Jian Cheng,
Cai-Feng Wang,
Yan Zhang,
Shengyang Yang and
Su Chen*
State Key Laboratory of Materials-Oriented Chemical Engineering, College of Chemistry and Chemical Engineering, Nanjing Tech University (Former Nanjing University of Technology), 5 Xin Mofan Road, Nanjing 210009, P. R. China. E-mail: chensu@njtech.edu.cn
First published on 22nd March 2016
We demonstrated a simple strategy for facile generation of high-quantum yield robust yellow photoluminescent (PL) carbon dots (CDs) doped with zinc ions. These as-synthesized CDs when synthesized using zinc ions and citric acid as the precursor via a one-pot solvothermal method produced zinc ion-doped CDs that yielded excitation-independent yellow PL emission and the highest QY reported to date of 51.2%. We also thoroughly discuss the formation mechanism of these CDs, whose high quality was attributed to the radiative recombination of electrons and holes trapped on the CD surface. We also showed the ability to find practical applications of these as-prepared CDs, such as for bifunctional photonic crystal films and for fluorescent microfibers and patterns.
Herein, for the first time, we demonstrated the use of a simple strategy involving the doping of zinc ions to generate robust yellow photoluminescent CDs with a QY of 51.2%. These as-synthesized CDs were made using zinc ions and citric acid as the precursor via a one-pot solvothermal method, producing excitation-independent CDs doped with zinc ions (denoted as Zn2+-doped CDs), which may have the highest reported QY of yellow PL-emitting CDs. We also thoroughly discuss the mechanism of formation of the as-synthesized CDs; this mechanism involves the radiative recombination of electrons and holes trapped on the CD surface. For practical applications, we utilized these strongly yellow PL Zn2+-doped CDs coupled with a poly(styrene-co-methacrylic acid) (PS-co-PMAA) mono-dispersed colloid to create a photonic crystal film (PC-CDs) with two functions (visible light optical and photoluminescence properties) by using the vertical deposition method. The as-prepared Zn2+-doped CDs could be also be a good candidate for applications in the inkjet printing pattern and LED fields. The strategy we developed is simple, and can be used to create other robust CDs, allowing CDs to be extended to promising applications.
The morphologies of the Zn2+-doped CDs were visualized by transmission electron microscopy (TEM) analyses. Fig. S1a, ESI† shows TEM images of the Zn2+-doped CDs, revealing the as-synthesized Zn2+-doped CDs to be uniform dispersions without apparent aggregation and with particle diameters of 2–5 nm (Fig. S1b, ESI†). In the high-resolution TEM (HRTEM) images we can distinctly see lattices corresponding to the Zn2+-doped CDs. Fig. 1a shows a lattice spacing of 0.34 nm, which corresponds to the spacing between graphene layers (002 facet), while the observed lattice spacing of 0.21 nm is consistent with the in-plane lattice spacing of graphene (100 facet). This result is similar to those of many other reported CDs.19,20 The Zn2+-doped CDs yielded XRD patterns (Fig. 1b) with a peak centered at 25.5° (0.34 nm),13 which was ascribed to disordered carbon atoms, similar to the graphite lattice spacing.
Atomic force microscopy (AFM) image of the as-synthesized Zn2+-doped CDs (Fig. S2a, ESI†) showed landform heights between 2.5 and 4.5 nm (Fig. S2b, ESI†). X-ray photoelectron spectroscopy (XPS) analysis indicated the Zn2+-doped CDs to be mainly composed of carbon, nitrogen, oxygen and zinc. These CDs yielded a high-resolution XPS spectrum of C1s exhibiting (sp2 C–C), (C–O, C–N), and (CO) main peaks at binding energy values of 284.5 eV, 285.5 eV and 288.0 eV (Fig. 1c). Fig. 1d shows the XPS spectrum of Zn2p peaks at 1045 eV and 1023 eV. Thermogravimetric analysis (TGA) indicated the presence of 10% zinc oxide in Zn2+-doped CDs for decomposition temperatures above 580 °C (Fig. S3a, ESI†). The above results also confirmed the CDs to be doped with zinc ions.
