Yongna Zhang’s research while affiliated with Chongqing Institute of Green and Intelligent Technology and other places

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Publications (16)


(a) Schematic diagram of reconfigurable transparent antenna and (b) the sheet resistance vs 2–6 GHz and @3.4 GHz (c) with different Fermi energy of graphene.
Simulated transmission (a), reflection (b), and absorption (c) coefficients of 2 × 2 units FSS with GSS structure vs frequency under different values of sheet resistance.
(a) Return loss for different antenna structures and FSS transmission parameters with GSS structure [blue line in Fig. 3(a)]; return loss (b) and phase (c) of the tunable structures with different graphene sheet resistances; (d) radiation performance for different sheet resistances: realized gain patterns at 3.42 GHz; (e) monostatic RCS vs frequency with different sheet resistance; and (f) 3D scattering patterns of the proposed tunable antenna at 3.75 GHz. The sheet resistances of graphene are 200, 500, 1500, and 2500 Ω/ϒ, respectively.
(a) Photograph of the FSS and GSS-loaded tunable antenna; (b) the optical transmittance of PET, GSS, metal mesh, patch antenna, and the total device; (c) the sheet resistance of graphene film with different bias voltages; (d) measured S11 of the proposed antenna return loss parameter S11 when the gate voltage is varied from 0 to 2 V; and (e) measured radiation patterns at 3.37 GHz with the GSS structure. The gate voltage is varied from 0 to 2 V and (f) monostatic RCS vs frequency with different voltage states.
Transparent antenna with RCS tunability based on graphene and metasurface in S band
  • Article
  • Publisher preview available

September 2024

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24 Reads

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2 Citations

Heng Zhang

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Yongna Zhang

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Li Shao

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[...]

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Mingxing Piao

In this paper, we propose a graphene-based radar cross section (RCS) tunable antenna that utilizes metal mesh and graphene, both of which are optically transparent. The graphene sandwich structure is introduced to replace traditional components like diodes, micro-electro-mechanical systems (MEMS), and varactors, acting as an electromagnetic wave controller and significantly simplifying the device's complexity. By applying different voltages, the electrical properties of graphene are altered, enabling the regulation of reflection, transmission, and absorption of electromagnetic waves. This not only modifies the antenna's pattern but also achieves a substantial reduction in out-of-band RCS. The radiation and scattering mechanism of the antenna is carefully elaborated. The numerical and experimental results match well, which validates the effectiveness of the proposed method. The optical transmittance of the device is 27.9% at 550 nm, and the out-of-band RCS reduction is 10.01 dB at 3.83 GHz. The transparent, RCS tunable antenna proposed has significant potential applications in optical and microwave stealth technology.

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Enhanced Asymmetric Light‐Plasmon Coupling in Graphene Nanoribbons for High‐Efficiency Transmissive Infrared Modulation

September 2023

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25 Reads

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30 Citations

Graphene plasmonic modulators can manipulate the mid‐infrared light in transmission mode, which is currently challenging for traditional liquid crystal and digital micromirror devices, opening up a new avenue for infrared scene projection, infrared optical communication, and hyper spectra imaging. Nevertheless, their efficiencies are not high enough due to the single‐layer atomic thickness and low free carrier density of graphene. Here, it is demonstrated that the modulation efficiency can be significantly improved by enhancing the asymmetric light‐plasmon coupling. A general theoretical model is established to describe the modulation behaviors of the modulator, revealing the critical role of the asymmetric coupling rate. By using dielectric environment engineering and graphene structure design experimentally to enhance the asymmetric coupling rate from 0.45×10 ¹² to 7.05×10 ¹² s ⁻¹ , the modulation efficiency has been improved from 4% to 41% at 1530 cm ⁻¹ , while maintaining the bandwidth as large as 230 cm ⁻¹ . The modulator outperforms previous transmission‐type graphene plasmonic modulators in both efficiency and bandwidth, presenting great potential in next‐generation infrared integrated photonics platforms.


Graphene nanowalls in photodetectors

July 2023

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123 Reads

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9 Citations

Graphene nanowalls (GNWs) have emerged as a promising material in the field of photodetection, thanks to their exceptional optical, electrical, mechanical, and thermodynamic properties. However, the lack of a comprehensive review in this domain hinders the understanding of GNWs' development and potential applications. This review aims to provide a systematic summary and analysis of the current research status and challenges in GNW-based photodetectors. We begin by outlining the growth mechanisms and methods of GNWs, followed by a discussion on their physical properties. Next, we categorize and analyze the latest research progress in GNW photodetectors, focusing on photovoltaic, photoconductive, and photothermal detectors. Lastly, we offer a summary and outlook, identifying potential challenges and outlining industry development directions. This review serves as a valuable reference for researchers and industry professionals in understanding and exploring the opportunities of GNW materials in photodetection.


