔEγ=0.1 keV if Eγ are equal.

I(γ): Calculated from I(γ+ce) in 118Sn(32S,p3nγ) dataset, assuming [E1], [E2] or [M1+E2] multipolarities for the transitions according to the level pattern, except as noted

I(γ): % branching from each level; Iγ from 118In(32S,p3nγ), except as noted.

M(γ): From α(K)exp, γγ(θ)(DCO), γγ(lin pol) data, except as noted.

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Band Transitions:

E(level)
(keV)		Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 1 - Sequence based on J=18+ state.
     4690.43+X 20  18+        
     5075.15+X 21  19+      384.77 7 
   960.00 12 
   100 14 
    45 5 
D
E1
     4690.43+X
     4115.10+X
18+
18-
     5364.98+X 21  20+      289.85 5 
   785.05 5 
   100 10 
    52 6 
M1

     5075.15+X
     4579.91+X
19+
19-
     5814.35+X 23  21+      233.65 5 
   449.45 15 
    96 11 
   100 12 
D
M1
     5580.69+X
     5364.98+X
20-
20+
     6387.8+X 3  22+      573.45 14 
   100
M1
     5814.35+X
21+
     6495.6+X 3  23(+)      107.8 1 
   100
D
     6387.8+X
22+
     6836.0+X 4  (24+)      340.40 25 
   100
M1
     6495.6+X
23(+)
     7142.5+X 5       306.50 25 
   100

     6836.0+X
(24+)
E(level)
(keV)		Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 2 - Sequence based on J=19 state.
     5277.56+X 23  19        
     5491.87+X 24  20      214.3 1 
  1377.0 5 
   100 11 
    29 7 
D

     5277.56+X
     4115.10+X
19
18-
     5945.82+X 25  21      453.95 5 
   100
D
     5491.87+X
20
     6533.2+X 3  22      587.4 1 
   100
D
     5945.82+X
21
     6682.3+X 4       149.1 3 
   100

     6533.2+X
22
     7096.4+X 5       414.10 15 
   100

     6682.3+X

E(level)
(keV)		Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 3 - Sequence based on J=(23+) state.
     7737.0+X 3  (23+)        
     8003.5+X 3  (24+)      266.50 15 
   100
D
     7737.0+X
(23+)
     8388.7+X 4  (25+)      385.20 15 
   100
D
     8003.5+X
(24+)
   8875+X 3  (26+)      486.0 25 
   870.60 15 ?
   100 25 
    ≤8
M1
E2
     8388.7+X
     8003.5+X
(25+)
(24+)
   9304+X 3  (27+)      429.30 15 
   100
M1
   8875+X
(26+)
   9717+X 3  (28+)      413.40 15 
   100
M1
   9304+X
(27+)
  10192+X 3  (29+)      474.60 15 
   100
M1
   9717+X
(28+)
  10655+X 3  (30+)      463.10 15 
   100
M1
  10192+X
(29+)

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Additional Gamma Data:















