3.1. Characterization of HES-SS-DOX@ICG NPs
HES-SS-DOX@ICG NPs were prepared using a facile but highly effective method based on the mutual interactions between DOX and ICG. A series of HES-SS-DOX@ICG NPs was prepared to screen out appropriate parameters for them. HES-SS-DOX@ICG NPs with a weight ratio of DOX to ICG at about 2.3 and an average size of around 170 nm were found to have the optimum properties against tumors, and, hence, they were used for all NP-involved experiments in this study.
Photographs in
Figure S1B provide visual evidence for the occurrence of interactions between free DOX and free ICG. In this study, the free DOX/ICG solution was prepared by dissolving DOX and ICG together in PBS with stirring. It was found that free DOX/ICG solution became somewhat flocculent after 6 h of stirring. Some floccus in the solution began to precipitate after about 12 h of stirring and most of the floccus were already precipitated to the bottom of the vial after stirring for 24 h (see white arrows in
Figure S1B). The change in color of the free DOX/ICG solution and the formation of dark brown precipitates confirm that ICG has been bound to DOX since both the free DOX solution and the free ICG solution with the designated concentration are completely transparent, and have their own colors (
Figure S1A). Some changes in colors were also observed when preparing the HES-SS-DOX@ICG solution. As shown in
Figure S1A, the freshly prepared HES-SS-DOX solution in PBS showed an aurantiacus color while the free ICG solution in PBS had a pale green color. After adding HES-SS-DOX conjugates and ICG into PBS at the formulated ratio and blending them, the color of the resulting HES-SS-DOX@ICG solution turned dark brown rapidly, and no precipitate was observed during the 24-h stirring process (
Figure S1C). The color change suggests that ICG molecules have been bound to HES-SS-DOX conjugates since the colors originally belonged to HES-SS-DOX conjugates and ICG have already disappeared, respectively. Considering the fact that HES-SS-DOX conjugates themselves are a kind of NPs [
9], the ICG-bound HES-SS-DOX conjugates should, thus, be present in the solution in the form of HES-SS-DOX@ICG NPs. The photographs in
Figure S1C exhibit that these HES-SS-DOX@ICG NPs were well dispersed in their solution without formation of any precipitate during the various stirring durations. The good dispersion of HES-SS-DOX@ICG NPs in these solutions could be ascribed to the contribution of their HES component. Since HES and the synthesized HES-SS-DOX conjugates are all fully water-soluble and the employed HES has its molecular weight of ca. 20 kDa, which is much higher than that of free DOX or free ICG, it can, thus, be envisioned that HES-SS-DOX conjugates would provide a large enough buoyant force to carry the bound ICG without inducing the formation of precipitates.
Previous investigations into the branched HES revealed that it had a notably higher ability to resist the α-amylase-mediated degradation as compared to linear HES [
24,
25], and, hence, in the present instance, the branched HES was selected as a starting material for the synthesis of HES-SS-DOX conjugates in order to endow HES-SS-DOX@ICG NPs with a prolonged circulation lifetime. Several studies have pointed out that the branched HES molecules and the resulting HES-SS-DOX conjugates in their hydrated state are in the rough shape of microspheres with the size of about 10 nm or somewhat larger [
9,
24,
25]. It can, thus, be conjectured that HES-SS-DOX@ICG NPs would have a similar size because ICG is a kind of small molecule and its content in HES-SS-DOX@ICG NPs is also low. This conjecture is unfortunately inconsistent with the actual observation. A typical TEM image for HES-SS-DOX@ICG NPs shows that they had their size range between about 100 and 200 nm (
Figure 1A), which is much larger than the size of HES-SS-DOX conjugates. This implies that these HES-SS-DOX@ICG NPs should be aggregates formed by a number of ICG-carried HES-SS-DOX conjugates.
