63-Eu-0

MT Reaction 0.0253-eV Maxwellian
Average
g-factor Resonance
Integral
14-MeV Fiss. Spec.
Average
1 (n,total) 4.553 (kb) 4.115 (kb) 0.904 − 5.200 (b) 6.853 (b)
2 (n,elastic) 6.940 (b) 7.473 (b) 1.077 − 2.870 (b) 4.702 (b)
4 (n,inelastic) ( E-thr = 21.64 keV ) 548.9 (mb) 1.839 (b)
16 (n,2n) ( E-thr = 8.035 MeV ) 1.765 (b) 2.095 (mb)
17 (n,3n) ( E-thr = 14.51 MeV ) − 2.129 (μb)
22 (n,na) 0.000 (b) 0.000 (b) − 0.000 (b) 765.5 (μb) 197.0 (nb)
28 (n,np) ( E-thr = 4.918 MeV ) 2.307 (mb) 824.7 (nb)
102 (n,γ) 4.546 (kb) 4.108 (kb) 0.904 2.222 (kb) 1.006 (mb) 311.2 (mb)
103 (n,p) 0.000 (b) 0.000 (b) − 361.8 (μb) 6.555 (mb) 22.85 (μb)
107 (n,a) 4.637 (μb) 4.215 (μb) 0.909 443.2 (μb) 5.219 (mb) 35.74 (μb)

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)
 .