Yi
Pan‡
ac,
Jun
Yang‡
ab,
Yaning
Fang‡
a,
Junhui
Zheng
b,
Rong
Song
a and
Changqing
Yi
*ac
aKey Laboratory of Sensing Technology and Biomedical Instruments (Guangdong Province), School of Engineering, Sun Yat-Sen University, Guangzhou, China. E-mail: yichq@mail.sysu.edu.cn; Fax: +86-20-39342380; Tel: +86-20-39342380
bGuangdong General Hospital, Guangzhou, China
cResearch Institute of Sun Yat-Sen University in Shenzhen, Shenzhen, China
First published on 15th November 2016
In this study, an efficient and mild approach is reported for the facile synthesis of a carbon quantum dot (CQD)-based dual-modal fluorescence (FL)/magnetic resonance (MR) imaging probe by doping Gd(III) into CQDs through a one-pot pyrolysis process at low temperature. The as-prepared Gd-encapsulated CQDs (GCDs), which have an average diameter of ∼15 nm, are highly water-soluble. The GCDs are observed to have a high MR response with a longitudinal relaxation of 57.42 mM−1 s−1 and a strong fluorescence brightness with an absolute quantum yield of 40% while containing only 1.0% (w/w) of Gd3+ content. Stemming from the minimum Gd-doping and the inert carbon coating, GCDs exhibit excellent biocompatibility and blood compatibility. Dual-modality bioimaging applications of GCDs are successfully demonstrated by the use of HeLa cells and mice as models, revealing their great potential in fundamental biomedical research studies and even clinical fields such as fluorescence-guided surgery and dual-modal FL/MR imaging of blood vessels.
Various synthesis strategies have been reported to prepare CQD-based multimodal imaging probes.8–20 One approach is to integrate magnetic Fe3O4 nanoparticles (NPs) into fluorescent CQDs by hydrothermal decomposition of organic precursors employing Fe3O4 NPs as seeds8–10 or by depositing Fe3O4 NPs on graphene oxide.11 However, magnetic NP-integrated CQDs suffer from the heavy accumulation in the reticuloendothelial organs mainly caused by their relatively large sizes.16
It has been reported that the incorporation of Gd into solid matrices can cause the slowing of tumbling of the Gd complex, thus significantly increasing r1 relaxivity.12 Therefore, combining Gd(III) and fluorescent CQDs should be a more promising approach for the preparation of CQD-based multi-modal imaging probes.12–19 The Gd-encapsulated CQDs (GCDs) can be prepared by simple pyrolysis in air of gadopentetate monomeglumine (GdPM),13 or gadopentetic acid (Gd-DTPA),16 or a mixture of gadopentetic acid, Tris base and betaine hydrochloride.12 Though these one-pot calcination methods are simple and time-saving, the poor hydrophilicity of the as-prepared GCDs caused by carbonization makes further functionalization of the probes difficult. And due to their relatively large sizes, the as-prepared GCDs might suffer from the non-negligible accumulation in the reticuloendothelial organs after systemic injection.20 Compared with the calcination in air at high temperature, preparation of the GCDs in aqueous solution under mild conditions, for example, by the hydrothermal approach with and without microwave assistance, should be more controllable and easy-to-accomplish, and the as-prepared GCDs exhibit high water solubility and colloidal stability under physiological conditions.14,15,19 The strategy of step-by-step surface modification in aqueous solution under mild conditions has also been demonstrated for the successful preparation of the GCDs, where Gd3+ ions are simply chelated onto the outer surface of the DTPA or cyclic DTPA dianhydride functionalized CQDs.17,18 Though these step-by-step surface modification methods can be used to prepare water soluble GCDs with relatively small sizes and good MR response, they still suffer from complicated and time-consuming multistep synthesis. Although various strategies have been successfully demonstrated for the synthesis of CQD-based FL/MR dual-modal imaging probes, their practical applications in biological process monitoring or medical diagnosis are still limited by either the low MR response or the weak fluorescence brightness. Therefore, continuous research efforts should be exerted to explore more efficient approaches for the synthesis of CQD-based multimodal probes with enhanced imaging performance.
