96-Cm-243

Reaction 0.0253-eV Maxwellian
Average
g-factor Resonance
Integral
14-MeV Fiss. Spec.
Average
total 727.6 (b) 730.0 (b) 1.003 6.023 (b) 8.001 (b)
elastic 8.853 (b) 9.894 (b) 1.118 2.612 (b) 4.205 (b)
inelastic ( E-thr = 42.17 keV ) 403.4 (mb) 1.292 (b)
(n,2n) ( E-thr = 5.717 MeV ) 249.3 (mb) 3.579 (mb)
(n,3n) ( E-thr = 12.72 MeV ) 1.004 (mb) 627.2 (nb)
fission 587.4 (b) 591.1 (b) 1.006 1.546 (kb) 2.753 (b) 2.432 (b)
(n,fission) 587.4 (b) 591.1 (b) 1.006 1.546 (kb) 1.629 (b) 2.420 (b)
(n,n,fiss) ( E-thr = 2.700 MeV ) 954.6 (mb) 11.55 (mb)
(n,2n,fiss) ( E-thr = 10.00 MeV ) 167.9 (mb) 27.15 (μb)
(n,3nfiss) ( E-thr = 18.00 MeV ) 63.95e-12 (b)
capture 131.4 (b) 129.0 (b) 0.982 205.5 (b) 863.3 (μb) 67.73 (mb)
 
νp 3.429 5.150
νd 3.010e-3 2.090e-3

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)
 .


νp, νd : numbers of prompt and delayed neutrons per fission.