Operation of nuclear reactors for the generation of electrical power can produce various radionuclides by fission within the fuel or by neutron activation in the structural materials and component systems of the reactor. 14C is mainly produced in reactors by 14N(n, p)14C reactions with nitrogen in the fuel, fuel cladding, coolant and moderator as a primary impurity, by 17O(n, α)14C reactions in oxide fuel, coolant and moderator, and by 13C(n, γ)14C reactions in graphite moderators. For all types of reactor except pressurised water reactors (PWRs), 14C is emitted mainly as CO21,2. In the case of boiling water reactors (BWRs), as equipped in all units in the Fukushima Dai-ichi nuclear power plant (FDNPP, 37°25′23″N, 141°01′59″E), 80–95% of the released 14C appears to be as CO2 and 5–20% as hydrocarbons2. Thus, 14C emissions from the coolant and moderator are expected during normal operation of a nuclear reactor, whereas accumulated 14C in the fuel and fuel cladding is expected to be emitted at the time of melt-down of the reactor. Thus, it is highly likely that 14C emission at the time of the accident might become much higher than during normal operations. Elevated 14C activities have been reported around many nuclear reactor sites worldwide during normal operations3. As an example of a nuclear accident, the Chernobyl NPP accident resulted in a maximum 14C excess of 281.6 Bq kg−1 C within the local environment, while the affected area, with a 14C excess of >10 Bq kg−1 C, extended to >40 km from the plant4,5. Accordingly, the release of 14C from the Chernobyl accident was estimated to be 44 PBq5. The large release of 14C from the Chernobyl accident is mainly attributed to the high production of 14C in the graphite moderators through the 13C(n, γ)14C reaction and the burning of the graphite during the accident.

Since the FDNPP accident on 11th March 2011 (Fig. 1), numerous studies of Fukushima-derived radionuclides in the worldwide environment have been conducted to reconstruct the history, levels and geochemical behaviours of the releases6,7. However, these studies mainly focused on relatively short-lived radionuclides such as 134,137Cs and 131I. Measurements of long-lived radionuclides such as 14C, 36Cl, 129I or 236U are still relatively limited and in particular, 14C remains as one of Fukushima’s most understudied radionuclides7. These “forgotten” radionuclides are mainly of academic interest because of their applicability as environmental tracers. However, 14C is one of the most important radionuclides for regional radiological assessment because it gives a significant fraction of the effective dose to the general public through the atmosphere-agricultural food-ingestion pathway.

Figure 1
figure 1

Map showing FDNPP and sampling sites in this study marked with open circles and numbers corresponding those in Table 1.

The Iwaki and Okuma tree rings in our previous studies are also shown with cross and open square, respectively8,9. The map was produced using software MapInfo Professional v5.5 using data from Digital Chart of the World (

Although 14C is not expected to constitute one of the most hazardous emissions from the Fukushima accident, from scientific and social points of view it is necessary to assess if there were any 14C releases during the accident. If 14C was indeed released, questions arise of how much was released and how it was distributed. However, such investigations have been delayed because there are not many suitable environmental materials that can capture the gaseous 14C release.

In our previous work on 14C analysis of tree rings from a 30-year-old Japanese cedar from Iwaki, approximately 50 km southwest of the FDNPP8, a local fossil fuel effect on the 14C activity was observed and identified as originating from increasing traffic on two nearby expressways that were opened in the 1990 s. In addition, a small but visible 14C increase observed in the 2011 tree ring was postulated to be caused by the release from the Fukushima accident. However, our later study on a 50-year-old Japanese cedar from Okuma, ~1 km southwest of the FDNPP confirmed significant 14C discharges during normal operations of the FDNPP between 1976 and 2010, but no visible 14C excess in 2011, at least in the southwest direction9. Recently, Povinec et al.10 discussed possible 14C contributions of Fukushima origin to the activity in offshore seawater collected on 3–7 June 2011. The profiles at two stations (37°30′N, 144°00′E and 38°00′N, 143°00′E) showed ∆14C values of around −20‰ at 100–200 m depth, implying approximately 9% contributions of Fukushima origin, on the assumption of a ∆14C value of −115‰ at 400–500 m depth as the ambient background value. Thus, the question remains unresolved as to whether the Fukushima accident in 2011 released significant amounts of 14C into the environment. If 14C was indeed released during the accident, the absence of a 14C signal in the Okuma 2011 tree ring sample might be due to the limited amount of 14C released from the damaged reactors during the accident, and/or the prevailing wind direction being away from Okuma during the releases, and/or the timing of the release being too early in relation to the main onset of photosynthetic activity. Within the context of this background, the current work (1) investigates 14C levels before and after the accident to identify any release from the accident by measuring 14C in annual tree rings of Japanese cedar trees from sites 2.5–38 km in a north and northwest direction from the FDNPP, (2) compares these values with the global and local atmospheric 14CO2 datasets, and (3) briefly discusses the difference in the magnitude of 14C released during the Fukushima accident compared to that at the Chernobyl NPP in 1986.

