ADOPTED LEVELS, GAMMAS for 199Hg

Author: Balraj Singh |  Citation: Nucl. Data Sheets 108, 79 (2007) |  Cutoff date: 15-Oct-2006 

 Full ENSDF file | Adopted Levels (PDF version) 


Q(β-)=-1.49×103 keV 3S(n)= 6662.9 keV 6S(p)= 7253.4 keV 7Q(α)= 825.0 keV 10
Reference: 2012WA38

References:
  A  199Au β- decay (3.139 d)  B  199Hg IT decay (42.67 M)
  C  muonic atom  D  199Tl ε decay (7.42 H)
  E  198Pt(α,3nγ)  F  198Hg(n,γ) E=23.1 EV
  G  198Hg(n,γ) E=89.9 EV  H  198Hg(d,p)
  I  199Hg(γ,γ):MOSSBAUER  J  199Hg(γ,γ’)
  K  199Hg(E,E’)  L  199Hg(n,n’γ)
  M  Coulomb Excitation  N  200Hg(p,d)
  O  200Hg(d,t) 

General Comments:

Nuclear structure calculations:

Particle-core coupling: 1983Gu02, 1979St04

Supersymmetries: 2004Jo11 (1/2-,3/2-,5/2- states interpreted below 500 keV), 1984Va36, 1983Su03

Asymmetric rotor: 1979Wu12 (asymmetric rotor)

Intermediate coupling: 1975Ma05

Schiff moments calculations: 2005Dm02, 2005De51.

RMS charge radius and deformation: 1986Ul02, 1974Pr09

L1 subshell fluorescent yield: 1985Ma50

Electric dipole moment: 1987La22. The null result, 0.7×10-26 15 e cm, improves by an order of magnitude the limits on several possible interactions which violate time-reversal symmetry.

2005Os02: electric quadrupole moment measurement of 199Hg+ 5d96s2 2D5/2 atomic state.

Mass measurement: 2003Ba49

Other reactions:

201Hg(p,t) E=25 MeV: 1988BeZT: measured σ(θ); DWBA analysis with DWUCK. Observed splitting of L=0 strength. No details available

For neutron resonances (total of 73 from 23 eV to 12 keV) see 198Hg(n,γ):resonances dataset

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










E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
     0.0ABCDEFGHIJKLMNO 1/2- STABLE      
   158.37859 10 ABCDEFGHI  LMNO 5/2- 2.45 ns 3     158.37851 10 
    100
E2
     0.0
1/2-
   208.20494 10 A CD FGHI  LMNO 3/2- 69 ps 3      49.82635 12 
   208.20481 12 
      4.13 11 
    100.0 13 
M1+E2
M1+E2
   158.37859
     0.0
5/2-
1/2-
   403.51 3    D FGH    MNO 3/2- 5.8 ps 12     195.30 5 
   245.1 10 
   403.50 4 
     15 2 
     ≤2.2
    100 5 
M1
[M1,E2]
M1+E2
   208.20494
   158.37859
     0.0
3/2-
5/2-
1/2-
   413.84 5  B D FG     MNO 5/2- 115 ps 23      10.4 2 S
   205.6 1 
   255.5 1 
   413.85 8 
 
