82-Pb-207

MT Reaction 0.0253-eV Maxwellian
Average
g-factor Resonance
Integral
14-MeV Fiss. Spec.
Average
1 (n,total) 11.99 (b) 13.44 (b) 1.121 5.354 (b) 6.405 (b)
2 (n,elastic) 11.28 (b) 12.73 (b) 1.128 2.376 (b) 5.108 (b)
4 (n,inelastic) ( E-thr = 572.5 keV ) 325.2 (mb) 1.287 (b)
16 (n,2n) ( E-thr = 6.774 MeV ) 2.651 (b) 7.073 (mb)
17 (n,3n) ( E-thr = 14.89 MeV ) 2.142 (μb)
22 (n,na) 0.000 (b) 0.000 (b) 1.300 (nb) 3.044 (μb) 1.282 (nb)
28 (n,np) ( E-thr = 7.528 MeV ) 3.339 (μb) 6.143 (nb)
102 (n,γ) 712.3 (mb) 712.3 (mb) 1.000 390.6 (mb) 3.728 (μb) 3.297 (mb)
103 (n,p) ( E-thr = 652.7 keV ) 1.210 (mb) 793.7 (nb)
107 (n,a) 0.000 (b) 0.000 (b) 4.513 (μb) 754.1 (μb) 484.7 (nb)

These cross sections are calculated from JENDL-3.2 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)
 .