45-Rh-105

Reaction 0.0253-eV Maxwellian
Average
g-factor Resonance
Integral
14-MeV Fiss. Spec.
Average
(n,total) 27.14 (kb) 28.44 (kb) 1.048 4.535 (b) 5.614 (b)
(n,elastic) 11.14 (kb) 12.47 (kb) 1.119 2.827 (b) 4.038 (b)
(n,inelastic) ( E-thr = 130.8 keV ) 213.3 (mb) 1.493 (b)
(n,2n) ( E-thr = 9.065 MeV ) 1.473 (b) 1.551 (mb)
(n,3n) ( E-thr = 16.14 MeV ) 1.155 (μb)
(n,na) ( E-thr = 3.988 MeV ) 146.8 (μb) 43.73 (nb)
(n,np) ( E-thr = 7.117 MeV ) 4.405 (mb) 935.6 (nb)
(n,nd) ( E-thr = 13.78 MeV ) 0.000 (b) 315.0e-12 (b)
(n,nt) ( E-thr = 13.84 MeV ) 0.000 (b) 78.13e-12 (b)
(n,γ) 16.00 (kb) 15.97 (kb) 0.998 17.04 (kb) 1.012 (mb) 78.03 (mb)
(n,p) ( E-thr = 1.145 MeV ) 12.56 (mb) 23.03 (μb)
(n,d) ( E-thr = 4.785 MeV ) 423.5 (μb) 109.6 (nb)
(n,t) ( E-thr = 7.540 MeV ) 13.49 (μb) 14.23 (nb)
(n,a) 0.000 (b) 0.000 (b) 25.95 (μb) 2.761 (mb) 1.644 (μb)

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)
 .