Superlattice formation from polydisperse ag nanoparticles by a vapor-diffusion method.
Superlattice formation from polydisperse ag nanoparticles by a vapor-diffusion method.
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DOI:
10.1002/anie.200601233
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发表时间:
2006-08
影响因子:
--
通讯作者:
Yang Yang-Yang;Shu-man Liu;K. Kimura
中科院分区:
文献类型:
--
作者:
Yang Yang-Yang;Shu-man Liu;K. Kimura
Plenteous development of synthetic methods affords more and more possibilities to endow nanoparticles with controlled morphology and surface properties that can be manipulated as “artificial atoms”. Assembly of these nanoparticles would provide an opportunity to investigate and further tailor their collective physical properties.[1] Superlattice formation by metal or semiconductor nanoparticles is currently being explored by strategies of bottomup assembly, which include solvent evaporation of metal nano-organosols on a substrate,[1, 2] crystallization of nanoparticles from bulk solution by sedimentation or precipitation,[3] wet deposition by supramolecular interactions between the nanoparticles and a surface,[2d, 4] and organization of nanoparticles at oil/water interfaces.[5] In most cases, obtaining superlattice structures strongly depends on highly monodisperse nanoparticles as building blocks. Recently, we reported that hydrophilic metal nanoparticles are excellent components for formation of two-or three-dimensional (2D or 3D) superlattices at the air/water interface by adjusting the concentration of the electrolyte.[6] Herein, we use hydrophilic mercaptosuccinic acid (MSA)-capped Ag nanoparticles as an example and report facile superlattice formation by vapor diffusion of hydrogen chloride (HCl) into their bulk aqueous solution. This new approach can induce the construction of perfect superlattice structure at air/water interfaces under relatively mild conditions and, in particular, high monodispersity of the initial nanoparticle ensemble is not strictly required.A transmission electron microscopy (TEM) image of the as-prepared MSA-capped Ag nanoparticles (Figure 1a) and their size histogram (Figure 1b) show that they are roughly spherical with an average diameter of 4.8 nm. The full width at half-maximum (fwhm) calculated from the distribution is about 1.4 nm, so the size polydispersity is up to 29%. The