52-Te-130

Reaction 0.0253-eV Maxwellian
Average
g-factor Resonance
Integral
14-MeV Fiss. Spec.
Average
total 4.037 (b) 4.534 (b) 1.123 4.975 (b) 5.876 (b)
elastic 3.851 (b) 4.348 (b) 1.129 3.455 (b) 4.995 (b)
inelastic ( E-thr = 845.9 keV ) 137.8 (mb) 870.0 (mb)
(n,2n) ( E-thr = 8.482 MeV ) 1.380 (b) 2.160 (mb)
(n,3n) ( E-thr = 14.62 MeV ) 5.516 (μb)
(n,na) ( E-thr = 3.775 MeV ) 1.236 (μb) 1.805 (nb)
(n,np) ( E-thr = 10.09 MeV ) 18.75e-12 (b) 3.659 (nb)
capture 186.2 (mb) 186.3 (mb) 1.000 252.0 (mb) 1.000 (mb) 5.516 (mb)
(n,p) ( E-thr = 4.218 MeV ) 1.316 (mb) 321.5 (nb)
(n,d) ( E-thr = 7.761 MeV ) 1.941 (μb) 11.74 (nb)
(n,t) ( E-thr = 9.566 MeV ) 517.1e-12 (b) 1.803 (nb)
(n,a) 0.000 (b) 0.000 (b) 110.3 (nb) 164.9 (μb) 40.65 (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).

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)
 .