46-Pd-110

MT Reaction 0.0253-eV Maxwellian
Average
g-factor Resonance
Integral
14-MeV Fiss. Spec.
Average
1 (n,total) 5.245 (b) 5.889 (b) 1.123 4.480 (b) 5.572 (b)
2 (n,elastic) 5.018 (b) 5.662 (b) 1.128 2.387 (b) 4.133 (b)
4 (n,inelastic) ( E-thr = 377.2 keV ) 412.7 (mb) 1.405 (b)
16 (n,2n) ( E-thr = 8.886 MeV ) 1.675 (b) 2.096 (mb)
17 (n,3n) ( E-thr = 15.10 MeV ) 4.281 (μb)
22 (n,na) ( E-thr = 4.464 MeV ) 5.884 (μb) 4.092 (nb)
28 (n,np) ( E-thr = 10.62 MeV ) 984.4 (nb) 5.233 (nb)
102 (n,γ) 227.0 (mb) 226.8 (mb) 0.999 2.813 (b) 1.031 (mb) 27.78 (mb)
103 (n,p) ( E-thr = 4.665 MeV ) 4.267 (mb) 1.159 (μb)
104 (n,d) ( E-thr = 8.284 MeV ) 3.000 (μb) 7.102 (nb)
105 (n,t) ( E-thr = 10.28 MeV ) 44.76 (nb) 1.699 (nb)
107 (n,a) 0.000 (b) 0.000 (b) 1.782 (μb) 812.0 (μb) 238.1 (nb)

These cross sections are calculated from JENDL-3.2 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).

MT is a number that defines a reaction type. For the relation between MT and reaction type, please see here or refer to the manual of ENDF formats.

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)
 .