Hong-Jie Yang and
Hsing-Yu Tuan*
Department of Chemical Engineering, National Tsing Hua University, 101, Section 2, Kuang-Fu Road, Hsinchu, Taiwan 30013, Republic of China. E-mail: hytuan@che.nthu.edu.tw; Fax: +886-3-571-5408; Tel: +886-3-572-3661
First published on 16th September 2014
Quantum dots (QDs) synthesis has been widely carried out in Schlenk line systems. However, there are two drawbacks of these systems, which have restricted their use for large scale or commercial production of QDs. One is the use of expensive and high-boiling point solvents and the other is that QDs need to be continuously produced with high production rate to reduce production costs. Nowadays, microfluidic flow systems are the most popularly used systems for the continuous production of QDs. However, their narrow channels limit the reaction volume and flow rate. In this report, a non-microfluidic flow reactor system has been developed to synthesize high quality CdSe QDs by injecting the solution containing the mixture of Cd–oleic acid (Cd–OA) and Se–tributylphosphine (Se–TBP) into near critical or supercritical hexane. The optical properties of the produced CdSe QDs can be fine-tuned to almost cover the entire visible region (450–630 nm) by changing the reaction parameters. The CdSe QDs produced with this approach are similar to those produced in Schlenk line, and can be functionalized with a ZnS shell to enhance PL efficiency. Moreover, we have also achieved a continuous synthesis of 5 g CdSe QDs with a production rate of 2.5 g h−1 to demonstrate the potential capability of mass production with this system. White light emitting diodes can be prepared by using CdSe QDs as the phosphor dye. Finally, other types of QDs, such as CdS, ZnS, and ZnSe, were also synthesized to demonstrate the generalization of the developed approach.
Among the various synthetic routes, hot injection and non-injection methods are the most successful and commonly used methods for the preparation of highly luminescent colloidal QDs with controllable size, shape, and surface passivation.28,29 However, the major drawbacks of these methods are the use of large amounts of expensive and high boiling point solvents, limited reaction temperature, unpredictable transport phenomena (hot injection), and difficulty in scaling-up the synthesis process.30–32 Therefore, the development of a greener method having the potential for scale up, and utilizing cheaper, less toxic chemicals and reaction medium (solvents) to synthesize QDs is desirable.
Usually, high molecular weight solvents with high boiling point (trioctylphosphine oxide or octadecene) have been used to synthesize QDs. One way for using low molecular weight solvents with low boiling point is to conduct experiments at high pressure.33 In addition, the reaction media can enhance their ability of solvating chemical compounds under sufficiently high pressure. The physicochemical properties (density, viscosity, dielectric constant) of near critical and supercritical fluids can also be tuned by varying the pressure and temperature of the system, which have been considered to be environmentally benign solvents.34 To date, research about the synthesis of nanomaterials under supercritical water and supercritical ethanol has been reported.35–38 However, metal oxide nanoparticles, such as Fe2O3, TiO2, CuO, ZnO, are easy to produce due to the oxidizing environment provided by supercritical water, making the synthesis of metals or non oxide based compound semiconductor difficult.39 In addition, several commonly used precursors and organic ligands may be incompatible with water or ethanol; thus, using low molecular weight and more hydrophobic organic solvents may be a way to overcome these problems. A study using a microfluidic reactor for synthesizing CdSe QDs by Marre et al. has proven that adopting a supercritical fluid as the solvent is compatible with currently used chemicals and the results are superior to the conventional solvent (squalane).33 However, the narrow pipeline and the micro-size reaction restrict the production rate. Therefore, the improvement of the synthesis of CdSe QDs using supercritical fluid technologies is desirable.
Here, we show a green and generalized approach for the synthesis of several types of colloidal fluorescing QDs. We use hexane which is a more environmentally friendly solvent than those previously used in hot injection methods. In addition, hexane is also a common industrial solvent, which implied that the cost of synthesizing QDs can be reduced. Using CdSe as an example, monodisperse CdSe QDs can be generated under near critical and supercritical hexane fluids, and their size can be fine tuned by changing the reaction temperature time. In addition, we improved the optical properties of CdSe QDs by coating ZnS shells to the surface of CdSe QDs, which has been a well-known tool to significantly enhance the quantum yield (QY) of CdSe QDs. Moreover, we use CdSe QDs as phosphors to prepare white light emitting diodes. To show the ability for the mass production of QDs in our system, we demonstrate the continuous synthesis of large scale CdSe QDs under supercritical hexane. Compared to a microfluidic reactor, our system possesses relatively high production rate due to the larger size of pipeline and reaction volume. The implementation of synthesizing CdSe QDs in flow reactor can offer several advantages over conventional methods, e.g., batch reactor, in terms of time and cost. Finally, we prove the general applicability of our system by producing several types of colloidal fluorescing QDs, including CdS, ZnS, and ZnSe QDs.
