搜索

x

留言板

尊敬的读者、作者、审稿人, 关于本刊的投稿、审稿、编辑和出版的任何问题, 您可以本页添加留言。我们将尽快给您答复。谢谢您的支持!

姓名
邮箱
手机号码
标题
留言内容
验证码

Au@Ag纳米长方体形貌调控的研究

王致远 张慧

引用本文:
Citation:

Au@Ag纳米长方体形貌调控的研究

王致远, 张慧

Study on the morphology control of Au@Ag nanocuboids

WANG Zhiyuan, ZHANG Hui
Article Text (iFLYTEK Translation)
PDF
导出引用
  • 金核银壳(Au@Ag)纳米颗粒兼具金的稳定性、生物相容性及银的优异电磁响应特性,在纳米医学、环境保护、传感和光学等领域具有重要应用价值。Au@Ag纳米长方体因其结构的各向异性,特别是表面等离激元共振(SPR)效应,在基础科学研究中扮演着重要角色。本研究通过晶种法,即在水相中调控Au纳米棒种子的尺寸、长径比(AR)及Ag前驱体用量,制备了形貌、尺寸与光学性质均可控的Au@Ag纳米长方体。实验表明,当Au纳米棒直径大于100 nm时,Au@Ag纳米长方体的顶角出现截断;当Au纳米棒直径小于100 nm时,Au@Ag纳米长方体的顶角随Au纳米棒AR的减小而变得更尖(~90°)。值得注意的是,当Au纳米棒的AR在一定范围内(~1.39到~3.15)时,均可生长形貌良好(顶角尖锐)的Au@Ag纳米长方体,这一发现为研究纳米长方体顶角的变化提供了一定参考。另外,纳米长方体的长度(~110 nm到~141 nm)与宽度(~60 nm到~104 nm)可通过调节硝酸银的量实现精准调控。同时,模拟计算结果表明,相对于纳米棒而言,Au@Ag纳米长方体不仅具有丰富的多级SPR模式,其尖角可产生巨大的电场增强。本研究进一步拓展了其在多个高科技产业中的应用前景。
    Au@Ag core-shell nanoparticles have emerged as promising platforms for photonic applications due to their synergistic integration of gold’s biocompatibility and silver’s exceptional plasmonic properties. And Nanoparticles with sharp corners exhibit electron accumulation at the tips under electromagnetic fields, generating enhanced localized electric fields. This phenomenon facilitates their applications in surface-enhanced Raman spectroscopy (SERS) and strong coupling interactions, among other fields. So, when Au@Ag core-shell nanoparticles coupled with sharp corners, there will be outstanding performance in trace molecule detection, biosensing and catalytic applications. This study systematically investigates the seed-mediated synthesis of Au@Ag nanocuboids with tunable morphology, size and surface plasmon resonance (SPR) by using gold nanorod (AuNR) seeds with different dimensions and adjusting the volume of silver precursors. Key synthesis parameters, including AuNR diameters, aspect ratios and AgNO3 volumes, are modulated to achieve morphological, size and optical control. In experiments adjusting the size of AuNR seeds for synthesizing Au@Ag nanocuboids, as the diameter of AuNR decreases from 136.5±5 nm to 11.2±2 nm and the aspect ratio increases from 1.39 to 8.20, the aspect ratio of Au@Ag nanocuboids increases from 1.18 to 2.69. Notably, when the diameter of AuNR is below 100 nm, the sharpness of the corners of Au@Ag nanocuboids progressively improves with increasing diameter and decreasing aspect ratio of the AuNRs. However, when the AuNR diameter exceeds 100 nm, the corners of the synthesized Au@Ag nanocuboids exhibit truncation. Meanwhile, the extinction spectrum reveals that, apart from the broadened and indistinct peaks caused by the size effect, Au@Ag nanocuboids can primarily excite the longitudinal plasmon resonance mode, transverse plasmon resonance mode, and octupolar plasmon resonance modes. Furthermore, the plasmon resonance peaks exhibit corresponding shifts in response to changes in the size and morphology of Au@Ag nanocuboids. Meanwhile, neither the characterization results of high-resolution transmission electron microscopy (HRTEM) nor selected area electron diffraction (SAED) can observe {111} crystal planes, indicating that the Au@Ag nanocuboids with the sharpest corners remains untruncated and exhibits an exceptional morphology. And high-angle annular dark-field scanning transmission electron microscopy (HAADF-STEM) combined with energy-dispersive X-ray spectroscopy (EDS) characterization reveals that the silver shell exhibits anisotropic growth features on the gold core, with its transverse thickness being significantly greater than the longitudinal thickness. Besides, Au@Ag nanocuboids dimensions are linearly regulated by the volume of AgNOO3 (100 mM) from 5 μL to 30 μL, yielding tunable lengths (110.3 ±7.8 nm to 141.3 ±5.5 nm), widths (59.7 ±2.1 nm to 103.7 ±5.6 nm), aspect ratios (1.85 to 1.36) and corresponding plasmon resonance peaks as validated by SEM and extinction spectrum. The simulation results of their extinction spectra are in better agreement with the experimental measurements, and for the nanocuboid with aspect ratio of 1.45, the strength of the electric field at the corners shows a tendency to be enhanced and then weakened with the decreasing of the sharpness of the top corners (r/L = 0.2% - 11.5%), in which the strength of the electric field enhancement is greatest at r/L = 0.5%.
    This work synthesizes Au@Ag nanocuboids with controllable sharpness of corners and dimension by adjusting the size and aspect ratio of AuNRs or changing the amount of silver precursors. The method proposed in this study for synthesizing sharp-cornered Au@Ag nanocuboids provides possibilities for customized fabrication of Au@Ag nanocuboids, thereby expanding their application prospects in nanophotonics, catalysis, sensing, photothermal therapy and other fields.
  • [1]

