Silica Coating of Water-Soluble CdTe/CdS Core-Shell Nanocrystals by Microemulsion Method

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CHINESE JOURNAL OF CHEMICAL PHYSICS VOLUME 20, NUMBER 6 DECEMBER 27, 2007 ARTICLE Silica Coating of Water-Soluble CdTe/CdS Core-Shell Nanocrystals by Microemulsion Method Yong Wang a, Shu-hua Niu b, Zhi-juan Zhang a, Hai-tao Wang a, Chun-wei Yuan a, De-gang Fu a a. State Key Laboratory of Bioelectronics, Southeast University, Nanjing 210096, China; b. College of Chemistry and Chemical Engineering, Southeast University, Nanjing 210096, China (Dated: Received on August 30, 2007; Accepted on October 10, 2007) Using Te powder as a tellurium source and Na 2 S as a sulfur source, core-shell CdTe/CdS NPs were synthesized at 50 C. UV-visible and photoluminescence (PL) spectra were used to probe the effect of CdS passivation on the CdTe quantum dots. As the thickness of CdS shell increases, there is a red-shift in the optical absorption spectra, as well as the PL spectra. The broadening absorption peaks and PL spectra indicate that the size distributions of CdTe/CdS NPs widen increasingly with the increase of CdS coverage. The PL spectra also show that the fluorescence intensity of CdTe QDs will increase when the particles are covered with CdS shell with ratio of S/Te less than 1.0, otherwise it will decrease if the ratio of S/Te is larger than 1.0. Furthermore, the (CdTe/CdS)@SiO 2 particles were prepared using a water-in-oil microemulsion method at room temperature in which hydrolysis of tetraethyl orthosilicate leads to the formation of monodispersed silica nanospheres. The obtained (CdTe/CdS)@SiO 2 particles show bright photoluminescence with their fluorescence intensity being enhanced 18.5% compared with that of CdTe NPs. TEM imaging shows that the diameter of these composite particles is 50 nm. These nanoparticles are suitable for biomarker applications since they are much smaller than cellular dimensions. Key words: Quantum dots, Photoluminescence, Microemulsion, Silica coating I. INTRODUCTION Semiconductor nanocrystals (NCs), or colloidal quantum dots (QDs), show unique size-dependent optical properties [1] and have great promise for applications in light-emitting devices [2-5] and biological labeling [6-9]. Alivisatos and co-workers first labeled 3T3 mouse fibroblast cells using CdSe/ZnS core-shell nanocrystals enclosed in silica shells [6]. Dubertret and co-workers [7] used DNA-conjugated QD-micelles as in vitro probes to hybridize to specific complementary sequences. They also performed in vivo imaging with QD-micelles by microinjecting early-stage Xenopus embryos. Furthermore, long-term multiple color imaging of live AX2 amoebae cells was performed using quantum dots bioconjugates by Simon et al. [8]. At present, the potential of QDs in biology has begun to be realized. For applications in biological labeling, the primary problem to be resolved is how to prepare QDs and make them biocompatible. There exist two general strategies for preparing QDs: organometallic synthesis based on the high-temperature thermolysis of precursors and aqueous synthesis using polyphosphates or thiols as stabilizing agents [1]. In the organometallic routes, trioctylphosphine oxide (TOPO) capped QDs are prepared with the thermolysis of highly Part of the special issue from The 6th China International Conference on Nanoscience and Technology, Chengdu (2007). Author to whom correspondence should be addressed. E-mail: fudegang@seu.edu.cn toxic organometallic precursors at relatively higher temperatures (250-450 C) [10-12]. The process is difficult to control and the as-prepared QDs are only soluble in nonpolar organic solutions without following surface modification. Transferring them into water is a prerequisite for biological applications, which requires an exchange of capping agents. However, ligand exchange will decrease the photoluminescence and stability of QDs [1]. Compared with the organometallic routes, the aqueous synthesis is cheaper, less toxic, more simple and reproducible [1,13]. Unfortunately, QDs synthesized in aqueous solution usually have low quantum yields and wide size distributions. They need some post-preparative