Zhenjun Li

Dr. Zhenjun Li

National Center for Nanoscience and Technology, Beijing 100190, China
orcid

Research Focus & Metrics

Academic Career Length

16Years (2011-Present)

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

Representative Publications

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29 November 2021 in Nanomaterials
Verified
Journal Article
Open access
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JZJiuzhou Zhao
Jiuzhou Zhao
ZLZhenjun Li
Zhenjun Li
Matthew ColeMatthew Cole
Matthew Cole
AWAiwei Wang
Aiwei Wang
XGXiangdong Guo
Xiangdong Guo
QDQing Dai
Qing Dai
The nanocone-shaped carbon nanotubes field-emitter array (NCNA) is a near-ideal field-emitter array that combines the advantages of geometry and material. In contrast to previous methods of field-emitter array, laser ablation is a low-cost and clean method that does not require any photolithography or wet chemistry. However, nanocone shapes are hard to achieve through laser ablation due to the micrometer-scale focusing spot. Here, we develop an ultraviolet (UV) laser beam patterning technique that is capable of reliably realizing NCNA with a cone-tip radius of ≈300 nm, utilizing optimized beam focusing and unique carbon nanotube–light interaction properties. The patterned array provided smaller turn-on fields (reduced from 2.6 to 1.6 V/μm) in emitters and supported a higher (increased from 10 to 140 mA/cm2) and more stable emission than their unpatterned counterparts. The present technique may be widely applied in the fabrication of high-performance CNTs field-emitter arrays.

21 April 2023 in Coatings
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Journal Article
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PGPeng Gao
Peng Gao
Jigang WangJigang Wang
Jigang Wang
JWJiao Wu
Jiao Wu
QXQingqing Xu
Qingqing Xu
LYLixue Yang
Lixue Yang
ZLZhenjun Li
Zhenjun Li
Green emitting long afterglow phosphor SrAl2O4: Eu2+, Dy3+ was synthesized via the combustion method. The physical phase analysis was carried out by X-ray diffraction, the results show that the introduction of Eu2+ into the lattice of the matrix resulted in a broad green emission centered at 508 nm, which is ascribed to the characteristic 4f65d1 to 4f7 electronic dipole allowed transition of Eu2+ ions. The doping of Eu2+ and Dy3+ did not change the physical phase of the crystals. Dy3+, as a coactivator, does not emit light itself, but can generate holes to form a trap energy level, which acts as an electron trap center to capture some of the electrons generated by the excitation of Eu2+. After excitation has ceased, let them gradually to transfer to the ground state for long afterglow luminescence. Then, we investigate the optical characterizations of different samples excited by X-ray. We found that SrAl2O4: Eu2+, 0.5% Dy3+ has this higher luminous intensity and afterglow. Its fluorescence lifetime is about 720 ns, and its quantum yield can reach 15.18%. Through search engine marketing (SEM) and energy dispersive X-ray spectroscopy (EDX), it has been proved that the sample has been successfully synthesized and its component content has been confirmed. The Eg value calculated from the diffuse reflectance spectrum is 4.61eV. The prepared SrAl2O4: Eu2+, Dy3+ luminescent powder is combined with Polydimethylsiloxane substrate for anticounterfeiting application, which provides a novel idea and method for the development of the anticounterfeiting field.

27 April 2011 in The Journal of Physical Chemistry C
Verified
Journal Article
Closed access
ZLZhenjun Li
Zhenjun Li
ZZZhenrong Zhang
Zhenrong Zhang
BKBruce D. Kay
Bruce D. Kay
ZDZdenek Dohnálek
Zdenek Dohnálek