It is know that ICG has highly conjugated electron configuration while showing an amphiphilic characteristic due to the presence of two polycyclic indole skeletons and two sulfate groups in its molecular structure [
23,
26]. A previous study reported that ICG was able to collaboratively assemble with epirubicin (EPI) to form ICG-EPI NPs via electrostatic, π–π stacking, and hydrophobic interactions. The resulting ICG-EPI NPs have their size of around 200 nm with EPI loading as high as ca. 92% [
23]. The results for ICG-EPI NPs suggest that (1) an ICG molecule can interact with several EPI molecules to form partners, and vice versa. The results also suggest that (2) the total binding force generated by different interactions between ICG molecules and EPI molecules can only bind a limited number of ICG and EPI molecules to form structurally stable aggregates, and the size of ICG-EPI NPs depends on the ratio of ICG to EPI. Taking into consideration the fact that DOX is extremely similar to EPI in structure, ICG molecules should also be able to interact with DOX molecules in the same way. In the present situation, ICG molecules are required to interact with HES-SS-DOX conjugates because DOX is already loaded onto HES. Since HES-SS-DOX conjugates are nearly spherical in shape [
9], some ICG molecules could be bound to the DOX molecules located inside HES-SS-DOX conjugates whereas others would be bound to the DOX molecules that reside in the superficial regions of HES-SS-DOX conjugates. As a result, only those ICG/DOX partners in the superficial regions of different HES-SS-DOX conjugates can further interact with each other and provide a collaborative force to bind a certain number of HES-SS-DOX conjugates together to aggregate into structurally stable HES-SS-DOX@ICG NPs, as observed in
Figure 1A.
The size of drug-loaded NPs is known to play a key role in regulating the in vivo performance of the NPs. It has been suggested that NPs with a size less than 200 nm are likely to accumulate in the tumor via the EPR effect, and large NPs such as those larger than 300 nm would be easily caught by RES in the liver and spleen [
1,
27,
28]. Therefore, the size of HES-SS-DOX@ICG NPs needs to be well modulated. In this study, besides the size of HES-SS-DOX@ICG NPs, the ratio of DOX to ICG is also an important parameter for their anti-cancer efficiency. The size and composition of HES-SS-DOX@ICG NPs were synchronously optimized by mainly altering the molar ratio of HES-SS-DOX conjugates and ICG. Since the absorption wavelength of HES-SS-DOX@ICG NPs partially overlaps with the detection wavelength of the bound ICG inside NPs, the size of HES-SS-DOX@ICG NPs was determined using their TEM images rather than the regularly used dynamic light scattering instrument. Based on TEM image analyses, the mean size of HES-SS-DOX@ICG NPs was measured as ca. 170 nm, which signifies that they are suitable for in vivo usage from the perspective of the size account. ζ potential of ICG, HES-SS-DOX, and HES-SS-DOX@ICG NPs was also measured, and data are depicted in
Figure 1B. It can be seen that ICG and HES-SS-DOX conjugates were negatively charged with ζ potential of around 1.6 and 11 mV and HES-SS-DOX@ICG NPs had their ζ potential of about 18 mV, which is significantly greater (
p < 0.05) than the sum of ζ potentials of ICG and HES-SS-DOX conjugates. This demonstrates that charges in the HES-SS-DOX@ICG NPs have been redistributed due to the collaborative interactions occurring between ICG and HES-SS-DOX conjugates.
The UV absorbance and fluorescence emission spectra of ICG and HES-SS-DOX@ICG NPs were detected and they are represented in
Figure 1C,D, respectively. Curves in
Figure 1C explicate that free ICG had a wide absorption band with the maximum intensity at about 777 nm.
