42-Mo-100

MT Reaction 0.0253-eV Maxwellian
Average
g-factor Resonance
Integral
14-MeV Fiss. Spec.
Average
1 (n,total) 5.527 (b) 6.211 (b) 1.124 4.137 (b) 5.962 (b)
2 (n,elastic) 5.328 (b) 6.012 (b) 1.128 2.246 (b) 4.519 (b)
4 (n,inelastic) ( E-thr = 541.0 keV ) 500.2 (mb) 1.419 (b)
16 (n,2n) ( E-thr = 8.385 MeV ) 1.385 (b) 2.205 (mb)
17 (n,3n) ( E-thr = 14.36 MeV ) 2.883 (μb)
22 (n,na) ( E-thr = 3.216 MeV ) 57.77 (μb) 18.74 (nb)
28 (n,np) ( E-thr = 10.72 MeV ) 3.100 (μb) 16.58 (nb)
102 (n,γ) 199.1 (mb) 199.1 (mb) 1.000 3.903 (b) 1.008 (mb) 20.96 (mb)
103 (n,p) ( E-thr = 5.502 MeV ) 1.838 (mb) 424.8 (nb)
104 (n,d) ( E-thr = 8.916 MeV ) 2.235 (μb) 7.352 (nb)
105 (n,t) ( E-thr = 9.630 MeV ) 1.259 (μb) 3.269 (nb)
107 (n,a) 0.000 (b) 0.000 (b) 14.59 (μb) 2.385 (mb) 1.159 (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)
 .