无机材料学报 ›› 2026, Vol. 41 ›› Issue (10): 1481-1488.DOI: 10.15541/jim20260019
余俊龙1(
), 蒋胤2, 郭江涛2, 杨培志2, 冯小波1(
)
收稿日期:2026-01-13
修回日期:2026-02-11
出版日期:2026-10-20
网络出版日期:2026-04-03
通讯作者:
冯小波, 教授. E-mail: fengxiaobo1220@gmail.com作者简介:余俊龙(2000-), 男, 硕士研究生. E-mail: 1661815134@qq.com
基金资助:
YU Junlong1(
), JIANG Yin2, GUO Jiangtao2, YANG Peizhi2, FENG Xiaobo1(
)
Received:2026-01-13
Revised:2026-02-11
Published:2026-10-20
Online:2026-04-03
Contact:
FENG Xiaobo, professor. E-mail: fengxiaobo1220@gmail.comAbout author:YU Junlong (2000-), male, Master candidate. E-mail: 1661815134@qq.com
Supported by:摘要:
黑磷量子点(Black phosphorus quantum dots, BPQDs)因其可调的带隙与高载流子迁移率在能源领域备受关注, 但其高质量可控制备仍是当前技术瓶颈。本研究提出了一种基于微波辅助液相剥离技术的简便、低成本、高效的BPQDs合成策略, 并探究其在提升场效应直流发电机(Field-effect direct-current generator, FENG)性能中的应用。通过系统调控微波温度、时间及前驱体/溶剂配比, 筛选出最佳工艺参数为150 ℃, 6 h, 1 : 2。在此条件下, 成功制备出平均尺寸低至1.47 nm且分布均匀的高质量BPQDs。与传统方法相比, 该策略在制备效率及产物结构完整性方面均展现出显著优势。进一步地, 将所制备的BPQDs与导电聚合物PEDOT:PSS复合, 构建了FENG的活性摩擦层。实验结果表明, 引入BPQDs后, 器件的输出性能显著提升; 相较于纯PEDOT:PSS器件, 平均峰值电流提升43.6%; 系统研究还发现, 通过升高合成温度减小BPQDs尺寸, 可线性提升器件的输出电压、电流及电荷转移速率, 在150 ℃时获得最佳输出。性能提升可归因于超小BPQDs优异的电学特性及其大比表面积对界面极化与电荷存储的促进作用。本工作不仅为BPQDs的绿色、可控制备提供了高效新方法, 还通过柔性自供能系统应用, 展示了其在能源转换领域的广阔应用潜力。
中图分类号:
余俊龙, 蒋胤, 郭江涛, 杨培志, 冯小波. 微波辅助可控合成黑磷量子点增强PEDOT:PSS场效应直流发电机性能[J]. 无机材料学报, 2026, 41(10): 1481-1488.
YU Junlong, JIANG Yin, GUO Jiangtao, YANG Peizhi, FENG Xiaobo. Controlled Microwave-assisted Synthesis of Black Phosphorus Quantum Dots Boosting PEDOT:PSS Field-effect Direct-current Generator Performance[J]. Journal of Inorganic Materials, 2026, 41(10): 1481-1488.