Graphene Growth across the Twin Boundaries of Copper Substrate

May 2022

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202 Reads

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6 Citations

Twin crystals, the formation energy of which is much smaller than that of ordinary grain boundaries, widely exist in the annealed copper and are hard to eliminate. The study of the effects of twin boundaries on graphene growth is of great significance to the understanding of graphene epitaxy. However, there are few studies on the effects of twin boundaries on the graphene growth process. Here, this article experimentally demonstrates that graphene islands are subjected to different compressive strains from the opposite copper crystal plane after growing across the twin boundary. Further results reveal that graphene can grow across different twin boundaries, such as atom steps, narrow valleys, and even micron‐scale ridges, without forming linear defect. Therefore, strain‐induced graphene doping can be manipulated with the type of twin boundaries and the location on the twin crystals. The transition region where the degree of doping changes monotonically across the twin boundary further confirms the different spatial doping phenomena of graphene islands. This work provides a new perspective for understanding the effect of twin boundaries on the graphene epitaxy, which is expected to have a potential impact on growing high‐quality graphene on twinned copper substrates.


(a) Schematic diagram of contact-free annealing configuration, from which the copper foil is suspended in the middle of furnace. (b,c) are the photographs of Cu foil annealed in argon atmosphere without and with 150 μL ethanol, respectively. The black dashed line in (c) corresponds to the grain boundaries between large grains and polygranular regions.
(a–f) and (g–l) are the photographs of copper foils annealed under different amounts of introduced ethanol, and their corresponding false-color images, respectively. (m) Statistics chart of the number of millimeter-sized grains and above on the copper foils, annealed under different amounts of ethanol introduced. (n) Statistics chart of number of grains on copper foils obtained in different annealing batches after different amounts of ethanol were introduced.
(a,b) are the photographs of the annealed copper foil with a decimeter-sized abnormally grown grain, respectively. (c) The XRD 2θ scan spectrum of the large grain. EBSD IPF maps in the normal direction (d); (001) pole figures (e); and KAM maps (f) of the single large grain of copper foil collected at the corresponding positions marked in (a). (ND, normal direction).
(a) Annealing sequence of copper foils. (b) EBSD IPF maps in the normal direction of copper foils at the different annealing temperatures shown in (a).
(a) Photographs of eight representative annealed copper foils with a decimeter-sized, abnormally grown grain. (b) The corresponding EBSD IPF maps in the normal direction of these large grains, collected at the corresponding positions marked with white dotted box in (a). Black dash line in (a) corresponds to grain boundaries between large grain and polygranular regions. ND, normal direction).
The Effect of Ethanol on Abnormal Grain Growth in Copper Foils

November 2021

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180 Reads

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6 Citations

Single-crystal Cu not only has high electrical and thermal conductivity, but can also be used as a promising platform for the epitaxial growth of two-dimensional materials. Preparing large-area single-crystal Cu foils from polycrystalline foils has emerged as the most promising technique in terms of its simplicity and effectiveness. However, the studies on transforming polycrystalline foil into large-area single-crystal foil mainly focus on the influence of annealing temperature and strain energy on the recrystallization process of copper foil, while studies on the effect of annealing atmosphere on abnormal grain growth behavior are relatively rare. It is necessary to carry out more studies on the effect of annealing atmosphere on grain growth behavior to understand the recrystallization mechanism of metal. Here, we found that introduction of ethanol in pure argon annealing atmosphere will cause the abnormal grain growth of copper foil. Moreover, the number of abnormally grown grains can be controlled by the concentration of ethanol in the annealing atmosphere. Using this technology, the number of abnormally grown grains on the copper foil can be controlled to single one. This abnormally grown grain will grow rapidly to decimeter-size by consuming the surrounding small grains. This work provides a new perspective for the understanding of the recrystallization of metals, and a new method for the preparation of large-area single-crystal copper foils.