treatments such as size-selective precipitation, photochemical etching, surface modification and/or passivating the QDs with higher band gap inorganic materials to improve their optical properties. Overcoating QDs core with higher band gap semiconductor materials such as ZnS or CdS permits passivation of the surface states [14-16], which improves the photoluminescence quantum yields and enhances the photochemical stability substantially. In previous work, citrate-stablized water-soluble CdSe/CdS NPs have been synthesized in aqueous solution [17-19]. These methods used N,N-dimethylselenourea as a selenium source with the assistance of microwave heating or laser irradiation and the reaction time was longer than 24 h. Here we report another aqueous route to synthesize water-soluble CdTe/CdS core-shell nanoparticles. Using Te powder as a tellurium source for preparing CdTe NPs and using Na 2 S aqueous solution as a sulfur source, core-shell CdTe/CdS NPs were synthesized at 685

686 Chin. J. Chem. Phys., Vol. 20, No. 6 Yong Wang et al. 50 C. The thickness of the CdS shell is easy to control by adjusting the molar ratio of Na 2 S to Te powder. The photoluminescence intensity of the obtained CdTe/CdS core-shell dots can be significantly improved if ratio of S/Te is less than 1.0. In order to improve the photochemical stability of QDs, they need to be encapsulated in inert materials such as polymers and silica [17,20,21]. Silica is an ideal choice, since not only will it protect the QDs from oxidation, but also its surfaces are nontoxic, biological compatible and can be easily functionalized for bioconjugation purposes [22]. In the past decade, silicacoating of various nanoparticles has been widely investigated and significant progress has been achieved, particularly in coating the metal nanoparticles such as Au and Ag [22,23-26]. The procedures to overcoat semiconductor nanoparticles with silica shells can be roughly divided into two methods. One is the socalled Stöber method [27], the other is the microemulsion approach. The silica coating procedure by Stöber method usually includes three steps [28]: (i) modification of the QDs nanoparticle surface using silane coupling agents such as silicon alkoxides with an amino or thiol group as surface primer, (ii) slow silica deposition from a sodium silicate solution, and (iii) extensive growth of the silica shells through sol-gel reaction of silicon alkoxide in ethanol/ammonia mixtures. By the Stöber method, organic-soluble CdSe/CdS and CdSe/ZnS NPs stabilized with TOPO were coated with silica successfully [6,29,30]. Liz-Marzán and co-workers demonstrated that the Stöber method was also applicable to water-soluble nanocrystals. They first prepared CdS@SiO 2 NPs by silica-coating of aqueous CdS stabilized by sodium citrate [31]. By similar procedure, thioglycolic acid capped CdTe NPs were coated with silica shell of 2-5 nm in thickness [32]. Water-soluble CdTe QDs encapsulated in 40-80 nm silica spheres were also achieved by this method [17]. In all above preparations, QDs must be surface-exchanged with silane such as 3-mercaptopropyl trimethoxysilane (MPS). A major disadvantage of the Stöber method for this purpose is the multiplicity of preparation steps which are difficult to control [22]. In comparison with the Stöber method, the microemulsion approach is very robust against reaction conditions and can yield more uniform spheres with smooth surfaces. Single CdSe/ZnS [22] core and multiple CdSe (or CdSe/ZnS) [33] cores encapsulated in single silica shell by the microemulsion method have been reported. These preparations are all based on organicsoluble QDs. Gao et al. coated water-soluble CdTe NPs with silica by microemulsion method and obtained CdTe@SiO 2 about 60 nm in diameter [34], but the fluorescence intensity of CdTe@SiO 2 decreased significantly during the preparation. Early studies have shown that passivating QDs with a wider band gap inorganic shell can substantially improve their photoluminescence and photochemical stability [14-16]. Such core-shell structures as CdS/Cd(OH) 2, CdSe/ZnSe, CdSe/ZnS, CdS/HgS/CdS, CdSe/CdS, and CdTe/CdS have been explored [16]. Therefore, using core-shell