    Mendez E, Fagundez P, Sosa P, Gutierrez M V, Botasini S 2021 Nanotechnology 32 045603

    [2]

    Bi C, Yin X, Zhao H 2024 RSC Adv. 14 20145

    [3]

    Xiong L, Ding H W, Li G Y 2022 Acta Phys. Sin. 71 047802(熊磊,丁洪伟,李光 元.银纳米粒子阵列中衍射诱导高品质因子的四偶极晶格等离子体模式2022物 理学报71 047802)

    [4]

    Lee D, Yoon S 2016 J. Phys. Chem. C 120 20642

    [5]

    McLellan J M, Siekkinen A, Chen J, Xia Y 2006 Chem. Phys. Lett. 427 122

    [6]

    Rycenga M, Camargo P H, Li W, Moran C H, Xia Y 2010 J. Phys. Chem. Lett. 1 696

    [7]

    Zhong J, Li J Y, Liu J, Xiang Y, Feng H, Liu R, Li W, Wang X H 2024 Nano Lett. 24 1579

    [8]

    Li J, Wang Q, Wang J, Li M, Zhang X, Luan L, Li P, Xu W 2021 Anal. Bioanal. Chem. 413 4207

    [9]

    Lin S, Guan H, Liu Y, Huang S, Li J, Hasi W, Xu Y, Zou J, Dong B 2021 ACS Appl. Mater. Interfaces 13 53289

    [10]

    Ma Y, Li W, Cho E C, Li Z, Yu T, Zeng J, Xie Z, Xia Y 2010 ACS Nano 4 6725

    [11]

    Liu K-K, Tadepalli S, Tian L, Singamaneni S 2015 Chem. Mater. 27 5261

    [12]

    Xing C, Zhong S, Yu J, Li X, Cao A, Men D, Wu B, Cai W, Li Y 2020 J. Mater. Chem. C 8 3838

    [13]

    Cho E C, Camargo P H C, Xia Y 2010 Adv. Mater. 22 744

    [14]

    Zheng Y, Zhong X, Li Z, Xia Y 2013 Part. Part. Syst. Char. 31 266

    [15]

    Sanchez-Iglesias A, Winckelmans N, Altantzis T, Bals S, Grzelczak M, Liz-Marzan L M 2017 J. Am. Chem. Soc. 139 107

    [16]

    Park J E, Lee Y, Nam J M 2018 Nano Lett. 18 6475

    [17]

    Lin S, Lin X, Han S, He L, Zhao H, Zhang J, Hasi W, Wang L 2019 J. Alloys Compd. 805 318

    [18]

    Okuno Y, Nishioka K, Kiya A, Nakashima N, Ishibashi A, Niidome Y 2010 Nanoscale 2 1489

    [19]

    Park K, Drummy L F, Vaia R A 2011 J. Mater. Chem. 21 15608

    [20]

    Tebbe M, Kuttner C, Mayer M, Maennel M, Pazos-Perez N, König T A F, Fery A 2015 J. Phys. Chem. C 119 9513

    [21]

