ADOPTED LEVELS, GAMMAS for 135Ce

Authors: Balraj Singh, Alexander A. Rodionov and Yuri L. Khazov |  Citation: Nucl. Data Sheets 109, 517 (2008) |  Cutoff date: 22-Jan-2008 

 Full ENSDF file | Adopted Levels (PDF version) 


Q(β-)=-3680 keV 16S(n)= 7855 keV 23S(p)= 6687 keV 23Q(α)= -357 keV 11
Reference: 2012WA38

References:
  A  135Ce IT decay (20 S)  B  135Pr ε decay (24 M)
  C  122Sn(16O,3nγ)  D  122Sn(18O,5nγ)
  E  124Sn(16O,5nγ) 

General Comments:

Nuclear structure calculations: 2004Yo04 (levels, transition rates), 1996Gr03 (analyzed band structures), 1992Zh10 (identical bands), 1985Jo03 (levels, transition rates IBA model), 1983Ch46 (yrast and near-yrast routhians, cranking model), 1982Ch30 (M1-γ spectra, core+ quasiparticle model).

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
     0.0ABCDE 1/2(+) 17.7 h 3 
% ε = 100
     
    82.67 5 ABCDE 3/2(+) 0.53 ns 6      82.64 7 
   100
M1(+E2)
     0.0
1/2(+)
   296.11 5 ABCDE (5/2+)      213.45 6 
   296.12 5 
   100 4 
    25 3 
M1
E2
    82.67
     0.0
3/2(+)
1/2(+)
   296.12 5  B    1/2(+),3/2(+)      213.45 6 ?
   296.12 5 
 
   100

M1(+E2)
    82.67
     0.0
3/2(+)
1/2(+)
   445.81 21 A CDE (11/2-) 20 s 1 
% IT = 100
   149.7 2 
   100
E3
   296.11
(5/2+)
   620.95 11  B    3/2(+),5/2(+)      324.9 2 
   324.9 2 
   538.2 2 
   620.9 2 
    ≈4.8
    ≈4.8
   100 11 
    19 3 
M1,E2
M1,E2
M1(+E2)
E2(+M1)
   296.11
   296.12
    82.67
     0.0
(5/2+)
1/2(+),3/2(+)
3/2(+)
1/2(+)
   696.47 21  B    (1/2+,3/2+,5/2+)      400.7 5 ?
   400.7 5 ?
   613.8 2 
   697.5 2 ?
   <22
   <22
   100 15 
   <77
[M1,E2]
[M1,E2]
M1(+E2)
M1,E2
   296.11
   296.12
    82.67
     0.0
(5/2+)
1/2(+),3/2(+)
3/2(+)
1/2(+)
   780.29 15  B    (1/2+,3/2+,5/2+)      484.3 3 
   484.3 3 
   697.5 2 
   780.6 10 
  ≈133
  ≈267
  <350
   100 24 
M1,E2
M1,E2
M1,E2
M1,E2
   296.11
   296.12
    82.67
     0.0
(5/2+)
1/2(+),3/2(+)
3/2(+)
1/2(+)
   806.90 19  B    (1/2,3/2,5/2+)      724.4 6 
   806.9 2 
    33 17 
   100 17 


    82.67
     0.0
3/2(+)
1/2(+)
  1016.84 15  B    (1/2+,3/2+,5/2+)      720.6 8 
   934.1 2 
  1016.9 2 
    58 25 
   100 17 
    85 12 
M1(+E2)
M1,E2

   296.11
    82.67
     0.0
(5/2+)
3/2(+)
1/2(+)
  1035.7 4   CDE (13/2-)      589.7 4 
   100
D+Q
   445.81
(11/2-)
  1145.2 4   CDE (15/2-)      109.5 2 
   699.6 4 
     1.6 4 
   100 11 

(Q)
  1035.7
   445.81
(13/2-)
(11/2-)
  1367.4 5 ? B    (1/2,3/2,5/2+)      747 1 
  1284.6 8 
  1367.3 6 
    63 40 
    63 19 
   100 19 



   620.95
    82.67
     0.0
3/2(+),5/2(+)
3/2(+)
1/2(+)
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
  1670.0 5   CDE (15/2-)      525 1 
   634.9 4 
    <8
   100 8 
D
D(+Q)
  1145.2
  1035.7
(15/2-)
(13/2-)
  1728.7 5 ? B    (1/2,3/2,5/2)     1107 1 ?
  1432.9 6 ?
  1646.0 8 ?
    32 14 
   100 18 
    64 14 



   620.95
   296.11
    82.67
3/2(+),5/2(+)
(5/2+)
3/2(+)
  1834.9 3  B    (1/2,3/2,5/2)     1538.9 4 
  1538.9 4 
  1751.9 6 
  ≈105
  ≈105
   100 17 



   296.11
   296.12
    82.67
(5/2+)
1/2(+),3/2(+)
3/2(+)
  1869.4 5   CDE (17/2-)      724.3 4 
   833.1 4 
    54 6 
   100 11 
D+Q
(Q)
  1145.2
  1035.7
(15/2-)
(13/2-)
  1950.6 9  B    (1/2,3/2,5/2+)     1143 2 
  1867 2 
  1951 1 
    21 14 
    93 40 
   100 30 



   806.90
    82.67
     0.0
(1/2,3/2,5/2+)
3/2(+)
1/2(+)
  2020.6 6  B    (1/2,3/2,5/2+)     1214.2 8 
  1937 2 
  2020 1 
   100 30 
    60 20 
    70 20 



