- Methodology article
- Open Access
Characterization of highly efficient heavy-ion mutagenesis in Arabidopsis thaliana
BMC Plant Biology volume 11, Article number: 161 (2011)
Heavy-ion mutagenesis is recognised as a powerful technology to generate new mutants, especially in higher plants. Heavy-ion beams show high linear energy transfer (LET) and thus more effectively induce DNA double-strand breaks than other mutagenic techniques. Previously, we determined the most effective heavy-ion LET (LETmax: 30.0 keV μm-1) for Arabidopsis mutagenesis by analysing the effect of LET on mutation induction. However, the molecular structure of mutated DNA induced by heavy ions with LETmax remains unclear. Knowledge of the structure of mutated DNA will contribute to the effective exploitation of heavy-ion beam mutagenesis.
Dry Arabidopsis thaliana seeds were irradiated with carbon (C) ions with LETmax at a dose of 400 Gy and with LET of 22.5 keV μm-1 at doses of 250 Gy or 450 Gy. The effects on mutation frequency and alteration of DNA structure were compared. To characterise the structure of mutated DNA, we screened the well-characterised mutants elongated hypocotyls (hy) and glabrous (gl) and identified mutated DNA among the resulting mutants by high-resolution melting curve, PCR and sequencing analyses. The mutation frequency induced by C ions with LETmax was two-fold higher than that with 22.5 keV μm-1 and similar to the mutation frequency previously induced by ethyl methane sulfonate. We identified the structure of 22 mutated DNAs. Over 80% of the mutations caused by C ions with both LETs were base substitutions or deletions/insertions of less than 100 bp. The other mutations involved large rearrangements.
The C ions with LETmax showed high mutation efficiency and predominantly induced base substitutions or small deletions/insertions, most of which were null mutations. These small alterations can be determined by single-nucleotide polymorphism (SNP) detection systems. Therefore, C ions with LETmax might be useful as a highly efficient reverse genetic system in conjunction with SNP detection systems, and will be beneficial for forward genetics and plant breeding.
Mutation induction is a powerful tool for analysis of gene function and breeding. Among the mutagens that have been used to induce mutations, chemical mutagens such as ethyl methane sulfonate (EMS), or ionising radiation such as X-rays or γ-rays, have been especially popular in plant science. EMS can produce point mutations, mainly G/C-to-A/T transitions, with high frequency [1, 2]. Such point mutations are easily detected by mutation-detection systems such as the CEL1 nuclease assay or high-resolution melting curve (HRM) analysis [3, 4]. In combination with a single-nucleotide polymorphism (SNP) detection system, EMS-mediated mutagenesis is a powerful reverse genetics approach, called Targeted Induced Local Lesions in Genomes (TILLING) [5–9]. Because of its mutation-inducing property, EMS is also very useful for producing leaky alleles in forward genetics. By contrast, X-rays and γ-rays induce DNA damage relatively randomly and cause many types of mutations including base substitutions, deletions and chromosomal alterations [10, 11]. Although X-rays and γ-rays are suitable for production of null mutations, the mutation frequency induced by X-rays and γ-rays is lower than that obtained by EMS.
Heavy-ion beams are accepted as a novel powerful mutagen because they are able to induce mutations with high frequency at a relatively low dose at which virtually all plants survive, and they induce a broad spectrum of phenotypes without affecting other plant characteristics [12, 13]. These characteristics of heavy-ion beams are advantageous for mutation breeding. Over 30 plant cultivars have been bred with the aid of heavy-ion beams in Japan [14, 15]. Heavy-ion beams comprise accelerated ions produced by an ion accelerator such as a cyclotron or synchrotron. A noted physical characteristic of a heavy-ion beam is that the accelerated particles densely deposit their energy in a localized region along the particle path. This is strikingly different from γ-rays and X-rays, which sparsely deposit their energy in a large targeted volume. The degree of locally deposited energy is represented by the linear energy transfer (LET; the energy transferred per unit length, keV μm-1). Whereas the LETs of γ-rays and X-rays are 0.2 and 2.0 keV μm-1, respectively, the LET of a heavy-ion beam for use in biological research ranges from 22.5 keV μm-1 to 4000 keV μm-1 in the RIKEN RI-beam factory (RIBF) . It is well known that high-LET radiation shows stronger biological effects than low-LET radiation. The LET of a heavy-ion beam is selectable by ion species, and depends on the characteristics of the ion with respect to electrical charge and velocity. When a high LET is required, a heavier and highly charged ion with a low velocity is selected.
