Open Access Article
Li Yanga,
Aimiao Qin
*a,
Shuoping Chena,
Lei Liaoa,
Jiangke Qinb and
Kaiyou Zhanga
aKey Lab New Processing Technology for Nonferrous Metals & Materials, Ministry of Education, Guangxi Key Laboratory in Universities of Clean Metallurgy and Comprehensive Utilization for Non-ferrous Metals Resources, College of Materials Science & Engineering, Guilin University of Technology, Guilin, China. E-mail: 592491245@qq.com
bCollege of Chemistry and Pharmaceutical Science, Guangxi Normal University, Guilin, China
First published on 6th February 2018
Manganese ion (Mn2+) bonded nitrogen-doped graphene quantum dots (Mn(II)-NGQDs) with water solubility have been successfully synthesized by a simple, one-pot hydrothermal carbonization, using sodium citrate, glycine and manganese chloride as raw materials. The photoluminescence (PL) characteristics of Mn(II)-NGQDs were studied in detail. The resulting Mn(II)-NGQDs show a remarkably enhanced PL intensity and quantum yield (QY = 42.16%) compared with the product without Mn(II)-doped (named as NG, QY = 27.06%) and the product doped with other metal ions. The Mn(II)-NGQDs not only display low toxicity and high cellular uptake efficiency for fluorescence live cell imaging in biological evaluations but also exhibit a fast, highly selective and sensitive fluorescence quenching effect toward Hg2+ ions, with a detection limit of 3.4 × 10−8 mol L−1.
To date, a myriad of strategies for fabricating GQDs and graphene derivatives have been explored, such as pyrolysis synthesis,14 electrochemical synthesis,15 microwave-assisted solid-phase synthesis,16 hydrothermal synthesis17 and etc. Among these synthesis approaches, the carbonization of citric acid to prepare GQDs were considered to be one of promising method, since it can provide stable quantum dots with high yields.18,19 However, there are a series of problems for the direct carbonization of citric acid to face, such as complicated preparation process, harsh reaction conditions (such as strong acid/alkali using), accurate pH control and tedious postprocessing, which may lead to great restrictions for the further biomedical applications of QDs.20–22
To extend and improve the physical and chemical properties of GQDs, different modification methods have been applied, including surface functional groups modification,23 heteroatoms doping24,25 and formation of composite.26,27 For example, the ways of functionalization with surface groups and heteroatoms doping (such as N,S) may significantly transform the optical properties, quantum yields, chemical activities and electronics structure of GQDs,28,29 which would provide interesting luminescent properties, such as pH-dependent and excitation-dependent photoluminescence (PL) behaviors.30,31 The interaction of GQDs and metal ions or rare earth elements32,33 in solution may lead to the excitation/emission spectrum suppression, amplification or shift, which has been used for high selectivity and sensitivity detection of different ions and specificity molecules. Han et al. reported the magnetic-fluorescent imaging behavior based on manganese(II)-carbon dots, indicating that the metal bonded GQDs could be good fluorescent probes for bioimaging.34
In this paper, in order to explore the doping effect of different metal ions on the PL behaviors of GQDs, we chose sodium citrate and glycine as carbon and nitrogen sources respectively to synthesize multifunctional GQDs for the first time. By using the facile and efficient hydrothermal method, Mn2+ bonded nitrogen-doped graphene quantum dots (Mn(II)-NGQDs) with water solubility and multifunction were successfully produced, which is the first case of Mn(II)-NGQDs with Mn2+ enhanced fluorescence via a confinement effect between Mn2+ and functional groups. The Mn(II)-NGQDs exhibit a strong emission with high quantum yield, and display a highly selective and sensitive fluorescence quenching response to Hg2+. Moreover, the Mn(II)-NGQDs show low cytotoxicity and are suitable for fluorescence live cell imaging, which would be used for bio-imaging application.
000 rpm for 10 min to remove the deposit. Subsequently, the supernatant of Mn(II)-NGQDs solution (6.52 mg mL−1, ESI†) was dialyzed (molecular weight cut off, 1000 Da) against water for 48 h. Afterwards, the pure and solid-state Mn(II)-NGQDs white powder was obtained by vacuum freeze drying. Finally, the resulted Mn(II)-NGQDs were dispersed in water as a stock solution for further characterization and detection.
