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Int. J. Radiation Oncology Biol. Phys., Vol. 60, No. 2, pp. 542–552, 2004 Copyright © 2004 Elsevier Inc. Printed in the USA. All rights reserved 0360-3016/04/$–see front matter doi:10.1016/j.ijrobp.2004.03.017 CLINICAL INVESTIGATION Pediatrics GENETIC EFFECTS OF RADIOTHERAPY FOR CHILDHOOD CANCER: GONADAL DOSE RECONSTRUCTION MARILYN STOVALL, PH.D.,* SARAH S. DONALDSON, M.D.,† RITA E. WEATHERS, B.S.,* LESLIE L. ROBISON, PH.D.,‡ ANN C. MERTENS, PH.D.,‡ JEANETTE FALCK WINTHER, M.D.,§ JORGEN H. OLSEN, M.D.,§ AND JOHN D. BOICE, JR., SC.D.㛳 *Department of Radiation Physics, The University of Texas M. D. Anderson Cancer Center, Houston, TX; †Department of Radiation Oncology, Stanford University Medical Center, Stanford, CA; ‡Department of Pediatrics, University of Minnesota, Minneapolis, MN; §Institute of Cancer Epidemiology, Danish Cancer Society, Copenhagen, Denmark; and 㛳International Epidemiology Institute, Rockville, MD, and Department of Medicine, Vanderbilt Medical Center and Vanderbilt-Ingram Comprehensive Cancer Center, Nashville, TN Purpose: To estimate the doses of radiation to organs of interest during treatment of childhood cancer for use in an epidemiologic study of possible heritable diseases, including birth defects, chromosomal abnormalities, cancer, stillbirth, and neonatal and premature death. Methods and Materials: The study population was composed of more than 25,000 patients with cancer in Denmark and the United States who were survivors of childhood cancer and subsequently had nearly 6,500 children of their own. Radiation therapy records were sought for the survivors who parented offspring who had adverse pregnancy outcomes (>300 offspring), and for a sample of all survivors in a case-cohort design. The records were imaged and centrally abstracted. Water phantom measurements were made to estimate doses for a wide range of treatments. Mathematical phantoms were used to apply measured results to estimate doses to ovaries, uterus, testes, and pituitary for patients ranging in age from newborn to 25 years. Gonadal shielding, ovarian pinning (oophoropexy), and field blocking were taken into account. Results: Testicular radiation doses ranged from <1 to 700 cGy (median, 7 cGy) and ovarian doses from <1 to >2,500 cGy (median, 13 cGy). Ten percent of the records were incomplete, but sufficient data were available for broad characterizations of gonadal dose. More than 49% of the gonadal doses were >10 cGy and 16% were >100 cGy. Conclusions: Sufficient radiation therapy data exist as far back as 1943 to enable computation of gonadal doses administered for curative therapy for childhood cancer. The range of gonadal doses is broad, and for many cancer survivors, is high and just below the threshold for infertility. Accordingly, the epidemiologic study has >90% power to detect a 1.3-fold risk of an adverse pregnancy outcome associated with radiation exposure to the gonads. This study should provide important information on the genetic consequences of radiation exposure to humans. © 2004 Elsevier Inc. Childhood cancer, Genetic damage, Radiation, Dosimetry. INTRODUCTION outcomes of cancer survivors and their children are becoming increasingly important. However, there is limited knowledge of the genetic consequences of treatments for childhood cancer. The objective of the ongoing Genetic Consequences of Childhood Cancer Treatment (GCCCT) study is to determine the extent to which curative treatment, i.e., radiation therapy and chemotherapy that are mutagenic in test The treatment of children with cancer has been a great success. In the United States alone, more than 270,000 survivors of childhood cancers are presently alive. Nearly 77% of these children survive to adulthood (1), and many are able to have children of their own. Consequently, the possible adverse effects of curative treatments on the health NO1-CP-40535). Acknowledgments—The program of studies would not have been possible without the efforts of the many participating survivors, data abstractors, a large field staff, central clerical and data processing staff, and clinical collaborators. Received Dec 3, 2003, and in revised form Mar 9, 2004. Accepted for publication Mar 21, 2004. Reprint requests to: Marilyn Stovall, Ph.D., Department of Radiation Physics, The University