To achieve these objectives, it is essential to understand pre-Fukushima atmospheric 14C levels observed in Japan so as to compare them with our tree ring data. In this study, the global 14C concentrations, which are represented by the Schauinsland Station (SIL), an atmospheric CO2 monitoring station in Germany11, are considered to be the ambient background values. This justification is based on the good agreement between the long-term global atmospheric data and regional atmospheric data in Japan, including CO2, tree ring and rice grain samples measured throughout Japan. Detailed discussion of this was made in our previous study9.

In summary, the analytical results of this study reveal that 14C, with a maximum specific activity of 42.4 Bq kg−1 C above the natural background, was released during the Fukushima accident and that the activity decreased with increasing distance from the plant. Unlike other Fukushima-derived radionuclides, the released 14C is limited to the local environment (probably approximately 30 km northwest from the FDNPP). The resulting dose to the local population is negligible compared to that from natural/nuclear weapons sources.


Figure 1 shows the sampling locations in this study, in addition to other sites used in previous studies. The analytical results (δ13C and 14C) are listed in Table 1. The 14C data are expressed as fraction modern (F14C) where modern is 0.7459 times the activity of the primary standard sample, NBS oxalic acid II (SRM-4990C). The corresponding specific activities of 14C are also given in Table 1. The weighted mean F14C of the eleven humic acid secondary standards (as used in the Fifth International Radiocarbon Inter-comparison (VIRI) as Sample T)12, employed to monitor accuracy and precision, is 0.6588, with a relative standard deviation of 0.2%. This is in excellent agreement with the consensus value of 0.6587 ± 0.0035 and accordingly confirms the overall ~0.2% precision and accuracy of the measurements in this study.

Table 1 Analytical results of tree rings from Fukushima, Japan*.

Significant variations in the 14C specific activities of the tree rings were observed, ranging from 280.4 ± 0.6 Bq kg−1 C in the 2010 ring from Futaba to 226.0 ± 0.5 Bq kg−1 C in the 2015 ring from Takase. Figure 2 shows the temporal variations in 14C specific activity in tree rings from the six sites in this study, together with global atmospheric 14CO2 values from SIL, and 14C measurements from local tree rings in Iwaki and Okuma8,9. The excess 14C activity in this study can be calculated by subtracting the ambient global atmospheric 14C values at SIL, with any resulting negative values most likely caused by a local fossil fuel effect on the 14C activity (Table 1).

Figure 2
figure 2

Temporal variations of 14C in tree-ring and atmospheric CO2.

The data points of the global atmospheric 14C values are the average value of May-August of the SIL11. Note that the SIL data points of 2013–2015 are extrapolated from the exponential fitting of 14C data in period 2000–2012. The data point of year 2011 ring in Futaba is shown as the average value with 1σ standard deviation of the six sub-rings, whereas that in Takase is the average value of the early and late-wood. The 1σ uncertainties of other samples are within the symbol point. The blue and dotted lines stand for the tree rings from Iwaki8 and Okuma9.

