Journal of Medical and Biological Engineering, 33(1): 23-28 23 Facile Method for Gold Nanocluster Synthesis and Fluorescence Control Using Toluene and Ultrasound Jimmy Kuan-Jung Li1,2 Zhi-Hua Cai1 Cherng-Jyh Ke1 Ching-Yun Chen1 Cheng-An J. Lin1,3 Walter H. Chang1,3,* 1 Department of Biomedical Engineering, Chung Yuan Christian University, Chungli 320, Taiwan, ROC 2 Medical Device Innovation Center, National Cheng Kung University, Tainan 704, Taiwan, ROC 3 Center for Nano Bioengineering, Chung Yuan Christian University, Chungli 320, Taiwan, ROC Received 6 Oct 2010; Accepted 20 Oct 2011; doi: 10.5405/jmbe.874 Abstract This study develops a method for the synthesis of environmentally safe, non-toxic, and color-tunable fluorescent nanomaterials using AuCl3 and toluene without additional surfactants or reduction agents. A facile method for the fluorescence control of gold nanoclusters using simple ultrasonic irradiation is reported. The cluster composition, size, and emission wavelength can be controlled by the ultrasonic irradiation time. There is low photobleaching and the quantum yields are sufficient for optical devices and biosensors. The proper control of ultrasonic conditions such as exposure time, temperature, frequency, duty cycle, and intensity allows the composition and color of fluorescent gold nanoclusters to be adjusted. The obtained materials will be very useful for multicolor molecular probe design in the future. Keywords: Ultrasound, Au, Nanoclusters, Composition, Fluorescence 1. Introduction Research on fluorescent semiconductor nanocrystals, also known as quantum dots, has shown tremendous advances over the past ten years in areas ranging from pure materials science to biological applications. However, most quantum dots are made of cadmium-based or lead-based materials, which contain toxic heavy metals and are therefore potentially harmful to the environment [1]. Artificial fluorescent nanoparticles are promising candidates for more environmentally safe quantum dots. Investigations have been conducted on semiconductor alternatives [2,3], and metallic [4-7], carbon-based [8], and silicon nanoparticles [9-11]. Small metal nanoclusters (NCs) have sizes comparable to the Fermi wavelength of electrons (ca. 0.7 nm), which gives them molecule-like properties, such as size-dependent fluorescence [12,13] and discrete electronic states [14,15]. The fluorescence properties and non-toxicity of Au NCs (AuNCs) make them potential labels for biological experiments [16,17]. The two major synthetic strategies for fabricating fluorescent AuNCs are the template-based and monolayer-protected NC methods. For the template-based method, Zheng et al. and * Corresponding author: Walter H. Chang Tel: +886-3-2654503; Fax: +886-3-2654581 E-mail: [email protected] Garcia-Martinez et al. studied color-tunable fluorescent AuNCs using poly(amidoamine) dendrimers [12,18], and Duan et al. proposed etching methods with hyperbranched and multivalent polymers [19]. For the monolayer-protected NC method, fluorescent AuNCs have been synthesized using glutathione, tiopronin, meso-2,3-dimercaptosuccunic acid, phenylethylthi olate, dodecanethiol, mercaptoundecanol, and bovine serum albumin, [17]. Recently, our group developed a precursor-induced nanoparticle etching technique with reduced lipoic acid as a protected ligand for red-luminescent AuNC synthesis [17]. Ultrasound is considered a ‘green’ technology due to its high efficiency, low instrumental requirements, significantly reduced process time compared with other conventional techniques, and its low cost [20]. It can be considered a combination of chemical reactions that utilizes the formed radicals and physical effects that are associated with an increase in temperature (pyrolysis and combustion) and shearing. The sonochemical synthesis of various types of nanoparticle and nanostructured material composed of noble metals [21,22], transition metals, semiconductors, carbon materials, and polymeric materials has received a lot of attention in recent years [23]. The size and shape of gold nanoparticles vary according to reaction temperature, type of surfactant, thiolated ligand, and ultrasound parameters such as frequency, intensity, duty cycle, and exposure time [23,24]. There have been no previous studies on the fluorescence control of AuNCs under 24 J. Med. Biol. Eng., Vol. 33 No. 1 2013 ultrasound irradiation. In this study, an environmentally friendly and facile method of tunable fluorescent AuNC synthesis and control using toluene and ultrasound irradiation is presented. 