With respect to HES-SS-DOX@ICG NPs, the band at ca. 483 nm was ascribed to their DOX component and the wide band with its shape that is somewhat similar to that for free ICG was moved to the higher wavelength interval, which is characterized by the maximum intensity at ca. 790 nm. In comparison to free ICG, the wavelength at the maximum intensity for HES-SS-DOX@ICG NPs was red-shifted by about 13 nm. In
Figure 1D, a pronounced difference in wavelength was also detected when the maximum fluorescence intensity for free ICG was compared with that for HES-SS-DOX@ICG NPs. On the basis of these results, it can be inferred that the collaborative force arisen from electrostatic, hydrophobic, and π–π stacking interactions between ICG molecules and HES-SS-DOX conjugates has driven them to organize into certain assemblies, which leads to significant wavelength shifts occurring for the ICG component in HES-SS-DOX@ICG NPs. The similar wavelength shifts for ICG have also been mentioned in some studies where ICG and DOX were used together for chemo/photothermal combination therapies, and our findings are basically consistent with the reported results [
23,
29,
30].
HES-SS-DOX@ICG NPs were already optimized to achieve high therapeutic efficiency and minimize the side effects of DOX, and the drug load of DOX and ICG in HES-SS-DOX@ICG NPs was formulated as 7.7% and 3.2%, respectively. Although a higher ICG amount could be loaded into HES-SS-DOX@ICG NPs, it was found that such formulated HES-SS-DOX@ICG NPs were able to fulfill the mission for the tumor eradication in vivo. Several major parameters for the optimal HES-SS-DOX@ICG NPs are summarized in
Table 1.
3.2. Stability Assessment
The physical stability of NPs is known to be closely associated with their performance [
27,
28]. HES-SS-DOX@ICG NP solutions in PBS were, thus, stored at ambient temperature for various durations up to seven days to test if any changes happened to them. Photographs in
Figure S2 exhibited that these solutions remained transparent without changes in their colors or formation of any precipitates during seven-day storage, which verifies that they are stable in PBS.
ICG has been used as imaging or photothermal agents for diagnostic and therapeutic purposes [
15,
16]. Despite its many applications, ICG usually shows poor stability in aqueous media and is prone to aggregate. The former could lead to short-lived ICG and the latter would cause the low efficiency of ICG. HES-SS-DOX@ICG NPs were tested to assess whether they have an ability to maintain the stability of the loaded ICG, and relevant results are presented in
Figure 2A. After two-day storage, the intensity of HES-SS-DOX@ICG NPs was remained at around 96% but the intensity of free ICG already dropped to 58% of its initial value. Thereafter, the UV absorbance intensity of free ICG progressively decreased until it reached approximately 34% at the end of two weeks. On the other hand, the absorbance intensity of HES-SS-DOX@ICG NPs decreased only slightly within two weeks and it remained as high as 92% on day 14. These results demonstrate that HES-SS-DOX@ICG NPs can effectively maintain the stability of the loaded ICG in aqueous medium. The protective effect of HES-SS-DOX@ICG NPs on the loaded ICG molecules can be attributed to the composition and structure of NPs themselves. As mentioned early, HES-SS-DOX@ICG NPs were composed of a number of ICG-bound HES-SS-DOX conjugates, and, hence, most ICG molecules were encapsulated inside the HES-SS-DOX@ICG NPs. Accordingly, in the HES-SS-DOX@ICG solution, most ICG molecules inside HES-SS-DOX@ICG NPs would not be directly exposed to the aqueous environment, which leads to their high stability.
3.3. Assessment of In Vitro Photothermal Effect
The photothermal conversion efficiency of HES-SS-DOX@ICG NPs was monitored to evaluate whether these NPs are able to preserve the deserved efficiency of the loaded ICG. In this study, the time and intensity of laser irradiation were set as 5 min and 0.75 W/cm
2, respectively, since several studies did for measuring the photo-thermal effect of ICG-involved agents.
