22-Ti-48

Reaction 0.0253-eV Maxwellian
Average
g-factor Resonance
Integral
14-MeV Fiss. Spec.
Average
(n,total) 12.38 (b) 12.91 (b) 1.043 2.284 (b) 3.173 (b)
(n,elastic) 4.055 (b) 4.578 (b) 1.129 945.1 (mb) 2.540 (b)
(n,inelastic) ( E-thr = 1.004 MeV ) 812.4 (mb) 630.1 (mb)
(n,2n) ( E-thr = 11.87 MeV ) 429.2 (mb) 63.63 (μb)
(n,na) ( E-thr = 9.646 MeV ) 19.02 (μb) 30.47 (nb)
(n,np) ( E-thr = 11.69 MeV ) 5.150 (mb) 1.547 (μb)
(n,γ) 8.328 (b) 8.332 (b) 1.001 3.714 (b) 330.8 (μb) 2.232 (mb)
(n,p) ( E-thr = 3.276 MeV ) 60.12 (mb) 286.5 (μb)
(n,d) ( E-thr = 9.415 MeV ) 1.200 (mb) 219.0 (nb)
(n,t) ( E-thr = 13.89 MeV ) 0.000 (b) 400.5e-12 (b)
(n,He-3) ( E-thr = 12.46 MeV ) 4.800e-15 (b) 19.90e-12 (b)
(n,a) ( E-thr = 2.074 MeV ) 33.00 (mb) 22.80 (μb)
MT = 203 ( E-thr = 3.276 MeV ) 65.27 (mb) 288.0 (μb)
MT = 207 ( E-thr = 2.074 MeV ) 33.02 (mb) 22.83 (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)
 .