Jingwei Li's research while affiliated with Chongqing University and other places

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Publications (24)


Carboxyl-Decorated UiO-66 Supporting Pd Nanoparticles for Efficient Room-Temperature Hydrodeoxygenation of Lignin Derivatives
  • Article

February 2024

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11 Reads

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2 Citations

Small

Ruixue Yangcheng

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Jingwei Li

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Jiadai He

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[...]

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Jianjian Wang

Hydrodeoxygenation (HDO) of lignin derivatives at room‐temperature (RT) is still of challenge due to the lack of satisfactory activity reported in previous literature. Here, it is successfully designed a Pd/UiO‐66‐(COOH) 2 catalyst by using UiO‐66‐(COOH) 2 as the support with uncoordinated carboxyl groups. This catalyst, featuring a moderate Pd loading, exhibited exceptional activity in RT HDO of vanillin (VAN, a typical model lignin derivative) to 2‐methoxyl‐4‐methylpheonol (MMP), and >99% VAN conversion with >99% MMP yield is achieved, which is the first metal‐organic framework (MOF)‐based catalyst realizing the goal of RT HDO of lignin derivatives, surpassing previous reports in the literature. Detailed investigations reveal a linear relationship between the amount of uncoordinated carboxyl group and MMP yield. These uncoordinated carboxyl groups accelerate the conversion of intermediate such as vanillyl alcohol (VAL), ultimately leading to a higher yield of MMP over Pd/UiO‐66‐(COOH) 2 catalyst. Furthermore, Pd/UiO‐66‐(COOH) 2 catalyst also exhibits exceptional reusability and excellent substrate generality, highlighting its promising potential for further biomass utilization.

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Characterizations of the heterodimensional-bilayer tin perovskites prepared with SnF2+Trp additives
a, Top-view SEM images with different magnifications. The scale bars represent 1 μm. b, Cross-sectional iDPC-STEM image and the enlarged image with FFT analyses. The lattice constant of ∼0.63 nm is corresponding to the (100) interplanar spacing of the 3D tin iodide perovskite. The scale bars represent 10 nm. c, Cross-sectional DPC-STEM image. The lattice fringe with a spacing of ∼2.2 nm is corresponding to the (002) plane of the 2D (n = 2) tin iodide perovskite. The scale bar represents 20 nm. The dark region in the 3D perovskite layer can be attributed to the film degradation under electron beam exposure. d, Absorption and PL (front/back side excitation) spectra of the perovskite film. e, XRD pattern shows the co-existence of 3D and 2D perovskites. Octothorpe mask denotes the signal of ITO substrate. f, Comparison of (001) XRD peaks of 3D perovskite in our 2D/3D tin perovskite film and those of FASnI3, FA0.9Cs0.1SnI3, FA0.3Cs0.7SnI3 and CsSnI3 perovskites.
GIWAXS data analysis of the heterodimensional-bilayer tin perovskite film
Schematic assignment of the GIWAXS patterns, suggesting that the 2D perovskites are mainly horizontally oriented. The strong Bragg spots suggest that the 3D perovskite has a highly-ordered and vertically-orientated crystal packing. The incident angles (α) of 0.1° and 0.3° corresponds to the penetration depth of 3-5 nm and > 100 nm, respectively.
Additional structure characterizations of the hetero-dimensional-bilayer tin perovskite film
a, XRD patterns of the film before and after transfer. b, Top view SEM image of the film transferred on a TEM copper grid. The scale bar represents 1 μm. These results suggest that the transferred film has the same 2D/3D structure as the spin-coated film on an ITO substrate.
Analysis of the lattice alignment of 2D and 3D perovskites
a-b, TEM images and corresponding SAED patterns of typical 2D (n = 1) (PEA)2SnI4 perovskite film with different positions (a) and (b). The SAED patterns are assigned to the triclinic (PEA)2SnI4 (ref. ¹³). The scale bars in TEM images represent 500 nm. c, Simulated ED patterns of the 3D, 2D (n = 1), and 3D/2D overlapped lattices viewed along the [001] direction. The lattice parameters were taken from the literature (ref. 11,13). It is shown that the diffraction spots of (110), (11̅\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\bar{1}$$\end{document}0), and (200) planes of 3D perovskite are overlapped with those of (200), (020), and (220) planes of 2D perovskite respectively, which is consistent with our experimental data. This suggests that the lattices of our 3D and 2D perovskites are well-aligned in the in-plane direction.
Additional device characteristics of the heterodimensional-bilayer tin perovskite LEDs
a, Angular distribution of the radiation intensity of device, which follows a Lambertian profile. b, EL spectra at different viewing angles. c, Histogram of peak EQEs. Statistics from 94 devices show an average peak EQE of 9.9% with a relative standard deviation of 8.4%.

