Comparison of RBE values of high- LET α-particles for the induction of DNA-DSBs, chromosome aberrations and cell reproductive death

<p>Abstract</p> <p>Background</p> <p>Various types of radiation effects in mammalian cells have been studied with the aim to predict the radiosensitivity of tumours and normal tissues, e.g. DNA double strand breaks (DSB), chromosome aberrations and cell reproductive inactivation. However, variation in correlations with clinical results has reduced general application. An additional type of information is required for the increasing application of high-LET radiation in cancer therapy: the Relative Biological Effectiveness (RBE) for effects in tumours and normal tissues. Relevant information on RBE values might be derived from studies on cells in culture.</p> <p>Methods</p> <p>To evaluate relationships between DNA-DSB, chromosome aberrations and the clinically most relevant effect of cell reproductive death, for ionizing radiations of different LET, dose-effect relationships were determined for the induction of these effects in cultured SW-1573 cells irradiated with gamma-rays from a Cs-137 source or with α-particles from an Am-241 source. RBE values were derived for these effects. Ionizing radiation induced foci (IRIF) of DNA repair related proteins, indicative of DSB, were assessed by counting gamma-H2AX foci. Chromosome aberration frequencies were determined by scoring fragments and translocations using premature chromosome condensation. Cell survival was measured by colony formation assay. Analysis of dose-effect relations was based on the linear-quadratic model.</p> <p>Results</p> <p>Our results show that, although both investigated radiation types induce similar numbers of IRIF per absorbed dose, only a small fraction of the DSB induced by the low-LET gamma-rays result in chromosome rearrangements and cell reproductive death, while this fraction is considerably enhanced for the high-LET alpha-radiation. Calculated RBE values derived for the linear components of dose-effect relations for gamma-H2AX foci, cell reproductive death, chromosome fragments and colour junctions are 1.0 ± 0.3, 14.7 ± 5.1, 15.3 ± 5.9 and 13.3 ± 6.0 respectively.</p> <p>Conclusions</p> <p>These results indicate that RBE values for IRIF (DNA-DSB) induction provide little valid information on other biologically-relevant end points in cells exposed to high-LET radiations. Furthermore, the RBE values for the induction of the two types of chromosome aberrations are similar to those established for cell reproductive death. This suggests that assays of these aberrations might yield relevant information on the biological effectiveness in high-LET radiotherapy.</p

Enhancement of radiation effectiveness by hyperthermia and incorporation of halogenated pyrimidines at low radiation doses as compared with high doses: implications for mechanisms

Application of the linear-quadratic (LQ) model for description of mammalian cell survival curves to evaluate radiosensitization in dependence on dose. Data on clonogenic assays concerning the combined effects of radiation with hyperthermia and halogenated-pyrimidines, were analyzed according to the LQ formula for cell survival: S(D)/S(0) = exp-(αD+βD(2)). Effects of these agents on the linear parameter α and the quadratic parameter β are compared to evaluate differences depending on the applied dose, and the possible relations to mechanisms of radiosensitization. The values of the linear parameter α, which determines the effectiveness at low doses, are for most cell lines and in most conditions more increased than the values of the parameter β which has a higher contribution at larger radiation doses. These results can be explained by the assumption that the probability of interaction of two DNA double-strand breaks (DSB) produced in close proximity by individual ionizing particles is more enhanced than interaction of DSB produced at larger distances by two separate particles. The observed differences between values of α and β imply that the radiation enhancement factors are larger at low doses mostly applied in clinical radiotherapy as compared with larger doses as mostly evaluated in experimental studie

Analysis of enhancement at small and large radiation doses for effectiveness of inactivation in cultured cells by combining two agents with radiation

