22-Ti-47

Reaction 0.0253-eV Maxwellian
Average
g-factor Resonance
Integral
14-MeV Fiss. Spec.
Average
(n,total) 4.892 (b) 5.314 (b) 1.086 2.325 (b) 3.334 (b)
(n,elastic) 3.266 (b) 3.687 (b) 1.129 1.403 (b) 2.422 (b)
(n,inelastic) ( E-thr = 162.8 keV ) 415.4 (mb) 885.1 (mb)
(n,2n) ( E-thr = 9.066 MeV ) 258.9 (mb) 129.7 (μb)
(n,na) ( E-thr = 9.148 MeV ) 285.8 (μb) 255.6 (nb)
(n,np) ( E-thr = 10.68 MeV ) 36.40 (mb) 6.082 (μb)
(n,γ) 1.626 (b) 1.627 (b) 1.001 1.339 (b) 355.2 (μb) 6.354 (mb)
(n,p) 0.000 (b) 0.000 (b) 102.1 (mb) 132.9 (mb) 17.75 (mb)
(n,d) ( E-thr = 8.412 MeV ) 1.138 (mb) 250.2 (nb)
(n,t) ( E-thr = 10.98 MeV ) 12.95 (μb) 7.898 (nb)
(n,He-3) ( E-thr = 11.22 MeV ) 959.5e-12 (b) 98.84e-12 (b)
(n,a) 0.000 (b) 0.000 (b) 33.16 (mb) 73.96 (mb) 3.338 (mb)
(n,2p) ( E-thr = 8.478 MeV ) 1.002 (mb) 164.1 (nb)
MT = 203 0.000 (b) 0.000 (b) 102.1 (mb) 169.3 (mb) 17.76 (mb)
MT = 207 0.000 (b) 0.000 (b) 33.16 (mb) 74.25 (mb) 3.338 (mb)

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)
 .