The 69th JSAP Spring Meeting 2022

Presentation information

Oral presentation

FS Focused Session "AI Electronics" » FS.1 Focused Session "AI Electronics"

[22p-E102-1~14] FS.1 Focused Session "AI Electronics"

Tue. Mar 22, 2022 1:30 PM - 5:30 PM E102 (E102)

Atsushi Uchida(Saitama Univ.), Takao Marukame(Toshiba)

2:30 PM - 2:45 PM

[22p-E102-4] High-density CNT/HfO2/CNT nano-junction memristors for reservoir computing

〇(P)Adha Sukma Aji1, Yutaka Ohno1,2 (1.VBL, Nagoya Univ., 2.IMaSS, Nagoya Univ.)

Keywords:cnt, memristors, physical reservoir

Recently, the research on brain-inspired computing is gaining tremendous interest to overcome the obstruction on von Neumann architecture. Reservoir computing is a novel artificial intelligence (AI) computing method that utilize the complex physical system. An array of numerous memristors has been demonstrated that could be exploited as a physical reservoir to run various AI applications with low power consumption, high data bandwidth, and low training cost. However, the main issues of conventional reservoir based on memristor array is the limit in the memory density. The higher number of memristors in the reservoir provides a better computing output. Here, we report the utilization of high-density memristors based on nano-junctions formed by carbon nanotubes (CNTs) for the application in physical reservoir computing.
Figure 1a shows the scanning electron micrograph image (SEM) of fabricated CNT reservior device with multiple terminals. The random network structure of a CNT thin film could generate high-density memristor at the cross-junctions of CNTs. To form the memristor structure, we inserted thin HfO2 of 10 nm between two CNT thin films. Multiple electrodes were connected to the top and bottom CNT films. The memristors were formed between the bottom and top CNT films. Consequently, each combination of two electrodes pairs can represent a memristor because the current path of each combination is different in the random CNT networks. In this fashion, numerous memristors can be obtained through the random network of CNTs in a ultra-small area and independently trained.
Figure 1b represents the I-V characteristics of a single combination of the CNT/HfO2/CNT memristors. The hysteresis indicates a clear memristor function. The change of the memristor's conductivity by the pulse input voltages is shown in Figure 1c.