ADOPTED LEVELS, GAMMAS for 197Au

Authors: Huang Xiaolong, Zhou Chunmei |  Citation: Nucl. Data Sheets 104, 283 (2005) |  Cutoff date: 1-Jan-2002 

 Full ENSDF file | Adopted Levels (PDF version) 


Q(β-)=-600 keV 4S(n)= 8072 keV 3S(p)= 5783.0 keV 7Q(α)= 972.4 keV 20
Reference: 2012WA38

References:
  A  197Pt β- decay (19.8915 H)  B  197Pt β- decay (95.41 M)
  C  197Au IT decay (7.73 S)  D  197Hg ε decay (64.14 H)
  E  197Hg ε decay (23.8 H)  F  196Pt(3He,d)
  G  197Au(γ,γ):MOSSBAUER  H  197Au(γ,γ’),(E,E’)
  I  197Au(E+,γ),(E+,E+’)  J  197Au(n,n),(n,n’)
  K  197Au(n,n’γ)  L  197Au(pol d,d),(d,d’)
  M  Coulomb Excitation 

General Comments:

Levels: For the interacting boson-fermion model, see 1989Wo04

Levels: For the theoretical investigation of hyperfine interactions and isotope shifts in gold, see 1984Ah07.

Levels: 1978Vi01 proposed rotational bands built on g.s. and 1/2+ first-excited state using Nilsson-particle asymmetric-rotor model. See 1978Mu08 for Nilsson-model interpretation of π=- states

Levels: For comparison with level spectra in 191Au, 193Au, 195Au, see 1974Tj02

Levels: For FCC (face-centered cubic) nuclear model, see 1987Da18 and 1987Co21.

Q-value: Note: Current evaluation has used the following Q record -600 3 8072.4 295782.6 6 967.8 17 2003Au03










E(level)
(keV)		XREFJπ(level) T1/2(level)E(γ)
(keV)		I(γ)M(γ)Final Levels
     0.0ABCDEFGHIJKLM 3/2+ STABLE      
    77.3510 20 ABCDEFG IJKLM 1/2+ 1.91 ns 1      77.351 2 
  100
M1+E2
     0.0
3/2+
   268.788 10 A  D F   JKLM 3/2+ 15.4 ps 13     191.437 10 
   268.78 5 
  100 3 
    6.2 3 
M1+E2
E2(+M1)
    77.3510
     0.0
1/2+
3/2+
   279.00 5  BC EF  IJKLM 5/2+ 18.6 ps 15     201.6 3 
   279.01 5 
    1.50 9 
  100 5 
E2
M1+E2
    77.3510
     0.0
1/2+
3/2+
   409.15 8  BC EF  IJ    11/2- 7.73 s 6 
% IT = 100
   130.2 1 
   409.1 1 
  100 4 
    3.4 11 
E3
M4
   279.00
     0.0
5/2+
3/2+
   502.5 3      F   JK M 5/2+ 1.77 ps +19-12     425.0 5 
   502.6 3 
    2.5 7 
  100 2 
E2
M1+E2
    77.3510
     0.0
1/2+
3/2+
   547.5 3          JKLM 7/2+ 4.61 ps +19-13     268.5
   278.7
   547.5 3 
    5.2 3 
    0.7 2 
  100 5 
M1+E2
[E2]
E2
   279.00
   268.788
     0.0
5/2+
3/2+
3/2+
   583           L         
   736.7 3          JKLM 7/2+ 1.09 ps +13-9     457.7 3 
   468.1 5 
  100 3 
    1.9 12 
M1+E2
E2
   279.00
   268.788
5/2+
3/2+
   855.5 4          JKLM 9/2+ 2.67 ps +25-15     308.0 5 
   576.5 4 
   13 4 
  100 4 
M1+E2
E2
   547.5
   279.00
7/2+
5/2+
   882           L         
   888.11 20      F   JKLM 1/2+      619.4 3 
   810.6 3 
   888.3 5 
   27 4 
  100 8 
    9 3 



   268.788
    77.3510
     0.0
3/2+
1/2+
3/2+
   936.0 3          JKLM (5/2+)      432.5 5 ?
   657.1 5 
   667.1 5 
   858.6 5 
   936.2 5 
   24 5 
   20 4 
   61 6 
   25 6 
  100 9 





