“…As a result, the partial cross sections σ eval (γ, in) fluctuate although the total photo-neutron yield cross section σ exp (γ, xn) seems to be reasonable. This can be seen clearly by calculating the differences between the experimental and evaluated integrated cross sections σ int,exp and σ int,eval for the (γ, 1n) reaction, ∆σ 1 = σ int,eval (γ, 1n) − σ int,exp (γ, 1n) , (39) and for the (γ, 2n) reaction,…”