      5 2 
      6 2 
    100 13 
[M1,E2]
[M1,E2]
[M1,E2]
E2
   403.51
   208.20494
   158.37859
     0.0
3/2-
3/2-
5/2-
1/2-
   455.462 17    D FG    L NO 1/2-,3/2-       51.93 6 
   247.26 3 
   297.07 6 
   455.46 3 
      0.19 6 
     75 4 
      2.8 3 
    100 5 
(M1)
M1
(E2)
M1
   403.51
   208.20494
   158.37859
     0.0
3/2-
3/2-
5/2-
1/2-
   492.297 18    D FG      NO 3/2-       36.83 3 
   284.09 3 
   333.93 4 
   492.30 4 
      0.51 11 
    100 5 
     80 4 
     69 3 
M1
M1
M1+E2
M1
   455.462
   208.20494
   158.37859
     0.0
1/2-,3/2-
3/2-
5/2-
1/2-
   532.48 10  B  E        NO 13/2+ 42.67 m 9 
% IT = 100
   118.6S
   374.1 1 
     ≈8E-5
    100 8 
[M4]
M4+E5
   413.84
   158.37859
5/2-
5/2-
   638 3            L NO        
   667 3        H     NO 5/2-,7/2-        
   667.4 9      FG      N  1/2,3/2        
   695 3 ?     FG                
   699 3        H     NO 5/2-,7/2-        
   711.4 25 ?     FG                
   736 5      FG         1/2,3/2,5/2+        
   750.40 3    D FG      NO 1/2-,3/2-      258.14 11 
   294.94 10 
   336.5 1 
   346.89 8 
   542.21 5 
   592.0 1 
   750.4 1 
      6.9 7 
      5.0 5 
     13.6 13 
     12.7 13 
     25 2 
     10 4 
    100 5 
[M1,E2]
[M1,E2]
[M1,E2]
[M1,E2]
[M1,E2]
[M1,E2]
[M1,E2]
   492.297
   455.462
   413.84
   403.51
   208.20494
   158.37859
     0.0
3/2-
1/2-,3/2-
5/2-
3/2-
3/2-
5/2-
1/2-
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   759 3        H               
   822 4               O        
   823.88 23     E           (17/2+)      291.4 2 
    100
(E2)
   532.48
13/2+
   969 4            L NO 7/2-,5/2-        
  1004.1 7 ?     FG  J L           
  1036 3      FG         1/2,3/2,5/2+        
  1104 4               O        
  1221.17 4    D FGH     NO 1/2(-),3/2(-)      470.77 13 
   728.86 11 
   765.7 2 
   807.3 1 
   817.67 10 
  1012.95 10 
  1062.8 1 
  1221.16 10 
      2.2 4 
      2.5 3 
     ≈0.7
      2.8 3 
     23.2 14 
    100 5 
     14.1 14 
      1.7 2 
[M1,E2]
[M1,E2]
[M1,E2]
[M1,E2]
[M1,E2]
[M1,E2]
[M1,E2]
[M1,E2]
   750.40
   492.297
   455.462
   413.84
   403.51
   208.20494
   158.37859
     0.0
1/2-,3/2-
3/2-
1/2-,3/2-
5/2-
3/2-
3/2-
5/2-
1/2-
  1267.7 8      FG    L    1/2,3/2,5/2+        
  1274.1 4 ?    E           (15/2+)      741.6 2 
    100
M1+E2
   532.48
13/2+
  1317.7 15      FG         1/2,3/2,5/2+        
  1327.8 9      FGH J    O 1/2-,3/2-        
  1357.2 3     E           (21/2+)      533.3 2 
    100
(E2)
   823.88
(17/2+)
  1358.9 9      FG  J    O 1/2,3/2        
  1439.5 16      FG  J    O 1/2-,3/2-        
  1456 6        H      O (7/2-,5/2-)        
  1517.8 25      FG  JK     1/2,3/2        
  1561 6 ?              O        
  1572.8 12      FG         1/2,3/2        
  1595.3 5      FG   K   O 1/2,3/2        
  1614.4 9 ?     FG   K            
  1653.2 8      FGH      O 1/2(-),3/2(-)        
  1686 7               O        
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
  1731.8 7      FG  J      1/2,3/2        
  1744.2 5      FG         1/2,3/2        
  1769.3 3     E           (19/2+)      945.4 2 
    100
(M1+E2)
   823.88
(17/2+)
  1780.9 5      FG       O 1/2,3/2        
  1800.1 12      FG         1/2,3/2,5/2+        
  1822.2 16      FG    L    1/2,3/2        
  1853 7            L  O        
  1927.3 15 ?     FG                
  1953 8               O        
  1971.4 5      FG         1/2,3/2        
  1988.3 20      FG         1/2,3/2        
  2038 8               O        
  2067 3      FG         1/2,3/2,5/2+        
  2094.0 12      FG       O 1/2,3/2        
  2107.3 4     E           (25/2+)      749.9 2 
    100
(E2)
  1357.2
(21/2+)
  2144.3 16      FG         1/2,3/2,5/2+        
  2175 9               O        
  2218 9               O        
  2228.4 11      FG       O 1/2,3/2        
  2241 4      FG         1/2,3/2        
  2265 3      FG         1/2,3/2        
  2279 9               O        
  2290.6 10      FG         1/2,3/2        
  2332.0 4     E           (21/2-)      974.8 2 
    100
(E1)
  1357.2
(21/2+)
  2345.3 12      FG       O 1/2,3/2        
  2399 3      FGH      O 1/2,3/2,5/2+        
  2412 3      FGH      O 1/2,3/2,5/2+        
  2425.6 4     E           (23/2-)     1068.6 2 
    100
(E1)
  1357.2
(21/2+)
  2451.4 15      FG         1/2,3/2,5/2+        
  2462.1 25      FGH        1/2,3/2        
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
  2487.8 4     E           (25/2-)      155.8 5 
   380.5 2 
    ≈10
    100 24 

