The leaves are like the hexagonal MK-4827 wimble with the shrinking diameter from 500 nm (on the top) to 100 nm (where connected with the stalk). This structure is similar with that reported by Lao et al.[10]. Figure 1c shows the HRTEM image of one ZnO stalk. It is single crystalline. The

digital diffraction patterns (DDPs) obtained by fast Fourier transformation of the marker region is shown in the inset, indexed and determined the wurtzite structure of ZnO orientations. The direction of the stalk is along the (0002) orientation of ZnO. Figure 2 TEM and HRTEM images and sketch map of the structure of one ZnO nanoflower. (a) TEM image of one ZnO nanoflower; (b) HRTEM image of the region in the stalk, which is marked by a small square in (a); (c) the enlarged image corresponding to the region marked by the big square in (a);

(d) a sketch map of the nanoflower structure. The nanowires in the junction of the branch are not very smooth. Therefore, we suggest that this branching should not be the epitaxy of a nanowire crystal face. It belongs to the secondary nucleation CB-5083 cost phenomena, which means that the nanowires grow to a certain length along the c-axis and a secondary nucleation appears at the top the nanowire. These crystal Selleck Repotrectinib nuclei grow along the new nuclear c-axis and form a flower-like structure. To verify our hypothesis, the samples were analyzed by transmission electron microscopy (TEM) in the following text. Figure 2a shows the TEM image of the nanoflower structure of the nanowires. Figure 2b shows Terminal deoxynucleotidyl transferase the HRTEM image of the region marked by the white square b in Figure 2a, which is located in the stalk. The interplanar distance

of 0.26 nm is corresponding to the wurtzite ZnO (0002) planes; hence, the growth orientation is along the c-axis. Figure 2c is the enlarged image corresponding to the region marked by the white square c in Figure 2a. A gap can be observed at the joint parts between the stalk and leaves, which is marked by the white circle in Figure 2c. This suggests that the leaves structure does not belong to the same epitaxial structure of the stalk, but rather due to the secondary nucleation. The growth mechanism of the nanoflower structure can be described as below: First, the nanowire grows along c-axis direction with a wurtzite structure. Then in the top region of the nanowire, there is secondary nucleation, and the c-axis of the new ZnO grains deviates from the direction before. The end planes of the leaves structures show the regular hexagon. These branches exhibit symmetry due to the constraints from space position. Figure 3 shows the top-viewed SEM images of the as-grown nanoflowers and the coated sample. The hexagonal leaves and the thin stalk can be observed.