An ideal FL/MR dual-modal imaging probe for future clinical translation should possess strong fluorescence brightness and a high MR response while containing as little Gd3+ content as possible.18 Due to the importance of the fluorescence intensity for bioimaging with high sensitivity and resolution, significant efforts have been devoted to the investigation of synthesis routes for improving the quantum yield (QY) of CQDs.21–29 Although the exact mechanism is still an open question, the photoluminescence (PL) properties of CQDs, such as QY, FL lifetime, as well as PL emission wavelength, strongly depend on the quantum-confinement effect, structural defects induced by surface modification and element doping. In particular, due to its good controllability, doping plays an important role in tuning the PL properties of CQDs. It has been reported that the carboxyl groups of critic acid (CA) and the amines of ethylenediamine are beneficial for condensation polymerization and further carbonization, thus greatly improving the QY of CQDs to 80% (quinine sulfate with QY = 0.54 as standard) via N-doping.29
Based on these understandings, an efficient and mild approach is reported in this study for the facile synthesis of biocompatible GCDs with high longitudinal relaxation and strong fluorescence brightness while containing as little Gd3+ content as possible. As illustrated in Fig. 1, CA monohydrate, branched polyethylenimine (BPEI) with an extremely high density of ethylene diamine units and Gd-DTPA were chosen as carbon, nitrogen and gadolinium sources, respectively. And the dual-modality applications of as-prepared GCDs are demonstrated by the use of HeLa cells and mice as models. Experimental results revealed that the GCDs are water soluble, biocompatible, and cell-membrane permeable. More importantly, the GCDs prepared in this study are observed to have a significantly higher MR response than commercially available contrast agents while still exhibiting strong fluorescence brightness with significantly improved QY, suggesting their potential for practical applications in fundamental biomedical research studies and even clinical fields.
The Gd content in GCDs was measured by a quadrupole-based iCAP Qc ICP-MS (ThermoFisher Scientific, Bremen, Germany) using the standard mode. The determination was carried out by external calibration in the range from 20 to 2000 ng L−1. In brief, 1.0 mL of nitric acid (65%) and 0.1 mg of GCDs were added to a centrifuge tube, and the mixture was allowed to react for 0.5 h. Then 1 mL of rhodium solution was added as an internal standard and diluted to a volume of 1.0 L. The final concentration of the internal standard was 1 μg L−1. The isotopes 103Rh, 158Gd and 160Gd were monitored with a dwell time of 0.1 s each. The MR property of GCDs was evaluated by capturing the T1-weighted MR images of GCDs in aqueous solution with a clinical 1.5T MRI instrument, where water protons in ultrapure water were used as the blank. T1-weighted MR imaging of GCDs in aqueous solution containing different Gd3+ concentrations (0.006, 0.013, 0.019, 0.032, 0.064 and 0.095 mM) was carried out, followed by the calculation of T1 and T2 relaxation rates.
MTT assay was employed to evaluate the cytotoxicity of the as-prepared GCDs using HeLa cells (Cells Bank of the Chinese Academy of Science) which were incubated in H-DMEM supplemented with 10% FBS and 1% penicillin–streptomycin under the conditions of 5% CO2 at 37 °C. In brief, HeLa cells were seeded on a 96-well plate at an initial density of 5 × 103 cells per well and incubated for 24 h. After removing the culture medium, GCDs with concentrations ranging from 0 to 1.0 mg mL−1 were introduced and co-incubated with the HeLa cells for another 24 h. Six groups of concentration were examined and for each group the experiment was repeated three times. After incubation for 24 h, the cells were washed with PBS and then 100 μL of culture medium and 20 μL of MTT solution (dissolved in PBS, 5 mg mL−1) were added to each well, followed by incubation for another 4 h. All the incubation processes stated above were performed at 37 °C with 5% CO2. Finally, the supernatant was removed and 150 μL of DMSO was added to each well. The samples were shaken for 10 min before absorbance value measurement. The absorbance at 570 nm was measured on a microplate reader. The optical density of the control group which received no GCD treatment represented 100% growth of the HeLa cells.