In a typical reaction, the stainless steel reactor was heated to the reaction temperature and pressurized to 800 psi. The reaction solution was taken from the glove box and injected into a 0.5 mL sample loop. Next, the HPLC pump was turned on with an injection rate of 8 mL min−1 for 10 s and then turned off. The stainless steel reactor was quickly cooled by an ice-water bath when the reaction ended. The products were removed from the reactor and purified by the addition of 10 mL toluene and 20 mL ethanol, and then centrifuged at 8000 rpm for 5 min. The washing processes were repeated at least twice. The size control of CdSe QDs was achieved by varying the reaction temperature and time. For example, at a reaction temperature of 200 °C, the diameters of 2.45 nm and 2.94 nm QDs can be generated under reaction times of 30 s and 5 min, respectively. Under the same reaction time of 30 s, QDs with diameters of 2.45 nm and 2.73 nm can be produced at reaction temperatures of 200 °C and 270 °C, respectively (Fig. S1†).
Stage 1 | Stage 2 | Stage 3 | |
---|---|---|---|
Heating rate | 1 °C min−1 | 1 °C min−1 | 1 °C min−1 |
Injection time | 10 min | 10 min | 10 min |
Injection rate | 3.12 mL h−1 | 4.62 mL h−1 | 6.6 mL h−1 |
Injection amount | 0.52 mL | 0.77 mL | 1.1 mL |
Reaction temperature | 160 °C to 170 °C | 170 °C to 180 °C | 180 °C to 190 °C |
In continuous reaction for the production of 5 g CdSe QDs, the reactor was heated to 300 °C and then pressurized to 1000 psi. A syringe containing 5.4 mL Cd–OA (1 M), 1.8 mL Se–TBP (3 M), and 2.8 mL anhydrous hexane prepared in a glove box was taken from the glove box and injected into the a 10 mL sample loop. Next, the HPLC pump was turned on with an injection rate of 1 min mL−1, and then slowly the micro control-metering valve was opened to maintain the system pressure (∼1000 psi). A flask was placed at the outlet of the micro control-metering valve to collect the products. After 20 min reaction time, another reaction solution was prepared and injected into the 10 mL sample loop. The injection procedure was repeated six times with total reaction volume of 60 mL and total reaction time of 2 h. The collected products were purified by the addition of ethanol and then centrifuged at 8000 rpm for 8 min. The washing processes were repeated at least twice.
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Fig. 1 (a) The physical properties of hexane. (b) Schematic picture of QDs synthesized under high pressure hexane. |
Fig. 1b shows a schematic picture of QDs synthesized under high pressure hexane. In a typical reaction, colloidal CdSe QDs were produced by the decomposition of Cd–OA and Se–TBP under near critical or supercritical hexane. Fig. 2 and Fig. 3 show the representative analysis results (TEM, HRTEM, XRD, optical measurement, and FTIR) of CdSe QDs produced by the decomposition of reaction mixtures containing 0.35 mL Cd–OA (1 M), 0.35 mL Se–TBP (1 M), and 0.3 mL hexane and synthesizing at 270 °C for 5 min. TEM images (Fig. 2) confirm the dot shape of the products with an average diameter of about 2.95 nm without any size selection. These dot shaped nanoparticles tend to self-assemble into close-packed two-dimensional arrays on the TEM grid, which indicates the monodispersity of the obtained product (Fig. 2a and b). From the fast Fourier transform spectra of the two-dimensional array nanoparticles (Fig. 2a inset), the pattern is consistent with a face centred cubic superlattice. HRTEM images (Fig. 2e and f) show distinct lattice planes, showing high crystallinity of the nanoparticles. The crystalline structure of the synthesized nanoparticles was investigated by XRD. Fig. 3b shows the XRD pattern of the CdSe QDs. The diffraction peaks correspond to the zinc blend and wurtzite structure of CdSe, which may be a combination of wurtzite structure with zinc blend stacking faults.45 Broad peaks in the XRD pattern indicate a small crystal with an average size of ∼2.9 nm calculated from the Scherrer equation. The size is in close agreement with the nanoparticle size obtained from the TEM images (Fig. 2).46 The