Xin-Gui Tang

Xin-Gui Tang

orcid

Research Focus & Metrics

Academic Career Length

28Years (1999-Present)

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

Representative Publications

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15 April 2021 in ACS Applied Electronic Materials
Verified
Journal Article
Closed access
KMKe Meng
Ke Meng
WLWenhua Li
Wenhua Li
XTXin-Gui Tang
Xin-Gui Tang
QLQiu-Xiang Liu
Qiu-Xiang Liu
YJYan-Ping Jiang
Yan-Ping Jiang

1 August 2018 in Journal of Alloys and Compounds
Verified
Journal Article
Closed access
ZTZhenhua Tang
Zhenhua Tang
JGJing Ge
Jing Ge
HNHao Ni
Hao Ni
BLBiao Lu
Biao Lu
XTXin-Gui Tang
Xin-Gui Tang
JGJu Gao
Ju Gao

1 September 2018 in Journal of Materiomics
Verified
Journal Article
Open access
MLMing-Ding Li
Ming-Ding Li
XTXin-Gui Tang
Xin-Gui Tang
SZSi-Ming Zeng
Si-Ming Zeng
YJYan-Ping Jiang
Yan-Ping Jiang
QLQiu-Xiang Liu
Qiu-Xiang Liu
WLWen-Hua Li
Wen-Hua Li

9 September 2020 in Journal of Materials Chemistry C
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Journal Article
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ZLZhi-Gang Liu
Zhi-Gang Liu
ZTZhen-Hua Tang
Zhen-Hua Tang
SHSong-Cheng Hu
Song-Cheng Hu
DYDi-Jie Yao
Di-Jie Yao
FSFei Sun
Fei Sun
XTXin-Gui Tang
Xin-Gui Tang
Progress in energy storage ceramics for applications has been of interest owing to their clean green nature and excellent ferroelectric/dielectric performances. In this study, lead-free Sm-doped 0.95BaTiO3–0.05Bi(Mg0.5Ti0.5)O3 (BT–BMT–xSm) relaxor ferroelectric ceramics were synthesized and confirmed to be an appropriate material for storage devices. After the introduction of Sm2O3 into BT–BMT ceramics, their hysteresis loops gradually shrank and became slender, which is beneficial to achieving high efficiency energy storage in ceramic capacitors. The maximum recoverable energy density for the BT–BMT–xSm (x = 0.03) sample reached 3.86 J cm−3 at normal temperature, and its corresponding energy efficiency reached 81.6%. Moreover, it was found from impedance spectroscopy that the breakdown field strength is related to the oxygen defect content in the samples. Ceramic samples with fewer defects have better insulation performance, which means that a high breakdown field strength will be obtained. With proper doping, enhanced relaxor behaviour and breakdown field strength were obtained to achieve excellent energy storage properties.

4 August 2019 in Nanomaterials
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Journal Article
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CLChao-Feng Liu
Chao-Feng Liu
XTXin-Gui Tang
Xin-Gui Tang
LWLun-Quan Wang
Lun-Quan Wang
HTHui Tang
Hui Tang
YJYan-Ping Jiang
Yan-Ping Jiang
ZTZhenhua Tang
Zhenhua Tang
The resistive switching (RS) characteristics of flexible films deposited on mica substrates have rarely been reported upon, especially flexible HfO2 films. A novel flexible Au/HfO2/Pt/mica resistive random access memory device was prepared by a sol-gel process, and a Au/HfO2/Pt/Ti/SiO2/Si (100) device was also prepared for comparison. The HfO2 thin films were grown into the monoclinic phase by the proper annealing process at 700 °C, demonstrated by grazing-incidence X-ray diffraction patterns. The ratio of high/low resistance (off/on) reached 1000 and 50 for the two devices, respectively, being relatively stable for the former but not for the latter. The great difference in ratios for the two devices may have been caused by different concentrations of the oxygen defect obtained by the X-ray photoelectron spectroscopy spectra indicating composition and chemical state of the HfO2 thin films. The conduction mechanism was dominated by Ohm’s law in the low resistance state, while in high resistance state, Ohmic conduction, space charge limited conduction (SCLC), and trap-filled SCLC conducted together.

1 February 2016 in Journal of Physics D: Applied Physics
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Journal Article
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TZT F Zhang
T F Zhang
XTXin-Gui Tang
Xin-Gui Tang
QLQ X Liu
Q X Liu
YJY P Jiang
Y P Jiang
XHX X Huang
X X Huang
QZQ F Zhou
Q F Zhou
(1 − x )Pb(Mg 1/3 Nb 2/3 )O 3 − x PbTiO 3 ( x = 0, 5, and 10 mol%) ceramics were prepared using a conventional mixed oxide solid state reaction method. The low-temperature relaxor behavior of (1 − x )Pb(Mg 1/3 Nb 2/3 )O 3 – x PbTiO 3 ceramics were examined in the temperature range from 120 to 523 K. A broad dielectric maximum that shifted to higher temperatures with increasing frequency, signified the relaxor-type behavior of these ceramics. The value of the relaxation parameter γ = 1.61–1.94 estimated from the linear fit of the modified Curie–Weiss law indicated the relaxor nature. High-temperature dielectric relaxation phenomena were found in the temperature region 600–850 K. Energy-storage properties were also analyzed, and the energy-storage density calculated from hysteresis loops reached about 0.47 J cm −3 at room temperature.