One of the most distinctive features in the present dataset is that all the rings, except one, within the post-accident 2012–2015 period, are distributed along the SIL curve or between the SIL and Iwaki curves. The former pattern suggests that the local atmospheric 14C record follows the exponential decline in global atmospheric 14CO2, whereas the latter reveals that the atmospheric 14C in the studied area might have been slightly affected by additional local fossil fuel combustion, as demonstrated in Iwaki8. In comparison with the global atmospheric 14C levels, the 14C depletion observed in Iwaki has been attributed to the two nearby expressways, open since the 1990s8. This may not be the case for the samples from Takase and Ogaki (both of which are close to the Joban expressway), because part of the expressway construction, between Joban-Tomioka IC (just south of FDNPP) and Yamamoto IC (north of Soma city), was not completed at the time of the Fukushima nuclear accident in 2011. This part was finally opened in March 2015. In addition, the southern part between Hirono IC and Joban-Tomioka IC was temporarily closed until radionuclide decontamination finished in 2014. Therefore, like other sites worldwide, the cause of the 14C depletion at Takase and Ogaki could be attributed to CO2 emissions from fossil fuel combustion derived from local industry, traffic and household heating, etc. In comparison with the SIL curve, the fact that no significantly elevated 14C pulse was observed in post-accident rings is in good agreement with the shutdown of all reactors in the FDNPP after the 2011 accident. In contrast, the 14C concentrations in pre-accident 2009–2010 rings show complex features. The 14C concentrations in the 2010 ring from Namie and the 2009–2010 rings from Shimotsushima and Yamakiya are consistent with the SIL values, again indicating the exponential decline in the global atmospheric 14CO2 activity. On the other hand, like the enhancement in 14C prior to the accident, observed in Okuma tree rings9, the elevated 14C in the 2009 rings from Futaba, Takase, Ogaki and Namie, and in the 2010 rings from Futaba, Takase and Ogaki, confirm the existence of 14C discharges during routine reactor operations, which is consistent with observations at other nuclear sites using similar technologies3. It should be pointed out that the 14C activities in 2009 and 2010 in the Futaba sample are higher than those observed in the Okuma sample by 8% and 6%, respectively. This difference can be attributed to the sample location. Okuma is located in the crosswind direction of the FDNPP while Futaba is located along the prevailing downwind direction. This observation confirms that meteorological conditions play an important role in 14C dispersion, as observed at other nuclear sites worldwide3.

Another distinctive feature in the present dataset can be observed in the 2011 rings. Unlike the 14C specific activities from the 2011 tree rings from Shimotsushima, Yamakiya, Namie, Okuma and Iwaki, which are indistinguishable from the global atmosphere (Fig. 2), samples from Futaba, Takase and Ogaki have significantly higher 14C specific activities than the corresponding SIL values, with excess 14C activities varying from 3.0 ± 0.7 Bq kg−1 C in Ogaki to 42.4 ± 0.8 Bq kg−1 C in Futaba (Sub-section 3) (Table 1). The six sub-sections of the 2011 ring at Futaba show large 14C variations (Table 1 and Fig. 3). The excess 14C activity sharply increased from 25.4 ± 0.7 and 23.3 ± 0.7 Bq kg−1 C in the oldest two sub-sections to 42.4 ± 0.8 and 37.9 ± 0.7 Bq kg−1 C in the two middle sections, and then immediately decreased to 7.4 ± 0.6 and 3.7 ± 0.6 Bq kg−1 C in the most recent parts of the ring. Although it is not possible to identify the exact growing periods for each sub-section, as described above, the ring profile of the Futaba sample shows that the first four and later two sub-sections belong to the early wood and late wood, respectively. This means that the excess 14C activity in the early wood (23–42 Bq kg−1 C) is 3–10 times higher than the late wood (4–7 Bq kg−1 C). Similarly, the 14C concentration in the early wood from Takase is about 2 times higher than that in the late wood. Such a pattern has been observed in the 1986 rings collected from three sites within 2–12 km of the Chernobyl nuclear power plant, as a result of the accident that occurred on the 26th April 19864.

Figure 3
figure 3

Variations of the observed excess 14C activity in the sub-sections of the 2011 ring from Futaba sample.


14C releases during the Fukushima accident

The elevated 14C activities in the 2009 and 2010 rings from Futaba, Ogaki and Takase confirm the discharge of 14C during routine reactor operations of the FDNPP, as observed in the Okuma tree rings9. On the other hand, the 14C levels in the post-accident 2012–2015 rings are indistinguishable from the general atmospheric values and this strongly suggests a fast response to the cessation in 14C discharges due to the shutdown of the FDNPP after the 2011 accident. However, the cause of the elevated 14C in the 2011 rings most probably differs from that of the pre-accident. There are several possibilities that could result in the elevated 14C activities in the 2011 rings around Fukushima: (1) 14C translocation or stored photosynthate from the previous year, (2) 14C discharges from normal operations prior to 11th March 2011, and (3) 14C release from the Fukushima accident.