   806.90
    82.67
     0.0
(1/2,3/2,5/2+)
3/2(+)
1/2(+)
  2051.5 5   CDE (19/2-)      181.9 4 
   906.2 4 
     3.8 10 
   100 9 

Q
  1869.4
  1145.2
(17/2-)
(15/2-)
  2125.3 5   CDE (19/2+) 8.2 ns 4     256.0 3 
   100
(E1)
  1869.4
(17/2-)
  2249.0 5   CDE (19/2-)      379.2 4 
   579.5 4 
    38 6 
   100 13 
D
Q
  1869.4
  1670.0
(17/2-)
(15/2-)
  2551.0 6   CDE (23/2+)      425.6 4 
   100
(Q)
  2125.3
(19/2+)
  2682.2 6   CDE (21/2-)      433.5 4 
   100
D+Q
  2249.0
(19/2-)
  2887.4 7   CDE (21/2-)      836 1 
  1019 1 
   100 20 
   100 20 
D

  2051.5
  1869.4
(19/2-)
(17/2-)
  2946.2 6    D  (19/2+)     1076.6 4 
   100

  1869.4
(17/2-)
  2948.0 6   CDE (23/2-)      265.7 4 
   896 1 
   100 13 
    88 13 
D

  2682.2
  2051.5
(21/2-)
(19/2-)
  3054.1 6   CD  (21/2+)      108.0 4 
   503.1 4 
   928.7 4 
   <25
   100 25 
   100 25 
D

D+Q
  2946.2
  2551.0
  2125.3
(19/2+)
(23/2+)
(19/2+)
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
  3076.2 6    D  (21/2+)      129.8 4 
   525.2 4 
   951.1 4 
   <43
   100 33 
   <67

D

  2946.2
  2551.0
  2125.3
(19/2+)
(23/2+)
(19/2+)
  3104.0 6   CDE (23/2-)      216 1 
  1052.1 4 
    <6
   100 13 

(Q)
  2887.4
  2051.5
(21/2-)
(19/2-)
  3229.0 6   CD  (23/2+)      152.7 4 
   175.1 4 
   678 1 
   <19
   100 13 
    38 13 
D
D(+Q)

  3076.2
  3054.1
  2551.0
(21/2+)
(21/2+)
(23/2+)
  3431.1 7   CD  (25/2+)      202.1 4 
   100
D(+Q)
  3229.0
(23/2+)
  3505.4 6   CDE (25/2-)      557.3 4 
   823.5 4 
   100 33 
   100 33 
D
Q
  2948.0
  2682.2
(23/2-)
(21/2-)
  3514.6 7   CD  (27/2+)      963.6 4 
   100
Q
  2551.0
(23/2+)
  3699.1 8   CD  (27/2+)      268.0 4 
   100
D+Q
  3431.1
(25/2+)
  3701.8 7   CDE (27/2-)      753.8 4 
   100
Q
  2948.0
(23/2-)
  3771.7 6 ?   DE (27/2+)      257 1 ?
  1220.6 4 
   <40
   100 20 

Q
  3514.6
  2551.0
(27/2+)
(23/2+)
  4032.3 7    DE (25/2-)      928 1 ?
   100

  3104.0
(23/2-)
  4065.4 6   CDE (25/2-)      962 1 
  1178.3 4 
   100 50 
   100 50 
D
(Q)
  3104.0
  2887.4
(23/2-)
(21/2-)
  4127.5 9   CD  (29/2+)      428.3 4 
   696 1 
   100 9 
   <18
D+Q

  3699.1
  3431.1
(27/2+)
(25/2+)
  4183.0 6    DE (27/2-)      117.9 4 
   150.7 4 
  1078.6 4 
    43 14 
   100 14 
    57 14 
D
D

  4065.4
  4032.3
  3104.0
(25/2-)
(25/2-)
(23/2-)
  4259.5 7   CD  (31/2+)      745.0 4 
   100
Q
  3514.6
(27/2+)
  4400.1 8    D  (31/2-)      698.3 4 
   100
Q
  3701.8
(27/2-)
  4460.4 6    DE (29/2-)      277.1 4 
   100
D(+Q)
  4183.0
(27/2-)
  4485.8 9   CD  (31/2+)      358.2 4 
   786.8 4 
   100 10 
    20 10 
D(+Q)

  4127.5
  3699.1
(29/2+)
(27/2+)
  4495.9 7    DE (27/2-)      313
   991 1 
 
   100


  4183.0
  3505.4
(27/2-)
(25/2-)
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
  4634.9 6    DE (29/2-)      139.1 4 
   452
   863.2 4 
   933 1 
  1130 1 
   <28
 
   100 20 
   <40
    60 20 
D

(D)
(D)
(Q)
  4495.9
  4183.0
  3771.7
  3701.8
  3505.4
(27/2-)
(27/2-)
(27/2+)
(27/2-)
(25/2-)
  4813.3 6    DE (31/2-)      178.5 4 
   318
   352.4 4 
   631
   100 11 
 
    22 11 
 
D(+Q)

D

  4634.9
  4495.9
  4460.4
  4183.0
(29/2-)
(27/2-)
(29/2-)
(27/2-)
  4830.3 7    DE (31/2-)      195?
   370.0 4 
 
   100

D+Q
  4634.9
  4460.4
(29/2-)
(29/2-)
  4978.6 9    D  (33/2+)      492.9 4 
   851 1 
   100 14 
   <29
D

  4485.8
  4127.5
(31/2+)
(29/2+)
  5062.2 7    DE (33/2-)      232
   249.0 4 
   427
   603
   803 1 ?
 
