Introduction
The introduction of computed tomography (CT) has tremendously improved diagnostic imaging. However, the high x-ray doses associated with CT procedures have raised health concerns [
1]. This is of particular importance for the paediatric patient population, recognized as one of the most important target groups in medical radiation protection. Technological developments in CT have substantially increased diagnostic applications and accuracy in paediatric patients. Children have a higher radiosensitivity compared to adults regarding x-ray-induced malignancies and the associated risk for exposure-induced death [
2]. Therefore, optimisation and justification of CT protocols for children is a topic of high importance in daily clinical practice [
3]. An initiative worth mentioning in this context is the Image Gently campaign of the Alliance for Radiation Safety in Paediatric Imaging, which tries to change practice by increasing awareness of the opportunities to reduce radiation dose in the imaging of children [
4]. Several studies have shown that the use of CT dose reduction techniques in paediatric CT imaging lowers the physical radiation dose [
5,
6]. However it remains unexplored if they also have an impact on the DNA damage induced by CT x-rays in children.
A recent study in the UK linked the exposure from x-rays in CT imaging during childhood to the development of brain tumours and leukaemia [
7]. However, the risk assessments at low doses remain subject of active debate. The lifespan study (LSS) of atomic bomb survivors showed a roughly linear relationship between cancer mortality and high doses of high dose rate radiation for an adult population [
8]. This resulted in the linear-no-threshold (LNT) hypothesis, implying a linear relationship between dose and biological effect without a dose threshold. Despite the considerable uncertainties and divergent views regarding the health effects and applicability of the LNT theory at low doses, the model is used for risk estimation by the international radiation protection community and referred to as the main paradigm of radiation protection [
9].
The use of sensitive biomarkers for the assessment of early x-ray effects in patients gives valuable information on dose–effect relationships for diagnostic x-rays. Earlier work demonstrated that the γ-H2AX foci assay can be used to determine the effects of CT exposure at the molecular level, namely the induction of DNA double-strand breaks (DSBs) [
10‐
13]. DSBs are considered to be the most deleterious cellular effects of x-rays, because they can result in loss or rearrangement of genetic information, leading to cell death or carcinogenesis [
14]. The phosphorylation of the histone variant H2AX is one of the earliest stages in the cellular response to DSBs and one γ-H2AX focus represents one DNA DSB, which can be quantified by immunofluorescence microscopy [
15].
A prospective multicentre study was set up in order to determine the number of x-ray-induced DNA DSBs in children undergoing a chest or abdomen CT examination. Herein, the γ-H2AX foci assay was used as an effect biomarker for radiation-induced DSBs. Blood doses were determined by a patient-specific full Monte Carlo dose simulation in order to correlate the induced DNA damage with the individual blood dose. BEIR VII age- and gender-specific risk models were used to assess the lifetime attributable risk (LAR) of cancer incidence and mortality associated with the CT examination of every individual patient.
Discussion
Our study provides evidence that CT induces DNA damage in paediatric patients, even at low doses (blood doses in the range of 0.15–8.85 mGy). Several studies reported γ-H2AX foci induction by CT x-ray exposure in adult patients [
10‐
13,
28]. However none of them investigated the DNA damage induced by CT radiation exposure in paediatric patients, nor the ultra-low dose region evaluated in the current study. Stephan et al. conducted a small scale pilot study with blood samples from ten paediatric patients undergoing CT examinations, in which chromosome analysis in lymphocytes showed a significant increase in dicentric frequencies and excess acentric fragments [
29]. However, the mean blood dose of the cohort of ten children in that study was 12.9 mGy compared to the low mean blood dose of 1.35 mGy for the 51 patients in the current study.
Currently, the vast majority of publications use the concept of effective dose to assess CT radiation burden. However, effective dose calculations can never be linked to an individual patient exposure, as reference phantoms need to be used and the quantity effective dose is designed for risk estimation in a population. To interpret the in vivo γ-H2AX foci data, it is very important to have an accurate blood dose calculation for every patient, which takes into account the patient’s anatomy, different types of CT systems, dose reduction technologies and various types of CT protocols. However, the latter analysis cannot be performed by using effective dose. This was accomplished by a Monte Carlo simulation of radiation transport in patient-specific 3D voxel models derived from the CT images. For dosimetry of paediatric patients the use of voxel models is a substantial improvement compared to dose calculation based on anthropomorphic paediatric standard phantoms, as the full Monte Carlo simulation takes into account the real anatomy of the patient.
