Honghe Zheng

Dr. Honghe Zheng


Research Focus & Metrics

Academic Career Length

15Years (2012-Present)

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

Representative Publications

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2 June 2014 in Journal of Materials Chemistry A
Verified
Journal Article
Closed access
PDF file
JSJie Shao
Jie Shao
ZWZhongming Wan
Zhongming Wan
HLHongmei Liu
Hongmei Liu
HZHuiyuan Zheng
Huiyuan Zheng
TGTian Gao
Tian Gao
HZHonghe Zheng
Honghe Zheng
Co 3 O 4 hollow dodecahedrons with controllable interiors are prepared through direct pyrolysis of ZIF-67 and exhibit high performance for Li-ion storage.

3 August 2021 in Advanced Materials
Verified
Journal Article
Closed access
PDF file
ZCZhang Cao
Zhang Cao
XZXueying Zheng
Xueying Zheng
QQQunting Qu
Qunting Qu
YHYunhui Huang
Yunhui Huang
HZHonghe Zheng
Honghe Zheng

19 July 2014 in Small
Verified
Journal Article
Closed access
PDF file
ZWZhongming Wan
Zhongming Wan
JSJie Shao
Jie Shao
JYJiaojiao Yun
Jiaojiao Yun
HZHuiyuan Zheng
Huiyuan Zheng
TGTian Gao
Tian Gao
HZHonghe Zheng
Honghe Zheng

19 September 2014 in Journal of Materials Chemistry A
Verified
Journal Article
Closed access
PDF file
LZLi Zhang
Li Zhang
LZLiya Zhang
Liya Zhang
LCLili Chai
Lili Chai
PXPeng Xue
Peng Xue
WHWeiwei Hao
Weiwei Hao
HZHonghe Zheng
Honghe Zheng
Silicon offers an extremely high theoretical specific capacity, but suffers from dramatic volume change during lithiation/delithiation processes, which typically leads to rapid anode degradation. Here we designed a facile and self-assembly strategy to construct a three-dimensional (3D) polymeric network as a promising binder for high-performance silicon submicro-particle (SiSMP) anodes through in situ interconnection of alginate chains by additive divalent cations. The highly cross-linked alginate network exhibits superb mechanical properties and strongly interacts with SiSMPs, which can tolerate the volume change of SiSMPs and restrict the volume expansion of the laminates to a large degree, thus effectively maintaining the mechanical and electrical integrity of the electrode and significantly improving the electrochemical performance. As a result, SiSMPs with a 3D binder network exhibit high reversible capacity, superior rate capability and much prolonged cycle life. Additionally, the 3D alginate binder was also successfully applied for the industrial submicro-silicon waste from solar cell production. With all of the advantages, the innovative way to tolerate the severe volume change by using a high-strength polymeric network may open a new approach to realize the industrial application of Si-based anodes in lithium-ion batteries.

10 May 2021 in ACS Energy Letters
Verified
Journal Article
Closed access
XZXueying Zheng
Xueying Zheng
LHLiqiang Huang
Liqiang Huang
WLWei Luo
Wei Luo
HWHaotian Wang
Haotian Wang
YDYiming Dai
Yiming Dai
YHYunhui Huang
Yunhui Huang

5 September 2012 in Dalton Transactions
Verified
Journal Article
Closed access
PDF file
Huan PangHuan Pang
Huan Pang
YMYahui Ma
Yahui Ma
GLGuochang Li
Guochang Li
JCJing Chen
Jing Chen
JZJiangshan Zhang
Jiangshan Zhang
WDWeimin Du
Weimin Du
Porous ZnO–NiO composite micropolyhedrons have been successfully synthesized by calcination of mixed oxalate (Zn0.9Ni0.1(C2O4)2·nH2O) precursors in air. The oxalate precursor micropolyhedrons were synthesized by a mild chemical precipitation method without any template or surfactant, and found to have a relatively low decomposition temperature. We have successfully explored the application of the resulting porous ZnO–NiO composite micropolyhedrons as electrochemical capacitors. Electrochemical study shows that the obtained ZnO–NiO composites under different conditions have different electrochemical supercapacitor properties in 3.0 or 1.0 M KOH solutions. The porous ZnO–NiO micropolyhedron material (P1) obtained by calcination of the oxalate precursor at 400 °C has a large specific capacitance 649.0 F g−1 in 3.0 M KOH solution and could maintain 99.1% of this value after 400 cycles at 5.8 A g−1. Even at a high current density of 58.0 A g−1, the specific capacitance of P1 is 395.2 F g−1.