structure QDs as seeds for silica-coating can improve the fluorescence intensity of the obtained silica-coated nanoparticles. Overcoating such core-shell structure QDs with silica has been reported [6,17,22,29,30,33,35], but they are almost all based on organic-soluble CdSe/CdS or CdSe/ZnS NCs. Although water-soluble CdSe/CdS NCs have been encapsulated into silica by the Stöber method, the luminescence intensity decreased strongly (about 20 times) in comparison with the uncoated nanoparticles [17]. Using the water-soluble core-shell CdTe/CdS NPs as cores, we have prepared triple layer structured (CdTe/CdS)@SiO 2 NPs by the microemulsion method. The hydrolysis and condensation of tetraethyl orthosilicate (TEOS) in water-in-oil emulsions leads to the formation of monodispersed silica nanospheres. Multiple CdTe/CdS dots were encapsulated into each SiO 2 nanosphere with the diameter of 50 nm. The PL intensity of the obtained (CdTe/CdS)@SiO 2 particles was enhanced 18.5% compared with the CdTe NPs. These triple layer structured nanoparticles are suitable for biolabeling since they are much smaller than the cellular dimensions, have enhanced fluorescence emission, and have silica shells that make them more biologically compatible. II. MATERIALS AND METHODS A. Materials NaBH 4, Tellurium powder, CdCl 2 2.5H 2 O, NaOH, H 2 SO 4, Tetraethyl orthosilicate (TEOS), and n- Hexanol were purchased from Sinopharm Chemical Reagent Co., Ltd. NH 3 H 2 O (25%) and Cyclohexane were purchased from Shanghai Chemical Reagent Co., Ltd. Triton X-100, (3-aminopropyl)triethoxysilane (APTES), and thioglycolic acid (TGA) were obtained from Alfa Aesar. All chemicals were of analytical grade and used without further purification. Deionized water was used in all preparations. B. Preparation of TGA capped CdTe quantum dots NaHTe was prepared using a modified synthesis route reported earlier [36]. Briefly, under Ar atmosphere, 1.2 mmol of sodium borohydride was transferred to a test tube and 5 ml of water was added, then 0.6 mmol of tellurium powder was added to the test tube under magnetic stirring. The reacting system was cooled by ice bath. During the reaction, a small pinhole connected to the tube was exposed to atmosphere to discharge the pressure from the resulting hydrogen. After approximately 10 h, the black tellurium powder disappeared and the colorless NaHTe solution was prepared. 2.4 mmol of CdCl 2 2.5H 2 O was dissolved in 125 ml of

Chin. J. Chem. Phys., Vol. 20, No. 6 Silica Coating of CdTe/CdS Core-Shell Nanocrystals 687 water, and 5.76 mmol of TGA was added under stirring, then 1 mol/l solution of NaOH was added dropwise to adjust the ph to 11.4. The solution was placed in a three-neck flask which is deaerated by Ar bubbling for 30 min. H 2 Te which was generated by dropping 10 ml of 0.5 mol/l H 2 SO 4 to freshly prepared NaHTe solution was passed through the solution accompany with the Ar flow. The resulted orange solution was then refluxed to control the growth of the CdTe NPs. C. Preparation of CdTe/CdS core-shell nanoparticles CdTe/CdS core-shell nanocrystals were synthesized by dropwise addition of the Na 2 S solution to the asprepared CdTe solution described above with their volume ratio was 1:1. After the Na 2 S was added, the solution was stirred for 1 h at 50 C. In order to achieve different shell thickness, four different molar ratios of Na 2 S to CdTe were adopted, which were 0.4, 0.8, 1.5, and 2.5. D. Silica coating of CdTe/CdS nanoparticles 7.5 ml of cyclohexane, 1.77 ml Triton X-100 and 1.8 ml of n-hexanol were added in a flask under stirring. After stirring for 30 min, 480 µl aqueous solution of as-prepared CdTe/CdS NPs and 60 µl of ammonia aqueous solution (25wt%) was added, followed by vigorous stirring for another 30 min. Then the W/O microemulsion system was formed. 