Figure 2B presents temperature profiles for different samples that were exposed to the laser irradiation for 5 min. Three kinds of HES-SS-DOX@ICG solutions showed elevating temperatures and their maximum temperature (T
max), which corresponds to the equilibrium temperature between the ICG-induced heat production and the heat loss of solutions, reached about 40 °C, 52 °C, and 66 °C after being irradiated for around 150 s, respectively. Afterward, the temperatures matching with HES-SS-DOX@ICG solutions slightly dropped. In addition, it is also observed that, as the ICG amount in HES-SS-DOX@ICG solutions increased from 5 to 20 μg/mL, the temperature curve moved toward the high temperature region in an ICG-dose dependent manner. Similar temperature responsive patterns were also commonly observed in other ICG-involved photothermal therapeutic systems [
17,
20]. The reason for the small temperature drops after T
max could be that the ICG-induced heat production is slightly less than the heat loss caused by the environment because T
max for these HES-SS-DOX@ICG solutions is significantly higher than the ambient temperature. In the case of free ICG solution (10 μg/mL), it had a notably slower temperature rising rate during the irradiation when compared with its HES-SS-DOX@ICG 10 μg/mL partner, and its T
max reached about 44 °C after irradiation for ca. 5 min, which was significantly lower than that (49 °C) for its HES-SS-DOX@ICG 10 μg/mL partner. With regard to two control samples including the HES-SS-DOX solution and water, their temperature was almost equal to their initial temperature after 5 min of irradiation without measurable changes.
Figure 2C provides a group of images taken from different samples that were exposed to irradiation for 5 min. Visual differences in colors can be viewed from these samples. Results presented in
Figure 2A–C verify that HES-SS-DOX@ICG NPs can effectively preserve the stability and photothermal efficiency of the loaded ICG. Based on these results, all subsequent experiments involved in photothermal effects were conducted under the same irradiation conditions (5 min, 0.75 W/cm
2).
3.7. In Vivo Imaging and Bio-Distribution
ICG has an intrinsic fluorescence nature, and, hence, HES-SS-DOX@ICG NPs that were accumulated in the tumor and organs can be tracked without additional radio labeling or fluorescent labeling.
Figure 5A presents two sets of fluorescence images taken from the back of H22-tumor-bearing mice. In the case of free ICG group, the fluorescence signal first appeared in the tumor region after 1 h of ICG injection, and, after that, fluorescence intensity progressively decreased as time extended up to 24 h. With regard to the HES-SS-DOX@ICG NP group, their fluorescence intensity changed in a trend as similar as that for free ICG, but the magnitude of fluorescence intensity was notably higher than that for free ICG. More quantitative results for the fluorescence intensity detected from mice are presented in
Figure 5B. In the HES-SS-DOX@ICG NP group, the maximum fluorescence intensity appeared at one hour post-injection and it was approximately three times as much as that of free ICG. After the peak intensity, the fluorescence intensity in the HES-SS-DOX@ICG NP group decreased but remained much higher than that in the free ICG group until the end of the detection.
Figure 5A,B explicate that greatly enhanced accumulation of HES-SS-DOX@ICG NPs at the tumor site, which has occurred in comparison to free ICG. These results can be attributed to the highly hydrophilic surface properties and appropriate size of HES-SS-DOX@ICG NPs, which facilitates them to approach tumors via passive EPR effect, and results in their enhanced intra-tumoral accumulation. In contrast to HES-SS-DOX@ICG NPs, free ICG molecules could be quickly quenched or fast cleared from the body of mice due to their instability and self-aggregation features when exposed to the physiological environment. On the basis of results presented in
Figure 5A,B, it can be drawn that one hour post-injection is the optimal time point to implement laser irradiation on the tumor area of mice to achieve the high photothermal effect.
Figure 5C shows representative ex vivo images of major organs and tumors, and
Figure 5D presents the average fluorescence intensity matched with two groups of mice. The images indicate that fluorescence signals mainly appeared in live tumors. Signals detected from liver reveal that HES-SS-DOX@ICG NPs and ICG molecules were, respectively, detained by liver to a certain extent due to the RES-rich nature of liver. Bar graphs in
Figure 5D indicate that, at 24 h after injection, the average fluorescence intensity at tumors excised from the HES-SS-DOX@ICG NP group was almost twice that of free ICG group, which strongly supported that HES-SS-DOX@ICG NPs are able to protect ICG from degradation and clearance while effectively delivering both DOX and ICG toward tumors.
