80-Hg-198

MT Reaction 0.0253-eV Maxwellian
Average
g-factor Resonance
Integral
14-MeV Fiss. Spec.
Average
1 (n,total) 14.80 (b) 16.46 (b) 1.112 5.228 (b) 6.620 (b)
2 (n,elastic) 12.81 (b) 14.47 (b) 1.129 2.789 (b) 5.073 (b)
4 (n,inelastic) ( E-thr = 413.9 keV ) 382.4 (mb) 1.513 (b)
16 (n,2n) ( E-thr = 8.343 MeV ) 2.050 (b) 3.239 (mb)
17 (n,3n) ( E-thr = 15.36 MeV ) 1.076 (μb)
22 (n,na) 0.000 (b) 0.000 (b) 10.24 (nb) 6.464 (μb) 3.006 (nb)
28 (n,np) ( E-thr = 7.139 MeV ) 25.71 (μb) 21.64 (nb)
102 (n,γ) 1.986 (b) 1.989 (b) 1.001 74.47 (b) 120.6 (nb) 31.42 (mb)
103 (n,p) ( E-thr = 593.5 keV ) 4.129 (mb) 2.558 (μb)
104 (n,d) ( E-thr = 4.903 MeV ) 469.2 (μb) 123.5 (nb)
107 (n,a) 0.000 (b) 0.000 (b) 2.670 (μb) 235.8 (μb) 234.9 (nb)

These cross sections are calculated from JENDL-4.0 at 300K.
The background color of each cell noted a cross section means the order of the cross-section value.
The unit of cross section, (b), means barns, and SI prefixes are used as following.
(kb) → 103(b),   (mb) → 10−3(b),  (μb) → 10−6(b),  (nb) → 10−9(b).

MT is a number that defines a reaction type. For the relation between MT and reaction type, please see here or refer to the manual of ENDF formats.

Maxwellian Average :
σmacs(T) =
2
 
 
π
EU
 
EL
σ(E,T) ⋅ E ⋅ exp (
E
  
kBT
) dE
 
EU
 
EL
E ⋅ exp (
E
  
kBT
) dE
,
where T denotes the temperature, and kB the Boltzmann constant. The upper and lower limits of integration, EL and EU are set to 10−5 eV and 10 eV, respectively.
Resonance Integral :
σri(T) =
EU
 
EL
σ(E,T) ⋅
1
 
E
dE ,
with  EL = 0.5 eV  and  EU = 10 MeV.
U-235 Thermal Fission-Neutron Spectrum Average (Fiss. Spec. Average) :
σfacs(T) =
EU
 
EL
σ(E,T) ⋅
 
4
 
πa3b
⋅ exp (
ab E
     
4 a
) ⋅ sinh
 
bE
dE
 
EU
 
EL
 
4
 
πa3b
⋅ exp (
ab E
     
4 a
) ⋅ sinh
 
bE
dE
,
with  EL = 10−5 eV  and  EU = 20 MeV. The parameters a and b are 0.988 MeV and 2.249 MeV−1, respectively.
Westcott g-factor :
g(T) =
σmacs(T)
 
σ(0.0253 eV,T)
 .