|Year : 2016 | Volume
| Issue : 7 | Page : 120-128
Carbon ions of different linear energy transfer (LET) values induce apoptosis & G2 cell cycle arrest in radio-resistant melanoma cells
ˇakula Jelena1, Korićanac Lela1, Keta Otilija1, Todorović Danijela2, AP Cirrone Giuseppe3, Romano Francesco3, Cuttone Giacomo3, Petrović Ivan1, Ristić-Fira Aleksandra1
1 Vinča Institute of Nuclear Sciences, University of Belgrade, Belgrade, Serbia
2 Medical Faculty, University of Kragujevac, Kragujevac, Serbia
3 National Institute for Nuclear Physics, Southern National Laboratory, via S. Sofia 62, Catania, Italy
|Date of Submission||18-Jun-2014|
|Date of Web Publication||6-Oct-2016|
Vinča Institute of Nuclear Sciences, University of Belgrade P.O. Box 522, 11001 Belgrade
Source of Support: None, Conflict of Interest: None
| Abstract|| |
Background & objectives: The main goal when treating malignancies with radiation is to deprive tumour cells of their reproductive potential. One approach is to induce tumour cell apoptosis. This study was conducted to evaluate the ability of carbon ions (  C) to induce apoptosis and cell cycle arrest in human HTB140 melanoma cells.
Methods: In this in vitro study, human melanoma HTB140 cells were irradiated with the 62 MeV/n carbon (  C) ion beam, having two different linear energy transfer (LET) values: 197 and 382 keV/μm. The dose range was 2 to 16 Gy. Cell viability was estimated by the sulforhodamine B assay seven days after irradiation. The cell cycle and apoptosis were evaluated 48 h after irradiation using flow cytometry. At the same time point, protein and gene expression of apoptotic regulators were estimated using the Western blot and q-PCR methods, respectively.
Results: Cell viability experiments indicated strong anti-tumour effects of  C ions. The analysis of cell cycle showed that  C ions blocked HTB140 cells in G2 phase and induced the dose dependent increase of apoptosis. The maximum value of 21.8 per cent was attained after irradiation with LET of 197 keV/μm at the dose level of 16 Gy. Pro-apoptotic effects of  C ions were confirmed by changes of key apoptotic molecules: the p53, Bax, Bcl-2, poly ADP ribose polymerase (PARP) as well as nuclear factor kappa B (NFκB). At the level of protein expression, the results indicated significant increases of p53, NFκB and Bax/Bcl-2 ratio and PARP cleavage. The Bax/Bcl-2 mRNA ratio was also increased, while no change was detected in the level of NFκB mRNA.
Interpretation & conclusions: The present results indicated that anti-tumour effects of  C ions in human melanoma HTB140 cells were accomplished through induction of the mitochondrial apoptotic pathway as well as G2 arrest.
Keywords: Apoptosis - carbon ions - cell cycle - LET - melanoma
|How to cite this article:|
Jelena ˇ, Lela K, Otilija K, Danijela T, Cirrone Giuseppe A P, Francesco R, Giacomo C, Ivan P, Aleksandra RF. Carbon ions of different linear energy transfer (LET) values induce apoptosis & G2 cell cycle arrest in radio-resistant melanoma cells. Indian J Med Res 2016;143, Suppl S1:120-8
|How to cite this URL:|
Jelena ˇ, Lela K, Otilija K, Danijela T, Cirrone Giuseppe A P, Francesco R, Giacomo C, Ivan P, Aleksandra RF. Carbon ions of different linear energy transfer (LET) values induce apoptosis & G2 cell cycle arrest in radio-resistant melanoma cells. Indian J Med Res [serial online] 2016 [cited 2021 Apr 22];143, Suppl S1:120-8. Available from: https://www.ijmr.org.in/text.asp?2016/143/7/120/191811
Metastatic melanoma is one of the most aggressive cancers resistant to most modalities of cancer therapy. Therefore, the development of a therapeutic modality for the treatment of this disease is of great interest  . Carbon (  C) ions efficiently eliminate radio-resistant tumours  and have a higher dose effect on malignant tumours compared to conventional radiotherapy  . Accelerated charged particles, including  C ions, lose their energy through interactions with atoms along their path in irradiated tissue. These release a large amount of energy at the end of their range, therefore, forming the Bragg peak  . The energy loss per unit of length along the particle track, i.e. linear energy transfer (LET) is at the origin of induced biological effects. For  C ions, the LET values of about 200 keV/μm produce the largest biological effectiveness  .
