In the present study, first the optimal parameters such as incubation time of PS, concentration of PS and light doses were find out. The time a PS requires to be localized maximum in RD cancer cells is the optimum uptake time. Thus, accumulation of PS is executed once for low concentration and then for high concentration, as shown in Fig. 1–2 below (for 5 µM concentration and also for 50 µM in the RD cell line). Figure 1 demonstrates the incubated time duration of Rh-640 perchlorate for 5 µM. The extreme absorbance corresponds to the optimum uptake time of Rh-640 perchlorate. While the first 2 hours showed an ascending cellular uptake in which absorbance kept on increasing with time interval and at 180 minutes or 3 hours of incubation it indicated maximum absorbance. After that a continued descending pattern was observed while the time for incubation was increasing. At this stage PS started excreting out of cells, which evaluates the capability of cells to absorb PS for assessing the efficacy standards(Atif, Fakhar-e-Alam et al. 2010). From Fig. 2, it can be seen easily that there is the same uptake of Rh640 perchlorate by RD cells regardless a different concentration of 50 µM was chosen. At 3 hours both concentrations (5 µM and 50 µM) showed the optimum uptake time of Rh-640 perchlorate because at this time there is enough PS accretion to produce a toxic effect upon laser light irradiation(Robertson, Evans et al. 2009). Figure 3 show that two different incubated doses have maximum peaks at highest absorbance which reveals the optimum incubation time to be 3 hours. As Rhodamine123 class of derivatives are cationic molecules which concentrate in mitochondria by mitochondrial transmembrane potential (ΔΨ m). RD cells are carcinomas of soft tissues and Rhodamine is selectively toxic towards carcinoma cells. Higher accumulation of PS at 3 hours of time may be attributed to higher transmembrane potential that increases mitochondrial outer membrane permeability. This affect may result in release of cytochrome C that impacts the mitochondrial function and initiates apoptosis .The selective killing of RD cells with higher concentration and PS uptake may be correlated with this affect(Zhang and Zhong 1990; Waterhouse, Goldstein et al. 2001; Castano, Demidova et al. 2004; Don and Hogg 2004).
Figure 4 depicts various concentrations ranging from 5 µM to 100 µM were selected and their relative absorbance in RD cells was calculated. It was to investigate the cytotoxic effect of PS and the impact of increasing PS concentrations. This explains the damage caused by the photosensitizer Rh-640 perchlorate in RD cells without light irradiation.
Figure 5 illustrates that PS has a low dark cytotoxicity, as Rh-640 perchlorate demonstrates good viability at 5 µM concentration. Reason behind it might be the survival of cancer cells that is much significant at low doses, resulting in less damage to cancer cells. According to this data Rh-640 perchlorate is less dark cytotoxic. It demonstrates that PS without light irradiation causes slight cell death, with cell viability remaining at roughly 100%.
The optimized concentration is 100 µM. Rh-640 perchlorate remains nearly nontoxic to cells without light irradiation. For enough cell death of RD cells, light irradiation is required. It is worth noting that the cytotoxic impact of the utilized photosensitizer is also dependent on the kind of cell line. A PS accumulates in mitochondria, potentially inducing apoptosis via the mitochondrial route. Hence, cell survival decreases (Wilson, Olivo et al. 1997; Rousset, Vonarx et al. 1999; Oleinick, Morris et al. 2002; Wu and Xing 2012). More precisely, larger doses and longer uptakes of PS affect the viability(Powers, Pribil et al. 1986).
Figure 6 depicts varied light dose concentrations in J/cm2, with the bars representing percent viability values at light doses ranging from 2 to 15 J/cm2. This will allow us to determine how damaging the light dose (in the low dose range) is for the RD cell line, as well as how it will behave in the absence of a PS. The irradiation range is set between 2 J/cm2 and 15 J/cm2, with a high viability persistence of up to 95%. In this range, the viability results are fairly similar to previously published studies on phototoxicity of non-ALA treated Rhabdomyosarcoma cells(Khursid, Atif et al. 2010). The cell death at a high dose is the result of necrosis which increases by increasing further light and drug doses. Thus, light alone does not produce enough cell death. The use of PS is necessary to reduce cell viability. The increase in percentage viability might be accounted for enhanced cell division resulting from the accelerated mitochondrial activity on light irradiation (Firdous, Nawaz et al. 2012).
