ADOPTED LEVELS, GAMMAS for 189Pt

Authors: T.D. Johnson, Balraj Singh |  Citation: Nucl. Data Sheets 142, 1 (2017) |  Cutoff date: 15-Apr-2017 

 Full ENSDF file | Adopted Levels (PDF version) 


Q(β-)=-2887 keV 22S(n)= 6720 keV 11S(p)= 5413 keV 14Q(α)= 3912 keV 10
Reference: 2017WA10

References:
  A  189Au ε decay (28.7 M)  B  189Au ε decay (4.59 M)
  C  176Yb(18O,5nγ)  D  188Os(α,3nγ),191Ir(p,3nγ)
  E  190Pt(p,d) 

General Comments:

189Pt produced and identified by 1955Sm42 in Ir(p,xn),E=50-130 MeV. Measured β, γ and half-life of the activity. Later studies of this decay: 1960Po07, 1960Ma28, 1961Kr02, 1961An02, 1962Kr04, 1962Ha24, 1962Gr27, 1963Th07, 1964Le07, 1964Kr03, 1965Ja12, 1967Na02, 1970Ba10, 1970Ba56, 1971Pl08, 1972Ba21, 1972He05, 1975Ru06, 1980Be27, 2000Mo05, 2000Zi04

Q-value: S(2n)=15927 26, S(2p)=9828 10 (2017Wa10)










E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
     0.0ABCDE 3/2- 10.87 h 12 
% ε = 100
     
     6.40 3 ABCD  5/2-        6.40 4 S
   100
[M1]
     0.0
3/2-
    45.78 25 A   E (1/2)-       39.47 3 
    45.69 3 
    14.4 23 
   100 25 
E2
M1+E2
     6.40
     0.0
5/2-
3/2-
    88.30 3 A   E 3/2-       42.75 5 ?
    82.2 5 
    88.41 3 
 
 
 
M1+E2
M1+E2
M1+E2
    45.78
     6.40
     0.0
(1/2)-
5/2-
3/2-
   172.79 6  BCDE 9/2- 464 ns 25 
% IT = 100
   166.40 5 
   100
E2
     6.40
5/2-
   191.4 2  BCDE (13/2+) 143 µs 5 
% IT = 100
    18.7 9 S
   100
[M2]
   172.79
9/2-
   202.2 5    D  (11/2+)       11.3S
 

   191.4
(13/2+)
   222.30 4 A     (3/2,5/2)-      134.26 4 
   176.1 5 
   215.68 5 
   221.95 16 
    24 4 
 
    62 9 
   100 12 
M1+E2

M1+E2
E2
    88.30
    45.78
     6.40
     0.0
3/2-
(1/2)-
5/2-
3/2-
   237.4 1 A CD  (9/2)-      231.0 1 
   100
E2
     6.40
5/2-
   261 5     E 1/2-,3/2-        
   285 5     E        
   348.45 5 A   E (5/2,3/2)-      110.8 5 ?
   126.31 5 
   259.68 10 
   302.4 5 ?
   342.0 5 
   348.15 15 
     4 1 
     8.8 12 
    13 4 
 
    20 4 
   100 7 
(E2)
M1+E2
M1+E2


M1(+E2)
   237.4
   222.30
    88.30
    45.78
     6.40
     0.0
(9/2)-
(3/2,5/2)-
3/2-
(1/2)-
5/2-
3/2-
   356.72 23   CD  (9/2-)      350.3 3 
   100

     6.40
5/2-
   447.67 8 A   E (3/2,5/2)-      225.7 5 
   359.4 5 
   441.04 14 
   447.77 9 
    20 4 
     8 3 
    69 8 
   100 13 
M1(+E2)

M1+E2
M1(+E2)
   222.30
    88.30
     6.40
     0.0
(3/2,5/2)-
3/2-
5/2-
3/2-
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   493.3 4  B DE 11/2-      321.1 5 
   100
M1+E2
   172.79
9/2-
   499.2 2   CD  (17/2+) 211.4 ps 55     307.8 1 
   100
E2
   191.4
(13/2+)
   529.62 11 A     (1/2,3/2,5/2)-      484.2 5 
   523.4 5 
   529.59 11 
    13 4 
    13 7 
   100 18 


M1(+E2)
    45.78
     6.40
     0.0
(1/2)-
5/2-
3/2-
   531.3 3   CD  (15/2+)      329.2 5 
   339.9 1 
 
   100

D+Q
   202.2
   191.4
(11/2+)
(13/2+)
   574 5     E 1/2-,3/2-        
   608.6 2   CD  (13/2-)      251.9 3 
   371.2 1 
    11 4 
   100 5 

(E2)
   356.72
   237.4
(9/2-)
(9/2)-
   653.8 2   CD  (15/2+)      462.4 1 
   100
D+Q
   191.4
(13/2+)
   712.0 2   CD  (13/2-)      539.5 3 
   100
(E2)
   172.79
9/2-
   843.7 6    D  (13/2-)      487.0 5 
   100

   356.72
(9/2-)
   902.9 7    D       409.6 5 
 

   493.3
11/2-
   944.0 2   CD  (17/2+)      290.2 5 
   412.7 1 
   444.8 5 
 
   100 15 
    30 9 

D+Q
(E2)
   653.8
   531.3
   499.2
(15/2+)
(15/2+)
(17/2+)
   955.0 2   CD  (21/2+) 175.4 ps 49     455.8 1 
   100
(E2)
   499.2
(17/2+)
   983.5 3   CD  (19/2+)      452.2 1 
   484.3 3 
   100 15 
    51 8 
(E2)
D+Q
   531.3
   499.2
(15/2+)
(17/2+)
  1048.5 7    D  (15/2-)      555.2 5 
   100

   493.3
11/2-
  1081.1 2   CD  (17/2-)      472.4 1 
   100
(E2)
   608.6
(13/2-)
  1160.87 14 A     (3/2+)      631.2 9 
   713.24 17 
   812.8 3 
  1071.5 6 
  1160.6 3 
    12.1 23 
   100 14 
    63 9 
    27 5 
    35 5 
E1
E1
E1
E1
E1
   529.62
   447.67
   348.45
    88.30
     0.0
(1/2,3/2,5/2)-
(3/2,5/2)-
(5/2,3/2)-
3/2-
3/2-
  1185.31 20   CD  (19/2+)      531.5 1 
   686.1 1 
    40 6 
   100 5 
(E2)
D+Q
   653.8
   499.2
(15/2+)
(17/2+)
  1361.5 2   CD  (17/2-)      280.4 3 
   649.5 1 
   707.7 1 
   862.3 1 
    17 5 
    56 9 
    64 10 
   100 15 
(E2)
Q
D
D
  1081.1
   712.0
   653.8
   499.2
(17/2-)
(13/2-)
(15/2+)
(17/2+)
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
  1414.0 6    D       470.0 5 
 

   944.0
(17/2+)
  1415.9 8    D  (17/2-)      572.2 5 
 

   843.7
(13/2-)
  1444.0 3   CD  (21/2+)      460.5 3 
   500.0 1 
   944.8 5 
    30 10 
   100 16 
    10 4 
D+Q
(E2)
Q
   983.5
   944.0
   499.2
(19/2+)
(17/2+)
(17/2+)
  1490.4 2   CD  (19/2-)      128.9 1 
   409.3 1 
   536 1 
    35 6 
   100 5 
 
(E2)
(E2)