E(level)
(keV)		Jπ(level)T1/2(level)E(γ)
(keV)		MultipolarityMixing
Ratio		Conversion
Coefficient		Additional Data
      241.09 1+      241.1 2 M1 0.187α=0.187
      280.19 1+      280.2 2 M1 0.1247α=0.1247
      338.15 1+      338.1 2 E2 0.0435α=0.0435
      354.85 1+       74.7 2 M1 5.09α=5.09 9
1+      354.9 2 M1 0.0666α=0.0666
      384.65 1+      384.6 2 M1 0.0540α=0.0540
      653.15 (0,1)+      268.4 2 M1 0.1400α=0.1400
      660.31 1+      322.1 2 M1 0.0860α=0.0860
      156.70+X 6-      138.0 1 M1 0.878α=0.878
6-      156.7 1 M1 0.614α=0.614
      361.87+X 7-      205.2 1 M1 0.291α=0.291
7-      343.1 1 M1+E21.6 60.050α=0.050 7
      779.57+X 10+ 1.20 ms 3 
% IT = 100
   417.7 1 E3 0.0757B(E3)(W.u.)=0.335 6, α=0.0757
      804.57+X 8+      442.7 2 E1 0.00649α=0.00649
     1370.17+X 11+      590.60 6 M1 0.0180α=0.0180
     2147.40+X 11-      777.23 2 E1 0.00194α=0.00194
     2170.64+X (11-)      800.47 3 E1 0.00183α=0.00183
     2188.31+X 12-      818.13 3 E1 1.75×10-3α=1.75×10-3
     2577.84+X 13-      389.53 3 M1 0.0522α=0.0522
     3085.18+X (13-)      896.87 3 (M1) 0.00641α=0.00641
     3149.64+X (13)-      571.8 1 (M1) 0.0195α=0.0195
     3264.44+X (14+)      343.35 15 M1 0.0727α=0.0727
(14+)     1040.25 5 E2 0.00267α=0.00267
     3284.34+X 14-      706.43 9 M1 0.01150α=0.01150
     3368.02+X 15-       83.67 3 M1 3.67α=3.67
E(level)
(keV)		Jπ(level)T1/2(level)E(γ)
(keV)		MultipolarityMixing
Ratio		Conversion
Coefficient		Additional Data
     3461.7+X (14)-      177.6 2 M1 0.433α=0.433
     3487.86+X 16-      119.83 3 M1 1.310α=1.310
     3580.06+X (15+)      315.8 2 M1 0.0907α=0.0907
     3584.79+X 17-       96.93 3 M1 2.40α=2.40
     3905.13+X 15-      640.75 15 E1 0.00287α=0.00287
     3945.72+X (16+)      365.7 1 (M1+E2) 0.048α=0.048 14
     4115.10+X 18-      530.17 10 M1 0.0236α=0.0236
     4140.67+X 17-      652.80 6 M1 0.01400α=0.01400
     4217.50+X 17-      312.4 1 E2 0.0551α=0.0551
17-      729.69 9 M1 0.01062α=0.01062
     4464.75+X 18+      247.3 1 E1 0.0270α=0.0270
     4506.33+X (17-)      560.65 15 E1 0.00382α=0.00382
     4579.91+X 19-      464.73 9 M1 0.0331α=0.0331
     4690.43+X 18+      549.75 9 E1 0.00399α=0.00399
     4867.31+X 19+      177.0 2 M1 0.437α=0.437
     5075.15+X 19+      960.00 12 E1 1.29×10-3α=1.29×10-3
     5134.33+X 19-      358.35 5 M1 0.0649α=0.0649
     5364.98+X 20+      289.85 5 M1 0.1139α=0.1139
     5543.11+X 20+      408.75 5 E1 0.00781α=0.00781
20+     1078.5 1 E2 0.00248α=0.00248
     5580.69+X 20-      713.4 1 E1 0.00230α=0.00230
     5814.35+X 21+      449.45 15 M1 0.0360α=0.0360
     6387.8+X 22+      573.45 14 M1 0.0194α=0.0194
     6492.67+X 22+      949.55 3 E2 0.00323α=0.00323
     6836.0+X (24+)      340.40 25 M1 0.0743α=0.0743
E(level)
(keV)		Jπ(level)T1/2(level)E(γ)
(keV)		MultipolarityMixing
Ratio		Conversion
Coefficient		Additional Data
     7563.42+X 24+     1070.75 5 E2 0.00251α=0.00251
   8370+X (24+)      633.0 25 M1 0.0151α=0.0151 3
   8875+X (26+)      486.0 25 M1 0.0295α=0.0295 6
(26+)      870.60 15 E2 0.00389α=0.00389
   9304+X (27+)      429.30 15 M1 0.0406α=0.0406
   9717+X (28+)      413.40 15 M1 0.0447α=0.0447
  10192+X (29+)      474.60 15 M1 0.0313α=0.0313
  10655+X (30+)      463.10 15 M1 0.0334α=0.0334

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Additional Level Data and Comments:

E(level)Jπ(level)T1/2(level)Comments
        0.01+ 8 s 4 
% ε = 100
configuration=πd-15/2νd-13/2 (1987Zu02).
      156.70+X6-   Jπ(level): From coincide cascade of γ-rays between J=10+ and J=5-: 10+ |) 417.7γ E3 |) 7- |) 205.2γ M1 |) 6- |) 156.7γ M1 |) 5-.
      361.87+X7-   Jπ(level): From coincide cascade of γ-rays between J=10+ and J=5-: 10+ |) 417.7γ E3 |) 7- |) 205.2γ M1 |) 6- |) 156.7γ M1 |) 5-.
      779.57+X10+ 1.20 ms 3 
% IT = 100
E(level): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
      804.57+X8+   E(level): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
     1370.17+X11+   E(level): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
     4690.43+X18+   E(level): Sequence based on J=18+ state.
     5075.15+X19+   E(level): Sequence based on J=18+ state.
     5277.56+X19   E(level): Sequence based on J=19 state.
     5364.98+X20+   E(level): Sequence based on J=18+ state.
     5491.87+X20   E(level): Sequence based on J=19 state.
     5814.35+X21+   E(level): Sequence based on J=18+ state.
     5945.82+X21   E(level): Sequence based on J=19 state.
     6387.8+X22+   E(level): Sequence based on J=18+ state.
     6495.6+X23(+)   E(level): Sequence based on J=18+ state.
     6533.2+X22   E(level): Sequence based on J=19 state.
     6682.3+X   E(level): Sequence based on J=19 state.
     6836.0+X(24+)   E(level): Sequence based on J=18+ state.
     7096.4+X   E(level): Sequence based on J=19 state.
     7142.5+X   E(level): Sequence based on J=18+ state.
     7737.0+X(23+)   E(level): Sequence based on J=(23+) state.
     8003.5+X(24+)   E(level): Sequence based on J=(23+) state.
     8388.7+X(25+)   E(level): Sequence based on J=(23+) state.
   8875+X(26+)   E(level): Sequence based on J=(23+) state.
   9304+X(27+)   E(level): Sequence based on J=(23+) state.
E(level)Jπ(level)T1/2(level)Comments
   9717+X(28+)   E(level): Sequence based on J=(23+) state.
  10192+X(29+)   E(level): Sequence based on J=(23+) state.
  10655+X(30+)   E(level): Sequence based on J=(23+) state.

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Additional Gamma Comments:

E(level)E(gamma)Comments
      280.19      280.2E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
      338.15      338.1E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
      354.85       74.7E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
I(γ): From 146Dy ε decay
      113.7E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
I(γ): From 146Dy ε decay
      354.9E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
I(γ): From 146Dy ε decay
      384.65      143.5E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
I(γ): From 146Dy ε decay
      384.6E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
I(γ): From 146Dy ε decay
      397.99      117.8E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
      565.91      285.7E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
I(γ): From 146Dy ε decay
      324.8E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
I(γ): From 146Dy ε decay
      565.9E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
I(γ): From 146Dy ε decay
      574.95      236.8E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
      618.4      618.4E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
      653.15      268.4E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
      660.31      305.5E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
I(γ): From 146Dy ε decay
      322.1E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
I(γ): From 146Dy ε decay
      419.3E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
I(γ): From 146Dy ε decay
      660.3E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
I(γ): From 146Dy ε decay
      664.83      664.9E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
      682.14      441.1E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
I(γ): From 146Dy ε decay
      682.1E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
I(γ): From 146Dy ε decay
      920.0      920.0E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
     1162.3      882.1E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
     1696.1     1696.1E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
     1726.96     1062.2E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
I(γ): From 146Dy ε decay
     1066.8E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
I(γ): From 146Dy ε decay
     1073.4E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
I(γ): From 146Dy ε decay
     1161.2E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
I(γ): From 146Dy ε decay
     1342.3E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
I(γ): From 146Dy ε decay
     1372.2E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
I(γ): From 146Dy ε decay
     1388.8E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
I(γ): From 146Dy ε decay
     1446.7E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
I(γ): From 146Dy ε decay
E(level)E(gamma)Comments
     1737.40     1084.4E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
I(γ): From 146Dy ε decay
     1171.2E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
I(γ): From 146Dy ε decay
     1352.8E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
I(γ): From 146Dy ε decay
     1399.3E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
I(γ): From 146Dy ε decay
     1496.3E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
I(γ): From 146Dy ε decay
     1737.4E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
I(γ): From 146Dy ε decay
     1923.8     1923.8E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
     2082.01     1727.1E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
I(γ): From 146Dy ε decay
     1743.8E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
I(γ): From 146Dy ε decay
     1801.8E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
I(γ): From 146Dy ε decay
     1841.0E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
I(γ): From 146Dy ε decay
     2082.0E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
I(γ): From 146Dy ε decay
     2156.80     1474.7E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
I(γ): From 146Dy ε decay
     1772.1E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
I(γ): From 146Dy ε decay
     1801.8E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
I(γ): From 146Dy ε decay
     1876.7E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
I(γ): From 146Dy ε decay
     1915.7E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
I(γ): From 146Dy ε decay
     2156.8E(γ): From 146Dy ε decay. States of probably two quasi-particle multiplet of configuration=πh11/2νh-111/2.
I(γ): From 146Dy ε decay
      156.70+X      138.0I(γ): From 146Tb IT decay
      156.7I(γ): From 146Tb IT decay
      361.87+X      205.2I(γ): From 146Tb IT decay
      343.1I(γ): From 146Tb IT decay
      804.57+X      442.7E(γ): From 144Sm(6Li,4nγ), ΔE assumed by the evaluators
     2760.31+X      572.00E(γ): From 115In(34S,3nγ), ΔE assumed by the evaluators
     3461.7+X      177.6E(γ): From 144Sm(6Li,4nγ), ΔE assumed by the evaluators
E(level)E(gamma)Comments
     3945.72+X      365.7M(γ): ΔJ=1
     4217.50+X      271.9E(γ): From 118Sn(32S,p3nγ), ΔE assumed by the evaluators
     5741.5+X      666.40E(γ): From 115In(34S,3nγ), ΔE assumed by the evaluators
     5809.1+X     2229.00E(γ): From 115In(34S,3nγ), ΔE assumed by the evaluators
     5853.7+X     1273.80E(γ): From 115In(34S,3nγ), ΔE assumed by the evaluators
     6439.9+X     1860.00E(γ): From 115In(34S,3nγ), ΔE assumed by the evaluators
     6836.0+X      340.40E(γ): From 115In(34S,3nγ), ΔE assumed by the evaluators
     7096.4+X      414.10E(γ): From 115In(34S,3nγ), ΔE assumed by the evaluators
     7142.5+X      306.50E(γ): From 115In(34S,3nγ), ΔE assumed by the evaluators
     8003.5+X      266.50E(γ): 266.5γ and 385.2γ (from 8388.8+x keV level) are in cascade in 2004Kr14 and in 2004Xi01, but in the second paper 385.2γ is placed below.. From 115In(34S,3nγ), ΔE assumed by the evaluators
     8302.5+X      739.10E(γ): From 115In(34S,3nγ), ΔE assumed by the evaluators
   8370+X      633.0E(γ): From 115In(34S,3nγ), ΔE assumed by the evaluators
     8388.7+X      385.20E(γ): From 115In(34S,3nγ), ΔE assumed by the evaluators
   8875+X      870.60E(γ): From 115In(34S,3nγ), ΔE assumed by the evaluators
   9304+X      429.30E(γ): From 115In(34S,3nγ), ΔE assumed by the evaluators
   9717+X      413.40E(γ): From 115In(34S,3nγ), ΔE assumed by the evaluators
  10192+X      474.60E(γ): From 115In(34S,3nγ), ΔE assumed by the evaluators
  10655+X      463.10E(γ): From 115In(34S,3nγ), ΔE assumed by the evaluators

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