A hemolysis assay was also carried out to evaluate the blood compatibility of GCDs.31,32 In brief, red blood cells were collected from human blood by centrifugation to remove the serum. Then, red blood cells were washed with PBS five times, followed by ten times dilution in PBS before usage. 0.1 mL of the diluted cell suspension was mixed with 1.5 mL of aqueous solution containing different concentrations of GCDs (0.65, 1.30, 1.94, 2.60 g L−1), and 1.5 mL of ultrapure water and PBS were used as positive and negative control, respectively. After mild shake and stew for 2 h at room temperature, the samples were centrifuged and the supernatants were collected for absorbance measurement which was performed on a UV-Vis spectrometer (DU730, Beckman) with a scanning range from 500 nm to 600 nm. Absorbance at 541 nm was specially recorded for the calculation of the hemolysis percentage using the following equation: Hemolysis (%) = (Abssample − Absnegativecontrol)/(Abspositivecontrol − Absnegative control) × 100%, where hemolysis for the positive control group and the negative control group were regarded as 100% and 0%, respectively.
MR imaging of HeLa cells was performed on a clinical 1.5T MRI instrument (Philip 1.5T Achieva), according to a previous study with some modification.16 Firstly, HeLa cells were cultured in 75 cm2 culture flasks. Upon reaching a confluence of 80%, 0.628 mg mL−1 GCDs and a culture medium without GCDs (as blank group) were added to two different culture flasks, respectively. After incubation for 24 h, the cells in both culture flasks were in turn washed with PBS, digested by trypsin, centrifuged and redispersed in PBS (pH = 7.4). Finally, the T1-weighted MR images of the HeLa cells were acquired using the following scanning parameters: TR/TE = 480/8.8 ms, 256 × 196 matrices, flip angle = 5°/26°, and slice thickness = 3 mm.
Fig. 2 (A) TEM image of GCDs. Inset: the histogram of GCD size distribution obtained from DLS measurements. (B) HRTEM image of GCDs. Inset: the HRTEM image of GCDs with lattice spacing. |
XPS and FTIR was performed to further characterize the structure and components of the as-prepared GCDs. XPS analysis revealed that the characteristic peaks correspond to Gd 4d (141 eV), C 1s (285 eV), N 1s (398 eV), O 1s (530 eV), and Gd 3d (1187 eV) (Fig. 3A), confirming that the as-prepared GCDs were composed of 58.52% C, 25.34% O, 15.3% N and 0.58% Gd (Table S2, ESI†), and elemental mapping revealed that Gd was distributed evenly within GCDs (Fig. S2, ESI†). The high-resolution Gd 4d XPS spectra exhibited Gd 4d5/2 and Gd 4d3/2 lines at 141.0 and 147.2 eV, respectively (Fig. 3B). In comparison to the corresponding elemental Gd 3d5/2 (1186.0 eV), a higher binding energy of 1187.5 eV was observed for Gd 3d5/2 in GCDs (Fig. 3C), possibly due to the different coordination environments.15,35 The presence of both Gd 4d and Gd 3d peaks reveals that Gd still existed in the form of Gd3+ in GCDs,12–16 suggesting that the chemical environment and Gd coordination were not significantly altered by the synthesis process. Maintaining the oxidation state of Gd3+ is quite important, because MR imaging depends on its half-filled f orbital with seven unpaired electrons and its symmetrical s ground state.