E1
  2332.0
  2107.3
(21/2-)
(25/2+)
  2494 3      FG         1/2,3/2        
  2521 10 ?              O        
  2629.7 4     E           (27/2-)      141.6
   204.3 2 
   522.3 2 
    <40
     20 4 
    100 20 



  2487.8
  2425.6
  2107.3
(25/2-)
(23/2-)
(25/2+)
  2765.9 5     E           (29/2-)      278.1 2 
    100
(Q)
  2487.8
(25/2-)
  3068.4 5     E           (31/2-)      438.7 2 
    100
(Q)
  2629.7
(27/2-)
  3133 13 ?       H               
  3199 13        H               
  3245 13        H               
  3273 13        H               
  3338 13        H               
  3413 14        H               
  3431 14        H               
  3511 14        H               
  3582 14        H               
  3604 14        H               
  3626 15        H               
  3648 15        H               
  3930 16 ?       H               
  3988 16        H               
  4052 16        H               
  4098 16        H               
  4491 18 ?       H               
  4808 19 ?       H               

E(level): From least squares adjustment to adopted Eγ’s where possible; from Eγ of primary γ’s for levels seen in (n,γ) reactions only; and from (d,p), (d,t) or (p,d) for levels seen only in particle reactions.

Jπ(level): Low-lying states are expected to have negative parity based on neutron hole in 3p1/2, 2f5/2, 3p3/2 coupled to 2+ core vibrations. The lowest high spin states have positive parity based on neutron hole in 1i13/2.

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Band Transitions:

E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 1 - DECOUPLED band BUILT ON νi13/2.
   532.48 10  13/2+ 42.67 m 9 
% IT = 100
     
   823.88 23  (17/2+)      291.4 2 
    100
(E2)
   532.48
13/2+
  1357.2 3  (21/2+)      533.3 2 
    100
(E2)
   823.88
(17/2+)
  2107.3 4  (25/2+)      749.9 2 
    100
(E2)
  1357.2
(21/2+)
E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 2 - νi13/2-1~#(5-,7-,9-,..198Hg core) (?)
  2332.0 4  (21/2-)        
  2425.6 4  (23/2-)     1068.6 2 
    100
(E1)
  1357.2
(21/2+)
  2487.8 4  (25/2-)      155.8 5 
   380.5 2 
    ≈10
    100 24 

E1
  2332.0
  2107.3
(21/2-)
(25/2+)
  2629.7 4  (27/2-)      141.6
   204.3 2 
   522.3 2 
    <40
     20 4 
    100 20 



