“…The lower curve-shifting efficiency for the pure phase and ALD 10c samples may be influenced by the weak Fermi energy-level pinning, while a small number of carriers may be involved in the response. Based on the Shockley–Read–Hall theory, the locations of the energy change, the test frequency, and the interface state density have a relatively definite relationship normalΔ E = ( E C − E T ) = k normalB T q 0.25em ln ( σ v D dos 2 π f ) where E T is the interface trap energy level, E C is the majority carrier conduction band edge, k B is the Boltzmann constant, T is the temperature, and f is the frequency. σ is the trap interface area, v is the carrier thermal rate, D dos is the major carrier energy band density of states, and InP corresponds to values of 8.50 × 10 –17 cm 2 , 4.16 × 10 7 cm/s, and 5.56 × 10 23 cm –3 …”