Probing the Influence of the Substrate Hole Shape on the Interaction between Helium Ions and Suspended Monolayer Graphene with Raman Spectroscopy

January 2021

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73 Reads

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4 Citations

The Journal of Physical Chemistry C

A helium ion beam (HIB) is ideal for milling monolayer graphene in nanopore applications, but the optimizing irradiation parameter requires a comprehensive microscopic understanding of the interaction between helium ions and the suspended graphene. In this work, we investigate the influence of the substrate hole shape on the interaction between helium ions and suspended monolayer graphene on a substrate with periodic structures of different shapes. Raman spectroscopy is used to correlate the dose of HIB irradiation with engineered defects on freestanding monolayer graphene. Raman characteristics of the suspended monolayer graphene are related to the pore size and shape of the supporting substrate upon helium ion irradiation. These provide insights into the influence of the substrate hole shape on the interaction between helium ions and a freestanding graphene membrane. Our results can be used to analyze ion-membrane interactions in the other suspended monolayer two-dimensional materials for sub-nanometer precision nanopore fabrication.


(A) The scheme of the setup of suspended graphene film; the FIB image (B) and the optical image of SiNx holes (C); the optical image of the graphene film (D).
(A) Schematics of the experimental setup for suspended and supported film; (B) Raman spectra of the continuous graphene monolayer film supported on the SiNx (a), suspended on the non-through hole(b) and through-hole(c) respectively; Raman mapping (scanning step: 0.5 μm) of the G band position (C), and G’ band position (D). The yellow dash ranges are through holes, the green dash range is the non-through hole.
(A) Raman spectra of suspended monolayer graphene exposed to helium beam with distinct ion doses. (B) The intensity ID/IG and IG’/IG change with distinct Helium ion doses, respectively. (C) Optical image of the Raman spectra mapping area. Raman spectra mapping of graphene nanopore film under helium ion beam for the G’ band intensity (D), G’ band intensity (E). The yellow dash ranges are through holes, the green dash range is the non-through hole.
The ID/ID’ ratio (A), plot of G (B) and G’ (C) peak position change with distinct Helium ion.
The Raman band shift of suspended graphene impacted by the substrate edge and helium ion irradiation

January 2021

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119 Reads

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5 Citations

Non-through and through nanopores were introduced to study the Raman band shift of suspended graphene by the substrate edge and the helium ion beam irradiation during the fabrication of nanopore in graphene. Before the ion beam irradiation, there is a blue-shift in the G band and G’ band of suspended graphene on the micro-scale non-through and through holes edge because of the n-type mixing for suspended graphene from the translocation. After different doses of the helium ion irradiation, G’ band Raman of suspended graphene on through are blue-shift, and the G band positions are red-shift. Helium ion irradiation introduces n-type doping during the graphene nanopore fabrication. The observed Raman shifts help us to gain more intrinsic properties of the graphene nanopore. Thus, Raman spectroscopy can be used as a quantitative diagnostic tool to character graphene-based nanopore.


Batch Production of Uniform Graphene Films Via Controlling Gas-Phase Dynamics in Confined Space

December 2020

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54 Reads

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14 Citations

Batch production of continuous and uniform graphene films is critical for the application of graphene. Chemical vapor deposition (CVD) has shown great promise for mass producing high-quality graphene films. However, the critical factors affected the uniformity of graphene films during the batch production need to be further studied. Herein, we propose a method for batch production of uniform graphene films by controlling the gaseous carbon source to be uniformly distributed near the substrate surface. By designing the growth space of graphene into a rectangular channel structure, we adjusted the velocity of feedstock gas flow to be uniformly distributed in the channel, which is critical for uniform graphene growth. The monolayer graphene film grown inside the rectangular channel structure shows high uniformity with average sheet resistance of 345 Ω sq-1 without doping. The experimental and simulation results show that the placement of the substrates during batch growth of graphene films will greatly affect the distribution of gas-phase dynamics near the substrate surface and the growth process of graphene. Uniform graphene films with large-scale can be prepared in batches by adjusting the distribution of gas-phase dynamics.


Citations (12)


... Device-based tuning methods commonly employ varactors and P-Intrinsic-N (PIN) diodes, which are widely used in microwave and millimeter-wave applications. [18][19][20] However, these components face inherent limitations in size and operational frequency, restricting their application in the terahertz region. ...

Reference:

Tri-band terahertz polarization reconfigurable reflective metasurface based on liquid crystal
Transparent antenna with RCS tunability based on graphene and metasurface in S band

... Graphene is a promising material in photonic and optoelectronic applications due to its superiority in terms of high carrier mobility, broadband optical response, and facile electrical tunability. It has been reported that highly doped graphene can support SPPs with stronger mode confinement and lower propagation losses compared to noble metals [15,16]. Modulating the propagating SPPs by controlling carrier density distribution in graphene is an effective way to enhance the light-matter interaction and improve the modulation depth [17,18]. ...