图1 不同温度下制备的BPQDs的(a) TEM照片和(b)粒径分布图
Fig. 1 (a) TEM images and (b) particle size distribution histograms of BPQDs synthesized at different temperatures
图2 BPQDs的形态与结构表征
Fig. 2 Morphology and structural characterization of BPQDs (a) TEM image; (b) Magnified TEM image; (c) High resolution TEM images showing lattice fringes; (d) Lateral size distribution histogram measured from TEM images; (e) AFM topographic image; (f) Corresponding height profiles along the white line in (e); (g) Height (thickness) distribution histogram measured from AFM image. Colorful figures are available on website
图3 BP和BPQDs的结构与化学表征
Fig. 3 Structural and chemical characterization of bulk BP and BPQDs (a) Comparison of Raman spectra for bulk BP and BPQDs; (b) XPS full survey spectrum of BPQDs; (c) High-resolution XPS spectrum with peak deconvolution for the P2p region of BPQDs; (d) FT-IR spectrum of BPQDs
图4 FENG装置的原理与结构
Fig. 4 Working principle and structure of the FENG device (a) Electrostatic charge region; (b) Band bending in the non-contact region; (c) Band bending in the contact region; (d) Energy band diagram of the entire BPQDs/PEDOT:PSS surface; (e) Schematic of dynamic electrostatic charge inducing carrier transport in the BPQDs/PEDOT:PSS layer, leading to electrical energy generation in the external circuit; (f) Energy band diagram of the entire BPQDs/PEDOT:PSS surface when the rubber friction layer contacts the FEP film
图5 器件的电学性能测试
Fig. 5 Electrical characterization of devices (a) Effect of BPQDs on the electrical performance of the FENG; (b-d) Influence of BPQDs prepared at different temperatures on the FENG’s (b) voltage, (c) current, and (d) transferred charge
图S2 不同黑磷前驱体和无水乙醇配比下制备的BPQDs的(a) TEM照片和(b)粒径分布图
Fig. S2 (a) TEM images and (b) particle size distribution histograms of BPQDs prepared with different ratios of black phosphorus precursors to anhydrous ethanol
| Comparison dimension | Core filler | Filler characteristics | Composite films fabrication | Operating mode | Key advantages | Output performance | Outstanding mechanism | Ref. |
|---|---|---|---|---|---|---|---|---|
| BPQDs/ PEDOT:PSS | BPQDs | Zero-dimensional quantum dots (1.47 nm), Tunable size/ bandgap, strong quantum confinement effect | Solution mixing followed by spin-coating | Contact- separation mode | Linearly tunable performance and ultrasmall size with size-dependent charge transfer rate | Output voltage up to 800 V and 43.6% increase in average peak current | Establishing a “synthesis temperature-size- output performance” linear tunability: dominant role of quantum confinemen | This work |
| MXene/ PEDOT:PSS | MXene (Ti3C2Tx) | High conductivity, layered structure, large lateral size | Vacuum filtering | Contact- separation mode | Ultrahigh sensitivity, fast response, and device integration | Output voltage ~29.6 V (10 N) | Intimate interface facilitates charge transport for high-sensitivity sensing | [S1] |
| Graphene/ PEDOT:PSS | CVD graphene | 2D monolayer, high conductivity, PEDOT:PSS- modified interface | Spin-coating | Contact- separation mode | High transparency, high flexibility, and versatile surface engineering | Output voltage of 52 V and current density of 2.4 µA/cm2 | Enhanced electrode conductivity and work function for improved overall output | [S2] |
表S1 BPQDs与MXene作为PEDOT:PSS纳米填料的特性对比
Table S1 Comparison of the characteristics between BPQDs and MXene as nanofillers in PEDOT:PSS
| Comparison dimension | Core filler | Filler characteristics | Composite films fabrication | Operating mode | Key advantages | Output performance | Outstanding mechanism | Ref. |
|---|---|---|---|---|---|---|---|---|
| BPQDs/ PEDOT:PSS | BPQDs | Zero-dimensional quantum dots (1.47 nm), Tunable size/ bandgap, strong quantum confinement effect | Solution mixing followed by spin-coating | Contact- separation mode | Linearly tunable performance and ultrasmall size with size-dependent charge transfer rate | Output voltage up to 800 V and 43.6% increase in average peak current | Establishing a “synthesis temperature-size- output performance” linear tunability: dominant role of quantum confinemen | This work |
| MXene/ PEDOT:PSS | MXene (Ti3C2Tx) | High conductivity, layered structure, large lateral size | Vacuum filtering | Contact- separation mode | Ultrahigh sensitivity, fast response, and device integration | Output voltage ~29.6 V (10 N) | Intimate interface facilitates charge transport for high-sensitivity sensing | [S1] |
| Graphene/ PEDOT:PSS | CVD graphene | 2D monolayer, high conductivity, PEDOT:PSS- modified interface | Spin-coating | Contact- separation mode | High transparency, high flexibility, and versatile surface engineering | Output voltage of 52 V and current density of 2.4 µA/cm2 | Enhanced electrode conductivity and work function for improved overall output | [S2] |
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