10 µl of APTES and 90 µl of TEOS were introduced. The silica growth was completed after 40 h of stirring. Acetone was used to terminate the reaction, followed by centrifuging. The resultant precipitate was washed in sequence with 1- butanol, 2-propanol, ethanol, and water to remove the surfactant and physically adsorbed molecules. Finally, aqueous dispersions of the (CdTe/CdS)@SiO 2 NPs were obtained. dots can be regulated ranging from 2 nm to 5 nm by controlling the reflux time of the reaction mixture [1]. In our preparation of CdTe/CdS core-shell nanocrystals, the concentrations of initial Cd 2+ and Te remain constant. The amount of Na 2 S needed to grow a CdS shell of desired thickness can be calculated from the average diameter of CdTe seeds. Figure 1(a) shows the absorption spectra of five samples with the ratio of S/Te value being 0, 0.4, 0.8, 1.5, and 2.5. All spectra were recorded under the room temperature and the same concentration of CdTe. The spectra have a red-shift with the increase of Na 2 S amount, reflecting an increased leakage of the exciton into the shell [15]. As the thickness of the CdS shell increases, the absorption maximum becomes less evident, which indicates an increased polydispersity. The evolution of the photoluminescence spectra with increasing thickness of CdS shell is displayed in Fig.1(b). The spectra are red-shifted and show broadening FWHM (full width at half maximum) with the S/Te from 0.4 to 2.5. This is due to the increasing size and size-distributions of quantum dots. When the ratios of S/Te are 0.4 and 0.8, a significant increase in PL intensity occurs, compared with CdTe NPs. This fluorescence enhancement resulted from passivating the sur- E. Characterization UV-Vis absorption spectra were recorded with a UV3150 spectrophotometer (Shimadzu, Japan). Photoluminescence (PL) measurements were performed using LS55 luminescence spectrometer (PerkinElmer). Transmission electron microscopy (TEM) and energydispersive X-ray analysis were performed on a Tecnai 20 microscope (FEI). TEM samples were prepared by dropping freshly prepared solution onto a 45-µm carbon-coated copper grid. III. RESULTS AND DISCUSSION A. UV-Vis and PL spectra of CdTe/CdS core-shell nanocrystals Nearly mono-dispersed CdTe NPs were synthesized and stabilized with TGA. The size of CdTe quantum FIG. 1 UV-Vis absorption spectra (a) and PL spectra (b) of CdTe NPs and CdTe/CdS NPs prepared with various molar ratios of S/Te. The initial molecule concentration of CdTe is 2.2 mmol/l.

688 Chin. J. Chem. Phys., Vol. 20, No. 6 face of nonradiative recombination sites with the higher band gap CdS. Otherwise, when the ratio of S/Te increases to 1.5, PL intensity declines to below that of CdTe NPs. As the ratio continues increasing to 2.5, the PL intensity further declines to a very low value. Bawendi et al. reported that the decrease in quantum yield of CdSe/ZnS NPs at higher coverage is attributed to the formation of defects in the ZnS shell and to the bulk lattice parameter of ZnS [15]. So the PL intensity of CdTe dots can be significantly enhanced by coating CdS shell in a particular S/Te range. In previous work, Fendler et al. prepared CdSe/CdS core-shell nanocrystsls [37]. But absorption and excitonic emission peaks of CdS NPs were observed in their system. In this study, these phenomena do not occur, which suggests that nearly all CdS forms shell of CdTe cores without separate nucleation. This indicates that one-pot synthesis of highly luminescent CdTe/CdS NPs can be achieved by this approach. B. Silica coating of CdTe/CdS nanoparticles Osseo-Asare and Arriagada demonstrated that monodisperse SiO2 spheres in the size range of 40-70 nm can be grown by controlled hydrolysis and condensation of tetraethoxysilane within reverse micelles [38]. By the reverse microemulsion method, Tan and co-workers prepared organic-dye-doped silica nanoparticles, the diameter of which is 60±3 nm [39]. These dye-doped silica nanospheres have high fluorescence intensity and photostability in comparison with pure dye molecules. We prepared the (CdTe/CdS)@ SiO2 particles by a modified W/O microemulsion by Tan et al. [39]. The W/O microemulsion system was made up of cyclohexane, Triton X-100, n-hexanol, CdTe/CdS aqueous solution and ammonia. Cyclohexane served as the continuous phase. The role of n-hexanol was as co-surfactant to the nonionic surfactant, Triton X-100. The water pool served as a nano-reactor and the ammonia was the catalyst. Figure 2 showed the TEM images of (CdTe/CdS)@SiO2 nanospheres prepared by the microemulsion method. Multiple