Tian Liu†
a,
Xunwei Liu†c,
Yanjie Yaoa,
Juan Zhoub,
Jun Zhu*b,
Gang Sun*c and
Dannong He*ab
aSchool of Materials Science and Engineering, Shanghai Jiao Tong University, 800 Dongchuan Road, Shanghai 200240, P. R. China. E-mail: hdn_nercn@163.com
bNational Engineering Research Center for Nanotechnology, 28 East Jiang Chuan Road, Shanghai 200241, P. R. China. E-mail: yzjzhu@163.com
cDepartment of Medical Imaging, Jinan Military General Hospital, 25 Shifan Road, Jinan, Shandong 250031, P. R. China. E-mail: cjr.sungang@vip.163.com
First published on 18th February 2015
Multimodality molecular imaging has recently attracted much attention, because it can take advantage of individual imaging modalities by fusing together information from several molecular imaging techniques. Herein, we report a bifunctional contrast agent connecting MR and luminescent imaging. The bifunctional contrast agent, carbon@Gd-DTPA microspheres, arise from carbon microspheres, which are synthesized on a large scale through a Na3cit-assisted solution route. The T1-agent, Gd-DTPA, is then conjugated to the carbon microspheres through N-ethyl-N9-[3-(dimethylamino)propyl]carbodiimide hydrochloride/N-hydroxysuccinimide (EDC/NHS) coupling chemistry using surface absorbed Na3cit molecules as an intermedium. Meanwhile, a formation mechanism of the carbon microspheres has been suggested. Furthermore, we also prove that the application of the carbon@Gd-DTPA bifunctional contrast agents for MR imaging and luminescent imaging can be established successfully. These results show that the primary Na3cit molecules have been confirmed to serve triplicate roles as an oriented agent to produce carbon microspheres, an intermedium to conjugate Gd-DTPA and surface passivation agents to improve photoluminescence.
To these days, the carbon based nanostructure is one of the most important group IV nanomaterials due to the environmentally benign element and relatively low cytotoxicity, and their surfaces can be functionalized with hydroxyl, carboxyl, and amino groups to make them water-soluble and be easier to crosslink with biomolecules. These different structured or shaped carbon nanomaterials, such as nanotubes, nanowires, nanospheres, porous carbon and hollow carbon spheres, have been synthesized and extensively applied.10–15 Specially, the emergence of photoluminescent carbon-based nanomaterials has presented exciting opportunities in the search for benign “nanolanterns”, which are highly desired in bioimaging, disease detection, and drug delivery because they are superior in chemical inertness, biocompatibility and potentially toxicity compared to fluorescent semiconductor nanocrystals.16–19 Actually, carbon is hardly considered as a luminescent material, but carbon nanoparticles could be made to brightly luminesce.20 Furthermore, intense research has focused on the preparation of carbon nanostructures with high photoluminescent efficiency through changing their structure or composition.21–24 Among them, the surface passivation of carbon nanoparticles is proved an effective strategy for enhancing multicolor photoluminescence. For example, a series of surface passivation agents has been used to improve the fluorescence of the carbon nanoparticles and their mechanism has been suggested by Liu et al.23,24
In the present work, we are aiming to synthesize carbon materials, which are used as a luminescent imaging agent. Moreover, the commercially applied T1 agent, Gd-DTPA, is grafted into the carbon material to develop a bifunctional contrast agent connecting MR and luminescent imaging. To prepare such the contrast agent, we have designed carbon microspheres via a Na3cit-assisted solution route. Furthermore, the surface absorbed Na3cit molecules used as an intermedium to conjugate Gd-DTPA to the carbon nanospheres through N-ethyl-N9-[3-(dimethylamino)propyl]carbodiimide hydrochloride/N-hydroxysuccinimide (EDC/NHS) coupling chemistry. Finally, a microsphere-like bifunctional contrast agent, carbon@Gd-DTPA, is obtained. To our surprise, the primary Na3cit molecules have been confirmed to serve triplicate roles as an oriented agent to produce carbon microsphere, an intermedium to conjugate Gd-DTPA and surface passivation agents to improve photoluminescence. The bifunctional contrast agents obtained in this study are potential candidates for biomedical engineering in the future.
Other samples were prepared under the similar reaction condition by changing Na3cit mass. The detailed reaction condition and corresponding results are summarized in Table 1.