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Spin coating epitaxial heterodimensional tin perovskites for light-emitting diodes
  • Article
  • Full-text available

January 2024

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331 Reads

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8 Citations

Nature Nanotechnology

Environmentally friendly tin (Sn) perovskites have received considerable attention due to their great potential for replacing their toxic lead counterparts in applications of photovoltaics and light-emitting diodes (LEDs). However, the device performance of Sn perovskites lags far behind that of lead perovskites, and the highest reported external quantum efficiencies of near-infrared Sn perovskite LEDs are below 10%. The poor performance stems mainly from the numerous defects within Sn perovskite crystallites and grain boundaries, leading to serious non-radiative recombination. Various epitaxy methods have been introduced to obtain high-quality perovskites, although their sophisticated processes limit the scalable fabrication of functional devices. Here we demonstrate that epitaxial heterodimensional Sn perovskite films can be fabricated using a spin-coating process, and efficient LEDs with an external quantum efficiency of 11.6% can be achieved based on these films. The film is composed of a two-dimensional perovskite layer and a three-dimensional perovskite layer, which is highly ordered and has a well-defined interface with minimal interfacial areas between the different dimensional perovskites. This unique nanostructure is formed through direct spin coating of the perovskite precursor solution with tryptophan and SnF2 additives onto indium tin oxide glass. We believe that our approach will provide new opportunities for further developing high-performance optoelectronic devices based on heterodimensional perovskites.

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Assembly of Multisurfaced Van der Waals Layered Compound GaSe via Thermal Oxidation

September 2023

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146 Reads

Advanced Functional Materials

Advanced Functional Materials

The investigation of the oxidation behavior of van der Waals chalcogenides holds significant importance in terms of preventing and controlling oxidation, utilizing surface oxidation structures to regulate properties, and advancing applications. Here, taking GaSe as a candidate, its thermal oxidation and surface structure evolution are intensively studied. Through systematic microscopic analyses, oxidized structures at multi‐scale (from atomic scale to millimeters) are resolved, and various assembly heterogeneous surfaces including Ga2Se3/Ga2O3 and Ga2O3 multilayers are uncovered at different oxidation temperatures. The temperature‐dependent oxidation behavior and surface structure evolution of the GaSe are revealed, and the oxidation mechanisms in the entire temperature range are also disclosed. Finally, the photoluminescence regulation of the GaSe is initially explored via thermal oxidation, demonstrating great potential for surface oxidation engineering. This study is not only of great importance for the deep understanding and utilization of GaSe oxidation, but also beneficial for materials/device design and development of relative systems.


A Customized Hydrophobic Porous Shell for MOF-5

August 2023

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68 Reads

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7 Citations

Journal of the American Chemical Society

The susceptibility to moisture of metal-organic frameworks (MOFs) is a critical bottleneck for their wider practical application. Constructing core-shell composites has been postulated as an effective strategy for enhancing moisture resistance, but for fragile MOFs this has rarely been accomplished. We report herein, for the first time, the construction of a customized hydrophobic porous shell, NTU-COF, on the particularly fragile MOF-5 by a "Plug-Socket Anchoring" strategy. Notably, the pore structure of MOF-5 was well maintained, and it could still achieve complete CO2/N2 separation under humid conditions. The homogeneous interface between MOF-5 and NTU-COF has been inspected at atomic resolution by a combination of cryogenic focused ion beam (cryo-FIB) and ultralow-dose (scanning) transmission electron microscope giving profound insight into the mechanism of assembly of the core-shell structure. This work presents a facile strategy for the fabrication of a hydrophobic porous shell for labile MOFs, and provides a general approach for solving the problem of moisture instability of porous materials for practical applications.


