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Ice template-assisted assembly of spherical PS-b-PAA micelles into novel layer-by-layer hollow spheres

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Novel microscale layer-by-layer hollow spheres are template-assembled by monodispersed spherical PS-b-PAA micelles during the sublimation of the frozen micellar solution.

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The aggregation of nanoscale building blocks, such as clusters,1 spheres,2,3 and superlattices,4–6 has attracted intense interest due to their importance in fundamental research and potential wide-ranging applications.

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To date, a wealthy of methods have been developed to assemble nanoparticles into two- and three-dimensional ordered aggregates, which offers opportunities to explore their novel collective optical, magnetic, and electronic properties.7–10

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For examples, Xia et al7. produced various uniform aggregates of spherical colloids following an approach combining physical template and capillary forces.

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Jenekhe and Chen11 obtained periodic structures assembled by poly(phenylquinoline)-block-polystyrene via solution evaporation.

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Stucky et al12. gained micro-sized hollow spheres co-assembled by silica and gold nanoparticles based on cysteine–lysine diblock copolypeptides.

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These novel structures have potential applications ranging from electro-optical devices 13,14 and separation membranes 15,16 to active biomaterial coating 17,18 and nano-reactors.18,19

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Our group has been studying the micellization of amphiphilic block copolymers and the ordered aggregation of the polymeric micelles.20,21

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Recently, we have prepared various morphological aggregates of micelles via different methods.21

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One strategy is to control ordered flower-like aggregation of micelles on a adjustable template of water polycrystal.

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The present study is focused on the formation of novel layer-by-layer hollow polymeric spheres by ice template-assisted aggregation of nanoscale micelles.

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To the best of our knowledge, this is the first report of obtaining such novel layer-by-layer hollow aggregates via such a simple and convenient method.

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The PS30-b-PAA51 micelles were firstly prepared as described elsewhere21 and characterized by dynamic laser scattering (DLS) and transform electronic microscopy (TEM).

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A drop of the aqueous micelle solution was first placed onto a clean glass slide and quickly frozen in liquid nitrogen.

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Then the ice in the frozen micellar sample was sublimated by freeze-drying under vacuum and the resultant samples were observed by scanning electron microscopy (SEM).

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Furthermore, the crystal formation process of pure water was monitored by polarized light microscopy (PLM).

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Fig. 1a shows the hydrodynamic diameter (Dh) distribution f(Dh) of the PS30-b-PAA51 micelles in aqueous solution obtained from DLS.

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Obviously, the diameter distribution of the micelles is monodispersed and the average Dh of the micelles is about 58 nm.

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Fig. 1b displays the TEM images of the micelles and we can clearly see the spherical shape of the micelles with about 40 nm in diameter.

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It must be noted that the hydrodynamic diameter Dh of the micelles measured by DLS is much larger than that observed by TEM.

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This is because the micelles are swollen in water due to the soluble PAA block, while TEM observation shows the dried aggregates.

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Usually, nanoparticles dispersed in water, such as the micelles shown in Fig. 1, aggregate to form random-shaped clusters when the water is removed.

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In order to achieve controlled aggregation of the nanoparticles, physical templates are usually used.7

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Can the solvent be used directly as a template to control the aggregation?

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To the best of our knowledge, liquid water is not a suitable candidate, but ice may be.

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Compared with other templates that can be added, the ice template can be formed and removed easily by freezing and sublimating.

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Fig. 2 gives the typical PLM image of the thin layer of ice template formed by freezing a drop of water in liquid nitrogen.

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The dark grid-like lines as shown in Fig. 2 divide the ice film into many micro-regions.

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These micro-regions are supposed to shrink gradually to form spherical micro-regions during the slow sublimation of H2O, which is similar to the sublimation of ice in winter.

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Thus, it is reasonable to think that ice as shown in Fig. 2 can be used as a template to guide the aggregation of the micelles.

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Herein, we aim to use this template to fulfil the controlled aggregation of the micelles shown in Fig. 1.

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Upon first rapidly freezing the micellar aqueous solution in liquid nitrogen and then freeze-drying, the resultant samples were observed by SEM and the SEM images are shown in Fig. 3.

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The resultant sample shown in Fig. 3a looks greatly different from the spheres in Fig. 1b.

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The most remarkable difference is the broken hollow spheres containing a cavity encapsulating a smaller spherical particle and the outer shell is about 100 nm in thickness, which can be seen in the insert-enlarged image in Fig. 3a.

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The fine structure of the shell can be seen in Fig. 3b.

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Obviously, the shell is formed by the packed small particles, which corresponds to the nanoscale spherical PS30-b-PAA51 micelles.

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These results confirm that the microscale layer-by-layer hollow spheres are just resulted from the assembly of the nanoscale PS30-b-PAA51 micelles.

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Thus, it can be concluded that the ice template plays a key role in the ordered assembly of the dispersed PS30-b-PAA51 micelles in water.

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According to what we have obtained above, we propose a schematic illustration of the ice template-assisted assembly of the nanoscale micelles into layer-by-layer hollow spheres in Fig. 4.

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The first step is to freeze the micellar solution instantly (A in Fig. 4), where the micelles are uniformly dispersed in the ice template.

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It should be noted out the ice template is divided into many micro-regions as schematically magnified in step B. Second, during the H2O sublimation process, the micro-regions in the ice template gradually shrink and become spherical and the micelles adhered to the surface of the micro-regions in the ice template are piled gradually into a three-dimensional (3D) spherical arrangement (B→C→D).

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Sublimation continuously, a spherical core-shell structure forms (E), where the shell is composed of the packed nanoscale PS30-b-PAA51 micelles and the core is still the frozen micellar solution.

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The further sublimation of H2O molecule existing in the frozen core results in formation of a cavity between the obtained spherical polymeric shell layer and the shrunk frozen core (F).

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Further continuing the sublimation of H2O under high vacuum state till the ice template is completely removed, the novel layer-by-layer polymeric spheres (G) are obtained.

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In summary, we have presented a convenient and simple approach to assemble nanoscale micelles into novel microscale layer-by-layer polymeric hollow spheres.

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This method can be extended to general polymeric micelles dispersed in water.

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We believe the method will broad a new way to produce novel structures as shown in this study.