Yulong Ana,
Xu Lin*a,
Yuxi Zhoua,
Yan Lia,
Yunwu Zhengb,
Chunhua Wub,
Kaimeng Xub,
Xijuan Chaib and
Can Liu*ab
aKey Laboratory for Forest Resources Conservation and Utilization in the Southwest Mountains of China, College of Material Science & Engineering, Southwest Forestry University, Kunming, China. E-mail: liucanswfu@163.com
bKey Laboratory of State Forestry Administration for Highly-Efficient Utilization of Forestry Biomass Resources in Southwest China, Southwest Forestry University, Kunming, China
First published on 5th August 2021
Carbon dots (CDs), as the most important type of carbon-based material, have been widely used in many fields because of their excellent properties. In particular, multicolor fluorescent CDs with high photoluminescence quantum yield are the focus of active research. Herein, red, green and blue CDs (RGB CDs) were successfully synthesized by a solvothermal method from o-phenylenediamine under different reaction conditions. The RGB-CDs have stable optical properties and significant photoluminescence characteristics. Structural and elemental analyses propose a conjugated structure and the surface state of the CDs as the main causes for the different color emission of RGB-CDs. In addition, a white fluorescent CD solution was prepared by mixing these multicolor fluorescent CDs in appropriate proportions.
Trichromatic luminescence and high PLQYs are essential to realize full-color display. The CDs with visible spectral emission can be obtained through a one pot pyrolysis method by adjusting the precursor or reaction conditions.6–10 Lin et al.11 developed a variety of colored fluorescent CDs using different precursors, and differences in particle size and nitrogen content were proposed to result in red-shifted emission. The emission wavelength of CDs changed from 426 to 603 nm by changing the precursors from (o-, m-, p-) phenylenediamine, and tricolour CDs were prepared. Bai et al.12 used citric acid and urea as precursors, and the luminescence of CDs changed from blue and green to red when the solvent was used water, ethanol, and dimethylformamide (DMF), respectively. Detailed characterization has shown that the eigenstates and surface states associated with CO/CN are derived from the multistate absorptions and blue, green, and red emission of CDs. Xiong and Yang's team13 used 3,5-diaminobenzoic acid and 3,4-diaminobenzoic acid to obtain red, green, and blue (RGB) color-emitting CDs (RGB-CDs) via a one-pot solvothermal route. The conjugated graphite structure of the carbon cores and the presence of oxygen on the surface states were the main causes for the RGB color emissions of CDs. However, at present, there are still many problems, such as the synthesis method is relatively complex and the source of raw materials is limited. Therefore, developing simple methods to prepare polychromatic CDs is still a great challenge.
In this study, we report the preparation of multicolour luminescent CDs using a simple one-pot pyrolysis method. By using o-phenylenediamine as the reaction precursor, adding reaction auxiliaries, and changing the reaction conditions, red, green, and blue luminescent CDs were obtained. The low cost of the precursor is of great significance for further developing the electro-optical application and the batch synthesis of CDs. The three CDs showed excellent and stable PL performance in solutions. Furthermore, a stable white fluorescent CDs solution was prepared by mixing the three CD solutions in appropriate proportions.
Fig. 1 Preparation of R-CD, G-CD, and B-CD tricolor CDs from o-phenylenediamine using different conditions. Photographs of tricolor dispersed in ethanol under λ = 365 nm UV irradiation. |
Transmission electron microscopy (TEM) was performed to examine the morphologies of the as-prepared samples. As shown in Fig. 2a–c, TEM images demonstrate that the R-CDs, G-CDs, and B-CDs were monodispersed and had similar sizes of ca. 2.5 nm. The high-resolution TEM images (Fig. 2d–f) of the samples show well-resolved lattice fringes of graphite carbon with an interplanar spacing of 0.19 nm.15,16 Obviously, the similar particle size of the three samples suggests that the quantum size effect was not the dominant mechanism responsible for the occurrence of chromatic emissions.17
Fig. 2 (a–c) TEM images of R-CD, G-CD, and B-CD. Inset: histograms and Gauss fittings of particle size distribution and (d–f) enlarged TEM images of R-CD, G-CD, and B-CD. |
The UV/Vis absorption spectra of the CDs were measured in ethanol, as shown in Fig. 3a. In the UV region, significant absorption peak is observed at 293 nm for three CDs, can be assigned to the intrinsic state (n–π*) transition from the aromatic sp2 domains (C–O and CO).18 However, in the lower-energy region, three CDs show distinct absorption behavior. The absorption peak of 440 nm is shown for G-CDs, which is consistent with the literature.19 The absorption peak of R-CDs red-shift by 10 nm compared to that of G-CDs, which means that a longer conjugation system is formed. In contrast, B-CDs not show absorption in the lower-energy region, which indicate that there is no large conjugation structure.