The use of stored photosynthate from the previous year (autumn and winter) has been studied previously in Sitka spruce and found to be relatively unimportant13. In addition, our previous study indicated elevated 14C activities in the Okuma tree rings from 1976 to 20109. However, the 14C activity abruptly decreased from 264.8 Bq kg−1 C (an excess of approx. 39.4 Bq kg−1 C) in the 2010 ring to a background level of 233.4 Bq kg−1 C in the 2011 ring. This fact indicates an immediate response to the shutdown of the FDNPP after the accident. Moreover, the 14C activities in the 2012 rings from Futaba, Takase and Ogaki declined abruptly from high values in the 2011 rings to a background value. These observations support a negligible stored photosynthate contribution to the 2011 ring in Okuma, and the 2012 rings in Futaba, Takase and Ogaki, from the previous years, which had significantly higher 14C activities.

14C produced in the coolant and moderator may be discharged into the immediate environment during normal operations, as demonstrated in the 2009 and 2010 rings within this study and the 1976–2010 rings at Okuma9. There is a positive correlation between the excess 14C activity and the average annual energy output from the six BWRs during the period of full operations within the FDNPP9:

where 14Cexcess and E are the excess 14C activity in the tree ring (Bq kg−1C) and the annual electrical energy output (GWe), respectively. Based on the annual electrical energy output (E = 0.35 GWe) generated during the period between 1st January and 11th March 201114, the excess 14C activity in the 2011 ring can be estimated to be approximately 2 Bq kg−1 C from the six BWRs. Obviously, this value is more than one order of magnitude lower than the actual maximum 14C excess (42.4 ± 0.8 Bq kg−1 C) measured in the third sub-section of the 2011 ring. Therefore, the estimation suggests that less than 5% of the excess 14C in the 2011 ring was from discharges during the routine operation of the FDNPP prior to the accident. This conclusion is further supported by the seasonal variations in wind direction. Figure S1 shows 72 h (3 day) air mass forward trajectory analysis for starting altitudes of 0 m above ground level (AGL) during the period between 1st January and 11th March 2011, calculated from the FNL database of the National Ocean and Atmospheric Administration (NOAA) and simulated by using the Hybrid Single-Particle Lagrangian Integrated Trajectory (HY-SPLIT) model15,16. These data suggest that in the costal area of Fukushima Prefecture, the wind direction was prevailing to the east or southeast during winter and to north or northwest during summer. Thus, such meteorological conditions would limit the capture of the discharged 14C along the northwest direction during the winter season in 2011 (January to early March). Also, as the majority of 14C in an annual tree ring is generally considered to be captured by photosynthesis during the summer season, 14C discharged from the FDNPP between January and March 2011 would be subject to much less captured due to the lower rate of photosynthesis during this period.

Thus, 14C release during the accident should be considered as the main source of the excess 14C activity in the 2011 tree ring. As described above, 14C can be produced within nuclear reactors by neutron reactions with nitrogen, oxygen and carbon in fuel, fuel cladding, and coolant and moderator. A summary of typical 14C production rates in various types of reactor has been given by IAEA2. For the BWR-type reactor, like those employed at the FDNPP, the calculated 14C production rates are 470, 630 and 190 GBq·GW(e)−1 a−1 in fuel, fuel cladding and coolant and moderator, respectively2. Therefore, the 14C produced in the damaged reactors (Units 1–3 in FDNPP) can be estimated if the electrical energy output and actual fuel-burn time in each reactor can be obtained.

As discussed in Miyake et al.17, the reactors in the FDNPP were normally shut down for regular inspection after every 300–400 days of operation. About 20% of the used fuel assemblies are replaced with new assemblies during each regular inspection. From the history of operation times and the number of replaced fuel assemblies, the actual fuel-burn time at the time of the Fukushima accident for Units 1–3 was estimated to fall between 850 and 1000 days17. Thus, based on the reported electrical energy output14, the calculated 14C production during the period of 850–1000 days before the accident would be 450–700, 600–940 and 180–280 GBq in fuel, fuel cladding and coolant and moderator, respectively. This reveals that a total 14C activity of 1.0–1.6 TBq might have accumulated in fuel and fuel claddings within Units 1–3 of the FDNPP.

The design of BWRs leads to a continuous release of 14C mainly produced in the coolant and moderator through the discharge stack during normal reactor operations. The 14C produced in the solid materials (i.e. fuel and fuel cladding) is generally not released during normal operation, however, the earthquake and subsequent tsunami that occurred on the 11th March 2011 damaged reactor Units 1–3 and in turn resulted in release of the 14C stored within these reactor units.