    Jiang R, Chen H, Shao L, Li Q, Wang J 2012 Adv. Mater. 24 OP200

    [22]

    Vernier C, Portalès H 2024 J. Chem. Phys. 161 124711

    [23]

    Hamon C, Constantin D 2020 J. Phys. Chem. C 124 21717

    [24]

    Chang S T, Dong W Y, Chen K C, He Y, Yen Y A, Kao C W, Deng J P 2021 J. Chin. Chem. Soc. 68 512

    [25]

    He B, Liu X, Chen L 2023 Nano Lett. 23 3963

    [26]

    Gómez-Graña S, Goris B, Altantzis T, Fernández-López C, Carbó-Argibay E, Guerrero-Martínez A, Almora-Barrios N, López N, Pastoriza-Santos I, Pérez-Juste J, Bals S, Van Tendeloo G, Liz-Marzán L M 2013 J. Phys. Chem. Lett. 4 2209

    [27]

    Ye X, Zheng C, Chen J, Gao Y, Murray C B 2013 Nano Lett. 13 765

    [28]

    Vigderman L, Zubarev E R 2013 Chem. Mater. 25 1450

    [29]

    Thambi V, Kar A, Ghosh P, Paital D, Gautam A R S, Khatua S 2019 ACS Omega 4 13733

    [30]

    da Silva J A, Netz P A, Meneghetti M R 2025 J. Chem. Inf. Model. 65 2730

    [31]

    da Silva J A, Netz P A, Meneghetti M R 2020 Langmuir 36 257

    [32]

    Jing H, Zhang Q, Large N, Yu C, Blom D A, Nordlander P, Wang H 2014 Nano Lett. 14 3674

    [33]

    Jiang R, Chen H, Shao L, Li Q, Wang J 2012 Adv. Mater. 24 OP200

    [34]

    Hamasaki Y, Nakashima N, Niidome Y 2012 J. Phys. Chem. C 117 2521

    [35]

    Xia Y, Xia X, Peng H C 2015 J. Am. Chem. Soc. 137 7947

    [36]

    Herrmann L O, Baumberg J J 2013 Small 9 3743

    [37]

    König T, Kodiyath R, Combs Z A, Mahmoud M A, El-Sayed M A, Tsukruk V V 2013 Part. Part. Syst. Char. 31 274

    [38]

    Liu M, Pang Y, Zhang B, De Luna P, Voznyy O, Xu J, Zheng X, Dinh C T, Fan F, Cao C, de Arquer F P G, Safaei T S, Mepham A, Klinkova A, Kumacheva E, Filleter T, Sinton D, Kelley S O, Sargent E H 2016 Nature 537 382

    [39]

    Pena-Rodriguez O, Diaz-Nunez P, Gonzalez-Rubio G, Manzaneda-Gonzalez V, Rivera A, Perlado J M, Junquera E, Guerrero-Martinez A 2020 Sci. Rep. 10 5921

    [40]

    Guo P, Sikdar D, Huang X, Si K J, Xiong W, Gong S, Yap L W, Premaratne M, Cheng W 2015 Nanoscale 7 2862

    [41]

    Tan S F, Wu L, Yang J K W, Bai P, Bosman M, Nijhuis C A 2014 Science 343 1496

    [42]

    Pramod P, Thomas K G 2008 Adv. Mater. 20 4300

    [43]

    Li N, Han Z, Huang Y, Liang K, Wang X, Wu F, Qi X, Shang Y, Yu L, Ding B 2020 J. Mater. Chem. C 8 7672

    [44]

    Hu H, Zhang S, Xu H 2019 Phys. Rev. A 99 033815

    [45]

    Lee Y M, Kim S E, Park J E 2023 Nano Converg. 10 34

    [46]

    Yang X, Li J, Zhao Y, Yang J, Zhou L, Dai Z, Guo X, Mu S, Liu Q, Jiang C, Sun M, Wang J, Liang W 2017 Nanoscale 10 142

    [47]

    Li Y, Zhang Y, Xu J, Kan C, Li Z, Shi D 2024 CrystEngComm 26 5799

    [48]