of Texas M. D. Anderson Cancer Center, Unit 544, 1515 Holcombe Blvd., Houston, TX 77030. Tel: (713) 745-8999; Fax (713) 794-1371; E-mail: [email protected] Supported in part by contracts and grants from Westlakes Research Institute (Agreement No. 01/12/99 DC), the Danish Cancer Society, and the National Cancer Institute (U24 CA55727 and 542 Genetic effects of radiotherapy for childhood cancer ● M. STOVALL et al. 543 Table 1. Characteristics of Childhood Cancer Survivor Study (CCSS [US]) and Danish populations who received radiation therapy (XRT) Total with XRT Male Female Age at end of XRT 0–4 yrs 5–9 yrs 10–14 yrs 15–19 yrs 20–25 yrs Unknown Total Year of 1st XRT 44–49 50–59 60–69 70–79 80–89 90 or later Unknown Total Primary diagnosis Leukemia Central nervous system tumor Hodgkin disease Non-Hodgkin lymphoma Kidney (Wilms’) Neuroblastoma Soft tissue sarcoma Bone tumors Retinoblastoma Other* Total CCSS % Danish % Total % 609 236 373 100% 38.8% 61.2% 151 77 74 100% 51.0% 49.0% 760 313 447 100% 41.2% 58.8% 82 113 177 180 48 9 609 13.5% 18.6% 29.1% 29.6% 7.9% 1.5% 100% 21 22 29 64 11 4 151 13.9% 14.6% 19.2% 42.4% 7.2% 2.6% 100% 103 135 206 244 59 13 760 13.6% 17.8% 27.1% 32.1% 7.8% 1.7% 100% 0 0 0 390 209 1 9 609 0.0% 0.0% 0.0% 64.0% 34.3% 0.2% 1.5% 100% 19 33 39 31 23 2 4 151 12.6% 21.9% 25.8% 20.5% 15.2% 1.3% 2.6% 100% 19 33 39 421 232 3 13 760 2.5% 4.3% 5.1% 55.4% 30.5% 0.4% 1.7% 100% 170 44 194 65 35 18 52 31 0 0 609 27.9% 7.2% 31.9% 10.7% 5.7% 3.0% 8.5% 5.1% 0.0% 0.0% 100% 10 20 32 21 6 3 14 6 8 31 151 6.6% 13.2% 21.2% 13.9% 4.0% 2.0% 9.3% 4.0% 5.3% 20.5% 100% 180 64 226 86 41 21 66 37 8 31 760 23.7% 8.4% 29.7% 11.3% 5.4% 2.8% 8.7% 4.9% 1.1% 4.1% 100% * Gonadal, thyroid, skin, and other carcinomas. systems, contribute to adverse conditions for the offspring of childhood cancer patients, including cancer, birth defects, chromosomal abnormalities, stillbirths, and neonatal and other premature deaths (2). Medical records are being reviewed to assess radiation doses and chemotherapy modalities used in childhood cancer treatment. Essential to the epidemiologic interpretation of these data is an accurate and reproducible assessment of radiation dose to the gonads. The purpose of this article is to describe the approach taken to reconstruct doses for survivors of childhood cancer and to present preliminary dosimetric data. Ideally, human studies of the risks associated with radiation provide estimates of absorbed dose to each subject that are accurate and specific for the relevant anatomic site. Patients undergoing radiation therapy are especially suitable for such studies because irradiation is performed under controlled conditions that are well documented. However, dosimetry estimation presents special challenges. Treatments typically involve delivery of high doses to the treatment site and a wide range of doses to other organs. The dose outside treatment beams decreases substantially with distance; for example, the dose to a site 10 cm from the edge of a treatment field may be less than 1% of the dose to the tumor. Even within a single organ, the dose may vary considerably, and for paired organs, such as the ovaries, the dose differential could be great. Results from studies of pediatric patients add another dimension to this problem because the age or size of the child at the time of the treatment must be considered in determining dose to sites of interest. There has been little investigation of the dose received by organs outside the primary treatment fields. In brief summary, the sources of radiation absorbed dose outside a treated volume are (1) leakage through the treatment head of the machine, (2) scatter from the collimators and beam modifiers, and (3) scatter within the patient from the treatment beams. The relative contributions of these three components to total dose have been reported by a few investigators (3–9). Fraass and van de Geijn (4) found that collimator scatter plus leakage is of the same order of magnitude as patient scatter. Kase et al. (5) also indicate that near the beam the collimator scatter contributes 20 – 40% of the total peripheral dose and that leakage becomes the main contributor at greater distances from the field edge. Greene et al. (7) found that collimator 544 I. J. Radiation Oncology ● Biology ● Physics Volume 60, Number 2, 2004 scatter was the dominant