Most of the gaseous releases of 14C, in the form of 14CO2 can be assimilated by plants through photosynthesis. It is well known that the start of net photosynthesis in spring mainly depends on the ambient temperature. Positive net photosynthesis will occur as long as the water in the soil is no longer frozen18. The majority of the atmospheric releases took place between the 12th and 22nd March, with a maximum release phase from the 14th to 17th March. The local average atmospheric temperature between 08:00 and 18:00 hours, during the period of 11th–25th March 2011, was about 5 °C ( Thus, local weather conditions would enable the released 14CO2 to be captured by photosynthesis although the rate might be low. This is supported by spatial and temporal investigations which demonstrated that the light-saturated photosynthetic capacity of Cryptomeria japonica fell to only half of its maximum value in winter19.

In comparing 14C concentrations in tree rings with those of atmospheric CO2, it is important to understand at what time the cellulose in a certain part of a tree ring was synthesized from the CO2 in the air. It has been reported that the early wood of each annual ring of a Kiso Hinoki tree (Chamaecyparis obtusa, Japanese cypress), grown in a rural forest at Gifu, Japan, was formed from the beginning of May to the end of July by assuming a uniform growth rate20. On the basis of consistent 14C data between the tree ring and global atmospheric CO2, it was explained that the time-lag between the fixation of CO2 by the tree through photosynthesis and cellulose formation using the photosynthetic products seems to be negligible during the growing season of the tree. Similar results for an oak tree grown in a suburb of Uppsala in Sweden showed that the total growing time was normally from June to the end of August, and that there was no clear evidence for any delay in 14C activity between the atmospheric CO2 and the cellulose fraction in the tree, on a time scale of weeks21. However, it has also been demonstrated that 14C values for tree ring cellulose in Sitka spruce from the United States Pacific Coast seemed to follow those of atmospheric CO2 with a delay of 5 to 6 weeks13. The Fukushima accident occurred on 11th March 2011 and the radioactive releases most likely lasted until the end of the month. If the early wood was formed from the beginning of March to the end of July by assuming an equal growth rate, and if the maximum excess in 14C corresponds to the maximum radioactive release period, the third and fourth sub-sections of the 2011 ring of the Futaba sample, which contained the highest excess 14C activities, would be formed between May and June 2011. If this is the case, our results seem to be compatible with a delay of around 5–6 weeks.

Spatial distribution of the Fukushima-derived 14C

There was a spatial trend in the 14C released during the Fukushima accident. Two samples collected southwest of the FDNPP (Okuma and Iwaki) and one sample north of FDNPP (Namie) showed no visible 14C excess in the 2011 ring (Fig. 2). However, an excess in 14C was clearly observed along the northwest direction from the FDNPP, gradually decreasing from an average of 23.4 Bq kg−1 C near the FDNPP (Futaba) to 0 Bq kg−1 C around 30 km from the plant (Fig. 4). Such a 14C distribution pattern is locally consistent with other fission-induced radionuclides such as 131I and 134,137Cs22,23,24. This feature confirms that the wind direction is a major factor in controlling the 14C distribution. This is particularly true for the Okuma sample that is located only around 1 km from the FDNPP, but in a cross-wind direction. In the early stages of the Fukushima accident, the prevailing wind direction was from the west and in the later stages from the southeast (Supplementary Table S1 and Fig. S2). Based on these meteorological conditions, it can be concluded that the majority of the released 14C was dispersed towards the Pacific Ocean and the remainder was distributed inland along a northwest direction. More detailed analysis of the excess 14C spatial distribution by the best fitting exponential plot of the data shows that influence of the Fukushima-derived 14C is probably limited to within less than 30 km from FDNPP (Fig. 4). A similar spatial pattern has been reported at other nuclear sites including Chernobyl5,25. At these sites, the distances influenced by nuclear-derived 14C were usually limited to tens of kilometres.

Figure 4
figure 4

Spatial distribution of the excess 14C activity in the 2011 rings and selected short-lived radioactive isotopes (131I and 134Cs) in soil22,23 to the northwest of the FDNPP.

Note that the average values with 1σ uncertainty of sub-samples from Futaba and Takase are shown. FTB: Futaba, TKS: Takase, OGK: Ogaki, SMTSM: Shimotsushima, and YMKY: Yamakiya.