   502.5
   279.00
   268.788
    77.3510
     0.0
5/2+
5/2+
3/2+
1/2+
3/2+
   948           L         
  1045.1 3          JK   (5/2+)      766.3 5 
   776.9 5 
  1044.2 5 
  100 16 
   69 12 
   48 21 



   279.00
   268.788
     0.0
5/2+
3/2+
3/2+
E(level)
(keV)		XREFJπ(level) T1/2(level)E(γ)
(keV)		I(γ)M(γ)Final Levels
  1120 10         IJ         691
  1100
 
 


   409.15
     0.0
11/2-
3/2+
  1150.5 3      F   JK   3/2+,5/2+      881.9 5 
  1073.4 5 
  1150.2 5 
  100 19 
   93 23 
   26 23 



   268.788
    77.3510
     0.0
3/2+
1/2+
3/2+
  1217.3 4           KL  (3/2+)     1139.5 5 
  1217.7 5 
   62 21 
  100 24 


    77.3510
     0.0
1/2+
3/2+
  1220.1 7         IJ         811
  1220
 
 


   409.15
     0.0
11/2-
3/2+
  1231.0 8            LM 11/2+ 0.91 ps 1     376
   683
   12
  100
M1,E2
E2
   855.5
   547.5
9/2+
7/2+
  1242.0 4          JK   (1/2+)      973.0 5 
  1242.2 5 
   17 14 
  100 33 


   268.788
     0.0
3/2+
3/2+
  1263           L         
  1370           L         
  1380           L         
  1412 4      F     L  9/2-,11/2-        
  1478           L         
  1488           L         
  1584           L         
  1708 4      F        3/2+,5/2+        
  1809           L         
  1820           L         
  1905           L         
  1997 4      F        5/2-,7/2-        
  2149 4      F        5/2-,7/2-        
  2251     F     L  5/2-,7/2-        
  2371           L         
  2405 15        H      +        
  2420 7      F        5/2-,7/2-        
E(level)
(keV)		XREFJπ(level) T1/2(level)E(γ)
(keV)		I(γ)M(γ)Final Levels
  2523 7      F        5/2-,7/2-        
  2620 15        H      +        
  2631 7      F        (5/2-,7/2-)        
  2650           L         
  2776 4      F        11/2+,13/2+        
  2880 15        H      +        
  3025 15        H      +        
  3175 15        H      -        
  3260 15        H      +        
  3515 15        H      +        

E(level): For the states connecting γ rays, E(levels) are from adopted scheme and adopted γ radiations using least-squares fit to data.

E(γ): From 197Au(n,n’γ), except where noted otherwise

I(γ): Relative photon branching from each level. Data are from (n,n’γ), except as noted.

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Additional Gamma Data:















E(level)
(keV)		Jπ(level)T1/2(level)E(γ)
(keV)		MultipolarityMixing
Ratio		Conversion
Coefficient		Additional Data
    77.3510 1/2+ 1.91 ns 1      77.351 2 M1+E2-0.368 144.36B(E2)(W.u.)=35 3, B(M1)(W.u.)=0.00409 16, α=4.36 14
   268.788 3/2+ 15.4 ps 13     191.437 10 M1+E20.14 11.174B(E2)(W.u.)=18 3, B(M1)(W.u.)=0.089 9, α=1.174 2
3/2+ 15.4 ps 13     268.78 5 E2(+M1)3.4 GT0.147B(E2)(W.u.)>18.5 19, B(M1)(W.u.)<0.00018, α=0.147 3
   279.00 5/2+ 18.6 ps 15     201.6 3 E2 0.37B(E2)(W.u.)=14.4 17, α=0.37
5/2+ 18.6 ps 15     279.01 5 M1+E2-0.40 40.380B(E2)(W.u.)=26 6, B(M1)(W.u.)=0.034 4, α=0.380 7
   409.15 11/2- 7.73 s 6 
% IT = 100
   130.2 1 E3 30.3B(E3)(W.u.)=0.003 +41-10, α=30.3
11/2- 7.73 s 6 
% IT = 100
   409.1 1 M4 3.97B(M4)(W.u.)=2.4 8, α=3.97
   502.5 5/2+ 1.77 ps +19-12     425.0 5 E2 0.0392B(E2)(W.u.)=7.6 23, α=0.0392
5/2+ 1.77 ps +19-12     502.6 3 M1+E2-0.24 90.084B(E2)(W.u.)=7 6, B(M1)(W.u.)=0.083 10, α=0.084 3
   547.5 7/2+ 4.61 ps +19-13     268.5M1+E2+0.055 100.465B(E2)(W.u.)=0.18 7, B(M1)(W.u.)=0.0116 10, α=0.465
7/2+ 4.61 ps +19-13     278.7[E2] 0.13B(E2)(W.u.)=6.8 20, α=0.13
7/2+ 4.61 ps +19-13     547.5 3 E2 0.021B(E2)(W.u.)=33 3, α=0.021
   736.7 7/2+ 1.09 ps +13-9     457.7 3 M1+E2-0.26 30.106B(E2)(W.u.)=21 6, B(M1)(W.u.)=0.175 23, α=0.106 1
7/2+ 1.09 ps +13-9     468.1 5 E2 0.031B(E2)(W.u.)=6 4, α=0.031
   855.5 9/2+ 2.67 ps +25-15     308.0 5 M1+E2-.30 90.30B(E2)(W.u.)=10 7, B(M1)(W.u.)=0.028 10, α=0.30 1
9/2+ 2.67 ps +25-15     576.5 4 E2 0.0186B(E2)(W.u.)=41 5, α=0.0186
  1231.0 11/2+ 0.91 ps 1     376M1,E2 0.120B(E2)(W.u.)=64 6, B(M1)(W.u.)=0.0238 21, α=0.120 67
11/2+ 0.91 ps 1     683E2 0.0127B(E2)(W.u.)=53.6 8, α=0.0127

