ADOPTED LEVELS, GAMMAS for 93Nb

Author: Coral M. Baglin |  Citation: Nucl. Data Sheets 112, 1163 (2011) |  Cutoff date: 15-Dec-2010 

 Full ENSDF file | Adopted Levels (PDF version) 


Q(β-)=-406.7 keV 20S(n)= 8830.6 keV 21S(p)= 6042.3 keV 16Q(α)= -1928.8 keV 23
Reference: 2012WA38

References:
  A  93Mo ε decay (6.85 H)  B  92Zr(α,t)
  C  93Nb(p,p’)  D  Coulomb Excitation
  E  93Nb(n,n’γ)  F  93Nb(γ,γ’) E=6465 KEV
  G  92Zr(3He,d)  H  94Mo(d,3He)
  I  91Zr(α,d)  J  90Zr(α,pγ)
  K  92Zr(p,p’), (pol p,p) IAR  L  96Mo(p,α)
  M  80Se(16O,p2nγ)  N  93Nb(d,d’), (pol d,d)
  O  93Nb(γ,XN)  P  93Zr β- decay
  Q  93Nb(E,E’)  R  93Mo ε decay (4.0×103 Y)
  S  93Nb IT decay (16.12 Y)  T  92Zr(p,α) IAR
  U  89Y(α,nγ)  V  92Zr(16O,15N)
  W  93Nb(γ,γ’): E<2.75 MeV  X  94Zr(p,2nγ)
  Y  82Se(16O,p4nγ) 

General Comments:

Other Reactions:

173Yb(24Mg,Fγ), E=134.5 MeV (2010Fo10): observed 950γ following fission of 197Pb compound nucleus.

89Y(α,α) (2009Ki16): Eα=16.21 and 19.47 MeV; measured σ(θ) in 1|’ to 2|’ steps from θ(lab)=20|’ to 170|’; deduced local optical model parameters; predicted (89Y~#α) α cluster states in 93Nb and calculated E2 reduced transition strengths within a Kπ=1/2- band based on the 31 level.

93Nb(t,t) (2007Ch20):

E(t)=12 MeV; measured σ(θ); deduced optical-model parameters.

93Nb(n,n’) (1996De01, 1994De41):

E(n)=14.1 MeV. Analyzed σ(E,θ) data of Takahashi et al. (OKTAVIAN report A-92-01); calculated contributions from multistep direct, compound nucleus, multistep compound nucleus mechanisms, and collective excitations.

93Nb(α,α’) (1960Cr05):

Eα≈30 MeV, θ(c.m.)≈45|’-85|’; observed g.s. and E(level)=2400 300 (possibly complex); measured σ(θ).

Q-value: Note: Current evaluation has used the following Q record

Q-value: Q(β-), S(n), S(p), Q(α): from 2009AuZZ (cf. 405 4, 8831.3 20, 6043.4 16, -1931.4 23, respectively, from 2003Au03).










E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
       0.0ABCDEFGHIJ LMN PQRS   WXY 9/2+ STABLE      
      30.77 2     E GH J L   P RS    X  1/2- 16.12 y 12 
% IT = 100
    30.77 2 
  100
M4
       0.0
9/2+
     686.79 10  B  E GH J L           X  3/2- 0.28 ps +48-14     655.9 2 
  100
(M1+E2)
      30.77
1/2-
     743.95 5   CDE    J   N        WX  7/2+ 0.51 ps 4     744.06 12 
  100
M1+E2
       0.0
9/2+
     808.82 7  BCDE G IJ L           X  5/2+ 6.16 ps 20      64.88 18 
   808.53 12 
    1.25 8 
  100.00 8 
(M1)
E2
     743.95
       0.0
7/2+
9/2+
     810.32 9  BC E   IJ L           X  5/2- > 1.0 ps    123.3 2 
   779.53 22 
   <1
  100

(E2)
     686.79
      30.77
3/2-
1/2-
     949.80 3 ABCDEF  IJ LMN        WXY 13/2+ 4.36 ps 15     949.81 3 
  100
E2
       0.0
9/2+
     970 10 ?      G                   1/2-,3/2-        
     978.91 5  BCDEF  IJ   N        WX  11/2+ 258 fs 18     978.94 14 
  100
M1+E2
       0.0
9/2+
    1082.68 5  BCDEFG  J L N         X  9/2+ > 2.8 ps    103.80 11 
   338.73 7 
  1082.53 15 
    9 3 
  100.0 17 
   35 3 

(E2+M1)
M1+E2
     978.91
     743.95
       0.0
11/2+
7/2+
9/2+
    1127.09 12     E    J             X  3/2,5/2,7/2      318.3 2 
  100
D+Q
     808.82
5/2+
    1284.26 13     E                  X  (5/2)- 0.17 ps +6-4     473.9 2 
   597.3 2 
  1253.5 2 
    5 4 
   25 4 
  100 4 

M1+E2

     810.32
     686.79
      30.77
5/2-
3/2-
1/2-
    1290 12  BC   GHI  L              1/2-,3/2-        
    1297.22 6  BCDEF  I             WX  9/2+ 0.21 ps 3     318.3 1 
   553.10 9 
  1297.38 9 
   44 8 
   52.2 20 
  100.0 25 
(M1)
(M1(+E2))
M1+E2
     978.91
     743.95
       0.0
11/2+
7/2+
9/2+
    1315.50 11   C E G I    N         X  5/2+ 0.37 ps +31-12     506.7 2 
   571.5 2 
   23.5 12 
  100.0 25 
M1+E2
M1+E2
     808.82
     743.95
5/2+
7/2+
    1335.04 4 A   E       M          XY 17/2+ < 14 ns    385.224 23 
  100
E2
     949.80
13/2+
    1369.86 17  B  E  H   L           X  5/2- > 0.55 ps    559.4 2 
   683.2 2 
  1338.9
  100 4 
   30 4 
   14
D+Q
D+Q

     810.32
     686.79
      30.77
5/2-
3/2-
1/2-
    1395.42 13     E                  X  (7/2-) > 0.55 ps    584.97 22 
   708.6 2 
  100 4 
    9 4 
D+Q
[E2]
     810.32
     686.79
5/2-
3/2-
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
    1455.0 8     E   I                 (1/2+,3/2+)      646.2 8 
  100

     808.82
5/2+
    1483.58 7     EF  I  L          WX  7/2(+) 45.7 fs 24     400.8 1 
   674.8 1 
  1483.46 16 
    8.2 18 
   24.4 15 
  100.0 16 

(M1+E2)
(M1+E2)
    1082.68
     808.82
       0.0
9/2+
5/2+
9/2+
    1490.99 5 A   EF  I  L           XY 15/2+ < 14 ns    155.94 3 
   541.29 7 
   22 5 
  100.0 16 
[M1,E2]
M1+E2
    1335.04
     949.80
17/2+
13/2+
    1499.94 6     E   I    N        WX  (9/2-) 0.84 ps 22     520.9 1 
   689.6 1 
   756.1 1 
  1499.9 1 
    2 2 
   18 3 
    6.9 10 
  100 2 
[E1]
[E2]
[E1]
(E1(+M2))
     978.91
     810.32
     743.95
       0.0
11/2+
5/2-
7/2+
9/2+
    1571.82 14  B  E G    L           X  3/2- 0.19 ps +15-7     287.4 2 
   761.4 2 
   885.1 2 
   20 5 
  100 5 
   37 5 

M1+E2
M1+E2
    1284.26
     810.32
     686.79
(5/2)-
5/2-
3/2-
    1588.06 17     E                  X  3/2(-),5/2(-) > 0.87 ps    777.8 2 
   901.2 2 
   18 8 
  100 8 
(M1+E2)
(M1+E2)
     810.32
     686.79
5/2-
3/2-
    1603.24 16 ?    E                     (9/2-)      520.5 4 ?
   624.5 3 ?
   859.1 3 ?
   37 5 
  100 5 
   63



    1082.68
     978.91
     743.95
9/2+
11/2+
7/2+
    1603.44 9     E                  X  11/2+ 0.32 ps +17-9     520.9 2 
   624.4 2 
   653.6 2 
   859.5 2 
  1603.5 2 
   13 3 
   33.0 15 
  100 3 
   26 4 
   23 3 
(M1(+E2))
(M1+E2)
M1+E2
[E2]

    1082.68
     978.91
     949.80
     743.95
       0.0
9/2+
11/2+
13/2+
7/2+
9/2+
    1665.66 12  B  E G I  L N         X  5/2+ 0.24 ps +7-5     856.9 2 
   921.6 2 
  1665.7 2 
   <1
  100 2 
    2 2 

M1+E2

     808.82
     743.95
       0.0
5/2+
7/2+
9/2+
    1679.50 10  B  EF  I  L N         X  5/2(+),7/2 0.22 ps +6-4     364.1 2 
   382.4 2 
   870.1 2 
   935.7 2 
  1679.58 24 
   60 3 
   16 3 
    7 3 
  100 3 
   37.4 17 
D+Q


D(+Q)