To evaluate the enhancement effect of two combined radiation-sensitizing agents in mammalian cells at small doses as compared to large doses using the linear-quadratic (LQ) mathematical model. Data on clonogenic assays concerning the radio-enhancement effects of combined halogenated pyrimidines and hyperthermia or combined cisplatin and hyperthermia, as published in earlier reports, were analyzed according to the LQ-formula: S(D)/S(0) = exp-(αD + βD(2)). Effects of sensitizing agents on the linear parameter α and the quadratic parameter β are compared in order to evaluate differences depending on the applied dose, the possible relations to mechanisms of radiation sensitization and to derive suggestions for applications. The values of the linear parameter α, which determines the effectiveness at low doses, are for all cell lines and all conditions more increased than the values of the parameter β which has a higher contribution at larger radiation doses. The combination of hyperthermia with halogenated pyrimidines to radiation as well as the combination of hyperthermia and cisplatin to radiation significantly increases the value of the linear parameter α, as compared to radiation alone or radiation combined with a single agent. The radiation enhancement factors of the values of linear and quadratic parameters demonstrate that the sensitizing agents have a larger effect on the linear parameter which is dominant at low radiation doses as is used in fractionated-radiation treatment in the clinic. Moreover, the effect is even further increased when two radiation sensitizers are use

Quantifying the combined effect of radiation therapy and hyperthermia in terms of equivalent dose distributions

To develop a method to quantify the therapeutic effect of radiosensitization by hyperthermia; to this end, a numerical method was proposed to convert radiation therapy dose distributions with hyperthermia to equivalent dose distributions without hyperthermia. Clinical intensity modulated radiation therapy plans were created for 15 prostate cancer cases. To simulate a clinically relevant heterogeneous temperature distribution, hyperthermia treatment planning was performed for heating with the AMC-8 system. The temperature-dependent parameters α (Gy(-1)) and β (Gy(-2)) of the linear-quadratic model for prostate cancer were estimated from the literature. No thermal enhancement was assumed for normal tissue. The intensity modulated radiation therapy plans and temperature distributions were exported to our in-house-developed radiation therapy treatment planning system, APlan, and equivalent dose distributions without hyperthermia were calculated voxel by voxel using the linear-quadratic model. The planned average tumor temperatures T90, T50, and T10 in the planning target volume were 40.5°C, 41.6°C, and 42.4°C, respectively. The planned minimum, mean, and maximum radiation therapy doses were 62.9 Gy, 76.0 Gy, and 81.0 Gy, respectively. Adding hyperthermia yielded an equivalent dose distribution with an extended 95% isodose level. The equivalent minimum, mean, and maximum doses reflecting the radiosensitization by hyperthermia were 70.3 Gy, 86.3 Gy, and 93.6 Gy, respectively, for a linear increase of α with temperature. This can be considered similar to a dose escalation with a substantial increase in tumor control probability for high-risk prostate carcinoma. A model to quantify the effect of combined radiation therapy and hyperthermia in terms of equivalent dose distributions was presented. This model is particularly instructive to estimate the potential effects of interaction from different treatment modalitie

Induction of linear tracks of DNA double-strand breaks by alpha-particle irradiation of cells

Understanding how cells maintain genome integrity when challenged with DNA double-strand breaks (DSBs) is of major importance, particularly since the discovery of multiple links of DSBs with genome instability and cancer-predisposition disorders(1,2). Ionizing radiation is the agent of choice to produce DSBs in cells(3); however, targeting DSBs and monitoring changes in their position over time can be difficult. Here we describe a procedure for induction of easily recognizable linear arrays of DSBs in nuclei of adherent eukaryotic cells by exposing the cells to a particles from a small Americium source (Box 1). Each a particle traversing the cell nucleus induces a linear array of DSBs, typically 10-20 DSBs per 10 mu m track length(4). Because a particles cannot penetrate cell-culture plastic or coverslips, it is necessary to irradiate cells through a Mylar membrane. We describe setup and irradiation procedures for two types of experiments: immunodetection of DSB response proteins in fixed cells grown in Mylar-bottom culture dishes (Option A) and detection of fluorescently labeled DSB-response proteins in living cells irradiated through a Mylar membrane placed on top of the cells (Option B). Using immunodetection, recruitment of repair proteins to individual DSB sites as early as 30 s after irradiation can be detected. Furthermore, combined with fluorescence live-cell microscopy of fluorescently tagged DSB-response proteins, this technique allows spatiotemporal analysis of the DSB repair response in living cells. Although the procedures might seem a bit intimidating, in our experience, once the source and the setup are ready, it is easy to obtain results. Because the live-cell procedure requires more hands-on experience, we recommend starting with the fixed-cell applicatio

Relative biological effectiveness of high linear energy transfer alpha-particles for the induction of DNA-double-strand breaks, chromosome aberrations and reproductive cell death in SW-1573 lung tumour cells

