Calculate the position of the intrinsic Fermi level with respect to the center of the bandgap in silicon at T=300 \mathrm{~K}.
The density of states effective carrier masses in silicon are m_{n}^{*}=1.08 m_{0} and m_{p}^{*}=0.56 m_{0}.
Calculate the position of the intrinsic Fermi level with respect to the center of the bandgap in silicon at T=300 \mathrm{~K}.
The density of states effective carrier masses in silicon are m_{n}^{*}=1.08 m_{0} and m_{p}^{*}=0.56 m_{0}.
The intrinsic Fermi level with respect to the center of the bandgap is
E_{F i}-E_{\text {midgap }}=\frac{3}{4} k T \ln \left(\frac{m_{p}^{*}}{m_{n}^{*}}\right)=\frac{3}{4}(0.0259) \ln \left(\frac{0.56}{1.08}\right)
or
E_{F i}-E_{\text {midgap }}=-0.0128 \mathrm{eV}=-12.8 \mathrm{meV}
Comment
The intrinsic Fermi level in silicon is 12.8 \mathrm{meV} below the midgap energy. If we compare 12.8 \mathrm{meV} to 560 \mathrm{meV}, which is one-half of the bandgap energy of silicon, we can, in many applications, simply approximate the intrinsic Fermi level to be in the center of the bandgap.