Qin Hua,
Man Chin Paaua,
Yan Zhangb,
Xiaojuan Gong‡
b,
Lei Zhang‡b,
Dongtao Lu‡b,
Yang Liu‡b,
Qiaoling Liu‡b,
Jun Yao*c and
Martin M. F. Choi*a
aPartner State Key Laboratory of Environmental and Biological Analysis, and, Department of Chemistry, Hong Kong Baptist University, 224 Waterloo Road, Kowloon Tong, Hong Kong SAR, China. E-mail: mfchoi@hkbu.edu.hk
bInstitute of Environmental Science, and School of Chemistry and Chemical Engineering, Shanxi University, Taiyuan 030006, China
cSchool of Civil & Environmental Engineering, National International Cooperation Base on Environment and Energy, University of Science and Technology Beijing, 30 Xueyuan Road, 100083 Beijing, China. E-mail: yaojun@ustb.edu.cn
First published on 7th April 2014
A fast and green approach to synthesise ultrasmall nitrogen (N) and sulfur (S)-doped carbon dots (N,S-C-dots) by microwave-assisted pyrolysis of the precursors rice as carbon source and N-acetyl-L-cysteine (NAC) as N and S dopant has been developed. The obtained N,S-C-dots were fully characterised by elemental analysis, Fourier transform infrared spectroscopy, X-ray photoelectron spectroscopy, transmission electron microscopy, UV-vis absorption and photoluminescence (PL) spectroscopy. The undoped C-dots (derived from rice only) and N,S-C-dots possess different chemical compositions, sizes and spectral properties. With the assistance of high-performance liquid chromatography coupled with fluorescence detection (HPLC-FD), the effect of different mass ratios of NAC to rice (NAC/rice) on N,S-C-dots was investigated. Higher NAC/rice ratio benefits the generation of N,S-C-dots with stronger fluorescence emission. In addition, the HPLC separated N,S-C-dots fractions were collected and further characterised by mass spectrometry, UV-vis absorption and PL spectroscopy, showing that the structural changes induced by doping with heteroatoms N and S plays a key role in regulating the PL properties of the N,S-C-dots. This work highlights the merits of synthesising N,S-C-dots from readily available natural bioresources and applying modern HPLC-FD technology to study the effect of doped heteroatoms on N,S-C-dots properties.
Impressive progresses have been made on the synthesis of C-dots with methods such as electrochemical oxidation,9,10 laser ablation,5,11,12 hydrothermal synthesis,13–15 pyrolysis,2,3,16 and microwave-assisted heating.17–20 Nevertheless, most of these synthetic methods suffer from shortcomings such as expensive equipment required, time-consuming procedures, slow and high cost. Recently Li et al.21 synthesised C-dots by simply mixing monosaccharide with basic solutions without additional energy input or external heating. More importantly, the synthesis of C-dots with naturally available bioresources is attractive in the area of nanotechnology. For example, carbonization of orange juice,13 potato,22 protein,23 willow bark,24 trapa bispinosa peel,25 hair fibre,26 and bombyx mori silk27 offer facile routes for synthesis of fluorescent C-dots. To date, there is a great interest in incorporating heteroatoms into C-dots framework to enhance the photoluminescence (PL) properties of C-dots. So far numerous strategies have been conducted to produce C-dots containing nitrogen. However, reports about fabricating C-dots containing other heteroatoms whether singly or dually doped with other dopants are still limited. Xu et al.28 synthesised phosphate functionalized two colour C-dots through acidic oxidation of sucrose by H3PO4. Wang et al.29 fabricated phosphorus-containing C-dots with strong green fluorescence from phytic acid and ethylenediamine. Sun et al.26 produced luminescent sulfur and nitrogen-co-doped C-dots from hair fibre. Dong et al.30 reported the preparation of highly fluorescent C-dots doped with nitrogen and sulfur atoms (N,S-C-dots) from citric acid and L-cysteine. Nevertheless, exploring new synthetic routes for synthesis of C-dots doped with heteroatoms is still a tricky challenge.
