2018
DOI: 10.1109/ted.2018.2859224
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Application of Single-Pulse Charge Pumping Method on Evaluation of Indium Gallium Zinc Oxide Thin-Film Transistors

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Cited by 18 publications
(7 citation statements)
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“…[37] Using the charge pumping technique as well, the IGZO/SiO 2 interface has a trap density of 6 × 10 10 cm −2 , while the interface state density spans a wide range from 10 9 to 10 14 eV −1 cm −2 . [25] Compared to previous results, the PMMA/DPPT-TT interface states are relatively numerous (Table I), but they can exhibit higher performance than other previous classes of polymer transistors. This may be caused by the following features:…”
contrasting
confidence: 59%
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“…[37] Using the charge pumping technique as well, the IGZO/SiO 2 interface has a trap density of 6 × 10 10 cm −2 , while the interface state density spans a wide range from 10 9 to 10 14 eV −1 cm −2 . [25] Compared to previous results, the PMMA/DPPT-TT interface states are relatively numerous (Table I), but they can exhibit higher performance than other previous classes of polymer transistors. This may be caused by the following features:…”
contrasting
confidence: 59%
“…The trap density and interfacial state distribution for various interfaces are summarized in Table I. Various techniques, including charge pumping, [25], [38] Berglund analysis, [35] optically assisted high-frequency CV characterization, [36] conductivity, [37] and Kelvin probes, [40] were utilized to investigate the interfacial states. According to Table I, the trap density of DPPT-TT/PMMA is 6 × 10 12 eV −1 cm −2 , which is greater than that of other organic and inorganic semiconductors.…”
mentioning
confidence: 99%
“…Indium oxide (In 2 O 3 ) films have high electron mobility, high carrier density, and excellent optical transmittance compared with other oxide semiconductors [17,18], making them an ideal material for transparent thin film transistors [19]. In order to obtain high-quality In 2 O 3 films, other elements are added, such as InSnO (ISO) [20][21][22], InZnSnO (IZTO) [23][24][25][26], InGaZnO (IGZO) [27][28][29][30], etc.…”
Section: Introductionmentioning
confidence: 99%
“…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.…”
Section: Resultsmentioning
confidence: 99%