Open Access Article
Kyunghyeon Lee‡
,
Joon Young Kim‡
and
Byeong-Hyeok Sohn*
Department of Chemistry, Seoul National University, Seoul 08826, Republic of Korea. E-mail: bhsohn@snu.ac.kr; Fax: +82-2-889-1568; Tel: +82-2-883-2154
First published on 22nd February 2022
Perovskite nanocrystals are synthesized in diblock copolymer micelles to improve their processability and stability. The copolymer micelle approach allows fluorescence from a stretchable or flexible substrate by coating processes, and stable emission in water by protecting the nanocrystals in the micelles. Fluorescent films in three primary colors of blue, green, and red are also produced with the assistance of anion exchange reactions for perovskite nanocrystals in the micelles. Then, by stacking films in three primary colors, we are able to produce a white-emitting film of copolymer micelles containing only perovskite nanocrystals without the support of other kinds of emissive materials.
Diblock copolymers typically form nanoscale spherical micelles consisting of soluble coronas and insoluble cores, in a selective solvent for the corona block, which can then be processed into a film by various coating techniques25,26 and can further be combined with functional polymers.27,28 Furthermore, the functionalization of copolymer micelles can be achieved effectively by incorporating nanoscale elements such as nanoparticles, quantum dots, and fluorophores into the micelles.29 For example, a single layer of diblock copolymer micelles on graphene was utilized as a template for the synthesis of catalytic nanoparticles.30,31
In this study, we demonstrate that the block copolymer micelle approach allows the processability of perovskite nanocrystals with adjustable fluorescence. Green fluorescent films were first produced by synthesizing CsPbBr3 perovskite nanocrystals in diblock copolymer micelles and coating them on various substrates including stretchable elastomers and flexible polymers. In the case of a freestanding film with green fluorescence, we observed a good stability of the emission against water. After anion exchange reactions, we also obtained blue- and red-emitting films of copolymer micelles having perovskite nanocrystals. Accordingly, by stacking them sequentially, we were able to fabricate a white-emitting film of copolymer micelles containing only perovskite nanocrystals without the support of other kinds of emissive materials.
000 g mol−1 for PS and 50
000 g mol−1 for P2VP. The polydispersity index is 1.05. PbBr2, CsBr, and ZnCl2 were purchased from Sigma-Aldrich. ZnI2 was acquired from Alfa Aesar. All solvents and chemicals were used as received.
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30 v/v concentrated H2SO4 and 30% H2O2), thoroughly rinsed with deionized water several times, and then dried with nitrogen prior to the coating process. A micellar film was obtained by spin-coating, dip-coating, or drop-casting from a solution of PS-b-P2VP micelles having perovskite nanocrystals onto various substrates such as quartz, Si wafers, poly(dimethylsiloxane) (PDMS) elastomers, and poly(ethylene terephthalate) (PET) films. A monolayer of the micelles on quartz was obtained by spin-coating (5000 rpm, 60 s) from a 0.5 wt% micellar solution or by dip-coating (80 mm min−1, 60 s) from a 0.4 wt% micellar solution. For a monolayer on PDMS, a 0.2 wt% micellar solution was used after treating PDMS with oxygen plasma at 80 W in 0.05 Torr for 30 s. A film of multilayered micelles was spin-coated (1000 rpm, 60 s) from a 2.0 wt% micellar solution. For a freestanding film, a drop-cast film of micelles on a Si wafer from a 2.0 wt% micellar solution was detached from the substrate by dissolving the underlying SiO2 layer with a 2.0 M aqueous solution of sodium hydroxide. For white emission, a red-emitting film of micelles was first drop-casted from a 2.0 wt% micellar solution on a SiO2 wafer. Then, green- and blue-emitting films of micelles were sequentially spin-coated (1000 rpm, 60 s) on the red-emitting film from a 0.5 wt% and 2.0 wt% micellar solution, respectively, to adjust the emission intensities.