In the present work, we report a “green” and facile approach to synthesise strongly fluorescent N,S-C-dots by microwave-assisted pyrolysis of rice and N-acetyl-L-cysteine (NAC) as precursors. Rice rich in carbon atoms can serve as an excellent carbon source. NAC comprising both N and S atoms can function as dopants for C-dots. It possesses good water-solubility, and is non-toxic and cost-effective. The synthesis is completed in a domestic microwave oven within 30 min. Doping N and S into C-dots greatly increases the quantum yield (ΦS) of C-dots. The obtained N,S-C-dots solution exhibits homogeneous phase without any noticeable precipitation at ambient conditions for six months, indicating their long-term colloidal stability. Herein, high-performance liquid chromatography coupled with fluorescence detection (HPLC-FD) has been successfully applied to study the effect of mass ratio of NAC to rice (NAC/rice) on the as-synthesised N,S-C-dots products. Remarkably, HPLC-FD is able to identify how different NAC/rice affects the PL of the N,S-C-dots products. Finally, the HPLC separated fractions of the undoped C-dots (derived from rice only) and N,S-C-dots were collected and characterised by matrix-assisted laser desorption/ionisation time-of-flight mass spectrometry (MALDI-TOF MS), UV-vis absorption and PL spectroscopy, probing the structural changes and PL of N,S-C-dots induced by doping with N and S. To our knowledge, this is the first report on microwave-assisted synthesis of N,S-C-dots using rice and NAC as precursors and application of HPLC-FD technique to analyse the separated N,S-C-dots fractions. Our work certainly adds to the database on the synthesis of C-dots from natural resource and provokes better understanding of the as-synthesised C-dots product.
:
99 v/v) as the mobile phase. The flow rate was set at 0.80 mL min−1, the injection volume was 20 μL and the column temperature was maintained at 25 ± 1 °C.
:
1 v/v). 2.0 μL of this solution was deposited on a MALDI target plate for two times separately. The sample was air-dried and was then inserted into the instrument. The MALDI-TOF MS were acquired in positive ionisation mode under a pulsed N2 laser at 337 nm. In general, 500 laser shots were averaged for each spectrum.
The doping of heteroatoms into N,S-C-dots was initially probed by elemental analysis in Table S1A (ESI),† revealing that the undoped C-dots are mainly composed of carbon (C), hydrogen (H) and oxygen (O) whereas the N,S-C-dots contain C, H, O, N, and S. The elemental content of the undoped C-dots differs significantly from the N,S-C-dots. Higher N and S contents and less O content are found for the N,S-C-dots. For ease of comparison, the elemental contents of the C-dots are expressed in terms of relative number of atom as depicted in Table S1B.† The empirical formulae for the undoped C-dots and the N,S-C-dots are C12H22O12 and C13H23O9N2S, respectively. The undoped C-dots and the N,S-C-dots contain almost the same number of C atoms. However, the numbers of O, N and S atoms in the N,S-C-dots differ significantly from that of the undoped C-dots. Three more O atoms are found in the undoped C-dots. By contrast, two N and one S atoms are found in the N,S-C-dots but not in the undoped C-dots. In other words, the three O atoms in the undoped C-dots were replaced by the N and S atoms in the N,S-C-dots after passivation with NAC, indicating that the N and S originated from NAC could co-dope into C-dots.
IR measurement was used to confirm the doping of N and S into C-dots and investigate the differences in surface functionality of the two kinds of C-dots. Fig. S1† depicts the IR spectra of the undoped C-dots (spectrum a) and the N,S-C-dots (spectrum b). A broad absorption peak attributing to the O–H stretching (∼3238–3470 cm−1) and sharp absorption peaks corresponding to C–H (2930 cm−1), C–O (1152 cm−1), and C–O–C stretching (1021 cm−1) are found for both undoped C-dots and N,S-C-dots. These functional groups are believed to be derived from rice as their carbon sources. The IR spectrum of rice possessing these functionalities is displayed in Fig. S2A.† More importantly, the characteristic absorption peaks C
O stretching (1716 cm−1), amido CON–H bending (1545 cm−1), amido CO–N (1375 cm−1) and C–S (1081 cm−1) stretching are identified in the N,S-C-dots, suggesting the presence of carboxylic, amido and alkyl sulfide functionalities on the N,S-C-dots. The disappearance of the S–H stretching (2550 cm−1) band in N,S-C-dots indicates that the initial S–H in NAC has been decomposed and S was incorporated into the N,S-C-dots.
