46-Pd-106

Reaction 0.0253-eV Maxwellian
Average
g-factor Resonance
Integral
14-MeV Fiss. Spec.
Average
total 5.051 (b) 5.661 (b) 1.121 4.316 (b) 5.737 (b)
elastic 4.733 (b) 5.344 (b) 1.129 2.295 (b) 4.246 (b)
inelastic ( E-thr = 105.0 keV ) 563.6 (mb) 1.423 (b)
(n,2n) ( E-thr = 9.652 MeV ) 1.440 (b) 829.7 (μb)
(n,3n) ( E-thr = 16.81 MeV ) 93.57 (nb)
(n,na) ( E-thr = 3.260 MeV ) 201.5 (μb) 71.82 (nb)
(n,np) ( E-thr = 9.435 MeV ) 308.8 (μb) 132.9 (nb)
(n,nd) ( E-thr = 16.24 MeV ) 205.9e-15 (b)
capture 317.1 (mb) 317.2 (mb) 1.000 7.801 (b) 972.5 (μb) 65.35 (mb)
(n,p) ( E-thr = 2.785 MeV ) 12.95 (mb) 8.201 (μb)
(n,d) ( E-thr = 7.189 MeV ) 633.2 (μb) 139.0 (nb)
(n,t) ( E-thr = 9.925 MeV ) 53.90 (nb) 627.2e-12 (b)
(n,He-3) ( E-thr = 8.756 MeV ) 68.30e-15 (b) 30.19e-15 (b)
(n,a) 2.568e-15 (b) 2.597e-15 (b) 1.011 124.1 (μb) 4.461 (mb) 6.829 (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)
 .