- Open Access
DNA double-strand break induction in Ku80-deficient CHO cells following Boron Neutron Capture Reaction
© Kinashi et al; licensee BioMed Central Ltd. 2011
- Received: 25 April 2011
- Accepted: 5 September 2011
- Published: 5 September 2011
Boron neutron capture reaction (BNCR) is based on irradiation of tumors after accumulation of boron compound. 10B captures neutrons and produces an alpha (4He) particle and a recoiled lithium nucleus (7Li). These particles have the characteristics of high linear energy transfer (LET) radiation and have marked biological effects. The purpose of this study is to verify that BNCR will increase cell killing and slow disappearance of repair protein-related foci to a greater extent in DNA repair-deficient cells than in wild-type cells.
Chinese hamster ovary (CHO-K1) cells and a DNA double-strand break (DSB) repair deficient mutant derivative, xrs-5 (Ku80 deficient CHO mutant cells), were irradiated by thermal neutrons. The quantity of DNA-DSBs following BNCR was evaluated by measuring the phosphorylation of histone protein H2AX (gamma-H2AX) and 53BP1 foci using immunofluorescence intensity.
Two hours after neutron irradiation, the number of gamma-H2AX and 53BP1 foci in the CHO-K1 cells was decreased to 36.5-42.8% of the levels seen 30 min after irradiation. In contrast, two hours after irradiation, foci levels in the xrs-5 cells were 58.4-69.5% of those observed 30 min after irradiation. The number of gamma-H2AX foci in xrs-5 cells at 60-120 min after BNCT correlated with the cell killing effect of BNCR. However, in CHO-K1 cells, the RBE (relative biological effectiveness) estimated by the number of foci following BNCR was increased depending on the repair time and was not always correlated with the RBE of cytotoxicity.
Mutant xrs-5 cells show extreme sensitivity to ionizing radiation, because xrs-5 cells lack functional Ku-protein. Our results suggest that the DNA-DSBs induced by BNCR were not well repaired in the Ku80 deficient cells. The RBE following BNCR of radio-sensitive mutant cells was not increased but was lower than that of radio-resistant cells. These results suggest that gamma-ray resistant cells have an advantage over gamma-ray sensitive cells in BNCR.
Kyoto University Research Reactor Institute (KURRI) has been investigating BNCT since 1990. BNCT has been utilized in the treatments of malignant glioma, malignant menigioma, malignant melanoma, Paget's disease, recurrent head and neck cancers, and lung tumors.
The principle underlying the Boron Neutron Capture Reaction (BNCR) is that tumor cells containing 10B can be destroyed efficiently by the 10B(n,α)7Li fission reaction through the delivery of effective thermal neutron doses at the target depth. During this reaction, an alpha particle and a recoiling 7Li ion with an average total kinetic energy of 2.34 MeV are released when compounds containing 10B that have accumulated in the tumor cells are exposed to thermal neutrons. These particles have the characteristics of high linear energy transfer (LET) radiation and produce enhanced biological effects. For example, it is generally accepted that high LET radiation induces more DNA-DSBs than low LET radiation.
DNA-DSBs are potentially lethal lesions created by ionizing radiation, and can be repaired by homologous recombination (HR) or non-homologous end joining (NHEJ) in mammalian cells. A number of essential proteins, including DNA-dependent protein kinase (DNA-PK), DNA-ligase IV, Rad50, and Artemis have been identified as regulators of NHEJ. Ku proteins are a component of DNA-dependent protein kinase (DNA-PK), and are involved in the repairing of DNA-DSBs by NHEJ. Xrs-5 cells (Ku80 mutant) lack functional Ku-protein, and are defective in DNA-dependent protein kinase (DNA-PK)-mediated non-homologous end-joining (D-NHEJ). Consequently, xrs-5 cells show high radiosensitivity to gamma, X-ray, or heavy-ion irradiation [1–3]
We report here that the amount of DNA damage induced by BNCR is significantly greater in D-NHEJ-defective cells compared with wild-type CHO-K1 cells, suggesting that a deficiency in the repair of DSBs indeed contributes to the enhanced sensitivity of D-NHEJ-defective cells to BNCR.
CHO K-1 (wild-type) cells and xrs5 cells (Obtained from Dr. P. Jeggo) were cultured at 37°C in a humidified 5% CO2 atmosphere in α-minimal essential medium (MEM) supplemented with 10% heat-inactivated calf serum (56°C for 30 min), penicillin (100 units/ml), and streptomycin (100 μg/ml). The cells were grown as a monolayer and maintained in the late exponential phase when the surface of the flask was almost confluent.
Boron compound and neutron irradiation
A stock solution of 10B-para-boronophenylalanine (BPA) and B-10 enriched boric acid (1000 μg/ml) was used for all experiments. The 10B concentrations were measured by prompt gamma ray (PGA) spectrometry using a thermal neutron guide tube installed at KUR.
CHO K-1 cells and xrs-5 cells exponentially growing in MEM were trypsinized and cell suspensions were incubated with 25 μg/ml boric acid or BPA at 1 hour prior to the neutron irradiation. The cells were placed in to the Teflon tube and irradiated at room temperature by neutrons from the 1MW research reactor at Kyoto University.
