63-Eu-151

MT Reaction 0.0253-eV Maxwellian
Average
g-factor Resonance
Integral
14-MeV Fiss. Spec.
Average
1 (n,total) 9.172 (kb) 8.260 (kb) 0.901 − 5.200 (b) 6.840 (b)
2 (n,elastic) 3.202 (b) 3.024 (b) 0.944 − 2.876 (b) 4.849 (b)
4 (n,inelastic) ( E-thr = 21.64 keV ) 592.3 (mb) 1.616 (b)
16 (n,2n) ( E-thr = 8.035 MeV ) 1.710 (b) 2.593 (mb)
17 (n,3n) ( E-thr = 14.51 MeV ) − 3.314 (μb)
22 (n,na) 0.000 (b) 0.000 (b) − 0.000 (b) 1.423 (mb) 381.3 (nb)
28 (n,np) ( E-thr = 4.918 MeV ) 2.854 (mb) 1.140 (μb)
102 (n,γ) 9.169 (kb) 8.257 (kb) 0.901 3.108 (kb) 1.013 (mb) 370.4 (mb)
103 (n,p) 0.000 (b) 0.000 (b) − 514.8 (μb) 7.479 (mb) 34.39 (μb)
107 (n,a) 8.806 (μb) 7.948 (μb) 0.903 888.4 (μb) 8.881 (mb) 72.71 (μb)

These cross sections are calculated from JENDL-3.3 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)
 .