3.8. Assessment of In Vivo Temperature Profiles and Photo-Thermal Effects
Several formulations were tested on H22-tumor-bearing mice to assess temperature changes in the tumor area of mice that were administered with different formulations for 1 h and subsequent laser irradiation for 5 min starting at 1 h after injection. Relevant results are represented in
Figure 6A. In PBS, free ICG and free ICG + free DOX groups, the endpoint temperature in the tumor area of the treated mice was detected as around 45.6 °C, 47.5 °C, and 47.8 °C, respectively, which indicates that these three agents have a limited capability to induce heat generation [
15]. In contrast to the mentioned three agents, the temperature profile for HES-SS-DOX@ICG NPs elucidates that these NPs were capable of generating laser-triggered hyperthermia at the tumor area with the temperature reaching about 53 °C after 5 min of laser irradiation, and such a local temperature is sufficient to cause heat-induced cytotoxicity against cancer cells [
15,
22]. Such induced hyperthermia at the tumor sites can be attributed to the dual effects of HES-SS-DOX@ICG NPs. One is that the NPs tendentiously accumulate in tumors (
Figure 5) and another one is that these NPs can protect the loaded ICG molecules from degradation during their circulation in vivo.
To evaluate the photo-thermal effect of applied agents on tumors of the treated mice, the irradiated tumors were excised from the mice at one hour post-irradiation and sectioned into slices for histological analysis using H&E staining. Mice in PBS groups were used as a control. As seen in
Figure 6B, micrographs corresponding to free ICG and free ICG + free DOX groups exhibit that a certain number of cells in the tumors were already necrotic or apoptotic, which is characterized by the reduced cell number and irregularly shaped nuclei (indicated by a dark purple color). By comparing the area of the dark purple color among these micrographs, it can be estimated that the free ICG has certain cytotoxicity to cancer cells, which is similar to that resulted from free ICG in combination with free DOX. In contrast to free ICG or a combination of free ICG and free DOX, HES-SS-DOX@ICG NPs showed significantly higher cytotoxicity to cancer cells, as shown by the large purple-free area in the matched micrograph. As described in the experimental section, tumor-bearing mice in these groups were subjected to different agents for 1 h, and, subsequently, to laser irradiation on the tumor area for 5 min, and tumors were excised at one hour post-irradiation. These mean that tumors were removed from the treated mice just a little longer than two hours after the injection. During this period of time, it can be inferred that only a small amount of DOX could be accumulated in the tumor site when the DOX-involved formulations were applied. Even so, DOX can only exert a very limited effect on the cancer cells during such a short period of time because DOX needs a longer time to enter the nucleus and to take its actions. Accordingly, the observed impairments to cancer cells in
Figure 6B should be mainly assigned to the photo-thermal effect of applied agents. Among these agents, the significantly higher anti-cancer photo-thermal cytotoxicity of HES-SS-DOX@ICG NPs can be attributed to their enhanced intra-tumoral accumulation (see
Figure 5) and proactive effect on the loaded ICG molecules.