component of the peripheral dose near the treatment beam. METHODS AND MATERIALS Population studied The details of the epidemiologic investigation can be found elsewhere (2, 10). All childhood cancer survivors who became parents were eligible for inclusion in the epidemiologic study. The GCCCT study utilizes a case-cohort design (11, 12). To date, dosimetry has been completed for a total of 760 patients treated with radiation. The characteristics of the cancer survivors who received radiation along with the primary diagnoses, are shown in Table 1. A unique aspect of the GCCCT study is the computation of organ doses for individual patients based on information in the radiation therapy records. For each patient, the doses to the ovaries, uterus, testes and pituitary are estimated for all radiation therapy delivered before the date of the relevant conception, using the methods described in this article. The epidemiologic results will be interpreted in light of dose– response evaluations. Dosimetry methods The method described here estimates radiation dose outside a treatment beam where conventional treatment-planning programs cannot be suitably applied. The method uses a dose measured in a water phantom to estimate organ doses in a three-dimensional mathematical phantom that simulates a patient of any size. This method has been used to estimate organ doses for individual patients in several large studies of the long-term effects of radiation therapy (13–15). Out-of-beam measurements in a water phantom The total radiation dose outside a treatment beam includes leakage through the head of the machine, scatter off the collimators, and scatter within the patient from the primary beam. It is essential that any estimate of dose include all these components. For this reason, the method described here is based on measurement of total radiation dose. The dose outside beams was measured on a three-dimensional grid in a large water phantom. Figure 1 shows a beam’s-eye view and a lateral view of the measurement setup. A typical set of data for one radiation energy consisted of measurements in four or more planes perpendicular to the central axis at depths ranging from 2–15 cm from the water surface. In each plane, dose was measured to a distance of 70 cm perpendicular to the central axis. Data were measured for field sizes of 5 ⫻ 5, 10 ⫻ 10, 15 ⫻ 15, and 20 ⫻ 20 cm2. The distance between measurement points was smaller near the water surface and beam edge to provide sufficient resolution in regions of rapid dose change. Outof-beam data were measured with the following beams: 60 Co (AECL Theratron-80, Mississauga, Ont., Canada), 4 MV (Varian Clinac 4, Palo Alto, CA), 6 and 10 MV (Varian Clinac 2100C, Palo Alto, CA), and 25 MV (Allis-Chalmers Fig. 1. Water phantom setup for out-of-beam measurements. (A) Beam’s-eye view. (B) Lateral view. Betatron, Milwaukee, WI). Additional data measured for AAPM Task Group 36 (16, 17) are included in the library of out-of-beam data; these are 18 MV (Varian Clinac 2100C, Palo Alto, CA) and 25 MV (Philips SL25, Andover, MA). Measurements were performed using thermoluminescent dosimeters (TLDs) containing lithium fluoride powder. The TLD measurements were verified by ionization chamber measurements at selected points. Dosimeter response was standardized in a 60Co beam with output measured by the Accredited Dosimetry Calibration Laboratory at The M. D. Anderson Cancer Center, which is sponsored by the National Institute of Standards and Technology. The measured data were applied to individual patients using one of three methods, depending on the distance from the point of calculation to the treatment beam. “In-beam” dose was calculated using depth-dose data in clinical use (18). “Near-beam” dose was calculated using a log-linear interpolation between points of measurement; this region varies 7–15 cm from the beam edge, depending on radiation energy. “Far-outside-beam” dose was calculated using a curve derived from measured data. For field sizes and depths other than those measured, a linear interpolation between measured data was used. Genetic effects of radiotherapy for childhood cancer ● M. STOVALL et al. 545 Fig. 2. Average height by sex and mathematical phantom height. Mathematical phantom The mathematical phantom simulates a person of any age. The size of the phantom