   100 11 
 
 
   <22

D(+Q)



  4830.3
  4813.3
  4634.9
  4460.4
  4259.5
(31/2-)
(31/2-)
(29/2-)
(29/2-)
(31/2+)
  5206.0 7    DE (33/2-)      375.6 4 
   392?
   571?
   746 1 
   100 25 
 
 
   <50
D



  4830.3
  4813.3
  4634.9
  4460.4
(31/2-)
(31/2-)
(29/2-)
(29/2-)
  5324.4 8    D  (35/2+)     1064.9 4 
   100
(Q)
  4259.5
(31/2+)
  5342.1 13    D  (35/2-)      942 1 
   100
Q
  4400.1
(31/2-)
  5359.3 7    DE (35/2-) 0.64 ps 11     153
   297.5 4 
   529
   545
 
 
 
 

D


  5206.0
  5062.2
  4830.3
  4813.3
(33/2-)
(33/2-)
(31/2-)
(31/2-)
  5427.8 10    D  (35/2+)      449.2 4 
   942 1 
   100 20 
   <40
D

  4978.6
  4485.8
(33/2+)
(31/2+)
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
  5651.1 7    DE (35/2-)      445.1 4 
   589?
   821 1 
   837?
   100 8 
 
   <15
 
D+Q

Q

  5206.0
  5062.2
  4830.3
  4813.3
(33/2-)
(33/2-)
(31/2-)
(31/2-)
  5751.5 7    DE (37/2-) 0.451 ps 21     100
   392.2 4 
   545
   689
 
 
 
 

D(+Q)


  5651.1
  5359.3
  5206.0
  5062.2
(35/2-)
(35/2-)
(33/2-)
(33/2-)
  5941.7 12    D  (37/2+)      514 1 
   963 1 
 
 


  5427.8
  4978.6
(35/2+)
(33/2+)
  6086.0 7    DE (37/2-)      434.9 4 
   727
   880 1 
  1024
   100 9 
 
   <18
 
D+Q



  5651.1
  5359.3
  5206.0
  5062.2
(35/2-)
(35/2-)
(33/2-)
(33/2-)
  6256.3 7    DE (39/2-) 0.299 ps 25     170
   504.6 4 
   605
   897
 
 
 
 

D


  6086.0
  5751.5
  5651.1
  5359.3
(37/2-)
(37/2-)
(35/2-)
(35/2-)
  6299.4 13    D  (39/2+)      975 1 
   100

  5324.4
(35/2+)
  6443.8 13    D  (39/2+)      502 1 
  1016 1 ?
 
 


  5941.7
  5427.8
(37/2+)
(35/2+)
  6477.1 17    D  (39/2-)     1135 1 
   100

  5342.1
(35/2-)
  6525.9 8    DE (39/2-)      440.0 4 
   775
   875 1 
  1167
   100 17 
 
   <33
 
D+Q



  6086.0
  5751.5
  5651.1
  5359.3
(37/2-)
(37/2-)
(35/2-)
(35/2-)
  6840.2 8    DE (41/2-) 0.163 ps +8-10     314
   583.6 4 
   754
  1089
 
 
 
 




  6525.9
  6256.3
  6086.0
  5751.5
(39/2-)
(39/2-)
(37/2-)
(37/2-)
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
  6993.7 8    DE (41/2-)      468.0 4 
   737
   908 1 
  1242
   100 33 
 
   <67
 
D



  6525.9
  6256.3
  6086.0
  5751.5
(39/2-)
(39/2-)
(37/2-)
(37/2-)
  7470.4 9    DE (43/2-)      477
   630 1 
   944?
  1214
 
 
 
 




  6993.7
  6840.2
  6525.9
  6256.3
(41/2-)
(41/2-)
(39/2-)
(39/2-)
  7493.1 9    DE (43/2-)      500 1 
   652
   968 1 
  1238
 
 
 
 
D



  6993.7
  6840.2
  6525.9
  6256.3
(41/2-)
(41/2-)
(39/2-)
(39/2-)
  8008.9 10    DE (45/2-)      517 1 
   538
  1168
 
 
 



  7493.1
  7470.4
  6840.2
(43/2-)
(43/2-)
(41/2-)
  8034.6 9 ?   DE (45/2-)      542?
   564 1 ?
  1041?
  1194?
 
 
 
 




  7493.1
  7470.4
  6993.7
  6840.2
(43/2-)
(43/2-)
(41/2-)
(41/2-)

Jπ(level): For high-spin states (J>11/2) the assignments are from γγ(θ) (DCO) and/or γ(θ) data and associated band structures. In Jπ arguments, ΔJ=2 statement refers to stretched quadrupole (most likely E2) transition and ΔJ=1 to stretched dipole (with possible quadrupole admixture) transition

M(γ): From ce data in 135Pr decay when multipolarity is explicitly defined such as M1, E2, etc. The assignments d or Q (most likely E2) are from angular correlation/distribution data in high-spin reactions.

