80-Hg-201

MT Reaction 0.0253-eV Maxwellian
Average
g-factor Resonance
Integral
14-MeV Fiss. Spec.
Average
1 (n,total) 22.28 (b) 24.16 (b) 1.084 5.263 (b) 6.707 (b)
2 (n,elastic) 14.50 (b) 16.37 (b) 1.129 2.776 (b) 4.573 (b)
4 (n,inelastic) ( E-thr = 1.568 keV ) 202.9 (mb) 2.100 (b)
16 (n,2n) ( E-thr = 6.256 MeV ) 2.277 (b) 13.91 (mb)
17 (n,3n) ( E-thr = 14.32 MeV ) 6.157 (μb)
22 (n,na) 0.000 (b) 0.000 (b) 930.3e-12 (b) 5.915 (μb) 2.561 (nb)
28 (n,np) ( E-thr = 7.680 MeV ) 4.636 (μb) 7.816 (nb)
102 (n,γ) 7.785 (b) 7.787 (b) 1.000 34.47 (b) 421.5 (nb) 19.74 (mb)
103 (n,p) ( E-thr = 723.1 keV ) 1.679 (mb) 828.2 (nb)
104 (n,d) ( E-thr = 5.444 MeV ) 262.6 (μb) 75.40 (nb)
107 (n,a) 0.000 (b) 0.000 (b) 2.372 (μb) 223.6 (μb) 169.3 (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)
 .