Radiation sources and measurement of neutron fluences
The Heavy Water Column of the Kyoto University Research Reactor was used for 1MW neutron irradiation. The thermal neutron fluences were measured by gold foil (3 mm in diameter, 0.05 mm thick) activation analysis. The gamma-ray dose including secondary gamma rays was measured with a Mg2SiO4 (Tb) thermo luminescence dosimeter. Boron concentrations in the cells were taken to be equivalent to those in the medium, as reported previously . The total absorbed dose resulting from thermal or epithermal neutron irradiation was calculated by the sum of the absorbed doses, which primarily was a result of the 1H(n,γ)2D, 14N(n,p)14C, and 10B(n,α)7Li reactions according to Kobayashi's model . The dose-converting coefficients of the 1H(n,γ)2D and 14N(n,p)14C reactions and details of the calculation method were described previously [5, 6]. Gamma-ray irradiation was produced using a cobalt-60 gamma-ray irradiator in the Research Reactor Institute, Kyoto University at a dose rate of 1.0 Gy/min.
Cell survival assay
Survival parameter D10 doses and their RBE values calculated from dose-survival fraction curves (Fig.1) of CHO-K1 and xrs-5 cells irradiated with KUR thermal neutron beam and gamma rays.
3.1 ± 0.2
1.1 ± 0.1
2.9 ± 0.2
1.4 ± 0.1
Co60 gamma ray
6.2 ± 0.3
2.0 ± 0.1
Immunofluorescent staining of γ-H2AX and 53BP1
The average number of foci per cell and their RBEa values in CHO-K1 cells irradiated by the KUR thermal neutron beam.
Time after irradiation
Average number of γ-H2AX foci/cell
Average number of 53BP1 foci/cell
Average number of γ-H2AX foci/cell
Average number of 53BP1 foci/cell
16.7 ± 4.2
15.6 ± 3.0
19.7 ± 3.0
14.2 ± 2.0
19.2 ± 4.0
16.8 ± 3.0
10.8 ± 4.0
8.8 ± 3.0
8.6 ± 3.0
7.6 ± 2.0
14.0 ± 4.2
10.4 ± 3.0
9.0 ± 3.2
8.0 ± 2.1*
6.0 ± 2.2
3.0 ± 1.2
11.0 ± 3.0
9.2 ± 3.0*
7.4 ± 3.0*
6.4 ± 1.0*
2.8 ± 2.0
1.0 ± 0.9
7.0 ± 3.2*
7.2 ± 1.1*
The average number of foci per cell and their RBEa values in xrs-5 cells irradiated by the KUR thermal neutron beam.
Time after irradiation
Average number of γ-H2AX foci
Average number of 53BP1 foci
Average number of γ-H2AX foci
Average number of 53BP1 foci
24.8 ± 4.0
22.3 ± 4.1
23.1 ± 3.0
19.2 ± 2.0
26.0 ± 4.2
24.0 ± 4.0
22.6 ± 4.0*
20.4 ± 4.2*
12.1 ± 3.0
11.8 ± 2.0
24.7 ± 4.2*
22.8 ± 4.0*
18.4 ± 3.2*
19.4 ± 3.1*
11.0 ± 2.2
10.2 ± 1.2
20.2 ± 3.0*
21.6 ± 3.0*
15.6 ± 2.0*
15.5 ± 2.0*
9.0 ± 2.0
8.8 ± 1.0
15.2 ± 2.1*
16.6 ± 2.0*
Statistical significance was calculated using the Student's t- tests. Results were considered significant for p values < 0.05.
The survival fractions of the CHO-K1 cells and the xrs-5 cells exposed to thermal neutrons and gamma rays are shown in Figure 1A and 1B. The level of cell survival following neutron irradiation decreased exponentially without a shoulder in the survival curve. The D10 dose parameters for survival following neutron and gamma-ray irradiation and their RBEs are listed in Table 1.
Tables 2 and 3 show the BNCR-RBE value as the ratio of average number of γ-H2AX and 53 BP1 foci per cell compared to that of gamma rays. The RBE values estimated by DNA-DSB focus assay varied depending on the assay time following BNCR irradiation.
We employed CHO-K1 cells and a DNA double-strand break (DSB) repair deficient derivative line (xrs-5) to investigate the relationship between DNA-DSB damage and cytotoxic potential following BNCR. In BNCR, it is thought that alpha particles and lithium atoms (which have a traveling range of 10-14 μm) from the 10B(n,α)7Li fission reaction cause DNA-DSBs. NHEJ-deficient xrs-5 cells (Ku80 mutant) are markedly sensitive to cell killing by gamma- or X-ray irradiation [1, 2]. In this report, we have shown that DNA-DSB repair deficient cells are also more sensitive to BNCR compared with low LET (linear energy transfer) irradiation. However, the RBE of the gamma-ray sensitive xrs-5 cells was not larger than that of the gamma-ray resistant CHO-K1 cells. In a previous study of BNCR, we reported that the RBEs of radio-resistant cells were larger than those of radio-sensitive cells using various malignant glioma cell lines . These results suggested that the gamma-ray resistant cells have an advantage over the gamma-ray sensitive cells in BNCR.