Back to top

Band Transitions:

E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 1 - νh11/2~#π[(h11/2)(g7/2)].
  2946.2 6  (19/2+)        
  3076.2 6  (21/2+)      129.8 4 
   525.2 4 
   951.1 4 
   <43
   100 33 
   <67

D

  2946.2
  2551.0
  2125.3
(19/2+)
(23/2+)
(19/2+)
  3229.0 6  (23/2+)      152.7 4 
   175.1 4 
   678 1 
   <19
   100 13 
    38 13 
D
D(+Q)

  3076.2
  3054.1
  2551.0
(21/2+)
(21/2+)
(23/2+)
  3431.1 7  (25/2+)      202.1 4 
   100
D(+Q)
  3229.0
(23/2+)
  3699.1 8  (27/2+)      268.0 4 
   100
D+Q
  3431.1
(25/2+)
  4127.5 9  (29/2+)      428.3 4 
   696 1 
   100 9 
   <18
D+Q

  3699.1
  3431.1
(27/2+)
(25/2+)
  4485.8 9  (31/2+)      358.2 4 
   786.8 4 
   100 10 
    20 10 
D(+Q)

  4127.5
  3699.1
(29/2+)
(27/2+)
  4978.6 9  (33/2+)      492.9 4 
   851 1 
   100 14 
   <29
D

  4485.8
  4127.5
(31/2+)
(29/2+)
  5427.8 10  (35/2+)      449.2 4 
   942 1 
   100 20 
   <40
D

  4978.6
  4485.8
(33/2+)
(31/2+)
  5941.7 12  (37/2+)      514 1 
   963 1 
 
 


  5427.8
  4978.6
(35/2+)
(33/2+)
  6443.8 13  (39/2+)      502 1 
  1016 1 ?
 
 


  5941.7
  5427.8
(37/2+)
(35/2+)
E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 2 - νs1/2~#νh11/22.
  2125.3 5  (19/2+) 8.2 ns 4       
  2551.0 6  (23/2+)      425.6 4 
   100
(Q)
  2125.3
(19/2+)
  3514.6 7  (27/2+)      963.6 4 
   100
Q
  2551.0
(23/2+)
  4259.5 7  (31/2+)      745.0 4 
   100
Q
  3514.6
(27/2+)
  5324.4 8  (35/2+)     1064.9 4 
   100
(Q)
  4259.5
(31/2+)
  6299.4 13  (39/2+)      975 1 
   100

  5324.4
(35/2+)
E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 3 - νh11/2~#πh11/22.
  4065.4 6  (25/2-)        
  4183.0 6  (27/2-)      117.9 4 
   150.7 4 
  1078.6 4 
    43 14 
   100 14 
    57 14 
D
D

  4065.4
  4032.3
  3104.0
(25/2-)
(25/2-)
(23/2-)
  4460.4 6  (29/2-)      277.1 4 
   100
D(+Q)
  4183.0
(27/2-)
  4830.3 7  (31/2-)      195?
   370.0 4 
 
   100

D+Q
  4634.9
  4460.4
(29/2-)
(29/2-)
  5206.0 7  (33/2-)      375.6 4 
   392?
   571?
   746 1 
   100 25 
 
 
   <50
D



  4830.3
  4813.3
  4634.9
  4460.4
(31/2-)
(31/2-)
(29/2-)
(29/2-)
  5651.1 7  (35/2-)      445.1 4 
   589?
   821 1 
   837?
   100 8 
 
   <15
 
D+Q

Q

  5206.0
  5062.2
  4830.3
  4813.3
(33/2-)
(33/2-)
(31/2-)
(31/2-)
  6086.0 7  (37/2-)      434.9 4 
   727
   880 1 
  1024
   100 9 
 
   <18
 
D+Q



  5651.1
  5359.3
  5206.0
  5062.2
(35/2-)
(35/2-)
(33/2-)
(33/2-)
  6525.9 8  (39/2-)      440.0 4 
   775
   875 1 
  1167
   100 17 
 
   <33
 
D+Q



  6086.0
  5751.5
  5651.1
  5359.3
(37/2-)
(37/2-)
(35/2-)
(35/2-)
  6993.7 8  (41/2-)      468.0 4 
   737
   908 1 
  1242
   100 33 
 
   <67
 
D



  6525.9
  6256.3
  6086.0
  5751.5
(39/2-)
(39/2-)
(37/2-)
(37/2-)
  7493.1 9  (43/2-)      500 1 
   652
   968 1 
  1238
 
 
 
 
D



  6993.7
  6840.2
  6525.9
  6256.3
(41/2-)
(41/2-)
(39/2-)
(39/2-)
E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
  8008.9 10  (45/2-)      517 1 
   538
  1168
 
 
 



  7493.1
  7470.4
  6840.2
(43/2-)
(43/2-)
(41/2-)
E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 4 - TRIAXIAL band.
   445.81 21  (11/2-) 20 s 1 
% IT = 100
     
  1035.7 4  (13/2-)      589.7 4 
   100
D+Q
   445.81
(11/2-)
  1145.2 4  (15/2-)      109.5 2 
   699.6 4 
     1.6 4 
   100 11 

(Q)
  1035.7
   445.81
(13/2-)
(11/2-)
  1869.4 5  (17/2-)      724.3 4 
   833.1 4 
    54 6 
   100 11 
D+Q
(Q)
  1145.2
  1035.7
(15/2-)
(13/2-)
  2051.5 5  (19/2-)      181.9 4 
   906.2 4 
     3.8 10 
   100 9 