  2487.8
  2425.6
  2107.3
(25/2-)
(23/2-)
(25/2+)
  2765.9 5  (29/2-)      278.1 2 
    100
(Q)
  2487.8
(25/2-)
  3068.4 5  (31/2-)      438.7 2 
    100
(Q)
  2629.7
(27/2-)
E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 3 - UNFAVORED band BUILT ON νi13/2
  1274.1 4  (15/2+)        
  1769.3 3  (19/2+)      945.4 2 
    100
(M1+E2)
   823.88
(17/2+)

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Additional Gamma Data:















E(level)
(keV)
Jπ(level)T1/2(level)E(γ)
(keV)
MultipolarityMixing
Ratio
Conversion
Coefficient
Additional Data
   158.37859 5/2- 2.45 ns 3     158.37851 10 E2 0.914B(E2)(W.u.)=17.6 3, α=0.914, α(K)=0.296, α(L)=0.461, α(M)=0.119, α(N+)=0.0374
   208.20494 3/2- 69 ps 3      49.82635 12 M1+E2-0.044 411.7B(E2)(W.u.)=12.5 25, B(M1)(W.u.)=0.043 4, α=11.7, α(L)=8.92 4, α(M)=2.08 1
3/2- 69 ps 3     208.20481 12 M1+E2-0.388 90.937B(E2)(W.u.)=16.1 11, B(M1)(W.u.)=0.0125 7, α=0.937, α(K)=0.751 4, α(L)=0.142, α(M)=0.0334 2, α(N+)=0.0106
   403.51 3/2- 5.8 ps 12     195.30 5 M1 1.23B(M1)(W.u.)=0.051 13, α=1.23, α(K)=1.007, α(L)=0.170, α(M)=0.0394, α(N+)=0.0126
3/2- 5.8 ps 12     245.1 10 [M1,E2] 0.43α=0.43 23
3/2- 5.8 ps 12     403.50 4 M1+E2+0.32 20.157B(E2)(W.u.)=8.1 20, B(M1)(W.u.)=0.035 8, α=0.157, α(K)=0.129 1, α(L)=0.0219 2, α(M)=0.00510 3, α(N+)=0.00162
   413.84 5/2- 115 ps 23     205.6 1 [M1,E2] 0.7α=0.7 4
5/2- 115 ps 23     255.5 1 [M1,E2] 0.38α=0.38 20
5/2- 115 ps 23     413.85 8 E2 0.0437B(E2)(W.u.)=4.8 10, α=0.0437, α(K)=0.0298, α(L)=0.0105, α(M)=0.00261, α(N+)=0.00082
   455.462 1/2-,3/2-       51.93 6 (M1) 10.1α=10.1, α(L)=7.74, α(M)=1.80, α(N+)=0.579
1/2-,3/2-      247.26 3 M1 0.637α=0.637, α(K)=0.523, α(L)=0.0877, α(M)=0.0204, α(N+)=0.00650
1/2-,3/2-      297.07 6 (E2) 0.111α=0.111, α(K)=0.0651, α(L)=0.0343, α(M)=0.00870, α(N+)=0.00272
1/2-,3/2-      455.46 3 M1 0.122α=0.122, α(K)=0.1004, α(L)=0.0166, α(M)=0.00385, α(N+)=0.00123