Fig. 3 (A) XPS survey spectra, (B) Gd 4d spectra, (C) Gd 3d spectra, (D) C 1s spectra, (E) N 1s spectra, and (F) O 1s spectra of GCDs. |
The deconvoluted XPS C 1s spectra exhibited a dominant peak centered at 284.5 eV which is attributed to C–C, further validating the presence of a graphitic sp2 carbon structure in GCDs (Fig. 3D).36 The stretching vibration band of C–H at 2981.8 cm−1 (νC–H) and the bending vibration band of C–H at 1398.3 cm−1 (δC–H) in FTIR spectra also confirmed the carbon framework of GCDs (Fig. S3, ESI†). Two peaks centered at 398.4 and 400.1 eV presented on the deconvoluted XPS N 1s spectra are respectively attributed to C–N and C–N–H, confirming the successful doping of N elements in GCDs (Fig. 3E). FTIR analysis revealed the presence of surface amino groups on GCDs, as evidenced by the presence of the obvious stretching vibration band of N–H at 3423.5 cm−1 and the bending vibration band of N–H at 1591.2 cm−1, and the percentage of free amines on the surface of GCDs was determined to be 2.6% (w/w) using Kaiser tests (Fig. S4, ESI†).37
FTIR analysis also revealed peaks at 3568.2, 1706.9 and 1010.7 cm−1 that are, respectively, the characteristic stretching vibration bands of O–H, CO, and C–O (Fig. S3, ESI†), indicating the presence of surface carboxyl groups which were either generated during the pyrolysis process and/or inherited from the DTPA precursors. This is also supported by the deconvoluted O 1s XPS spectra, finding a dominant peak centered at 530.1 eV and a shoulder peak centered at 531.3, eV which were attributed to C–O and CO, respectively (Fig. 3F). The surface carboxyl and amino groups endow GCDs with good colloidal stability and cell-membrane permeability.
GCDs are highly fluorescent, and can emit strong PL upon excitation with light of a wide range of wavelengths (curve c of Fig. 4A). Unexpectedly, different from conventional CQDs, GCDs prepared in this study exhibited a wavelength-independent emission, where the fluorescence intensity increased to the maximum then decreased while the emission peak showed no obvious change upon excitation with light with wavelengths from 290 nm to 420 nm. The strongest emission peaks of GCDs which reflect their dominant energy gap are around 445 nm at the maximum excitation wavelength of 354 nm. It is possible that the fluorescence origin sites of GCDs were altered by simultaneous doping of N and Gd elements, resulting in a uniform chemical feature and the state of those sp2 clusters contained on the surface of GCDs.39–41 It has been reported previously that the N atom is the electron-acceptor in the heteroatom doped CQDs, showing obvious charge transfer and thus high QY.28 Therefore, as expected, the absolute QY of GCDs with heavy N-element doping was determined to be 40% which was significantly higher than previous studies,12–19 indicating the extra-high PL efficiency. As shown in Fig. 4A, the wavelength of the absorption peak of GCDs is almost the same as the maximum excitation wavelength of GCDs, indicating that most of the absorption is transformed into fluorescence and thus also possibly contributes to its high QY. The PL lifetime of GCDs was determined to be 9.65 ns (Fig. S5, ESI†), also reflecting its excellent optical properties and thus endowing GCDs with the ability to be applied in FL bioimaging especially for future FL-guided surgery and immune-fluorescence histology.