  1361.5
  1081.1
   955.0
(17/2-)
(17/2-)
(21/2+)
  1512.1 2   CD  (21/2-)       21.7S
   150.6 3 
   326.8 1 
   557.1 1 
 
    10 4 
    84 5 
   100 5 

(E2)
D
D
  1490.4
  1361.5
  1185.31
   955.0
(19/2-)
(17/2-)
(19/2+)
(21/2+)
  1529.3 3   CD  (25/2+)      574.3 1 
   100
(E2)
   955.0
(21/2+)
  1555.7 3   CD  (23/2+)      572.2 3 
   600.7 5 
   100 16 
    22 7 
(E2)
D+Q
   983.5
   955.0
(19/2+)
(21/2+)
  1695.7 3   C   (23/2-)      183.6 1 
   740.7 3 
   100 6 
     4 2 
D+Q

  1512.1
   955.0
(21/2-)
(21/2+)
  1714.3 3   CD  (25/2-)       18.6S
   202.2 1 
 
   100

(E2)
  1695.7
  1512.1
(23/2-)
(21/2-)
  1727.4 4    D  (23/2+)      542.1 5 
   772.4 5 
 
 


  1185.31
   955.0
(19/2+)
(21/2+)
  2009.5 3   C   (25/2+)      565.5 1 
  1054.5 5 
  <100
    14 5 

Q
  1444.0
   955.0
(21/2+)
(21/2+)
  2055.2 3   CD  (27/2-)      340.9 1 
   100
D+Q
  1714.3
(25/2-)
  2189.5 3   CD  (29/2+)      660.2 1 
   100
Q
  1529.3
(25/2+)
  2219.4 4   CD  (27/2+)      663.7 3 
   100
Q
  1555.7
(23/2+)
  2291.4 3   CD  (29/2-)      236.2 3 
   577.1 1 
    15 3 
   100 6 
D+Q
(E2)
  2055.2
  1714.3
(27/2-)
(25/2-)
  2303.7 3   C   (29/2-)      248.5 3 
   589.4 1 
    22 4 
   100 6 
D+Q
(E2)
  2055.2
  1714.3
(27/2-)
(25/2-)
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
  2539.7 4   C   (27/2+)     1010.4 5 
   100
D+Q
  1529.3
(25/2+)
  2620.4 3   C   (31/2-)      316.7 1 
   329.0 3 
   565.2 1 
   100 15 
    42 7 
    87 13 
D+Q
D+Q
(E2)
  2303.7
  2291.4
  2055.2
(29/2-)
(29/2-)
(27/2-)
  2635.5 3   C   (29/2+)      626.0 1 
  1106.2 3 
   100 5 
    17 6 
Q
Q
  2009.5
  1529.3
(25/2+)
(25/2+)
  2688.4 3   CD  (31/2-)      397.0 3 
   633.2 1 
    63 10 
   100 15 
D+Q
Q
  2291.4
  2055.2
(29/2-)
(27/2-)
  2729.4 3   C   (29/2+)      189.7 5 
   539.9 3 
  1200.1 5 
 
   100 32 
    41 14 

(E2)
Q
  2539.7
  2189.5
  1529.3
(27/2+)
(29/2+)
(25/2+)
  2818.6 5   C        763.4 5 
   100

  2055.2
(27/2-)
  2839.8 3   C   (33/2-)      536.1 1 
   548.4 3 
   100 15 
    46 8 
(E2)
(E2)
  2303.7
  2291.4
(29/2-)
(29/2-)
  2864.7 3   CD  (33/2+)      675.2 1 
   100
Q
  2189.5
(29/2+)
  2874.2 3   C   (33/2-)      582.8 1 
   100
(E2)
  2291.4
(29/2-)
  2931.6 4   C   (31/2+)      712.2 3 
   100
Q
  2219.4
(27/2+)
  2979.3 3   C   (31/2+)      249.9 3 
   439.6 5 
   759.9 5 
  <100
 
    19 6 


Q
  2729.4
  2539.7
  2219.4
(29/2+)
(27/2+)
(27/2+)
  3066.2 4   C   (33/2+)      876.7 3 
   100
Q
  2189.5
(29/2+)
  3201.0 3   C   (33/2+)      134.8 5 
   565.5 1 
 
   100

(E2)
  3066.2
  2635.5
(33/2+)
(29/2+)
  3292.4 3   C   (35/2-)       91.4 3 
   418.2 3 
   452.6 3 
   473.8 5 
   604.0 1 
   672.0 1 
    15 5 
    15 5 
    20 7 
 
    54 8 
   100 5 
D
D+Q
D+Q

Q
Q
  3201.0
  2874.2
  2839.8
  2818.6
  2688.4
  2620.4
(33/2+)
(33/2-)
(33/2-)

(31/2-)
(31/2-)
  3376.4 4   C   (37/2+)      511.7 3 
   100
(E2)
  2864.7
(33/2+)
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
  3420.1 3   C   (35/2+)      219.1 3 
   353.9 5 
   440.8 5 
   580.3 3 
   100 16 
    42 14 
 
    74 23 
D+Q


D
  3201.0
  3066.2
  2979.3
  2839.8
(33/2+)
(33/2+)
(31/2+)
(33/2-)
  3452.7 4   C   (37/2-)      612.9 3 
   100
Q
  2839.8
(33/2-)
  3455.4 3   C   (35/2+)      163.0 5 
   254.4 3 
   476.1 3 
   523.8 5 
    37 11 
    55 16 
   100 15 
    27 8 

D+Q

(E2)
  3292.4
  3201.0
  2979.3
  2931.6
(35/2-)
(33/2+)
(31/2+)
(31/2+)
  3574.1 4   C   (37/2-)      699.9 3 
   100
Q
  2874.2
(33/2-)
  3582.3 3   C   (37/2+)      381.3 1 
   717.6 3 
   100 16 
    41 13 
(E2)

  3201.0
  2864.7
(33/2+)
(33/2+)
  3640.7 3   C   (39/2+)       58.4S
   185.3 1 
   188.0 3 
   220.6 1 
 
   100 15 
    25 8 
    67 11 

(E2)
D
(E2)
  3582.3
  3455.4
  3452.7
  3420.1
(37/2+)
(35/2+)
(37/2-)
(35/2+)
  3648.7 3   C   (39/2-)      356.3 1 
   100
(E2)
  3292.4
(35/2-)
  3672.9 6   C        808.2 5 
 

  2864.7
(33/2+)
  3809.3 3   C   (41/2-)      160.6 1 
   100
D+Q
  3648.7
(39/2-)
  3848.6 3   C   (43/2+)      207.9 1 
   100
(E2)
  3640.7
(39/2+)
  3947.0 5   C   (41/2+)      570.6 3 
   100
(E2)
  3376.4
(37/2+)
  3976.0 6   C        393.7 5 
 

  3582.3
(37/2+)
  4168.6 6   C   (41/2-)      715.9 5 
   100
Q
  3452.7
(37/2-)
  4367.8 3   C   (47/2+)      519.2 1 
   100
(E2)
  3848.6
(43/2+)
  4437.2 3   C   (43/2-)      627.9 1 
   788.5 5 
   100 15 
    16 5 
D+Q
Q
  3809.3
  3648.7
(41/2-)
(39/2-)
  4647.4 7   C   (45/2+)      700.4 5 
   100
Q
  3947.0
(41/2+)
  4686.2 3   C   (45/2+)      318.4 3 
   837.6 1 
    19 6 
   100 15 