Sample | Na3cit mass | Morphology | ID/IG in Raman spectra |
---|---|---|---|
1 | 0 g | Nanospheres with 400 nm in diameter | — |
2 | 0.1 g | Microspheres with 1.5 μm in diameter | 0.660 |
3 | 0.3 g | Microspheres with 4 μm in diameter | 0.645 |
4 | 0.5 g | Microspheres with 5 μm in diameter | 0.618 |
5 | Sample 2 modified by Gd-DTPA | Microspheres about 1.5 μm with a smooth surface | — |
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Fig. 1 SEM images of obtained carbon architecture with different mass of Na3cit: (a) 0, (b) 0.1 g, (c) 0.3 g and (d) 0.5 g. |
To evaluate the effect of Na3cit on the structure of carbon microspheres, FT-IR spectra of the products were performed. As shown in Fig. 2, the bands at 1640 cm−1 of CC stretching vibrations are observed in the absence of Na3cit (curve 1), which implies that the carbonization process from cross-linking by intermolecular dehydration has been induced in our experiment. Moreover, the other obvious bands in the range of 1000–1200 cm−1 are also found, resulting from C–OH stretching vibrations and –OH bending vibrations. The results reveal the existence of resulted conjugate structures and residual hydroxy groups. However, when Na3cit is introduced (curves 2–4), the band at 3300 cm−1 of –OH stretching vibrations is strengthened and widen, but the bands at 1000–1200 cm−1 are weaken, which implies that the Na3cit molecules could take part in the carbonization process. As we known, there are three COO− groups and –OH group in the Na3cit molecules, so besides intramolecular dehydration of glucose, there is intermolecular dehydration between Na3cit and glucose molecules. Thus, the obtained carbon microspheres would be modified by Na3cit molecules, which leads to the decrease of residual hydroxy groups and the increase of residual carboxyl groups, and further the association of carboxyl groups and hydroxy groups by hydrogen bonding. Therefore, the band at 3300 cm−1 could be strengthened and widen due to the association of carboxyl groups and hydroxy group by hydrogen bond, but the bands at 1000–1200 cm−1 could be weaken due to the decrease of residual hydroxy groups. Meanwhile, the new bands at about 1700, 1600 and 1380 cm−1 appear and their intensities are gradually improved with the addition of Na3cit. Generally, the bands at about 1600 and 1400 cm−1 are attributed to characteristic asymmetric and symmetric stretching vibrations of COO−, respectively, and the band at about 1700 cm−1 is attributed to characteristic COOH stretching vibrations. Therefore, the occurrence of the band at 1600 and 1380 cm−1 further proves that the carbon microspheres have been modified by Na3cit. Moreover, their intensity is increased and the band at 1600 cm−1 is shifted to lower wavenumber, which shows the strong interaction of residual carboxyl groups with the increasing of Na3cit mass. Additionally, the occurrence of the band at 1700 cm−1 also proves the strong hydrogen bonding interaction between carboxyl groups and hydroxy groups. Therefore, the above results reveal that Na3cit has an important effect on the morphology and structure of the carbon microspheres.
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Fig. 2 FT-IR spectra of obtained carbon architecture with different mass of Na3cit: (1) 0, (2) 0.1 g, (3) 0.3 g and (4) 0.5 g. |
To further shed light on Na3cit effect, Raman spectra is presented. Fig. 3 shows the Raman spectra of the obtained products. There are no obvious peaks observed in the absence of Na3cit (curve 1). However, with the addition of Na3cit, the spectra exhibit two broad and strongly peaks at 1380 and 1580 cm−1, respectively, which shows that Na3cit is helpful for the crystalline graphite.25 Furthermore, the peak at 1380 cm−1 is usually associated with the vibrations of carbon atoms with dangling bonds for the in-plane terminations of disordered graphite, and it is labeled as the D-band. The peak at 1580 cm−1 (G-band) (corresponding to the E2g mode) is closely related to the vibration in all sp2 bonded carbon atoms in a 2-dimensional hexagonal lattice, such as in a graphene layer. The relative integrated intensity ratio of the D- and G-bands (ID/IG) reveals the graphite degree.26,27 Therefore, the Raman spectra of sample 2–4 are integrated and their values of ID/IG are calculated. As shown in Table 1, with the increasing the Na3cit mass, the values of ID/IG decrease, which further proves that Na3cit can contribute to the crystalline graphite of the carbon microspheres.
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Fig. 3 Raman spectra of obtained carbon architecture with different mass of Na3cit: (1) 0, (2) 0.1 g, (3) 0.3 g and (4) 0.5 g. |
Furthermore, these polysaccharides result in the hydrophilic surface of carbon spheres. And the increase of Na3cit mass could lead to more and more Na3cit molecules anchoring on the surface of carbon spheres. In other words, Na3cit molecules, used as a kind of passivation agent, take part in the formation of carbon spheres. Additionally, due to many carboxyl groups in Na3cit molecules, a few of hydrogen bonds on the hydrophilic surface of carbon spheres could be formed, which possibly enlarges the interspaces between polysaccharides chains. Therefore, the size of carbon spheres could be enhanced, and the carbon microspheres would be formed with increasing the Na3cit mass. Thus, we suggest that the Na3cit molecules play a role in the formation of carbon microspheres during the hydrothermal process as an oriented agent and a surface passivation agent.