   492.297 3/2-       36.83 3 M1 27.9α=27.9, α(L)=21.31, α(M)=4.97
3/2-      284.09 3 M1 0.435α=0.435, α(K)=0.357, α(L)=0.597, α(M)=0.0139, α(N+)=0.00442
3/2-      333.93 4 M1+E2+0.22 20.271α=0.271, α(K)=0.222 2, α(L)=0.376 1, α(M)=0.00875 3, α(N+)=0.00279
3/2-      492.30 4 M1 0.0994α=0.0994, α(K)=0.0818, α(L)=0.0135, α(M)=0.00313, α(N+)=0.00100
   532.48 13/2+ 42.67 m 9 
% IT = 100
   118.6[M4] 2310α=2310, α(K)=175, α(L)=1523, α(M)=499, α(N+)=174
13/2+ 42.67 m 9 
% IT = 100
   374.1 1 M4+E5+0.092 156.0B(E5)(W.u.)=143 25, B(M4)(W.u.)=2.01 5, α=6.0, α(K)=3.55, α(L)=1.95, α(M)=0.527, α(N+)=0.171
   750.40 1/2-,3/2-      258.14 11 [M1,E2] 0.37α=0.37 20
1/2-,3/2-      294.94 10 [M1,E2] 0.25α=0.25 14
1/2-,3/2-      336.5 1 [M1,E2] 0.18α=0.18 10
1/2-,3/2-      346.89 8 [M1,E2] 0.16α=0.16 9
1/2-,3/2-      542.21 5 [M1,E2] 0.05α=0.05 3
1/2-,3/2-      592.0 1 [M1,E2] 0.040α=0.040 22
1/2-,3/2-      750.4 1 [M1,E2] 0.022α=0.022 11
E(level)
(keV)
Jπ(level)T1/2(level)E(γ)
(keV)
MultipolarityMixing
Ratio
Conversion
Coefficient
Additional Data
   823.88 (17/2+)      291.4 2 (E2) 0.117α=0.117, α(K)=0.0682, α(L)=0.0369, α(M)=0.00937, α(N+)=0.00293
  1221.17 1/2(-),3/2(-)      470.77 13 [M1,E2] 0.07α=0.07 4
1/2(-),3/2(-)      728.86 11 [M1,E2] 0.024α=0.024 12
1/2(-),3/2(-)      765.7 2 [M1,E2] 0.021α=0.021 11
1/2(-),3/2(-)      807.3 1 [M1,E2] 0.019α=0.019 9
1/2(-),3/2(-)      817.67 10 [M1,E2] 0.018α=0.018 9
1/2(-),3/2(-)     1012.95 10 [M1,E2] 0.011α=0.011 5
1/2(-),3/2(-)     1062.8 1 [M1,E2] 0.010α=0.010 4
1/2(-),3/2(-)     1221.16 10 [M1,E2] 0.007α=0.007 3
  1274.1 (15/2+)      741.6 2 M1+E2-1.3 50.020α=0.020 6, α(K)=0.016 5, α(L)=0.0029 7
  1769.3 (19/2+)      945.4 2 (M1+E2) 0.013α=0.013 6
  2107.3 (25/2+)      749.9 2 (E2) 0.0109α=0.0109, α(K)=0.00849, α(L)=0.00183
  2487.8 (25/2-)      380.5 2 E1 0.0161α=0.0161, α(K)=0.0133, α(L)=0.00215, α(M)=0.00050, α(N+)=0.00016