D+Q
  4367.8
  3848.6
(47/2+)
(43/2+)
  4688.1 3   C   (45/2-)      250.9 1 
   100
D+Q
  4437.2
(43/2-)
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
  4708.4 3   C   (47/2+)      340.6 3 
   859.8 1 
    49 8 
   100 16 

Q
  4367.8
  3848.6
(47/2+)
(43/2+)
  4795.3 3   C   (45/2-)      986.0 1 
   100
Q
  3809.3
(41/2-)
  4848.7 4   C   (45/2-)     1039.4 3 
   100
Q
  3809.3
(41/2-)
  4879.3 3   C   (49/2+)      170.9 3 
   193.1 1 
   511.5 3 
    41 13 
   100 16 
    58 9 
D+Q
(E2)
D+Q
  4708.4
  4686.2
  4367.8
(47/2+)
(45/2+)
(47/2+)
  5042.3 3   C   (49/2-)      193.6 5 
   247.0 3 
   333.9 3 
   354.2 3 
    23 7 
   100 15 
    90 14 
    98 15 
(E2)
(E2)
D
(E2)
  4848.7
  4795.3
  4708.4
  4688.1
(45/2-)
(45/2-)
(47/2+)
(45/2-)
  5353.7 3   C   (53/2+)      474.4 1 
   100
(E2)
  4879.3
(49/2+)
  5464.5 9   C   (49/2+)      817.1 5 
   100
Q
  4647.4
(45/2+)
  5502.1 4   C   (53/2-)      459.8 1 
   100
(E2)
  5042.3
(49/2-)
  6474.8 5   C   (57/2-)      972.7 3 
   100
Q
  5502.1
(53/2-)
  6476.5 4   C   (55/2+)     1122.8 1 
   100
D+Q
  5353.7
(53/2+)
  6761.9 7   C        287.1 5 
   100

  6474.8
(57/2-)
  6841.6 5   C   (57/2+)      365.1 3 
   100
D+Q
  6476.5
(55/2+)
  7272.3 7   C        430.7 5 
   100

  6841.6
(57/2+)
  7358.0 9   C        596.1 5 
 

  6761.9

  7582.5 7   C        740.9 5 
 

  6841.6
(57/2+)
  7764.8 9   C        492.5 5 
 

  7272.3

  8135.3 10   C        777.3 5 
 

  7358.0

  8843.1 11   C        707.8 5 
 

  8135.3

E(level): From least square fit to Eγ values

Jπ(level): Suggested values from 188Os(α,3nγ),191Ir(p,3nγ), up to 2865 keV, except where noted. These values are derived from γγ(θ), excitation functions, and Nilsson model assumptions. These are in general agreement with Jπ values suggested from multipolarity assignments and yrast arguments from (18O,5nγ), which were used for Jπ assignments beyond 2865 keV.

E(γ): From (18O,5nγ) (2009Hu12) except where noted

I(γ): From 176Yb(18O,5nγ) unless otherwise 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 - γ cascade based on (39/2+).
  3640.7 3  (39/2+)        
  3848.6 3  (43/2+)      207.9 1 
   100
(E2)
  3640.7
(39/2+)
  4367.8 3  (47/2+)      519.2 1 
   100
(E2)
  3848.6
(43/2+)
  4879.3 3  (49/2+)      170.9 3 
   193.1 1 
   511.5 3 
    41 13 
   100 16 
    58 9 
D+Q
(E2)
D+Q
  4708.4
  4686.2
  4367.8
(47/2+)
(45/2+)
(47/2+)
  5353.7 3  (53/2+)      474.4 1 
   100
(E2)
  4879.3
(49/2+)
  6476.5 4  (55/2+)     1122.8 1 
   100
D+Q
  5353.7
(53/2+)
  6841.6 5  (57/2+)      365.1 3 
   100
D+Q
  6476.5
(55/2+)
  7272.3 7       430.7 5 
   100

  6841.6
(57/2+)
  7764.8 9       492.5 5 
 

  7272.3

E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 2 - 13/2+ band, α=+1/2
   191.4 2  (13/2+) 143 µs 5 
% IT = 100
     
   499.2 2  (17/2+) 211.4 ps 55     307.8 1 
   100
E2
   191.4
(13/2+)
   955.0 2  (21/2+) 175.4 ps 49     455.8 1 
   100
(E2)
   499.2
(17/2+)
  1529.3 3  (25/2+)      574.3 1 
   100
(E2)
   955.0
(21/2+)
  2189.5 3  (29/2+)      660.2 1 
   100
Q
  1529.3
(25/2+)
  2864.7 3  (33/2+)      675.2 1 
   100
Q
  2189.5
(29/2+)
  3376.4 4  (37/2+)      511.7 3 
   100
(E2)
  2864.7
(33/2+)
  3947.0 5  (41/2+)      570.6 3 
   100
(E2)
  3376.4
(37/2+)
  4647.4 7  (45/2+)      700.4 5 
   100
Q
  3947.0
(41/2+)
  5464.5 9  (49/2+)        
E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 3 - 13/2+ band, α=-1/2
   531.3 3  (15/2+)        
   983.5 3  (19/2+)      452.2 1 
   484.3 3 
   100 15 
    51 8 
(E2)
D+Q
   531.3
   499.2
(15/2+)
(17/2+)
  1555.7 3  (23/2+)      572.2 3 
   600.7 5 
   100 16 
    22 7 
(E2)
D+Q
   983.5
   955.0
(19/2+)
(21/2+)
  2219.4 4  (27/2+)      663.7 3 
   100
Q
  1555.7
(23/2+)
  2931.6 4  (31/2+)      712.2 3 
   100
Q
  2219.4
(27/2+)
E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 4 - Band based on (17/2+).
   944.0 2  (17/2+)        
  1444.0 3  (21/2+)      460.5 3 
   500.0 1 
   944.8 5 
    30 10 
   100 16 
    10 4 
D+Q
(E2)
Q
   983.5
   944.0
   499.2
(19/2+)
(17/2+)
(17/2+)
  2009.5 3  (25/2+)      565.5 1 
  1054.5 5 
  <100
    14 5 

Q
  1444.0
   955.0
(21/2+)
(21/2+)
  2635.5 3  (29/2+)      626.0 1 
  1106.2 3 
   100 5 
    17 6 
Q
Q
  2009.5
  1529.3
(25/2+)
(25/2+)
  3201.0 3  (33/2+)      134.8 5 
   565.5 1 
 
   100

(E2)
  3066.2
  2635.5
(33/2+)
(29/2+)
  3582.3 3  (37/2+)      381.3 1 
   717.6 3 
   100 16 
    41 13 
(E2)

  3201.0
  2864.7
(33/2+)
(33/2+)
  3976.0 6       393.7 5 
 

  3582.3
(37/2+)
E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 5 - γ cascade based on (49/2-).
  5042.3 3  (49/2-)        
  5502.1 4  (53/2-)      459.8 1 
   100
(E2)
  5042.3
(49/2-)
  6474.8 5  (57/2-)      972.7 3 
   100
Q
  5502.1
(53/2-)
  6761.9 7       287.1 5 
   100

  6474.8
(57/2-)
  7358.0 9       596.1 5 
 

  6761.9

  8135.3 10       777.3 5 
 

  7358.0

  8843.1 11       707.8 5 
 

  8135.3

E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 6 - The g.s. band
     0.0 3/2- 10.87 h 12 
% ε = 100
     