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Additional Level Data and Comments:

E(level)Jπ(level)T1/2(level)Comments
     0.03/2+ STABLE <β22>1/2=(-)0.11 (1989Wa11).
    77.35101/2+ 1.91 ns 1  μ=+0.420 3 (197Au standard,2001StZZ,1989Ra17,1968Co17).
   279.005/2+ 18.6 ps 15  μ=+0.53 5 (2001StZZ,1989Ra17,1986Ba19)
Jπ(level): From angular correlations of deexcitation γ rays in Coul. ex.
   409.1511/2- 7.73 s 6 
% IT = 100
μ=(+)5.98 (2001StZZ,1989Ra17,1983Ha48,1984Ha12), Q=+1.68 5 (2001StZZ,1996Se06)
See 1974Tj02 for ΔJ=2 bands of 191Au, 193Au, 195Au up to J=23/2 based on decoupled h11/2 proton state.
   502.55/2+ 1.77 ps +19-12  μ=+3.0 5 (2001StZZ,1989Ra17,1988St16,1988St09)
Jπ(level): From angular correlations of deexcitation γ rays in Coul. ex.
T1/2(level): From Doppler-broadened lineshape technique (1988St16) in Coul. ex.
   547.57/2+ 4.61 ps +19-13  μ=+0.84 8 (2001StZZ,1989Ra17,1988St16,1988St09) (from g=+0.241 21 in Coul. ex.), +0.52 7 (1989Ra17,1986Ba19) (from g=+0.15 2 in Coul. ex.), +0.53 7 (2001StZZ).
Jπ(level): From angular correlations of deexcitation γ rays in Coul. ex.
T1/2(level): From Doppler-broadened lineshape technique (1988St16) in Coul. ex.
   736.77/2+ 1.09 ps +13-9  μ=+1.7 5 (2001StZZ,1989Ra17,1988St16,1988St09)
Jπ(level): From angular correlations of deexcitation γ rays in Coul. ex.
T1/2(level): From Doppler-broadened lineshape technique (1988St16) in Coul. ex.
   855.59/2+ 2.67 ps +25-15  μ=+1.5 6 (2001StZZ,1989Ra17,1988St16,1988St09)
Jπ(level): From angular correlations of deexcitation γ rays in Coul. ex.
T1/2(level): From Doppler-broadened lineshape technique (1988St16) in Coul. ex.
   936.0(5/2+)   Jπ(level): Tentative 5/2+ assignment (1971Ba29) from (n,n’),(n,n’γ) based on observed γ decay, Hauser-Feshbach calculations.
  1045.1(5/2+)   Jπ(level): Tentative 5/2+ assignment (1971Ba29) from (n,n’),(n,n’γ) based on observed γ decay, Hauser-Feshbach calculations.
  1231.011/2+ 0.91 ps 1  μ=+2.0 10 (2001StZZ,1989Ra17,1988St16,1988St09)
E(level): From Coulomb excitation and Mossbauer studies. ΔE not given by authors.
Jπ(level): From angular correlations of deexcitation γ rays in Coul. ex.
T1/2(level): From Doppler-broadened lineshape technique (1988St16) in Coul. ex.
  14129/2-,11/2-   XREF: L(1405).
  19975/2-,7/2-   Jπ(level): L=3 in 196Pt(3He,d).
  21495/2-,7/2-   Jπ(level): L=3 in 196Pt(3He,d).
  22515/2-,7/2-   Jπ(level): L=3 in 196Pt(3He,d).
  2405+   Jπ(level): From excitation character in (γ,γ’),(e,e’).
  24205/2-,7/2-   Jπ(level): L=3 in 196Pt(3He,d).
  25235/2-,7/2-   Jπ(level): L=3 in 196Pt(3He,d).
  2620+   Jπ(level): From excitation character in (γ,γ’),(e,e’).
  277611/2+,13/2+   L=6 in 196Pt(3He,d).
  2880+   Jπ(level): From excitation character in (γ,γ’),(e,e’).
  3025+   Jπ(level): From excitation character in (γ,γ’),(e,e’).
  3175-   Jπ(level): From excitation character in (γ,γ’),(e,e’).
  3260+   Jπ(level): From excitation character in (γ,γ’),(e,e’).
  3515+   Jπ(level): From excitation character in (γ,γ’),(e,e’).