    Yang T H, Ahn J, Shi S, Wang P, Gao R, Qin D 2021 Chem. Rev. 121 796

  • [1] 郑钦仁, 詹涪至, 折俊艺, 王建宇, 石若立, 孟国栋. 石墨烯的形貌特征对其场发射性能的影响. 物理学报, doi: 10.7498/aps.73.20231784
    [2] 李凯, 孙捷, 杜在发, 钱峰松, 唐鹏昊, 梅宇, 徐晨, 严群, 柳鸣, 李龙飞, 郭伟玲. 带有垂直石墨烯的金属热电堆红外探测器. 物理学报, doi: 10.7498/aps.72.20221564
    [3] 井建迎, 刘琨, 吴张羿, 刘玥萌, 江俊峰, 徐天华, 晏伟铖, 熊艺扬, 战晓寒, 肖璐, 刘津畅, 刘铁根. 基于紫磷增敏的即插即用式双通道光纤表面等离激元共振折射率计. 物理学报, doi: 10.7498/aps.72.20231110
    [4] 叶高杰, 殷澄, 黎思瑜, 俞强, 王贤平, 吴坚. 金属纳米颗粒双圆环阵列的表面格点共振效应. 物理学报, doi: 10.7498/aps.72.20230199
    [5] 李健康, 李睿. 利用数值模拟研究表面增强相干反斯托克斯拉曼散射增强基底. 物理学报, doi: 10.7498/aps.70.20201773
    [6] 李盼. 表面等离激元纳米聚焦研究进展. 物理学报, doi: 10.7498/aps.68.20190564
    [7] 朱旭鹏, 石惠民, 张轼, 陈智全, 郑梦洁, 王雅思, 薛书文, 张军, 段辉高. 表面等离激元耦合体系及其光谱增强应用. 物理学报, doi: 10.7498/aps.68.20190782
    [8] 冯仕靓, 王靖宇, 陈舒, 孟令雁, 沈少鑫, 杨志林. 表面等离激元“热点”的可控激发及近场增强光谱学. 物理学报, doi: 10.7498/aps.68.20190305
    [9] 万婷, 罗朝明, 闵力, 陈敏, 肖磊. 基于合金介电常数的可控特性增强光子自旋霍尔效应. 物理学报, doi: 10.7498/aps.67.20171824
    [10] 蒋行, 周玉荣, 刘丰珍, 周玉琴. 后退火处理对铟锡氧化物表面等离激元共振特性的影响. 物理学报, doi: 10.7498/aps.67.20180435
    [11] 黄运欢, 李璞. 金纳米棒复合体的消光特性. 物理学报, doi: 10.7498/aps.64.207301
    [12] 李萌, 牛贺莹, 姚路炎, 王栋梁, 周忠坡, 马恒. 胆甾液晶掺杂活性层对有机太阳能电池性能的影响. 物理学报, doi: 10.7498/aps.63.248403
    [13] 张兴坊, 闫昕. 金纳米球壳表面等离激元共振波长调谐特性研究. 物理学报, doi: 10.7498/aps.62.037805
    [14] 王玥, 刘丽炜, 胡思怡, 李其扬, 孙振皓, 苗馨卉, 杨小川, 张喜和. 基于COMSOL Multiphysics对Cu2S量子点的表面等离激元共振模拟研究. 物理学报, doi: 10.7498/aps.62.197803
    [15] 邹伟博, 周骏, 金理, 张昊鹏. 金纳米球壳对的局域表面等离激元共振特性分析. 物理学报, doi: 10.7498/aps.61.097805
    [16] 丛超, 吴大建, 刘晓峻, 李勃. 金银三层纳米管局域表面等离激元共振特性研究. 物理学报, doi: 10.7498/aps.61.037301
    [17] 杨振岭, 刘玉强, 杨延强. 银纳米颗粒对四苯基卟啉Q带荧光寿命的延长. 物理学报, doi: 10.7498/aps.61.037805
    [18] 丛超, 吴大建, 刘晓峻. 椭圆截面金纳米管的局域表面等离激元共振特性研究. 物理学报, doi: 10.7498/aps.60.046102
    [19] 方 方, 郑时有, 周广有, 陈国荣, 孙大林. 氢致LaMg2Ni合金薄膜的光电性能变化. 物理学报, doi: 10.7498/aps.57.3813
    [20] 王 浩, 曾谷城, 廖常俊, 蔡继业, 郑树文, 范广涵, 陈 勇, 刘颂豪. GaxIn1-xP缓冲层组分对InP自组装形貌影响的研究. 物理学报, doi: 10.7498/aps.54.1726
计量
  • 文章访问数:  25
  • PDF下载量:  2
  • 被引次数: 0
出版历程
  • 上网日期:  2025-06-12

/

返回文章
返回