    1315.50
    1297.22
     808.82
     743.95
       0.0
5/2+
9/2+
5/2+
7/2+
9/2+
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
    1683.36 8  B  EF  I  L N         X  9/2+ 104 fs +17-14     600.7 2 
   704.2 2 
   939.3 2 
  1683.2 2 
   17 4 
   42 4 
  100 3 
   57.4 19 

M1+E2
M1+E2
(M1+E2)
    1082.68
     978.91
     743.95
       0.0
9/2+
11/2+
7/2+
9/2+
    1686.34 9  B  EF  I              X  13/2+ 0.17 ps +4-3     707.4 2 
   736.5 2 
  1686.3 2 
   88 4 
   90 4 
  100 4 
M1+E2
D+Q
[E2]
     978.91
     949.80
       0.0
11/2+
13/2+
9/2+
    1694.0?    E        N                 950?
  100

     743.95
7/2+
    1703.51 16     E G                X  3/2+,5/2+ 0.15 ps +19-6     387.9 2 
   894.8 2 
  100 4 
   87 4 
(M1(+E2))
(M1+E2)
    1315.50
     808.82
5/2+
5/2+
    1772.96 17     E      L           X  (LE7/2) 87 fs +14-10     318.27 17 ?
   646.0 2 
   964.0 2 
   25
   86 4 
  100 4 



    1455.0
    1127.09
     808.82
(1/2+,3/2+)
3/2,5/2,7/2
5/2+
    1779.27 17     E      L           X  (5/2-) 73 fs +30-19     969.0 2 
  1092.4 2 
  100 5 
    8 5 
(M1(+E2))
(M1(+E2))
     810.32
     686.79
5/2-
3/2-
    1784.40 25     E      L              (5/2+)      701.71 24 
  100

    1082.68
9/2+
    1812.34 21     E                  X  (19/2) 104 fs +35-24     477.3 2 
  100

    1335.04
17/2+
    1840.07 17     E                  X  3/2-,5/2- 71 fs +24-17    1029.6 2 
  1153.4 2 
   20 4 
  100 4 
(M1+E2)
M1+E2
     810.32
     686.79
5/2-
3/2-
    1908.1 11   C E                     (5/2)     1908.1 11 
  100

       0.0
9/2+
    1910.68 7   C E                 WX  7/2+,9/2+,11/2+ 162 fs 13     613.4 1 
   828.1 1 
  1910.6 1 
   10 3 
    7 3 
  100 3 
(M1+E2)
M1+E2
M1+E2
    1297.22
    1082.68
       0.0
9/2+
9/2+
9/2+
    1915.92 10     E                  X  7/2 62 fs 7     600.4 2 
   833.4 2 
  1107.2 2 
  1172.1 2 
  1915.5 2 
   36 4 
  100 4 
    4 4 
   12 4 
    5 4 
D+Q
D(+Q)



    1315.50
    1082.68
     808.82
     743.95
       0.0
5/2+
9/2+
5/2+
7/2+
9/2+
    1947.73 22   C E        N         X  3/2,5/2,7/2 0.16 ps +9-5    1137.4 2 
  100
D(+Q)
     810.32
5/2-
    1949.72 10   C E        N         X  (7/2+) 0.5 ps +11-2     270.1 2 
   866.8 2 
   971.1 2 
  1140.8 2 
  1205.9 2 
  100 5 
    9 5 
   <2
  100 5 
   89 4 


[E2]
(M1+E2)

    1679.50
    1082.68
     978.91
     808.82
     743.95
5/2(+),7/2
9/2+
11/2+
5/2+
7/2+
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
    1949.81 13     EF       N         X  (11/2) 0.6 ps +26-3     266.4 2 
   346.4 2 
  1949.8 2 
   32 5 
   50 5 
  100 5 



    1683.36
    1603.44
       0.0
9/2+
11/2+
9/2+
    1968.27 17     E                 WX  (13/2-)      365.0 2 
   477.3 2 
   45 3 
  100 3 


    1603.24
    1490.99
(9/2-)
15/2+
    1968.87 5     E        N        WX  11/2+ 111 fs 19     282.5 1 
   285.4 1 
   990.0 1 
  1019.0 1 
  1225.0 1 
  1968.9 1 
   23 5 
   29 6 
   64 5 
   31 4 
   12 5 
  100 3 
[M1,E2]
[M1,E2]
M1+E2
M1+E2
[E2]

    1686.34
    1683.36
     978.91
     949.80
     743.95
       0.0
13/2+
9/2+
11/2+
13/2+
7/2+
9/2+
    1997.12 17     E                  X  3/2-,5/2- 64 fs +15-12    1186.9 2 
  1310.2 2 
  100 5 
   12 5 
M1+E2
(M1+E2)
     810.32
     686.79
5/2-
3/2-
    2002.52 10  B  E                  X  (11/2+) > 0.55 ps    399.1 2 
   502.4 2 
   511.5 2 
  1023.7 2 
  1052.8 2 
   20 2 
   12 2 
   <2
   10 2 
  100 2 

[E1]

[E2]
(M1+E2)
    1603.44
    1499.94
    1490.99
     978.91
     949.80
11/2+
(9/2-)
15/2+
11/2+
13/2+
    2012.41 18                        X  (LE5/2)- 21 fs +20-8     440.4 2 
  1325.8 2 
    6 5 
  100 5 

M1+E2
    1571.82
     686.79
3/2-
3/2-
    2019.7 4     E                     (7/2-,9/2-)     1209.4 4 
  100

     810.32
5/2-
    2023.91 18                        X  (LE5/2)- 54 fs +28-17     452.1 2 
  1337.1 2 
    3 3 
  100 3 

M1+E2
    1571.82
     686.79
3/2-
3/2-
    2037.2 3     E                     (9/2+,11/2+)      537.2 3 
  1087.4 6 
  100
   28


    1499.94
     949.80
(9/2-)
13/2+
    2099.23 17     E      L           X  (3/2-,5/2,7/2) 92 fs +43-25     703.8 2 
  1288.9 2 
  100 7 
   46 7 

D(+Q)
    1395.42
     810.32
(7/2-)
5/2-
    2122.67 6     E                 WX  9/2+ 97 fs 16     639.0 1 
  1143.7 1 
  1378.9 1 
  2122.6 1 
   36 3 
   71 3 
   29 3 
  100 3 

M1+E2
M1+E2

    1483.58
     978.91
     743.95
       0.0
7/2(+)
11/2+
7/2+
9/2+
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
    2126.89 12     E                  X  (5/2-,7/2,9/2-) 0.16 ps +12-8     626.9 2 
   731.3 2 
  1316.61 20 
  1383.1 2 
  100 4 
   18 4 
   10 4 
   13 4 




    1499.94
    1395.42
     810.32
     743.95
(9/2-)
(7/2-)
5/2-
7/2+
    2132.6 5  B  E      L              (GE7/2)     1153.7 5 
  100

     978.91
11/2+
    2153.60 20  B  E                  X  (1/2,3/2,5/2-) 80 fs +19-14    2122.8 2 
  100

      30.77
1/2-
    2162.64 12  B  E        N         X  (11/2+,13/2,15/2+) 0.28 ps +21-9     671.7 2 
  1183.7 2 
  1212.8 2 
   24 3 
  100 4 
   61 4 



    1490.99
     978.91
     949.80
15/2+
11/2+
13/2+
    2170.65 10  B  E                  X  9/2+ 0.24 ps +11-6    1087.6 2 
  1192.5 2 
  1221.6 2 
  1361.1 2 
  1426.1 2 
  2171.4 5 
   10 3 
  100 3 
   60 3 
   31 3 
   27 3 
   14 2 






    1082.68
     978.91
     949.80
     808.82
     743.95
       0.0
9/2+
11/2+
13/2+
5/2+
7/2+
9/2+
    2180 10       G      N            3/2+,5/2+        
    2180.04 5 A                       Y (17/2)-      689.053 19 
   844.96 6 
  100.0 25 
   37.5 25 
E1

    1490.99
    1335.04
15/2+
17/2+
    2184.14 21     E                  X  76 ps +31-21     849.1 2 
  100

    1335.04
17/2+
    2203.5 3     E                     (9/2+)      600.4 3 ?
   808.3 4 
  2203.2 4 
   24
  100
   33



    1603.24
    1395.42
       0.0
(9/2-)
(7/2-)
9/2+
    2250  C                              
    2280.7 7   C E                     (7/2-)     1536.7 7 
  100

     743.95
7/2+
    2310.9 9                         Y      976
  100

    1335.04
17/2+
    2320 10  B    G                   3/2+,5/2+        
    2330.0 5  B  E                         1351.1 5 
  100

     978.91
11/2+
    2367.5 10  BC EF                    9/2,13/2(+)     2367.3 10 
  100

       0.0
9/2+
    2506.88 8                       WX  66 fs +21-14    1527.9 1 
  2506.9 1 
 
 


     978.91
       0.0
11/2+
9/2+
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
    2520 10  BC   G      N            (1/2+)        
    2584.2 7  BC E G                   3/2+,5/2+     1775.4 7 
  100

     808.82
5/2+
    2752.84 5 A                         (19/2)+      572.796 19 
  1261.91 14 
  1417.75 10 
  100 4 
   59 4 
   55 4 



