Cheng Li

Prof. Cheng Li

School of Instrumentation Science and Opto‐Electronics Engineering, Beihang University, Beijing 100191, China
orcid

Research Focus & Metrics

Academic Career Length

13Years (2014-Present)

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

Representative Publications

View All Publications
17 October 2016 in Advanced Materials
Verified
Journal Article
Closed access
PDF file
FYFeifan Yu
Feifan Yu
QLQianwen Liu
Qianwen Liu
XGXin Gan
Xin Gan
MHMingxiang Hu
Mingxiang Hu
TZTianyi Zhang
Tianyi Zhang
Ruitao LvRuitao Lv
Ruitao Lv

24 September 2018 in Optics Letters
Verified
Journal Article
Closed access
PDF file
Cheng LiCheng Li
Cheng Li
XYXiyu Yu
Xiyu Yu
WZWei Zhou
Wei Zhou
YCYubo Cui
Yubo Cui
JLJian Liu
Jian Liu
SFShangchun Fan
Shangchun Fan
We demonstrate here an ultrafast, miniature, and high-performance fiber-tip Fabry–Perot (F-P) humidity sensor with ∼300  nm-thick graphene oxide (GO) diaphragm suspended onto the end face of a capillary tube with an inner diameter of 50 μm and a cavity length of ∼100  μm. The sensitivity to relative humidity (RH) spanning from ∼10%RH to ∼90%RH was examined based on the wavelength shift in the interference spectrum. Due to the intrinsic hydrophilicity of the porous GO membrane, the developed sensor exhibited an average wavelength variation of ∼0.2  nm/%RH, which indicated a relatively broad and readily detectable RH linear measurement range. More prominently, an ultrahigh response time of 60 ms was achieved over other alternative F-P humidity sensors previously reported, to our knowledge.

9 October 2015 in Optics Express
Verified
Journal Article
Open access
PDF file
Cheng LiCheng Li
Cheng Li
QLQianwen Liu
Qianwen Liu
XPXiaobin Peng
Xiaobin Peng
SFShangchun Fan
Shangchun Fan
A miniature Fabry-Perot interferometric sensor with an ultra-high temperature sensitivity was constructed by using an approximate 8-layer graphene diaphragm. The extremely thin diaphragm was transferred onto the endface of a ferrule with an inner diameter of 125 μm, and van der Waals interactions between the graphene diaphragm and its substrate created a low finesse Fabry-Perot interferometer with a cavity length of 42.86 μm. Temperature testing demonstrated a temperature-induced cavity length change of 352 nm/°C with a good linearity in the range of 20-60 °C. The result conformed well to the proposed analytical models relating to thermal expansion of trapped gas, thermal-optical property of graphene diaphragm and deflection behavior of bulged graphene blister. However, the ultra-thin diaphragm exhibited a small deflection deformation characteristic due to the applied higher loads.

26 September 2014 in Microsystem Technologies
Verified
Journal Article
Closed access
PDF file
Cheng LiCheng Li
Cheng Li
JXJun Xiao
Jun Xiao
TGTingting Guo
Tingting Guo
SFShangchun Fan
Shangchun Fan
Wei JinWei Jin
Wei Jin

31 May 2023 in ACS Applied Materials & Interfaces
Verified
Journal Article
Closed access
WFWenjing Fan
Wenjing Fan
Cheng LiCheng Li
Cheng Li
XLXiaoshi Li
Xiaoshi Li
He TianHe Tian
He Tian

28 February 2022 in IEEE Sensors Journal
Verified
Journal Article
Closed access
Cheng LiCheng Li
Cheng Li
SLShanshan Lu
Shanshan Lu
CZChao Zhong
Chao Zhong
XSXuefeng Song
Xuefeng Song
Herein we demonstrate a miniature flexible optical fiber Fabry-Perot (F-P) underwater ultrasonic sensor with chitosan diaphragm coated onto the tip of a capillary with an inner diameter of $50~\mu $ m. Due to its low Young’s modulus and high surface finish, the chitosan film with a thickness of ~955 nm, formed by low-speed spin-coating of a 3% solution of biotech chitosan dissolved in 2% acetic acid, enables a high sensitivity to low-frequency ultrasonic sound pressure for the developed sensor. Because of the molecular permeability of chitosan, this type of sensor contributes to effectively reducing the working point shift of the F-P sensor caused by static pressure in underwater ultrasonic measurement. Then the ultrasonic test in a water tank offered a high sound pressure sensitivity of 52.6 mV/kPa in the tested ultrasonic range of 100 kHz to 800 kHz with a noise-limited minimum detectable pressure level of ~2.37 mPa/Hz 1/2 . Also, the directivity measurement showed the maximum signal deviation of 2.47 dB in response to ultrasound pressure in the angle range of −90° – 90°. The proposed technique greatly simplifies the miniaturized integration of all-optical ultrasonic detectors, thus suggesting the great potential in ultra-high sensitivity hydrophone in biomedical photoacoustic measurement.