Fig. 3b–d show the PL emission (PL) spectra of the three CDs recorded in ethanol solution, in which the emission maxima of R-CDs, G-CDs, and B-CDs can be observed at λ = 600, 541, and 406 nm, respectively. The emission spectra of B-CDs exhibit classical excitation-dependent properties, namely, red-shifting of the emission peaks with increasing excitation wavelength (Fig. 3d). According to previous reports, this shifting can be assigned to surface-defect emission.20 According to previous reports, this shifting can be assigned to intrinsic and defect emission the spectra of B-CDs present an obvious blue-light emission under UV excitation (320–380 nm), with a peak at 406 nm and a PLQY of 10.0% under excitation at 340 nm. In contrast, the emission of G-CDs and R-CDs exhibit an excitation-independent feature. For G-CDs (Fig. 3c), intense green emissions are observed, forming a wide emission band cantered at 541 nm under excitations at 380–440 nm, and a PLQY of 10.5% was obtained at an excitation of 400 nm. Meanwhile, the R-CDs excited at 490–560 nm show two fluorescence peaks at 600 and 650 nm, as can be seen from the corresponding PL spectrum (Fig. 3b). A PLQY of 9.5% for the red-light emission was achieved under an excitation of 500 nm. The emission peak remained unchanged when changing the excitation wavelength, which differs from B-CDs emission, this can be attributed to nitrogen organic fluorophores, the so-called molecular states emission.20–22
Fourier transform infrared (FT-IR) spectroscopies were conducted to characterize the surface functional groups of the samples. As shown in Fig. 4a, the three CDs exhibit similar FT-IR spectra, indicating their similar chemical compositions. R-CD, G-CD, and B-CD possess abundant hydrophilic groups according to the O–H and N–H stretching vibrations at 3050–3650 cm−1, ensuring good solubility in polar organic solvents.16,23 Other peaks corresponding to the functional groups, such as CO (1630 cm−1), H–N (1500 cm−1), CC (1270 cm−1), C–NH–C (1160 cm−1), C–C (1030–1060 cm−1), were also observed, which can be partially attributed to the stretching vibrations of the bonds between C, N, and O in the aliphatic group. Moreover, the origin of the distinct chromatic emissions was confirmed by determining the PL lifetimes (Fig. 4b). Average lifetimes of 3.6, 4.4, and 2.6 ns were obtained in ethanol for the red, green, and blue emissions. The corresponding error bars of these CDs are shown in Fig. S1.† The PL lifetime of B-CDs is much shorter than that of RG-CDs, indicating that they have different PL mechanisms between B-CDs and RG-CDs.25
X-ray photoelectron spectroscopy (XPS) measurements were performed to gain more insight into the chemical bond composition. As shown in Fig. 4c, the XPS survey spectra of different CD samples demonstrate three main peaks at 285.0, 399.0, and 532.0 eV, respectively, corresponding to C 1s, N 1s, and O 1s, indicating that all the CDs mainly comprise C, N, and O. Table 1 shows the proportions of the three elements in R-CD, G-CD, and B-CD. As can be seen, the element proportions differ appreciably between different samples with B-CD having the highest O 1s intensity, this may be attributed to the fact that B-CD are prepared at relatively higher carbonization temperatures. The high-resolution XPS spectra (Fig. 4d and Table 1) of C 1s confirm the existence of sp2 CC/CN bonds (284.8 eV), C–N/C–O bonds (286.3 eV), and CO bonds (288.2 eV). The proportion of the CC/CN components increased from B-CDs to G-CDs to R-CDs, which signify more sp2 carbon structure are formed.
R-CD | G-CD | B-CD | |
---|---|---|---|
C 1s | 81.5% | 75.2% | 79.7% |
O 1s | 2.6% | 2.9% | 9.7% |
N 1s | 15.9% | 21.9% | 10.6% |
CC/CN | 93.0% | 92.0% | 85.0% |
C–N/C–O | 4.0% | 4.0% | 10.0% |
CO | 3.0% | 4.0% | 5.0% |
According to previous reports, the solvothermal route of phenylenediamine can form polyaniline fluorophore generally,24 like as formation of G-CDs in this study. The addition of potassium hydrogen sulfate can activate the amino group and enhance the solvothermal reaction activity, which may form a phenylenediamine with larger conjugate domain than that of G-CDs, like as formation of R-CD. However, at higher reactant concentration and reaction temperature, phenylenediamine may not be able to slowly form a thermodynamically stable polyaniline, can only form a kinetically stable molecule, resulting in the lack of conjugated structure in the interiors of the CDs. In B-CDs, high degrees of oxidation leading to rich surface-defect density, electrons and holes radiatively recombine under illumination by excitation light, causing blue photoluminescence (Fig. 5a). The oxygen-containing functional group such as C–O, CO, and OC–OH in B-CDs surface produce many distinct energy levels, with the fluorescent emission then depending on excitation wavelength.25,26 Therefore, we speculate that the fluorescence of B-CDs originates from the surface-defect state, and the fluorescence of R- and G-CDs originate the molecular state.
In order to explore the stability of the fluorescence of CDs, we studied its spectral changes in different visible and ultraviolet light continuous irradiation time (Fig. S2†), different temperatures (Fig. S3†) and different polar solvent environment (Fig. S4†). The maximum attenuation rate of the fluorescence intensity of the CDs under visible light for 7 days is less than 15%. Meanwhile, the attenuation rate of the fluorescence intensity of the CDs is less than 20% after 8 hours of continuous ultraviolet light (λ = 365 nm) (Fig. S5a and b†). When the temperature of the CDs reaches 80 °C the fluorescence attenuation rate of the CDs also has not more than 20% (Fig. S5c†). The CDs show some stability in different polar solvents, especially B-CDs, whose emission peak ranges within 10 nm, and the fluorescence ranges of G-CDs and R-CDs are 30 nm and 50 nm. The results show that RGB-CDs have good stability which makes them have great potential for sustainable applications in lighting equipment.
One application of RGB-CDs is to achieve white glow. Considering the liquid fluorescence stability of CDs, we prepared 1 mg mL−1 solutions of the tricolored CDs, and a stable white fluorescent CDs solution was obtained by mixing the solutions in a R-CDs:G-CDs:B-CDs ratio of 1:1:2 (Fig. 5b). Under UV light of 365 nm, their emission maxima locate at 415, 550, and 605 nm, respectively, almost the same with those of the original CDs (Fig. 5c). The 1931 CIE chromaticity coordinate of the white fluorescent CDs was (0.38, 0.37) (Fig. S6†).
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/d1ra02298a |
This journal is © The Royal Society of Chemistry 2021 |