80-Hg-0

MT Reaction 0.0253-eV Maxwellian
Average
g-factor Resonance
Integral
14-MeV Fiss. Spec.
Average
1 (n,total) 394.8 (b) 393.8 (b) 0.998 − 5.258 (b) 6.653 (b)
2 (n,elastic) 24.36 (b) 27.29 (b) 1.121 − 2.783 (b) 4.935 (b)
4 (n,inelastic) ( E-thr = 1.568 keV ) 304.6 (mb) 1.692 (b)
16 (n,2n) ( E-thr = 6.256 MeV ) 2.165 (b) 6.473 (mb)
17 (n,3n) ( E-thr = 13.55 MeV ) 105.2 (μb) 4.217 (μb)
22 (n,na) 0.000 (b) 0.000 (b) − 2.010 (nb) 3.980 (μb) 1.782 (nb)
28 (n,np) ( E-thr = 6.603 MeV ) 8.043 (μb) 9.742 (nb)
102 (n,γ) 370.4 (b) 366.5 (b) 0.989 88.35 (b) 322.3 (nb) 20.14 (mb)
103 (n,p) 0.000 (b) 0.000 (b) − 15.91 (μb) 2.025 (mb) 1.120 (μb)
104 (n,d) ( E-thr = 4.367 MeV ) 201.6 (μb) 58.59 (nb)
107 (n,a) 0.000 (b) 0.000 (b) − 2.484 (μb) 168.2 (μb) 163.5 (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)
 .