We further characterized Zn2+-doped CDs by acquiring Fourier transform infrared (FTIR) and microscopic Fourier transform infrared (MFTIR) spectra (Fig. S3b and S4, ESI†). The peaks observed at 3430 cm−1, 1650 cm−1 and 1120 cm−1 were ascribed to the hydroxyl group (–OH), carbonyl group (CO), and asymmetric stretching vibrations of C–N, respectively. The strong intensity of the Zn–O bands near 700 cm−1 and 450 cm−1 imply that oxygen formed complexes with the metal. We also obtained carboxylic acid spectra showing a main symmetric νs (COO–) band at about 1450 cm−1 and asymmetric νas (COO–) band at about 1650 cm−1.6,21 By contrast, in the FTIR spectra of the Zn2+-doped CDs sample with an undoped control sample, the intensities of the Zn2+-doped CDs characteristic peaks at 3430 cm−1 (–OH) and 1650 cm−1 (CO) were found to be decreased. (Fig. S3b, ESI†), together with the MFTIR evidence shows that red color area (the color represented the intensity of characteristic peak. From red to blue, the intensity is decrease) noticed at 3430 cm−1 (–OH) and 1650 cm−1 (CO) can be transferred or decreased to partially yellow color area (Fig. S4, ESI†). It is clear that the asymmetric carboxylate vibrations of the control sample appeared at higher frequencies than did those of the Zn2+-doped CDs sample. This difference can be associated with a stronger interaction of the carboxylic acid with the zinc sites. Carboxylate ions can coordinate in several ways, including as a unidentate ligand, chelating ligand and bridging bidentate ligand. Since each type of coordination has a specific νas (COO–) and νs (COO–) peak position, the peak separation (Δν (COO–) = (νas (COO–) − νs (COO–))) can be used to determine which type of coordination is being used by the carboxylate. According to the peak separation (Δν (COO–) > 160 cm−1) and zinc–oxygen binding (Zn–O), the plausible complex structure for the carboxylate ions and Zn2+ product involved the carboxylate functioning as a chelating ligand.22,23
Fig. 2 shows a series of optical characterization of as-prepared CDs. The product, Zn2+-doped CDs, displayed high fluorescence and a bright yellow color under a UV lamp at a very low concentration (0.1 mg mL−1). A sharp absorption peak in the UV/Vis spectrum centered at 460 nm as well as a narrow high-intensity PL peak at an emission wavelength of 580 nm (λex = 380 nm) were observed (Fig. 2a). The QY of the as-obtained Zn2+-doped CDs was found to be as high as 51.2% using rhodamine 6G in ethanol as a standard (see details in the ESI†). To the best of our knowledge, this is the highest QY value ever reported for yellow PL CDs, with the previous record high being only 12%.24 Another indication of optical characterization is that the PL of Zn2+-doped CDs did not display any dependence on the excitation wavelength, in contrast to the dependence that is displayed by other traditional CDs (Fig. 2b). Interestingly, the PL intensity of the emission in this case was found to increase with decreasing excitation wavelength. This relationship had not been previously observed. The unique PL prosperity is highly associated with zinc doping behaviour. We further investigated the PL properties and fluorescence decay behaviours of Zn2+-doped CDs and of control CDs, shown in Fig. 2c and d, respectively. Under the same tested conditions, an obvious red-shift of the PL peak occurred when comparing the Zn2+-doped CD sample with the control sample (Fig. 2c). Also, a substantial tail (asymmetric peak) was observed in the PL curve of the control sample, as has been found in most reported CDs. However, this tail decreased in extent upon doping the CDs with zinc ions. Moreover, the symmetry of the PL peak significantly improved upon doping the CDs with zinc ions, indicative of a more uniform particle size. Furthermore, fluorescence decays of Zn2+-doped CDs and control CDs were measured by using the time-correlated single photon counting (TCSPC) technique (Fig. 2d). We calculated the average PL lifetime (τ−) of Zn2+-doped CDs and control CDs to be 6.8 ± 0.05 ns and 5.5 ± 0.05 ns, respectively (χ2 < 1.1) (see details in the ESI†). The Zn2+-doped CDs average PL lifetime was found to be longer than that of control CDs. Mechanistically, the longer PL lifetime of carbon-based photoluminescence has been attributed to passivated defects (passivated by organic or inorganic compounds via either covalent linkages or chemical adsorption) on the CD surfaces acting as excitation energy traps.26 More specifically, due to the zinc ions doped onto the CDs, the CD surfaces became passivated, and exhibited longer PL lifetimes than did the control CDs. That is, the Zn2+-doped CDs displayed greater PL stability.