Several oncogenes and tumour suppressor genes play a pivotal role in modulating response of tumour cells to radiation. The product of the p53 tumour suppressor gene regulates genomic stability and cellular response to DNA damage, but can also affect the sensitivity of tumour cells to radiation-induced apoptosis  . Wild-type p53 protein appeared to be a positive regulator of Bax (Bcl-2 associated X protein) expression. In addition, p53 can transcriptionally downregulate the expression of Bcl-2. Thus, p53 expression may influence the ratio of Bax/Bcl-2 and subsequently determine the induction of apoptosis  . Constitutive activation of nuclear factor kappa B (NFκB) induce overexpression of its downstream targets such as Bcl-xL (B-cell lymphoma-extra large), Bcl-2, vascular endothelial growth factor and interleukin-8, which may in turn mediate resistance to apoptosis induced by chemotherapy and radiation  .
Understanding the specific biological effects of high LET radiation on cancer cells could provide valuable data for the design of novel therapeutic applications in the treatment of cancers which are resistant to conventional clinical approaches  . Available data suggests that heavy ions induce DNA double-strand breaks (DSBs) and have inhibitory effects on malignant cells  . However, their clinical application is limited by the side effects caused by secondary particles in the "tail part" of the Bragg curve, thus increasing dose. In contrast to other heavy ions,  C ions are a promising tool for cancer radiotherapy and these are under investigation at various research and therapeutic centers. Radiation with  C ions is efficient in elimination of hypoxic tumours, since oxygen enhancement ratio is reduced for this type of radiation ,, .
This study was undertaken to estimate the effectiveness of  C ions of different LET values, on human HTB140 melanoma cells which are highly radio-resistant to conventional radiation and protons , . Since molecular mechanisms involved in  C ions induced apoptosis and cell cycle arrest are important for the elimination of tumour cells, these were also investigated.
| Material & Methods|| |
Irradiations with  C ions, viability assays and cell sample preparations for biological tests were carried out at National Institute for Nuclear Physics (INFN), Southern National Laboratory (LNS), Catania, Italy. Biological assays i.e., flow cytometry, Western blot analysis and real time-polymerase chain reaction (q-PCR) were performed in the Laboratory of Molecular Biology and Endocrinology, Vinθa Institute of Nuclear Sciences, University of Belgrade, Belgrade, Serbia.
Cell culture: Human HTB140 melanoma cells were obtained from the American Tissue Culture Collection (ATCC, Rockville, MD, USA) and cultured in the RPMI 1640 cell culture medium supplemented with 10 per cent foetal bovine serum and penicillin/streptomycin (all from Sigma-Aldrich Chemie GmbH, Steinheim, Germany), in a humidified atmosphere of 5 per cent CO 2 at 37 °C (Heraeus, Hanau, Germany).
Irradiation conditions: Exponentially growing HTB140 human melanoma cells were irradiated with the 62 MeV/n  C ion beams produced by the superconducting cyclotron at INFN - LNS. Two positions for irradiation within the Bragg curve were obtained by interposing Perspex plates (Polymethyl methacrylate - PMMA) of different thickness between the final collimator and the cell monolayer. The Perspex plates were 7.7 and 7.9 mm thick, giving relative doses of 49 and 87.5 per cent, respectively. Cells were irradiated with single dose levels of 2, 4, 8, 12 and 16 gray (Gy), with the average dose rate of 11.45 ± 0.31 Gy/min. Reference dosimetry was performed by the plane-parallel Markus ionization chamber (Advanced Markus Chamber, 0.02 cm 2 , Type 34045, PTW Freiberg, Germany), calibrated according to the International Atomic Energy Agency Technical Report Series (IAEA-TRS) code of practice , . For both positions the corresponding LET values were calculated by numerical simulations carried out with the GEANT4 (GeometryANd Tracking) code  and were 197 and 382 keV/μm, respectively. Cell monolayers were fixed vertically in a special device for irradiation, facing the horizontal beam.