2. Experiments Three experiments were conducted. For the first experiment, gold trichloride (AuCl3) powders were dissolved in five solvents for fluorescence testing. 4 ml of solvent (acetone, chloroform, water, methanol, or toluene) (Aldrich) was added into 30 mg of AuCl3 powders (Sigma) under 3 min of vigorous stirring (Vortexer Genie 2 G-560, Scientific Industries, USA) or 60 min of ultrasound irradiation (30 W, 40 kHz,Bransonic 3510, Branson Ultrasonic, The Netherlands) and then centrifuged at 4000 rpm for 5 min (Allegra X-30, Beckman Coulter, USA). The sample vial was held with styrofoam in the middle of the tank and irradiated by ultrasound through the water bath. The fluorescence of each supernatant was then analyzed by photoluminescence (PL) spectroscopy (FP-6200, Jasco, Japan). For the second experiment, three Au compounds (AuCl3, HAuCl4, and AuBr3) (Sigma) were dissolved in toluene for fluorescence testing. A given Au compound was mixed with toluene (Sigma) as a 25-mM solution under 3 min of vigorous stirring or 60 min of ultrasound irradiation, and then centrifuged at 4000 rpm for 5 min. The fluorescence of each supernatant was then analyzed by PL spectroscopy. In the third experiment, the supernatants of AuCl3 in toluene (AuCl3@toluene) solutions were treated for various ultrasound irradiation times. 25-mM AuCl3 solutions were prepared from AuCl3 powders and toluene with 3 min of vigorous stirring. The supernatants were harvested after 5 min of centrifuging (4000 rpm). The supernatants were treated for various periods (0, 30, 60, 120, and 180 min) of ultrasound exposure (30 W, 40 kHz), and then centrifuged at 4000 rpm for 5 min to be harvested as the test samples. The photo-characteristics of the supernatants were analyzed by UV-vis absorption spectroscopy (Cary 50, Varian, USA) and PL spectroscopy, and their photo-stabilities were tested under continuous 320-nm UV irradiation. The size and composition of samples were then evaluated using high-resolution transmission electron microscopy (HRTEM, JEM-2100, JEOL, Japan), atomic force microscopy (AFM, JSPM-5200, JEOL, Japan) and electrospray ionization (ESI) mass spectrometry (LC-ESI-Mass, Mass, USA). Figure 1. PL spectra of supernatants of five kinds of mixture (AuCl3@acetone, chloroform, water, methanol, or toluene) after 3 min of vigorous stirring and 5 min of centrifuging. Figure 2. PL spectra of supernatants of five kinds of mixture (AuCl3@acetone, chloroform, water, methanol, or toluene) after 60 min of ultrasound irradiation and 5 min of centrifuging. 3. Results and discussion Figure 1 shows that the supernatant of AuCl3@toluene has a broad fluorescence spectrum, whereas those of the other tested solutions (AuCl3@acetone, chloroform, water, or methanol) do not. After 60 min of ultrasound irradiation, an obvious fluorescence peak appears for supernatant of AuCl3@toluene; there is no response for the other tested solutions (Fig. 2). After vigorous stirring, only the supernatant of AuCl3@toluene exhibits fluorescence (Fig. 3). Figure 3. PL spectra of supernatants of three kinds of mixture (HAuCl4, AuBr3, or AuCl3@toluene) after 3 min of vigorous stirring and 5 min of centrifuging. Fluorescence Control of Gold Nanoclusters Using Ultrasound Figure 4 shows that the surface plasma resonance (absorption peak at 520 nm) associated with Au nanoparticles with a particle size > 2nm [25] does not appear for the compounds tested here. Instead, an absorption peak at around 300 to 350 nm appears for all supernatants of AuCl3@toluene after vigorous stirring or ultrasound irradiation. This finding is in agreement with the results of previous studies [12,19], in which they synthesized fluorescent AuNCs using templatebased methods. The absorbance increases and the absorption peak red-shifts with increasing ultrasound irradiation time. 0 min 30 min 60 min 120 min 25 AuNCs derived via other synthesis routes (10-3-10-6) [7,15,17] and