     6.40 3  5/2-        6.40 4 S
   100
[M1]
     0.0
3/2-
   237.4 1  (9/2)-      231.0 1 
   100
E2
     6.40
5/2-
   608.6 2  (13/2-)      251.9 3 
   371.2 1 
    11 4 
   100 5 

(E2)
   356.72
   237.4
(9/2-)
(9/2)-
  1081.1 2  (17/2-)      472.4 1 
   100
(E2)
   608.6
(13/2-)
  1490.4 2  (19/2-)      128.9 1 
   409.3 1 
   536 1 
    35 6 
   100 5 
 
(E2)
(E2)

  1361.5
  1081.1
   955.0
(17/2-)
(17/2-)
(21/2+)
E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 7 - ΔJ=2 band based on (25/2-).
  1714.3 3  (25/2-)        
  2303.7 3  (29/2-)      248.5 3 
   589.4 1 
    22 4 
   100 6 
D+Q
(E2)
  2055.2
  1714.3
(27/2-)
(25/2-)
  2839.8 3  (33/2-)      536.1 1 
   548.4 3 
   100 15 
    46 8 
(E2)
(E2)
  2303.7
  2291.4
(29/2-)
(29/2-)
  3452.7 4  (37/2-)      612.9 3 
   100
Q
  2839.8
(33/2-)
  4168.6 6  (41/2-)      715.9 5 
   100
Q
  3452.7
(37/2-)
E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 8 - ΔJ=2 band based on (29/2-).
  2291.4 3  (29/2-)        
  2874.2 3  (33/2-)      582.8 1 
   100
(E2)
  2291.4
(29/2-)
  3574.1 4  (37/2-)      699.9 3 
   100
Q
  2874.2
(33/2-)

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Additional Gamma Data:















