“…Conversely, when the gate voltage decreases from V top to V base , the Fermi level at the interface decreases, leading to electron movement from the gate to the source, but the previously trapped electrons at the interface are left because of its long emission time . Therefore, integrating the obtained current over time allows us to determine the interface trap charges ( Q it ), which can be expressed as following equation: Q normali normalt = prefix∫ t start t stop I r + I f − I noise d t D normali normalt = Q normali normalt q · W · L where I r , I f , I noise , q , W , L , t start , and t stop are current during rising time, current during falling time, noise current, elemental charge, channel width, channel length, start point of the pulse, and stop point of the pulse, respectively. The schematic illustrations of electron capturing and emission behavior during the gate voltage pulse are shown in Figure b,c.…”