Based on radiobiological considerations, it has been suggested that heavy-ion beams predominantly induce double-strand breaks (DSBs) [17, 18]. A high yield of DSBs after heavy-ion beam irradiation was revealed by experiments on both animal and plant cells [19, 20]. Therefore, significant DNA damage is likely to be caused by heavy-ion irradiation, although sequencing analysis of heavy-ion-induced DNA alterations is limited. Shikazono et al. reported that about half of the mutations induced by carbon (C) ions with LET of 101-124 keV μm-1 were small alterations, including base substitutions and comparatively small insertions/deletions (under 100 bp), whereas the other half were rearrangements such as translocations, inversions, and comparatively large insertions/deletions (over 100 bp) . These results indicate that heavy-ion irradiation induces a broad range of mutations.
In a previous study, we found that the LET value affects the albino-mutant incidence in the M2 generation and that 30 keV μm-1 is the most effective LET value in Arabidopsis thaliana mutagenesis . This high-efficiency LET (termed LETmax) should be beneficial not only for forward genetics and breeding, but also for reverse genetics . However, the mechanisms that contribute to the efficient mutagenesis of LETmax irradiation are still unclear. Because mutagens such as EMS, γ-rays, and heavy-ion beams must be chosen appropriately depending on the experimental purpose or target genes, it is also important to know the nature of mutations induced by C ions with LETmax. In the present study, we investigated the relationship between mutation induction and parameters of heavy-ion irradiation, which comprised the number of irradiated ion particles and LET. We also determined mutations in knock-out mutants induced by C-ion irradiation with LETmax in A. thaliana, as a first step to characterize the nature of C-ion induced mutations.
Analysis of particle number and LET effects on mutation frequency
To achieve increased mutation efficiency with heavy-ion irradiation, the effects of both the number of irradiated ion particles and the LET value should be studied. The number of ion particles could determine the number of DSBs per cell nucleus, while the LET value might affect the efficiency of DSB induction (see Discussion). In a previous study, we found that C-ion irradiation with LETmax induced a three-fold higher mutation frequency than that with 22.5 keV μm-1 . To confirm the effect of both LET and particle number more precisely, C-ion irradiation was applied at doses that ranged from 50 to 600 Gy; the survival percentage in the M1 generation and albino incidence in the M2 generation were measured. The number of ion particles per cell nucleus was calculated based on the assumptions that seeds have a specific density of 1 and the size of the nucleus is 100 μm2 (see Methods). The dose (in Gy) is proportional to the LET (in keV μm-1) and the number of irradiated particles. The effect of C ions with LET of 30.0 keV μm-1 on survival percentage was greater than that at LET of 22.5 keV μm-1 (Figure 1). For C ions with LET of 30.0 keV μm-1, about 12,500 particles per 100 μm2 were needed to cause lethality, whereas at 22.5 keV μm-1 over 14,000 particles per 100 μm2 were required. The LET value had a more striking effect on the mutation frequency in the M2 generation than the M1 generation (Figure 2). Carbon ions with LET of 30.0 keV μm-1 produced a 3.28% albino incidence at the most effective particle number (8,320 per 100 μm2). By contrast, C ions with LET of 22.5 keV μm-1 produced only a 1.26% albino incidence, even at the most effective particle number (12,480 per 100 μm2). The difference in LET effect on mutation frequency between 22.5 keV μm-1 and 30.0 keV μm-1 was obvious, especially under irradiation with over 4,000 particles, which indicated that the particle number is also important to obtain a high mutation frequency. These findings indicate that C ions with LET of 30.0 keV μm-1 have a different mutational effect from those with 22.5 keV μm-1 and raise the question as to what DNA alterations are caused by these irradiation conditions.
