Bandgap and Structure Engineering via Cation Exchange: From Binary Ag₂S to Ternary AgInS₂, Quaternary AgZnInS alloy and AgZnInS/ZnS Core/Shell Fluorescent Nanocrystals for Bioimaging

Abstract

Attention on semiconductor nanocrystals have been largely focused because of their unique optical and electrical properties, which can be applied as light absorber and luminophore. However, the band gap and structure engineering of nanomaterials is not so easy because of their finite size. Here we demonstrate an approach for preparing ternary AgInS2 (AIS), quaternary AgZnInS (AZIS), AgInS2/ZnS and AgZnInS/ZnS nanocompounds based on cation exchange. First, pristine Ag2S quantum dots (QDs) with different sizes were synthesized in one-pot, followed by the partial cation exchange between In(3+) and Ag(+). Changing the initial ratio of In(3+) to Ag(+), reaction time and temperature can control the components of the obtained AIS QDs. Under the optimized conditions, AIS QDs were obtained for the first time with a cation disordered cubic phase and high photoluminescence (PL) quantum yield (QY) up to 32% in aqueous solution, demonstrating the great potential of cation exchange in the synthesis for nanocrystals with excellent optical properties. Sequentially, Zn(2+) ions were incorporated in situ through a second exchange of Zn(2+) to Ag(+)/In(3+), leading to distinct results under different reaction temperature. Addition of Zn(2+) precursor at room temperature produced AIS/ZnS core/shell NCs with successively enhancement of QY, while subsequent heating could obtain AZIS homogeneous alloy QDs with a successively blue-shift of PL emission. This allow us to tune the PL emission of the products from 483 to 675 nm and fabricate the chemically stable QDs core/ZnS shell structure. Based on the above results, a mechanism about the cation exchange for the ternary nanocrystals of different structures was proposed that the balance between cation exchange and diffusion is the key factor of controlling the band gap and structure of the final products. Furthermore, photostability and in vitro experiment demonstrated quite low cytotoxicity and remarkably promising applications in the field of clinical diagnosis.

From Indium‐Doped Ag2S to AgInS2 Nanocrystals: Low‐Temperature In Situ Conversion of Colloidal Ag2S Nanoparticles and Their NIR Fluorescence

“…The Ag 3d peak is split into 3d 5/2 (368.03 eV) and 3d 3/2 (374.04 eV) peaks, the In 3d peak is split into 3d 5/2 (444.53 eV) and 3d 3/2 (452.1 eV) peaks, and the peaks at 161.55 and 162.82 eV correspond to S 2p transitions. These observed binding energies are in agreement with reported data for AgInS 2 NCs . Thus, these XPS results confirm the formation of stoichiometric AgInS 2 NCs, which is in agreement with the results of PXRD and HRTEM analyses.…”

“…These observed binding energies are in agreement with reportedd ata for AgInS 2 NCs. [35,36] Thus, these XPS results confirm the formation of stoichiometricA gInS 2 NCs, which is in agreement with the resultso fP XRD and HRTEM analyses.…”

Narrow band-edge photoluminescence from AgInS2 semiconductor nanoparticles by the formation of amorphous III–VI semiconductor shells

“…The expected redshift is usually explained by the leakage of excitons from the core into the shell, whose bandgap is essentially smaller than the HOMO-LUMO gap of insulating organic ligands on its surface 20 . The blueshift, in contrast, is often explained as the result of changes in surface defect levels by surface passivation with ZnS and/ or the result of partial alloying by cation exchange from copper and indium into zinc [21][22][23] . In our experiments, we also observed a blueshift in PL when AgInS 2 NPs were reacted with zinc acetate (Zn(OAc) 2 ) and elemental sulfur at 200°C, as shown in the optical spectra in Fig.…”

Continuous‐wave laser irradiation to form Cd1−xZnxSe shell on CdSe QDs in silicate glasses

“…The blueshift of band‐edge emission (Figure B) is further evidence of Zn incorporation. It has been reported that the reason for this blueshift is due to the decrease in the size of CdSe QDs as the surface of CdSe QDs transform to Cd 1−x Zn x Se with the progress of cation exchange …”