82-Pb-206

MT Reaction 0.0253-eV Maxwellian
Average
g-factor Resonance
Integral
14-MeV Fiss. Spec.
Average
1 (n,total) 10.88 (b) 12.28 (b) 1.129 5.308 (b) 6.187 (b)
2 (n,elastic) 10.85 (b) 12.25 (b) 1.129 2.809 (b) 5.020 (b)
4 (n,inelastic) ( E-thr = 150.0 keV ) 241.3 (mb) 1.163 (b)
16 (n,2n) ( E-thr = 8.126 MeV ) 2.252 (b) 3.596 (mb)
17 (n,3n) ( E-thr = 14.89 MeV ) 1.201 (μb)
22 (n,na) 0.000 (b) 0.000 (b) 194.7 (nb) 23.22 (μb) 11.33 (nb)
28 (n,np) ( E-thr = 7.289 MeV ) 7.684 (μb) 8.833 (nb)
102 (n,γ) 26.56 (mb) 26.58 (mb) 1.001 114.8 (mb) 997.7 (μb) 3.939 (mb)
103 (n,p) ( E-thr = 753.7 keV ) 3.337 (mb) 1.631 (μb)
107 (n,a) 646.4e-12 (b) 646.7e-12 (b) 1.000 16.45 (μb) 375.8 (μb) 1.112 (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)
 .