The IR of NAC is shown in Fig. S2B† for comparison. Interestingly, an absorption peak associated with the C
O stretching (1716 cm−1) which is absent from the IR spectrum of rice is observed in the undoped C-dots, suggesting the possible oxidation of carbon. In addition, the IR spectra of both undoped C-dots and N,S-C-dots possess a distinctive absorption peak at 1653 cm−1, indicating the formation of C
C unsaturated bonds in the carbon cores which are consistent with other fluorescent C-dots.20,22 In summary, the pyrolysis of rice and doping of N and S heteroatoms into C-dots should have taken place at high temperature under microwave irradiation, resulting in the formation of N,S-C-dots covered with carboxylic acid, amido and alkyl sulfide moieties. These functional groups are potential linkers for attachment of therapeutic moieties for targeted drug delivery.
To gain further insight into the surface functional groups and element states of C-dots, XPS of C-dots were acquired. Fig. 1 and 2 depict the survey scan of the undoped C-dots and the N,S-C-dots, respectively. For the undoped C-dots, three peaks centred at 285.0, 400.5 and 532.3 eV associated with C1s, N1s and O1s are identified (Fig. 1A). For the N,S-C-dots, an additional peak at 165.0 eV attributing to S2p is observed (Fig. 2A), inferring the presence of S in the C-dots.30 The peak associated with N1s of N,S-C-dots is much more intense than that of the undoped C-dots, indicating that a higher content of N in the C-dots. These results further confirm the incorporation of heteroatoms N and S from NAC into N,S-C-dots. Fig. 1B and 2B illustrate the C1s XPS spectra of the undoped C-dots and the N,S-C-dots, respectively. For the undoped C-dots, the C1s spectrum is deconvoluted into three peaks at 284.6, 286.2 and 287.9 eV corresponding to C
C, C–O and C
O, respectively.31–34 For the N,S-C-dots, additional peaks at 283.9, 285.2 and 289.0 eV associated with C–S–C, C–N and O–C
O are observed.31,35–37 Fig. 2C reveals the S2p XPS of N,S-C-dots. The S2p XPS could be fitted into two peaks at 163.4 and 164.8 eV corresponding to S2p2/3 and S2p1/3 C–S–C, respectively.30,37 Again, these confirm the doping of N and S onto the surface of the as-synthesised N,S-C-dots. In summary, the XPS data show the presence of C
C, C–O and C
O surface-functionalities on the undoped C-dots whereas the C
C, C–O, C
O, C–S–C, C–N and O–C
O surface-functionalities are on the N,S-C-dots. Both XPS and IR confirm the surface of N,S-C-dots is co-doped with N and S atoms.
TEM has been used extensively as a powerful tool in the study of NPs from which the morphology and size can be identified. Fig. 3A and C shows the representative TEM images of the undoped C-dots and the N,S-C-dots, respectively. Both undoped C-dots and N,S-C-dots are mostly of spherical morphology and disperse rather evenly on the TEM grid surface. The corresponding histograms obtained by statistical analysis of approximately 100 particles using the ImageJ software are displayed in Fig. 3B and D. The Gaussian fitting curves reveal that the corresponding particle size distributions of undoped C-dots and N,S-C-dots are 1.3–6.4 nm and 0.7–2.6 nm with average diameters of 3.3 ± 0.5 nm and 1.4 ± 0.2 nm, respectively. It is obvious that the N,S-C-dots are smaller than the undoped C-dots and the N,S-C-dots have narrower size range. In brief, doping N and S into C-dots could inhibit the growth of carbon core, allowing the formation of ultrasmall C-dots (<2 nm).
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| Fig. 3 (A) TEM image and (B) particle size distribution histogram of undoped C-dots. (C) TEM image and (D) particle size distribution histogram of N,S-C-dots. | ||
In quest of exploring the optical properties of the as-prepared C-dots, the UV-vis absorption and PL spectra are acquired and depicted in Fig. 4. For the undoped C-dots, an absorption peak at 275 nm corresponding to the n → π* transition of C
O bond and a shoulder peak at ca. 225 nm attributing to the π → π* transition of the aromatic sp2 domain (spectrum a in Fig. 4A) are observed.38,39 For the N,S-C-dots (spectrum b in Fig. 4A), in addition to the n → π* transition at 263 nm, a prominent absorption peak at 335 nm is found, probably attributing to the formation of excited defect surface states induced by the N and S heteroatoms.40–42 Fig. 4B and C display the PL spectra of the undoped C-dots and the N,S-C-dots under various excitation wavelengths (λex), respectively. The PL spectra are bathochromically shifted with the increase in the λex, indicating that the PL band can be tuned by adjusting the λex. The emission peaks (λem) are red-shifted from 412 to 558 nm for the undoped C-dots and from 415 to 545 nm for the N,S-C-dots when the λex moves from 300 to 500 nm. The λex-dependent PL behaviour is common with C-dots. This means that the λem can be tuned by just controlling the λex without changing C-dots. The emission intensities of the N,S-C-dots are much stronger than that of the undoped C-dots. Obviously, doping N and S into the C-dots surface could introduce surface states with a concomitant effect of enhancing the fluorescence of C-dots.