Q
  1869.4
  1145.2
(17/2-)
(15/2-)
  2887.4 7  (21/2-)      836 1 
  1019 1 
   100 20 
   100 20 
D

  2051.5
  1869.4
(19/2-)
(17/2-)
  3104.0 6  (23/2-)      216 1 
  1052.1 4 
    <6
   100 13 

(Q)
  2887.4
  2051.5
(21/2-)
(19/2-)
E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 5 - Four-quasiparticle band.
  4495.9 7  (27/2-)        
  4634.9 6  (29/2-)      139.1 4 
   452
   863.2 4 
   933 1 
  1130 1 
   <28
 
   100 20 
   <40
    60 20 
D

(D)
(D)
(Q)
  4495.9
  4183.0
  3771.7
  3701.8
  3505.4
(27/2-)
(27/2-)
(27/2+)
(27/2-)
(25/2-)
  4813.3 6  (31/2-)      178.5 4 
   318
   352.4 4 
   631
   100 11 
 
    22 11 
 
D(+Q)

D

  4634.9
  4495.9
  4460.4
  4183.0
(29/2-)
(27/2-)
(29/2-)
(27/2-)
  5062.2 7  (33/2-)      232
   249.0 4 
   427
   603
   803 1 ?
 
   100 11 
 
 
   <22

D(+Q)



  4830.3
  4813.3
  4634.9
  4460.4
  4259.5
(31/2-)
(31/2-)
(29/2-)
(29/2-)
(31/2+)
  5359.3 7  (35/2-) 0.64 ps 11     153
   297.5 4 
   529
   545
 
 
 
 

D


  5206.0
  5062.2
  4830.3
  4813.3
(33/2-)
(33/2-)
(31/2-)
(31/2-)
  5751.5 7  (37/2-) 0.451 ps 21     100
   392.2 4 
   545
   689
 
 
 
 

D(+Q)


  5651.1
  5359.3
  5206.0
  5062.2
(35/2-)
(35/2-)
(33/2-)
(33/2-)
  6256.3 7  (39/2-) 0.299 ps 25     170
   504.6 4 
   605
   897
 
 
 
 

D


  6086.0
  5751.5
  5651.1
  5359.3
(37/2-)
(37/2-)
(35/2-)
(35/2-)
  6840.2 8  (41/2-) 0.163 ps +8-10     314
   583.6 4 
   754
  1089
 
 
 
 




  6525.9
  6256.3
  6086.0
  5751.5
(39/2-)
(39/2-)
(37/2-)
(37/2-)
E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
  7470.4 9  (43/2-)      477
   630 1 
   944?
  1214
 
 
 
 




  6993.7
  6840.2
  6525.9
  6256.3
(41/2-)
(41/2-)
(39/2-)
(39/2-)
  8034.6 9  (45/2-)      542?
   564 1 ?
  1041?
  1194?
 
 
 
 




  7493.1
  7470.4
  6993.7
  6840.2
(43/2-)
(43/2-)
(41/2-)
(41/2-)
E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 6 - νh11/2~#νh11/22.
  3701.8 7  (27/2-)        
  4400.1 8  (31/2-)      698.3 4 
   100
Q
  3701.8
(27/2-)
  5342.1 13  (35/2-)      942 1 
   100
Q
  4400.1
(31/2-)
  6477.1 17  (39/2-)     1135 1 
   100

  5342.1
(35/2-)

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Additional Gamma Data:















