2018
DOI: 10.1109/led.2017.2786547
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Weak Localization and Weak Antilocalization in Double-Gate a-InGaZnO Thin-Film Transistors

Abstract: We demonstrate manipulation of quantum interference by controlling the competitions between weak localization (WL) and weak antilocalization (WAL) via variation of the gate voltages of doublegate amorphous InGaZnO thin-film transistors. Our study unveils the full profile of an intriguing universal dependence of the respective WL and WAL contributions on the channel conductivity. This universality is discovered to be robust against interface disorder.

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Cited by 4 publications
(2 citation statements)
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“…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. The Zr element has a strong binding capacity to oxygen (Zr-O: 776 KJ/mol), higher than that of the In element to oxygen (In-O: 348 KJ/mol), which can inhibit the formation of oxygen vacancies.…”
Section: Introductionmentioning
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. The Zr element has a strong binding capacity to oxygen (Zr-O: 776 KJ/mol), higher than that of the In element to oxygen (In-O: 348 KJ/mol), which can inhibit the formation of oxygen vacancies.…”
Section: Introductionmentioning
confidence: 99%
“…This effect, is similar to the MME widely observed in dual‐gate thin‐film transistors, in which applying double gates biases would enhance the charge transport in the channel with more weighted bulk accumulation of carriers. [ 37–41 ] In details as shown by Figure 3b,c, the gate voltage could reduce the built‐in electric field formed at the charge‐transfer interface, and facilitates the hole distribution away from the interface, similar to the positive bias situation in a p–n junction; [ 42 ] while in turn, the electric field from the charge‐transfer interface could also reorganize the energy alignment at the gate dielectric interface, modulating the gate accumulated carriers’ spatial distribution with respect to the semiconductor–dielectric interface.…”
Section: Resultsmentioning
confidence: 99%