    2180.04
    1490.99
    1335.04
(17/2)-
15/2+
17/2+
    2832.8 9             M           Y 21/2+      522
  1497.6
    4.9 7 
  100 7 

E2
    2310.9
    1335.04

17/2+
    2838 4  BC  F       N            11/2        
    2980 20  BC                              
    3086.0 10                         Y (21/2)      906
  100
Q
    2180.04
(17/2)-
    3150 20  BC                              
    3512 17  B      I                        
    3667.8 13                         Y      835
  100

    2832.8
21/2+
    3674.0 15                         Y (25/2)      588
  100

    3086.0
(21/2)
    3684.8 12                         Y      852
  100

    2832.8
21/2+
    3720 30  B                               
    3840 17  B      I                        
    3930 30         I                        
    4060 30         I                        
    4104.7 12             M           Y 25/2(+)      420
  1271.9
    9.7 7 
  100 5 
D+Q
Q
    3684.8
    2832.8

21/2+
    4224 17  B      I                        
    4340 20  B                               
    4403.0 18                         Y (29/2)      729
  100

    3674.0
(25/2)
    4460 20  B                               
    4548 17  B      I                        
    4650 20 ? B                               
    4700 30  B                               
    4810 30  B                               
    4864.6 16             M           Y 29/2(+)      759.9
  100
E2
    4104.7
25/2(+)
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
    5000 30  B                               
    5155.1 18                         Y     1481
  100

    3674.0
(25/2)
    5340 40  B                               
    5490 40  B                               
    5904.3 19             M           Y 33/2(+)     1039.7
  100
E2
    4864.6
29/2(+)
    6464.3 10      F                    11/2(+)     3626 3 
  4095 3 
  4514 3 
  4783 3 
  4971 3 
  4979 3 
  5168 3 
  5384 3 
  5486 3 
  5516 3 
  6465 3 
   29 9 
   29 9 
   11.4 11 
   11.1 4 
    9.3 4 
    4.3 11 
   10.7 7 
   16.8 7 
    0.7 7 
  100.0 18 
   35.7 7 
D
D
D



D
D

(M1)
(M1)
    2838
    2367.5
    1949.81
 
    1490.99
    1483.58
    1297.22
    1082.68
     978.91
     949.80
       0.0
11/2
9/2,13/2(+)
(11/2)
 
15/2+
7/2(+)
9/2+
9/2+
11/2+
13/2+
9/2+
    7372.3 21                         Y (35/2-)     1468
  100
D+Q
    5904.3
33/2(+)
    7435.3 21                         Y 37/2(-)     1531
  100
Q
    5904.3
33/2(+)
    7828.3 23                         Y 39/2(-)      393
  100
M1
    7435.3
37/2(-)
    8325.4 25                         Y 41/2(-)      497
  100
D
    7828.3
39/2(-)
    8377.4 21                         Y (37/2)      942
  1005
  100 10 
   59 6 
D+Q
D
    7435.3
    7372.3
37/2(-)
(35/2-)
    8940 3                         Y (43/2-)      615
  100
M1
    8325.4
41/2(-)
    9134.4 22                         Y (41/2-)     1699
  100
(E2)
    7435.3
37/2(-)
    9425 3                         Y (45/2+)      485
  100
E1
    8940
(43/2-)
    9699.4 22                         Y (39/2-,41/2-)     2264
  100

    7435.3
37/2(-)
    9782.4 23 ?                        Y     1405?
  100

    8377.4
(37/2)
    9922.4 23                         Y (43/2-)      223
   788
   70 10 
  100 13 

M1
    9699.4
    9134.4
(39/2-,41/2-)
(41/2-)
   10955.4 25                         Y     1033
  100

    9922.4
(43/2-)
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
    7435.3+X                        Y 1.5 µs 5       
   11059      G   K               5/2+ 13 keV 5       
   11981 5           K        TU     1/2+ 90 keV 9       
  ≈12171                    U     24 keV      
   12503      G   K               3/2+ 38 keV 3       
   12570 40       G                   7/2+,9/2+        
   12993          K               1/2+ 42 keV 3       
   13090 40       G                   9/2-,11/2-        
   13542          K               68 keV 5       
   13581          K               3/2+ 45 keV 5       
   13839          K               3/2+ 63 keV 3       
   14091          K               30 keV 3       
   14363          K               5/2+ 51 keV 5       
   14477          K               7/2- 43 keV 7       
   16400 50               O           - 5.05 MeV      

E(level): From least-squares fit to adopted Eγ, assigning 1 keV uncertainty to Eγ data for which the authors did not assign an uncertainty.

T1/2(level): From Coulomb excitation, if not indicated otherwise.

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Band Transitions:

E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 1 - π=- MIXED SYMMETRY STATES.
    1779.27 17  (5/2-) 73 fs +30-19       
    1840.07 17  3/2-,5/2- 71 fs +24-17    1029.6 2 
  1153.4 2 
   20 4 
  100 4 
(M1+E2)
M1+E2
     810.32
     686.79
5/2-
3/2-
E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 2 - K=37/2 OBLATE M1 BAND?
    7435.3 21  37/2(-)        
    7828.3 23  39/2(-)      393
  100
M1
    7435.3
37/2(-)
    8325.4 25  41/2(-)      497
  100
D
    7828.3
39/2(-)
    8940 3  (43/2-)      615
  100
M1
    8325.4
41/2(-)
E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 3 - π=- 2-PHONON IS STATES.
    1284.26 13  (5/2)- 0.17 ps +6-4       
    1395.42 13  (7/2-) > 0.55 ps    584.97 22 
   708.6 2 
  100 4 
    9 4 
D+Q
[E2]
     810.32
     686.79
5/2-
3/2-
    1499.94 6  (9/2-) 0.84 ps 22     520.9 1 
   689.6 1 
   756.1 1 
  1499.9 1 
    2 2 
   18 3 
    6.9 10 
  100 2 
[E1]
[E2]
[E1]
(E1(+M2))
     978.91
     810.32
     743.95
       0.0
11/2+
5/2-
7/2+
9/2+
    1571.82 14  3/2- 0.19 ps +15-7     287.4 2 
   761.4 2 
   885.1 2 
   20 5 
  100 5 
   37 5 

M1+E2
M1+E2
    1284.26
     810.32
     686.79
(5/2)-
5/2-
3/2-
E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 4 - π=+ 1-PHONON IV STATES.
    1297.22 6  9/2+ 0.21 ps 3       
    1315.50 11  5/2+ 0.37 ps +31-12     506.7 2 
   571.5 2 
   23.5 12 
  100.0 25 
M1+E2
M1+E2
     808.82
     743.95
5/2+
7/2+
    1483.58 7  7/2(+) 45.7 fs 24     400.8 1 
   674.8 1 
  1483.46 16 
    8.2 18 
   24.4 15 
  100.0 16 

(M1+E2)
(M1+E2)
    1082.68
     808.82
       0.0
9/2+
5/2+
9/2+
    1603.44 9  11/2+ 0.32 ps +17-9     520.9 2 
   624.4 2 
   653.6 2 
   859.5 2 
  1603.5 2 
   13 3 
   33.0 15 
  100 3 
   26 4 
   23 3 
(M1(+E2))
(M1+E2)
M1+E2
[E2]

    1082.68
     978.91
     949.80
     743.95
       0.0
9/2+
11/2+
13/2+
7/2+
9/2+
E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 5 - π 1g9/2~#(2+,92Zr).
     743.95 5  7/2+ 0.51 ps 4       
     808.82 7  5/2+ 6.16 ps 20      64.88 18 
   808.53 12 
    1.25 8 
  100.00 8 
(M1)
E2
     743.95
       0.0
7/2+
9/2+
     949.80 3  13/2+ 4.36 ps 15     949.81 3 
  100
E2
       0.0
9/2+
     978.91 5  11/2+ 258 fs 18     978.94 14 
  100
M1+E2
       0.0
9/2+
    1082.68 5  9/2+ > 2.8 ps    103.80 11 
   338.73 7 
  1082.53 15 
    9 3 
  100.0 17 
   35 3 

(E2+M1)
M1+E2
     978.91
     743.95
       0.0
11/2+
7/2+
9/2+

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Additional Gamma Data:















E(level)
(keV)
Jπ(level)T1/2(level)E(γ)
(keV)
MultipolarityMixing
Ratio
Conversion
Coefficient
Additional Data
      30.77 1/2- 16.12 y 12 
% IT = 100
    30.77 2 M4 1.693×105B(M4)(W.u.)=11.49 20, α=1.693×105
     686.79 3/2- 0.28 ps +48-14     655.9 2 (M1+E2)-0.13 +9-140.00187B(E2)(W.u.)=11 +16-11, B(M1)(W.u.)=0.27 +14-27, α=0.00187
     743.95 7/2+ 0.51 ps 4     744.06 12 M1+E2+0.236 181.41×10-3B(E2)(W.u.)=10.2 17, B(M1)(W.u.)=0.099 8, α=1.41E-3
     808.82 5/2+ 6.16 ps 20      64.88 18 (M1) 0.767B(M1)(W.u.)=0.160 12, α=0.767 13
5/2+ 6.16 ps 20     808.53 12 E2 1.20×10-3B(E2)(W.u.)=10.4 4, α=1.20E-3
     810.32 5/2- > 1.0 ps    779.53 22 (E2) 1.31×10-3B(E2)(W.u.)<78, α=1.31E-3
     949.80 13/2+ 4.36 ps 15     949.81 3 E2 8.12×10-4B(E2)(W.u.)=6.70 23, α=8.12E-4
     978.91 11/2+ 258 fs 18     978.94 14 M1+E2-0.255 87.69×10-4B(E2)(W.u.)=5.96 20, B(M1)(W.u.)=0.085 6, α=7.69E-4
    1082.68 9/2+ > 2.8 ps    338.73 7 (E2+M1)-0.09 20.00911B(E2)(W.u.)<14, B(M1)(W.u.)<0.14, α=0.00911 16
9/2+ > 2.8 ps   1082.53 15 M1+E21.8 GT6.08×10-4B(E2)(W.u.)=1.03 9, B(M1)(W.u.)<0.00035, α=6.08E-4
    1127.09 3/2,5/2,7/2      318.3 2 D+Q-0.20 60.01053α=0.01053
    1284.26 (5/2)- 0.17 ps +6-4     597.3 2 M1+E2+0.14 4B(E2)(W.u.)=6 +4-5, B(M1)(W.u.)=0.11 +4-5
    1297.22 9/2+ 0.21 ps 3     318.3 1 (M1) 0.01053B(M1)(W.u.)=0.73 18, α=0.01053
9/2+ 0.21 ps 3     553.10 9 (M1(+E2))+0.02 30.00282B(E2)(W.u.)=0.2 +7-2, B(M1)(W.u.)=0.16 3, α=0.00282 24
9/2+ 0.21 ps 3    1297.38 9 M1+E2+0.355 254.45×10-4B(E2)(W.u.)=1.52 10, B(M1)(W.u.)=0.022 4, α=4.45E-4
    1315.50 5/2+ 0.37 ps +31-12     506.7 2 M1+E2-1.4 8B(E2)(W.u.)=2.3×102 +12-22, B(M1)(W.u.)=0.029 +25-29
5/2+ 0.37 ps +31-12     571.5 2 M1+E2+0.14 4B(E2)(W.u.)=16 +11-16, B(M1)(W.u.)=0.25 +9-22
    1335.04 17/2+ < 14 ns    385.224 23 E2 0.01002B(E2)(W.u.)>0.19, α=0.01002
    1369.86 5/2- > 0.55 ps    559.4 2 D+Q-0.32 7 
5/2- > 0.55 ps    683.2 2 D+Q-0.34 5 
    1395.42 (7/2-) > 0.55 ps    584.97 22 D+Q-0.10 2 
(7/2-) > 0.55 ps    708.6 2 [E2] B(E2)(W.u.)<19
    1483.58 7/2(+) 45.7 fs 24     674.8 1 (M1+E2)-0.11 8B(E2)(W.u.)=8 +12-8, B(M1)(W.u.)=0.285 25
7/2(+) 45.7 fs 24    1483.46 16 (M1+E2)-0.13 7B(E2)(W.u.)=0.9 +10-9, B(M1)(W.u.)=0.109 7
    1490.99 15/2+ < 14 ns    155.94 3 [M1,E2] 0.15α=0.15 9
15/2+ < 14 ns    541.29 7 M1+E2-0.104 17B(E2)(W.u.)>0.00020, B(M1)(W.u.)>7.8E-6
E(level)
(keV)
Jπ(level)T1/2(level)E(γ)
(keV)
MultipolarityMixing
Ratio
Conversion
Coefficient
Additional Data
    1499.94 (9/2-) 0.84 ps 22     520.9 1 [E1] B(E1)(W.u.)=4.E-5 +5-4
(9/2-) 0.84 ps 22     689.6 1 [E2] B(E2)(W.u.)=24 8
(9/2-) 0.84 ps 22     756.1 1 [E1] B(E1)(W.u.)=4.9E-5 15
(9/2-) 0.84 ps 22    1499.9 1 (E1(+M2))-0.02 16B(E1)(W.u.)=9.2E-5 25, B(M2)(W.u.)=0.07 +120-7
    1571.82 3/2- 0.19 ps +15-7     761.4 2 M1+E2-0.28 3B(E2)(W.u.)=22 +10-18, B(M1)(W.u.)=0.16 +6-13
3/2- 0.19 ps +15-7     885.1 2 M1+E2-1.60 14B(E2)(W.u.)=37 +15-30, B(M1)(W.u.)=0.011 +5-9
    1588.06 3/2(-),5/2(-) > 0.87 ps    777.8 2 (M1+E2)-4.0 +13-35B(E2)(W.u.)<14, B(M1)(W.u.)<0.00078
3/2(-),5/2(-) > 0.87 ps    901.2 2 (M1+E2)-0.53 6B(E2)(W.u.)<9.6, B(M1)(W.u.)<0.024
    1603.44 11/2+ 0.32 ps +17-9     520.9 2 (M1(+E2))-0.07 9B(E2)(W.u.)=0.6 +16-6, B(M1)(W.u.)=0.032 +12-19
11/2+ 0.32 ps +17-9     624.4 2 (M1+E2)+0.11 6B(E2)(W.u.)=1.5 +17-15, B(M1)(W.u.)=0.047 +14-26
11/2+ 0.32 ps +17-9     653.6 2 M1+E2+0.17 3B(E2)(W.u.)=9 +4-6, B(M1)(W.u.)=0.13 +4-7
11/2+ 0.32 ps +17-9     859.5 2 [E2] B(E2)(W.u.)=20 +7-12
    1665.66 5/2+ 0.24 ps +7-5     921.6 2 M1+E2+1.4 2B(E2)(W.u.)=92 +22-29, B(M1)(W.u.)=0.039 +11-14
    1679.50 5/2(+),7/2 0.22 ps +6-4     364.1 2 D+Q-0.17 9 
5/2(+),7/2 0.22 ps +6-4     935.7 2 D(+Q)+0.09 9 
    1683.36 9/2+ 104 fs +17-14     704.2 2 M1+E2+0.21 4B(E2)(W.u.)=10 5, B(M1)(W.u.)=0.113 +19-22
9/2+ 104 fs +17-14     939.3 2 M1+E2-0.20 4B(E2)(W.u.)=5.3 +22-23, B(M1)(W.u.)=0.114 +17-20
9/2+ 104 fs +17-14    1683.2 2 (M1+E2)-0.34 25B(E2)(W.u.)=0.4 +6-4, B(M1)(W.u.)=0.0106 +22-24
    1686.34 13/2+ 0.17 ps +4-3     707.4 2 M1+E2-0.09 3B(E2)(W.u.)=1.9 14, B(M1)(W.u.)=0.115 +22-28
13/2+ 0.17 ps +4-3     736.5 2 D+Q-0.27 13 
13/2+ 0.17 ps +4-3    1686.3 2 [E2] B(E2)(W.u.)=3.5 +7-9
    1703.51 3/2+,5/2+ 0.15 ps +19-6     387.9 2 (M1(+E2))-0.02 6B(E2)(W.u.)=4 +22-4, B(M1)(W.u.)=1.3 +6-13
3/2+,5/2+ 0.15 ps +19-6     894.8 2 (M1+E2)-0.3 1B(E2)(W.u.)=10 +8-10, B(M1)(W.u.)=0.09 +4-9
    1779.27 (5/2-) 73 fs +30-19     969.0 2 (M1(+E2))+0.04 6B(E2)(W.u.)=0.5 +17-5, B(M1)(W.u.)=0.31 +9-13
(5/2-) 73 fs +30-19    1092.4 2 (M1(+E2))+0.05 9B(E2)(W.u.)=0.04 +14-4, B(M1)(W.u.)=0.017 +12-13
E(level)
(keV)
Jπ(level)T1/2(level)E(γ)
(keV)
MultipolarityMixing
Ratio
Conversion
Coefficient
Additional Data
    1910.68 7/2+,9/2+,11/2+ 162 fs 13     613.4 1 (M1+E2)-0.20 12B(E2)(W.u.)=5 +7-5, B(M1)(W.u.)=0.048 16
7/2+,9/2+,11/2+ 162 fs 13     828.1 1 M1+E2-0.61 17B(E2)(W.u.)=6 4, B(M1)(W.u.)=0.010 5
7/2+,9/2+,11/2+ 162 fs 13    1910.6 1 M1+E2+3.9 364.52×10-4B(E2)(W.u.)=4.4 7, B(M1)(W.u.)=0.0010 +18-10, α=4.52E-4 23
    1915.92 7/2 62 fs 7     600.4 2 D+Q+0.06 4 
7/2 62 fs 7     833.4 2 D(+Q)-0.01 2 
    1947.73 3/2,5/2,7/2 0.16 ps +9-5    1137.4 2 D(+Q)+0.05 4 
    1949.72 (7/2+) 0.5 ps +11-2     971.1 2 [E2] B(E2)(W.u.)=0.18 +19-18
(7/2+) 0.5 ps +11-2    1140.8 2 (M1+E2)+0.21 5B(E2)(W.u.)=0.33 +21-33, B(M1)(W.u.)=0.010 +4-10
    1968.87 11/2+ 111 fs 19     282.5 1 [M1,E2] 0.021α=0.021 7
11/2+ 111 fs 19     285.4 1 [M1,E2] 0.021α=0.021 7
11/2+ 111 fs 19     990.0 1 M1+E2-0.83 16B(E2)(W.u.)=21 7, B(M1)(W.u.)=0.030 8
11/2+ 111 fs 19    1019.0 1 M1+E2-0.28 7B(E2)(W.u.)=1.6 9, B(M1)(W.u.)=0.021 5
11/2+ 111 fs 19    1225.0 1 [E2] B(E2)(W.u.)=3.4 16
    1997.12 3/2-,5/2- 64 fs +15-12    1186.9 2 M1+E2-0.31 11B(E2)(W.u.)=12 +8-9, B(M1)(W.u.)=0.17 +4-5
3/2-,5/2- 64 fs +15-12    1310.2 2 (M1+E2)-0.29 12B(E2)(W.u.)=0.8 7, B(M1)(W.u.)=0.015 +7-8
    2002.52 (11/2+) > 0.55 ps    502.4 2 [E1] B(E1)(W.u.)<0.00040
(11/2+) > 0.55 ps   1023.7 2 [E2] B(E2)(W.u.)<2.6
(11/2+) > 0.55 ps   1052.8 2 (M1+E2)-0.63 76.50×10-4B(E2)(W.u.)<7.3, B(M1)(W.u.)<0.018, α=6.50E-4 13
    2012.41 (LE5/2)- 21 fs +20-8    1325.8 2 M1+E2+4.5 +15-9B(E2)(W.u.)=2.4×102 +10-23, B(M1)(W.u.)=0.020 +15-20
    2023.91 (LE5/2)- 54 fs +28-17    1337.1 2 M1+E2-4.7 +8-13B(E2)(W.u.)=9.×101 +3-5, B(M1)(W.u.)=0.007 +4-5
    2099.23 (3/2-,5/2,7/2) 92 fs +43-25    1288.9 2 D(+Q)-0.05 5 
    2122.67 9/2+ 97 fs 16    1143.7 1 M1+E2+3.8 +19-10B(E2)(W.u.)=34 7, B(M1)(W.u.)=0.003 3
9/2+ 97 fs 16    1378.9 1 M1+E2-0.19 8B(E2)(W.u.)=0.20 17, B(M1)(W.u.)=0.0103 21
    6464.3 11/2(+)     5516 3 (M1) 1.62×10-3α=1.62×10-3