Enhanced Asymmetric Light‐Plasmon Coupling in Graphene Nanoribbons for High‐Efficiency Transmissive Infrared Modulation
  • Citing Article
  • September 2023

... The irradiated area appears darker in comparison to the pristine graphite foil, attributed to graphene nanosheets exhibiting increased light absorption rates, compared to those of planar graphene ( Figure 1b). 29,30 Moreover, the wettability of the surface of the LIVGNs experiences a dramatic enhancement compared to that of the graphite foil. The contact angle (CA) of a water droplet on the pristine graphite foil is ∼60°( Figure 1c, left). ...

Graphene nanowalls in photodetectors

... Through analysis of the geometrical relationships of the twin crystal planes, it is found that the single-crystal graphene could be epitaxially grown on specific twinned substrates. 25,26 In short, the growth of large-scale high-quality graphene films on Cu foils has been achieved. The prospect of producing large-scale, highquality, single-crystal graphene on Cu foils via a roll-toroll process appears to be feasible, indicating a new era of scalable and efficient graphene production. ...

Graphene Growth across the Twin Boundaries of Copper Substrate

... Lu et al. [10] and Tseng et al. [11] found that AGG occurred in electroplated (111)-oriented nanotwinned Cu above a certain temperature, resulting in ultra-large grains with (100) orientation. Li et al. [12] introduced ethanol into the argon annealing atmosphere, which induced the AGG of Cu foil into a single crystal. Wu et al. [13] utilized a large-grained seed to trigger AGG in Cu foils, and pre-oxidation treatment was conducted to synthesize various facet indices. ...

The Effect of Ethanol on Abnormal Grain Growth in Copper Foils

... He ion with energy 37.3 eV is sufficient to eject the carbon atom in a crystal of graphite after collision, which produces many types of defects in graphite and changes its structural properties [143]. He et al. [144] and colleagues performed a related investigation. The influence of substrate edge topography on defect development in suspended GR upon helium ion implantation was investigated experimentally using a GR membrane with bilayer domains. ...

Investigation of Substrate Swell-Induced Defect Formation in Suspended Graphene upon Helium Ion Implantation
  • Citing Article
  • July 2021

The Journal of Physical Chemistry C

... Increased ion irradiation can explain vacancy formation when using plasma power of 1.7 kW, as shown in numerous studies. [57][58][59][60][61][62] Doubling the processing pressure did not inuence the graphene synthesized using a power of 1.7 kW (Fig. S4 †). However, we achieved some control of the graphene layer number, defect density, and defect type for samples grown at 700 C using power of 0.7 kW. ...

Probing the Influence of the Substrate Hole Shape on the Interaction between Helium Ions and Suspended Monolayer Graphene with Raman Spectroscopy
  • Citing Article
  • January 2021

The Journal of Physical Chemistry C

... Carbon graphitization in the composite materials was further identified by Raman spectroscopy, as shown in Figure 4(c). Graphitic structure regularity was predicted from the peak values of the D, G, and 2D bands on the Raman shift, namely, �1350, �1580, and �2700 cm −1 , respectively [73,74]. All synthesized TiO 2 /Fe 3 O 4 /C nanocomposites have a G band with higher intensity than the D band, indicating that the sp 2 bond was more dominant than the sp 3 bond. ...

The Raman band shift of suspended graphene impacted by the substrate edge and helium ion irradiation

... Upon developing rapid synthesis of large-area graphene with high film uniformity, grand challenges arise pertaining to preparing multiple pieces of graphene samples in one batch. 81 Among these, ensuring batch uniformity becomes an increasingly important subject and needs to be addressed when scaling graphene production from lab to fab. The key to achieving this goal is to guarantee the uniform distribution of carbon species above surface of each substrate. ...

Batch Production of Uniform Graphene Films Via Controlling Gas-Phase Dynamics in Confined Space

... It could be found that the C 0 values kept changing with increasing frequency, indicating that the eddy current loss contributed to the magnetic loss could be excluded. Consequently, the magnetic loss of Co@CM at such a low filling content was mainly derived from the intrinsic magnetic properties as well as the high shape anisotropy of Co nanosheets, causing natural resonance and exchange resonance [55], which was in accordance with the multiple resonances in the μ'' curves of all the samples. ...

Microwave plasma assisted reduction synthesis of hexagonal cobalt nanosheets with enhanced electromagnetic performances