Since the range of the 62 MeV/n  C ions is short, with a very narrow Bragg peak, the precision of positioning of the cell samples was checked by placing GafChromic HS films (ISP Technologies, Wayne, New Jersey, USA) before and after each irradiation. Irradiations were carried out in air at room temperature.
Cell viability assay: Sulforhodamine B (SRB) assay, based on the measurement of cellular protein content, is used for estimating cell viability  . Control and irradiated cells were seeded in 96-well plates at a density of 3000 cells per well. After an incubation period of seven days, cell monolayers were fixed with 10 per cent trichloroacetic acid and stained with 0.4 per cent SRB for 30 min. The excess dye is removed by washing with 1 per cent acetic acid. The protein-bound dye was dissolved in 10 mM Tris base solution for absorbance determination at 550 nm with a reference wavelength at 650 nm, using an ELISA plate reader (Wallac, Victor2 1420 Multilabel counter, PerkinElmer, Turku, Finland).
Flow cytometric analysis of cell cycle and apoptosis: For flow cytometric evaluation of the cell cycle status, control and irradiated cells were washed with phosphate-buffered saline (PBS), pH 7.4 and fixed overnight with cold 70 per cent ethanol, following incubation at 37 °C in PBS containing 500 μg/ml ribonuclease A (RNase A, Sigma-Aldrich Chemie GmbH) for 30 min and staining with 50 μg/ml propidium iodide (PI, Sigma-Aldrich Chemie GmbH). After incubation at room temperature for 30 min, cells were analyzed by flow cytometry (CyFlow, Partec, Mόnster, Germany) using FloMax software (Partec, Germany). For each sample, 10 000 cells were analyzed. Sub-G1 cells were scored as apoptotic population.
Western blot analysis: For the Western blot analysis cells were collected, washed with PBS, lysed in a cell lysis buffer and samples were prepared as previously described  . The membranes were incubated with primary antibodies against p53, Bcl-2, Bax, NFκB and PARP (poly ADP ribose polymerase) (Cell Signaling, Danvers, MA, USA) (1:1000 dilution) at 4°C overnight. The membranes were subjected to three 10 min washes with PBS with Tween 20 (PBST) and then incubated with horse radish peroxidase (HRP)-conjugated secondary antibody (HRP, Cell Signaling, 1:5000 dilution) at 4°C for 2 h. The proteins were visualized with an enhanced chemiluminescence (BM Chemiluminescence western blotting kit, Sigma-Aldrich Chemie GmbH) and exposed on to an X-ray film. The densitometry of the protein bands on the X-ray film was conducted using Image J Analysis PC software (National Institutes of Health, USA).
Real time polymerase chain reaction (q-PCR): Total RNA was isolated from the melanoma cells using Qiagen RNeasy Mini Kit (Qiagen Gmbh, Hilden, Germany) and quantified by measurement of the absorbance at 260 nm using NanoDrop 1000 (Thermo Scientific, Waltham, MA, USA). Purity was assessed from the 260/280 nm absorbance ratio. RNA was converted to cDNA using The RevertAid™ First strand cDNA Synthesis Kit (Fermentas, Vilnius, Lithuania) according to manufacturer's instructions. Real-time PCR was done using the The SYBR® Green PCR Master Mix (Applied Biosystems, Foster City, CA, USA), 50 ng of cDNA and forward and reverse primer in final concentration of 50 nM in a 10 μl reaction volume. The PCR was performed using the following conditions - two min step at 50 °C, 10 min step at 95 °C, followed by 40 cycles of 95 °C for 15 sec, and finally one min at 60 °C. Expression of the housekeeping ribosomal protein L19 (RPL19) gene was used for normalization of bax, bcl-2 and NFκB to enable cross-comparisons among the samples. The sequences for primers were as follows ,, : RPL19 - forward 5'TCGCCAATGCCAACTCTCGTC3'; reverse 5'AGCCCGGGAATGGACAGTCAC3'.
Bax - forward 5'GGGGACGAACTGGACAGTAA3'; reverse 5'CAGTTGAAGTTGCCGTCAGA3'.
Bcl-2 - forward 5'ATGTGTGTGGAGAGCGTCAA3'; reverse 5'ACAGTTCCACAAAGGCATCC3'.
