46-Pd-110

Reaction 0.0253-eV Maxwellian
Average
g-factor Resonance
Integral
14-MeV Fiss. Spec.
Average
total 5.244 (b) 5.892 (b) 1.123 4.399 (b) 5.858 (b)
elastic 5.019 (b) 5.666 (b) 1.129 2.341 (b) 4.161 (b)
inelastic ( E-thr = 105.0 keV ) 453.2 (mb) 1.658 (b)
(n,2n) ( E-thr = 8.895 MeV ) 1.601 (b) 2.064 (mb)
(n,3n) ( E-thr = 15.10 MeV ) 1.389 (μb)
(n,na) ( E-thr = 4.493 MeV ) 23.39 (μb) 19.01 (nb)
(n,np) ( E-thr = 10.72 MeV ) 2.687 (μb) 17.27 (nb)
capture 225.6 (mb) 225.5 (mb) 0.999 3.284 (b) 3.179 (mb) 33.97 (mb)
(n,p) ( E-thr = 4.835 MeV ) 2.818 (mb) 700.3 (nb)
(n,d) ( E-thr = 8.480 MeV ) 61.29 (μb) 28.44 (nb)
(n,t) ( E-thr = 10.30 MeV ) 9.963 (nb) 336.3e-12 (b)
(n,He-3) ( E-thr = 11.64 MeV ) 180.9e-27 (b) 9.305e-18 (b)
(n,a) 0.000 (b) 0.000 (b) 2.925 (μb) 1.204 (mb) 365.7 (nb)

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)
 .