E(level)
(keV)
Jπ(level)T1/2(level)E(γ)
(keV)
MultipolarityMixing
Ratio
Conversion
Coefficient
Additional Data
     6.40 5/2-        6.40 4 [M1] 924α=924 22, α(M)=714 17, α(N)=177 5, α(O)=31.8 8, α(P)=2.13 5
    45.78 (1/2)-       39.47 3 E2 369α=369, α(L)=277 4, α(M)=71.2 11, α(N)=17.3 3, α(O)=2.67 4, α(P)=0.00221 4
(1/2)-       45.69 3 M1+E20.32 327α=27 3, α(L)=20.7 21, α(M)=5.1 6, α(N)=1.25 13, α(O)=0.205 20, α(P)=0.00575 12
    88.30 3/2-       42.75 5 M1+E20.14 218.7α=18.7 14, α(L)=14.3 11, α(M)=3.4 3, α(N)=0.84 7, α(O)=0.145 10, α(P)=0.00745 12
3/2-       82.2 5 M1+E20.21 211.6α=11.6 3, α(K)=9.17 22, α(L)=1.88 7, α(M)=0.443 18, α(N)=0.109 5, α(O)=0.0191 7, α(P)=0.00107 3
3/2-       88.41 3 M1+E20.21 29.43α=9.43, α(K)=7.49 12, α(L)=1.49 4, α(M)=0.350 11, α(N)=0.086 3, α(O)=0.0152 4, α(P)=0.000870 14
   172.79 9/2- 464 ns 25 
% IT = 100
   166.40 5 E2 0.684B(E2)(W.u.)=0.088 5, α=0.684, α(K)=0.267 4, α(L)=0.314 5, α(M)=0.0805 12, α(N)=0.0197 3, α(O)=0.00310 5, α(P)=2.53E-5 4
   191.4 (13/2+) 143 µs 5 
% IT = 100
    18.7 9 [M2] 3.8×104B(M2)(W.u.)=0.08 3, α=3.8×104 10, α(L)=2.77×10+4 73, α(M)=7.6E+3 21, α(N)=1.92E+3 52, α(O)=3.28E+2 88, α(P)=15.8 42
   222.30 (3/2,5/2)-      134.26 4 M1+E20.8 32.3α=2.3 3, α(K)=1.6 4, α(L)=0.56 8, α(M)=0.137 23, α(N)=0.034 6, α(O)=0.0056 8, α(P)=0.00018 5
(3/2,5/2)-      215.68 5 M1+E20.9 40.54α=0.54 12, α(K)=0.41 12, α(L)=0.1032 15, α(M)=0.0249 8, α(N)=0.00614 18, α(O)=0.001046 16, α(P)=4.5×10-5 15
(3/2,5/2)-      221.95 16 E2 0.253α=0.253, α(K)=0.1306 19, α(L)=0.0926 14, α(M)=0.0235 4, α(N)=0.00575 9, α(O)=0.000921 14, α(P)=1.263×10-5 18
   237.4 (9/2)-      231.0 1 E2 0.222α=0.222, α(K)=0.1180 17, α(L)=0.0786 11, α(M)=0.0200 3, α(N)=0.00488 7, α(O)=0.000783 11, α(P)=1.147×10-5 17
   348.45 (5/2,3/2)-      110.8 5 (E2) 3.22α=3.22 8, α(K)=0.622 10, α(L)=1.95 5, α(M)=0.505 13, α(N)=0.123 4, α(O)=0.0192 5, α(P)=6.75×10-5 12
(5/2,3/2)-      126.31 5 M1+E20.54 93.08α=3.08 10, α(K)=2.29 14, α(L)=0.60 4, α(M)=0.146 10, α(N)=0.0359 25, α(O)=0.0061 4, α(P)=0.000261 17
(5/2,3/2)-      259.68 10 M1+E21.4 +8-40.25α=0.25 5, α(K)=0.184 48, α(L)=0.0533 22, α(M)=0.0130 4, α(N)=0.00320 9, α(O)=0.000538 25, α(P)=2.01×10-5 57
(5/2,3/2)-      348.15 15 M1(+E2)0.7 LT0.181α=0.181 24, α(K)=0.148 21, α(L)=0.0256 19, α(M)=0.0060 4, α(N)=0.00147 10, α(O)=0.000262 20, α(P)=1.67×10-5 25
   447.67 (3/2,5/2)-      225.7 5 M1(+E2)0.8 LT0.58α=0.58 9, α(K)=0.47 9, α(L)=0.0895 16, α(M)=0.0211 4, α(N)=0.00520 9, α(O)=0.000915 20, α(P)=5.3×10-5 10
(3/2,5/2)-      441.04 14 M1+E21.3 +20-60.062α=0.062 23, α(K)=0.049 20, α(L)=0.0100 22, α(M)=0.0024 5, α(N)=0.00058 12, α(O)=0.000102 23, α(P)=5.3×10-6 23
(3/2,5/2)-      447.77 9 M1(+E2)0.7 LT0.092α=0.092 12, α(K)=0.076 11, α(L)=0.0128 12, α(M)=0.0030 3, α(N)=0.00073 7, α(O)=0.000131 12, α(P)=8.5×10-6 12
   493.3 11/2-      321.1 5 M1+E2-16.2 +17-210.0817α=0.0817, α(K)=0.0525 8, α(L)=0.0222 4, α(M)=0.00553 9, α(N)=0.001356 20, α(O)=0.000222 4, α(P)=5.34×10-6 8
   499.2 (17/2+) 211.4 ps 55     307.8 1 E2 0.0913B(E2)(W.u.)=13.8 4, α=0.0913, α(K)=0.0573 8, α(L)=0.0257 4, α(M)=0.00643 9, α(N)=0.001575 23, α(O)=0.000257 4, α(P)=5.79E-6 9
   529.62 (1/2,3/2,5/2)-      529.59 11 M1(+E2)1.4 LT0.052α=0.052 15, α(K)=0.042 13, α(L)=0.0073 16, α(M)=0.0017 4, α(N)=0.00042 9, α(O)=7.5×10-5 17, α(P)=4.7E-6 15
   608.6 (13/2-)      371.2 1 (E2) 0.0536α=0.0536, α(K)=0.0363 5, α(L)=0.01308 19, α(M)=0.00324 5, α(N)=0.000794 12, α(O)=0.0001313 19, α(P)=3.75×10-6 6
   712.0 (13/2-)      539.5 3 (E2) 0.0206α=0.0206, α(K)=0.01546 22, α(L)=0.00393 6, α(M)=0.000950 14, α(N)=0.000234 4, α(O)=3.97×10-5 6, α(P)=1.632E-6 23
   944.0 (17/2+)      444.8 5 (E2) 0.0332α=0.0332, α(K)=0.0238 4, α(L)=0.00714 10, α(M)=0.001746 25, α(N)=0.000429 6, α(O)=7.18×10-5 10, α(P)=2.49E-6 4
E(level)
(keV)
Jπ(level)T1/2(level)E(γ)
(keV)
MultipolarityMixing
Ratio
Conversion
Coefficient
Additional Data
   955.0 (21/2+) 175.4 ps 49     455.8 1 (E2) 0.0312B(E2)(W.u.)=2.47 7, α=0.0312, α(K)=0.0225 4, α(L)=0.00660 10, α(M)=0.001612 23, α(N)=0.000396 6, α(O)=6.65E-5 10, α(P)=2.36E-6 4
   983.5 (19/2+)      452.2 1 (E2) 0.0318α=0.0318, α(K)=0.0229 4, α(L)=0.00677 10, α(M)=0.001654 24, α(N)=0.000406 6, α(O)=6.82×10-5 10, α(P)=2.40E-6 4
  1081.1 (17/2-)      472.4 1 (E2) α(K)=0.0207 3, α(L)=0.00589 9, α(M)=0.001436 21, α(N)=0.000353 5, α(O)=5.94×10-5 9, α(P)=2.18E-6 3
  1160.87 (3/2+)      631.2 9 E1 0.00511α=0.00511, α(K)=0.00427 6, α(L)=0.000646 10, α(M)=0.0001477 22, α(N)=3.64×10-5 6, α(O)=6.46E-6 10, α(P)=4.12E-7 6
(3/2+)      713.24 17 E1 0.00401α=0.00401, α(K)=0.00335 5, α(L)=0.000503 7, α(M)=0.0001149 17, α(N)=2.83×10-5 4, α(O)=5.04E-6 7, α(P)=3.25E-7 5
(3/2+)      812.8 3 E1 0.00311α=0.00311, α(K)=0.00261 4, α(L)=0.000388 6, α(M)=8.86×10-5 13, α(N)=2.18E-5 3, α(O)=3.90E-6 6, α(P)=2.55E-7 4
(3/2+)     1071.5 6 E1 0.00187α=0.00187, α(K)=0.001572 22, α(L)=0.000230 4, α(M)=5.24×10-5 8, α(N)=1.290E-5 19, α(O)=2.31E-6 4, α(P)=1.546E-7 22