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Additional Level Data and Comments:

E(level)Jπ(level)T1/2(level)Comments
       0.09/2+ STABLE Q=-0.32 2, μ=+6.1705 3
Δ<r2>(91gIβ normalization,93Nb)=+0.312 2 (2009Ch25) from LASER spectroscopy (optical pumping in ion beam cooler buncher); authors also report isotope shift and hfs coefficients.
E(level): Δ<r2>(91gIβ normalization,93Nb)=+0.312 2 (2009Ch25) from LASER spectroscopy (optical pumping in ion beam cooler buncher); authors also report isotope shift and hfs coefficients.
     686.793/2- 0.28 ps +48-14  E(level): Interpreted in (p,2nγ) as symmetric one-phonon state with configuration of (π p1/2-1)#(first 2+ state in 94Mo) (2006Or09).
     743.957/2+ 0.51 ps 4  E(level): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors. π 1g9/2~#(2+,92Zr).
     808.825/2+ 6.16 ps 20  Other T1/2: >2.8 ps from (α,pγ).
E(level): Other T1/2: >2.8 ps from (α,pγ). From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors. π 1g9/2~#(2+,92Zr).
     810.325/2- > 1.0 ps E(level): Interpreted in (p,2nγ) as symmetric one-phonon state with configuration of (π p1/2-1)#(first 2+ state in 94Mo) (2006Or09).
     949.8013/2+ 4.36 ps 15  E(level): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors. π 1g9/2~#(2+,92Zr).
     978.9111/2+ 258 fs 18  E(level): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors. π 1g9/2~#(2+,92Zr).
    1082.689/2+ > 2.8 ps E(level): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors. π 1g9/2~#(2+,92Zr).
    1127.093/2,5/2,7/2   E(level): Isoscalar excitation is proposed by 2010Or01 for this state in (p,2nγ).
    1284.26(5/2)- 0.17 ps +6-4  E(level): π=- 2-PHONON IS STATES.
T1/2(level): From DSAM in (n,n’γ).
    12901/2-,3/2-   XREF: H(1320)L(1279).
    1297.229/2+ 0.21 ps 3  E(level): π=+ 1-PHONON IV STATES.
    1315.505/2+ 0.37 ps +31-12  XREF: γ(1330).
E(level): π=+ 1-PHONON IV STATES.
T1/2(level): From DSAM in (n,n’γ).
    1335.0417/2+ < 14 ns E(level): Isoscalar excitation is proposed by 2010Or01 for this state in (p,2nγ).
    1369.865/2- > 0.55 ps T1/2(level): From DSAM in (n,n’γ).
    1395.42(7/2-) > 0.55 ps E(level): π=- 2-PHONON IS STATES.
T1/2(level): From DSAM in (n,n’γ).
    1455.0(1/2+,3/2+)   E(level): From (p,2nγ).
Jπ(level): From statistical analysis in (n,n’γ).
    1483.587/2(+) 45.7 fs 24  E(level): π=+ 1-PHONON IV STATES.
    1490.9915/2+ < 14 ns Other T1/2: >0.52 ps from (n,n’γ).
E(level): Other T1/2: >0.52 ps from (n,n’γ). Isoscalar excitation is proposed by 2010Or01 for this state in (p,2nγ).
    1499.94(9/2-) 0.84 ps 22  E(level): π=- 2-PHONON IS STATES.
    1571.823/2- 0.19 ps +15-7  E(level): π=- 2-PHONON IS STATES.
T1/2(level): From DSAM in (n,n’γ).
    1588.063/2(-),5/2(-) > 0.87 ps E(level): Isoscalar excitation is proposed by 2010Or01 for this state in (p,2nγ).
T1/2(level): From DSAM in (n,n’γ).
    1603.24(9/2-)   Possibly the same level as that adopted at 1603.8 keV even though Jπ from (n,n’γ) differs.
E(level): Possibly the same level as that adopted at 1603.8 keV even though Jπ from (n,n’γ) differs.
    1603.4411/2+ 0.32 ps +17-9  E(level): π=+ 1-PHONON IV STATES.
    1665.665/2+ 0.24 ps +7-5  E(level): Isoscalar excitation is proposed by 2010Or01 for this state in (p,2nγ).
T1/2(level): From DSAM in (n,n’γ).
E(level)Jπ(level)T1/2(level)Comments
    1679.505/2(+),7/2 0.22 ps +6-4  E(level): Isoscalar excitation is proposed by 2010Or01 for this state in (p,2nγ).
T1/2(level): From DSAM in (n,n’γ).
    1683.369/2+ 104 fs +17-14  T1/2(level): From DSAM in (n,n’γ).
    1686.3413/2+ 0.17 ps +4-3  T1/2(level): From DSAM in (n,n’γ).
    1703.513/2+,5/2+ 0.15 ps +19-6  XREF: γ(1710).
E(level): Isoscalar excitation is proposed by 2010Or01 for this state in (p,2nγ).
T1/2(level): From DSAM in (n,n’γ).
    1772.96(LE7/2) 87 fs +14-10  E(level): Isoscalar excitation is proposed by 2010Or01 for this state in (p,2nγ).
T1/2(level): From DSAM in (n,n’γ).
    1779.27(5/2-) 73 fs +30-19  E(level): From 80Se(16O,p2nγ). Uncertainty in Eγ unstated by authors. π=- MIXED SYMMETRY STATES.
    1784.40(5/2+)   E(level): From (p,2nγ).
Jπ(level): From statistical analysis in (n,n’γ).
    1812.34(19/2) 104 fs +35-24  T1/2(level): From DSAM in (n,n’γ).
    1840.073/2-,5/2- 71 fs +24-17  E(level): From 80Se(16O,p2nγ). Uncertainty in Eγ unstated by authors. π=- MIXED SYMMETRY STATES.
    1910.687/2+,9/2+,11/2+ 162 fs 13  E(level): Isovector excitation is proposed by 2010Or01 for this state in (p,2nγ).
    1915.927/2 62 fs 7  E(level): Isovector excitation is proposed by 2010Or01 for this state in (p,2nγ).
T1/2(level): From DSAM in (n,n’γ).
    1947.733/2,5/2,7/2 0.16 ps +9-5  T1/2(level): From DSAM in (n,n’γ).
    1949.72(7/2+) 0.5 ps +11-2  E(level): Two levels at essentially the same energy are proposed in (n,n’γ) near 1950 keV and 1968 keV because, in each case, the authors were unable to fit experimental data for all the attributed γ rays (based on γγ coin) by means of a statistical theory excitation function for a single level. Isoscalar excitation is proposed by 2010Or01 for this state in (p,2nγ).
T1/2(level): From DSAM in (n,n’γ).
    1949.81(11/2) 0.6 ps +26-3  E(level): Two levels at essentially the same energy are proposed in (n,n’γ) near 1950 keV and 1968 keV because, in each case, the authors were unable to fit experimental data for all the attributed γ rays (based on γγ coin) by means of a statistical theory excitation function for a single level.
T1/2(level): From DSAM in (n,n’γ).
    1968.27(13/2-)   E(level): Two levels at essentially the same energy are proposed in (n,n’γ) near 1950 keV and 1968 keV because, in each case, the authors were unable to fit experimental data for all the attributed γ rays (based on γγ coin) by means of a statistical theory excitation function for a single level.