specific to each age group was determined using measurements made for a study funded by the National Safety Council (NSC) and reported by the Society of Automotive Engineers (19). The NSC measurements were done in 1972 on more than 4,000 American children between 3 months and 19 years of age. Dimensions for newborns and children 1, 3, 5, 10, 15, and 19 (adult) years of age were selected because sizes and proportions for patients between these ages can be approximated by linear interpolation. In children under age 15 there is very little gender difference in average height, so no distinction is made for height by sex in the mathematical phantom. In Fig. 2, the height for selected phantom age is plotted against average height for age for males and females from CDC standard growth charts (available at: www.cdc.gov/nchs/ about/major/nhanes/growthcharts/clinical_charts.htm [2002]); the agreement is excellent at ages less than 15 years. Average height for age is used for all patients because height and weight information for individuals is often not available from radiotherapy records. Figure 3 shows the frontal view of the external surface of the 1-, 3-, 5-, 10-, and 15 year-old phantoms and the adult phantom. Arms and legs Fig. 3. Mathematical phantom, ages 1 through 15 years and adult. 546 I. J. Radiation Oncology ● Biology ● Physics Volume 60, Number 2, 2004 Fig. 4. Total absorbed dose in a water phantom from 10 ⫻ 10 cm2 fields of 60Co gamma rays and 4-, 6-, 10-, 18-, and 25-MV photons at 10-cm depth, normalized to 100% on the central axis at depth of maximum dose (Dmax). From Stovall et al. (16), with permission, of the American Association of Physicists in Medicine. of the phantoms can be moved mathematically to simulate their positions during treatment. The difference in proportions of body regions (trunk, leg, and arm length and head size) is taken into account when calculating the size of a patient at a specific age. Organs were located in the phantoms using standard anatomy references (20 –24). For the GCCCT study described here the organs of interest are ovaries, testes, uterus, and pituitary. However, the phantom also contains additional organs for use in other studies: skeleton, brain, parotid glands, salivary glands, thyroid, breasts, lungs, adrenal glands, kidneys, stomach, gallbladder, pancreas, liver, small intestine, colon, rectum, bladder, and vagina. The phantom includes the locations of active bone marrow, which is divided into 40 partitions. The weight of each partition depends on patient age (25, 26). Individual organs contain between 1 and 400 points of calculation, depending on the size of the organs and the degree of detail needed. Points within organs are evenly spaced to allow calculation of minimum, maximum, and average doses. Calculation of dose to organs outside treatment beams To calculate dose to an anatomic site outside a treatment beam for an individual patient and a specific treatment, the beam data measured in water are positioned on the appropriate size for age mathematical phantom. Additional input specifies the size of the field on the surface of the patient, beam energy, and treatment dose at maximum depth (Dmax). Treatment dose at any other depth is corrected to dose at Genetic effects of radiotherapy for childhood cancer ● M. STOVALL et al. 547 Fig. 5. Mathematical phantom for 3-year-old girl with central nervous system tumor treated with 8 ⫻ 8 cm2 left and right lateral fields to the posterior fossa, tumor dose of 4,000 cGy, from a 60Co beam. Dmax using standard central axis depth-dose data (18). Plane geometry is used to calculate the lateral distance from the nearest field edge and depth from the surface to each of the points in the organs or anatomic regions of interest. For patients whose gonads were inside or close to treatment beams, special techniques were sometimes used to reduce gonadal dose, including field blocking, testicular shields (i.e., clam shells), or relocation of the ovaries by means of oophoropexy. In general, these techniques reduce high gonadal doses to 10% or less of the unshielded dose (27–36). Most special techniques are documented in the patients’ medical records and doses are reduced accordingly. RESULTS Figure 4 shows an example of out-of-beam data measured in water, a 10 ⫻ 10 cm2 beam at 10-cm depth for six energies (16, 17). Fig. 7. Mathematical phantom for 16-year-old male patient with osteosarcoma treated with 12 ⫻ 17 cm2 anterior and posterior fields to the left midfemur, tumor dose of 5,500 cGy, from a 6-MV photon beam. Using the mathematical phantom, organ doses for three typical treatments are illustrated as examples: dose to pituitary, thyroid, breasts, and ovaries in a 3-year-old patient treated for brain cancer (Fig. 5); dose to pituitary, thyroid, breasts, and ovaries in a 5-year-old patient with a Wilms’ tumor (Fig. 6); and dose to pituitary, thyroid, breasts, and testes in a 16-year-old patient with osteosarcoma of the femur (Fig. 7). Table 2 lists typical doses to the gonads and uterus for radiation therapy of several common childhood cancers. The data in Table 2 show the considerable variation in dose among patients, depending on distance from the treatment field, tumor dose, and radiation energy. Figures 8 and 9 show that doses to the gonads in the current study are higher and cover a wider range than any previously conducted study of genetic effects. Testicular doses ranged from ⬍1 to 700 cGy (median, 7 cGy) and ovarian doses from ⬍1 to more than 2,500 cGy (median, 13 cGy). Figure 10 shows doses to the uterus for female patients. DISCUSSION Fig. 6. Mathematical phantom for 5-year-old girl with Wilms’ tumor treated with 12 ⫻ 15 cm2 anterior and posterior fields to the left abdomen, tumor dose of 2,500 cGy, from a 6-MV photon beam. Limitations of the mathematical phantom method The calculation method described here is suitable for estimating dose at any distance from square and rectangular beams for patients of any age. Commercial treatment-planning computers should be used to calculate dose to points in the field in either blocked or unblocked regions and to points within 5 cm of the beam edge. For more distant 548 I. J. Radiation Oncology ● Biology ● Physics Volume 60, Number 2, 2004 Table 2. Typical radiation doses (cGy) to gonads and uterus for common childhood cancers Gonadal dose range Tumor treated Craniospinal tumors Leukemia Hodgkin’s disease Age (yrs) at radiotherapy 7 4 15 Wilms’ tumor (kidney) Neuroblastoma 4 2 Osteosarcoma 15 Regions treated Tumor dose range Males Females Uterine dose range Brain Brain only or brain ⫹ spine Chest only Chest and abdomen Chest, abdomen, pelvis 4,500–5,500 1,800–2,500 3,500–4,500 3,500–4,500 3,500–4,500 2–7 1–84 3–13 13–54 250–500 3–13 2–2,000 6–23 73–175 300–4,500 3–13 2–2,400 5–22 56–142 300–4,500 Abdomen Chest Abdomen Limb 1,500–2,500 1,200–2,500 1,200–2,500 5,500 18–67 2–21 7–54 115–200 139–330 4–35 28–125 16–55 85–230 4–34 22–120 20–55 points, where head leakage is the major contributor to total dose, the method described here is suitable (37). The method described here is designed for therapy machines without multileaf collimators (MLC) or universal wedges (UW). Although the data presented could be used to estimate out-of-beam doses for a given number of monitor units from machines with MLCs and UWs, data measured specifically for these machines is preferred (38). Individual dose estimates are based on details of treatment documented in the patients’ records. Therefore, quality of dosimetry also depends on collection and management of data for individual patients. Diligence is required to collect records of all radiation therapy before the date of the outcome under investigation. Complete documentation includes details, such as daily log, diagram or photograph of field placement, tumor dose, and special shielding or procedures to reduce gonadal dose. With sufficient effort, complete radiation therapy records can be obtained for approximately 85%–90% of patients, depending on the time period, institution where therapy was delivered, and primary disease site. Information about assisted pregnancies, sperm banking, and other procedures performed to preserve or enhance fertility is also of interest with doses reaching the threshold dose for infertility. Sources of uncertainty in the estimation of radiation dose to gonads include misspecification of gonadal position with respect to the treatment fields; missing information on the use of gonadal shields or oophoropexy; and incorrect recording of treatment doses, field sizes and blocking position. Biologic uncertainties include issues of paternity for male survivors and the use of technology-enhanced