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Additional Level Data and Comments:

E(level)Jπ(level)T1/2(level)Comments
     0.01/2- STABLE μ=+0.5058855 9 (1989Ra17,1961Ca21)
Electric dipole moment (d)<2.1×10-28 e cm (2001Ro05).
E(level): Electric dipole moment (d)<2.1×10-28 e cm (2001Ro05).
   158.378595/2- 2.45 ns 3  μ=+0.88 3 (1989Ra17,1977Kr11), Q=+0.95 7 (1989Ra17,1979Ha08)
Isomer shift (1985La21,1983Gu02).
   455.4621/2-,3/2-   XREF: L(?).
   532.4813/2+ 42.67 m 9 
% IT = 100
μ=-1.014703 3 (1989Ra17,1973Re04), Q=+1.2 5 (1989Ra17,1986Ul02)
Isomer shift (1979St04,1985Kl09).
E(level): DECOUPLED band BUILT ON νi13/2.
   638   XREF: L(?).
   667.41/2,3/2   Jπ(level): 1/2,3/2 is from strong population through a primary γ from 1/2+ resonance in (n,γ) (negative parity favored from syst of transition strengths), 1/2,3/2,5/2+ is from weak population from 1/2+ resonance.
   7361/2,3/2,5/2+   XREF: F(?).
Jπ(level): 1/2,3/2 is from strong population through a primary γ from 1/2+ resonance in (n,γ) (negative parity favored from syst of transition strengths), 1/2,3/2,5/2+ is from weak population from 1/2+ resonance.
   823.88(17/2+)   E(level): DECOUPLED band BUILT ON νi13/2. From (α,3nγ).
Jπ(level): From proposed rotational band structure in (α,3nγ).
  1004.1   XREF: J(1000).
  10361/2,3/2,5/2+   XREF: γ(?).
Jπ(level): 1/2,3/2 is from strong population through a primary γ from 1/2+ resonance in (n,γ) (negative parity favored from syst of transition strengths), 1/2,3/2,5/2+ is from weak population from 1/2+ resonance.
  1221.171/2(-),3/2(-)   XREF: γ(?).
  1267.71/2,3/2,5/2+   Jπ(level): 1/2,3/2 is from strong population through a primary γ from 1/2+ resonance in (n,γ) (negative parity favored from syst of transition strengths), 1/2,3/2,5/2+ is from weak population from 1/2+ resonance.
  1274.1(15/2+)   E(level): From 199Hg IT decay. UNFAVORED band BUILT ON νi13/2. From (α,3nγ).
Jπ(level): From proposed rotational band structure in (α,3nγ).
  1317.71/2,3/2,5/2+   XREF: γ(?).
Jπ(level): 1/2,3/2 is from strong population through a primary γ from 1/2+ resonance in (n,γ) (negative parity favored from syst of transition strengths), 1/2,3/2,5/2+ is from weak population from 1/2+ resonance.
  1327.81/2-,3/2-   XREF: J(1340).
  1357.2(21/2+)   E(level): DECOUPLED band BUILT ON νi13/2. From (α,3nγ).
Jπ(level): From proposed rotational band structure in (α,3nγ).
  1358.91/2,3/2   XREF: γ(?)J(1380).
Jπ(level): 1/2,3/2 is from strong population through a primary γ from 1/2+ resonance in (n,γ) (negative parity favored from syst of transition strengths), 1/2,3/2,5/2+ is from weak population from 1/2+ resonance.
  1439.51/2-,3/2-   XREF: J(1420).
  1517.81/2,3/2   XREF: F(?)J(1530)K(1490).
Jπ(level): 1/2,3/2 is from strong population through a primary γ from 1/2+ resonance in (n,γ) (negative parity favored from syst of transition strengths), 1/2,3/2,5/2+ is from weak population from 1/2+ resonance.
  1572.81/2,3/2   Jπ(level): 1/2,3/2 is from strong population through a primary γ from 1/2+ resonance in (n,γ) (negative parity favored from syst of transition strengths), 1/2,3/2,5/2+ is from weak population from 1/2+ resonance.
  1595.31/2,3/2   XREF: γ(?)O(?).
Jπ(level): 1/2,3/2 is from strong population through a primary γ from 1/2+ resonance in (n,γ) (negative parity favored from syst of transition strengths), 1/2,3/2,5/2+ is from weak population from 1/2+ resonance.