3.9. In Vivo Anti-Cancer Efficacy
H22-tumor-bearing mice were administered with different formulations to evaluate synergistic anti-tumor efficacy of applied agents, and results are elucidated in
Figure 7A–D. As shown in
Figure 7A, the tumor volume of mice in PBS, PBS + laser, and free ICG groups unremittingly increased as time advanced, which indicates that these treatments were ineffective. Chemotherapies alone basing on free DOX with or without laser irradiation, or HES-SS-DOX@ICG NPs without laser irradiation could partially inhibit the tumor growth, and treatments based on DOX with or without laser irradiation showed higher tumor growth inhibition than that corresponding to free ICG together with laser irradiation. Tumor volume versus time curves reveal that treatments associated with free DOX + free ICG, free DOX + free ICG + laser, and HES-SS-DOX@ICG NPs without laser irradiation had similar anti-tumor efficacy without significant differences among these groups. Significantly, HES-SS-DOX@ICG NPs together with laser irradiation had the highest tumor inhibition efficacy among all these groups, and all tumors in this group were fully eradicated during a 14-day treatment period within which only one injection and one single subsequent laser irradiation were performed, which was further shown by the excised tumors and the average tumor weight (
Figure 7B,C). The high anti-cancer efficacy detected from the group matching with HES-SS-DOX@ICG NPs + laser irradiation can be ascribed to the synergistic effects arisen from HES-SS-DOX@ICG NPs due to their several merits, including a high photo-thermal conversion rate (
Figure 2B and
Figure 6A), a redox-responsive and irradiation enhanced DOX release (
Figure 2D), and tendentiously intra-tumoral accumulation (
Figure 5A).
In
Figure 7D, weight loss was observed from four groups involving free DOX starting from around one day after the injection, which indicates toxic effects induced by free DOX. No significant weight loss was recorded for mice in six other groups during the treatment period. In particular, mice in the group corresponding to HES-SS-DOX@ICG NPs + laser irradiation had a body weight quite similar to that in the PBS group, which suggests that the toxic effects associated with free DOX can be significantly reduced given that HES-SS-DOX@ICG NPs rather than free DOX were utilized. Moreover, the treatment based on the employed HES-SS-DOX@ICG NPs is also relatively safe for combinational chemo-PTT therapy.
DOX is an anthracycline glycoside antibiotic with wide-spectrum anti-tumor activity against a range of malignancies [
32,
33,
34,
35,
36]. Despite its wide use, DOX can cause severe side effects [
32]. In particular, DOX-induced myocardial impairment could potentially lead to heart failure [
32,
35,
36]. In this regard, further investigations were conducted to find out whether any cardiac impairment occurs to mice that were treated with different agents. Major organs such as heart, liver, spleen, lung, and kidney were harvested at the end of treatments and sectioned into slices for histopathological analysis. Several sets of H/E staining micrographs are presented in
Figure S3. Micrographs matching with groups of free ICG and HES-SS-DOX@ICG NPs, no matter with or without laser irradiation, show that heart, liver, spleen, lung, and kidney of the treated mice had normal histological structures without visual pathological changes when comparing with the matched ones in the control group (PBS group). In DOX and DOX + ICG groups, micrographs for liver, spleen, lung, and kidney of the treated mice exhibited that these organs had normal histological structures regardless of whether laser irradiation is applied. However, the micrographs for heart showed pathological changes [
37,
38], as indicated by irregularly oriented arrangements of myocardial fibers and aggregated inflammatory cardiac muscle cells. Results presented in
Figure 7 and
Figure S3 demonstrated that presently developed HES-SS-DOX@ICG NPs have not resulted in impairments to the normal organs of the treated mice no matter whether they are used with laser irradiation.
The residual tumors harvested at the end of treatments were also sectioned into slices for histological analysis, and their H/E staining micrographs are presented in
Figure 8. In comparison to the control (PBS group), many cells in the tumors of mice that were treated with free ICG + laser were necrotic or apoptotic, which is indicated by the reduced cell number and the shrunken or broken nuclei (denoted by a dark purple color). The treatments involved in free DOX with or without laser irradiation had a similar efficacy against tumors, but they seemed to be somewhat more efficient than that in the free ICG + laser group in view of the increased purple-free area in the matched micrographs. In the absence of laser irradiation, the treatment based on free ICG + free DOX only had a limited efficiency against tumors. Together with laser irradiation, the efficiency of this treatment was significantly improved, as shown by the large purple-free area in the corresponding micrograph. Similarly, only with laser irradiation, HES-SS-DOX@ICG NPs would be able to fully eradicate cancer cells. The results presented in
Figure 8 were basically consistent with those elucidated in
Figure 7.