methods to become pregnant. Because radiation-induced infertility occurs at sufficiently high gonadal doses, there is an upper limit to the gonadal dose for the cancer survivors who became pregnant. Those who exceed this range are scrutinized as outliers and would be excluded if an explanation for an impossibly high dose could not be found. Thus the potential bias due to uncertainties in the radiotherapy procedures would be in the direction of an underestimation of dose and perhaps overestimation of risk; however, because cancer survivors who had children born with a genetic condition will be compared with all survivors who had children, it is unlikely that there will be any systematic bias in the estimation of dose that could distort the estimation of risk, other than the “normal” variation associated with any exposure misclassification. Uncertainties in the biologic aspects such as paternity would work in the opposite direction and tend to allow high doses inappropriately and result in an Fig. 8. Absorbed radiation dose to testes of Childhood Cancer Survivor Study (CCSS-US) and Danish patients. Fig. 9. Absorbed radiation dose to ovaries of Childhood Cancer Survivor Study (CCSS-US) and Danish patients. Genetic effects of radiotherapy for childhood cancer ● M. STOVALL et al. 549 because of knowledge of the primary cancer, the age at diagnosis, the calendar year of diagnosis and the treatment center. For example, knowing that a child was treated for retinoblastoma would be sufficient in itself to categorize gonadal dose–-in this instance, in the dose category ⬍10 cGy. Children treated for glioblastoma and children treated for leukemia without spinal fields, similarly could be accurately characterized with respect to gonadal dose. Imputation is anticipated for less than 5% of the patients. Fig. 10. Absorbed radiation dose to uterus of Childhood Cancer Survivor Study (CCSS-US) and Danish patients. under-ascertainment of risk if cases differed appreciably from the comparison cohort, which seems unlikely. Despite these and other sources of uncertainty, deriving dose estimates consistently across a population of patients produces doses that do not differ systematically between cases and the comparison group and thus allow a meaningful estimate of radiation risks. Because radiotherapy procedures are so well characterized, radiation doses to the gonads will be reproducible and of the order of 1 Gy or less. This level of dose is higher than currently experienced in occupational settings and is in the range where cancer risks have been observed in human studies. Thus the study will be able to provide important and meaningful data on the possible genetic consequences of relatively high doses of ionizing radiation. Because adverse pregnancy outcomes are so rare, every effort is made to capture dosimetric information and estimate gonadal doses so that the statistical power of the epidemiologic study is as strong as possible. In a few instances where radiotherapy records were incomplete, we were able to impute gonadal dose with little uncertainty Comparison of dose estimates using the mathematical phantom and anthropomorphic phantoms To validate doses calculated using the method described above, an extensive comparison of organ doses estimated using the mathematical phantom and measurements in an anthropomorphic phantom (Alderson Radiation Therapy Phantom, available at: www.pi-medical.nl/rs-art.htm [2002]) was done as part of a study of second tumors in patients treated for cervical cancer (39). The anthropomorphic phantom irradiations utilized the same TLD dosimetry system that was used for the water phantom measurements. The comparison of organ doses calculated using the mathematical phantom and measured in an anthropomorphic phantom is summarized in Table 3; results show agreement to within 20% for most organs. This agreement is acceptable from the perspective of the large range of doses outside a beam. The two methods differ, however, in that the organs may not be in exactly the same location, and for each organ there are many more points of calculation in the mathematical phantom than points of measurement in the anthropomorphic phantom. Comparison of results with the mathematical phantom and published data Van der Giessen et al. (37, 40) compared their out-of-beam measurements with our