Confirmation of mutation efficiency of C ions with LETmax
The elongated hypocotyl (hy) and glabrous (gl) mutants were screened in the M2 generation after C-ion irradiation under three conditions: LET of 22.5 keV μm-1 at a dose of 250 Gy (6,933 per 100 μm2), 22.5 keV μm-1 at a dose of 450 Gy (12,480 per 100 μm2), and 30.0 keV μm-1 at a dose of 400 Gy (8,320 per 100 μm2). Mutation frequencies and the structure of mutated DNAs in these conditions were compared. The hy and gl mutants are well characterised and the genes responsible for the respective phenotypes have been determined [24–31]. Consequently, these mutants have been used previously for similar mutated DNA analyses [21, 32, 33]. Screening of 29,595 M2 plants revealed that 23 mutants were induced by C ions with LET of 30.0 keV μm-1 at a dose of 400 Gy. The mutation frequency with 30.0 keV μm-1 was approximately two-fold higher than that in the other irradiation conditions (Table 1). These results support the preceding data in which C ions with LET of 30.0 keV μm-1 were more effective for mutation induction than those with 22.5 keV μm-1.
Characterisation of mutated DNA structure caused by C-ion irradiation
To investigate the structure of mutated DNA in the isolated mutants caused by C-ion irradiation, DNA from the isolated mutants was subjected to HRM, PCR, and sequencing analyses using primers specific for the genes responsible for the hy and gl phenotypes (see Methods). Among the 33 hy and gl mutants isolated, 18 independent mutant lines were identified. This is because mutants isolated from the same batch were thought to have originated from the same M1 plants. To confirm that all mutants classified in the same mutant line had an identical DNA mutation, all of the mutants derived from the same batch were confirmed by PCR and sequencing analysis. Because the number of identified mutant lines was limited, the following mutants were also included in the characterisation of the DNA mutations: altered meristem program (amp) 1, pinoid (pid) 1, and yellow variegated (var) 2 (see Methods) [34–36].
The identified DNA mutations are listed in Table 2. In total, 22 mutations were identified. Mutations of 17 of the 18 independent hy and gl mutant lines were determined successfully. In addition, two mutations in the AMP1 gene, two mutations in the PID1 gene, and one mutation in the VAR2 gene were identified. The C-ion-induced mutations consisted of base substitutions, deletions, insertions, and translocations. Of the 22 alleles, only four showed rearrangements, including translocations and a large deletion; these were detected in high-dose irradiated mutants (400 Gy and 450 Gy). Eighteen mutants had base substitutions or deletions/insertions less than 100 bp (Tables 2 and 3). Of the four alleles with a base substitution, three were transversions and one was a transition. Among these, only one allele (C-27-gl1) had a missense mutation (D→N), whereas the other alleles had nonsense mutations that resulted in production of C-terminally truncated proteins. In total, 21 alleles were null mutants. Whether the C-27-gl1 allele was a null mutation was not elucidated, although the phenotype of the C-27-gl1 mutant was similar to that of a null mutant of GL1 (data not shown). The size and type of mutations induced by 22.5 keV μm-1 and 30.0 keV μm-1 LET did not differ. These results indicated that C ions with LETs of 22.5 or 30.0 keV μm-1 mainly caused small alterations and that most of the induced mutants were null mutants.
Two reciprocal translocations and one complex rearrangement were detected (Figure 3). For the complex rearrangement (C30-73-gl1), only one breakpoint at the TTG1 gene was detected by TAIL-PCR. The other possible irradiation-induced breakpoints in the mutant could not be determined by any PCR analysis. However, five breakpoints were identified successfully in the mutants with rearrangements. Of the five breakpoints, four contained deletions (ranging from 9 to 28 bp), one had no deletion, and none had duplications (Figure 3). These five breakpoints were repaired, which resulted in six rejoined sites. Half of the rejoined sites showed short regions of sequence homology (microhomology; 2-5 bp), whereas the other half had inserted DNA fragments (3-16 bp), termed filler DNA . Fourteen rejoining sites of simple deletions are listed in Table 3. Eight of these rejoined sites showed 1-3 bp microhomology.
