Yui Umeharaa,
Toki Kageyamaa,
Aoi Sona,
Yu Kimuraa,
Teruyuki Kondo*a and
Kazuhito Tanabe*b
aDepartment of Energy and Hydrocarbon Chemistry, Graduate School of Engineering, Kyoto University, Nishikyo-ku, Kyoto, 615-8510, Japan. E-mail: teruyuki@scl.kyoto-u.ac.jp; Fax: +81-75-383-2504; Tel: +81-75-383-7055
bDepartment of Chemistry and Biological Science, College of Science and Engineering, Aoyama Gakuin University, 5-10-1 Fuchinobe, Chuo-ku, Sagamihara, 252-5258, Japan. E-mail: tanabe.kazuhito@chem.aoyama.ac.jp; Fax: +81-42-759-6493; Tel: +81-42-759-6229
First published on 29th May 2019
Tumor-selective accumulation of gold nanorods (GNR) has been demonstrated for visualization of tumor hypoxia by photoacoustic imaging. We prepared GNRs with hypoxia-targeting nitroimidazole units (G-NI) on their surface. Biological experiments revealed that G-NI produced a strong photoacoustic signal in hypoxic tumor cells and tissues.
Recently, several technologies including oxygen-responsive electrodes,8,9 functional nanomaterials,10–12 fluorescence13–20 or phosphorescence emission21–32 and magnetic resonance imaging (MRI)33–36 have been adapted to visualize tumor hypoxia. Although these methods are useful for diagnosis, each has considerable limitations. For example, oxygen-responsive electrodes are invasive, and can measure the oxygen status in only a small region. Emission probes are highly sensitive to hypoxic cells, but the visualization of deep-seated pathological tissue is difficult because the emitted light does not permeate living tissues. MRI approaches require a large amount of probe to be administered to allow detection of oxygen levels. Thus, the development of a versatile detection system for tumor hypoxia remains a challenge.
In the past decade, photoacoustic imaging (PAI) has emerged as a promising modality for diagnosis.37–39 Compared with optical imaging using fluorescence or phosphorescence, photoacoustic signals can penetrate more deeply into tissue, while maintaining high spatial resolution in biomedical imaging. In addition, PAI offers faster imaging than MRI. For application of PAI to diagnosis, plasmonic nanostructures, such as gold nanoparticles including nanorods (GNRs), nanoshells, and nanostars have been proposed as molecular probes, because they show robust photoacoustic signals.40 These nanoparticles have been delivered to tumor tissue and modification of their surface allowed to visualize some receptors such as HER2, integrin, and EGFR by PAI.41,42
In light of these favorable features, we attempted to construct a molecular probe to detect tumor hypoxia by PAI using such gold nanoparticles. We employed GNRs as the PAI probe to target hypoxia because they can be excited by near-infrared light irradiation, which is preferred for bioimaging.40 To visualize hypoxic tissue by PAI, we modified the GNRs with 2-nitroimidazole derivatives (NIs), which have the property of accumulating in hypoxic cells.43–45 NIs are selectively reduced by nitroreductase under hypoxic conditions to form reactive products that bind irreversibly to cellular nucleophiles, resulting in their accumulation in hypoxic cells and regions. Therefore, we predicted that GNRs modified by NIs (G-NIs) would accumulate in hypoxic tumor tissue to show strong photoacoustic signals from this pathological tissue. Here, we report the preparation and characterization of G-NIs as PAI probe for tumor hypoxia.
The synthesis of G-NIs is summarized in Scheme 1. The GNRs were modified by polyethylene glycol that carried thiol and amino terminals (HS–PEG–NH2), using the high affinity of the gold surface for thiol groups to give G-PEGs. Coupling of the amino groups of G-PEGs with the 2-nitroimidazole derivative, NI-CO2H,31,32 gave desired G-NIs. To confirm the immobilization of the NI units on the surface of the GNRs, FT-IR measurements were performed (Fig. 1A). The strong band at around 1100 cm−1 was assigned to the C–O–C stretching vibration of the aliphatic ether associated with PEG units.46 It is striking that the band around 1650 cm−1 observed for G-NIs was attributed to the CO vibration46 of the amide group, indicating that the NI units were immobilized on the surface of the GNRs. We also characterized the G-NIs by transmission electron microscopy (TEM) and absorption spectra. The TEM images of the nanoparticles indicated that the longitudinal and transverse lengths of G-NIs were 13 ± 1 nm and 36 ± 2 nm, respectively, and that their aspect ratio was 2.8. Absorption spectra revealed that modification of the surface of GNRs by PEG and NI units had a negligible effect on the size and shape of GNRs. Furthermore, measurement of the zeta potential value of nanoparticles verified that the GNR surface was modified. GNRs showed a negative charge (−13.5 ± 0.5 mV), while the charge of G-PEGs became positive (+4.9 ± 0.4 mV) because of the displacement of the surface molecules by PEG molecules bearing terminal amino groups. In addition, surface modification of G-PEGs by NI units to form G-NIs resulted in a decrease of their charge to +0.26 ± 0.2 mV, indicating that terminal amino groups were consumed to form an amide bond with NI-CO2H. We also synthesized control nanoparticles bearing fluorescent ATTO-647 to give G-NI-Fs in a similar way (Scheme 1).