optical properties (absorption and PL spectra) of the as-synthesized CdSe QDs are shown in Fig. 3a. The first absorption and PL maxima are about 551 nm and 566 nm (15 nm Stokes shift), respectively. QY of the as-synthesized CdSe QDs is about 15%. The sharp peak in the absorption spectra and the narrow full-width half-maximum value in the PL spectra (32 nm) further indicate the narrow size distribution of the as-synthesized CdSe QDs. In addition, the average diameters of CdSe QDs can be calculated from first absorption peak in the UV-vis spectra. The calculated value is about 3 nm, which is very close to the results obtained from the XRD pattern (Fig. 3b) and the TEM images (Fig. 2).47
The CdSe QDs synthesized by our supercritical equipment can be easily dispersed in most organic solvents. Intuitively, the OA and TBP should be surface ligands on the CdSe QDs because hexane is a non-coordinating solvent. To confirm this hypothesis and understand the surface state of the as-synthesized CdSe QDs, FTIR and XPS were performed. Fig. 3c shows the FTIR spectra of OA, TBP, and the as-synthesized CdSe QDs. For liquid OA, the carboxylic acid group would generate O–H stretch (broad peak between 3500 and 2500 cm−1), in plane O–H stretch (1466 cm−1), CO stretch (1711 cm−1), and C–O stretch (1285 cm−1), and the remaining peaks at 2850 cm−1, 2920 cm−1, and 3005 cm−1 were attributed to the symmetric CH2 stretch, the asymmetric CH2 stretch, and the C–H stretch in C
C–H, respectively.48 For pure TBP, C–P stretch (appeared at 1300 cm−1 to 1000 cm−1), symmetric CH2 stretch (2870 cm−1), asymmetric CH2 stretch (2925 cm−1), asymmetric in-plane (1463 cm−1), and symmetric rocking mode (1376 cm−1) of CH3 group were detected.49 In comparison with the FTIR spectra of liquid OA and pure TBP, we can measure the symmetric CH2 stretch (2872 cm−1) and the asymmetric CH2 stretch (2923 cm−1) both contributed from OA and TBP, C–P stretch (1030 cm−1 and 1080 cm−1) assigned to TBP, and C–H stretch in C
C–H (3030 cm−1) generated by OA. It is worth noting that the C
O stretch (1711 cm−1) in the IR spectra of pure OA disappeared in the IR spectra of the as-synthesized CdSe QDs. Instead, a new band at about 1500 cm−1 was assigned to the COO− asymmetric vibration, and the COO− symmetric vibration may overlap with the asymmetric in-plane or symmetric rocking mode of CH3 group.50 In addition, P can also be detected in the XPS full spectrum (Fig. 3d), which indicates that the TBP indeed exists on the CdSe QDs surface. According to the analysis results based on FTIR and XPS, the surface of the CdSe QDs was passivated by OA (from Cd–OA) and TBP (from Se–TBP). In some studies, OA and TBP have been shown as stabilizers to coordinate the nucleation and growth of nanocrystals in the growth process. We believe that OA and TBP play the same roles in our system.51,52
The QY of the CdSe QDs synthesized by our synthetic route is about 15% (Fig. 3a). The QY is sensitive to the surface properties of the QDs such as surface ligands or dispersion medium (solvent).53,54 Numerous methods have been developed to improve the QY of the QDs such as organic or inorganic passivation.55 Obviously, inorganic passivation is superior to organic passivation. For now, the most used method is the ZnS passivation approach, which is an effective method that can separate the core from the surrounding medium to prevent the photo-oxidation and stabilize the surface. Therefore, ZnS passivation of CdSe QDs was performed. Fig. 4 shows the absorption and PL spectra of CdSe QDs and CdSe@ZnS QDs. There is a small red shift in UV-vis absorption spectrum (4 nm) and PL spectrum (4 nm), which is a common phenomenon after coating ZnS shell. We can see that the QY is significantly enhanced by simply comparing the intensity of the PL peaks and the digital photos in the inset (the optical density at the first absorption peak and the concentration of the CdSe QDs and CdSe@ZnS QDs solutions were set to a similar value). The calculated QY of CdSe@ZnS QDs is 65%, which is significantly enhanced compared to the raw materials, CdSe QDs (15%).