In this study, we characterised the mutation frequencies and structure of mutated DNAs in knock-out mutants caused by C-ion irradiation with LET of 22.5 keV μm-1 or 30.0 keV μm-1 (LETmax). The mutation frequency for C-ions with LET of 30.0 keV μm-1 was higher than that for C ions at 22.5 keV μm-1, as indicated by frequencies of albino mutants (Figure 2) and hy and gl mutants (Table 1). Although the number of mutants identified is too small for accurate statistical analysis, the hy and gl mutation frequencies induced by C ions with LET of 30 keV μm-1 are similar to that induced by EMS (0.87‰) and 2.5-fold higher than that induced by X-rays (0.32‰) . By contrast, the structure of mutated DNA induced by C ions with LET of 22.5 keV μm-1 or 30.0 keV μm-1 was almost identical. In both cases, over 80% of the determined mutations were small alterations and the remainder were rearrangements (Table 2). The proportion of large genetic alterations that followed repair of irradiation-induced damage might be higher than that observed in this study because a large alteration affecting an essential gene might not be transmitted to the M2 generation . Twenty-one of the 22 mutated DNAs characterised were null mutations since these mutations cause a frameshift or a nonsense mutation. The actual proportion of base substitutions induced by irradiation might be higher than that detected in this study, because some might represent silent mutations that could not be identified in the current screening. Base substitutions and small deletions/insertions were detectable by the CEL1 nuclease assay or HRM analysis. Indeed, most of the mutations identified in this study were determined by HRM (see Methods). From our results, we suggest that C-ion irradiation at LETmax can be used for effective TILLING to obtain null mutants.
Mutagens must be selected according to the experimental purpose or target genes. Carbon-ion irradiation has potential advantages for several aspects of mutagenesis. First, C-ion irradiation is more practical to administer than EMS. EMS treatment of tissues or plantlets is sometimes time-consuming because of its penetration capability. On the other hand, the irradiation times required with C-ions are short; only a few seconds irradiation is needed for imbibed seeds, tissues, and plantlets, or a few minutes for dry seeds. Indeed, by irradiation of tissue cultures or plantlets with C-ion beams, over 20 novel cultivars in diverse plant species have been produced. Second, C-ion irradiation may be advantageous in the induction of truncation mutants rather than generation of allelic series, because our data indicated that small indel mutations occurred more frequently than base-change mutations. To generate an allelic series, EMS induction of base substitutions is useful. Finally, C-ion irradiation might have potential to induce deletions with desired sizes by selection of an appropriate LET value (see below). To clarify the beneficial characteristics of mutation induction by C-ion irradiation, whole-genome investigation of mutations such as missense and silent mutations is needed.
The proportion of small alterations, such as base substitutions or small deletions/insertions and rearrangements, induced by C ions with LET of 30.0 keV μm-1 or 22.5 keV μm-1 is more similar to that induced by low-LET radiation (electrons) than that induced by C ions at 101-124 keV μm-1 LET (Table 4). Similar proportions were reported in irradiation experiments on transgenic mice, in which C ions with LET of 21.3 keV μm-1 preferentially induced small alterations (68%), as did γ-rays (71%) . Suzuki et al. reported that the proportions of large and small deletions differed between C ions with LETs of 39 keV μm-1 and 124 keV μm-1 in an irradiation experiment on human cells . These data indicate that C ions with moderate LET (around 30 keV μm-1) might have different effects on DNA alterations from C ions with LET of 101-124 keV μm-1. However, the structure of breakpoints was similar between the current study (22.5 keV μm-1 or 30.0 keV μm-1) and a previous study (101-124 keV μm-1) . In the present study, five of the six breakpoints of rearrangements had deletions, whereas no breakpoint contained a duplication (Figure 3). A previous study revealed that the breakpoints induced by C ions with LET of 101-124 keV μm-1 preferentially have deletions (11 out of 17), whereas the breakpoints induced by electrons tend to have duplications (6 out of 8) . These results imply that the process of DSB production and repair after irradiation with C ions with LETs of 22.5 keV μm-1 or 30.0 keV μm-1 might be similar to those with 101-124 keV μm-1. Therefore, 30.0 keV μm-1 appears to represent a moderate LET between low-LET radiation and 101-124 keV μm-1.
Previously, we had no clear answer to the question of why C ions with 30 keV μm-1 LET can induce a higher mutation frequency than other LET values. The current study showed no difference in the structure of mutated DNAs between C-ion irradiation at 22.5 keV μm-1 and 30 keV μm-1. Thus, the DSB repair process in both conditions might be the same, although the possibility of existence of a LET-dependent DNA repair pathway cannot be excluded. One possible explanation for the difference in mutation frequencies between these irradiation conditions is the difference in the efficiency of DSB production. Although the number of irradiated particles with LET of 22.5 keV μm-1 was larger than that with 30.0 keV μm-1, 22.5 keV μm-1 did not induce a higher mutation frequency than 30.0 keV μm-1 (Figure 2). Therefore, it is likely that 30.0 keV μm-1 C ions induced DSBs more effectively than 22.5 keV μm-1 C ions. With regard to C ions with LET values exceeding 30.0 keV μm-1, the mutation frequency was not higher than that of LETmax (30 keV μm-1) . Under these irradiation conditions, the particle number might not be sufficient to produce the same mutation effect as that with LET of 30 keV μm-1. For example, with irradiation of 4,000 particles per 100 μm2 at 61.5 keV μm-1, the absorbed dose reached about 400 Gy, at which point the M1 plants could not survive . Collectively, our results indicate that both an appropriate LET value and an adequate particle number might be needed to obtain the highest mutation efficiency with heavy-ion beam irradiation.