The ΦS of C-dots is determined.† The ΦS excited at 340 nm is only 0.090% for the undoped C-dots (curve 1 in Fig. S3†). The ΦS of the N,S-C-dots are 1.16 and 2.36% when excited at 340 and 390 nm (curves 2 and 3 in Fig. S3†), respectively using quinine sulfate as the reference. The ΦS of N,S-C-dots is about 13–26 times of the undoped C-dots, indicating that doping N and S into C-dots could greatly improve its ΦS. These results are consistent with a previous report that reduced C-dots have higher ΦS than that of oxidised C-dots.43 Our undoped C-dots contain higher oxygen content, i.e., oxygenated functionalities (vide supra) and is therefore more oxidised than the N,S-C-dots.
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| Fig. 6 (A) MALDI-TOF MS and (B) expanded MS in the mass range 985–1385 Da of fraction 12 in N,S-C-dots. | ||
For comparison, the MS of fraction 12 in the undoped C-dots possessing the strongest fluorescence emission was acquired and displayed in Fig. 7. The MS feature is different from that of the N,S-C-dots. A large number of higher mass fragments are observed for the undoped C-dots. The highest mass ion is located at 7705 Da (Fig. 7A) which is about 3 times that of the N,S-C-dots (Fig. 6A), indicating that the N,S-C-dots is smaller (lighter) than the undoped C-dots which is consistent with their sizes. The average size of the undoped C-dots is about 2.4 times that of the N,S-C-dots (Fig. 3). However, the mass spectral feature in the mass range 1000–3000 Da shows some similarity to that of the N,S-C-dots. Fig. 7B depicts the expanded MS of fraction 12 in the mass range 1000–1400 Da. Fragments of m/z 115 and 175 are common, indicating that the chemical composition of the undoped C-dots is similar to that of the N,S-C-dots since both are derived from the same carbon source, i.e., rice. Again, the fragment (m/z 115) is from the loss of a C5H7O3 molecule and the fragment (m/z 115) is from a glucose unit (C6H10O5, m/z 162) minus a –CH2OH group (31) and an O atom (16). Also a series of minor mass spacing in the mass units of 18, 17, and 15 corresponding to the loss of H2O, –OH, and –CH3 moieties are also found. Interestingly, at the higher mass range 3500–7000 Da, regular mass spacings of 131 corresponding to a C5H7O4 unit are found for the undoped C-dots (Fig. 7A) which is not observed in the MS of the N,S-C-dots.
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| Fig. 7 (A) MALDI-TOF MS of fraction 12 in the undoped C-dots. (B) and (C) are expanded MS in the mass ranges 1000–1400 and 3790–5830 Da, respectively. | ||
Fig. 7C displays the expanded MS of fraction 12 in the undoped C-dots in the mass range 3790–5830 Da. We speculate that the fragment (m/z 131) is derived from the residual amylopectin on the undoped C-dots surface. To further confirm this, the dissolved amylopectin obtained by sonication of rice powder in DDI water was subjected to MS analysis and the results are depicted in Fig. S5A.† The highest mass ion of rice is located at 9428 Da. The MS displays very regular mass spacings of fragments (m/z 162). Fig. S5B and C† show the expanded MS in the mass range 1190–3230 and 3210–5250 Da, respectively. Numerous evenly distributed mass spacing in mass units of 162 corresponding to a glucose unit (C6H10O5) are identified on both expanded MS, indicating that the rice sample is mainly composed of amylopectin and amylose. As such, we can deduce that the 131 mass unit in the MS of the undoped C-dots is also a fragment of amylopectin corresponding to the loss of a –CH2OH group (31) from a glucose unit (162). These results suggest that synthesis without NAC fails to completely carbonise amylopectin/amylose but NAC can greatly improve the carbonisation of rice under our experimental conditions. Other attributes of the N,S-C-dots are that they possess stronger fluorescence and are smaller in size as compared to the undoped C-dots.
