Scanning electron microscopy (SEM) images show that cobalt hydroxides can be synthesized into nanosheets, as shown in Fig. 1, and that there are differences in the morphology depending on the reaction temperature [Lee et al.]. Based on the formation of triangular islands over a large area, the nanosheets synthesized gather to form a continuous sheet at 60°C (Figs. 1a and b). Their chemical bonding states, which consist mainly of cobalt hydroxide and cobalt oxide, were confirmed using X-ray photoelectron spectroscopy (XPS) (Fig. 1c). Unlike the previously reported nanosheets or sheets synthesized at a reaction temperature of 80°C, the continuous arrangement and accumulation of triangular islands remain unclear (Fig. 1d); however, approximately round sheets with contrast were continuously dominated to form a sheet (Fig. 1e). In the XPS O1s spectra (Fig. 1f), the intensity of the hydroxyl peak was the highest, and the C = O ratio appeared to be relatively high, unlike in the previous case. This is because the residue of the precursor used in synthesizing the nanosheets is higher owing to the relatively high reaction temperature.
The thickness of the synthesized cobalt hydroxide nanosheet varies depending on the reaction temperature; the higher the reaction temperature, the thicker is the synthesis [M. Lee et al.]. The thickness of the nanosheets synthesized at a reaction temperature of 80°C with high synthesis reproducibility, and a thickness of 3 nm or more was measured using atomic force microscopy (AFM) (Fig. 2a); the measured thickness was approximately 4 nm (Fig. 2b). To confirm the consistency of the measured nanosheet thickness at the nanoscale level, a TEM image of the nanosheet portion that was transferred to a TEM grid was acquired. To intuitively assess the thickness of the nanosheet using the projected TEM image, an image was acquired on a partially folded area (Fig. 2c), and the line profile of this area was obtained to confirm the intuitive thickness. Because it is a folded region, is the thickness measured intuitively was twice the actual nanosheet thickness; therefore, it was confirmed that the nanosheet thickness assessed from the TEM image is consistent with the that measured using AFM.
To analyze the crystal structure of the synthesized cobalt hydroxide nanosheets, continuous nanosheets synthesized at a reaction temperature of 80°C were transferred to a Quantifoil grid (Fig. 3a); Fig. 3a shows an overfocused image. Although the image appears slightly distorted, it was confirmed that the transferred nanosheet covered the mesh of the grid (Fig. 3b). Figure 3c shows a high-angle annular dark-field scanning transition electron microscopy (HAADF-STEM) image of the nanosheet, which shows that the nanosheet with the same shape as that in Fig. 1e was transferred well. Element mapping was performed on the nanosheet in the same area using energy-dispersive X-ray spectroscopy (EDS), as shown in Fig. 3c, and a uniform element distribution was confirmed throughout.
HR-TEM was performed to confirm the crystallinity of the cobalt hydroxides (Fig. 4a). The pristine synthesized nanosheet was amorphous; no precision spots or ring patterns were identified in the digital diffractogram of the imaged field of view. However, after continuous irradiation with the electron beam, as shown in Fig. 4b, a partially crystallized region appeared, and a distinct spot and ring pattern were observed in the accompanying digital diffractogram. The longer the electron-beam irradiation period, the higher the crystallinity.
As shown in Fig. 5a, crystallization proceeded with the continuous electron-beam irradiation, and this phenomenon was confirmed in the entire amorphous sheet irradiated with parallel beams (Fig. 5b). A thorough inspection of the crystallization (Figs. 5c and d) revealed distinct phases in the partial region indicated by the dashed line, and the digital diffractogram of this region suggests phase transitions from amorphous to crystalline that were caused by the electron beam. The synthesized nanosheet was composed of amorphous cobalt hydroxide, and the electron-beam irradiation caused the transformation into hexagonal and cubic phases. Cobalt hydroxide can undergo frequent phase transitions to cobalt oxides owing to external energy [Lee et al.; Chen et al; Jang et al.]. Among them, cobalt oxides with various stoichiometric compositions are Co3O4 and CoO. Co3O4 exhibits a spinal structure, whereas CoO exhibits hexagonal and cubic phases. The crystal structures at the top and bottom of Fig. 5c belong to CoO; the white line indicates the hexagonal phase (wurtzite structure), and the yellow line indicates the cubic phase (rock salt structure). The successive images of the same area demonstrate that part of the cubic phase formed at the bottom transitioned to the hexagonal phase (Fig. 5d). Figure 5e shows an enlarged image of both the phases shown at the top of Figs. 5c and d. The structures of the atomic models of the accompanying hexagonal and cubic phases matched well.
The partial transitions from amorphous cobalt oxide to cobalt oxide phase was confirmed using a continuous electron beam (Fig. 6). The transition phase consisted of a combination of hexagonal and cubic phases, with the cubic phase being dominant. The areas marked with the colored dashed lines indicate the several regions of the cubic cobalt oxides. Because the transitioned cubic phase is nanosized, the digital diffractogram shows an increase in the number of spots owing to the different orientations of those continuously transferred in the random area.