To explore the effect of Na3cit on the surface passivation of the as-prepared carbon microspheres, we carried out a detailed photoluminescent (PL) study with different excitation wavelengths at 400 nm and 800 nm. Both in Fig. 5a and b, two PL peaks can be found without addition of Na3cit, such as 460 nm and 520 nm for 400 nm excitation (Fig. 5a) and 460 nm and 540 nm for 800 nm excitation (Fig. 5b), which is similar to the reported literature.28 Further observation finds that their intensity is gradually enhanced and their peaks are blue-shifted with the increasing of Na3cit, which shows that Na3cit has an important effect on PL properties of carbon spheres. According to the previous literature, the surface passivation processes and basic medium can contribute to the fluorescence enhancement and the increase in distribution of carbon nanoparticles emitting at shorter wavelengths, respectively.23,28 Therefore, it is reasonable that the pH increase with the Na3cit addition during hydrothermal process and the surface passivation effect of Na3cit are accomplished simultaneously when Na3cit is introduced into present reaction, which contributes to the fluorescence change.
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Fig. 5 The photoluminescence spectra of obtained carbon architecture with excitation wavelengths at (a) 400 nm and (b) 800 nm with different mass of Na3cit: (1) 0, (2) 0.1 g, (3) 0.3 g and (4) 0.5 g. |
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Fig. 6 (a) SEM image and (b) energy dispersive X-ray analysis of carbon@Gd-DTPA microspheres (sample 5). |
The quantum yield (QY) of obtained carbon@Gd-DTPA microspheres were measured according to a reported literature,30 in which the rhodamine 6G ethanol solutions (QY = 95%) was chose as a standard. As shown in Fig. 7, the QY of carbon microspheres before and after loading Gd-DTPA is measured and calculated to be 0.9% and 3.4%, respectively. Additionally, the inset shows that the room-temperature PL spectra of carbon microspheres before and after loading Gd-DTPA, which reveals that carbon microspheres are successfully modified by Gd-DTPA. Compared with the values of sample 2, the intensity of sample 5 is dramatically increased, which could attribute to larger conjugated system after being modified by Gd-DTPA.
The luminescence and magnetic resonance imaging of carbon@Gd-DTPA were further investigated to evaluate their multifunction. Confocal imaging of HCT 116 cells was performed to evaluate the fluorescent imaging of living cells. As shown in Fig. 8a, the confocal image reveals the result of HCT116 cells incubated with carbon@Gd-DTPA microspheres for 2 h. Blue and green fluorescence emissions are recorded as HCT116 cells and carbon@Gd-DTPA microspheres under the excitation of 488 nm lasers, respectively. The result reveals that the carbon@Gd-DTPA microspheres have excellent fluorescent imaging and are partly internalized into cells through endocytosis, which demonstrates this newly developed carbon@Gd-DTPA microspheres can be used in cell tracer applications. On the other hand, MRI signals of carbon@Gd-DTPA microspheres were measured in vitro. Different mass concentrations of carbon@Gd-DTPA microspheres in the centrifuge tubes, as well as pure water for the background signal, were measured for their T1 relaxation time by a 3T MR imaging scanner. T1-weighted maps in Fig. 8b show that the T1-weighted MR imaging signal intensity is continuously enhanced, resulting in brighter images with increasing the mass. The above results further reveal that carbon@Gd-DTPA is successfully fabricated with luminescence and MR properties.
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Fig. 8 (a) Confocal microscopy images of HCT 116 cells labeled with carbon@Gd-DTPA microspheres (sample 5), and (b) T1-weighted maps of various contents of carbon@Gd-DTPA microspheres (sample 5). |
To examine the feasibility of the using of the obtained carbon@Gd-DTPA microspheres in biomedical applications, their cytotoxicity was investigated. As shown in Fig. 9, the effect of varying concentrations (0.001–1 mg mL−1) of carbon@Gd-DTPA microspheres on the viability of L929 cells after exposure for 12 h is revealed. The cellular viabilities decrease with an increasing carbon@Gd-DTPA microspheres concentration, and about 70% cell viabilities are maintained even up to a relatively high dose of 1 mg mL−1. Therefore, the MTT assay results demonstrate that the obtained microspheres have a low cytotoxicity.
Footnote |
† These authors contributed equally to this work. |
This journal is © The Royal Society of Chemistry 2015 |