(3/2+)     1160.6 3 E1 1.63×10-3α=1.63×10-3, α(K)=0.001364 20, α(L)=0.000199 3, α(M)=4.52E-5 7, α(N)=1.115E-5 16, α(O)=2.00E-6 3, α(P)=1.344E-7 19
  1185.31 (19/2+)      531.5 1 (E2) 0.0214α=0.0214, α(K)=0.01597 23, α(L)=0.00411 6, α(M)=0.000994 14, α(N)=0.000244 4, α(O)=4.15×10-5 6, α(P)=1.685E-6 24
  1361.5 (17/2-)      280.4 3 (E2) 0.1207α=0.1207, α(K)=0.0723 11, α(L)=0.0366 6, α(M)=0.00919 14, α(N)=0.00225 4, α(O)=0.000365 6, α(P)=7.22×10-6 11
  1444.0 (21/2+)      500.0 1 (E2) 0.0248α=0.0248, α(K)=0.0183 3, α(L)=0.00494 7, α(M)=0.001200 17, α(N)=0.000295 5, α(O)=4.98×10-5 7, α(P)=1.92E-6 3
  1490.4 (19/2-)      128.9 1 (E2) 1.77α=1.77, α(K)=0.473 7, α(L)=0.977 15, α(M)=0.252 4, α(N)=0.0615 9, α(O)=0.00963 14, α(P)=4.68×10-5 7
(19/2-)      409.3 1 (E2) 0.0412α=0.0412, α(K)=0.0288 4, α(L)=0.00938 14, α(M)=0.00231 4, α(N)=0.000566 8, α(O)=9.43×10-5 14, α(P)=3.00E-6 5
  1512.1 (21/2-)      150.6 3 (E2) 0.985α=0.985 16, α(K)=0.338 5, α(L)=0.486 8, α(M)=0.1251 21, α(N)=0.0305 5, α(O)=0.00480 8, α(P)=3.22×10-5 5
  1529.3 (25/2+)      574.3 1 (E2) 0.01780α=0.01780, α(K)=0.01351 19, α(L)=0.00328 5, α(M)=0.000789 11, α(N)=0.000194 3, α(O)=3.31×10-5 5, α(P)=1.428E-6 20
  1555.7 (23/2+)      572.2 3 (E2) 0.0180α=0.0180, α(K)=0.01362 20, α(L)=0.00331 5, α(M)=0.000797 12, α(N)=0.000196 3, α(O)=3.35×10-5 5, α(P)=1.440E-6 21
  1714.3 (25/2-)      202.2 1 (E2) 0.346α=0.346, α(K)=0.1653 24, α(L)=0.1362 20, α(M)=0.0347 5, α(N)=0.00849 12, α(O)=0.001353 20, α(P)=1.581×10-5 23
  2291.4 (29/2-)      577.1 1 (E2) 0.01760α=0.01760, α(K)=0.01337 19, α(L)=0.00323 5, α(M)=0.000778 11, α(N)=0.000191 3, α(O)=3.27×10-5 5, α(P)=1.414E-6 20
  2303.7 (29/2-)      589.4 1 (E2) 0.01677α=0.01677, α(K)=0.01278 18, α(L)=0.00304 5, α(M)=0.000731 11, α(N)=0.000180 3, α(O)=3.08×10-5 5, α(P)=1.352E-6 19
  2620.4 (31/2-)      565.2 1 (E2) 0.0185α=0.0185, α(K)=0.01398 20, α(L)=0.00343 5, α(M)=0.000827 12, α(N)=0.000203 3, α(O)=3.47×10-5 5, α(P)=1.478E-6 21
  2729.4 (29/2+)      539.9 3 (E2) 0.0206α=0.0206, α(K)=0.01543 22, α(L)=0.00392 6, α(M)=0.000948 14, α(N)=0.000233 4, α(O)=3.96×10-5 6, α(P)=1.629E-6 23
  2839.8 (33/2-)      536.1 1 (E2) 0.0209α=0.0209, α(K)=0.01567 22, α(L)=0.00401 6, α(M)=0.000968 14, α(N)=0.000238 4, α(O)=4.04×10-5 6, α(P)=1.654E-6 24
(33/2-)      548.4 3 (E2) 0.0198α=0.0198, α(K)=0.01492 21, α(L)=0.00375 6, α(M)=0.000904 13, α(N)=0.000222 4, α(O)=3.78×10-5 6, α(P)=1.576E-6 23
  2874.2 (33/2-)      582.8 1 (E2) 0.01721α=0.01721, α(K)=0.01309 19, α(L)=0.00314 5, α(M)=0.000756 11, α(N)=0.000186 3, α(O)=3.18×10-5 5, α(P)=1.385E-6 20
  3201.0 (33/2+)      565.5 1 (E2) 0.0185α=0.0185, α(K)=0.01396 20, α(L)=0.00343 5, α(M)=0.000825 12, α(N)=0.000203 3, α(O)=3.46×10-5 5, α(P)=1.476E-6 21
E(level)
(keV)
Jπ(level)T1/2(level)E(γ)
(keV)
MultipolarityMixing
Ratio
Conversion
Coefficient
Additional Data
  3376.4 (37/2+)      511.7 3 (E2) 0.0234α=0.0234, α(K)=0.01736 25, α(L)=0.00460 7, α(M)=0.001117 16, α(N)=0.000275 4, α(O)=4.65×10-5 7, α(P)=1.83E-6 3
  3455.4 (35/2+)      523.8 5 (E2) 0.0221α=0.0221, α(K)=0.01649 24, α(L)=0.00429 7, α(M)=0.001039 15, α(N)=0.000255 4, α(O)=4.33×10-5 7, α(P)=1.739E-6 25
  3582.3 (37/2+)      381.3 1 (E2) 0.0498α=0.0498, α(K)=0.0341 5, α(L)=0.01192 17, α(M)=0.00295 5, α(N)=0.000723 11, α(O)=0.0001197 17, α(P)=3.52×10-6 5
  3640.7 (39/2+)      185.3 1 (E2) 0.467α=0.467, α(K)=0.206 3, α(L)=0.197 3, α(M)=0.0504 8, α(N)=0.01232 18, α(O)=0.00195 3, α(P)=1.95×10-5 3
(39/2+)      220.6 1 (E2) 0.259α=0.259, α(K)=0.1326 19, α(L)=0.0949 14, α(M)=0.0241 4, α(N)=0.00590 9, α(O)=0.000944 14, α(P)=1.282×10-5 18
  3648.7 (39/2-)      356.3 1 (E2) 0.0600α=0.0600, α(K)=0.0401 6, α(L)=0.01510 22, α(M)=0.00375 6, α(N)=0.000919 13, α(O)=0.0001515 22, α(P)=4.12×10-6 6
  3848.6 (43/2+)      207.9 1 (E2) 0.315α=0.315, α(K)=0.1541 22, α(L)=0.1213 18, α(M)=0.0309 5, α(N)=0.00756 11, α(O)=0.001205 17, α(P)=1.478×10-5 21
  3947.0 (41/2+)      570.6 3 (E2) 0.0181α=0.0181, α(K)=0.01370 20, α(L)=0.00334 5, α(M)=0.000804 12, α(N)=0.000198 3, α(O)=3.37×10-5 5, α(P)=1.448E-6 21
  4367.8 (47/2+)      519.2 1 (E2) 0.0226α=0.0226, α(K)=0.01681 24, α(L)=0.00441 7, α(M)=0.001068 15, α(N)=0.000262 4, α(O)=4.45×10-5 7, α(P)=1.772E-6 25
  4879.3 (49/2+)      193.1 1 (E2) 0.405α=0.405, α(K)=0.185 3, α(L)=0.1654 24, α(M)=0.0423 6, α(N)=0.01033 15, α(O)=0.001641 24, α(P)=1.767×10-5 25
  5042.3 (49/2-)      193.6 5 (E2) 0.402α=0.402 7, α(K)=0.184 3, α(L)=0.164 3, α(M)=0.0418 8, α(N)=0.01021 19, α(O)=0.00162 3, α(P)=1.76×10-5 3
(49/2-)      247.0 3 (E2) 0.179α=0.179, α(K)=0.0996 15, α(L)=0.0601 9, α(M)=0.01520 23, α(N)=0.00372 6, α(O)=0.000598 9, α(P)=9.77×10-6 14
(49/2-)      354.2 3 (E2) 0.0610α=0.0610, α(K)=0.0406 6, α(L)=0.01542 22, α(M)=0.00383 6, α(N)=0.000939 14, α(O)=0.0001547 23, α(P)=4.17×10-6 6
  5353.7 (53/2+)      474.4 1 (E2) 0.0282α=0.0282, α(K)=0.0205 3, α(L)=0.00581 9, α(M)=0.001417 20, α(N)=0.000348 5, α(O)=5.86×10-5 9, α(P)=2.16E-6 3
  5502.1 (53/2-)      459.8 1 (E2) 0.0305α=0.0305, α(K)=0.0220 3, α(L)=0.00642 9, α(M)=0.001567 22, α(N)=0.000385 6, α(O)=6.46×10-5 9, α(P)=2.31E-6 4

