52-Te-120

Reaction 0.0253-eV Maxwellian
Average
g-factor Resonance
Integral
14-MeV Fiss. Spec.
Average
total 6.014 (b) 6.500 (b) 1.081 4.974 (b) 5.888 (b)
elastic 3.656 (b) 4.127 (b) 1.129 3.449 (b) 4.786 (b)
inelastic ( E-thr = 565.1 keV ) 372.3 (mb) 997.3 (mb)
(n,2n) ( E-thr = 10.38 MeV ) 1.090 (b) 327.1 (μb)
(n,3n) ( E-thr = 18.04 MeV ) 68.16 (nb)
(n,na) ( E-thr = 302.3 keV ) 10.02 (mb) 7.086 (μb)
(n,np) ( E-thr = 7.275 MeV ) 12.55 (mb) 1.905 (μb)
(n,nd) ( E-thr = 14.62 MeV ) 2.198e-12 (b)
capture 2.341 (b) 2.342 (b) 1.001 22.52 (b) 1.054 (mb) 101.5 (mb)
(n,p) ( E-thr = 202.2 keV ) 26.46 (mb) 188.5 (μb)
(n,d) ( E-thr = 4.946 MeV ) 1.148 (mb) 256.4 (nb)
(n,t) ( E-thr = 8.381 MeV ) 5.147 (μb) 9.909 (nb)
(n,He-3) ( E-thr = 4.645 MeV ) 244.8e-12 (b) 88.12e-12 (b)
(n,a) 0.000 (b) 0.000 (b) 5.348 (mb) 12.11 (mb) 690.3 (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)
 .