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| Fig. 1 Schematic illustration of the preparation procedure of the PS-b-P2VP micelles with CsPbBr3 nanocrystals in the P2VP core. | ||
Upon the addition of CsBr into the micellar solution, we immediately observed green emission. The inset of Fig. 2a shows a green-emitting solution under UV illumination. The photoluminescence (PL) spectrum (solid line) from the solution has a maximum intensity at 515 nm with a full width at half maximum (FWHM) of 21 nm, which matches with the value in previous reports.6,32 It is noted that CsPbBr3 nanocrystals in PS-b-P2VP micelles showed the quantum yield of 51% and the fluorescence lifetime of 8 ns in the ref. 23. In the UV-Vis spectrum (dashed line), we can also find a characteristic absorption edge of CsPbBr3 near 510 nm. To confirm the formation of the CsPbBr3 nanocrystals, TEM images were obtained as shown in Fig. 2b. Micelles appear as dim gray spheres with blurred boundaries. Inside the micelles, however, we can distinguish 2–4 dark nanoparticles of ∼6 nm in diameter. We note that the hydrodynamic diameter of PS-b-P2VP micelles having CsPbBr3 nanocrystals by DLS is ∼69 nm (Fig. S1†). The high-resolution TEM image (inset of Fig. 2b) confirms the orthorhombic crystalline structure of the CsPbBr3 perovskite, where the measured values of 4.2 Å and 6.0 Å for d-spacing correspond to the (200) and (002) lattice planes, respectively. The size of the perovskite nanocrystals in the block copolymer micelles can be modified by adjusting the amount of perovskite precursor or by employing block copolymers with various molecular weights,29 which can affect the absorption and fluorescence properties of the perovskite nanocrystals.33
We can fabricate a film consisting of a monolayer of PS-b-P2VP micelles by adjusting the coating conditions. Fig. 3a shows an SEM image of a spin-coated monolayer of PS-b-P2VP micelles containing CsPbBr3 nanocrystals, in which the spherical micelles (∼42 nm in diameter) are arranged in a quasi-hexagonal order with an inter-particle distance of ∼55 nm without overlapping. A monolayer of micelles was also fabricated by dip-coating (Fig. S2†). As shown in the inset of Fig. 3b, we can observe uniform green fluorescence from a spin-coated monolayer on a quartz substrate. In the PL spectrum of this monolayer (Fig. 3b), the maximum intensity is located at 515 nm with a FWHM of 22 nm, identical to that from the micellar solution (Fig. 2a), implying that the micelles with CsPbBr3 nanocrystals were coated without deterioration.
In addition, we prepared a monolayer of PS-b-P2VP micelles having CsPbBr3 nanocrystals on a stretchable PDMS elastomer by spin-coating, which was confirmed by SEM (Fig. S3a†). As shown in Fig. 4, the micelle-coated PDMS elastomer exhibited green fluorescence, which was maintained under the extension of the elastomer. The fluorescence spectrum of the stretchable film (Fig. 4b) is almost identical to that of the monolayer film (Fig. 3). After recovered from extension, the elastomer still showed fluorescence without severe defects on the surface, presumably because the micelles arranged in the monolayer can be separated by extending their relative distance without being damaged during extension.34 The monolayer of micelles on the PDMS elastomer was preserved after extension without deterioration of the spherical shape of the micelles (Fig. S3b†). We note that the fluorescent PDMS elastomer coated with a monolayer of the micelles can be stretched up to ∼90% of its length before break.
The emission color of the CsPbBr3 nanocrystals can be tuned by anion-exchange reactions.22 Fig. 5a shows micellar solutions with various fluorescence colors after treating the solution of PS-b-P2VP micelles having CsPbBr3 nanocrystals with ZnCl2 and ZnI2. With an increase in the amount of ZnCl2, the fluorescence color changed from green to light blue and then blue. In contrast, the emission turned into yellow and then red color with the addition of ZnI2. The PL spectra in Fig. 5b confirm variations in the emission color, in which the maximum intensity appears at 479 nm (light blue line) and 460 nm (blue line) after exchanging bromide with chloride and at 578 nm (yellow line) and 677 nm (red line) after anion exchange with iodide. It is noted that these PL spectra show relative intensities without normalization, and a PL spectrum of the green emission was obtained using a 1/3 diluted solution due to the high fluorescence intensity. We also note that the PL intensities highly decrease after anion-exchange reactions as reported in the literature.35 The decrease of PL intensities in perovskite nanocrystals after anion-exchange reactions is associated with deep trap states in the bandgap due to halide vacancies by different anion sizes.36,37
Due to the weak fluorescence intensity from a monolayer of PS-b-P2VP micelles containing perovskite nanocrystals after anion exchange reactions, a film consisting of multilayered micelles was fabricated by lowering the spinning speed (1000 rpm) during spin-coating. Fig. 6 is an SEM image of the PS-b-P2VP micelles having CsPbBr3 nanocrystals on a Si substrate after spin-coating. From the top-view image, we can find that spherical micelles are preserved and randomly arranged overall, although a quasi-hexagonal arrangement can be locally observed. The side-view image (inset of Fig. 6) confirms that the film thickness (∼129 nm) is larger than the micelle diameter (∼42 nm), indicating a multilayer of micelles.