are comparable to those reported by Zheng et al. (20~30%) [12], Duan et al. (10~20%) [19], and Liu et al. (10~20%) [26]. Although the quantum yield values of the fluorescent AuNCs reported here is only a quarter of those of traditional Cd-based quantum dots, they are in the range required for optical devices and biosensors. Figure 7 shows that there is low photobleaching under 320-nm UV exposure for the fluorescent AuNCs synthesized here. This result is similar to those obtained for traditional semiconductor quantum dots (CdSe/ZnS) and template-based NCs [12,19], but quite different from those obtained for monolayer- protected AuNCs [17]. 180 min (a) 0 min 30 min 60 min 120 min 180 min (a) (b) Figure 4. (a) Photographs of samples harvested at ultrasonic exposure times of 0, 30, 60, 120, and 180 min under daylight. (b) UV-vis absorption spectra of the samples in (a). Figure 5 shows the PL spectra of the samples obtained under 350-nm light excitation. There is an obvious red-shift of the fluorescence peak with increasing ultrasound irradiation time. The intensity of the fluorescence peak initially increases with ultrasound irradiation time (from 0 to 60 min), and then decreases after longer exposures (120 and 180 min). Figure 6 shows the nonshifted emission peak that appears with the change of the excitation wavelength for each sample. These data give strong evidence that the observed emission is real luminescence from the relaxed states rather than a scattering effect. The wavelength difference between the emission and excitation peaks widening with increasing ultrasound irradiation time also supports this. Previous study suggests that the fluorescence mechanisms in our samples are caused by the excitation of inner electrons instead of the vibrations of the energy band [26]. The increased size of the Stokes shift and energy gap imply that the particle size of the fluorescent AuNCs increases with ultrasound irradiation time. Using quinine sulfate (Sigma) (quantum yield = 0.54 in H2SO4) as the reference, the quantum yields of fluorescent AuNCs with 0, 60, and 180 min of ultrasonic irradiation were 15 2.5%, 20.8 2.3%, and 17.4 4.2% in toluene, respectively. These values are approximately 2 ~ 3 orders of magnitude higher than the quantum yields of fluorescent (b) Figure 5. (a) Photographs of samples harvested at ultrasonic irradiation times of 0, 30, 60, 120, and 180 min under UV excitation. (b) PL spectra of the samples in (a). Because of the resolution limit of TEM (about 1 nm), our samples could not be detected in TEM images. This is consistent with the results obtained for fluorescent AuNCs synthesized by other groups [12,19,26]. AFM scans (Fig. 8) reveal that only the sample treated with 180 min of ultrasonic irradiation could be detected, with the largest cluster height found to be 1.6 nm. The mean diameter was below 0.5 nm, but the standard deviation was higher than 0.6 nm (beyond the detection limitation of AFM). This indicates that even in the group with 180 min of ultrasonic irradiation, most clusters are smaller than 1.0 nm. The results of ESI mass spectrometry analysis show strong evidence of composition control using ultrasonic irradiation (Fig. 9). There are many kinds of cluster composition, especially with mass-to-charge (m/z) ratios smaller than 382.31 (Fig. 9a). The two most abundant compositions are Au11 (m/z = 359.20, m/e = 1.82) and Au16 (m/z = 382.31, m/e = 1.94). After 60 min of ultrasonic irradiation, the composition becomes purer, with the most abundance being Au16 (m/z = 382.33, m/e = 1.94) (Fig. 9b). For a longer 26 J. Med. Biol. Eng., Vol. 33. No. 1 2013 (a) Figure 7. Photostability test results of samples with 0 min (black), 60 min (red), and 180 min (blue) of ultrasonic irradiation and an organic blue fluorescent dye, quinine sulfate (dark cyan), under continuous 320-nm excitation. (b) Figure 8. AFM images (0.5 μm × 0.5 μm) of a sample after 180 min of ultrasonic irradiation. The highest spot is about 1.6 nm. (c) Figure 6. PL excitation spectra of samples with (a) 0 min, (b) 60 min, and (c) 180 min of ultrasonic irradiation. ultrasonic irradiation time (180 min) (Fig. 9c), the most abundant composition is Au16 (m/z = 382.39, m/e = 1.94), and more kinds of