In addition the results of the present study show that lower patient doses related to more effective CT dose reduction strategies for paediatric patients also result in a similar decrease in DNA DSBs as effect biomarker. It is internationally recognized that CT dose optimization is essential, especially for children taking into account not only dose reduction but also diagnostic image quality. A number of CT dose surveys showed substantial differences between practices for the same type of examination, suggesting that not all institutions have suitably optimized their CT protocols [
30,
31]. Dose-saving strategies are continuously evolving in terms of imaging techniques as well as dose management, and the results of the present study stress the importance of dose reduction in paediatric CT imaging. As already shown by the values of the calculated blood doses and the comparison of DLP and CTDI
vol values with national DRLs, paediatric CT radiation doses were substantially low in all participating radiology departments. One of the institutions (hospital D in Fig.
4) achieved very low doses (mean blood dose, 0.71 mGy) by using iterative reconstruction for all CT examinations; however, only chest CT patients were recruited in this institution. For the patient cohort of institution D, a very low mean level of induced γ-H2AX foci per cell (0.10 foci/cell) was recorded. Hospital E achieved a mean blood dose of 0.95 mGy corresponding to 0.13 induced foci/cell, and the data for this hospital are a mixture of chest CT and abdomen CT investigations. For both types of examination DLP values in this hospital were very low compared to the DRL (reported in Table
4). The median DLP value for abdomen CT patients in hospital E was 60.00 mGy cm (range 33.00–87.20 mGy cm), which is lower than the 25th percentile of 100 mGy cm.
When the number of induced γ-H2AX foci is plotted versus blood dose, the data point to a low-dose hypersensitivity. The observed low-dose hypersensitive response in paediatric CT is consistent with the data of a previous study on paediatric patients undergoing a cardiac catheterization [
17]. The in vitro dose–response curve for umbilical cord blood shows the same behaviour in the low dose range and supports the in vivo results.
The observed low-dose hypersensitivity challenges the LNT hypothesis, assuming less DNA damage, and can be explained by the “bystander effect” [
32]. Genetic/epigenetic changes occur not only in cells hit by the ionizing particles but also in non-irradiated cells that are neighbouring directly hit cells. The bystander effect amplifies the effects of radiation by increasing the number of affected cells, owing to cell–cell communication or soluble factors released by irradiated cells. Bystander effects are observed after co-cultivation of irradiated and non-irradiated cells and transfer of medium from irradiated to non-irradiated cells [
33,
34]. For cells in direct contact, bystander signalling can occur through gap junction intercellular communication [
35,
36]. A second route by which bystander responses are mediated is through the release of soluble factors from cells that have been irradiated. These factors have been extensively studied and several of these key molecules are central players involved in stress responses and cell–cell signalling, which are not generally specific to radiation exposure [
35]. Moreover, many aspects of bystander-mediated response have close parallels to inflammatory responses. This was recently shown in a gene set enrichment analysis that highlighted different gene expression profiles in whole blood samples irradiated with low and high doses of x-rays. Functional analysis of genes differentially expressed at 0.05 Gy showed the enrichment of chemokine and cytokine signalling [
37]. In a study by Mancuso et al., DNA damage, apoptosis and tumour induction were observed in the shielded cerebellum of mice heterozygous for
Patched after partial-body irradiations [
38]. This indicates that bystander effects in vivo have carcinogenic potential.
A possible confounder in the present study could be the increase in DSB levels due to the administration of contrast agent and the corresponding emission of secondary radiation in CT imaging. However, previous studies showed that there was no biological dose-enhancing effect if radiation and contrast agent are within the diagnostic range [
11,
39].
Epidemiological data indicate a higher relative risk of cancer per unit of radiation dose for children compared to adults, and children have also a longer lifetime for radiation-related cancer to occur [
2]. We observed a non-significant age dependency in our present study of x-ray-induced DNA DSBs. To study age dependence, the study population should be broadened and a more uniform distribution of the ages is required.