Structural characterizations of the bottom-up 2D/3D heterojunction at the buried interface
a, TOF-SIMS profile of ITO/NiOx/PTAA/Al2O3/perovskite with bottom-up 2D/3D perovskite heterojunction at buried interface (2D spacer species: CN⁻ and Cl⁻, ammonium salt: CN⁻). The 2D perovskites are located in the region between the vertical orange dashed lines. b, 2D GIWAXS mappings of the control and target perovskite films with different incidence angles. c, PL spectra of the target perovskite film obtained from different incident directions. The inset shows the zoomed-in image between wavelengths of 550 and 750 nm. The perovskite films were deposited on ITO/NiOx/PTAA/Al2O3 substrate. d, Cross-sectional HRTEM image of the target PSC. The inset shows the enlarged TEM image of the region enclosed by a yellow box. The areas enclosed by the dashed white lines show the formed 2D perovskite. The distances measured show the lattice parameters for 3D and 2D perovskites. e, Device configuration of the inverted PSCs with bottom-up 2D/3D perovskite heterojunction at the buried interface.
Charge-carrier dynamics
a,b, TRPL spectra of the control and target perovskite films deposited on a bare glass substrate (a) and glass/NiOx/PTAA/Al2O3 substrate (b). TRPL measurements were conducted with excitation from the glass side and with an emission wavelength of 810 nm. The solid line shows the fitting curves. To simulate the TRPL data, we used a model based on the continuity equation for the carrier concentration n(z, t): ∂n∂t=D∂2n∂z2−k1n−k2n2−k3n3\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\frac{\partial n}{\partial t}\,=\,D\,\frac{{\partial }^{2}n}{{\partial z}^{2}}\,-\,{k}_{1}\,n\,-\,{k}_{2}\,{n}^{2}-{k}_{3}\,{n}^{3}$$\end{document}, where D is the carrier diffusion coefficient, k1 the non-radiative monomolecular bulk recombination constant, k2 the radiative bimolecular recombination constant and k3 the Auger coefficient. c,d, TRS measurements for the control (c) and target (d) perovskite films on NiOx/glass substrate. TRS measurements were performed with excitation from the glass side. The solid line shows the fitting curves. The details of the fits are provided in Methods. Norm ΔR, normalized change in reflection.
Device performance and stability
a, PCE histogram of 20 PSCs with (target) and without (control) bottom-up 2D/3D heterojunction at buried interface. The solid line is a Gauss peak fit of the distribution. b, J–V curves obtained in forward and reverse scans of the champion target PSCs. The insets show the relevant photovoltaic parameters. c, Comparison of the photovoltaic performance of the inverted PSC in this work with literature that reported PCEs over 23% (refs. 4,6–8,11,12,14–16,55). More details are shown in Supplementary Table 4. d, J–V curve of the best-performing target device with an area of 1 cm². The insets show the relevant photovoltaic parameters. e, PCE of the unencapsulated control and target devices measured at maximum power point under continuous one-sun illumination at 55 ± 5 °C in N2 atmosphere. The initial PCE of control, target-1 and target-2 devices is 21.73%, 24.42% and 24.11%, respectively. f, Damp-heat stability of the encapsulated control and target devices following the ISOS standards (85 °C and 85% RH). The initial PCE of control and target devices is 22.15 ± 0.13% and 24.32 ± 0.20%. The error bar is the standard deviation of three devices. Data are presented as mean values ± s.e.m.
Source data
2D/3D heterojunction engineering at the buried interface towards high-performance inverted methylammonium-free perovskite solar cells

