90-Th-228

MT Reaction 0.0253-eV Maxwellian
Average
g-factor Resonance
Integral
14-MeV Fiss. Spec.
Average
1 (n,total) 154.3 (b) 158.0 (b) 1.024 5.832 (b) 7.683 (b)
2 (n,elastic) 31.30 (b) 35.14 (b) 1.122 2.751 (b) 4.768 (b)
4 (n,inelastic) ( E-thr = 58.01 keV ) 498.4 (mb) 2.398 (b)
16 (n,2n) ( E-thr = 7.137 MeV ) 1.897 (b) 7.389 (mb)
17 (n,3n) ( E-thr = 12.62 MeV ) 85.78 (mb) 23.13 (μb)
18 (n,fission) 150.1 (mb) 150.2 (mb) 1.001 1.382 (b) 598.9 (mb) 375.7 (mb)
19 (n,f) 150.1 (mb) 150.2 (mb) 1.001 1.275 (b) 308.6 (mb) 371.7 (mb)
20 (n,nf) ( E-thr = 2.500 MeV ) 289.2 (mb) 3.943 (mb)
21 (n,2nf) ( E-thr = 10.00 MeV ) 551.2 (μb) 1.899 (μb)
38 (n,3nf) ( E-thr = 17.00 MeV ) 483.6e-21 (b)
102 (n,γ) 122.9 (b) 122.7 (b) 0.999 1.123 (kb) 1.233 (mb) 132.2 (mb)
 
456 νp 1.813 3.636
455 νd 1.115e-2 7.689e-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).

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)
 .


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