Electrical Characteristic Impact on Channel Shape of n-Channel TFT on Solid-Phase Crystallized Polycrystalline-Ge
Background and purpose To realize monolithic three-dimensional LSI and flexible mobile devices, it is essential to form semiconductor thin-film transistors (TFTs) on an insulator at low temperatures (<500 °C). Germanium (Ge) has garnered significant attention as a promising material for these applications due to its high carrier mobilities (electron: 3,900 cm²/V·s, hole: 1,900 cm²/V·s) and low crystallization temperature. We have successfully synthesized high-quality polycrystalline (poly-) Ge thin films using an advanced solid-phase crystallization (SPC) technique [1,2] and have fabricated accumulation-mode p-channel TFTs with excellent electrical properties [3]. More recently, we also demonstrated inversion-mode n-channel TFTs and CMOS inverter on SPC poly-Ge [4,5]. However, further improvements are needed, particularly in enhancing the ON/OFF ratio [4]. To address this, we aim to reduce OFF-state leakage current by shrinking the channel width, which is expected to significantly improve the ON/OFF ratio of n-channel poly-Ge TFTs. Experiments The TFT was fabricated on a poly-Ge/glass substrate, with details of the SPC process provided elsewhere [1]. The fabrication process flow and device structure are illustrated in Fig. 1. To form the n-type source/drain (S/D) regions, phosphorus (P) ion implantation was carried out at an energy of 50 keV and a dose of 1×10¹⁵ cm⁻². Following implantation, annealing was performed at 500 °C for 2 hours to activate and recrystallize the implanted regions. The active region was then defined by SPC-Ge isolation etching, followed by backfilling with sputter-deposited SiO₂. Two different island shapes—conventional rectangular and dumbbell-shaped channel TFT patterns—were formed on the same chip, as shown in the microscope images in Fig. 1. Next, the Ge surface was cleaned using plasma sacrificial oxidation followed by wet treatment. A stacked gate insulator consisting of GeO₂ (3 nm) and SiO₂ (20 nm) was then deposited. Post-deposition annealing (PDA) was performed at 400 °C for 30 minutes in N₂ to improve the gate dielectric quality. For the gate and S/D electrodes, thermally evaporated Al was used and patterned using a lithography process. Finally, contact annealing was carried out at 300 °C for 30 minutes in N₂. Results and discussion Figure 2(a) shows the I D-V D characteristics of the fabricated n-TFT with the updated dumbbell-shaped channel while Figure 2(b) shows the I D-V G transfer characteristics of both the conventional rectangular channel and the updated dumbbell-shaped channel. By comparing the I D-V G with those two types of channel shapes, we observe that channel shrinking has a preferable effect on improving the ON/OFF ratio, particularly by reducing the OFF-state current.To further investigate this effect, we examined the relationship between the ON/OFF ratio and channel width reduction. Figure 3 illustrates the I D-V G trend with different channel widths. The results indicate that while the ON-state current remains relatively stable as the channel width decreases, the OFF-state current significantly declines with channel width reduction. Additionally, we compared the electrical performance of the dumbbell-shaped channel and a narrow channel with the same width, as shown in Figure 4. The comparison reveals a substantial reduction in OFF-state current while maintaining a highly consistent ON-state current. This significant reduction in OFF current may be attributed to several factors. One possible reason is the decrease in grain boundaries within the channel region, which helps suppress leakage current in the OFF state. Another potential factor is improved channel controllability by the gate voltage. Previous studies have reported that shrinking the channel width can reduce leakage current at the back interface of the semiconductor thin film due to the edge effect [6,7]. Although further studies are required, these findings suggest that TFT performance can be enhanced by reducing the channel width and increasing the number of channels. Acknowledgements This work was partially supported by NEDO unreached challenge 2050 (P14004), JST-SPRING (JPMJSP2136), JST-ASPIRE, and the Cooperative Research Project of RIEC No. R06/A06, Tohoku University. The ion implantation was conducted at the CMS, Kyushu Institute of Technology.
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