NFκB - forward 5'AAACACTGTGAGGATGGGATCTG3'; reverse 5'CGAAGCCGACCACCATGT3'.
The relative changes in gene expression data were analyzed by the ΔΔCT method. The results were analyzed by Standard 7500 System (Applied Biosystem, USA).
Statistical analysis : The measurements were made in triplicate during each experiment, while each experiment was repeated three times, excluding the cell viability experiment which was performed in quadruplicate. The significance of the differences among original values of the experimental groups was assessed by the independent Student's t test. The mean value of control sample was arbitrarily calculated as 100 per cent, while mean values of irradiated samples were presented as percentage of control ± S.D. For cell cycle analysis number of cells in G1, S and G2 phases was presented as percentage of diploid cells. Number of diploid cells was arbitrarily calculated as 100 per cent.
| Results|| |
Since HTB140 cells are radio-resistant cells  , irradiation doses used in this study were adapted to the specificity of the cell line, thus being higher than those commonly used for the analysis of cell growth inhibition  and ranged from 2 to 16 Gy. In our previous study  , the effects of  C ions on HTB140 cells were analyzed for a broad spectrum of LET values (82-742 keV/μm), and the anti-tumour effect was highest after irradiation with about 200 keV/μm. Therefore, LET value of 197 keV/μm was chosen for the analysis of pro-apoptotic ability of carbon ions.
Effectiveness of carbon ions on inactivation of HTB140 melanoma cells: The efficiency of  C ions on HTB140 melanoma cells was examined by measuring cell viability seven days after irradiation. This time point was reported to be optimal for the evaluation of radiation effects on HTB140 cells  . Percentage of viable cells varied from 31.6 to 39 per cent and from 37.1 to 56.6 per cent compared to control for LET values of 197 and 382 keV/μm, respectively. These results indicated that the viability of HTB140 melanoma cells was significantly suppressed by  C ions ( P<0.001 for all irradiated samples), with more prominent inhibitory effects observed after irradiation with  C ions of 197 keV/μm ([Figure 1]).
|Figure 1. Viability of HTB140 cells obtained by Sulforhodamine B (SRB) assay, seven days after irradiation with12C ions of 197 and 382 keV/μm. Applied irradiation doses were from 2 to 16 Gy. Mean values obtained from four experiments are presented as percentage of control ± SD. Control value was set as 100 per cent. ***P <0.001 compared to control|
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Cell cycle distribution: In the control samples, 17 per cent of cells were detected in G2 phase. The increase in the percentage of G2 phase cells was obtained in irradiated samples ranging from 23 to 29 per cent for  C ions of 197 keV/μm and from 21.8 to 26.2 per cent for  C ions of 382 keV/μm ([Figure 2]). The results showed that the population of cells in G2 phase increased in all irradiated samples, with more pronounced changes detected after irradiation with the LET of 197 keV/μm.
|Figure 2. Cell cycle analysis of HTB140 cells estimated by flow cytometry, 48 h after irradiation with 12C ions of 197 and 382 keV/ìm. Applied irradiation doses were from 2 to 16 Gy. The percentage of cells in G1, S and G2 phases was obtained with the FloMax software. Mean values obtained from three experiments are presented. *P <0.05; G2 phase at different irradiation doses compared to control|
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Analysis of apoptotic signaling pathway induced by carbon ions: Nuclear staining with PI was performed to detect apoptosis in irradiated cells. The percentage of apoptotic cells and corresponding apoptotic indexes of HTB140 cells were evaluated 48 h after irradiation. Cells exposed to  C ions exhibited a significant number of cells in sub-G1 phase. Dose dependent increase in the level of apoptosis was observed in both irradiation positions. The highest values obtained after irradiation with 16 Gy were 21.8 ± 0.16 and 15.4 ± 0.04 for  C ions of 197 and 382 keV/μm, respectively [Table 1].