CdTe/CdS dots were FIG. 2 TEM images of (CdTe/CdS)@SiO2 nanospheres with different magnification. The initial concentration of CdTe/CdS NPs for this preparation is 2.0 10 5 mol/l. Yong Wang et al. encapsulated within each silica nanosphere, which was in agreement with previous achievement [34]. The average diameter of silica spheres is 50 nm. The silica shell thickness could be tuned by varying the molar ratio of water to surfactant, since this altered the size of the aqueous domain. Energy-dispersive X-ray analysis confirmed the presence of all the following elements: Cd, Te, S, Si, and O. The elements Cd, Te, and S were expected to be from CdTe/CdS NPs, and Si and O were expected to be from SiO2. This also demonstrated the formation of (CdTe/CdS)@SiO2 NPs. Figure 3 depicted the PL spectra of the CdTe NPs, CdTe/CdS NPs and the (CdTe/CdS)@SiO2 NPs. As seen from Fig.3, the silica shell caused a 15 nm blue shift of the photoluminescence maximum, compared with that of CdTe/CdS NPs. This differed from the previous reports on silica coating of QDs [22,23,34]. It should be noticed that the triple layer structured (CdTe/CdS)@SiO2 NPs showed a strong photoluminescence. The PL intensity of (CdTe/CdS)@SiO2 NPs was enhanced 18.5% compared with that of CdTe NPs, although it was lower than that of CdTe/CdS NPs. In previous work, the Sto ber method was usually adopted for coating water-soluble QDs with silica shells [17,31,32]. There is little reporting of silica-coating of water-soluble QDs by reverse microemulsion method. Gao et al. made a valuable attempt to accomplish this [34], but the fluorescence intensity of their QDs decreased significantly after being silica-coated. The photoluminescence of QDs can be substantially improved by passivating their surface states with a wider band gap semiconductor shell. Moreover, the shell also can prevent the core from ambient conditions, thus substantially enhance the QD s photochemical stability. Here we first synthesized water-soluble CdTe/CdS coreshell NPs, then prepared the highly luminescent triple FIG. 3 PL spectra of TGA-capped CdTe dots (a), CdTe/CdS core-shell NPs (b), and (CdTe/CdS)@SiO2 nanospheres (c). All the three samples were dispersed in water with the same molecule concentration of CdTe, which is 6.0 10 5 mol/l. c 2007 Chinese Physical Society

Chin. J. Chem. Phys., Vol. 20, No. 6 Silica Coating of CdTe/CdS Core-Shell Nanocrystals 689 layer structured (CdTe/CdS)@SiO 2 NPs by microemulsion method. Our synthesis of (CdTe/CdS)@SiO 2 NPs presents a simple and effective route to silica-coating water-soluble QDs. IV. CONCLUSION In summary, we have presented an aqueous route to prepare water-soluble CdTe/CdS core-shell NPs. The thickness of CdS shell is easily controlled by adjusting the molar ratios of S/Te. It is demonstrated that the PL intensity of CdTe NPs can be significantly increased at particular CdS coverage. Furthermore, using the water-soluble CdTe/CdS NPs as the cores, we prepared triple layer structured (CdTe/CdS)@SiO 2 NPs by the microemulsion method, whose PL intensity was enhanced 18.5% compared with that of CdTe NPs. The diameter of these triple layer structured NPs is 50 nm. The (CdTe/CdS)@SiO 2 NPs are suitable for biolabeling since they are much smaller than the cellular dimensions and the silica shells make them more biological compatible. V. ACKNOWLEDGMENTS This work was supported by the National Nature Science Foundation of China (No.60121101) and the National Basic Research Program of China (No.2006CB705602-8 and No.2006CB0N1305). [1] N. Gaponik, D. V. Talapin, A. L. Rogach, K. Hoppe, E. V. Shevchenko, A. Kornowski, A. Eychmller, and H. Weller, J. Phys. Chem. B 106, 7177 (2002). [2] V. L. Colvin, M. C. Schlamp, and A. P. Alivisatos, Nature 370, 354 (1994). [3] M. C. Schlamp, X. Peng, and A. P. Alivisatos, J. Appl. Phys. 82, 5837 (1997). [4] H. Mattoussi, L. H. Radzilowski, B. O. Dabbousi, E. L. Thomas, M. G. Bawendi, and M. F. Rubner, J. Appl. Phys. 83, 7965 (1998). [5] M. Gao, C. Lesser, S. Kirstein, H. Möhwald, A. L. Rogach, and H. Weller, J. Appl. Phys. 87, 2297 (2000). [6] M. J. Bruchez, M. Moronne, P. Gin, S. Weiss, and A. P. 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