Two mechanisms have been most commonly proposed to explain the PL mechanism of CDs, namely electronic conjugate structures25 and emissive traps.26 Herein, we inferred that the strong yellow PL emission of the Zn2+-doped CDs mainly resulted from the surface passivation of the CDs doped with zinc ions. A similar result has already been reported by the Sun group,15 and the strengthened PL of the semiconductor-doped CDs may be rationalized in terms of improved surface passivation by a combination of doping the surface with inorganic compounds and then functionalizing the surface with an organic compound. In fact, the PL emissions in CDs were attributed to radiative recombination of the electrons and holes trapped at the CD surface. Hence, it is reasonable that more new energy levels resulted from the addition of zinc ions, producing more diverse surface sites and occurrence of a PL red-shift.
Proposed energy level diagrams for the undoped CDs and Zn2+-doped CDs are illustrated in Fig. 3. We proposed Zn2+-doped CD features similar to those of undoped CDs, with their full-color emissions mainly derived from different surface states. For the Zn2+-doped CDs, besides the HOMO and HOMO+1 energy levels, a new HOMO+2 energy level was proposed to be introduced after Zn2+ doping. Hence, electron transitions could occur from the new HOMO+2 to the LUMO and then the excited electrons could be deactivated by radiative recombination at the same time. This process could cause the PL emission to occur in the yellow region. The control CDs, however, having no energy level introduced, can only induce blue fluorescence as their electron transitions occur from the HOMO+1 level to the LUMO. The excited electrons generated by absorption of short wavelength light (HOMO to LUMO) can relax to the HOMO+1 and HOMO+2 levels through radiative recombination that results in a broad excitation-independent emission.
Fig. 3 Schematic illustration of proposed energy levels and electron transitions graphic of undoped CDs (left) and Zn2+-doped CDs (right). |
The second set of experiments was focused on fabrication of PC film loaded with fluorescent quantum dots (QDs). Up to now, semiconductor QDs have been applied by being coupled with colloidal crystals either by in situ growth methods or by electrostatic fixation on the surfaces of the polymer spheres.27 However, in most cases, the in situ growth methods do not yield high-quality (PL and QY) QDs. The electrostatic interaction between QDs and colloidal crystals is usually weak and thus leads to easy phase separation. To make the best use of the good coordination ability of these as-prepared Zn2+-doped CDs, we for the first time employed the vertical deposition method and monodisperse colloidal photonic crystals of PS-co-PMAA spheres (average size 250 nm, Fig. 4c) combined with Zn2+-doped CDs to create bifunctional films with PC structure color and bright yellow PL (Fig. 4a and b). Under a UV lamp, the color of the film can be changed from red to a bright yellow fluorescent color. More importantly, brightly yellow PL Zn2+-doped CDs composited photonic crystal film and non-fluorescent CDs (without Zn2+-doped) composited photonic crystal film we can clear distinguish (Fig. S5, ESI†). Fig. 4d shows the reflection spectra of the PC film and PC-CD film. There was a clear redshift of the wavelength but with a decrease of intensity of the reflection spectrum, which might have been caused by the changed band structure of the PCs. This result could be explained by the effects of the coordination between the Zn2+-doped CDs and PS-co-PMAA colloidal crystals containing carboxyl groups. This interaction allowed the Zn2+-doped CDs to firmly bind to the colloidal crystals, forming uniform fluorescent film. Such films have potentially extensive applications in the sensor and anti-fake fields (photonic crystal structure color under vis-light and PL under UV light).
In practice, it would be possible to use high-QY Zn2+-doped CD products as phosphor to create white light-emitting diodes (WLEDs). Indeed, there are several reports showing the use of CDs to make WLEDs.28 However, in most cases, the QYs of CDs applied in WLEDs are fairly low, and they emit a dull blue color, limiting their applications. Herein, we employed the yellow PL Zn2+-doped CDs to make a WLED with Commission International d'Eclairage (CIE) coordinates of (0.36, 0.34) (Fig. 4). The result indicated that the Zn2+-doped CDs with robust yellow PL emission can act as the phosphor materials for achieving high-performance WLEDs. On the other hand, we further tried to make use of high-QY Zn2+-doped CD solutions such as dye ink to construct fluorescent patterns via inkjet printing (Fig. S6, ESI†).11 As expected, the pattern had a bright yellow color with a picture of a “panda” under UV light. Also, we fabricated one-dimensional fluorescent microfiber arrays via microfluidic technology (Fig. S6, ESI†).
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c5ra27808b |
This journal is © The Royal Society of Chemistry 2016 |