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Additional Gamma Comments:

E(level)E(gamma)Comments
    77.3510    77.351E(γ): From 197Hg ε decay (64.14 h)
   268.788   191.437E(γ): From 197Pt β- decay (19.8915 h)
I(γ): From 197Hg ε decay (64.14 h)
   268.78E(γ): From 197Pt β- decay (19.8915 h)
I(γ): From 197Hg ε decay (64.14 h)
   279.00   201.6I(γ): From Coul. ex.
   279.01I(γ): From Coul. ex.
   409.15   130.2E(γ): From 197Hg ε decay (23.8 h)
I(γ): From 197Hg ε decay (23.8 h)
M(γ): From 197Hg ε decay (23.8 h)
   409.1E(γ): From 197Hg ε decay (23.8 h)
I(γ): From 197Hg ε decay (23.8 h)
M(γ): From 197Hg ε decay (23.8 h)
   502.5   425.0E(γ): From Coulomb excitation and Mossbauer studies. From Coulomb excitation and Mossbauer studies. ΔE not given by authors.
M(γ): From mult=d,E2 (from RULER program on the basis of given T1/2 and branching) and ΔJ and Δπ between transition levels
   547.5   268.5E(γ): From Coulomb excitation and Mossbauer studies
I(γ): From Coul. ex.
   278.7E(γ): From Coulomb excitation and Mossbauer studies
I(γ): From Coul. ex.
   547.5E(γ): From Coulomb excitation and Mossbauer studies
I(γ): From Coul. ex.
   736.7   457.7E(γ): From Coulomb excitation and Mossbauer studies
   468.1E(γ): From Coulomb excitation and Mossbauer studies. ΔE not given by authors.
M(γ): From mult=d,E2 (from RULER program on the basis of given T1/2 and branching) and ΔJ and Δπ between transition levels
   855.5   308.0I(γ): from Iγ(308γ)/Iγ(577γ)=14/86 (1988St16) and Iγ(308γ)/Iγ(577γ)=8/92 (1981Ve12).
   576.5I(γ): see 308γ notes.
   888.11   619.4E(γ): From Coulomb excitation and Mossbauer studies
I(γ): From Coul. ex.
   810.6E(γ): From Coulomb excitation and Mossbauer studies
I(γ): From Coul. ex.
  1120   691E(γ): From 197Au(e+,γ),(e+,e+’)
  1100E(γ): From 197Au(e+,γ),(e+,e+’)
  1220.1   811E(γ): From 197Au(e+,γ),(e+,e+’)
  1220E(γ): From 197Au(e+,γ),(e+,e+’)
  1231.0   376E(γ): From Coulomb excitation and Mossbauer studies. From Coulomb excitation and Mossbauer studies. ΔE not given by authors.
I(γ): from Iγ(376γ)/Iγ(683γ)=11/89 (1981Ve12) in Coul. ex.. From 197Hg ε decay (64.14 h)
M(γ): From mult=d,E2 (from RULER program on the basis of given T1/2 and branching) and ΔJ and Δπ between transition levels
   683E(γ): From Coulomb excitation and Mossbauer studies

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