    1968.8711/2+ 111 fs 19  E(level): Two levels at essentially the same energy are proposed in (n,n’γ) near 1950 keV and 1968 keV because, in each case, the authors were unable to fit experimental data for all the attributed γ rays (based on γγ coin) by means of a statistical theory excitation function for a single level. Isoscalar excitation is proposed by 2010Or01 for this state in (p,2nγ).
    1997.123/2-,5/2- 64 fs +15-12  T1/2(level): From DSAM in (n,n’γ).
    2002.52(11/2+) > 0.55 ps E(level): Isoscalar excitation is proposed by 2010Or01 for this state in (p,2nγ).
T1/2(level): From DSAM in (n,n’γ).
    2019.7(7/2-,9/2-)   E(level): From (p,2nγ).
Jπ(level): From statistical analysis in (n,n’γ).
    2023.91(LE5/2)- 54 fs +28-17  E(level): Isoscalar excitation is proposed by 2010Or01 for this state in (p,2nγ).
T1/2(level): From DSAM in (n,n’γ).
    2099.23(3/2-,5/2,7/2) 92 fs +43-25  T1/2(level): From DSAM in (n,n’γ).
    2122.679/2+ 97 fs 16  E(level): Isoscalar excitation is proposed by 2010Or01 for this state in (p,2nγ).
    2126.89(5/2-,7/2,9/2-) 0.16 ps +12-8  T1/2(level): From DSAM in (n,n’γ).
    2153.60(1/2,3/2,5/2-) 80 fs +19-14  E(level): From (p,2nγ).
Jπ(level): From statistical analysis in (n,n’γ).
T1/2(level): From DSAM in (n,n’γ).
    2162.64(11/2+,13/2,15/2+) 0.28 ps +21-9  E(level): Isoscalar excitation is proposed by 2010Or01 for this state in (p,2nγ).
T1/2(level): From DSAM in (n,n’γ).
E(level)Jπ(level)T1/2(level)Comments
    2170.659/2+ 0.24 ps +11-6  E(level): Isoscalar excitation is proposed by 2010Or01 for this state in (p,2nγ).
T1/2(level): From DSAM in (n,n’γ).
    2184.14 76 ps +31-21  T1/2(level): From DSAM in (n,n’γ).
    2280.7(7/2-)   E(level): From (p,2nγ).
Jπ(level): From statistical analysis in (n,n’γ).
    283811/2   XREF: B(2810).
    3086.0(21/2)   Jπ(level): Based on value suggested in (16O,p4nγ) but, in some cases, the evaluator shows the resulting Jπ values in parentheses here.
    3150   XREF: C(3050).
    3674.0(25/2)   Jπ(level): Based on value suggested in (16O,p4nγ) but, in some cases, the evaluator shows the resulting Jπ values in parentheses here.
    4403.0(29/2)   Jπ(level): Based on value suggested in (16O,p4nγ) but, in some cases, the evaluator shows the resulting Jπ values in parentheses here.
    6464.311/2(+)   Γγ=0.038 17
Γγ: from (γ,γ’) E=6465 keV.
E(level): Γγ: from (γ,γ’) E=6465 keV.
    7372.3(35/2-)   Jπ(level): Based on value suggested in (16O,p4nγ) but, in some cases, the evaluator shows the resulting Jπ values in parentheses here.
    7435.337/2(-)   E(level): K=37/2 OBLATE M1 BAND?.
Jπ(level): Based on value suggested in (16O,p4nγ) but, in some cases, the evaluator shows the resulting Jπ values in parentheses here.
    7828.339/2(-)   E(level): K=37/2 OBLATE M1 BAND?.
Jπ(level): Based on value suggested in (16O,p4nγ) but, in some cases, the evaluator shows the resulting Jπ values in parentheses here.
    8325.441/2(-)   E(level): K=37/2 OBLATE M1 BAND?.
Jπ(level): Based on value suggested in (16O,p4nγ) but, in some cases, the evaluator shows the resulting Jπ values in parentheses here.
    8377.4(37/2)   Jπ(level): Based on value suggested in (16O,p4nγ) but, in some cases, the evaluator shows the resulting Jπ values in parentheses here.
    8940(43/2-)   E(level): K=37/2 OBLATE M1 BAND?.
Jπ(level): Based on value suggested in (16O,p4nγ) but, in some cases, the evaluator shows the resulting Jπ values in parentheses here.
    9134.4(41/2-)   Jπ(level): Based on value suggested in (16O,p4nγ) but, in some cases, the evaluator shows the resulting Jπ values in parentheses here.
    9425(45/2+)   Jπ(level): Based on value suggested in (16O,p4nγ) but, in some cases, the evaluator shows the resulting Jπ values in parentheses here.
    9922.4(43/2-)   Jπ(level): Based on value suggested in (16O,p4nγ) but, in some cases, the evaluator shows the resulting Jπ values in parentheses here.
   110595/2+ 13 keV 5  Γp0=4 keV 2.
E(level): From (p,2nγ).
T1/2(level): From Zr(p,p’), (pol p,p) IAR.
   119811/2+ 90 keV 9  E(level): From (p,2nγ).
T1/2(level): From Zr(p,p’), (pol p,p) IAR.
   12171 24 keV Analog of possible 93Zr(1169 level) (1972Ri04).
E(level): Analog of possible 93Zr(1169 level) (1972Ri04).
   125033/2+ 38 keV 3  Γp0=8.0 keV 8.
E(level): From (p,2nγ). γ emitted within 1.3 ps of formation of parent state (2007Wa45).
Jπ(level): From partial wave analysis of analyzing power in 92Zr(pol p,p) IAR.
T1/2(level): From Zr(p,p’), (pol p,p) IAR.
   129931/2+ 42 keV 3  Γp0=10 keV 1.
E(level): From (p,2nγ).
T1/2(level): From Zr(p,p’), (pol p,p) IAR.
   13542 68 keV 5  E(level): From (p,2nγ).
T1/2(level): From Zr(p,p’), (pol p,p) IAR.
   135813/2+ 45 keV 5  E(level): From (p,2nγ). γ emitted within 1.3 ps of formation of parent state (2007Wa45).
Jπ(level): From partial wave analysis of analyzing power in 92Zr(pol p,p) IAR.
T1/2(level): From Zr(p,p’), (pol p,p) IAR.
E(level)Jπ(level)T1/2(level)Comments
   138393/2+ 63 keV 3  Γp0=14.0 keV 14.
E(level): From (p,2nγ). γ emitted within 1.3 ps of formation of parent state (2007Wa45).
Jπ(level): From partial wave analysis of analyzing power in 92Zr(pol p,p) IAR.
T1/2(level): From Zr(p,p’), (pol p,p) IAR.
   14091 30 keV 3  E(level): From (p,2nγ).
T1/2(level): From Zr(p,p’), (pol p,p) IAR.
   143635/2+ 51 keV 5  Γp0|<2.0 keV.
E(level): From (p,2nγ). γ emitted within 1.3 ps of formation of parent state (2007Wa45).
Jπ(level): From partial wave analysis of analyzing power in 92Zr(pol p,p) IAR.
T1/2(level): From Zr(p,p’), (pol p,p) IAR.
   144777/2- 43 keV 7  Γp0=2.0 keV 3.
E(level): From (p,2nγ).
T1/2(level): From Zr(p,p’), (pol p,p) IAR.
   16400- 5.05 MeV GDR. Γ from (γ,xn).
E(level): GDR. Γ from (γ,xn).

