Shi-Jin Ding

Prof. Dr. Shi-Jin Ding


Research Focus & Metrics

Academic Career Length

29Years (1998-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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18 March 2020 in Nano Letters
Verified
Journal Article
Closed access
TWTian-Yu Wang
Tian-Yu Wang
JMJia-Lin Meng
Jia-Lin Meng
MRMing-Yi Rao
Ming-Yi Rao
ZHZhen-Yu He
Zhen-Yu He
LCLin Chen
Lin Chen
DZDavid Wei Zhang
David Wei Zhang

5 January 2021 in Materials Horizons
Verified
Journal Article
Closed access
PDF file
JMJialin Meng
Jialin Meng
TWTianyu Wang
Tianyu Wang
ZHZhen-Yu He
Zhen-Yu He
LCLin Chen
Lin Chen
HZHao Zhu
Hao Zhu
DZDavid Wei Zhang
David Wei Zhang
The data processing efficiency of traditional computers is suffering from the intrinsic limitation of physically separated processing and memory units. Logic-in-memory and brain-inspired neuromorphic computing are promising in-memory computing paradigms for improving the computing efficiency and avoiding high power consumption caused by extra data movement. However, memristors that can conduct digital memcomputing and neuromorphic computing simultaneously are limited by the difference in the information form between digital data and analogue data. In order to solve this problem, this paper proposes a flexible low-dimensional memristor based on boron nitride (BN), which has ultralow-power non-volatile memory characteristic, reliable digital memcomputing capabilities, and integrated ultrafast neuromorphic computing capabilities in a single in situ computing system. The logic-in-memory basis, including FALSE, material implication (IMP), and NAND, are implemented successfully. The power consumption of the proposed memristor per synaptic event (198 fJ) can be as low as biology (fJ level) and the response time (1 μs) of the neuromorphic computing is four orders of magnitude shorter than that of the human brain (10 ms), paving the way for wearable ultrahigh efficient next-generation in-memory computing architectures.

22 August 2018 in Discover Nano
Verified
Journal Article
Open access
PDF file
YHYa-Wei Huan
Ya-Wei Huan
SSSun Shunming
Sun Shunming
CGChenjie GU
Chenjie GU
WLWenjun Liu
Wenjun Liu
SDShi-Jin Ding
Shi-Jin Ding
WZWei Zhang
Wei Zhang
Ultra-wide bandgap beta-gallium oxide (β-Ga2O3) has been attracting considerable attention as a promising semiconductor material for next-generation power electronics. It possesses excellent material properties such as a wide bandgap of 4.6–4.9 eV, a high breakdown electric field of 8 MV/cm, and exceptional Baliga’s figure of merit (BFOM), along with superior chemical and thermal stability. These features suggest its great potential for future applications in power and optoelectronic devices. However, the critical issue of contacts between metal and Ga2O3 limits the performance of β-Ga2O3 devices. In this work, we have reviewed the advances on contacts of β-Ga2O3 MOSFETs. For improving contact properties, four main approaches are summarized and analyzed in details, including pre-treatment, post-treatment, multilayer metal electrode, and introducing an interlayer. By comparison, the latter two methods are being studied intensively and more favorable than the pre-treatment which would inevitably generate uncontrollable damages. Finally, conclusions and future perspectives for improving Ohmic contacts further are presented.

27 February 2013 in Discover Nano
Verified
Journal Article
Open access
PDF file
ZYZhi-Yuan Ye
Zhi-Yuan Ye
Hongliang LuHongliang Lu
Hongliang Lu
YGYang Geng
Yang Geng
YGYu-Zhu Gu
Yu-Zhu Gu
ZXZhang-Yi Xie
Zhang-Yi Xie
WZWei Zhang
Wei Zhang
High-quality Ti-doped ZnO films were grown on Si, thermally grown SiO2, and quartz substrates by atomic layer deposition (ALD) at 200°C with various Ti doping concentrations. Titanium isopropoxide, diethyl zinc, and deionized water were sources for Ti, Zn, and O, respectively. The Ti doping was then achieved by growing ZnO and TiO2 alternately. A hampered growth mode of ZnO on TiO2 layer was confirmed by comparing the thicknesses measured by spectroscopic ellipsometry with the expected. It was also found that the locations of the (100) diffraction peaks shift towards lower diffraction angles as Ti concentration increased. For all samples, optical transmittance over 80% was obtained in the visible region. The sample with ALD cycle ratio of ZnO/TiO2 being 20 had the lowest resistivity of 8.874 × 10−4 Ω cm. In addition, carrier concentration of the prepared films underwent an evident increase and then decreased with the increase of Ti doping concentration.

4 October 2018 in ACS Applied Materials & Interfaces
Verified
Journal Article
Closed access
TWTian-Yu Wang
Tian-Yu Wang
ZHZhen-Yu He
Zhen-Yu He
HLHao Liu
Hao Liu
LCLin Chen
Lin Chen
HZHao Zhu
Hao Zhu
DZDavid Wei Zhang
David Wei Zhang

9 January 2018 in Discover Nano
Verified
Journal Article
Open access
PDF file
QMQian Ma
Qian Ma
HZHe-Mei Zheng
He-Mei Zheng
YSYan Shao
Yan Shao
BZBao Zhu
Bao Zhu
WLWenjun Liu
Wenjun Liu
DZDavid Wei Zhang
David Wei Zhang
Atomic-layer-deposition (ALD) of In2O3 nano-films has been investigated using cyclopentadienyl indium (InCp) and hydrogen peroxide (H2O2) as precursors. The In2O3 films can be deposited preferentially at relatively low temperatures of 160–200 °C, exhibiting a stable growth rate of 1.4–1.5 Å/cycle. The surface roughness of the deposited film increases gradually with deposition temperature, which is attributed to the enhanced crystallization of the film at a higher deposition temperature. As the deposition temperature increases from 150 to 200 °C, the optical band gap (Eg) of the deposited film rises from 3.42 to 3.75 eV. In addition, with the increase of deposition temperature, the atomic ratio of In to O in the as-deposited film gradually shifts towards that in the stoichiometric In2O3, and the carbon content also reduces by degrees. For 200 °C deposition temperature, the deposited film exhibits an In:O ratio of 1:1.36 and no carbon incorporation. Further, high-performance In2O3 thin-film transistors with an Al2O3 gate dielectric were achieved by post-annealing in air at 300 °C for appropriate time, demonstrating a field-effect mobility of 7.8 cm2/V⋅s, a subthreshold swing of 0.32 V/dec, and an on/off current ratio of 107. This was ascribed to passivation of oxygen vacancies in the device channel.