cluster with m/z ratios larger than 382.39 appear. The fluorescence properties (wavelengths and quantum yields) of the fluorescent AuNCs are similar to those of PAMAM-encapsulated Au13 clusters [12] and PEI stabilized clusters [19]. The ESI mass spectrometry data also show that the fluorescent AuNCs harvested from the mixture of AuCl3@toluene at the beginning mainly contain Au11 and Au16 gold atoms. After 60 min of ultrasonic irradiation, the cluster compositions become purer and larger, with a wider Stokes shift and a higher quantum yield. Longer ultrasonic irradiation (180 min) might induce larger cluster size formation according to the results of the emission red shift (Fig. 5 and Fig. 6) and increased number of compositions (Fig. 9). From the above results, it could be hypothesized that the decomposition of toluene might be induced by vigorous stirring or ultrasound irradiation, the remains of which react with AuCl3 to form AuNCs. The cavitation effect of ultrasonic irradiation is a potential mechanism of size and composition control of AuNCs through the surfactant- and reduction-agent-free method [27,28]. According to the cavitation-enhanced crystal nucleation model proposed by Grossier et al. [29], ultrasonic irradiation might induce an increase in the size of AuNCs via the cavitation effect. During acoustic cavitation, free radicals are formed due to the dissociation of vapors trapped in cavities [20]. Free radicals of toluene decomposition produced by vigorous stirring or ultrasound irradiation and their oxides might act as surfactants of AuNCs and cause the variation of cluster compositions. Fluorescence Control of Gold Nanoclusters Using Ultrasound 27 4. Conclusion (a) Fluorescent AuNCs were tuned according to size and color through a facile ultrasound irradiation method. This surfactantand reduction-agent-free method is more environmentally friendly than other methods, which utilize inorganic fluorescent nanoparticles. Ultrasonic irradiation can easily modulate cluster composition, size, fluorescence color, quantum yield, and Stokes shift via exposure time. The optical properties, namely absorption, PL, PL excitation, and photostability characteristics, of the AuNCs are similar to those reported in previous studies. Furthermore, there is low photobleaching and the quantum yields are sufficient for optical devices and biosensors. Although the mechanism of this synthesis method for fluorescent AuNCs still needs to be clarified, it is believed that the proper control of ultrasonic irradiation conditions such as exposure time, temperature, frequency, duty cycle, and intensity, offers a good strategy for the composition and color control of fluorescent AuNC synthesis. These materials will be very useful for multicolor molecular probe design in the future. Acknowledgements We gratefully acknowledge the financial support via research grants from the Taiwan National Science Council (NSC 101-2627-M-033-001, NSC 101-2120-M-038-001, NSC 101-2628-E-033-001-MY3). References [1] [2] (b) [3] [4] [5] [6] [7] [8] [9] (c) Figure 9. ESI mass spectra of samples with (a) 0, (b) 60, and (c) 180 min of ultrasonic irradiation. B. A. Rzigalinski and J. S. Strobl, “Cadmium-containing nanoparticles: perspectives on pharmacology and toxicology of quantum dots,” Toxicol. Appl. Pharmacol., 238: 280-288, 2009. N. Pradhan, D. Goorskey, J. Thessing and X. Peng, “An alternative of CdSe nanocrystal emitters: pure and tunable impurity emissions in ZnSe nanocrystals,” J. Am. Chem. Soc., 127: 17586-17587, 2005. D. J. Bharali, D. W. Lucey, H. Jayakumar, H. E. Pudavar and P. N. Prasad, “Folate-receptor-mediated delivery of InP quantum dots for bioimaging using confocal and two-photon microscopy,” J. Am. Chem. Soc., 127: 11364-11371, 2005. L. A. Peyser, A. E. Vinson, A. P. Bartko and R. M. Dickson, “Photoactivated fluorescence from individual silver nanoclusters,” Science, 291: 103-106, 2001. J. Zheng, J. T. Petty and R. M. Dickson, “High quantum yield blue emission from water-soluble Au8 nanodots,” J. Am. Chem. Soc., 125: 7780-7781, 2003. J. T. Petty, J. Zheng, N. V. Hud and R. M. Dickson, “DNA-templated Ag nanocluster formation,” J. Am. Chem. Soc., 126: 5207-5212, 2004. Y. Negishi, K. Nobusada and