E(level)
(keV)
Jπ(level)T1/2(level)E(γ)
(keV)
MultipolarityMixing
Ratio
Conversion
Coefficient
Additional Data
    82.67 3/2(+) 0.53 ns 6      82.64 7 M1(+E2)0.4 LT2.19B(M1)(W.u.)=0.022 3, α=2.19 15, α(K)=1.77 4, α(L)=0.33 9, α(M)=0.071 21, α(N)=0.015 5, α(O)=0.0024 6, α(P)=0.000133 3, α(N+)=0.018 5
   296.11 (5/2+)      213.45 6 M1 0.1429α=0.1429, α(K)=0.1221 18, α(L)=0.01645 23, α(M)=0.00344 5, α(N)=0.000763 11, α(O)=0.0001238 18, α(P)=9.40×10-6 14, α(N+)=0.000897 13
(5/2+)      296.12 5 E2 0.0508α=0.0508, α(K)=0.0407 6, α(L)=0.00792 12, α(M)=0.001704 24, α(N)=0.000371 6, α(O)=5.64×10-5 8, α(P)=2.68E-6 4, α(N+)=0.000431 6
   296.12 1/2(+),3/2(+)      296.12 5 M1(+E2)0.9 LT0.0576α=0.0576 22, α(K)=0.0487 24, α(L)=0.0071 3, α(M)=0.00148 7, α(N)=0.000328 14, α(O)=5.24×10-5 14, α(P)=3.6E-6 3, α(N+)=0.000384 15
   445.81 (11/2-) 20 s 1 
% IT = 100
   149.7 2 E3 3.73B(E3)(W.u.)=7.2E-3 4, α=3.73, α(K)=1.515 23, α(L)=1.72 3, α(M)=0.396 7, α(N)=0.0851 14, α(O)=0.01182 19, α(P)=8.39E-5 13, α(N+)=0.0970 16
   620.95 3/2(+),5/2(+)      324.9 2 M1,E2 0.042α=0.042 5, α(K)=0.035 5, α(L)=0.00551 21, α(M)=0.00117 6, α(N)=0.000257 11, α(O)=4.04×10-5 7, α(P)=2.6E-6 5, α(N+)=0.000300 11
3/2(+),5/2(+)      324.9 2 M1,E2 0.042α=0.042 5, α(K)=0.035 5, α(L)=0.00551 21, α(M)=0.00117 6, α(N)=0.000257 11, α(O)=4.04×10-5 7, α(P)=2.6E-6 5, α(N+)=0.000300 11
3/2(+),5/2(+)      538.2 2 M1(+E2)0.7 LT0.0123α=0.0123 7, α(K)=0.0105 7, α(L)=0.00140 6, α(M)=0.000292 11, α(N)=6.5×10-5 3, α(O)=1.05E-5 5, α(P)=7.9E-7 6, α(N+)=7.6E-5 3
3/2(+),5/2(+)      620.9 2 E2(+M1)1.2 GT0.0067α=0.0067 7, α(K)=0.0057 6, α(L)=0.00081 6, α(M)=0.000170 11, α(N)=3.76×10-5 25, α(O)=6.0E-6 5, α(P)=4.1E-7 5, α(N+)=4.4E-5 3
   696.47 (1/2+,3/2+,5/2+)      400.7 5 [M1,E2] 0.024α=0.024 4, α(K)=0.020 4, α(L)=0.00295 14, α(M)=0.000621 23, α(N)=0.000137 6, α(O)=2.18×10-5 15, α(P)=1.5E-6 4, α(N+)=0.000160 8
(1/2+,3/2+,5/2+)      400.7 5 [M1,E2] 0.024α=0.024 4, α(K)=0.020 4, α(L)=0.00295 14, α(M)=0.000621 23, α(N)=0.000137 6, α(O)=2.18×10-5 15, α(P)=1.5E-6 4, α(N+)=0.000160 8
(1/2+,3/2+,5/2+)      613.8 2 M1(+E2)0.7 LT0.0088α=0.0088 6, α(K)=0.0076 5, α(L)=0.00100 5, α(M)=0.000209 10, α(N)=4.64×10-5 21, α(O)=7.5E-6 4, α(P)=5.7E-7 4, α(N+)=5.44E-5 25
(1/2+,3/2+,5/2+)      697.5 2 M1,E2 0.0057α=0.0057 12, α(K)=0.0049 10, α(L)=0.00066 11, α(M)=0.000138 21, α(N)=3.1×10-5 5, α(O)=4.9E-6 9, α(P)=3.6E-7 9, α(N+)=3.6E-5 6
   780.29 (1/2+,3/2+,5/2+)      484.3 3 M1,E2 0.014α=0.014 3, α(K)=0.0121 24, α(L)=0.00172 18, α(M)=0.00036 4, α(N)=8.0×10-5 8, α(O)=1.28E-5 15, α(P)=8.9E-7 21, α(N+)=9.4E-5 10
(1/2+,3/2+,5/2+)      484.3 3 M1,E2 0.014α=0.014 3, α(K)=0.0121 24, α(L)=0.00172 18, α(M)=0.00036 4, α(N)=8.0×10-5 8, α(O)=1.28E-5 15, α(P)=8.9E-7 21, α(N+)=9.4E-5 10
(1/2+,3/2+,5/2+)      697.5 2 M1,E2 0.0057α=0.0057 12, α(K)=0.0049 10, α(L)=0.00066 11, α(M)=0.000138 21, α(N)=3.1×10-5 5, α(O)=4.9E-6 9, α(P)=3.6E-7 9, α(N+)=3.6E-5 6
(1/2+,3/2+,5/2+)      780.6 10 M1,E2 0.0044α=0.0044 9, α(K)=0.0037 8, α(L)=0.00050 9, α(M)=0.000104 17, α(N)=2.3×10-5 4, α(O)=3.7E-6 7, α(P)=2.8E-7 7, α(N+)=2.7E-5 5
  1016.84 (1/2+,3/2+,5/2+)      720.6 8 M1(+E2)1 LT0.0058α=0.0058 6, α(K)=0.0050 5, α(L)=0.00066 5, α(M)=0.000137 10, α(N)=3.03×10-5 23, α(O)=4.9E-6 4, α(P)=3.7E-7 4, α(N+)=3.6E-5 3
(1/2+,3/2+,5/2+)      934.1 2 M1,E2 0.0029α=0.0029 6, α(K)=0.0025 5, α(L)=0.00032 6, α(M)=6.8×10-5 11, α(N)=1.50E-5 25, α(O)=2.4E-6 5, α(P)=1.8E-7 4, α(N+)=1.8E-5 3
  1035.7 (13/2-)      589.7 4 D+Q-0.42 +6-10 
  1670.0 (15/2-)      634.9 4 D(+Q)-0.02 5 
  1869.4 (17/2-)      724.3 4 D+Q-0.25 9 
  2125.3 (19/2+) 8.2 ns 4     256.0 3 (E1) 0.0188B(E1)(W.u.)=1.8E-6 1, α=0.0188, α(K)=0.01613 24, α(L)=0.00212 3, α(M)=0.000441 7, α(N)=9.71E-5 14, α(O)=1.547E-5 23, α(P)=1.080E-6 16, α(N+)=0.0001136 17
  2682.2 (21/2-)      433.5 4 D+Q-0.16 4 
  3054.1 (21/2+)      928.7 4 D+Q-0.16 8 
E(level)
(keV)
Jπ(level)T1/2(level)E(γ)
(keV)
MultipolarityMixing
Ratio
Conversion
Coefficient
Additional Data
  3229.0 (23/2+)      175.1 4 D(+Q)+0.05 8 
  3431.1 (25/2+)      202.1 4 D(+Q)+0.07 7 
  3699.1 (27/2+)      268.0 4 D+Q-0.07 2 
  4127.5 (29/2+)      428.3 4 D+Q-0.11 3 
  4460.4 (29/2-)      277.1 4 D(+Q)-0.03 5 
  4485.8 (31/2+)      358.2 4 D(+Q)-0.06 7 
  4813.3 (31/2-)      178.5 4 D(+Q)+0.06 7 
  4830.3 (31/2-)      370.0 4 D+Q-0.10 6 
  5062.2 (33/2-)      249.0 4 D(+Q)-0.02 +4-6 
  5651.1 (35/2-)      445.1 4 D+Q-0.23 3 
  5751.5 (37/2-) 0.451 ps 21     392.2 4 D(+Q)-0.04 6 
  6086.0 (37/2-)      434.9 4 D+Q-0.18 5 
  6525.9 (39/2-)      440.0 4 D+Q-0.19 +8-11 