data for high-energy photons and found agreement within 15%. Van der Giessen and Bierhuizen Table 3. Comparison of organ doses (cGy) estimated using a mathematical phantom and an anthropomorphic phantom, AP/PA pelvic fields, 60Co gamma rays, 15 cm ⫻ 15 cm2 field size, 80-cm source-skin distance, and 3000 cGy dose to Dmax each field Organ Mathematical phantom (average of many points for each organ) Anthropomorphic phantom Alderson female (average of TLD in several phantom slices) Brain Breast Kidney Lung Ovaries Salivary glands Stomach Thyroid Total active bone marrow 5 29 140 26 3,670 7 87 10 818 6 30 130 30 3,440 10 89 14 831 Abbreviations: AP/PA ⫽ Antero-posterior/postero-anterior; Dmax ⫽ maximum depth; TLD ⫽ thermoluminescent dosimetry. 550 I. J. Radiation Oncology ● Biology ● Physics Table 4. Detectable relative risks (RR) and associated power for total malformations among the offspring of survivors of childhood cancer RR Radiation (n ⫽ 1,960) 35% Radiation (n ⫽ 2,800) 50% All survivors (n ⫽ 5,600) 100% 1.20 1.25 1.30 1.35 1.40 54% 70% 82% 90% 95% 65% 80% 91% 96% 99% 84% 94% 99% 99% 99% (40) also presented an extensive review of other published data and found no large (⬎25%) systematic differences. François et al. (41, 42) described a mathematical phantom similar to ours, based on measurements in a water phantom. For individual organ doses, their data agree with ours to ⫾ 30%, with no systematic differences. Differences in organ doses could be explained to some extent by differences in organ locations. Epidemiologic relevance Radiation-induced heritable diseases have not been convincingly demonstrated in humans and estimates of genetic risks for radiation protection purposes are based on mouse experiments (43). The most comprehensive epidemiologic study involved Japanese atomic bomb survivors and their children; this study found little evidence for inherited defects attributable to parental exposure to radiation (44, 45). Studies of workers exposed to occupational radiation or populations exposed to environmental radiation appear to involve sample sizes that are too small and exposures that are too low to convincingly detect inherited genetic damage (46 – 49). In contrast, studies of survivors of childhood cancer offer a unique opportunity to provide quantitative information on inherited genetic disease in offspring conceived after exposure. Large numbers of subjects are available, with a wide range of gonadal dose. In some instances the doses are just below the threshold dose for infertility. Previous studies of the offspring of survivors of childhood cancer have not linked radiation therapy or mutagenic chemotherapy with increased rates of childhood cancer or Volume 60, Number 2, 2004 leukemia (50 –52) or with congenital malformations (53– 58). Offspring of female but not male survivors of Wilms’ tumor have increased rates of low birth weight and possibly birth defects attributable perhaps to radiation-induced damage to uterine musculature, abdominopelvic structures, and blood flow and not germinal mutations (59, 60). Few studies, however, have attempted to quantify chemotherapy or radiation dose to testes, ovaries, or uterus and none has been of sufficient size to detect a moderate increase in heritable risk in offspring (61, 62). Study power In Table 4, we present the relative risks and the associated power to detect a difference in total malformations occurring among the offspring of childhood cancer survivors. The power values are given for a one-sided 5% nominal significance level. The baseline malformation rate is calculated as the number of offspring with malformations (n ⫽ 242) reported in 4,225 offspring of siblings of Danish cancer survivors in the initial analyses (2). The sample size in the total sibling offspring group (comparison group) is estimated to be 11,500. Conservative assumptions are that between 35% and 50% of all the parents received treatment with radiation (60, 63). The power computations are based on comparisons of (1) the offspring of all cancer survivors and the offspring of the survivors’ siblings, and (2) the offspring of all cancer survivors and the offspring of survivors who were treated with radiation. The total survivors’ exposure to some form of mutagenic therapy will fall between these ranges. 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