As a contrast, other common metal ions doped in NG (M-NG, M = Ag+, Al3+, Ba2+, Cr3+, Ca2+, Cd2+, Co2+, Cu2+, Fe2+, Fe3+, K+, Mg2+, Zn2+, Ni2+ or Pb2+), were also prepared using the similar method as Mn(II)-NGQDs, except for using different metal salts. In addition, the NG without metal doping was also prepared using the above experimental procedure.
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| Fig. 1 Schematic illustration of the synthesis of Mn(II)-NGQDs and cells imaging and Hg2+ detection. | ||
According to the XRD patterns of Mn(II)-NGQDs and NG (Fig. S2, ESI†), both of Mn(II)-NGQDs and NG exhibit two broad peaks centered at 9.2° (2θ) and 31.5° (2θ), corresponding to the (001) and (002) plane of graphitic nitride carbon,36,37 respectively. Compared with NG, the board peak at 31.5° (2θ) of Mn(II)-NGQDs is weakened obviously, indicating that in Mn(II)-NGQDs, the Mn2+ ions bond with the functional groups at the edge of NG, and may help to divide the large graphene sheets to small graphene domains.
Fig. 3a shows the FTIR spectra of Mn(II)-NGQDs and NG. The broad band at 3406 cm−1 corresponds to the stretching vibration of O–H and N–H. The strong and broad absorption band ranging from 1500 cm−1 to 1750 cm−1 with a center at 1580 cm−1 corresponded to the stretching vibrations of C
O and C
C in the aromatic ring. The bands at 1407 cm−1 and 830 cm−1 were assigned to the C–H bending and C–H stretching, respectively. The bands at 1258 cm−1 and 1078 cm−1 were attributed to the stretching vibrations of O–H and C–O–C, respectively.16,38,39 The small peaks at 1495 cm−1 and 1449 cm−1 corresponded to the NH3+ symmetric bending and C–N stretching vibration, respectively,39,40 which confirmed that nitrogen atoms have been successfully doped into the Mn(II)-NGQDs and NG. However, compared to NG, the C–O stretching vibration at 1078 cm−1 and NH3+ symmetric bending at 1495 cm−1 in Mn(II)-NGQDs disappear, indicating the existence of Mn2+ ions which have bonded to the NG. Moreover, the C–N stretching vibration of Mn(II)-NGQDs at 1449 cm−1 increases obviously, indicates that more nitrogen elements are preserved after the coordination effect of Mn2+ ions. Fig. 3b shows the Raman spectra of Mn(II)-NGQDs and NG. Both of Mn(II)-NGQDs and NG demonstrate a G band at 1645 cm−1, which relates to the vibration of the sp2 hybridization of graphitic carbon, and a D band at 1411 cm−1, which corresponds to the carbon lattice distortion. Compared to NG, Mn(II)-NGQDs show a more weak G band at 1645 cm−1 and a larger intensity ratio ID/IG increase from 1.29 to 2.23. Similar to the previous analysis,41–43 more structural defects, larger sp2 domains and smaller sp2 fragments are expected to be present in the Mn(II)-NGQDs. It is indicated that the bonding of Mn2+ can change the morphology of NG.