9 July 2023 in Nanomaterials
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PGPeng Gao
Peng Gao
QLQuanxiao Liu
Quanxiao Liu
JWJiao Wu
Jiao Wu
JJJun Jing
Jun Jing
WZWenguan Zhang
Wenguan Zhang
ZLZhenjun Li
Zhenjun Li
A series of long-afterglow luminescent materials (SrAl2O4: Eu2+ (SAOE), SrAl2O4: Eu2+, Dy3+ (SAOED) and SrAl2O4: Eu2+, Dy3+, Gd3+ (SAOEDG)) was synthesized via the combustion method. Temperature and concentration control experiments were conducted on these materials to determine the optimal reaction temperature and ion doping concentration for each sample. The crystal structure and luminescent properties were analyzed via X-ray diffraction (XRD), photoluminescence (PL), and afterglow attenuation curves. The outcomes demonstrate that the kind of crystal structure and the location of the emission peak were unaffected by the addition of ions. The addition of Eu2+ to the matrix’s lattice caused a broad green emission with a central wavelength of 508 nm, which was attributed to the characteristic 4f65d1 to 4f7 electronic dipole, which allowed the transition of Eu2+ ions. While acting as sensitizers, Dy3+ and Gd3+ could produce holes to create a trap energy level, which served as an electron trap center to catch some of the electrons produced by the excitation of Eu2+ but did not itself emit light. After excitation ceased, this allowed them to gently transition to the ground state to produce long-afterglow luminescence. It was observed that with the addition of sensitizer ions, the luminous intensity of the sample increased, and the afterglow duration lengthened. The elemental structure and valence states of the doped ions were determined with an X-ray photoelectron spectrometer (XPS). Scanning electron microscopy (SEM) and energy dispersive X-ray spectroscopy (EDX) were used to characterize the samples. The results show that the sample was synthesized successfully, and the type and content of ions in the fluorescent powder could be determined. The fluorescence lifetime, quantum yield, bandgap value, afterglow decay time, and coordinate position in the coherent infrared energy (CIE) diagram of the three best sample groups were then analyzed and compared. Combining the prepared phosphor with ink provides a new idea and method for the field of anti-counterfeiting through screen printing.

11 November 2021 in Nanomaterials
Verified
Journal Article
Open access
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JXJianfeng Xiao
Jianfeng Xiao
JZJiuzhou Zhao
Jiuzhou Zhao
GLGuanjiang Liu
Guanjiang Liu
Matthew ColeMatthew Cole
Matthew Cole
SZShenghan Zhou
Shenghan Zhou
QDQing Dai
Qing Dai
Silicon carbide (SiC) nanostructure is a type of promising field emitter due to high breakdown field strength, high thermal conductivity, low electron affinity, and high electron mobility. However, the fabrication of the SiC nanotips array is difficult due to its chemical inertness. Here we report a simple, industry-familiar reactive ion etching to fabricate well-aligned, vertically orientated SiC nanoarrays on 4H-SiC wafers. The as-synthesized nanoarrays had tapered base angles >60°, and were vertically oriented with a high packing density >107 mm−2 and high-aspect ratios of approximately 35. As a result of its high geometry uniformity—5% length variation and 10% diameter variation, the field emitter array showed typical turn-on fields of 4.3 V μm−1 and a high field-enhancement factor of ~1260. The 8 h current emission stability displayed a mean current fluctuation of 1.9 ± 1%, revealing excellent current emission stability. The as-synthesized emitters demonstrate competitive emission performance that highlights their potential in a variety of vacuum electronics applications. This study provides a new route to realizing scalable field electron emitter production.

28 December 2022 in Journal of Materials Chemistry C
Verified
Journal Article
Closed access
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XLXinchuan Liu
Xinchuan Liu
YLYuanxun Li
Yuanxun Li
JXJianfeng Xiao
Jianfeng Xiao
JZJiuzhou Zhao
Jiuzhou Zhao
CLChi Li
Chi Li
ZLZhenjun Li
Zhenjun Li
It remains difficult to obtain a carbon nanotube (CNT) emitter that simultaneously exhibits high current density, low fluctuation, and long service time because CNTs are easily detached from the substrate in a strong electric field due to the weak adhesion between direct-growth CNTs and heterogeneous substrates. Herein, a mold-aligned transfer anchoring method is employed to anchor vertically aligned CNT film and CNT arrays on a metallic substrate using silver conductive paint via an annealing process. After 100 h of continuous testing with an initial current of ∼2 mA and a current density of ∼900 mA cm−2, the decay rate of the emission current of the anchored CNT emitter decreased by ∼88%, and the current fluctuation was ∼57% lower than that of the unanchored CNT emitter. Furthermore, a metal wire with a width of ∼90 μm could be clearly distinguished by a CNT cold cathode X-ray imaging system. These results testify that the proposed anchoring method can significantly improve the stability and lifetime of CNT field emitters with a high current density, which provides a new route for developing the cold cathode of X-ray sources and other industrial applications in the vacuum electronics field.