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Additional Level Data and Comments:

E(level)Jπ(level)T1/2(level)Comments
   445.81(11/2-) 20 s 1 
% IT = 100
E(level): TRIAXIAL band.
  1035.7(13/2-)   E(level): TRIAXIAL band.
  1145.2(15/2-)   E(level): TRIAXIAL band.
  1869.4(17/2-)   E(level): TRIAXIAL band.
  2051.5(19/2-)   E(level): TRIAXIAL band.
  2125.3(19/2+) 8.2 ns 4  μ=-0.66 10 (1989Ra17,1982Ze01)
E(level): νs1/2~#νh11/22.
  2551.0(23/2+)   E(level): νs1/2~#νh11/22.
  2887.4(21/2-)   E(level): TRIAXIAL band.
  2946.2(19/2+)   E(level): νh11/2~#π[(h11/2)(g7/2)].
  3076.2(21/2+)   E(level): νh11/2~#π[(h11/2)(g7/2)].
  3104.0(23/2-)   E(level): TRIAXIAL band.
  3229.0(23/2+)   E(level): νh11/2~#π[(h11/2)(g7/2)].
  3431.1(25/2+)   E(level): νh11/2~#π[(h11/2)(g7/2)].
  3514.6(27/2+)   E(level): νs1/2~#νh11/22.
  3699.1(27/2+)   E(level): νh11/2~#π[(h11/2)(g7/2)].
  3701.8(27/2-)   E(level): νh11/2~#νh11/22.
  4065.4(25/2-)   E(level): νh11/2~#πh11/22.
  4127.5(29/2+)   E(level): νh11/2~#π[(h11/2)(g7/2)].
  4183.0(27/2-)   E(level): νh11/2~#πh11/22.
  4259.5(31/2+)   E(level): νs1/2~#νh11/22.
  4400.1(31/2-)   E(level): νh11/2~#νh11/22.
  4460.4(29/2-)   E(level): νh11/2~#πh11/22.
  4485.8(31/2+)   E(level): νh11/2~#π[(h11/2)(g7/2)].
  4495.9(27/2-)   E(level): Four-quasiparticle band.
  4634.9(29/2-)   E(level): Four-quasiparticle band.
E(level)Jπ(level)T1/2(level)Comments
  4813.3(31/2-)   E(level): Four-quasiparticle band.
  4830.3(31/2-)   E(level): νh11/2~#πh11/22.
  4978.6(33/2+)   E(level): νh11/2~#π[(h11/2)(g7/2)].
  5062.2(33/2-)   E(level): Four-quasiparticle band.
  5206.0(33/2-)   E(level): νh11/2~#πh11/22.
  5324.4(35/2+)   E(level): νs1/2~#νh11/22.
  5342.1(35/2-)   E(level): νh11/2~#νh11/22.
  5359.3(35/2-) 0.64 ps 11  E(level): Four-quasiparticle band.
T1/2(level): From ΔS(a) method (2005JaZZ).
  5427.8(35/2+)   E(level): νh11/2~#π[(h11/2)(g7/2)].
  5651.1(35/2-)   E(level): νh11/2~#πh11/22.
  5751.5(37/2-) 0.451 ps 21  E(level): Four-quasiparticle band.
T1/2(level): From ΔS(a) method (2005JaZZ).
  5941.7(37/2+)   E(level): νh11/2~#π[(h11/2)(g7/2)].
  6086.0(37/2-)   E(level): νh11/2~#πh11/22.
  6256.3(39/2-) 0.299 ps 25  E(level): Four-quasiparticle band.
T1/2(level): From ΔS(a) method (2005JaZZ).
  6299.4(39/2+)   E(level): νs1/2~#νh11/22.
  6443.8(39/2+)   E(level): νh11/2~#π[(h11/2)(g7/2)].
  6477.1(39/2-)   E(level): νh11/2~#νh11/22.
  6525.9(39/2-)   E(level): νh11/2~#πh11/22.
  6840.2(41/2-) 0.163 ps +8-10  E(level): Four-quasiparticle band.
T1/2(level): From ΔS(a) method (2005JaZZ).
  6993.7(41/2-)   E(level): νh11/2~#πh11/22.
  7470.4(43/2-)   E(level): Four-quasiparticle band.
  7493.1(43/2-)   E(level): νh11/2~#πh11/22.
  8008.9(45/2-)   E(level): νh11/2~#πh11/22.
  8034.6(45/2-)   E(level): Four-quasiparticle band.