Ionizing radiation-induced foci (IRIF) of DNA repair-related proteins accumulated at DNA double-strand break (DSB) sites have been suggested to be a powerful biodosimetric tool. However, the relationship between IRIF induction and biologically relevant endpoints, such as cell death and formation of chromosome rearrangements is less clear, especially for high linear energy transfer (LET) radiation. It is thus not sufficiently established whether IRIF are valid indicators of biological effectiveness of the various radiation types. This question is more significant in light of the recent advancements in light ion-beam and radionuclide therapy. Dose-effect relationships were determined for the induction of DNA-DSBs, chromosome aberrations and reproductive cell death in cultured SW-1573 cells irradiated with gamma-rays from a Cs-137 source or with alpha-particles from an Am-241 source. Values of relative biological effectiveness (RBE) of the high LET alpha-particles were derived for these effects. DNA-DSB were detected by scoring of gamma-H2AX foci, chromosome aberrations by fragments and translocations using premature chromosome condensation and cell survival by colony formation. Analysis of dose-effect relations was based on the linear-quadratic model. Except for the survival curves, for other effects no significant contribution was derived of the quadratic term in the range of doses up to 2 Gy of gamma-rays. Calculated RBE values derived for the linear component of dose-effect relations for gamma-H2AX foci, cell reproductive death, chromosome fragments and colour junctions are 1.0 +/- 0.3, 14.7 +/- 5.1, 15.3 +/- 5.9 and 13.3 +/- 6.0, respectively. RBE values calculated at a certain biological effect level are 1, 4, 13 and 13, respectively. The RBE values derived from the LQ model are preferred as they are based on clinically relevant doses. The results show that with low LET radiation only a small fraction of the numerous DNA-DSBs yield chromosome damage and reproductive cell death. It is concluded that many of the chromosomal aberrations detected by premature chromosome condensation do not cause reproductive cell death. Furthermore, RBE values for DNA-DSB detectable by gamma-H2AX foci shortly after irradiation, provide no information relevant to applications of high LET radiation in radiotherapy. The RBE values of chromosome aberrations assessed by premature chromosome condensation are close to the value for reproductive cell death. This suggests possible relevance to assess RBE values for radiotherapy with high LET ion

Dynamics of chromosomal aberrations, induction of apoptosis, BRCA2 degradation and sensitization to radiation by hyperthermia

Hyperthermia can transiently degrade BRCA2 and thereby inhibit the homologous recombination pathway. Induced DNA-double strand breaks (DSB) then have to be repaired via the error prone non-homologous end-joining pathway. In the present study, to investigate the role of hyperthermia in genotoxicity and radiosensitization, the induction of chromosomal aberrations was examined by premature chromosome condensation and fluorescence in situ hybridisation (PCC-FISH), and cell survival was determined by clonogenic assay shortly (0-1 h) and 24 h following exposure to hyperthermia in combination with ionizing radiation. Prior to exposure to 4 Gy γ-irradiation, confluent cultures of SW‑1573 (human lung carcinoma) and RKO (human colorectal carcinoma) cells were exposed to mild hyperthermia (1 h, 41˚C). At 1 h, the frequency of chromosomal translocations was higher following combined exposure than following exposure to irradiation alone. At 24 h, the number of translocations following combined exposure was lower than following exposure to irradiation only, and was also lower than at 1 h following combined exposure. These dynamics in translocation frequency can be explained by the hyperthermia-induced transient reduction of BRCA2 observed in both cell lines. In both cell lines exposed to radiation only, potentially lethal damage repair (PLDR) correlated with a decreased number of chromosomal fragments at 24 h compared to 1 h. With combined exposure, PLDR did not correlate with a decrease in fragments, as in the RKO cells at 24 h following combined exposure, the frequency of fragments remained at the level found after 1 h of exposure and was also significantly higher than that found following exposure to radiation alone. This was not observed in the SW‑1573 cells. Cell survival experiments demonstrated that exposure to hyperthermia radiosensitized the RKO cells, but not the SW‑1573 cells. This radiosensitization was at least partly due to the induction of apoptosis, which was only observed in the RKO cells and which may have been induced by BRCA2 degradation or different types of chromosomal aberrations. An important observation of this study is that the genotoxic effect of hyperthermia shortly after combined epxosure (to hyperthermia and radiation) is not observed at 24 h after treatmen