Doping Gd3+ into GCDs renders them the MRI modality. The T1 enhanced contrast capability of GCDs was thus evaluated on a clinical 1.5T MR instrument. As shown in Fig. 4B, the brightness of grey-scaled T1-weighted MR images enhanced with the increase of Gd3+ concentration, confirming the concentration-dependent positive contrast enhancement. The excellent MR response was further demonstrated by the large slope of the r1 relaxivity curve (Fig. 4B), from which the r1 relaxivity of GCDs was calculated to be 57.42 mM−1 s−1, significantly higher than that of the commercially available Gd contrast agents such as DTPA analogues Gadovist® (4.34 mM−1 s−1),42 Magnevists® (3.2 mM−1 s−1)/Omniscans® (3.3 mM−1 s−1),43 and ProHance®(4.3 mM−1 s−1).44 It has been well-established that the r2/r1 ratio of MR contrast agents is an important parameter to determine their classification and estimate their efficiency. The contrast agents favor positive contrast enhancement when the r2/r1 value is close to 1.0, otherwise they are considered as negative contrast agents when the ratio of r2/r1 is larger than 1.5.20 Based on the relaxivites of GCDs, the ratio of r2/r1 was calculated to be 1.14, indicating that GCDs is a T1-contrast agent. Clinically, a T1-contrast agent with high relaxivity is much more desirable than a T2 agent.45
Taking the high toxicity of Gd3+ into account, an ideal Gd-based MRI contrast agent should contain a minimum amount of Gd while exhibiting as high r1 relaxivity as possible. As quantitated by ICP-MS using HNO3 digestion, there is only 1.0% (w/w) Gd in GCDs, significantly lower than previous reports.12–17 Though the relationship between the Gd content in nanostructured MR contrast probes and their longitudinal relaxivity is still an open question, the incorporation of Gd into solid matrices can cause the slowing of tumbling of the Gd complex and maximize its function in curtailing the longitudinal relaxation time of hydrogen protons, thus significantly increasing r1 relaxivity,12,46,47 and the high local concentration of Gd3+ caused by the high specific surface ratios of GCDs might also contribute to its high r1 relaxivity.48 It is worth noting that the r1 relaxivity could achieve such a high level with only little amount of Gd, indicating that GCDs synthesized in this study is a promising T1-weighted MRI contrast agent for medical translation.
Due to the intrinsic biocompatibility of CQDs and the negligible leakage of Gd3+, an outstanding biocompatibility is expected for GCDs. A typical MTT assay was carried out with HeLa cells to examine the comparative cell viability upon treatment with different concentrations of GCDs for 24 h. As shown in Fig. 5B, over 80% cell viability was observed even with the GCD concentration up to 1.0 mg mL−1 (equivalent Gd concentration is 0.06 mM), confirming the good biocompatibility of GCDs towards HeLa cells and emphasizing its potential application in bioimaging.
Because hemolysis in vivo can result in jaundice, anemia, and other pathological conditions, the hemolytic potential of GCDs is also evaluated.31,32 In this study, ultrapure water acted as a positive control while the PBS acted as a negative control. As shown in Fig. 5C, GCDs displayed the same phenomena and fitted similar absorbance curves as the negative control group among the concentration range from 0.65 g L−1 to 2.60 g L−1, validating their negligible hemolytic potential. All the above results confirm the excellent biocompatibility and blood compatibility of GCDs which guarantee its applicability in in vivo imaging.
In addition, the grey-scaled T1-weighted images of HeLa cells upon treatment with 0.628 mg mL−1 GCDs were captured on a clinical MRI instrument. As shown in Fig. 6E, compared to the blank group, significantly enhanced signals were observed in the cells upon treatment with GCDs, indicating the obvious positive contrast enhancement. Cross-validation between the FL and MR results confirmed that GCDs were successfully internalized by HeLa cells and the FL and MR efficiency of GCDs was maintained, demonstrating the great potential of GCDs as in vivo FL and MR dual-response imaging probes.
Perfusion imaging is a kind of functional MR imaging technique which can reveal the blood perfusion state and provide information towards hemodynamics. Thanks to the high r1 relaxivity of GCDs, the peak intensity in cardiac and aortic perfusion scan reached 3400 in the mice injected with GCDs (Fig. 7C and D), whereas the values generated by Gd-DTPA (Magnevists®) were only 650 and 1000 (Fig. 7G and H), respectively. The significantly enhanced MR response by GCDs confirmed the great potential of GCDs in DCE perfusion MR imaging, especially in MR angiography.
Footnotes |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c6tb02115h |
‡ These authors contributed equally to this work. |
This journal is © The Royal Society of Chemistry 2017 |