The initial step of the cellular response to DNA-DSBs is the phosphorylation of histone H2AX, which induces γ-H2AX foci [8, 9]. Subsequently, the 53BP1 protein accumulates at DSB lesions with γ-H2AX . It has been reported that γ-H2AX foci are a particularly sensitive DNA damage marker following low-dose irradiation . In our study, there was no variation in the appearance of γ-H2AX or 53BP1 foci in the CHO-K1 cells. In the xrs-5 cells, 53BP1 foci were greatly induced by BNCR relative to gamma-rays. H2AX foci were increased to a lesser extent by BNCR (Figures 3-B,6-B). We calculated the BNCR-RBE value as the ratio of average number of foci per cell compared to that of gamma rays (Tables 2, 3). The BNCR-RBEs estimated using the number of γ-H2AX foci in CHO-K1 and xrs-5 cells were 0.85-2.50 and 1.07-2.04, respectively. The BNCR-RBEs estimated using the number of 53BP1 foci in CHO-K1 and xrs-5 cells were 1.10-7.20 and 1.16-2.12, respectively.
In the case of CHO-K1 cells, the RBEs estimated by foci number following BNCR was varied and increased depending on the repair time. The BNCR-RBEs at 60, 90, and 120 min after BNCR in xrs-5 cells were substantially consistent and correlated with the cell killing effect of BNCR. The DSBs remaining after BNCR irradiation suggested that the constant RBE values were due to the inability of xrs-5 cells to carry out DNA repair.
In survival studies using mammalian cells, as the LET increases, the RBE increases slowly at about 10 keV/μm and more rapidly reaches a maximum at about 100 keV/μm . Using a chromosomal damage assay induced by heavy ions, Kawata et al. reported that the RBE for chomatid breaks reached a maximum value of around 2 at a LET of about 100 keV/μm . In BNCR studies, the LET range of the 1.47 MeV (α-particle) and 0.84 MeV (7Li-particle) particles are 50-231 keV/μm and 65-266 keV/μm, respectively. Using DSB repair-deficient cells, other researchers reported that the RBE did not increase with high LET irradiation [14–16]. Our RBEs for xrs-5 cells were not greater than the RBEs for wild-type CHO-K1 cells and are consistent with other reports concerning high LET and NHEJ-deficient cells. Previous studies showed that RBE correlated with the repair capacity of the cells, and the RBE of repair-deficient cells was smaller than that of repair-proficient cells . These studies reported that a RBE maximum was found at LET values between 150 and 200 keV/μm in a repair-proficient cell (CHO-K1 cell) line; on the other hand, in a repair-deficient cell line (xrs-5), the RBE failed to show a maximum, and decreased continuously for LET values above 100 keV/μm, using high LET carbon ions of different energies .
Previous studies of the induction and rejoining of DNA-DBSs in mammalian cells exposed to high LET radiation demonstrated that the number of γ-H2AX foci did not always correlate with cell killing . In a study of melanoma cells irradiated with proton and lithium beams, it was reported that the size of γ-H2AX foci was an accurate parameter correlating the rejoining of DSBs induced by different types of LET radiation and radio sensitivity . In our BNCR study, the size of γ-H2AX foci induced by neutron irradiation was unequal and rather larger than the size of foci induced by gamma rays (Figures 4, 5). It was previously reported that irradiation with 130 keV/μm high LET, nucleon nitrogen ions increased the size of induced γ-H2AX foci, while the size of low LET, x-ray induced γ-H2AX foci did not change . Another study reported that the size of γ-H2AX foci was increased after high LET lithium beam irradiation, and was correlated with cell killing . Here, we revealed that BNCR induced larger γ-H2AX foci, depending on time after irradiation, while on the other hand, the BNCR-induced foci in the CHO-K1 and xrs5 cells consisted of mixed small and large foci. The thermal neutron beam from KUR is a wide range beam that includes gamma rays and prompt gamma rays. At the absorbed dose of 2Gy, the composition of 4He and 7Li ions, thermal neutrons, epithermal neutrons, fast neutrons, and gamma rays are 63.1, 4.6, 0.5, 3.4, and 28.4%, respectively. These various components of the absorbed dose explained the lower RBE and lower DNA-DSB damage. In addition, the distribution of boron in the nucleus of the cells and the bystander effect of BNCR  will affect the efficiency of high LET radiation on cell survival and DNA-DSBs.
Our study demonstrated that BNCR induced high cytotoxic effects and low capacity to repair DNA-DSBs in NHEJ repair-deficient mutant xrs-5 cells. The RBE following BNCR of radio-sensitive mutant cells was not increased and rather was lower than that of radio-resistant cells. These results suggest that gamma-ray resistant cells have an advantage over gamma-ray sensitive cells in BNCR.
This study was supported by a Grant-in-Aid for Scientific Research from the Ministry of Education, Culture, Sports, Science and Technology of Japan.
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