Alternatively, the difference in DSB qualities might be a possible explanation for the LET-dependent difference in mutation induction efficiency between 22.5 keV μm-1 and 30.0 keV μm-1. Monte Carlo calculations indicate that high-LET radiation induces a higher fraction of complex DSBs than low-LET radiation [42, 43] and complex DSBs are difficult to repair [44, 45]. The data from the Monte Carlo calculations are in good accordance with experimental measurements of the higher yield of short DNA fragments after high-LET irradiation in both animals and plants [20, 46]. Therefore, it is likely that the quality of DSBs induced by C ions with LET of 30.0 keV μm-1 might be slightly more complex than that induced by C ions with LET of 22.5 keV μm-1, and that the complex DSBs might be difficult to repair, although more-detailed theoretical and experimental data with LETs around 30.0 keV μm-1 are required to clarify this hypothesis.
The current data indicate that the structures of mutated DNA caused by C-ion irradiation with LETs of 22.5 keV μm-1 or 30.0 keV μm-1 differed from those induced by C-ion irradiation with LET of 101-124 keV μm-1. In Mesorhizobium loti, irradiation by iron ions (LET 640 keV μm-1) induced larger deletions compared with deletions induced by C ions (LET 23 keV μm-1) . These results raise the possibility that the structure of mutated DNA might be controlled by selection of an appropriate LET value. To achieve this, further experimental data under irradiation conditions with different LETs is needed as well as theoretical analysis of the quality of DSBs.
C ions at LETmax showed higher mutation efficiency than those with LET of 22.5 keV μm-1, with an efficiency that appears similar to that with EMS. To achieve such efficiency with heavy-ion beam irradiation, both LET and particle number must be optimised. In Arabidopsis, 30.0 keV μm-1 at 400 Gy (8,320 per 100 μm2) was the most effective dose. C ions at LETmax and 22.5 keV μm-1 predominantly induced null mutations. Over 80% of the null mutations were base substitutions or small deletions/insertions, which can be detected by SNP detection systems such as the CEL1 nuclease assay or HRM analysis. It is concluded that C ions with LET of 30.0 keV μm-1 might be suitable as a powerful TILLING technology in conjunction with a SNP detection system to produce null mutants.
Dry seeds of A. thaliana ecotype Columbia (Col-0) were packed in a plastic bag to obtain a monolayer of seeds. The seeds were irradiated with 12C6+ ions (22.5 keV μm-1 or 30.0 keV μm-1 LET) with a dose range of 50 Gy to 500 Gy using the E5 beam line in the RIKEN RI-beam factory. The ions were accelerated up to 1.62 GeV, at which the LET value of the 12C6+ ions was 22.5 keV μm-1. The LET value of the 12C6+ ions was adjusted to 30.0 keV μm-1 by reducing the velocity of the ions. To reduce the ion velocity, the ions were passed through a combination of absorbers . All LET values were calculated behind the seeds. The irradiated M1 seeds were surface-sterilised by dipping in 1% sodium hypochlorite for 10 min, washed five times with sterilised water, and incubated on 0.7% agar-containing Murashige and Skoog (MS) medium supplemented with MS vitamins and 3% sucrose at 4°C in the dark for 4 d to induce vernalisation. Subsequently, the seeds were incubated at 22°C under long-day conditions (16 h light, 8 h dark). Seedlings that developed true leaves were transplanted into plastic trays (13 × 9 cm2) that contained soil. Eleven seedlings were planted in each tray and grown at 22°C under long-day conditions in a greenhouse. The M2 seeds were collected from all plants in each tray and were treated as one batch.
Analysis of particle effect on plant survival and DNA mutation
Measurement of percentage survival of irradiated M1 seeds and albino incidence in the M2 generation was performed as described previously . At least three independent experiments at different doses of irradiation were carried out for each LET value. To estimate the number of particles per cell nucleus, the number of particles at each dose was calculated for a water area of 100 μm2 with a specific gravity of 1, as described previously .