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Additional Gamma Comments:

E(level)E(gamma)Comments
      30.77      30.77E(γ): from IT decay
M(γ): from α(K)exp and subshell ratios in IT decay.
     686.79     655.9E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
M(γ): D+Q from (α,pγ); Δπ=no from level scheme.
     743.95     744.06E(γ): weighted average of 743.82 17 from (n,n’γ), 743.92 16 from from Coulomb excitation and 744.2 1 from (p,2nγ).
M(γ): from γ(θ) in Coulomb excitation and RUL.
     808.82      64.88E(γ): weighted average of 65.0 2 from (p,2nγ) and 64.6 3 from Coulomb excitation.
I(γ): from Coulomb excitation. Other: <1.0 from (p,2nγ).
M(γ): d from RUL; Δπ=no from level scheme.
     808.53E(γ): weighted average of 808.42 22 from (n,n’γ) and 808.58 15 from Coulomb excitation.
I(γ): from Coulomb excitation.
M(γ): Q from (16O,p2nγ); not M2 from RUL.
     810.32     123.3E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
     949.80     949.81E(γ): from ε decay (6.85 h).
M(γ): Q from (16O,p2nγ); not M2 from RUL.
     978.91     978.94E(γ): weighted average of 978.83 22 from (n,n’γ) and 979.01 18 from Coulomb excitation. Other Eγ: 979.3 1 from (p,2nγ).
M(γ): D+Q from γ(θ) in Coulomb excitation; not E1+M2 from RUL.
    1082.68     103.80E(γ): weighted average of 103.7 2 from (p,2nγ), 103.94 15 from (n,n’γ) and 103.5 3 from Coulomb excitation.
I(γ): unweighted average of 10.9 9 from Coulomb excitation, 3 2 from (p,2nγ) and 14.4 24 from (n,n’γ). The weighted average from (n,n’γ) and Coulomb excitation is 10.1 22.
     338.73E(γ): weighted average of 338.67 17 from (n,n’γ), 338.77 9 from Coulomb excitation and 338.6 2 from (p,2nγ).
I(γ): weighted average from (p,2nγ) and Coulomb excitation.
M(γ): D+Q from (p,2nγ); Δπ=no from level scheme.
    1082.53E(γ): weighted average of 1082.3 3 from (n,n’γ), 1082.6 3 from Coulomb excitation and 1082.6 2 from (p,2nγ).
I(γ): unweighted average of 29 4, 30.9 15 and 40.0 23 from Coulomb excitation, 38 2 from (p,2nγ). Others: 51.5 15, 37, 33, and 18 6 from (n,n’γ). The weighted average of all data is 39 4.
M(γ): d(+Q) from (n,n’γ); not E1+M2 from RUL.
    1127.09     318.3E(γ): from (p,2nγ). 318.27 17 from (n,n’γ) for triplet, 318.16 20 from Coulomb excitation for doublet.
    1284.26     473.9E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
     597.3E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
M(γ): D+Q from γγ(θ) in (p,2nγ); Δπ=no from RUL.
    1253.5E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
M(γ): not M2 from RUL.
    1297.22     318.3E(γ): from (p,2nγ). 318.27 17 from (n,n’γ) for triplet, 318.16 20 from Coulomb excitation for doublet.
I(γ): unweighted average of 32.1 19 and 61 3 from Coulomb excitation, 53 2 from (n,n’γ), 31 5 from (p,2nγ). The weighted average is 44 7.
M(γ): d(+Q) from (n,n’γ) and Coulomb excitation; adopted Δπ=no.
     553.10E(γ): weighted average of 553.07 25 from (n,n’γ), 553.3 4 from Coulomb excitation and 553.1 1 from (p,2nγ).
I(γ): weighted average of 49 4 and 57 6 from Coulomb excitation, 51 2 from (n,n’γ), 61 5 from (p,2nγ).
M(γ): d(+Q) from (n,n’γ); adopted Δπ=no.
    1297.38E(γ): weighted average of 1297.2 4 from (n,n’γ), 1297.3 3 from Coulomb excitation and 1297.4 1 from (p,2nγ).
I(γ): weighted average of 100 6 and 100 6 from Coulomb excitation, 100 4 from (n,n’γ), 100 5 from (p,2nγ).
M(γ): D+Q from (p,2nγ); not E1+M2 from RUL.
    1315.50     506.7M(γ): D+Q from γγ(θ) in (p,2nγ); Δπ=no from RUL.
     571.5M(γ): D+Q from (p,2nγ); Δπ=(no) from level scheme.
    1335.04     385.224E(γ): weighted average of 385.22 2, 385.38 9 from ε decay (6.85 h), 385.07 17 from (n,n’γ) and 385.1 2 from (p,2nγ).
M(γ): Q from (16O,p2nγ); not M2 from RUL.
    1369.86     559.4E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
     683.2E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
    1395.42     584.97I(γ): from (p,2nγ).
M(γ): D+Q from γ(θ) in (n,n’γ) and γγ(θ) in (p,2nγ).
     708.6E(γ): From (p,2nγ).
I(γ): from (p,2nγ). However, values of 54 and 43 are reported in (n,n’γ).. From (p,2nγ).
E(level)E(gamma)Comments
    1483.58     400.8E(γ): From (p,2nγ).
I(γ): weighted average of 7 2 from (p,2nγ) and 11 3 from (n,n’γ).. From (p,2nγ).
     674.8E(γ): from (p,2nγ).
I(γ): weighted average of 23.5 12 from (n,n’γ) and 27 2 from (p,2nγ).
    1483.46E(γ): weighted average of 1482.8 4 from (n,n’γ) and 1483.5 1 from (p,2nγ). Other: 1483.8 2 from 2010Or01 in (p,2nγ).
I(γ): weighted average from (n,n’γ) and (p,2nγ).
    1490.99     155.94E(γ): from ε decay (6.85 h).
I(γ): average of 22.3 20 from ε decay (6.85 h), 30.2 21 from 82Se(16O,p4nγ) and 14 2 from (p,2nγ).
     541.29M(γ): D+Q from (p,2nγ); M1 from 82Se(16O,p4nγ).
    1499.94     520.9E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
     689.6E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
M(γ): not M2 from RUL.
     756.1E(γ): from (p,2nγ).
I(γ): weighted average of 8 2 from (p,nγ) and 6.5 12 from (n,n’γ).
    1499.9E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
M(γ): d(+Q) from γ(θ) in (n,n’γ); Δπ=yes from level scheme.
    1571.82     287.4E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
     761.4E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
M(γ): D+Q from (p,2nγ); not E1+M2 from RUL.
     885.1E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
M(γ): D+Q from (p,2nγ); not E1+M2 from RUL.
    1588.06     777.8E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
M(γ): D+Q from γγ(θ) in (p,2nγ); large δ favors Δπ=no.
     901.2E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
M(γ): D+Q from γγ(θ) in (p,2nγ); Δπ=(no) from level scheme.
    1603.44     520.9E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
M(γ): d(+Q) from γγ(θ) in (p,2nγ); Δπ=(no) from level scheme.
     624.4I(γ): weighted average of 33.3 18 from (n,n’γ) and 32 3 from (p,2nγ).
M(γ): from γγ(θ) in (p,2nγ); Δπ=(no) from level scheme.
     653.6M(γ): D+Q from γγ(θ) in (p,2nγ); not E1+M2 from RUL.
     859.5E(γ): from (p,2nγ).
I(γ): unweighted average of 29.8 18 from (n,n’γ) and 22 3 from (p,2nγ).
M(γ): not M2 from RUL.
    1603.5E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
    1665.66     856.9E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
     921.6E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
M(γ): D+Q from (p,2nγ) and (n,n’γ); Δπ=no from RUL.
    1665.7E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
    1679.50     364.1E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
M(γ): from (p,2nγ).
     382.4E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
     870.1E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
     935.7E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
M(γ): from (p,2nγ).
    1679.58E(γ): weighted average of 1679.7 2 from (p,2nγ) and 1679.1 4 from (n,n’γ).
I(γ): weighted average of 38 2 from 1973Va09 in (n,n’γ) and 36 3 from (p,nγ).
E(level)E(gamma)Comments
    1683.36     600.7E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
     704.2E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
M(γ): D+Q from γγ(θ) in (p,2nγ); not E1+M2 from RUL.
     939.3I(γ): weighted average from (n,n’γ) and (p,2nγ).
M(γ): D+Q from γγ(θ) in (p,2nγ); not E1+M2 from RUL.
    1683.2I(γ): weighted average of 58.3 21 (1973Va09) in (n,n’γ) and 54 4 from (p,2nγ).
M(γ): D+Q from (p,2nγ); Δπ=no from level scheme.
    1686.34     707.4E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
M(γ): D+Q from γγ(θ) in (p,2nγ); not E1+M2 from RUL.
     736.5E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
    1686.3E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
M(γ): not M2 from RUL.
    1694.0     950E(γ): order of 744γ and 950γ not known from (n,n’γ).
    1703.51     387.9E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
M(γ): d(+Q) from (p,2nγ); Δπ=no from level scheme.
     894.8E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
M(γ): D+Q from (p,2nγ); Δπ=no from level scheme.
    1772.96     646.0E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
M(γ): M2 and higher-order multipolarity excluded by RUL.
     964.0E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
M(γ): M2 and higher-order multipolarity excluded by RUL.
    1779.27     969.0E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
M(γ): d(+Q) from (p,2nγ); Δπ=(no) from level scheme.
    1092.4E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
M(γ): d(+Q) from (p,2nγ); Δπ=(no) from level scheme.
    1812.34     477.3E(γ): for doubly-placed γ.. From (p,2nγ).
I(γ): From (p,2nγ).
    1840.07    1029.6E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
M(γ): D+Q from (p,2nγ); Δπ=(no) from level scheme.
    1153.4E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
M(γ): D+Q from γγ(θ) in (p,2nγ); not E1+M2 from RUL for either possible value of δ.
    1910.68     613.4E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
M(γ): D+Q from γγ(θ) in (p,2nγ); Δπ=(no) from level scheme.
     828.1E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
M(γ): D+Q from γγ(θ) in (p,2nγ); not E1+M2 from RUL.
    1910.6E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
M(γ): D+Q from γ(θ) in (n,n’γ); not E1+M2 from RUL.
    1915.92     600.4E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
     833.4E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
    1107.2E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
    1172.1E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
    1915.5E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
E(level)E(gamma)Comments
    1947.73    1137.4E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
M(γ): from (p,2nγ).
    1949.72     270.1E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
     866.8E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
     971.1E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