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Additional Gamma Comments:

E(level)E(gamma)Comments
    82.67    82.64E(γ): from 135Pr ε decay
M(γ): from α(K)exp and K/L ratio in 135Pr ε decay and α(exp) deduced from intensity balance in 135Ce IT decay. In a ce spectrum shown by 1970Dr04 (in 135Ce IT decay), K/L ratio seems much smaller than K/L(theory for M1)=7.3, suggesting some E2 admixture
   296.11   213.45E(γ): from 135Pr ε decay. Eγ=212.9 2 in IT decay. Multiply placed
   296.12E(γ): from 135Pr ε decay. Eγ=295.8 5 in IT decay. Multiply placed
I(γ): from IT decay
M(γ): α(K)exp in IT decay gives E2(+M1) with δ>1.2, ΔJπ requires E2
   296.12   213.45E(γ): Multiply placed
I(γ): probable weak component
   296.12E(γ): Multiply placed
   445.81   149.7E(γ): from (16O,3nγ)
   620.95   324.9E(γ): Multiply placed with intensity suitably divided
I(γ): Multiply placed with intensity suitably divided
   324.9E(γ): Multiply placed with intensity suitably divided
I(γ): Multiply placed with intensity suitably divided
   696.47   400.7E(γ): Multiply placed with undivided intensity
I(γ): Multiply placed with undivided intensity
   400.7E(γ): Multiply placed with undivided intensity
I(γ): Multiply placed with undivided intensity
   697.5E(γ): Multiply placed with undivided intensity
I(γ): Multiply placed with undivided intensity
   780.29   484.3E(γ): Multiply placed with intensity suitably divided
I(γ): Multiply placed with intensity suitably divided
   484.3E(γ): Multiply placed with intensity suitably divided
I(γ): Multiply placed with intensity suitably divided
   697.5E(γ): Multiply placed with undivided intensity
I(γ): Multiply placed with undivided intensity
  1035.7   589.7M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions
  1145.2   699.6M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=2, quadrupole (E2)
  1670.0   525M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions
   634.9M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions
  1834.9  1538.9E(γ): Multiply placed with intensity suitably divided
I(γ): Multiply placed with intensity suitably divided
  1538.9E(γ): Multiply placed with intensity suitably divided
I(γ): Multiply placed with intensity suitably divided
  1869.4   724.3I(γ): other: 227 23 in (16O,3nγ)
M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions
   833.1M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=2, quadrupole (E2)
  2051.5   906.2M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=2, quadrupole (E2)
  2125.3   256.0M(γ): ΔJ=1, dipole from γγ(θ) and assigned Jπ’s
  2249.0   379.2M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions
   579.5M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=2, quadrupole (E2)
E(level)E(gamma)Comments
  2551.0   425.6M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=2, quadrupole (E2)
  2682.2   433.5M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions
  2887.4   836M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions
  2948.0   265.7M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions
  3054.1   108.0M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions
   928.7M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions
  3076.2   525.2M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions
  3104.0  1052.1M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=2, quadrupole (E2)
  3229.0   152.7M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions
   175.1M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions
  3431.1   202.1M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions
  3505.4   557.3M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions
   823.5M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=2, quadrupole (E2)
  3514.6   963.6M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=2, quadrupole (E2)
  3699.1   268.0M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions
  3701.8   753.8M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=2, quadrupole (E2)
  3771.7  1220.6M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=2, quadrupole (E2)
  4065.4   962M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions
  1178.3M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=2, quadrupole (E2)
  4127.5   428.3M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions
  4183.0   117.9M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions
   150.7M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions
  4259.5   745.0M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=2, quadrupole (E2)
  4400.1   698.3M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=2, quadrupole (E2)
  4460.4   277.1M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions
E(level)E(gamma)Comments
  4485.8   358.2M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions
  4634.9   139.1M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions
   863.2M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions
   933M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions
  4813.3   178.5M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions
   352.4M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions
  4830.3   370.0M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions
  4978.6   492.9M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions
  5062.2   249.0M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions
  5206.0   375.6M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions
  5324.4  1064.9M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=2, quadrupole (E2)
  5342.1   942M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=2, quadrupole (E2)
  5359.3   297.5E(γ): Possibly the most intense branch
M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions
  5427.8   449.2M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions
  5651.1   445.1M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions
   821M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=2, quadrupole (E2)
  5751.5   392.2E(γ): Possibly the most intense branch
M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions
  6086.0   434.9M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions
  6256.3   504.6E(γ): Possibly the most intense branch
M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions
  6525.9   440.0M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions
  6840.2   583.6E(γ): Possibly the most intense branch
  6993.7   468.0M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions
  7470.4   630E(γ): Possibly the most intense branch
  7493.1   500M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions
  8008.9   517E(γ): Possibly the most intense branch
E(level)E(gamma)Comments

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