July 2023

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905 Reads

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111 Citations

Nature Energy

The main bottlenecks limiting the photovoltaic performance and stability of inverted perovskite solar cells (PSCs) are trap-assisted non-radiative recombination losses and photochemical degradation at the interface between perovskite and charge-transport layers. We propose a strategy to manipulate the crystallization of methylammonium-free perovskite by incorporating a small amount of 2-aminoindan hydrochloride into the precursor inks. This additive also modulates carrier recombination and extraction dynamics at the buried interface via the formation of a bottom-up two-dimensional/three-dimensional heterojunction. The resultant inverted PSC achieves a power conversion efficiency of 25.12% (certified 24.6%) at laboratory scale (0.09 cm²) and 22.48% at a larger area (1 cm²) with negligible hysteresis. More importantly, the resulting unencapsulated devices show superior operational stability, maintaining >98% of their initial efficiency of >24% after 1,500 hours of continuous maximum power point tracking under simulated AM1.5 illumination. Meanwhile, the encapsulated devices retain >92% of initial performance for 1,200 hours under the damp-heat test (85 °C and 85% relative humidity).




Topological Isomerism in Three-Dimensional Covalent Organic Frameworks

April 2023

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75 Reads

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29 Citations

Journal of the American Chemical Society

Although isomerism is a typical and significant phenomenon in organic chemistry, it is rarely found in covalent organic framework (COF) materials. Herein, for the first time, we report a controllable synthesis of topological isomers in three-dimensional COFs via a distinctive tetrahedral building unit under different solvents. Based on this strategy, both isomers with a dia or qtz net (termed JUC-620 and JUC-621) have been obtained, and their structures are determined by combining powder X-ray diffraction and transmission electron microscopy. Remarkably, these architectures show a distinct difference in their porous features; for example, JUC-621 with a qtz net exhibits permanent mesopores (up to ∼23 Å) and high surface area (∼2060 m2 g-1), which far surpasses those of JUC-620 with a dia net (pore size of ∼12 Å and surface area of 980 m2 g-1). Furthermore, mesoporous JUC-621 can remove dye molecules efficiently and achieves excellent iodine adsorption (up to 6.7 g g-1), which is 2.3 times that of microporous JUC-620 (∼2.9 g g-1). This work thus provides a new way for constructing COF isomers and promotes structural diversity and promising applications of COF materials.


Citations (15)


... However, high k and the low σ are still major issues. Therefore, research on further developing SnSe 2 for TE or other applications is on-going [49][50][51][52][53][54][55]. ...

Reference:

Suppressing the thermal conductivity to enhance the thermoelectric performance of SnSe2 using the high-energy ball milling in a pressurised N2 atmosphere
Phase-dependent microstructure modification leads to high thermoelectric performance in n-type layered SnSe2
  • Citing Article
  • November 2023

Acta Materialia

... Hybrid perovskite solar cells embody a convergence of organic and inorganic components within the perovskite structure, presenting a promising avenue for efficient, cost-effective, and scalable solar energy harvesting [6,7]. Their capacity to tailor bandgaps, exhibit high absorption coefficients, and undergo processing through solution-based methods positions these solar cells at the forefront of potentially revolutionizing the renewable energy landscape [8,9]. This introduction lays the foundation for an in-depth exploration of hybrid perovskite solar cells, emphasizing their key characteristics and transformative impact on the renewable energy sector [10,11]. ...

2D/3D heterojunction engineering at the buried interface towards high-performance inverted methylammonium-free perovskite solar cells

Nature Energy

... [40] However, compared to nGeTe-mSb 2 Te 3 , the thermoelectric properties of nGeTe-mBi 2 Te 3 , such as GeBi 2 Te 4 , have received less attention, despite its tunability to exhibit both p-type and n-type transport. [41][42][43] The detailed crystal structure of nGeTe-mBi 2 Te 3 has not been extensively investigated. Understanding the crystal structure is crucial for comprehending the dominant mechanisms, which govern the carrier or phonon transport. ...

