21-Sc-45

MT Reaction 0.0253-eV Maxwellian
Average
g-factor Resonance
Integral
14-MeV Fiss. Spec.
Average
1 (n,total) 49.89 (b) 52.83 (b) 1.059 2.175 (b) 3.346 (b)
2 (n,elastic) 22.74 (b) 25.67 (b) 1.129 1.159 (b) 2.678 (b)
4 (n,inelastic) ( E-thr = 12.68 keV ) 663.2 (mb) 633.0 (mb)
16 (n,2n) ( E-thr = 11.58 MeV ) 240.0 (mb) 37.87 (μb)
102 (n,γ) 27.14 (b) 27.16 (b) 1.000 11.84 (b) 1.045 (mb) 6.173 (mb)
103 (n,p) 0.000 (b) 0.000 (b) 130.6 (mb) 59.00 (mb) 25.64 (mb)
107 (n,a) ( E-thr = 405.9 keV ) 53.50 (mb) 2.518 (mb)

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)
.