|Table 1. The percentage of sub-G1 HTB140 cells 48 h after irradiation evaluated using flow cytometry |
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A remarkable rise of p53 protein was detected after irradiation with  C ions of 197 keV/μm, reaching an increase of 327 to 737 per cent when compared to the control ( P<0.05 for 2 Gy; P<0.01 for 4 and 8 Gy; P<0.001 for 12 and 16 Gy) ([Figure 3]A). Irradiations with  C ions of 382 keV/μm induced the rise of p53 when doses higher than 4 Gy were applied. The obtained rise was from 137 to 295 per cent, when compared to the control level ( P<0.05 for 4 Gy; P<0.01 for 8, 12 and 16 Gy) ([Figure 3]B).
|Figure 3 . Level of the p53 protein 48 h after irradiation with 12C ions of 197 (A) and 382 keV/μm (B), obtained by Western blot. â - Actin was used as internal loading control. Irradiation doses were from 2 to 16 Gy. Mean values obtained from three experiments are presented as percentage of control ± SD. Control value was set as 100 per cent. *P <0.05, **<</i> 0.01, ***<0.001 compared to the control|
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[Figure 4]A shows significant dose dependent increase of Bax/Bcl-2 ratio, after irradiation with  C ions of 197 keV/μm. The increase was from 1.24 to 3.38 when compared to the control value which was set to 1 ( P<0.05 for 2 Gy; P<0.01 for 4 Gy; P<0.001 for 8-16 Gy). The ratio of Bax/Bcl-2 was increased after irradiation with  C ions of 382 keV/μm, for the doses of 8, 12 and 16 Gy and ranged from 1.65 to 2.52 ([Figure 4]B).
|Figure 4. Bax/Bcl-2 ratio 48 h after irradiation of HTB140 cells with 12C ions of 197 (A) and 382 keV/μm (B) , obtained by Western blot. Irradiation doses were from 2 to 16 Gy. â-Actin was used as internal loading control. Mean values, obtained from three experiments, of Bax/Bcl-2 ratios for irradiated samples were normalized to Bax/Bcl-2 ratio for control sample which was set as 1. P*<0.05, **<0.01, ***<0.001 compared to the control|
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Western blot experiments demonstrated an increase in the cleavage of PARP in all irradiated cells. Greater dose-dependent pattern of PARP cleavage was detected following the exposure to 382 keV/μm C ions. In our experiments, expression of the p65 subunit of NFκB was detected by Western blot. The obtained results indicated its increase in all irradiated samples. Irradiation with  C ions of 197 keV/μm led to an increase of 246-410 per cent (P<0.05 for 2-4 Gy; P<0.01 for 8-16 Gy), while  C ions of 382 keV/μm triggered the increase of 277-377 per cent compared to control (P<0.001) ([Figure 5]).
|Figure 5. Level of the nuclear factor kappa B (NFêB) protein 48 h after irradiation with 12C ions of 197 (A) and 382 keV/μm (B) , obtained by Western blot. â-Actin was used as internal loading control. Irradiation doses were from 2 to 16 Gy. Mean values obtained from three experiments are presented as percentage of control ± SD. Control value was set as 100 per cent. P*<0.05, **<0.01, ***<0.001 compared to the control|
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Except changes in expression on protein level, pro-apoptotic effects of  C ions were also verified on the specific gene expression level. The Bax/Bcl-2 mRNA ratio increased in all irradiated samples. The more pronounced changes were detected for higher doses of  C ions having LET of 197 keV/μm, reaching the value of 3.5 after irradiation with 16 Gy ([Figure 6]). Unlike the expression of the NFκB protein, expression of the NFκB mRNA did not show significant change after irradiation with  C ions having the two defined LET values ([Figure 7]).
|Figure 6. The ratio of Bax/Bcl-2 mRNA in HTB140 human melanoma cells 48 h after irradiation with 12C ions of 197 (A) and 382 keV/μm (B) . Irradiation doses were 2 - 16 Gy. RPL19 was used as internal control. Mean±SD values, obtained from three experiments, of Bax/Bcl-2 ratios for irradiated samples were normalized to Bax/Bcl-2 ratio for control sample which was set as 1. P*<0.05, **<0.01, ***<0.001 compared to the control|
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|Figure 7. Expression of NFêB mRNA in HTB140 human melanoma cells 48 h after irradiation with 12C ions of 197 (A) and 382 keV/μm (B) . Irradiation doses were 2 - 16 Gy. RPL19 was used as internal control. Mean ± SD values obtained from three experiments are presented as percentage of control value, which was set as 100 per cent. P*<0.05, **<0.01, ***<0.001 compared to the control|
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| Discussion|| |
Irradiation with protons and  C ions has been shown to be effective in eliminating tumours resistant to conventional radiotherapy  . Carbon ions show LET-dependent anti-tumour effects with the maximum being at 200 keV/μm 4 . Further increase of LET value does not lead to better anti-tumour effects  . This could be attributed to the overkill effect  .