Scheme 1 Reagents and conditions: (a) HS–PEG–NH2 (MW 5000), quant. (b) EDC, DMAP, HOBt, NI-CO2H (c) EDC, DMAP, HOBt, NI-CO2H, ATTO 647N NHS. |
We next assessed the cytotoxic properties of G-NIs using the human lung carcinoma cell line A549. For the assessment of cytotoxicity, the cells were cultured for 24 h in the presence of various concentrations of G-NIs and then subjected to a cell viability assay (Fig. 2A). We confirmed that almost all of the cells had a high survival rate even in the presence of G-NIs up to 2.5 μM, indicating that G-NIs had low cytotoxicity in this concentration range. To evaluate the specific accumulation of G-NIs in hypoxic cells, we applied G-NI-Fs to the cellular imaging of A549 cells. The cells were pre-incubated under aerobic (20% O2) or hypoxic (0.3% O2) conditions for 24 h, followed by incubation with G-NI-Fs for 3 h. After washing, the cells were subjected to microscopy. As shown in Fig. 2B, there were significantly higher levels of G-NI-Fs fluorescence emission in the cells cultured under hypoxic conditions than in those cultured under aerobic conditions. Thus, G-NI-Fs was selectively retained in hypoxic cells.
Further assessment of accumulation of gold nanoparticles in A549 cells were conducted. The hypoxic cells were incubated in the presence of G-NI or G-PEG, and then the cell lysates were harvested for the measurement of ICP MS. The concentration of G-NI and G-PEG in hypoxic cells were estimated to be 1630 ± 427 and 111 ± 6 fmol per cell, respectively. The evidence that the amount of G-NI in aerobic cells was 120 ± 4 fmol per cell led to the conclusion that NI units on the nanoparticles are responsible for their accumulation in hypoxic cells. We next evaluated the effect of particle size on the cellular uptake. We newly synthesized small-sized gold nanorods with NI units (S-G-NI), the longitudinal and transverse lengths of which were 8 ± 3 nm and 20 ± 7 nm, respectively (Fig. S1†). As a control, we also synthesized small nanorods without NI units (S-G-PEG). The ICP MS measurements of cell lysate revealed that uptake of S-G-NI in hypoxic cells was highly efficient (ca. 16 pmol per cell), but S-G-PEG also accumulated in hypoxic cells with moderate efficiency (ca. 7.7 pmol per cell). Thus, the small G-NI had low selectivity toward hypoxic cells. In addition, recent report showed that gold nanoparticles with large size (ca. 120 nm) had low cellular uptake.47 In light of these properties, we presumed that the gold nanoparticles with size of ca. 40 nm is favorable for molecular imaging of hypoxic cells.
The intracellular localization of the nanoparticles was evaluated using G-NI-Fs and several tracking reagents to conduct multicolor imaging. We merged the images of G-NI-Fs fluorescence with that of cytoplasmic organelle-specific fluorescence molecules targeting lysosomes, mitochondria, and endoplasmic reticulum (ER) (Fig. S2†). We observed a merged yellow color for G-NI-Fs and fluorescent agents targeting lysosomes and ER, while the mitochondria-targeting fluorescent agent did not give any merged signal. Thus, nanoparticles seem to have efficient access to the lysosome and ER in the cytoplasm. We also evaluated TEM images of A549 cells that were incubated with G-NIs, and confirmed that G-NIs accumulated in the cell vacuoles (Fig. 2D).
Further attempts were made to visualize hypoxic tumor cells in mice using PAI. For the imaging of tumor tissue, we selected colon 26 cells and transplanted them into the lower thigh of nude mice, because these cells are widely used for the study of tumor hypoxia in vivo. After the tumor grew to 5 mm in size, G-NIs in saline (5 pmol) were administered intravenously. As shown in Fig. 3A, obvious photoacoustic signals were obtained from the tumor tissue 24 h after injection of G-NIs. Given that injection of the control G-PEGs, which did not have NI units, led to only ambiguous images, G-NIs accumulated in hypoxic tumor cells in mice due to the function of their NI units. In a separate experiment, we performed ex vivo imaging using G-NI-Fs, and confirmed robust emission from G-NI-Fs in tumor tissue as well as in liver and kidney (Fig. S3†). We next evaluated the effect of PEG units in G-NIs on the accelerated blood clearance (ABC) phenomenon.48 The amount of anti-PEG IgM was measured by ELISA after the injection of G-NIs, G-PEGs or GNRs to mice. Although slight amount of anti-PEG IgM in serum was produced after administration of G-NIs (Fig. 4), this level was much lower than that produced after G-PEGs administration. A clear image of tumor tissue was obtained even after the second injection of G-NIs (Fig. 4B), indicating that the effect of clearance of nanoparticles on PAI was negligible. Thus, it is reasonable to conclude that G-NIs possessed appropriate properties for visualization of hypoxic tumor tissue by PAI.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c9ra00951e |
This journal is © The Royal Society of Chemistry 2019 |