82-Pb-204

MT Reaction 0.0253-eV Maxwellian
Average
g-factor Resonance
Integral
14-MeV Fiss. Spec.
Average
1 (n,total) 12.94 (b) 14.52 (b) 1.122 − 5.284 (b) 6.218 (b)
2 (n,elastic) 12.23 (b) 13.81 (b) 1.129 − 2.787 (b) 5.011 (b)
4 (n,inelastic) ( E-thr = 150.0 keV ) 310.4 (mb) 1.176 (b)
16 (n,2n) ( E-thr = 8.436 MeV ) 2.178 (b) 2.685 (mb)
17 (n,3n) ( E-thr = 15.39 MeV ) − 654.9 (nb)
22 (n,na) 0.000 (b) 0.000 (b) − 2.868 (μb) 103.4 (μb) 102.5 (nb)
28 (n,np) ( E-thr = 6.670 MeV ) 31.06 (μb) 19.04 (nb)
102 (n,γ) 703.2 (mb) 703.6 (mb) 1.001 2.385 (b) 578.7 (μb) 32.83 (mb)
103 (n,p) 0.000 (b) 0.000 (b) − 66.02 (μb) 5.583 (mb) 4.161 (μb)
107 (n,a) 181.0 (nb) 181.1 (nb) 1.001 51.08 (μb) 1.077 (mb) 4.697 (μb)

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)
 .