Furthermore, more information of the surface functional groups of Mn(II)-NGQDs and NG is further provided by XPS analysis (Fig. 4). The full-range spectra (Fig. 4a) show that, both of Mn(II)-NGQDs and NG contain C, N and O elements, and there is about 0.21% Mn (atomic fraction) in Mn(II)-NGQDs (Table S1, ESI†). Fig. 4b shows the C 1s XPS spectrum of the Mn(II)-NGQDs, which ranged from 280 to 292 eV. There are four adjacent peaks at 284.3 eV, 284.9 eV, 285.9 eV and 288.1 eV, which can be attributed to C–C/C
C, C–N, C–O and C
O bonding respectively.9 The N 1s spectrum of Mn(II)-NGQDs (Fig. 4d) exhibits three peaks at 398.9 eV, 399.2 eV and 400.9 eV, which are associated with C–N–C, N–(C)3 and N–H groups.11,39,40 The O 1s spectra of Mn(II)-NGQDs (see Fig. S3a, ESI†) and NG (see Fig. S3b, ESI†) show two peaks at 531.0 eV and 531.8 eV, which are associated with O–H and C–O–C groups, respectively.17 These spectra reveals that nitrogen element has successfully introduced into the Mn(II)-NGQDs and NG, and Mn(II)-NGQDs and NG has been functioned with some groups, such as –COOH, –OH and N–H group. The high resolution XPS spectrum of Mn 2p (Fig. 4b) shows a dominant peak at 641 eV assigned to Mn2+, indicating that the oxidation state of Mn on the surface of Mn(II)-NGQDs remains unchanged.34 Compared to the XPS spectrum of NG, the C 1s (Fig. 4e) and N 1s (Fig. 4f) spectra of Mn(II)-NGQDs in the peak shape are very similar to those of NG, which means that the introduction of Mn2+ ions cannot affect the carbon-based species. However, the atomic fraction (Table S1, ESI†) of N in Mn(II)-NGQDs (4.24%) is dramatically increasing compared with that of NG (2.2%), which may indicate that more N–H groups are preserved by the coordination effect of Mn2+ ion. The above results clearly reveal that Mn(II)-NGQDs and NG have been successfully produced.
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| Fig. 4 (a) XPS survey spectra of Mn(II)-NGQDs and NG; (b) C 1s and (c) N 1s region of Mn(II)-NGQDs, (d) C 1s and (e) N 1s region of NG; XPS high resolution of (f) Mn 2p. | ||
O groups.44 NG and other M–NG also display the two peaks which are similar to Mn(II)-NGQDs (Fig. S4, ESI†). As shown in Fig. 5a, the maximum excitation wavelength (370 nm) of Mn(II)-NGQDs gets a red shift than the UV-vis absorption band (340 nm), which can be ascribed to a distribution of the deferent surface energy traps of the carbon dots. The emission wavelength (λem = 443) of Mn(II)-NGQDs has no obvious change, compared with NG, but the fluorescence intensity of Mn(II)-NGQDs shows much stronger than that of NG. Fig. 5b shows that the emission spectra of Mn(II)-NGQDs have an excitation independent feature as the excitation wavelength gradually increases from 350–400 nm, with the maximum excitation wavelength and the maximum emission wavelength at 370 and 443 nm, respectively. The excitation independent phenomenon were also observed in previous reported,19,22 which may be due to the uniform size of Mn(II)-NGQDs and the unitary PL process of n–π* transition of the aromatic N in Mn(II)-NGQDs. Fig. 5c and d show the emission spectra and QY of Mn(II)-NGQDs with different concentrations of Mn2+ ion in reaction system under the excitation wavelength of 370 nm. The results indicate that the strongest synergistic effect with functional groups in reaction systems appears at the concentration Mn2+ ion of 2 × 10−3 mol L−1. The highest fluorescence QY of the obtained Mn(II)-NGQDs was determined to be 42.16%, which is much higher than that of NG (27.06%) and the previous report of N-GQDs (28.10%).39 This implied that the induced Mn2+ into NG significantly enhanced the fluorescence QY of NG.
To further confirm that the enhanced PL indeed arises from the Mn2+-assisted process, the control experiments were carried out by utilizing other Mn salts to replace manganese chloride, including manganese acetate, manganese sulfate and manganese nitrate, the results show that they can still enhance the fluorescence (Fig. S5a, ESI†), indicating that Mn2+ plays a key role in the enhanced PL from the Mn(II)-NGQDs. Furthermore, holding any other factors constant, citric acid was chosen to replace citric sodium as carbon precursor to prepare Mn(II)-NGQDs and NG for comparison. The comparison experiment results show that, choosing citric acid as precursor for high quality fluorescent quantum dots is unsuitable (Fig. S5b, ESI†). This indicates that citric sodium precursor also plays an important role in the improved PL of Mn(II)-NGQDs.
The as-synthesized Mn(II)-NGQDs also exhibit a good stability (Fig. S5c, ESI†). The PL spectra of the Mn(II)-NGQDs are almost the same with the fresh Mn(II)-NGQDs after 7 days of storage under ambient conditions. In addition, the synergy process of Mn2+ ion with functional groups would also be influenced by the reaction temperature (Fig. S5d, ESI†) and time, the optimum hydrothermal temperature and time were considered as 180 °C and 10 hours, respectively.