In estimating radioactive exposure at the time of the accident, exposure by inhalation of gaseous 131I is rather difficult to estimate due to a lack of direct information on levels and transport. Considering the fact that gaseous CO2 may behave closer to gaseous iodine than to particulate forms of radioactive discharges, the distribution of 14C might provide us with information for estimating gaseous iodine exposure. Indeed, the spatial distribution of 14C has some similarity to that of 134,137Cs and 131I but only in that there was a decrease in activity with increasing distance from the plant (Fig. 4). However, this figure also demonstrates that while the 14C activity falls off to a value indistinguishable from background by around 30 km, the 134Cs and 131I activities are measureable at >60 km. The spatial distributions of the latter radionuclides in the terrestrial environment were thought to be influenced not only by wind transport but also by precipitation in each location as well as their ratios as particulate forms in the air6. In contrast, the 14C is fixed by photosynthesis and cellulose formation, and expected to remain in the same locations, whereas the post-depositional behaviours of 134,137Cs and 129,131I are prone to redistribution. Therefore the relationships between these radionuclides might be more complex. It should also be noted that whereas there will be no background level of 131I or 134Cs, the 14C is being measured against an existing and significant global background level of activity and this could be a contributing factor in determining an excess activity. Nevertheless, to clarify these findings, more detailed analysis should be conducted in future.

In addition, the spatial distribution of 14C in tree rings might also provide us with a rough estimate of the possible flow of emitted radioactivity at the time of the accident. In particular, investigation of the distribution of 14C around current nuclear power plants worldwide might help us to estimate risks and to design efficient measures for radiation protection in the case of accidents.

Comparison of the Fukushima- and Chernobyl-derived 14C

It would be interesting to estimate the total 14C activity released into the atmosphere during the Fukushima accident and to compare it with the Chernobyl release. However, any detailed discussion of this is beyond the limited data available within this study. More spatial sampling and a model calculation are required to estimate the total releases of 14C and will form the basis of a future study. Nevertheless, a rough comparison of 14C releases between the accidents from Fukushima and Chernobyl can be made as follows.

The Fukushima accident resulted in the release of 14C, with excess values up to 42.4 Bq kg−1 C at ~3 km from the damaged reactors and with a significantly affected (14Cexcess > 5 Bq kg−1 C) area up to ~15 km to the northwest. However, the Chernobyl NPP accident resulted in a maximum 14C excess of 281.6 Bq kg−1 C within the local environment, while the affected area, with a 14C excess of >10 Bq kg−1 C, extended to >40 km from the plant4,5. Therefore, in comparison with the Chernobyl accident, releasing a 14C activity of 44 PBq5, the observed Fukushima-derived 14C release was very likely significantly smaller.

This difference can be reasonably explained by the different type of reactors employed at the Chernobyl and Fukushima NPPs, although the scale of the accidents was officially the same. The Chernobyl NPP was equipped with a graphite moderator which could produce 14C at a rate of >3000 GBq·GW(e)−1·a−1 alone2. However, all three damaged reactors in the FDNPP are of the BWR-type which have a total 14C production rate of 1300 GBq·GW(e)−1·a−1 2. Thus, it is clear that the lower 14C production rate in the FDNPP would result in a much lower release of 14C compared to Chernobyl where, in particular, burning of graphite significantly enhanced the 14C releases.

Implication of dose contribution to the public from the Fukushima-derived 14C

The effective dose to individuals due to 14C releases can be estimated following the model proposed by the IAEA26. In this model, it is assumed that the main 14C exposure pathway for individuals is via ingestion of foodstuffs (atmospheric carbon assimilation by photosynthesis, leading to its presence in the food chain), and that 14C activity equilibrium has been reached between atmospheric 14CO2 and foodstuffs. The effective dose is therefore proportional to the specific activity of the foodstuffs. However, such estimation is also beyond the scope of this study because information such as the fraction of the food carbon coming from local production and the dose coefficient are lacking. Nevertheless, a qualitative assessment of the dose contribution from Fukushima-derived 14C can be determined due to the fact that the activity level of the Fukushima-derived 14C is significantly lower than that produced by the global weapons tests in the 1950 s and 1960 s. This finding indicates that, unlike the large releases of other radionuclides (i.e., radiocesium and radioiodine) during the accident22,23,27, the influence of 14C was not only limited to the local environment, probably within ~30 km from the FDNPP, but also, the resulting dose to the population is negligible compared to the natural/nuclear weapons dose.