Mutant screening and identification of mutated genes
From the M2 generation, elongated hypocotyl (hy) and glabrous (gl) mutants were screened by germination of the M2 seeds on MS agar medium. M2 plants that showed the hy and gl phenotypes were isolated. Genomic DNA was purified from the isolated mutant and wild-type plants four weeks after germination using the DNeasy Plant Mini Kit (QIAGEN, Hilden, Germany). The purified DNAs were subjected to HRM analysis using primers specific for the putative mutated genes (HY1, HY2, HY3, and HY4 for the hy mutants; GL1, GL2, and TTG1 for the gl mutants; see Additional file 1). HRM analysis was performed on a LightCycler 480s (Roche Diagnostics, Penzberg, Germany) in a reaction mixture that contained 10 ng wild-type DNA, 10 ng mutant DNA, 0.5 mM of each primer, and 3 mM MgCl2 in the LightCycler 480 High Resolution Melting Master containing ResoLight dye (Roche Diagnostics) adjusted to a total volume of 10 μl with PCR-grade water. The reaction conditions comprised an activation step at 95°C for 10 min followed by 50 cycles of 95°C for 10 s, a touchdown of 65°C to 55°C for 10 s (0.5°C cycle-1), and 72°C for 10 s. Before the HRM step, the products were heated to 95°C for 1 min and frozen to 40°C for 1 min. HRM analysis was carried out over the range from 65°C to 95°C, rising at 4.4°C s-1 with 25 acquisitions per degree. All reactions were performed in replicate (duplicate or triplicate) in 96-well plates. When a positive signal was identified, the amplified fragment was sequenced using the Big Dye Terminator v. 3.1 Cycle Sequencing Kit (Applied Biosystems) and a 3730xl DNA Analyser (Applied Biosystems) with the same primers as those used for HRM analysis. When the whole or part of the coding region could not be amplified, flanking sequence analysis using TAIL-PCR was performed . Primers used for flanking sequence analysis are listed in Additional file 2. Because of the limited number of hy and gl mutant lines identified, mutations induced in three additional well-characterised morphological mutants, namely altered meristem program (amp) 1 , pinoid (pid) 1 , and yellow variegated (var) 2 , were isolated and their mutated genes were determined by PCR or HRM analysis and sequenced using specific primers (see Additional files 1 and 2). The M3 seeds of the mutants were harvested and the phenotype of the M3 plants was analysed to confirm whether the phenotype of the mutants was inherited.
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We thank the RIKEN Research Resources Center of the Brain Science Institute for performing DNA sequencing. This experiment was performed at RIBF operated by the RIKEN Nishina Center and CNS, University of Tokyo. We also acknowledge the Internship Program for Chinese Graduate Students affected by Sichun Earthquake from RIKEN for YL. This work was partially supported by grants from the research project Utilizing Advanced Technologies in Agriculture, Forestry and Fisheries from the Ministry of Agriculture, Forestry and Fisheries of Japan, Social Infrastructure Technology Development Program from RIKEN and the Funding Program for Next Generation World-Leading Researchers, initiated by the Council for Science and Technology Policy from the Japan Society for the Promotion of Science for TA. This work was also supported by Grants-in-Aid for Scientific Research (no. 20780009 and no. 23770070 to YK) from the Ministry of Education, Culture, Sports, Science and Technology of Japan, and the Special Postdoctoral Research Program of RIKEN (to YK).
TA conceived the study, designed the research, coordinated the project and obtained the beam times. YK and TA participated in the design of the molecular genetic analyses. YK, TH, HS, SO, YH, and TA performed C-ion irradiation. YK, TH, HS, YL, and SO conducted mutant screening. YL and SO participated in growing plants. YK, TH, and YL carried out the molecular genetic analyses. YK and TA were primarily responsible for drafting and revising the manuscript with contributions from the co-authors. All authors read and approved the final manuscript.
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Kazama, Y., Hirano, T., Saito, H. et al. Characterization of highly efficient heavy-ion mutagenesis in Arabidopsis thaliana. BMC Plant Biol 11, 161 (2011). https://doi.org/10.1186/1471-2229-11-161
- Mutation Frequency
- Linear Energy Transfer
- Ethyl Methane Sulfonate
- Ethyl Methane Sulfonate
- High Mutation Frequency