The above results demonstrate that light doses of 2 J/cm2 to 15 J/cm2 may be suitable for PDT corresponding to the viability nearly 100%. To treat RD cells only light is less phototoxic. This makes Rh-640 perchlorate, an essential PS to kill RD cells.
The bar chart in Fig. 7 is the therapeutic outcome of RD cancer cells when incubated with Rh-640 perchlorate. The laser doses of 2,5,15 J/cm2 are used. Different 3 light doses are chosen which are irradiated on seven different PS concentrations (0-100 µM). It also includes non-treated cells labeled as control.
The light dose of 2 J/cm2 was selected for the first treatment arm. The effect of this light dose is shown in Fig. 7. It demonstrates how much toxicity is produced using light dose of 2 J/cm2 by varying concentrations of PS from 5 µM to 100 µM. By increasing concentration while giving the same light dose increases the toxic effect. At 70 µM and 100 µM, the behavior is essentially same. When cells are exposed to 100 µM, their viability drops by 85% PS chemically conjugates with its target receptors that include a variety of cell surface receptors. Direct phototoxicity causes irreversible photo damage in some organelles and membranes in PDT(Kou, Dou et al. 2017).
The PDT effect at 5 J/cm2 is shown in Fig. 8. The experiment was repeated by keeping the concentrations of PS same but this time at 5 J/cm2. This also shows a gradual decrease in percentage viability. PS is inducing damage together with an applied light dose of 5 J/cm2. In the end at 100 µM, the viability is 80% that shows a 5% increase in toxicity.
The 3rd treatment section is at 15 J/cm2 with varying concentrations of PS. Its bar chart is shown in Fig. 9, which demonstrates that the efficacy of PDT increases by increasing the concentration of Rh-640 perchlorate at light dose of 15 J/cm2. This time 16% drop in viability (compared to the previous light dose) occurs at 100 µM concentration of Rh-640 perchlorate.
The comparative PDT effect at 2 J/cm2, 5 J/cm2, and 15 J/cm2 and at different concentrations is demonstrated in Fig. 10. By comparing different doses, we suggest that the best PDT outcome is at 15 J/cm2. Different concentrations of PS are used which shows that the viability of cells decreases with increasing concentration of light dose. The bars shown in Fig. 10 demonstrate the experimental values of viability; it also includes the control or non-treated cells. This is a relative comparison for analyzing the effect of PS and light dose to the RD cells. Therapeutic outcome at low doses of drug and light is not much effective in reducing cell viability. The dose of light at 15 J/cm2 and the concentration of PS at 100 µM produces enough toxicity. It's because of the high quantum yield of Rh 640 perchlorate at high concentrations, which causes cell damage due to the fast rate of singlet oxygen formation. Because haemoglobin and myoglobin absorb less than 600 nm and water over 1000 nm, the optical window is restricted within this range(Lovell, Liu et al. 2010). Poor phototoxicity and low yield of triplet state is observed by Rhodamine derivatives. To overcome this their macro cycle is combined with halogens like heavy metals that enhance the spin-orbit coupling, singlet oxygen quantum yield as well as, triplet lifetime up to 10-fold. From all other Rhodamine derivatives, Rh-640 perchlorate (nearly similar to Rhodamine 101) shows the highest quantum(Sharman, Allen et al. 1999; Zhang, Zhang et al. 2014). This effect is amplified in Rh 640 perchlorate, which is based on Xanthene and contains chlorine in its macrostructure, making it hazardous at light exposures (0–15 J/cm2). The vitality of cells diminishes with increasing quantities of light dosage and PS.
Figure 11 shows that, when compared to other light doses, the 100 µM concentration at 15 J/cm2 may prove to be more effective in the PDT of RD cell line. When RD cells are not treated with Rh-640 perchlorate, their cellular viability is found to be high. The viability of the cells decreases from 100–69% after treatment with PS concentration of 100 µM.