In this study the effects of  C ions on cell viability were estimated seven days after irradiation. The data demonstrated that the  C ions significantly decreased viability of HTB140 melanoma cells. Decrease of viability could be caused by the induction of apoptosis or cell cycle arrest. For the majority of cells, especially radio-resistant ones, apoptosis occurs after one or more cell divisions. Usually the maximum number of apoptotic cells in in vitro conditions can be found 48 h after irradiation  .
Estimation of cell cycle distribution 48 h after irradiation of HTB140 indicated significant increase of G2 fraction as compared to non-irradiated cells. The results are consistent with other studies suggesting that the  C ion irradiated cells undergo prolonged G2 arrest. The longer G2 arrest may be attributed to the higher level of unrepaired DNA damages. These findings are in agreement with our previous results signifying induction of DSBs in HTB140 cells after exposure to  C ions  .
Carbon ions are known to have lethal effects on radio-resistant tumours and can induce apoptosis effectively regardless of p53 gene status. In addition, even in cells having the p53, exposure to high LET radiation results in cell death with a higher apoptotic ratio than in cells exposed to conventional radiation  . Results obtained in this study indicated that the induction of apoptosis was caused by the increase of the p53 tumour suppressor protein. Similar results were reported for radio-resistant glioblastoma cells irradiated by  C ions  . Anti-apoptotic factor Bcl-2, which negatively regulates apoptotic suicide machinery, is overexpressed in many cancers, including melanoma  . The impact of  C ions on Bcl- 2 overexpressing tumours is yet to be characterized. Western blot analysis demonstrated expression of Bcl- 2 by HTB140 cells. This might be one of the reasons of their high radio-resistance. To determine whether apoptosis related molecules contribute to the inhibitory effects of  C ions on HTB140 cells, the relative Bcl-2 and Bax expression levels were assessed. It was noted that  C ions increased the ratio of Bax and Bcl-2 in a dose and LET-dependent manner, both on protein and gene expression levels. These findings imply that the treatments used are able to induce apoptosis through shifting the Bax/Bcl-2 ratio in favour of apoptosis.
Apoptotic cell death is confirmed by the cleavage of PARP protein which is apparent in samples irradiated with higher doses of  C ions of 197 keV/μm. The detected percentage of apoptosis was in the range that was already reported for other radio-resistant cells irradiated with  C ions  . Except for its important role in apoptosis, PARP protein has an influence on NFκB activation. However, its role in this process is still controversial  . This transcription factor is upregulated in different cancers, including melanoma  , and is involved in the regulation of cell survival, apoptosis, angiogenesis and tumour cell invasion . Results obtained showed that NFêB transcription factor was expressed in HTB140 melanoma cells, with the increased expression level after irradiation with  C ions. This increase was dose and LET-dependent. However, the level of NFêB mRNA was not significantly changed after the same treatment. These findings are in agreement with the data that suggest the involvement of NFêB in the modulation of survival response of cells irradiated by  C ions  .
In summary, our results indicated significant anti-tumour effects of  C ions. The intensity of the analyzed effects was LET-dependent. Carbon ions having LET of 382 keV/μm did not induce a higher level of HTB140 cell growth inhibition than that of 197 keV/μm. The results also suggest that  C ions are promising for clinical use as an anti-cancer agent in treating radio-resistant tumours. However, molecular mechanisms involved in anti-tumour effects of these ions require further investigations.
| Acknowledgment|| |
The research leading to these results has received funding from the European Union Seventh Framework Programme FP7/2007- 2013 under Grant Agreement nΒ° 262010 - ENSAR. This work was also financially supported by the Ministry of Education, Science and Technological Development of Serbia (grants 173046 and 171019) and by Istituto Nazionale di Fisica Nucleare, Laboratori Nazionali del Sud, Italy.
Conflicts of Interest
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