  1653.21/2(-),3/2(-)   Jπ(level): 1/2,3/2 is from strong population through a primary γ from 1/2+ resonance in (n,γ) (negative parity favored from syst of transition strengths), 1/2,3/2,5/2+ is from weak population from 1/2+ resonance.
  1731.81/2,3/2   XREF: J(1700).
Jπ(level): 1/2,3/2 is from strong population through a primary γ from 1/2+ resonance in (n,γ) (negative parity favored from syst of transition strengths), 1/2,3/2,5/2+ is from weak population from 1/2+ resonance.
  1744.21/2,3/2   XREF: γ(?).
Jπ(level): 1/2,3/2 is from strong population through a primary γ from 1/2+ resonance in (n,γ) (negative parity favored from syst of transition strengths), 1/2,3/2,5/2+ is from weak population from 1/2+ resonance.
  1769.3(19/2+)   E(level): From 199Hg IT decay. UNFAVORED band BUILT ON νi13/2. From (α,3nγ).
Jπ(level): From proposed rotational band structure in (α,3nγ).
E(level)Jπ(level)T1/2(level)Comments
  1780.91/2,3/2   Jπ(level): 1/2,3/2 is from strong population through a primary γ from 1/2+ resonance in (n,γ) (negative parity favored from syst of transition strengths), 1/2,3/2,5/2+ is from weak population from 1/2+ resonance.
  1800.11/2,3/2,5/2+   XREF: γ(?).
Jπ(level): 1/2,3/2 is from strong population through a primary γ from 1/2+ resonance in (n,γ) (negative parity favored from syst of transition strengths), 1/2,3/2,5/2+ is from weak population from 1/2+ resonance.
  1822.21/2,3/2   Jπ(level): 1/2,3/2 is from strong population through a primary γ from 1/2+ resonance in (n,γ) (negative parity favored from syst of transition strengths), 1/2,3/2,5/2+ is from weak population from 1/2+ resonance.
  1971.41/2,3/2   Jπ(level): 1/2,3/2 is from strong population through a primary γ from 1/2+ resonance in (n,γ) (negative parity favored from syst of transition strengths), 1/2,3/2,5/2+ is from weak population from 1/2+ resonance.
  1988.31/2,3/2   Jπ(level): 1/2,3/2 is from strong population through a primary γ from 1/2+ resonance in (n,γ) (negative parity favored from syst of transition strengths), 1/2,3/2,5/2+ is from weak population from 1/2+ resonance.
  20671/2,3/2,5/2+   XREF: γ(?).
Jπ(level): 1/2,3/2 is from strong population through a primary γ from 1/2+ resonance in (n,γ) (negative parity favored from syst of transition strengths), 1/2,3/2,5/2+ is from weak population from 1/2+ resonance.
  2094.01/2,3/2   XREF: γ(?)O(?).
Jπ(level): 1/2,3/2 is from strong population through a primary γ from 1/2+ resonance in (n,γ) (negative parity favored from syst of transition strengths), 1/2,3/2,5/2+ is from weak population from 1/2+ resonance.
  2107.3(25/2+)   E(level): DECOUPLED band BUILT ON νi13/2. From (α,3nγ).
Jπ(level): From proposed rotational band structure in (α,3nγ).
  2144.31/2,3/2,5/2+   Jπ(level): 1/2,3/2 is from strong population through a primary γ from 1/2+ resonance in (n,γ) (negative parity favored from syst of transition strengths), 1/2,3/2,5/2+ is from weak population from 1/2+ resonance.
  2228.41/2,3/2   XREF: O(?).
Jπ(level): 1/2,3/2 is from strong population through a primary γ from 1/2+ resonance in (n,γ) (negative parity favored from syst of transition strengths), 1/2,3/2,5/2+ is from weak population from 1/2+ resonance.
  22411/2,3/2   XREF: F(?).
Jπ(level): 1/2,3/2 is from strong population through a primary γ from 1/2+ resonance in (n,γ) (negative parity favored from syst of transition strengths), 1/2,3/2,5/2+ is from weak population from 1/2+ resonance.