Sampling site and materials

Five blocks (sample Nos 1 and 3–6) of Japanese cedar (Cryptomeria japonica), cut from large branches of living cedar trees, were collected from Futaba, Ogaki, Shimotsushima, Yamakiya and Namie on the 11th–13th November 2014 (Fig. 1). In addition, using a 10 mm diameter tree-ring borer, one core sample (sample No. 2) was collected from a cedar tree in Takase on the 18th May 2015. These cedar trees are 10–30 years old approximately and >3 m in height. Care was taken to sample about 2 m above ground level to avoid any possible local canopy effects from 14C released from soils28. Being within 40 km from the FDNPP, the sampling sites were heavily contaminated by radionuclides released during the 2011 Fukushima accident22,23,24.

Short-term wind direction data (every 10 minutes) were obtained from several meteorological stations near the FDNPP. From these data, the frequency/direction of the wind was determined for the total cedar tree growth period. The photosynthetic period was estimated to be between the daylight hours of 08:00–18:00 (JST) approx. Due to a power failure in the FDNPP and its adjacent areas during the accident, the available meteorological data could only be obtained intermittently from the stations at Namie (10 km northwest of FDNPP), Iitate (38 km northwest of FDNPP) and Kawauchi (20 km southwest of FDNPP), the nearest available stations to the FDNPP. The main wind directions recorded in these stations are summarized in Supplementary Table S1 and two rose diagrams of the wind directions during the period of the two radioactive plumes (14th–15th and 21st–22nd March 2011) are shown in Supplementary Fig. S2.

Chemical preparations and 14C measurements

In the case of the Futaba sample (No. 1), individual annual rings were cut for the years 2009–2010 and 2012–2014. To investigate any 14C seasonal/temporal variations, six approximately equal sub-sections of the 2011 ring were separated. Due to the higher growth rate in the early wood compared with the late wood, sub-sections 1–4 fell within the early wood period, while sub-sections 5–6 are the late wood. In the case of the sample from Takase (No. 2), the early- and late-wood in the 2011 ring were cut separately, in addition to entire annual rings for years 2009–2010 and 2012–2015. The entire annual rings representing years 2009–2013 were cut for the samples (Nos 3–6) from Ogaki, Shimotsushima, Yamakiya and Namie.

The alpha cellulose fraction of each tree ring was chemically extracted and prepared for 14C analysis. Detailed procedures for the chemical extraction, combustion, CO2 purification and graphite preparation are described elsewhere29; however, a brief description is as follows: The alpha cellulose fraction was isolated using a combination of solvent extraction, bleaching with hypochlorite solution and acid-base-acid extraction. The isolated alpha cellulose was then combusted at 850 °C in an evacuated quartz tube containing CuO (as the source of oxygen) and Ag foil to mop up halides and other contaminants. The resulting CO2 was cryogenically purified and a 3 ml sub-sample converted to graphite for subsequent 14C measurement by accelerator mass spectrometry (AMS). A further aliquot of CO2 from each sample was measured for δ13C by conventional isotope ratio mass spectrometry (IRMS) using a VG SIRA 1129. In addition to the primary standard (SRM-4990C), in-house secondary standard samples comprising bulk barley mash from the Third International Radiocarbon Inter-comparison (TIRI Sample A with a fraction modern value of 1.1635)30, and individually combusted humic acid standards (VIRI Sample T with a fraction modern value of 0.6587 ± 0.0035)12, were used for quality control. Individually combusted interglacial wood samples (Heidelberg wood, VIRI Sample K) acted as the background standard sample. These standards were prepared and measured by the same procedures as the tree ring samples in order to assess the total uncertainty and background in the 14C measurements.

14C activities were calculated by 14C/13C ratio measurements using a National Electrostatics Corporation 5MV Tandem AMS in the SUERC AMS Laboratory, a Natural Environmental Research Council (NERC) Recognised Facility31. All but the background wood samples were measured to achieve better than 0.2% uncertainties for both the 14C counting statistics and the repeat measurement scatter.

Additional Information

How to cite this article: Xu, S. et al. Radiocarbon Releases from the 2011 Fukushima Nuclear Accident. Sci. Rep. 6, 36947; doi: 10.1038/srep36947 (2016).

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