In-doping induced resonant level and thermoelectric performance enhancement in n-type GeBi2Te4 single crystals with intrinsically low lattice thermal conductivity
  • Citing Article
  • May 2023

... [16] Due to the same reason, the building units like 2,4,6tris(phenyl)benzene, 1,4-bimethyl-2,3,5,6-tetra-(phenyl)benzene, or hexa(phenyl)benzene with twisting planar configuration have also been employed to build 3D COFs with topologies of fjh, [17] pto, [18] mhq, [18] pts, [19] or she. [20] This is also true for the building blocks of triptycene, bicarbazole, organic cages or hexaphenyltriphenylene with relatively high connectivity, leading to 3D COFs with topologies of stp, [21] ceq, [22] dia, [23] qtz, [24] acs, [25] and nia. [26] In addition, the assembly between secondary building blocks through rigid linkages is used to construct 3D COFs with nbo, [27] rra, [28] and srs [29] nets. ...

Topological Isomerism in Three-Dimensional Covalent Organic Frameworks
  • Citing Article
  • April 2023

Journal of the American Chemical Society

... at −0.1 V. The bands at 1408 cm −1 and 1358 cm −1 were attributed to the characteristic vibration bands of carbonate () indicated that M-PtBiMo IMSs cleaved C-C bonds to achieve the desired 10-electron complete oxidation of EG while providing a higher energy conversion efficiency (CH 2 OH-CH 2 OH + 14OH − / 2CO 3 2− + 10H 2 O + 10e − ).49,50 ...

Subnanoscale Dual-Site Pd-Pt Layers Make PdPtCu Nanocrystals CO-Tolerant Bipolar Effective Electrocatalysts for Alcohol Fuel Cell Devices
  • Citing Article
  • April 2023

Nano Letters

... Precisely, the TOF of Ru@ SCC-KU was estimated to be 0.44 H 2 s −1 at 50 mV, which was higher than that of Ru/C (0.33 H 2 s −1 ) and Pt/C (0.38 H 2 s −1 ). These values confirm that Ru@SCC-KU is an excellent commercial catalyst and competitive HER activity with other reported electrocatalysts 38,56 . ...

Boosting alkaline hydrogen evolution performance by constructing ultrasmall Ru clusters/Na+, K+-decorated porous carbon composites
  • Citing Article
  • March 2023

Nano Research

... This being the case, in contrast to MOFs, the topologies of 3D COFs is limited till date to 24. The majority of the 3D COF topologies such as dia, 31 qtz, 32 bor, 33 ctn, 33 pts, 34 lon, 35 rra, 36 and ljh 37 are based on tetrahedral (Td, 4-connected) building units. Triangular prism (D3h, 6-connected) based building units have also been successfully used in the construction of many 3D COF topologies viz. ...

Topological Isomerism in Three-Dimensional Covalent Organic Frameworks

... In the transformation of biomass-derived polyols, humins formation from side reactions which is liable to occur during C6 sugar alcohols hydrogenolysis is a serious problem because high-temperature reactions are required for the hydrogenolysis of C-O bonds due to the strong bond even with noble metals. 44,45 Moreover, the selective transformation of polyols such as sorbitol and glucose to diols and triols is difficult because polyols have many OH groups with similar reactivities in the flexible alkyl chain. In contrast, isosorbide has two different functional groups like two secondary OH groups and four ether bonds in the rigid structure, and the reactivity difference of these functional groups can be used for the selective transformation. ...

