In the XRD pattern, three peak including (111), (220), and (311) can be clearly seen, which corresponds to the cubic CdTe/CdS and CdTe/CdS/ZnS quantum dots.
In Figure 2c, three diffraction rings can be clearly seen, which can be well indexed as (112), (204), and (312) planes of the chalcopyrite CuInS2, respectively.
For the nanoparticle shown in Fig. 2c, the lattice distortion can be clearly seen, which is related to the procedure that Zn atom moves into the lattice and induces disorder in the η′ phase [17].
Owing to the non-covalent interaction, a very interesting charge redistribution at the hybrid ZrS2/B20 can be clearly seen, which is different from those of the MoS2/SnO2 and Ag3PO4/GR heterostructures [33, 35].
Compared to the spectrum of pure BSA, the characteristic peaks of BSA-GNPs such as at 1,654, 2,958 and 3,421 cm−1 can be clearly seen, which indicating the modification of BSA on the Au nanoparticles.
Although 1 3 exhibit similar assembly hierarchy going from 1-D ribbon through 2-D supramolecular layer to 3-D supramolecular architecture, the side-chain-effect can be clearly seen which modulates intra-chain or inter-chain Cu⋯Cu distance; inter-chain C H⋯S supramolecular interactions and even the co-existence of guest water molecules.
Two ribbons are clearly seen, which is related to the PEA.
In Figure 2b, a particle attached at the end of the nanotube is clearly seen, which is also consistent with SEM observation.
Two phonon modes at 223 and 249 cm−1 are clearly seen, which is assigned to the InAs-like and GaAs-like transverse optical phonon modes, respectively.
Here, in the upper right inset, a round particle at the tip of the nanowire is clearly seen, which indicates the nanowire is most likely grown by the VLS mechanism.
As indicated in the inset in the figure, the first step degradation occurring in all nanofiber combinations can be clearly seen at 293°C which can be assigned due to the degradation of silk fibroins.