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Additional Level Data and Comments:

E(level)Jπ(level)T1/2(level)Comments
     0.03/2- 10.87 h 12 
% ε = 100
μ=-0.422 7 (1989Du01,2000SaZZ,2014StZZ), Q=-0.95 4 (1992Hi07,1989Du01,2016St14)
RMS charge radius <r2>1/2=5.4060 fm 35 (2013An02 evaluation).
E(level): The g.s. band.
     6.405/2-   E(level): Transition unobserved. Energy from energy level differences. The g.s. band.
Jπ(level): The 6.4 level is populated by an M1+E2 γ from the 88.4 level which is 1/2-,3/2- from L=1 in (p,d). The 172.8 and 493 levels are populated with low log ft (≈5) from 189Au ε decay (4.59 min) indicating Jπ=9/2-,11/2-,13/2-. An E2 γ from 172.6 to 6.2 thus establishes Jπ(6.2)=5/2-, Jπ(88.4)=3/2-, and Jπ(172.6)=9/2-. From γ(θ) on oriented nuclei the 493 level is uniquely determined as 11/2-.
    88.303/2-   E(level): Transition unobserved. Energy from energy level differences.
Jπ(level): The 6.4 level is populated by an M1+E2 γ from the 88.4 level which is 1/2-,3/2- from L=1 in (p,d). The 172.8 and 493 levels are populated with low log ft (≈5) from 189Au ε decay (4.59 min) indicating Jπ=9/2-,11/2-,13/2-. An E2 γ from 172.6 to 6.2 thus establishes Jπ(6.2)=5/2-, Jπ(88.4)=3/2-, and Jπ(172.6)=9/2-. From γ(θ) on oriented nuclei the 493 level is uniquely determined as 11/2-.
   172.799/2- 464 ns 25 
% IT = 100
E(level): Transition unobserved. Energy from energy level differences.
Jπ(level): The 6.4 level is populated by an M1+E2 γ from the 88.4 level which is 1/2-,3/2- from L=1 in (p,d). The 172.8 and 493 levels are populated with low log ft (≈5) from 189Au ε decay (4.59 min) indicating Jπ=9/2-,11/2-,13/2-. An E2 γ from 172.6 to 6.2 thus establishes Jπ(6.2)=5/2-, Jπ(88.4)=3/2-, and Jπ(172.6)=9/2-. From γ(θ) on oriented nuclei the 493 level is uniquely determined as 11/2-.
   191.4(13/2+) 143 µs 5 
% IT = 100
E(level): From 189Au ε decay (28.7 min). 13/2+ band, α=+1/2.
   237.4(9/2)-   E(level): The g.s. band.
   348.45(5/2,3/2)-   XREF: E(340).
   493.311/2-   E(level): Transition unobserved. Energy from energy level differences.
Jπ(level): The 6.4 level is populated by an M1+E2 γ from the 88.4 level which is 1/2-,3/2- from L=1 in (p,d). The 172.8 and 493 levels are populated with low log ft (≈5) from 189Au ε decay (4.59 min) indicating Jπ=9/2-,11/2-,13/2-. An E2 γ from 172.6 to 6.2 thus establishes Jπ(6.2)=5/2-, Jπ(88.4)=3/2-, and Jπ(172.6)=9/2-. From γ(θ) on oriented nuclei the 493 level is uniquely determined as 11/2-.
   499.2(17/2+) 211.4 ps 55  Q(transition)=11.05 29 (2013He25).
E(level): From 189Au ε decay (28.7 min). 13/2+ band, α=+1/2.
T1/2(level): From 176Yb(18O,5nγ), using the recoil-distance method (2013He25).
   531.3(15/2+)   E(level): 13/2+ band, α=-1/2.
   608.6(13/2-)   E(level): The g.s. band.
   944.0(17/2+)   E(level): From 189Au ε decay (4.59 min). Band based on (17/2+).
   955.0(21/2+) 175.4 ps 49  Q(transition)=2.49 7 (2013He25).
E(level): From 189Au ε decay (28.7 min). 13/2+ band, α=+1/2.
T1/2(level): From 176Yb(18O,5nγ), using the recoil-distance method (2013He25).
   983.5(19/2+)   E(level): 13/2+ band, α=-1/2.
  1081.1(17/2-)   E(level): The g.s. band.
  1444.0(21/2+)   E(level): From 189Au ε decay (4.59 min). Band based on (17/2+).
  1490.4(19/2-)   E(level): The g.s. band.
  1529.3(25/2+)   E(level): From 189Au ε decay (28.7 min). 13/2+ band, α=+1/2.
  1555.7(23/2+)   E(level): 13/2+ band, α=-1/2.
  1714.3(25/2-)   E(level): ΔJ=2 band based on (25/2-).
  2009.5(25/2+)   E(level): From 189Au ε decay (4.59 min). Band based on (17/2+).
  2189.5(29/2+)   E(level): From 189Au ε decay (28.7 min). 13/2+ band, α=+1/2.
  2219.4(27/2+)   E(level): 13/2+ band, α=-1/2.
  2291.4(29/2-)   E(level): ΔJ=2 band based on (29/2-).
  2303.7(29/2-)   E(level): ΔJ=2 band based on (25/2-).
E(level)Jπ(level)T1/2(level)Comments
  2635.5(29/2+)   E(level): From 189Au ε decay (4.59 min). Band based on (17/2+).
  2839.8(33/2-)   E(level): ΔJ=2 band based on (25/2-).
  2864.7(33/2+)   E(level): From 189Au ε decay (28.7 min). 13/2+ band, α=+1/2.
  2874.2(33/2-)   E(level): ΔJ=2 band based on (29/2-).
  2931.6(31/2+)   E(level): 13/2+ band, α=-1/2.
  3201.0(33/2+)   E(level): From 189Au ε decay (4.59 min). Band based on (17/2+).
  3376.4(37/2+)   E(level): From 189Au ε decay (28.7 min). 13/2+ band, α=+1/2.
  3452.7(37/2-)   E(level): ΔJ=2 band based on (25/2-).
  3574.1(37/2-)   E(level): ΔJ=2 band based on (29/2-).
  3582.3(37/2+)   E(level): From 189Au ε decay (4.59 min). Band based on (17/2+).
  3640.7(39/2+)   E(level): γ cascade based on (39/2+).
  3848.6(43/2+)   E(level): γ cascade based on (39/2+).
  3947.0(41/2+)   E(level): From 189Au ε decay (28.7 min). 13/2+ band, α=+1/2.
  3976.0   E(level): From 189Au ε decay (4.59 min). Band based on (17/2+).
  4168.6(41/2-)   E(level): ΔJ=2 band based on (25/2-).
  4367.8(47/2+)   E(level): γ cascade based on (39/2+).
  4647.4(45/2+)   E(level): From 189Au ε decay (28.7 min). 13/2+ band, α=+1/2.
  4879.3(49/2+)   E(level): γ cascade based on (39/2+).
  5042.3(49/2-)   E(level): γ cascade based on (49/2-).
  5353.7(53/2+)   E(level): γ cascade based on (39/2+).
  5464.5(49/2+)   E(level): From 189Au ε decay (28.7 min). 13/2+ band, α=+1/2.
  5502.1(53/2-)   E(level): γ cascade based on (49/2-).
  6474.8(57/2-)   E(level): γ cascade based on (49/2-).
  6476.5(55/2+)   E(level): γ cascade based on (39/2+).
  6761.9   E(level): γ cascade based on (49/2-).
E(level)Jπ(level)T1/2(level)Comments
  6841.6(57/2+)   E(level): γ cascade based on (39/2+).
  7272.3   E(level): γ cascade based on (39/2+).
  7358.0   E(level): γ cascade based on (49/2-).
  7764.8   E(level): γ cascade based on (39/2+).
  8135.3   E(level): γ cascade based on (49/2-).
  8843.1   E(level): γ cascade based on (49/2-).

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Additional Gamma Comments:

E(level)E(gamma)Comments
     6.40     6.40E(γ): Transition unobserved. Energy from energy level differences
    45.78    39.47E(γ): From 189Au ε decay (28.7 min)
I(γ): From 189Au ε decay (28.7 min)
M(γ): From Ice data in 189Au ε decay (28.7 min) and 189Au ε decay (4.59 min).
    45.69E(γ): From 189Au ε decay (28.7 min)
I(γ): From 189Au ε decay (28.7 min)
M(γ): From Ice data in 189Au ε decay (28.7 min) and 189Au ε decay (4.59 min).
    88.30    42.75E(γ): From 189Au ε decay (28.7 min)
M(γ): From Ice data in 189Au ε decay (28.7 min) and 189Au ε decay (4.59 min).
    82.2E(γ): From 189Au ε decay (28.7 min)
M(γ): From Ice data in 189Au ε decay (28.7 min) and 189Au ε decay (4.59 min).
    88.41E(γ): From 189Au ε decay (28.7 min)
M(γ): From Ice data in 189Au ε decay (28.7 min) and 189Au ε decay (4.59 min).
   172.79   166.40E(γ): Using the higher precision value from 4.59 min ε decay
M(γ): From Ice data in 189Au ε decay (28.7 min) and 189Au ε decay (4.59 min).
   191.4    18.7E(γ): Transition unobserved. Energy from energy level differences
   202.2    11.3E(γ): Transition unobserved. Energy from energy level differences
   222.30   134.26E(γ): From 189Au ε decay (28.7 min)
I(γ): From 189Au ε decay (28.7 min)
M(γ): From Ice data in 189Au ε decay (28.7 min) and 189Au ε decay (4.59 min).
   176.1E(γ): From 189Au ε decay (28.7 min)
   215.68E(γ): From 189Au ε decay (28.7 min)
I(γ): From 189Au ε decay (28.7 min)
M(γ): From Ice data in 189Au ε decay (28.7 min) and 189Au ε decay (4.59 min).
   221.95E(γ): From 189Au ε decay (28.7 min)
M(γ): From Ice data in 189Au ε decay (28.7 min) and 189Au ε decay (4.59 min).
   237.4   231.0E(γ): Weighted average from (18O,4nγ) and 28.7 min ε decay.
M(γ): From Ice data in 189Au ε decay (28.7 min) and 189Au ε decay (4.59 min).
   348.45   110.8E(γ): From 189Au ε decay (28.7 min)
I(γ): From 189Au ε decay (28.7 min)
M(γ): From Ice data in 189Au ε decay (28.7 min) and 189Au ε decay (4.59 min).
   126.31I(γ): From 189Au ε decay (28.7 min)
M(γ): From Ice data in 189Au ε decay (28.7 min) and 189Au ε decay (4.59 min).
   259.68E(γ): From 189Au ε decay (28.7 min)
I(γ): From 189Au ε decay (28.7 min)
M(γ): From Ice data in 189Au ε decay (28.7 min) and 189Au ε decay (4.59 min).
   302.4E(γ): From 189Au ε decay (28.7 min)
   342.0E(γ): From 189Au ε decay (28.7 min)
I(γ): From 189Au ε decay (28.7 min)
   348.15E(γ): From 189Au ε decay (28.7 min)
M(γ): From Ice data in 189Au ε decay (28.7 min) and 189Au ε decay (4.59 min).
   447.67   225.7E(γ): From 189Au ε decay (28.7 min)
I(γ): From 189Au ε decay (28.7 min)
M(γ): From Ice data in 189Au ε decay (28.7 min) and 189Au ε decay (4.59 min).
   359.4E(γ): From 189Au ε decay (28.7 min)
   441.04E(γ): From 189Au ε decay (28.7 min)
I(γ): From 189Au ε decay (28.7 min)
M(γ): From Ice data in 189Au ε decay (28.7 min) and 189Au ε decay (4.59 min).
   447.77E(γ): From 189Au ε decay (28.7 min)
I(γ): From 189Au ε decay (28.7 min)
M(γ): From Ice data in 189Au ε decay (28.7 min) and 189Au ε decay (4.59 min).
   493.3   321.1E(γ): From 189Au ε decay (4.59 min)
E(level)E(gamma)Comments
   499.2   307.8M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
   529.62   484.2E(γ): From 189Au ε decay (28.7 min)
I(γ): From 189Au ε decay (28.7 min)
   523.4E(γ): From 189Au ε decay (28.7 min)
I(γ): From 189Au ε decay (28.7 min)
   529.59E(γ): From 189Au ε decay (28.7 min)
I(γ): From 189Au ε decay (28.7 min)
M(γ): From Ice data in 189Au ε decay (28.7 min) and 189Au ε decay (4.59 min).
   531.3   329.2E(γ): Only in (α,3nγ)
   339.9M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
   608.6   371.2M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
   653.8   462.4M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
   712.0   539.5M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
   944.0   412.7M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
   444.8M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
   955.0   455.8M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
   983.5   452.2M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
   484.3M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  1081.1   472.4M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  1160.87   631.2E(γ): From 189Au ε decay (28.7 min)
I(γ): From 189Au ε decay (28.7 min)
M(γ): From Ice data in 189Au ε decay (28.7 min) and 189Au ε decay (4.59 min).
   713.24E(γ): From 189Au ε decay (28.7 min)
I(γ): From 189Au ε decay (28.7 min)
M(γ): From Ice data in 189Au ε decay (28.7 min) and 189Au ε decay (4.59 min).
   812.8E(γ): From 189Au ε decay (28.7 min)
I(γ): From 189Au ε decay (28.7 min)
M(γ): From Ice data in 189Au ε decay (28.7 min) and 189Au ε decay (4.59 min).
  1071.5E(γ): From 189Au ε decay (28.7 min)
I(γ): From 189Au ε decay (28.7 min)
M(γ): From Ice data in 189Au ε decay (28.7 min) and 189Au ε decay (4.59 min).
  1160.6E(γ): From 189Au ε decay (28.7 min)
I(γ): From 189Au ε decay (28.7 min)
M(γ): From Ice data in 189Au ε decay (28.7 min) and 189Au ε decay (4.59 min).
  1185.31   531.5M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
   686.1M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  1361.5   280.4M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
   649.5M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
   862.3M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
E(level)E(gamma)Comments
  1444.0   460.5M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
   500.0M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
   944.8M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  1490.4   128.9M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
   409.3M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
   536E(γ): only in (α,3nγ). Uncertainty assumed by evaluators.
  1512.1   150.6M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
   326.8M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  1529.3   574.3M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  1555.7   572.2M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
   600.7M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  1695.7   183.6M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  1714.3    18.6E(γ): in (α,3nγ) and the previous evaluation, this γ was placed from a 1530 keV level with (23/2-). In (18O,5nγ), coincidence relations found the 740.7 feeding the 945 keV level. This matches the 184 γ feeding the 1512 keV level followed by the 557 γ populating the 954 keV level. The 18.6 keV and and 184 γ’s match and are parallel to the 202 γ feeding the 1512 keV level but with the order of the 18.6 and 184 γ rays now reversed. See 2009Hu12 for further discussion.. Transition unobserved. Energy from energy level differences
   202.2M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  2009.5   565.5E(γ): Multiply placed with intensity suitably divided
I(γ): Multiply placed with intensity suitably divided
  1054.5M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  2055.2   340.9M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  2189.5   660.2M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  2219.4   663.7M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  2291.4   236.2M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
   577.1M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  2303.7   248.5M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
   589.4M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  2539.7  1010.4M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  2620.4   316.7M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
   329.0M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
   565.2M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
E(level)E(gamma)Comments
  2635.5   626.0M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  1106.2M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  2688.4   397.0E(γ): Observed only in 176Yb(18O,5nγ)
M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
   633.2M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  2729.4   539.9E(γ): Multiply placed with intensity suitably divided
I(γ): Multiply placed with intensity suitably divided
M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  1200.1M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  2839.8   536.1M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
   548.4M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  2864.7   675.2M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  2874.2   582.8M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  2931.6   712.2M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  2979.3   759.9M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  3066.2   876.7M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  3201.0   565.5E(γ): Multiply placed with intensity suitably divided
I(γ): Multiply placed with intensity suitably divided
M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  3292.4    91.4M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
   418.2M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
   452.6M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
   604.0M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
   672.0M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  3376.4   511.7M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  3420.1   219.1M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
   580.3M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  3452.7   612.9M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  3455.4   254.4M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
   523.8M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
E(level)E(gamma)Comments
  3574.1   699.9M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  3582.3   381.3M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  3640.7   185.3M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
   188.0M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
   220.6M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  3648.7   356.3M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  3809.3   160.6M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  3848.6   207.9M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  3947.0   570.6M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  4168.6   715.9M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  4367.8   519.2M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  4437.2   627.9M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
   788.5M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  4647.4   700.4M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  4686.2   837.6M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  4688.1   250.9M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  4708.4   859.8M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  4795.3   986.0M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  4848.7  1039.4M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  4879.3   170.9M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
   193.1M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
   511.5M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  5042.3   193.6M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
   247.0M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
   333.9M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
   354.2M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
E(level)E(gamma)Comments
  5353.7   474.4M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  5464.5   817.1M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  5502.1   459.8M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  6474.8   972.7M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  6476.5  1122.8M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.
  6841.6   365.1M(γ): From directional correlation of oriented nuclei (DCO) ratios from (18O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1+E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1.

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