Fig. 5e and f show the PL spectra and QYs of various M–NG. All of the other M–NG display a weaker emission behavior compared to Mn(II)-NGQDs (Fig. 5e). Fig. 5f indicates that the QYs of seven kinds of M′–NG (M′ = Ni2+, Mg2+, Zn2+, Ba2+, Co2+, Ag+ and Ca2+) are similar to that of NG, while other seven kinds of M′′–NG (M′′ = Cu2+, Cr2+, Cd2+, Fe2+, Fe3+, Al3+ and Pb2+) have much lower QYs than that of NG.
Why only the introduction of Mn2+ ion into NG can obviously enhance their fluorescence? The mechanism is conjectured as the follows: in the hydrothermal reaction of glycine and sodium citrate, parts of carboxyl groups of sodium citrate may not be carbonized and retain on the surface of NG. These carboxyl groups have high reactivity for further condensation and carbonization, that is why a large amount of irregular graphene nanosheets and some agglomeration were observed in NG samples without Mn2+ doping. These irregular graphene nanosheets and large particles would reduce the fluorescent emission behavior. However, in the reaction process of Mn(II)-NGQDs, Mn2+ ions can bond with functional groups such as carboxyl groups on the surface of NG. These bonded Mn2+ ions not only make NG lose reactivity for further condensation and carbonization, but also prevent the grain growth and agglomeration of the particles of NG. Therefore, the Mn(II)-NGQDs show well dispersed QDs with uniform size and shape, and exhibit a high QY than that of NG. It is notable that, compared to Mn2+, other metal ions (such as Fe2+, Co2+, Ni2+, Mg2+, Zn2+, Ba2+, Ag+ and Ca2+) do not display such confinement effect to control the shape and grain growth of NG. TEM images of NG doping with other metal ions display similar morphology to pure NG, some large irregular sheets and small QDs can be observed (Fig. S6, ESI†). All of these M–NG display weaker fluorescent emission than Mn(II)-NGQDs. This confirms our conjecture and indicates that Mn2+ plays a key role in the synthesis of Mn(II)-NGQDs with enhanced fluorescent properties.
To discuss the sensitivity of Mn(II)-NGQDs as fluorescent probe for Hg2+ detection, the emission spectra of Mn(II)-NGQDs (λex = 370 nm) in the presence of different concentrations of Hg2+ ion (in the range of 0 to 5.0 × 10−6 mol L−1) were recorded and shown in Fig. 6b. A gradually decrease emission intensity at 443 nm is observed with the increase concentration of Hg2+ ion, implying that the fluorescence of Mn(II)-NGQDs solution is sensitive to Hg2+. As shown in Fig. 6c, the quenching efficiency (F/F0) displays a good linear response to the concentration of Hg2+ in the range of 0 to 3.5 × 10−6 mol L−1 (Fig. 6d). The linear equation is calculated to be F0/F = 0.9815–0.112 [Hg2+] (R2 = 0.9942), where F0 and F are emission intensities at 443 nm in the absence and presence of Hg2+ ion, respectively. Under this experiment condition, the limit of detection (LOD) for Hg2+ is calculated to be 3.4 × 10−8 mol L−1 by the 3δ/S (δ is the standard deviation of the lowest signal and S is the slope of linear calibration plot), which is much lower than most of other reported of common fluorescent probes (see Table S2, ESI†).46–50
The selectivity of the Mn(II)-NGQDs toward Hg2+ was also explored. Different metal ions such as Cu2+, Mn2+, Ag+, Pb2+, K+, Ba2+, Zn2+, Co2+, Hg2+, Al3+, Fe2+, Fe3+, Ni2+, Mg2+, Cd2+ and Hg2+ ions were added into the probe solution respectively, and the solution was analyzed after incubation of 10 min. The results in Fig. 6e manifest that these metal ions except Hg2+ ion have almost no interference on the fluorescence intensity of Mn(II)-NGQDs, the fluorescence intensity is apparently quenched only by Hg2+ ion. Therefore, the fluorescence sensor based on Mn(II)-NGQDs shows a higher selectivity for Hg2+ detection over the other metal ions. Similarly, the effects of non buffer (Milli-Q water) on the detection of Hg2+ were performed, the results show that Mn(II)-NGQDs also exhibit a highly selective and sensitive capability to Hg2+ in Milli-Q water (Fig. S7, ESI†), which is similar to that in the HMTA buffer.
