Xiao-fang Jiang

Xiao-fang Jiang

orcid

Research Focus & Metrics

Academic Career Length

11Years (2016-Present)

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

Representative Publications

View All Publications
6 January 2020 in Journal of Applied Polymer Science
Verified
Journal Article
Closed access
PDF file
XHXiaowen Hu
Xiaowen Hu
XZXinmin Zhang
Xinmin Zhang
WYWenmin Yang
Wenmin Yang
XJXiao-fang Jiang
Xiao-fang Jiang
XJXinshuai Jiang
Xinshuai Jiang
GZGuofu Zhou
Guofu Zhou

29 January 2021 in Journal of Materials Chemistry A
Verified
Journal Article
Closed access
PDF file
JHJinlong Hu
Jinlong Hu
XXXin Xu
Xin Xu
YCYijun Chen
Yijun Chen
Shaohang WuShaohang Wu
Shaohang Wu
ZWZhen Wang
Zhen Wang
FGFei Guo
Fei Guo
Defect passivation with natural amino acid molecules is reported, resulting in largely enhanced photovoltages in blade-coated MAPbI3perovskite solar cells and modules.

2 July 2020 in Advanced Science
Verified
Journal Article
Open access
PDF file
XHXiaowen Hu
Xiaowen Hu
CLChang Liu
Chang Liu
ZZZhiyong Zhang
Zhiyong Zhang
XJXiao-fang Jiang
Xiao-fang Jiang
JGJuan Garcia
Juan Garcia
KWKai Wang
Kai Wang
Simultaneously achieving high efficiency and high durability in perovskite solar cells is a critical step toward the commercialization of this technology. Inverted perovskite photovoltaic (IP‐PV) cells incorporating robust and low levelized‐cost‐of‐energy (LCOE) buffer layers are supposed to be a promising solution to this target. However, insufficient inventory of materials for back‐electrode buffers substantially limits the development of IP‐PV. Herein, a composite consisting of 1D cation‐doped TiO2 brookite nanorod (NR) embedded by 0D fullerene is investigated as a top modification buffer for IP‐PV. The cathode buffer is constructed by introducing fullerene to fill the interstitial space of the TiO2 NR matrix. Meanwhile, cations of transition metal Co or Fe are doped into the TiO2 NR to further tune the electronic property. Such a top buffer exhibits multifold advantages, including improved film uniformity, enhanced electron extraction and transfer ability, better energy level matching with perovskite, and stronger moisture resistance. Correspondingly, the resultant IP‐PV displays an efficiency exceeding 22% with a 22‐fold prolonged working lifetime. The strategy not only provides an essential addition to the material inventory for top electron buffers by introducing the 0D:1D composite concept, but also opens a new avenue to optimize perovskite PVs with desirable properties.

28 December 2018 in Nanoscale
Verified
Journal Article
Closed access
PDF file
XWXiao Wu
Xiao Wu
XJXiao-fang Jiang
Xiao-fang Jiang
XHXiaowen Hu
Xiaowen Hu
DZDing-Feng Zhang
Ding-Feng Zhang
SLShuang Li
Shuang Li
QXQing-Hua Xu
Qing-Hua Xu
Solution-processed organo-lead halide perovskites have emerged as promising optical gain media for tunable coherent light sources. The lasing performance is generally determined by the as-synthesized crystal quality. Noble metal nanostructures have been widely utilized to enhance optical responses due to their unique property of localized surface plasmon resonance. Herein, we report a simple method to enhance the near-infrared amplified spontaneous emission (ASE) performance of MAPbI3 polycrystalline films by solution-processing a PMMA spacer layer and an Au NR-doped PMMA top layer on perovskite thin films. As a result, the ASE threshold of the triple-layer perovskite film was significantly reduced by around 36% and the ASE intensity increased by 13.9-fold, compared to the pristine film. The underlying mechanism was attributed to the combined effects of surface passivation by PMMA and plasmon resonance enhancement of Au NRs. The passivation effect results in suppressing the nonradiative recombination and prolonging excited state decay, which have been investigated by transient absorption and pump–probe measurements. The plasmon effect is systematically studied through distance-dependent and spectra-dependent plasmon enhanced emission. The perovskite films with PMMA and Au NR coating showed great stability for 180 min under intense pulse laser continuous irradiation. The improved ASE performance still remained after leaving the film under the atmosphere for more than one month. We have successfully demonstrated a highly stable and sustained ASE output from MAPbI3 films under pulse laser excitation. This study provides a general approach for exploring plasmonic nanostructures in combination with polymers in the development and application of low-cost solution-processed semiconductor lasers.

8 June 2021 in Journal of Materials Chemistry C
Verified
Journal Article
Closed access
PDF file
XLXueting Long
Xueting Long
JWJieyu Wu
Jieyu Wu
SYSirui Yang
Sirui Yang
ZDZiqi Deng
Ziqi Deng
YZYusen Zheng
Yusen Zheng
LXLiang Xu
Liang Xu
With bay - and ortho -substituted perylenetetracarboxylic diimide derivatives, one-photon and two-photon excited ACQ-to-AIE conversion is realized through simple positional isomerization.

3 October 2024 in Nano Letters
Verified
Journal Article
Open access
HGHaotian Gu
Haotian Gu
HXHaoyuan Xu
Haoyuan Xu
CYChao Yang
Chao Yang
YFYifan Feng
Yifan Feng
GGGuanfeng Gao
Guanfeng Gao
XJXiao-fang Jiang
Xiao-fang Jiang
Chiral microlasers hold great promise for optoelectronics from integrated photonic devices to high-density quantum information processing. Despite significant progress in lead-halide perovskite emitters, chiral lasing with high dissymmetry factors (glum) has not yet been realized. Here, we demonstrate chiral single-mode microlasers with exceptional stability and tunable emission across the visible range by combining CsPbClxBr3-x perovskite microrods (MRs) with a cholesteric liquid crystal (CLC) layer. The MRs lase via a whispering gallery mode (WGM) microcavity and confer chirality through the encapsulated CLC layer, thus exhibiting circularly polarized lasing with dissymmetry factors reaching 1.62. Importantly, we demonstrate wavelength-tunable high dissymmetry chiral lasers in a broad spectral range by tuning the halide composition and using CLC layers with the desired photonic bandgap (PBG). This facile approach to generate chiral lasing not only is applicable to semiconductor nano- and microcrystals but also paves the way for potential integration into nanoscale photonic devices.