Significant promotion of MgO in bifunctional Pt-WO -MgO catalysts for the chemoselective conversion of glucose to lower polyols
  • Citing Article
  • January 2023

Catalysis Communications

... 正丁烷分子结构相对稳定, C-C 键键能较高, 难以有效利用, 目前大部分作为低价值燃料烧掉, 化 工 利 用 率 较 低 [1] 。 全 球 正 面 临 石 化 资 源 短 缺 问 题, 将正丁烷转化成乙烯、 丙烯、 丁烯和丁二烯等具 有高附加值的轻烯烃具有较高的经济意义。同时, 正丁烷的转化研究也具有重要的科学意义, 因为轻 质烷烃的 C-C 和 C-H 键的有效活化一直是一个 有待解决的关键科学问题 [2] 。因此, 针对正丁烷的 催化裂解研究显得非常重要。 目前, 正丁烷催化裂解催化剂主要有金属氧化 物催化剂 [3,4] 和分子筛催化剂 [5] 。由于正丁烷结构相 对稳定、 C-C 键键能较高, 金属氧化物催化剂催化 正丁烷转化所需反应温度通常在 700°C 以上 [6] 。为 降低金属氧化物催化剂的反应温度, 通常在反应中 引入气相氧分子 [7][8][9] , 氧活化后的 C-H 键容易断裂 及氧可以降低反应活化能 [10] , 从而降低正丁烷发生 催化裂解所需温度。但是气相氧分子存在很容易 导致深度氧化反应产生更多的 CO x , 降低目的烯烃 选择性 [11] 。纯分子筛催化剂活化正丁烷能力较弱, 研究发现烯烃比烷烃更容易发生催化裂解反应 [12] 。 因此, 在 ZSM-5 分子筛上引入脱氢位点, 有利于提 高丁烷的转化率和烯烃选择性 [13][14][15] 。丁烷先在脱氢 位点上发生脱氢反应, 生成的丁烯在分子筛的酸性 位点上进行裂解反应, 从而提高丁烷的转化率和烯 烃选择性 [13] 。但是在分子筛上引入脱氢金属, 易发 生氢转移、 芳烃化等副反应, 而且在金属改性分子 筛的过程中容易对分子筛的骨架结构造成破坏, 影 响其催化活性 [16] 。近年来, 二氧化铈基复合氧化物 在烷烃的脱氢和裂解方面引起了广泛关注 [17][18][19][20][21][22] 。二 氧化铈基复合氧化物具有优异的储氧性能, 通过 Ce 4+ 还原 Ce 3+ 释放氧空位吸附的活性氧 [23] 。活性氧 参与反应时, 可以活化烷烃分子, 降低反应活化能, 提高烷烃的转化能力。二氧化铈基复合氧化物还 具有酸性位点 [21,[23][24] [25][26][27][28][29][30][31][32][33][34] 。然而单纯 Pt 呈现出较低脱氢性能 和快速失活等缺点, 在 Pt 基催化剂上添加金属 Ga 能 够显著改善金属 Pt 的脱氢性能 [35][36][37][38][39][40][41] 。这是由于 Ga 的存在, 增加了表面 Pt 活性中心的电子密度, 降低 了烯烃脱附能 [35,37] 。Ga 还增加了氧化物表面与 Pt 纳 米颗粒之间的相互作用, 起到隔离 Pt 活性中心、 增 加表面原子的流动性, 抑制 Pt 的烧结失活 [40] 。而且, 研究表明在 CeO 2 上引入 Ga, 可以提高 CeO 2 的还原 能力和储氧性能, 改善氧迁移率 [42,43] ...

Dehydrogenation of Propane and n -Butane Catalyzed by Isolated PtZn 4 Sites Supported on Self-Pillared Zeolite Pentasil Nanosheets
  • Citing Article
  • August 2022

ACS Catalysis

... MEA performance is also affected by the way that the catalyst layer is fabricated, and significant research efforts have been exerted in investigating novel fabrication procedures [22][23][24][25][26][27]. Tsai et al. placed Pt-Ru nanoparticles in dense carbon nanotubes that directly grow on carbon cloth, and this method decreased the Pt-Ru load to 0.4 mg cm −2 and increased the power density by 27% [23]. ...

Interface-rich Au-doped PdBi alloy nanochains as multifunctional oxygen reduction catalysts boost the power density and durability of a direct methanol fuel cell device
  • Citing Article
  • April 2022

Nano Research