46-Pd-108

Reaction 0.0253-eV Maxwellian
Average
g-factor Resonance
Integral
14-MeV Fiss. Spec.
Average
total 10.01 (b) 10.27 (b) 1.026 4.362 (b) 5.822 (b)
elastic 1.962 (b) 2.214 (b) 1.128 2.327 (b) 4.260 (b)
inelastic ( E-thr = 105.0 keV ) 478.1 (mb) 1.498 (b)
(n,2n) ( E-thr = 9.314 MeV ) 1.544 (b) 1.366 (mb)
(n,3n) ( E-thr = 15.91 MeV ) 438.4 (nb)
(n,na) ( E-thr = 3.896 MeV ) 80.79 (μb) 38.82 (nb)
(n,np) ( E-thr = 10.04 MeV ) 80.73 (μb) 96.31 (nb)
capture 8.046 (b) 8.057 (b) 1.001 243.2 (b) 3.574 (mb) 60.99 (mb)
(n,p) ( E-thr = 3.757 MeV ) 9.856 (mb) 3.422 (μb)
(n,d) ( E-thr = 7.798 MeV ) 220.7 (μb) 59.58 (nb)
(n,t) ( E-thr = 10.14 MeV ) 18.93 (nb) 439.5e-12 (b)
(n,He-3) ( E-thr = 10.16 MeV ) 8.309e-18 (b) 999.6e-18 (b)
(n,a) 435.8e-24 (b) 440.7e-24 (b) 0.000 26.65 (μb) 2.519 (mb) 1.581 (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)
 .