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Page 8 of 33                          Mao et al. Chem Synth 2023;3:26  https://dx.doi.org/10.20517/cs.2022.41









































                Figure 3. (A) Valence band spectra of Cu Se NPs and (B) Mott-Schottky diagram; (C) Schematic diagram of energy band diagrams in
                                           2-x
                newly deposited (pristine), lithiated (charged), and fully delithiated (discharged)  states [70] . Copyright © American Chemical Society
                2018.
               Similarly, the carrier density surface treatment could also be utilized for the formation of the plasmonic
               copper chalcogenides NCs, as illustrated in Figure 5E . The TEM micrographs in Figure 5F and G showed
                                                            [68]
               copper sulfide NPs. The attained tetradecahedrons and nano-disks have similar Cu S  phases; however,
                                                                                       31 16
               they presented different optical properties, as shown in Figure 5H. The nano-disks produced without Sn
                                                                                                         4+
               treatment exhibited a strong LSPR absorption in the NIR region because of the collective oscillation of free
               charge carriers. In sharp contrast, the plasmonic feature was diminished with the Sn  treatment. This
                                                                                          4+
               suggested that Cu vacancies or trapped free charge holes could be efficiently filled by trace amounts of Sn 4+
               [81] . The dramatic change of the LSPR peak is due to the phase transition, as shown in Figure 5I. Specifically,
               a higher density of copper vacancies results in a blue shift of the LSPR peak, a higher absorption intensity, a
               narrower bandwidth, and an increase in bandgap absorption . The main factors that trigger the phase
                                                                    [82]
               transition are the generation of copper vacancies and the rearrangement of Cu cations and S anions .
                                                                                                  [83]
               Chen et al. demonstrated that the Sn  could direct the evolution of djurleite Cu S  from nano-disk to
                                                4+
                                                                                      31 16
               tetradecahedron in the c-axis orientation . The Cu S  NCs were transformed into more copper-deficient
                                                  [68]
                                                           31 16
               Cu S  NPs by heat treatment with amine-functional ligands. The roxbyite Cu S  NPs demonstrated a
                                                                                     7 4
                  7 4
               stronger and shorter LSPR peak while retaining the shape of the djurleite Cu S  NPs. Swihart et al. also
                                                                                  31 16
               reported that the conversion of CuS and Cu S was possible through heat treatment in various organic
                                                      2
               reagents after surface treatment .
                                          [79]
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