O bond (Fig. S6A†).38,39 However, their spectral features are different, inferring that they represent different C-dots species in the undoped C-dots product. As expected for reversed-phase HPLC separation, the earlier eluted solutes should have higher polarity than that of the later eluted ones. The earlier eluted fractions 1–10 display more prominent absorption bands at 250–285 nm corresponding to the n → π* transition of C
O bond, inferring that they contain more surface-attached oxygenated functionalities (e.g., carboxylic and carbonyl groups) whereas the later fractions 11 and 12 probably contain less oxygenated groups or more sp2 domains in the C-dots. Upon excitation at 340 nm, fractions 1–12 show emission bands in the range 410–424 nm (Fig. S6B†) which is consistent with that of the unseparated ones. For the N,S-C-dots, although all fractions exhibit typical absorption spectral characteristics of the unseparated N,S-C-dots mixture, their spectra are more distinctive. They show shoulder or absorption bands between 240–268 nm assigned to the n → π* transition of C
O bond38,39 and another absorption bands ca. 300–360 nm ascribed to the excited defect surface states induced by the heteroatoms N and S (Fig. 8A).40–42 These absorption bands are prominent and hypsochromically shifted from 347 to 323 nm for fraction 2 to 11. Fractions 2, 3, 5–7, and 9–12 exhibit more distinctive double absorption bands, not observed before, corresponding to the n → π* transition of C
O bond and the defect surface state induced by N and S atoms. For the later eluted fractions 7–12, the n → π* band is less prominent, indicating that they possess less C
O and COOH groups; thus, they are less polar and retain better on the C18 column. When fractions 1–12 are excited at 340 nm, the emission spectrum is bathochromatically shifted from 382 to 423 nm (Fig. 8B). These observations indicate that each C-dots species displays its unique spectral properties and their co-existence in a C-dots product would also contribute to the λex-dependent PL behaviour of the as-synthesised C-dots.
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| Fig. 8 (A) and (B) are the absorption and fluorescence emission spectra of peak 1–12 (from bottom to top) of N,S-C-dots in Fig. 5C, respectively. | ||
Table 1 summarises the ΦS of fractions 1–12 in the N,S-C-dots upon excitation at 390 nm and using quinine sulfate as the reference. Apparently, fraction 12 displays the highest ΦS (7.37%) which is about 3 times that of the unseparated N,S-C-dots mixture (2.36%). Our results demonstrate that some absorbing species displaying no or low PL are also present in the N,S-C-dots mixture.46 By HPLC fractionation, C-dots species exhibiting appreciable PL performance could be isolated and possibly be a promising cellular imaging probe.
| Fraction | 1 | 2 | 3 | 4 | 5 | 6 | 7 | 8 | 9 | 10 | 11 | 12 |
|---|---|---|---|---|---|---|---|---|---|---|---|---|
| ΦS (%) | 0.81 | 0.91 | 0.82 | 1.85 | 2.05 | 1.37 | 2.03 | 1.43 | 1.97 | 1.46 | 2.36 | 7.37 |
O bond of the undoped C-dots produces rather weak fluorescence emission. By contrast, when C-dots is doped with heteroatoms N and S, its absorption band could bathochromatically shift to 335 nm attributing to the formation of excited defect surface state which can enhance fluorescence emission. Moreover, our HPLC analysis has demonstrated that an as-synthesised N,S-C-dots product comprises numerous C-dots species. They are similar in particle size and mass but exhibit unique PL properties and ΦS, inferring that particle size is not the key parameter that determines the PL properties of the N,S-C-dots species. It is anticipated that our developed method will open new avenues in synthesising strongly emitted C-dots from biomaterials. It also exhibits a potential of fast, easy and inexpensive large-scale production of C-dots from natural material.
Footnotes |
| † Electronic supplementary information (ESI) available: Elemental analysis data, IR spectra of C-dots, rice and NAC, determination of quantum yield, plots of integrated PL intensity against absorbance of undoped C-dots and N,S-C-dots, MALDI-TOF MS of HPLC fractions of N,S-C-dots, MS and expanded MS of rice, and absorption and PL spectra of HPLC fractions of undoped C-dots. See DOI: 10.1039/c4ra02170c |
| ‡ Exchange student on visit to Hong Kong Baptist University. |
| This journal is © The Royal Society of Chemistry 2014 |