52-Te-125

Reaction 0.0253-eV Maxwellian
Average
g-factor Resonance
Integral
14-MeV Fiss. Spec.
Average
total 4.708 (b) 5.149 (b) 1.094 4.974 (b) 5.880 (b)
elastic 3.415 (b) 3.856 (b) 1.129 3.457 (b) 4.321 (b)
inelastic ( E-thr = 35.79 keV ) 182.0 (mb) 1.496 (b)
(n,2n) ( E-thr = 6.630 MeV ) 1.328 (b) 8.808 (mb)
(n,3n) ( E-thr = 16.14 MeV ) 770.8 (nb)
(n,na) ( E-thr = 2.257 MeV ) 29.89 (μb) 12.50 (nb)
(n,np) ( E-thr = 8.769 MeV ) 13.87 (μb) 31.49 (nb)
(n,nd) ( E-thr = 12.96 MeV ) 0.000 (b) 234.1e-12 (b)
capture 1.293 (b) 1.293 (b) 1.000 21.86 (b) 1.000 (mb) 52.52 (mb)
(n,p) 0.000 (b) 0.000 (b) 80.36 (μb) 4.846 (mb) 3.959 (μb)
(n,d) ( E-thr = 6.441 MeV ) 547.0 (μb) 129.8 (nb)
(n,t) ( E-thr = 6.730 MeV ) 7.672 (μb) 8.861 (nb)
(n,a) 0.000 (b) 0.000 (b) 46.01 (μb) 2.392 (mb) 6.063 (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).

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)
 .