Aiwei Tang

Prof. Dr. Aiwei Tang


Research Focus & Metrics

Academic Career Length

21Years (2006-Present)

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

Representative Publications

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11 February 2021 in Nano Letters
Verified
Journal Article
Closed access
ZLZhenyang Liu
Zhenyang Liu
HYHanjun Yang
Hanjun Yang
JWJunyu Wang
Junyu Wang
YYYucheng Yuan
Yucheng Yuan
KHKatie Hills-Kimball
Katie Hills-Kimball
OCOu Chen
Ou Chen

20 November 2024 in Nature
Verified
Journal Article
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YBYangyang Bian
Yangyang Bian
XYXiaohan Yan
Xiaohan Yan
FCFei Chen
Fei Chen
QLQian Li
Qian Li
BLBo Li
Bo Li
HSHuaibin Shen
Huaibin Shen

24 January 2019 in Advanced Optical Materials
Verified
Journal Article
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HZHan Zhang
Han Zhang
NHNing Hu
Ning Hu
ZZZaiping Zeng
Zaiping Zeng
QLQingli Lin
Qingli Lin
FZFengjuan Zhang
Fengjuan Zhang
ZDZuliang Du
Zuliang Du

5 June 2020 in Chemistry of Materials
Verified
Journal Article
Open access
DZDongxu Zhu
Dongxu Zhu
MZMatteo L. Zaffalon
Matteo L. Zaffalon
Valerio PinchettiValerio Pinchetti
Valerio Pinchetti
RBRosaria Brescia
Rosaria Brescia
FMFabrizio Moro
Fabrizio Moro
LMLiberato Manna
Liberato Manna
We report here the synthesis of undoped and Cu-doped Cs2ZnCl4 nanocrystals (NCs) in which we could tune the concentration of Cu from 0.7 to 7.5%. Cs2ZnCl4 has a wide band gap (4.8 eV), and its crystal structure is composed of isolated ZnCl4 tetrahedra surrounded by Cs+ cations. According to our electron paramagnetic resonance analysis, in 0.7 and 2.1% Cu-doped NCs the Cu ions were present in the +1 oxidation state only, while in NCs at higher Cu concentrations we could detect Cu(II) ions (isovalently substituting the Zn(II) ions). The undoped Cs2ZnCl4 NCs were non emissive, while the Cu-doped samples had a bright intragap photoluminescence (PL) at ∼2.6 eV mediated by band-edge absorption. Interestingly, the PL quantum yield was maximum (∼55%) for the samples with a low Cu concentration ([Cu] ≤ 2.1%), and it systematically decreased when further increasing the concentration of Cu, reaching 15% for the NCs with the highest doping level ([Cu] = 7.5%). The same (∼2.55 eV) emission band was detected under X-ray excitation. Our density functional theory calculations indicated that the PL emission could be ascribed only to Cu(I) ions: these ions promote the formation of trapped excitons, through which an efficient emission takes place. Overall, these Cu-doped Cs2ZnCl4 NCs, with their high photo- and radio-luminescence emission in the blue spectral region that is free from reabsorption, are particularly suitable for applications in ionizing radiation detection.

8 May 2020 in ACS Energy Letters
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Journal Article
Open access
DZDongxu Zhu
Dongxu Zhu
JZJuliette Zito
Juliette Zito
Valerio PinchettiValerio Pinchetti
Valerio Pinchetti
ZDZhiya Dang
Zhiya Dang
AOAndrea Olivati
Andrea Olivati
SBSergio Brovelli
Sergio Brovelli
We developed a hot-injection synthesis approach to prepare colloidal double perovskite Cs2NaBiCl6 nanocrystals (NCs) having a cubic shape and average size around 10 nm. We also examined the effects of replacing Na+ with Ag+ cations inside such NCs by preparing and characterizing a series of Cs2Na1-xAgxBiCl6 alloy NC samples with x ranging from 0 to 1. While pure Cs2NaBiCl6 NCs did not show any photoluminescence (PL) emission, Cs2Na1-xAgxBiCl6 NCs featured broad PL bands peaked at around 690nm and characterized by large Stokes shifts (≥1.5 eV). Interestingly, the PL quantum yield of these compounds was maximized for low amounts of Ag+ incorporated, reaching >3% for the Cs2Na0.95Ag0.05BiCl6 composition. Our density functional theory calculations coupled with spectroscopic investigations revealed that Cs2Na1-xAgxBiCl6 NCs are characterized by a complex photophysics stem-ming from the interplay of: i) the radiative recombination via trapped excitons localized in spatially connected AgCl6-BiCl6 octahedra; ii) surface traps, located on undercoordinated surface Bi centers, behaving as phonon-assisted nonradiative decay channel; iii) a thermal equilibrium between trapping and detrapping channels. Ultimately, we found that the system that showed the most efficient radiative emission was also the one having efficient concomitant non-radiative pathways, thus exhibiting an overall reduced PL performance. These results offer insights into developing double perovskite NCs with enhanced optoelectronic efficiency.

27 August 2015 in Journal of Materials Chemistry C
Verified
Journal Article
Closed access
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ZLZhenyang Liu
Zhenyang Liu
ATAiwei Tang
Aiwei Tang
MWMiao Wang
Miao Wang
CYChunhe Yang
Chunhe Yang
FTFeng Teng
Feng Teng
A simple heating-up colloidal approach has been developed to synthesize quaternary Cu–In–Zn–S (CIZS) nanocystals with different emission colors, which can be tuned by varying the Cu : In : Zn precursor ratios. The as-obtained products have a quasi-triangular shape with a small size distribution, and their crystal phase can be varied from cubic zinc-blende to hexagonal wurtzite structure with an increase of Cu stoichiometry. The inductively coupled plasma optical emission spectrometry (ICP-OES) results reveal that the as-obtained CIZS nanocrystals are Cu-deficient, and the Cu-vacancies have a significant effect on their optical properties. Moreover, the photoluminescence (PL) spectra of the CIZS nanocrystals recorded at different growth periods indicate that the partial cation exchange of Cu+ and In3+ with Zn2+ takes charge of the growth process. After coating a ZnS shell over the CIZS nanocrystals, the PL quantum yield (PLQY) is improved greatly and a blue-shift of the PL peak is observed as compared to that of plain CIZS nanocrystals. More interestingly, the highly luminescent CIZS/ZnS core/shell nanocrystals with different colors have been incorporated into poly(dimethylsiloxane) (PDMS) to be fabricated on an engraved “BJTU” glass substrate, and the as-obtained PDMS membranes exhibit a bright emission under UV light, which also show good stability when they are bent arbitrarily or immersed in water. This heating-up method has also been extended to the preparation of five-component Cu–Ag–In–Zn–S and Cu–Mn–In–Zn–S nanocrystals, which possess a cubic zinc-blende crystal structure and have bright luminescence. Our work may shed light on the synthesis of multi-component semiconductor nanocrystals.