Next, we tested the ability of the supercritical equipment to control the size of the CdSe QDs by varying reaction parameters. We observed that the size of the CdSe QDs can simply be regulated by changing the growth time and reaction temperature (Fig. S1†). By varying these two reaction parameters, a series of absorption and PL spectra of CdSe QDs synthesized with particle sizes ranging from approximately 2.01 nm to 5.61 nm (calculated from absorption spectra, Fig. 5a), emission wavelengths ranging from 450 nm to 630 nm (covering almost the entire visible region, Fig. 5b), QY of about 5–15%, and color ranging from green to red were obtained (Fig. 5a inset). The TEM images of three CdSe QDs samples with average diameters of about 2.2 nm (Fig. 6a), 2.9 nm (Fig. 6b), and 4.0 nm (Fig. 6c) demonstrate that the size of CdSe QDs can be controlled by manipulating the reaction conditions. According to the experimental results, large size CdSe QDs tend to form at high reaction temperature and long growth time. For example, at the same growth time of 5 min reaction time, CdSe QDs with 3 nm and 3.51 nm size were generated at 270 °C and 330 °C, respectively. At the same growth temperature of 270 °C, CdSe QDs with 2.6 nm and 3 nm size were produced with the growth time of 1 and 5 min, respectively. This trend is consistent with many published literature.56,57
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Fig. 6 (a–c) TEM images and size distribution histogram of three CdSe QDs samples with average diameter and standard deviation. |
Using continuous reactor to perform chemical synthesis is an efficient way to lower production costs. Compared with conventional batch reactor, continuous reactor has many advantages such as safety, low cost, and both time and space saving.58,59 A well-known continuous reactor, microfluidic reactor, has shown their ability to generate several types of QDs with controllable size and shape.60,61 However, two drawbacks inside the narrow channels makes us reconsider its feasibility. First, the narrow channels confine the volume flow rate, which indicates the difficulty of scale up. Second, the system tends to block if nanocrystals or other insoluble materials precipitate. Supercritical fluid equipment had been demonstrated in the continuous synthesis of Ge and Si nanowires in the past.62 In this article, we also show the ability to scale up using this supercritical fluid equipment by performing continuously producing 5 g CdSe QDs with a production rate of about ∼2.5 g h−1. The schematic picture of our continuous flow system is shown in Fig. 7a. The digital image of the 5 g CdSe QDs produced by this system is shown in Fig. 7b, and Fig. 7c shows the 5 g CdSe QDs irradiated by UV lamp. Fig. 7d also shows a digital image of the 5 g CdSe QDs dispersed in hexane. These results show that the mass production of CeSe QDs by our supercritical fluid equipment is feasible. Compared to the conventional batch reactor to produce QDs, the injection rate can be precisely controlled by the HPLC pump, which can reduce the error caused by manual operation. When compared with the microfluidic reactor, the channel to deliver reactants has a higher volume flow rate because of a relatively large diameter (1/8′′ i.d.) and the reactor also has a larger volume (10 mL). Therefore, the production rate is superior to the microfluidic reactor (1/16′′ i.d.)
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Fig. 7 (a) Schematic picture of our continuous flow system. (b–d) Photographs of 5 g CdSe QDs synthesized by the continuous flow system, under UV excitation, and dispersed in hexane. |
The CdSe QDs synthesized by our approach can be used as phosphors in some applications. For example, white LEDs have received considerable attention because of their many advantages over conventional light such as long lifetime and high efficiency.63 White light can be generated by mixed blue and yellow emission. Therefore, we can simply fabricate white LEDs by combining blue LED chips with yellow CdSe QDs. The photograph of the device is shown in Fig. 8. Furthermore, we have also synthesized other QDs to prove the general applicability of this system. Fig. 9 shows the TEM, HRTEM images, SAED, and XRD patterns of CdS, ZnS, and ZnSe QDs, which were produced by using similar experimental conditions as described for CdSe QDs. Based on the TEM image, the statistical average diameters for the CdS, ZnS, and ZnSe QDs were about 3.8 nm, 4.3 nm, and 4.6 nm, respectively. Clear lattice planes were observed by HRTEM images, which confirmed the high crystallinity of these nanoparticles. The crystal structures confirmed by SAED and XRD patterns were face centered cubic, hexagonal, and face centered cubic for the CdS, ZnS, and ZnSe, respectively. In addition, the optical properties of these QDs (UV-vis absorption and PL spectra) are shown in Fig. 10. Based on the abovementioned results and the various advantages, we believe that the supercritical equipment has the potential to enable the production of a wide variety of nanomaterials.
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Fig. 8 (a) Schematic diagram and (b) photography of white LEDs fabricated by combination of a blue LED chip with yellow CdSe QDs. |
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Fig. 10 UV-vis absorption (solid line) and PL spectra (dotted line) of (a) CdS, (b) ZnS, and (c) ZnSe QDs. |
Footnote |
† Electronic supplementary information (ESI) available: UV-vis absorption and PL spectra of CdSe QDs. See DOI: 10.1039/c4ra05279j |
This journal is © The Royal Society of Chemistry 2014 |