A green-emitting film in Fig. 7 was obtained by the same procedure used to prepare the film shown in Fig. 6, with the exception of a flexible PET film as substrate. Because of the multilayered micelles having CsPbBr3 nanocrystals, the film exhibits much brighter fluorescence than the monolayer shown in the inset of Fig. 3b. In Fig. 7, we can also observe blue and red emissions from the films of multilayered micelles with perovskite nanocrystals after halide exchange reactions, which were prepared under the same spin-coating condition. As shown in the PL spectra given in the photographs, the maximum intensities of blue, green, and red emissions appear at 464 nm, 512 nm, and 660 nm, respectively. Each wavelength of the maximum intensity is almost same as that observed in a solution of the corresponding micelles. However, the fluorescence intensities of both red- and blue-emitting films were considerably lower than that of the green-emitting film as shown in the PL spectra given in the photographs. It is worthwhile to note that the emissions of all three colors are apparently unchanged from curved films as displayed in Fig. 7, presumably because the perovskite nanocrystals are imbedded in polymeric micelles.
Since fluorescent films in three primary colors of blue, green, and red can be produced as shown in Fig. 7, a white-emitting film can be expected with combination of PS-b-P2VP micelles containing perovskite nanocrystals. However, there were large variations in the PL intensities of the three colors so that it was necessary to adjust the thickness of each colored layer with a proper coating condition for reasonable white emission. A red-emitting film of micelles was first drop-casted from a thicker micellar solution (2.0 wt%) compared to a spin-coating solution (0.5 wt%). Then, green- and blue-emitting films of micelles were sequentially spin-coated onto the red-emitting film. A thicker solution (2.0 wt%) was also used for the blue-emitting film. It is noted that the thickness (∼18 μm) of the white-emitting film (Fig. S4†) was substantially larger than that (∼129 nm) of the green-emitting film (Fig. 6). After sequential coating of micelles having red-, green-, and blue-emitting perovskite nanocrystals, a PL spectrum of white emission was obtained as shown in Fig. 8, which has three maxima at 462, 517, and 673 nm. Each wavelength of the three maxima corresponds to that in the spectra of the individual films of three primary colors of perovskite nanoparticles. We note that this observation can be an evidence against halogen migration or segregation, which would be restricted by the stacked structure of the film as well as by the corona layer encompassing the nanocrystals. The polymeric parts in the film would suppress the diffusion of halogen anions associated with photo-induced charge carriers.24 The color coordinate of the spectrum is (0.29, 0.31) marked as a white dot in the CIE diagram (inset of Fig. 8), which is close to the white color of (0.31, 0.33). It is worthwhile to note that a white-emitting film is demonstrated with three primary colors from perovskite nanocrystals in polymeric micelles without other emissive materials.22,38 We also note that a decent choice of emission colors can be expected by adjusting the intensity of each color, based on the triangle mark with three color coordinates of blue, green, and red emissions of the spectrum (inset of Fig. 8).
To fabricate a freestanding film of PS-b-P2VP micelles having perovskite nanocrystals without a supporting substrate, a film of the micelles was drop-casted and detached from the substrate. As shown in the inset of Fig. 9, a green-emitting film of ∼10 μm in thickness was separated from the substrate without discernible damage and was freely held. Freestanding films of blue and red emissions were also obtained by drop-casting. Although the films were immersed in water for longer than 30 min during the detaching process, there was no noticeable deterioration in emissions (Fig. 9), so that we intentionally submerged a green-emitting film in water (Fig. 10). After 30 min, the film well maintained green fluorescence (Fig. 9 and 10), indicating that the water-sensitive perovskite nanocrystals were protected by the hydrophobic polystyrene corona of the polymeric micelles.39 In addition, proper protection can apparently be obtained by favor of the film structure, in which polystyrene coronas overlap with each other, when the extremely low water permeability of polystyrene is considered.40
Footnotes |
| † Electronic supplementary information (ESI) available. See DOI: 10.1039/d2ra00098a |
| ‡ Equal contribution. |
| This journal is © The Royal Society of Chemistry 2022 |