  22651/2,3/2   Jπ(level): 1/2,3/2 is from strong population through a primary γ from 1/2+ resonance in (n,γ) (negative parity favored from syst of transition strengths), 1/2,3/2,5/2+ is from weak population from 1/2+ resonance.
  2290.61/2,3/2   Jπ(level): 1/2,3/2 is from strong population through a primary γ from 1/2+ resonance in (n,γ) (negative parity favored from syst of transition strengths), 1/2,3/2,5/2+ is from weak population from 1/2+ resonance.
  2332.0(21/2-)   E(level): νi13/2-1~#(5-,7-,9-,..198Hg core) (?). From (α,3nγ).
Jπ(level): From proposed rotational band structure in (α,3nγ).
  2345.31/2,3/2   XREF: γ(?)O(2360).
Jπ(level): 1/2,3/2 is from strong population through a primary γ from 1/2+ resonance in (n,γ) (negative parity favored from syst of transition strengths), 1/2,3/2,5/2+ is from weak population from 1/2+ resonance.
  23991/2,3/2,5/2+   XREF: O(2384).
Jπ(level): 1/2,3/2 is from strong population through a primary γ from 1/2+ resonance in (n,γ) (negative parity favored from syst of transition strengths), 1/2,3/2,5/2+ is from weak population from 1/2+ resonance.
  24121/2,3/2,5/2+   XREF: H(2424)O(?).
Jπ(level): 1/2,3/2 is from strong population through a primary γ from 1/2+ resonance in (n,γ) (negative parity favored from syst of transition strengths), 1/2,3/2,5/2+ is from weak population from 1/2+ resonance.
  2425.6(23/2-)   E(level): νi13/2-1~#(5-,7-,9-,..198Hg core) (?). From (α,3nγ).
Jπ(level): From proposed rotational band structure in (α,3nγ).
  2451.41/2,3/2,5/2+   XREF: F(?).
Jπ(level): 1/2,3/2 is from strong population through a primary γ from 1/2+ resonance in (n,γ) (negative parity favored from syst of transition strengths), 1/2,3/2,5/2+ is from weak population from 1/2+ resonance.
  2462.11/2,3/2   Jπ(level): 1/2,3/2 is from strong population through a primary γ from 1/2+ resonance in (n,γ) (negative parity favored from syst of transition strengths), 1/2,3/2,5/2+ is from weak population from 1/2+ resonance.
  2487.8(25/2-)   E(level): νi13/2-1~#(5-,7-,9-,..198Hg core) (?). From (α,3nγ).
Jπ(level): From proposed rotational band structure in (α,3nγ).
  24941/2,3/2   Jπ(level): 1/2,3/2 is from strong population through a primary γ from 1/2+ resonance in (n,γ) (negative parity favored from syst of transition strengths), 1/2,3/2,5/2+ is from weak population from 1/2+ resonance.
  2629.7(27/2-)   E(level): νi13/2-1~#(5-,7-,9-,..198Hg core) (?). From (α,3nγ).
Jπ(level): From proposed rotational band structure in (α,3nγ).
  2765.9(29/2-)   E(level): νi13/2-1~#(5-,7-,9-,..198Hg core) (?). From (α,3nγ).
Jπ(level): From proposed rotational band structure in (α,3nγ).
  3068.4(31/2-)   E(level): νi13/2-1~#(5-,7-,9-,..198Hg core) (?). From (α,3nγ).
Jπ(level): From proposed rotational band structure in (α,3nγ).

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Additional Gamma Comments:

E(level)E(gamma)Comments
   158.37859   158.37851E(γ): From 199Au β- decay
M(γ): From 199Au β- decay
   208.20494    49.82635E(γ): From 199Au β- decay
I(γ): From 199Au β- decay
M(γ): From 199Au β- decay
   208.20481E(γ): From 199Au β- decay
I(γ): From 199Au β- decay
M(γ): From 199Au β- decay
   413.84   413.85M(γ): from γγ(θ) Coul ex
   532.48   118.6E(γ): From 199Hg IT decay
I(γ): From 199Hg IT decay
   374.1E(γ): From 199Hg IT decay
I(γ): From 199Hg IT decay
   823.88   291.4E(γ): From (α,3nγ)
M(γ): From (α,3nγ)

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