52-Te-0

Reaction 0.0253-eV Maxwellian
Average
g-factor Resonance
Integral
14-MeV Fiss. Spec.
Average
total 8.203 (b) 8.732 (b) 1.065 4.974 (b) 5.879 (b)
elastic 3.756 (b) 4.241 (b) 1.129 3.455 (b) 4.885 (b)
inelastic ( E-thr = 35.79 keV ) 142.9 (mb) 966.9 (mb)
(n,2n) ( E-thr = 6.630 MeV ) 1.373 (b) 2.164 (mb)
(n,3n) ( E-thr = 14.62 MeV ) 3.429 (μb)
(n,na) ( E-thr = 302.3 keV ) 74.84 (μb) 31.63 (nb)
(n,np) ( E-thr = 7.275 MeV ) 33.56 (μb) 16.49 (nb)
(n,nd) ( E-thr = 12.74 MeV ) 0.000 (b) 19.57e-12 (b)
capture 4.447 (b) 4.491 (b) 1.010 56.36 (b) 1.008 (mb) 22.40 (mb)
(n,p) 0.000 (b) 0.000 (b) 26.99 (μb) 2.832 (mb) 1.695 (μb)
(n,d) ( E-thr = 4.946 MeV ) 68.25 (μb) 28.30 (nb)
(n,t) ( E-thr = 6.505 MeV ) 769.3 (nb) 2.677 (nb)
(n,He-3) ( E-thr = 4.645 MeV ) 262.6e-15 (b) 368.4e-15 (b)
(n,a) 413.5 (nb) 417.7 (nb) 1.010 44.82 (μb) 1.137 (mb) 3.834 (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)
 .