To clarify whether the fluorescence quenching is a static or dynamic quenching process, the fluorescence decay characterization was conducted. Fig. S8 (ESI†) show the fluorescence decay profile of Mn(II)-NGQDs in the absence and presence of Hg2+ ions, respectively. The fluorescence decay profile of Mn(II)-NGQDs follows a single exponential fitting that indicated the presence of only one emitting species with lifetimes. However, the fluorescence decay profile of NG follows a tri-exponential fitting (Fig. S8, Table S3, ESI†), which indicates the presence of three emitting species with different lifetimes. It is possible due to the mixture of NG with nanosheets and QDs, which resulting a complex different lifetimes emission.51 The average lifetime of Mn(II)-NGQDs is 7.58 ns, which is shorter than that of NG (8.88 ns) and also support our point that the doping with Mn2+ can influence the morphology of NG. The lifetime data in Table S3 (ESI†) shows that the average lifetime of Mn(II)-NGQDs have not significantly change with the concentration increase of Hg2+ ions. It is indicated that the static quenching takes place during complex formation between Hg2+ ions and Mn(II)-NGQDs.52,53
The quenching effect can be attributed to the chelating reaction between the functional groups (such as carboxyl, hydroxyl and amino groups) on the surface of Mn(II)-NGQDs and Hg2+ ion, which can decelerate the radiative recombination of the exciton of n → π* transition through an effective electron transfer process, leading to the fluorescent quenching.54 In order to further understand the binding between Mn(II)-NGQDs and Hg2+, the UV absorption spectra of Mn(II)-NGQDs without Hg2+ and in the presence of Hg2+ (4.0 × 10−6 mol L−1) were recorded (Fig. 6f). The absorption peaks at 340 nm (due to the n → π* transition) for Mn(II)-NGQDs is remarkably declined in the presence of Hg2+, demonstrating the surface states of the quantum dots can be influenced by the binding of Mn(II)-NGQDs with Hg2+. This means that compared to other metal ions, Hg2+ ion shows a more powerful affinity and faster chelating toward the functional groups on the surface of the Mn(II)-NGQDs. In addition, the photoinduced electron transfer from conduction band to the state of Hg2+ would be located between the conduction band and valence band of Mn(II)-NGQDs, causing the fluorescence quenching. These results also indicate that the fluorescence quenching of Mn(II)-NGQDs by Hg2+ is a static quenching process.
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| Fig. 7 Cell viability of HepG2 cells after incubation with Mn(II)-NGQDs (0–300 μg mL−1) for 4 and 24 h, respectively. | ||
The utilization of Mn(II)-NGQDs in cellular imaging was also investigated by confocal laser scanning microscopy (CLSM) observation. As shown in Fig. 8, the obvious blue fluorescent signal can be observed in the cytoplasm of Raw264.7 (Fig. 8a1) and HepG2 cells (Fig. 8b1) incubated with Mn(II)-NGQDs at a concentration of 40 μg mL−1 for 3 h, indicating that the Mn(II)-NGQDs can be efficiently internalized by Raw264.7 and HepG2 cells and facilely enter into the cells for efficiency cell imaging.55,56 Moreover, both the Raw264.7 (Fig. 8a2) and HepG2 cells (Fig. 8b2) incubated with Mn(II)-NGQDs still kept their normal morphology and strongly adhered onto cell plates, revealing the good biocompatibility of Mn(II)-NGQDs. Thus, the Mn(II)-NGQDs can be served as an efficient and non-toxic and fluorescence bioimaging probe for various biomedical applications.
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| Fig. 8 CLSM images and bright field of Raw264.7 mouse macrophages (a1; a2) and HepG2 human liver cancer cells (b1; b2) incubated with Mn(II)-NGQDs (40 μg mL−1) for 3 h by excitation at 405 nm. | ||
Footnote |
| † Electronic supplementary information (ESI) available. See DOI: 10.1039/c7ra12133d |
| This journal is © The Royal Society of Chemistry 2018 |