T. Tsukuda, “Glutathione-protected gold clusters revisited: bridging the gap between gold(I)-thiolate complexes and thiolate-protected gold nanocrystals,” J. Am. Chem. Soc., 127: 5261-5270, 2005. Y. P. Sun, B. Zhou, Y. Lin, W. Wang, K. A. Fernando, P. Pathak, M. J. Meziani, B. A. Harruff, X. Wang, H. Wang, P. G. Luo, H. Yang, M. E. Kose, B. Chen, L. M. Veca and S. Y. Xie, “Quantum-sized carbon dots for bright and colorful photoluminescence,” J. Am. Chem. Soc., 128: 7756-7757, 2006. F. Erogbogbo, K. T. Yong, I. Roy, G. Xu, P. N. Prasad and M. T. Swihart, “Biocompatible luminescent silicon quantum dots for imaging of cancer cells,” ACS Nano, 2: 873-878, 2008. 28 J. Med. Biol. Eng., Vol. 33 No. 1 2013 [10] A. Troia, A. Giovannozzi and G. Amato, “Preparation of tunable silicon q-dots through ultrasound,” Ultrason. Sonochem., 16: 448-451, 2009. [11] S. Klein, O. Zolk, M. F. Fromm, F. Schrodl, W. Neuhuber and C. Kryschi, “Functionalized silicon quantum dots tailored for targeted siRNA delivery,” Biochem. Biophys. Res. Commun., 387: 164-168, 2009. [12] J. Zheng, C. Zhang and R. M. Dickson, “Highly fluorescent, water-soluble, size-tunable gold quantum dots,” Phys. Rev. Lett., 93: 077402-1-077402-4, 2004. [13] C. C. Huang, Z. Yang, K. H. Lee and H. T. Chang, “Synthesis of highly fluorescent gold nanoparticles for sensing mercury(II),” Angew. Chem.-Int. Edit., 46: 6824-6828, 2007. [14] S. Chen, R. S. Ingram, M. J. Hostetler, J. J. Pietron, R. W. Murray, T. G. Schaaff, J. T. Khoury, M. M. Alvarez and R. L. Whetten, “Gold nanoelectrodes of varied size: transition to molecule-like charging,” Science, 280: 2098-2101, 1998. [15] D. Lee, R. L. Donkers, G. Wang, A. S. Harper and R. W. Murray, “Electrochemistry and optical absorbance and luminescence of molecule-like Au38 nanoparticles,” J. Am. Chem. Soc., 126: 6193-6199, 2004. [16] R. A. Sperling, P. Rivera Gil, F. Zhang, M. Zanella and W. J. Parak, “Biological applications of gold nanoparticles,” Chem. Soc. Rev., 37: 1896-1908, 2008. [17] C. A. Lin, T. Y. Yang, C. H. Lee, S. H. Huang, R. A. Sperling, M. Zanella, J. K. Li, J. L. Shen, H. H. Wang, H. I. Yeh, W. J. Parak and W. H. Chang, “Synthesis, characterization, and bioconjugation of fluorescent gold nanoclusters toward biological labeling applications,” ACS Nano, 3: 395-401, 2009. [18] J. C. Garcia-Martinez and R. M. Crooks, “Extraction of Au nanoparticles having narrow size distributions from within dendrimer templates,” J. Am. Chem. Soc., 126: 16170-16178, 2004. [19] H. Duan and S. Nie, “Etching colloidal gold nanocrystals with hyperbranched and multivalent polymers: a new route to fluorescent and water-soluble atomic clusters,” J. Am. Chem. Soc., 129: 2412-2413, 2007. [20] E. V. Rokhina, P. Lens and J. Virkutyte, “Low-frequency ultrasound in biotechnology: state of the art,” Trends Biotechnol., 27: 298-306, 2009. [21] Y. Nagata, Y. Mizukoshi, K. Okitsu and Y. Maeda, “Sonochemical formation of gold particles in aqueous solution,” Radiat. Res., 146: 333-338, 1996. [22] H. X. Xu and K. S. Suslick, “Sonochemical synthesis of highly fluorescent Ag nanoclusters,” ACS Nano, 4: 3209-3214, 2010. [23] K. Okitsu, M. Ashokkumar and F. Grieser, “Sonochemical synthesis of gold nanoparticles: effects of ultrasound frequency,” J. Phys. Chem. B., 109: 20673-20675, 2005. [24] A. Gedanken, “Using sonochemistry for the fabrication of nanomaterials,” Ultrason. Sonochem., 11: 47-55, 2004. [25] K. S. Lee and M. A. El-Sayed, “Gold and silver nanoparticles in sensing and imaging: sensitivity of plasmon response to size, shape, and metal composition,” J. Phys. Chem. B, 110: 19220-19225, 2006. [26] Z. Liu, L. Peng and K. Yao, “Intense blue luminescence from self-assembled Au-thiolate clusters,” Mater. Lett., 60: 2362-2365, 2006. [27] S. Theerdhala, D. Alhat, S. Vitta and D. Bahadur, “Synthesis of shape controlled ferrite nanoparticles by sonochemical technique,” J. Nanosci. Nanotechnol., 8: 4268-4272, 2008. [28] J. Gonzalez-Garcia, M. D. Esclapez, P. Bonete, Y. V. Hernandez, L. G. Garreton and V. Saez, “Current topics on sonoelectrochemistry,” Ultrasonics, 50: 318-322, 2010. [29] R. Grossier, O. Louisnard and Y. Vargas, “Mixture segregation by an inertial cavitation bubble,” Ultrason. Sonochem., 14: 431-437, 2007.
© Copyright 2025 Paperzz