Ming Gao

Prof. Dr. Ming Gao

orcid

Research Focus & Metrics

Academic Career Length

8Years (2019-Present)

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

Representative Publications

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8 April 2019 in Nanomaterials
Verified
Journal Article
Open access
PDF file
MGMing Gao
Ming Gao
DLDanni Liu
Danni Liu
HYHuanhuan Yang
Huanhuan Yang
HHHao Huang
Hao Huang
QLQian Luo
Qian Luo
PCPaul Chu
Paul Chu
As a layered nano-sheet material, layered graphitic carbon nitride (g-C3N4) has attracted attention in multifunctional photocatalytic applications. However, g-C3N4 is electrochemically inert consequently hampering electrochemical applications. In this work, low-temperature nitrogen plasma processing was conducted to modify g-C3N4 to enhance the electrocatalytic performance in the hydrogen evolution reaction (HER). The plasma produced significant morphological and chemical changes on the surface of g-C3N4 via active species, and nitrogen atoms were incorporated into the surface while the bulk properties did not change. The modification improved the surface hydrophilicity and electrocatalytic HER activity, as well as excellent stability in HER after 2000 cycles. Our results revealed that plasma treatment was a promising technique to improve the HER of carbon-based layered nano-sheet materials.

6 January 2024 in Coatings
Verified
Journal Article
Open access
PDF file
诗王诗文 王
诗文 王
YWYu Wang
Yu Wang
MGMing Gao
Ming Gao
YHYifan Huang
Yifan Huang
Dielectric barrier discharge (DBD) plasma surface modification has certain aging effect. This article studies the aging effect of plasma (DBD) on the surface modification of carbon fibers. The test results show that plasma (DBD) treatment reduces the impurity particles on the surface of carbon fibers and makes the surface texture coarser. In addition, there is no significant change. After plasma (DBD) treatment, the content of C–O–C, C–O and C=O on the surface of carbon fibers increased from 3.20%, 7.76% and 1.64% to 7.06%, 21.50 and 6.08%, respectively. This is due to the high-energy particle bombardment of the fiber surface, which forms activated carbon atoms on the surface. The free electrons of these activated carbon atoms combine with ionized oxygen in the air. However, with the passage of time, the content of C–O–C, C–O and C=O gradually decreases to 3.31%, 8.57% and 1.77%, respectively. This is because some functional groups formed on the treated carbon fiber surface are not firmly bound, and some of these functional groups containing O2 groups will combine with surrounding substances through irreversible chemical oxidation reactions to produce CO2, which leaves the carbon fiber surface as a gas. The treated carbon fibers will immediately become hydrophilic, and the water contact angle decreases from 148.71° to 0°. With the passage of time, the water contact angle gradually increases to 118.16°, and the hydrophobicity recovers.

20 February 2023 in Surfaces and Interfaces
Verified
Journal Article
Closed access
CXChengfeng Xiong
Chengfeng Xiong
YWYu Wang
Yu Wang
LLLiangliang Lin
Liangliang Lin
MGMing Gao
Ming Gao
YHYifan Huang
Yifan Huang
PCPaul K Chu
Paul K Chu

19 January 2023 in Advanced Materials Interfaces
Verified
Journal Article
Open access
RHRuoyu Han
Ruoyu Han
CLChen Li
Chen Li
MGMing Gao
Ming Gao
YCYuchen Cao
Yuchen Cao
WYWei Yuan
Wei Yuan
YHYifan Huang
Yifan Huang
Electrical explosion, characterized by ultrafast atomization and quenching rate (dT/dt ≈ 1010–1012 K s–1) of the sample, is a unique approach for “one‐step” synthesis of nanomaterials. Experiments are carried out with layered graphite and Bi2Se3 under the action of electrical explosion in a confined reaction tube. High‐speed photography and electrophysical diagnostics are applied to characterize dynamic processes. SEM and EDS are used to characterize surface micro‐morphology of reaction products. The layered materials are first exfoliated to thin nanosheets/nanocrystals by shock waves and turbulent flow of the explosion. As the ionized explosion products (>10 000 K) contacts the sample, intense heat transfer happens, simultaneously atomizing the sample and quenching the plasmas. As a result, nanoparticles grow on the surface of thin sheets, forming “dot‐sheet” structure. The size distribution of the nanoparticles typically ranges from 10 to 100 nm, following Log‐normal distribution. The dotted graphite nanosheets gather together and form a stacked/cabbage‐like structure. By contrast, Bi2Se3 case accompanies with chemical reactions, causing surface corrosion and showing more possibilities: nanocrystals and nanotubes growth on different areas of the sample.

21 March 2024 in Applied Surface Science Advances
Verified
Journal Article
Open access
CXChengfeng Xiong
Chengfeng Xiong
MGMing Gao
Ming Gao
HHHao Huang
Hao Huang
YWYu Wang
Yu Wang
XGXiaobin Gu
Xiaobin Gu
YHYifan Huang
Yifan Huang

27 July 2023 in Journal of Vacuum Science & Technology A
Verified
Journal Article
Open access
PDF file
FMFang-Fang Ma
Fang-Fang Ma
QZQuanzhi Zhang
Quanzhi Zhang
DHDao-Man Han
Dao-Man Han
ZXZilan Xiong
Zilan Xiong
MGMing Gao
Ming Gao
YWYou-Nian Wang
You-Nian Wang
The fabrication process of modern microelectronic devices faces a significant challenge regarding the uniformity of wafer processing during plasma etching. Particularly, nonuniformity is prominent at the wafer edge due to varying electrical properties, leading to sheath bending and distorted ion trajectories. To address this issue, a wafer terminating structure known as a focus ring is employed to modify the sheath structure near the edge of the wafer and ensure uniform ion fluxes. However, the focus ring is subject to erosion caused by the plasma, making it crucial to minimize the ion energy bombarding the focus ring. In light of this, this paper investigates the impact of parameters such as the wafer-focus ring gap, focus ring height, and dielectric constant of the focus ring on the ion angle onto the wafer and the ion energy onto the focus ring. To conduct the analysis, a 2D3V particle-in-cell/Monte Carlo collision model is utilized. The study reveals the existence of horizontal electric fields with opposite directions at the wafer edge and the inner edge of the focus ring. Optimizing the ion angle onto the wafer edge can be achieved by adjusting the material and geometry of the focus ring. Furthermore, reducing the ion energy at the focus ring can be accomplished by increasing the height or decreasing the dielectric constant of the focus ring.