Electrons are particles with half-integer spin. And they obey Fermi-Dirac statistics. The function of Fermi-Dirac distribution is written as follows:
"P(E,T)=\\dfrac{1}{exp( \\dfrac{E-E_F}{kT})}"
where "P(E,T)" - the probability that the electron occupies an energy level "E" , above or below the Fermi level "E_F"
Then
"P(E_F+2k_BT,T)= \\dfrac{1}{1+exp(\\dfrac{E_F+2k_BT-E_F}{k_BT})}=\\dfrac{1}{e^2}=0.119 \\newline\nin \\ percentage \\ P(E_F+2k_BT,T) =11.9\\%"
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