Cytotoxic activity and influence on acetylcholinesterase of series dinuclear platinum(II) complexes with aromatic nitrogen-containing heterocyclic bridging ligands: Insights in the mechanisms of action.

Herein, the stability, lipophilicity, in vitro cytotoxicity, and influence on acetylcholinesterase of five dinuclear platinum(II) complexes with the general formula [{Pt(en)Cl}2(µ-L)]2+ (L is a different aromatic nitrogen-containing heterocyclic bridging ligands pyrazine (pz, Pt1), pyridazine (pydz, Pt2), quinoxaline (qx, Pt3), phthalazine (phtz, Pt4) and quinazoline (qz, Pt5), while en is bidentate coordinated ethylenediamine) were evaluated. The most active analyzed platinum complexes induced time-dependent growth inhibition of A375, HeLa, PANC-1, and MRC-5 cells. The best efficiency was achieved on HeLa and PANC-1 cells for Pt1, Pt2, and Pt3 at the highest concentration, while Pt1 was significantly more potent than cisplatin at a lower concentration. Additionally, a lower effect on normal cells was observed compared to cisplatin, which may indicate potentially fewer side effects of these complexes. Selected complexes induce reactive oxygen species and apoptosis on tumor cell lines. The most potent reversible acetylcholinesterase (AChE) inhibitors were Pt2, Pt4, and Pt5. Pt1 showed similar inhibitory potential toward AChE as cisplatin, but a different type of inhibition, which could contribute to lower neurotoxicity. Docking studies revealed that Pt2 and Pt4 were bound to the active gorge above the catalytic triad. In contrast, the other complexes were bound to the edge of the active gorge without impeding the approach to the catalytic triad. According to this, Pt1 represents a promising compound with potent anticancer properties, high selectivity, and low neurotoxicity.

A radiobiological study of carbon ions of different linear energy transfer in resistant human malignant cell lines.

PURPOSE: Analysis of elimination of four human radioresistant malignant cell lines to mono-energetic and non mono-energetic incoming carbon ion beams, characterized by different linear energy transfer (LET) qualities is performed. Comparisons with protons from the middle of the therapeutic spread out Bragg peak (SOBP) and reference γ-rays are also included. MATERIALS AND METHODS: HTB140 cells were irradiated at five positions, with different LET, along the 62 MeV carbon pristine Bragg peak. To provide reliable reproducibility of irradiations at INFN-LNS, as the carbon Bragg peak is very narrow, precise positioning of samples for desired LET value is complicated. The peak was slightly widened using two ripple filters. After defining irradiation position and LET at the peak itself where cell killing is almost the highest, irradiation position with the same LET value was found within somewhat broadened peak. HTB140, MCF-7, HTB177 and CRL5876 cells were irradiated at the two described positions. Additionally, irradiations in the middle of 62 MeV proton SOBP and reference γ-rays were performed. Doses ranged from 0.5 to 16 Gy. Cell survival and corresponding radiobiological parameters were assessed seven days after irradiations. RESULTS: When moving irradiation position along the carbon Bragg curve, LET rises from 85 to 747 keV/µm, while surviving fraction at 2 Gy (SF2) for HTB140 cells, falls from 0.72 to 0.57 further rising to 0.73 on the distal fall-off part of the curve. Improved cell radiosensitivity is seen for the doses below 4 Gy. Relative biological effectiveness (RBE) increases from 4.56 to 7.69 and drops to 4.23. Almost the highest cell killing LET, being ∼200 keV/µm, is used to irradiate HTB140, MCF-7, HTB177 and CRL5876 cells within the pristine and slightly broadened Bragg peak. After irradiations with protons of the mid SOBP, carbon ions of the pristine and slightly widened Bragg peak RBE ranges for HTB140 cells from 2.08, 4.81 to 7.06, for MCF-7 from 1.70, 3.28 to 4.17, for HTB177 from 1.98, 4.18 to 5.08 and for CRL5876 from 1.33, 2.57 to 3.51. CONCLUSIONS: Significant elimination of HTB140 cells is observed along the carbon Bragg curve. The highest one is achieved by LET that is at the level of already reported. For the same LET, mono-energetic carbon ions provide higher cell elimination than the non mono-energetic. For all cell lines, both carbon ion beams, more the monoenergetic one, express stronger killing rate than protons and especially γ-rays.

Biological outcomes of γ-radiation induced DNA damages in breast and lung cancer cells pretreated with free radical scavengers.

PURPOSE: Investigation of effects on DNA of γ-irradiated human cancer cells pretreated with free radical scavengers is aimed to create reference data which would enable assessment of the relative efficiency of high linear energy transfer (LET) radiations used in hadron therapy, i.e. protons and carbon ions. MATERIALS AND METHODS: MCF-7 breast and HTB177 lung cancer cells are irradiated with γ-rays. To minimize indirect effects of irradiation, dimethyl sulfoxide (DMSO) or glycerol are applied as free radical scavengers. Biological response to irradiation is evaluated through clonogenic cell survival, immunocytochemical and cell cycle analysis, as well as expression of proteins involved in DNA damage response. RESULTS: Examined cell lines reveal similar level of radioresistance. Application of scavengers leads to the rise of cell survival and decreases the number of DNA double strand breaks in irradiated cells. Differences in cell cycle and protein expression between the two cell lines are probably caused by different DNA damage repair mechanisms that are activated. CONCLUSION: The obtained results show that DMSO and glycerol have good scavenging capacity, and may be used to minimize DNA damage induced by free radicals. Therefore, they will be used as the reference for comparison with high LET irradiations, as well as good experimental data suitable for validation of numerical simulations.

Comparison of human lung cancer cell radiosensitivity after irradiations with therapeutic protons and carbon ions.

The aim of this study was to investigate effects of irradiations with the therapeutic proton and carbon ion beams in two non-small cell lung cancers, CRL5876 adenocarcinoma and HTB177 large cell lung carcinoma. The DNA damage response dynamics, cell cycle regulation, and cell death pathway activation were followed. Viability of both cell lines was lower after carbon ions compared to the therapeutic proton irradiations. HTB177 cells showed higher recovery than CRL5876 cells seven days following the treatments, but the survival rates of both cell lines were lower after exposure to carbon ions with respect to therapeutic protons. When analyzing cell cycle distribution of both CRL5876 and HTB177 cells, it was noticed that therapeutic protons predominantly induced G1 arrest, while the cells after carbon ions were arrested in G2/M phase. The results illustrated that differences in the levels of phosphorylated H2AX, a double-strand break marker, exist after therapeutic proton and carbon ion irradiations. We also observed dose- and time-dependent increase in the p53 and p21 levels after applied irradiations. Carbon ions caused larger increase in the quantity of p53 and p21 compared to therapeutic protons. These results suggested that various repair mechanisms were induced in the treated cells. Considering the fact that we have not observed any distinct change in the Bax/Bcl-2 ratio following irradiations, it seemed that different types of cell death were involved in the response to the two types of irradiations that were applied.