Using the calculated organ doses, the LAR for cancer mortality in the paediatric patient population undergoing a low dose chest or abdomen CT was of the order of 0.1 ‰ according to the BEIR VII data assuming the LNT hypothesis. The thyroid gland, breast tissue and gonads are structures that have an increased sensitivity to radiation in growing children. Some of these regions, such as thyroid and breast tissue, are routinely involved in chest CT imaging. Miglioretti et al. [
27] calculated radiation exposure and LAR for cancer incidence from a random sample of paediatric CTs. Their calculated LARs are an order of magnitude higher than those reported in the current study: abdomen CT 1–4 ‰ versus 0.3 ‰ (median), chest CT 2–3 ‰ versus 0.1–0.4 ‰ (median boys–girls). The main reason for the lower risk estimates in the current study are lower patient doses compared to the work of Miglioretti et al. [
27]. They reported a mean ED of 12.5 mSv for abdomen CT and 6.3 mSv for chest CT, whereas in the present work the median ED values were 2.8 mSv and 1.1 mSv respectively. The lower doses and corresponding risk estimates in the current work reflect the use of contemporary state-of-the-art low dose CT equipment and the successful implementation of dose reduction strategies for paediatric CT imaging by the participating radiology departments (as illustrated in Table
4).
Large uncertainties are associated with the risk estimates summarized in Table
5. The BEIR VII committee estimates that the excess cancer mortality due to radiation can be estimated within a factor of 2 (at 95 % confidence level). For leukaemia the corresponding factor is 4. The LNT model applied by the BEIR VII committee is based mainly on epidemiological data for radiation-induced cancers in the atomic bomb survivors in the dose range of about 100 mSv to 2.5 Sv [
8]. For lower doses involved in diagnostic radiology, epidemiological data are not available to support the LNT model mainly owing to the necessary sample size [
40]. Application of the LNT hypothesis in the low dose range may lead to an overestimation of the risk in case of the existence of a dose threshold or an underestimate in case of cooperative multicellular radiation effects such as bystander effects. It is anticipated that significant insights into dose response and cancer risks in the low dose range will emerge from molecular epidemiology studies incorporating biomarkers and bioassays [
41]. The low-dose hypersensitivity observed in the γ-H2AX foci dose response of the present study indicates that LAR estimates based on the LNT model may potentially underestimate the risks of paediatric CT imaging.
For conclusions with respect to the risk of stochastic effects of x-rays, the present study has limitations. Biological damage in T lymphocytes reflects only the damage in one tissue, namely the blood. However, we may assume that DNA damage and repair in peripheral blood lymphocytes are representative for other normal tissues [
42]. Using the γ-H2AX foci assay, only DNA DSBs induced by CT x-rays are detected but not the outcome of the DNA repair process. DNA DSBs are considered to be particularly biologically important because their repair is more difficult than other types of DNA damage. Cells have evolved mechanisms to monitor genome integrity and they respond to DNA damage by activating a complex DNA damage response pathway. Erroneous repair of DNA DSBs can result in chromosomal rearrangements, including translocations, which are associated with tumorigenesis [
43]. An increase in chromosomal aberrations due to a defect in DNA repair, as observed in ataxia-telangiectasia (AT) patients, leads to genetic instability, which in turn enhances the rate of cancer development [
44]. In the framework of cancer risk, a direct assessment of mutations in DNA or chromosomal aberrations induced by CT x-rays in paediatric patients’ lymphocytes would provide added value taking into account the mutagen–carcinogen link. However, this kind of study is not obvious in view of the low sensitivity of contemporary mutagenicity assays.
The present study emphasizes the need to optimize and minimize radiation exposure in paediatric CT imaging: lower patient doses entail less DNA damage in children. This implies the need for justification of the indications for which medical imaging involving ionizing radiation is used. From a patient’s perspective, the benefits of a medically necessary CT scan far exceed the small radiation-induced cancer risk. However, some studies suggest that a third of paediatric CT scans are unnecessary [
1]. This indicates that the referring physician and radiologist should consider whether the exam is truly clinically indicated and was not recently performed in another hospital. Furthermore, they should check if no alternative diagnostic procedure might be available, one not involving ionizing radiation such as ultrasound and MRI. When CT is indicated, great care should be taken to optimize radiation exposures in order to minimize the risk for carcinogenic effects later in life. Strategies to optimize radiation doses in paediatric CT imaging are adjustment of the CT parameters to the child’s size (guidelines on individual size/weight parameters [
45]), the scan length should be restricted to the region of interest and dose reduction techniques should be implemented taking into account the required image quality (ATM, iterative reconstruction and/or adaptive collimation). The observations of the present work should encourage medical practitioners to maximize the benefit-to-risk ratio of CT imaging in paediatric radiology.