WikiPhysicsSemiconductorsDopingDopingn=Nc⋅e−(Ec−EF)kTn=N_c\cdot e^{\frac{-(E_c-E_F)}{kT}}n=Nc⋅ekT−(Ec−EF)p=Nv⋅e−(EF−Ev)kTp=N_v\cdot e^{\frac{-(E_F-E_v)}{kT}}p=Nv⋅ekT−(EF−Ev)EcE_cEc is the position of the conduction band minimumEvE_vEv is the position of the valence band maxmimumkkk is Boltzmann’s constantNxN_xNx are the effective density of statesnp=ni2np=n_i^2np=ni2nin_ini = Intrinsic carrier concentrationni=NcNve−Eg2ktn_i=\sqrt{N_cN_v}e^{\frac{-E_g}{2kt}}ni=NcNve2kt−EgEgE_gEg = Band Gap = Ec−EvE_c-E_vEc−EvSubstitutional Doping Donated electrons are delocalisedIons are immobileNc≡2[2πmnkTh2]3/2N_c \equiv 2 \left[ \frac{2\pi m_nkT}{h^2}\right]^{3/2}Nc≡2[h22πmnkT]3/2Nv≡2[2πmpkTh2]3/2N_v \equiv 2 \left[ \frac{2\pi m_pkT}{h^2}\right]^{3/2}Nv≡2[h22πmpkT]3/2Equations