    1140.8E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
M(γ): D+Q from (p,2nγ); Δπ=(no) from level scheme.
    1205.9E(γ): from (p,2nγ).
I(γ): weighted average of 85 6 from (n,n’γ) and 92 5 from (p,2nγ).
    1949.81     266.4E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
     346.4E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
    1949.8E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
    1968.27     365.0E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
     477.3E(γ): for doubly-placed γ.. From (p,2nγ).
I(γ): From (p,2nγ).
    1968.87     282.5E(γ): from (p,2nγ).
I(γ): weighted average of 18 5 from (n,n’γ) and 27 5 from (p,2nγ).
     285.4E(γ): from (p,2nγ).
I(γ): weighted average of 21 6 from (n,n’γ) and 34 5 from (p,2nγ).
     990.0E(γ): From (p,2nγ).
I(γ): note that branching from (n,n’γ) varies widely (34 6 (1973Va09), 127 (1992De08), 48 (1983Av05)).. From (p,2nγ).
M(γ): D+Q from γγ(θ) in (p,2nγ); not E1+M2 from RUL.
    1019.0I(γ): weighted average of 28 3 from (n,n’γ) and 38 5 from (p,2nγ).
M(γ): D+Q from γγ(θ) in (p,2nγ); not E1+M2 from RUL.
    1225.0E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
M(γ): M2 and higher-order multipolarity excluded by RUL.
    1968.9E(γ): from (p,2nγ).
I(γ): weighted average of 100 6 from (n,n’γ) and 100 5 from (p,2nγ).
    1997.12    1186.9E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
M(γ): D+Q from γγ(θ) in (p,2nγ); not E1+M2 from RUL.
    1310.2E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
M(γ): D+Q from γγ(θ) in (n,n’γ); Δπ=no from level scheme.
    2002.52     399.1E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
     502.4E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
     511.5E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
    1023.7E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
    1052.8E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
M(γ): D+Q from γ(θ) in (n,n’γ); large δ favors Δπ=no.
    2012.41     440.4E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
    1325.8E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
M(γ): D+Q from γγ(θ) in (p,2nγ); not E1+M2 from RUL.
E(level)E(gamma)Comments
    2023.91     452.1E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
    1337.1E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
M(γ): D+Q from γγ(θ) in (p,2nγ); not E1+M2 from RUL.
    2099.23     703.8E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
    1288.9E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
    2122.67     639.0E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
    1143.7E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
M(γ): D+Q from γγ(θ) in (p,2nγ); not E1+M2 from RUL.
    1378.9E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
M(γ): D+Q from γγ(θ) in (p,2nγ); not E1+M2 from RUL.
    2122.6E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
M(γ): D+Q from (p,2nγ); Δπ=no from level scheme.
    2126.89     626.9E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
     731.3E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
    1316.61E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
    1383.1E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
    2153.60    2122.8E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
    2162.64     671.7E(γ): from (p,2nγ).
I(γ): weighted average of 25 4 from (p,2nγ) and 22 6 from (n,n’γ).
    1183.7E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
    1212.8E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
    2170.65    1087.6E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
    1192.5E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
    1221.6E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
M(γ): M2 and higher-order multipolarity excluded by RUL.
    1361.1E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
M(γ): M2 and higher-order multipolarity excluded by RUL.
    1426.1E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
    2180.04     689.053M(γ): from (16O,p4nγ).. From γ(θ), DCO ratio and/or linear polarization in 82Se(16O,p4nγ).
    2184.14     849.1E(γ): From (p,2nγ).
I(γ): From (p,2nγ).
    2203.5     808.3E(γ): for doublet in (n,n’γ).
    2310.9     976E(γ): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors.
I(γ): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors.
E(level)E(gamma)Comments
    2506.88    1527.9E(γ): from (p,2nγ).
    2506.9E(γ): from (p,2nγ).
    2832.8     522E(γ): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors.
I(γ): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors.
    1497.6E(γ): from (16O,p2nγ).
I(γ): from (16O,p4nγ).
M(γ): From γ(θ), DCO ratio and/or linear polarization in 82Se(16O,p4nγ).
    3086.0     906E(γ): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors.
I(γ): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors.
M(γ): From γ(θ), DCO ratio and/or linear polarization in 82Se(16O,p4nγ).
    3667.8     835E(γ): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors.
I(γ): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors.
    3674.0     588E(γ): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors.
I(γ): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors.
    3684.8     852E(γ): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors.
I(γ): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors.
    4104.7     420E(γ): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors.
I(γ): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors.
M(γ): From γ(θ), DCO ratio and/or linear polarization in 82Se(16O,p4nγ).
    1271.9E(γ): from (16O,p2nγ).
I(γ): from (16O,p4nγ).
M(γ): From γ(θ), DCO ratio and/or linear polarization in 82Se(16O,p4nγ).
    4403.0     729E(γ): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors.
I(γ): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors.
    4864.6     759.9E(γ): From 80Se(16O,p2nγ). Uncertainty in Eγ unstated by authors.
I(γ): From 80Se(16O,p2nγ). Uncertainty in Eγ unstated by authors.
M(γ): From γ(θ), DCO ratio and/or linear polarization in 82Se(16O,p4nγ).
    5155.1    1481E(γ): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors.
I(γ): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors.
    5904.3    1039.7E(γ): From 80Se(16O,p2nγ). Uncertainty in Eγ unstated by authors.
I(γ): From 80Se(16O,p2nγ). Uncertainty in Eγ unstated by authors.
M(γ): From γ(θ), DCO ratio and/or linear polarization in 82Se(16O,p4nγ).
    6464.3    5516E(γ): Interpreted in (p,2nγ) as symmetric one-phonon state with configuration of (π p1/2-1)#(first 2+ state in 94Mo) (2006Or09).
M(γ): Mult=d (probably M1), from (γ,γ’) E=6465 keV.
    6465E(γ): Interpreted in (p,2nγ) as symmetric one-phonon state with configuration of (π p1/2-1)#(first 2+ state in 94Mo) (2006Or09).
M(γ): Mult=d (probably M1), from (γ,γ’) E=6465 keV.
    7372.3    1468E(γ): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors.
I(γ): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors.
M(γ): From γ(θ), DCO ratio and/or linear polarization in 82Se(16O,p4nγ).
    7435.3    1531E(γ): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors.
I(γ): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors.
M(γ): From γ(θ), DCO ratio and/or linear polarization in 82Se(16O,p4nγ).
    7828.3     393E(γ): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors.. γ emitted within 1.3 ps of formation of parent state (2007Wa45).
I(γ): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors.
M(γ): From γ(θ), DCO ratio and/or linear polarization in 82Se(16O,p4nγ).
    8325.4     497E(γ): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors.. γ emitted within 1.3 ps of formation of parent state (2007Wa45).
I(γ): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors.
M(γ): From γ(θ), DCO ratio and/or linear polarization in 82Se(16O,p4nγ).
    8377.4     942E(γ): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors.
I(γ): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors.
M(γ): From γ(θ), DCO ratio and/or linear polarization in 82Se(16O,p4nγ).
    1005E(γ): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors.
I(γ): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors.
M(γ): From γ(θ), DCO ratio and/or linear polarization in 82Se(16O,p4nγ).
    8940     615E(γ): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors.. γ emitted within 1.3 ps of formation of parent state (2007Wa45).
I(γ): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors.
M(γ): From γ(θ), DCO ratio and/or linear polarization in 82Se(16O,p4nγ).
    9134.4    1699E(γ): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors.
I(γ): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors.
M(γ): From γ(θ), DCO ratio and/or linear polarization in 82Se(16O,p4nγ).
    9425     485E(γ): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors.
I(γ): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors.
M(γ): From γ(θ), DCO ratio and/or linear polarization in 82Se(16O,p4nγ).
E(level)E(gamma)Comments
    9699.4    2264E(γ): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors.
I(γ): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors.
    9782.4    1405E(γ): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors.
I(γ): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors.
    9922.4     223E(γ): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors.
I(γ): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors.
     788E(γ): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors.
I(γ): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors.
M(γ): From γ(θ), DCO ratio and/or linear polarization in 82Se(16O,p4nγ).
   10955.4    1033E(γ): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors.
I(γ): From 82Se(16O,p4nγ); uncertainty in Eγ unstated by authors.

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