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Articles

Low-temperature formation of source–drain contacts in self-aligned amorphous oxide thin-film transistors

, , , , , , , , , , , , & show all
Pages 111-117 | Received 30 Sep 2014, Accepted 13 Apr 2015, Published online: 22 May 2015

Figures & data

Figure 1. (a) Cross-sectional scheme and (b) optical micrograph of SA a-IGZO TFTs.

Figure 1. (a) Cross-sectional scheme and (b) optical micrograph of SA a-IGZO TFTs.

Figure 2. (a) Transfer (VGSIDS) and (b) output (VDSIDS) characteristics of SA TFTs with W = 15 µm, L = 5 µm, and SP = 10 µm.

Figure 2. (a) Transfer (VGS−IDS) and (b) output (VDS−IDS) characteristics of SA TFTs with W = 15 µm, L = 5 µm, and SP = 10 µm.

Figure 3. Dependence of the RSHEET of hydrogen plasma, Ar plasma, and Ca-treated a-IGZO on the channel length at V = 2.0 V. The layout of the resistor structure is shown in the inset.

Figure 3. Dependence of the RSHEET of hydrogen plasma, Ar plasma, and Ca-treated a-IGZO on the channel length at V = 2.0 V. The layout of the resistor structure is shown in the inset.

Figure 4. Transfer (VGSIDS) characteristics dependence on (a) ‘L’ scaling and (b) ‘SP’ scaling of SA TFTs.

Figure 4. Transfer (VGS−IDS) characteristics dependence on (a) ‘L’ scaling and (b) ‘SP’ scaling of SA TFTs.

Figure 5. (a and c) Evolution of the transfer characteristics (VGSIDS) of SA TFTs (W = 15 µm and L = 5 µm) as a function of the duration time at +1.0 MV/cm (VGS = +20 V and VDS = 0 V) and at −1.0 MV/cm (VGS = −20 V and VDS = 0 V). (b and d) VTH shift as a function of the stress time in the positive and negative directions.

Figure 5. (a and c) Evolution of the transfer characteristics (VGS−IDS) of SA TFTs (W = 15 µm and L = 5 µm) as a function of the duration time at +1.0 MV/cm (VGS = +20 V and VDS = 0 V) and at −1.0 MV/cm (VGS = −20 V and VDS = 0 V). (b and d) VTH shift as a function of the stress time in the positive and negative directions.

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