22-Ti-50

Reaction 0.0253-eV Maxwellian
Average
g-factor Resonance
Integral
14-MeV Fiss. Spec.
Average
(n,total) 3.936 (b) 4.421 (b) 1.123 2.510 (b) 3.501 (b)
(n,elastic) 3.757 (b) 4.241 (b) 1.129 1.008 (b) 3.111 (b)
(n,inelastic) ( E-thr = 1.585 MeV ) 653.8 (mb) 390.3 (mb)
(n,2n) ( E-thr = 11.17 MeV ) 830.0 (mb) 165.7 (μb)
(n,3n) ( E-thr = 19.48 MeV ) 59.46e-12 (b)
(n,na) ( E-thr = 10.94 MeV ) 8.519 (nb) 2.800 (nb)
(n,np) ( E-thr = 12.42 MeV ) 56.51 (μb) 164.1 (nb)
(n,γ) 179.5 (mb) 179.6 (mb) 1.001 88.33 (mb) 260.2 (μb) 427.4 (μb)
(n,p) ( E-thr = 6.229 MeV ) 10.88 (mb) 5.804 (μb)
(n,d) ( E-thr = 10.15 MeV ) 3.722 (μb) 36.96 (nb)
(n,t) ( E-thr = 14.10 MeV ) 144.4e-12 (b)
(n,He-3) ( E-thr = 14.36 MeV ) 227.8e-15 (b)
(n,a) ( E-thr = 3.513 MeV ) 7.232 (mb) 3.310 (μb)
MT = 203 ( E-thr = 6.229 MeV ) 10.93 (mb) 5.968 (μb)
MT = 207 ( E-thr = 3.513 MeV ) 7.232 (mb) 3.313 (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)
 .