57-La-0

Reaction 0.0253-eV Maxwellian
Average
g-factor Resonance
Integral
14-MeV Fiss. Spec.
Average
total 19.06 (b) 20.35 (b) 1.068 5.067 (b) 6.226 (b)
elastic 10.07 (b) 11.37 (b) 1.128 2.907 (b) 5.240 (b)
inelastic ( E-thr = 73.13 keV ) 348.9 (mb) 974.1 (mb)
(n,2n) ( E-thr = 7.525 MeV ) 1.800 (b) 1.593 (mb)
(n,3n) ( E-thr = 16.37 MeV ) 668.9 (nb)
(n,na) ( E-thr = 2.002 MeV ) 146.9 (μb) 44.48 (nb)
(n,np) ( E-thr = 6.129 MeV ) 2.433 (mb) 561.4 (nb)
(n,nd) ( E-thr = 10.76 MeV ) 122.7e-18 (b) 528.8e-12 (b)
(n,nt) ( E-thr = 13.37 MeV ) 0.000 (b) 30.10e-12 (b)
capture 8.984 (b) 8.984 (b) 1.000 11.92 (b) 1.002 (mb) 7.030 (mb)
(n,p) 0.000 (b) 0.000 (b) 9.466 (μb) 4.197 (mb) 1.400 (μb)
(n,d) ( E-thr = 3.802 MeV ) 634.5 (μb) 168.8 (nb)
(n,t) ( E-thr = 4.525 MeV ) 12.71 (μb) 18.01 (nb)
(n,He-3) ( E-thr = 7.073 MeV ) 18.36e-15 (b) 3.657e-12 (b)
(n,a) 0.000 (b) 0.000 (b) 27.34 (μb) 2.116 (mb) 1.656 (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)
 .