3-Li-0

Reaction 0.0253-eV Maxwellian
Average
g-factor Resonance
Integral
14-MeV Fiss. Spec.
Average
(n,total) 72.44 (b) 72.62 (b) 1.002 1.468 (b) 1.849 (b)
(n,elastic) 1.024 (b) 1.154 (b) 1.127 1.016 (b) 1.642 (b)
(n,inelastic) ( E-thr = 546.3 keV ) 368.6 (mb) 181.6 (mb)
(n,2n) ( E-thr = 6.614 MeV ) 70.69 (mb) 50.06 (μb)
(n,γ) 44.88 (mb) 44.90 (mb) 1.001 20.21 (mb) 8.014 (μb) 8.513 (μb)
(n,p) ( E-thr = 3.185 MeV ) 513.5 (μb) 323.6 (μb)
(n,d) ( E-thr = 8.868 MeV ) 9.022 (mb) 10.15 (μb)
(n,t) 71.37 (b) 71.41 (b) 1.001 32.27 (b) 2.129 (mb) 25.10 (mb)
MT = 205 ( E-thr = 2.822 MeV ) 279.9 (mb) 18.52 (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)
 .