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Mutation Research 499 (2002) 135–141 Effects of irradiated medium with or without cells on bystander cell responses Hongning Zhou a,, Masao Suzuki a , Charles R. Geard a , Tom K. Hei a,b a Center for Radiological Research, Vanderbilt Clinic 11-201, College of Physicians and Surgeons, Columbia University, 630 West 168th Street, New York, NY 10032, USA b Environmental Health Sciences, School of Public Health, Columbia University, New York, NY 10032, USA Received 20 July 2001; received in revised form 11 September 2001; accepted 15 October 2001 Abstract Recent studies have indicated that extranuclear or extracellular targets are important in mediating the bystander genotoxic effects of -particles. In the present study, human–hamster hybrid (A L ) cells were plated on either one or both sides of double-mylar dishes 2–4 days before irradiation, depending on the density requirement of experiments. One side (with or without cells) was irradiated with -particles (from 0.1 to 100 Gy) using the track segment mode of a 4 MeV Van de Graaff accelerator. After irradiation, cells were kept in the dishes for either 1 or 48 h. The non-irradiated cells were then collected and assayed for both survival and mutation. When one side with cells was irradiated by -particles (1, 10 and 100 Gy), the surviving fraction among the non-irradiated cells was significantly lower than that of control after 48h co-culture. However, such a change was not detected after 1 h co-culture or when medium alone was irradiated. Furthermore, co-cultivation with irradiated cells had no significant effect on the spontaneous mutagenic yield of non-irradiated cells collected from the other half of the double-mylar dishes. These results suggested that irradiated cells released certain cytotoxic factor(s) into the culture medium that killed the non-irradiated cells. However, such factor(s) had little effect on mutation induction. Our results suggest that different bystander end points may involve different mechanisms with different cell types. © 2002 Elsevier Science B.V. All rights reserved. Keywords: Bystander effect; -Particle irradiation; Double-mylar; Mutagenesis 1. Introduction Over the past several years, considerable evidence has indicated that extranuclear and extracellular targets are also important in mediating the genotoxic effects of radiation [1–8]. When only a fraction of the cell pop- Presented at Bystander Effects Workshop, Dublin, Ireland, December 2000. Corresponding author. Tel.: +1-212-305-9981/0846; fax: +1-212-305-3229. E-mail address: [email protected] (H. Zhou). ulation is irradiated by -particles, biological effects, such as sister chromatid exchange [1,2], induction of micronuclei [3], gene mutation [4,5] and expression of certain stress-related genes [6,7] have been observed in a significantly higher proportion of cells than those that are actually traversed by an -particle. These studies suggest that damage signals might be trans- mitted from irradiated to neighboring non-irradiated cells in the same population, leading to the induction of genetic changes among these bystander cells [5,7]. Alternatively, the bystander effects might be mediated by the release of cytokines or other soluble factors 0027-5107/02/$ – see front matter © 2002 Elsevier Science B.V. All rights reserved. PII:S0027-5107(01)00285-8

Effects of irradiated medium with or without cells on bystander cell responses

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Page 1: Effects of irradiated medium with or without cells on bystander cell responses

Mutation Research 499 (2002) 135–141

Effects of irradiated medium with or withoutcells on bystander cell responses�

Hongning Zhoua,∗, Masao Suzukia, Charles R. Gearda, Tom K. Heia,ba Center for Radiological Research, Vanderbilt Clinic 11-201, College of Physicians and Surgeons,

Columbia University, 630 West 168th Street, New York, NY 10032, USAb Environmental Health Sciences, School of Public Health, Columbia University, New York, NY 10032, USA

Received 20 July 2001; received in revised form 11 September 2001; accepted 15 October 2001

Abstract

Recent studies have indicated that extranuclear or extracellular targets are important in mediating the bystander genotoxiceffects of�-particles. In the present study, human–hamster hybrid (AL) cells were plated on either one or both sides ofdouble-mylar dishes 2–4 days before irradiation, depending on the density requirement of experiments. One side (with orwithout cells) was irradiated with�-particles (from 0.1 to 100 Gy) using the track segment mode of a 4 MeV Van de Graaffaccelerator. After irradiation, cells were kept in the dishes for either 1 or 48 h. The non-irradiated cells were then collectedand assayed for both survival and mutation. When one side with cells was irradiated by�-particles (1, 10 and 100 Gy), thesurviving fraction among the non-irradiated cells was significantly lower than that of control after 48 h co-culture. However,such a change was not detected after 1 h co-culture or when medium alone was irradiated. Furthermore, co-cultivation withirradiated cells had no significant effect on the spontaneous mutagenic yield of non-irradiated cells collected from the otherhalf of the double-mylar dishes. These results suggested that irradiated cells released certain cytotoxic factor(s) into the culturemedium that killed the non-irradiated cells. However, such factor(s) had little effect on mutation induction. Our results suggestthat different bystander end points may involve different mechanisms with different cell types. © 2002 Elsevier Science B.V.All rights reserved.

Keywords:Bystander effect;�-Particle irradiation; Double-mylar; Mutagenesis

1. Introduction

Over the past several years, considerable evidencehas indicated that extranuclear and extracellular targetsare also important in mediating the genotoxic effects ofradiation [1–8]. When only a fraction of the cell pop-

� Presented at Bystander Effects Workshop, Dublin,Ireland, December 2000.

∗ Corresponding author. Tel.:+1-212-305-9981/0846;fax: +1-212-305-3229.E-mail address:[email protected] (H. Zhou).

ulation is irradiated by�-particles, biological effects,such as sister chromatid exchange [1,2], induction ofmicronuclei [3], gene mutation [4,5] and expression ofcertain stress-related genes [6,7] have been observedin a significantly higher proportion of cells than thosethat are actually traversed by an�-particle. Thesestudies suggest that damage signals might be trans-mitted from irradiated to neighboring non-irradiatedcells in the same population, leading to the inductionof genetic changes among these bystander cells [5,7].Alternatively, the bystander effects might be mediatedby the release of cytokines or other soluble factors

0027-5107/02/$ – see front matter © 2002 Elsevier Science B.V. All rights reserved.PII: S0027-5107(01)00285-8

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136 H. Zhou et al. / Mutation Research 499 (2002) 135–141

into the culture medium [8–10]. However, the exactmechanism(s) of the phenomenon is unclear.

Although cell–cell communication appears to playan important role in mediating the bystander effect[5,7], there is no evidence to rule out possible con-tributions from the transfers of soluble mediatorsgenerated in irradiated medium. It is most likelythat multiple mechanisms are involved in bystandereffects. Previous studies using medium transferredhave shown that medium from irradiated cells caninduce bystander effect in non-irradiated cells [8–10].To clearly identify the potential contribution ofmedium alone and of medium plus cell irradiation tothe bystander effect, the double-mylar method wasutilized in this study.

The double-mylar technique is useful for evaluatingthe roles of medium in bystander effects since cellscan be plated on either one or both sides of the dishes(Fig. 1), the distance between the mylar surfaces inthe double-mylar dishes is 9.5 mm. Since, low energy�-particles can only traverse a very limited distance,

Fig. 1. Schematic diagram of a representative 35 mm i.d. double-mylar cell culture dish where only the upper layer contains amonolayer of attached cells (A). When�-particles traverse thebottom mylar layer, no cells are hit. In contrast, when a monolayerof cells are plated on both mylar layers which are separated by9.5 mm (B),�-particles would traverse the bottom but not the toplayer of cells. A hole on each side of the ring serves as a fillingport for medium.

typically less than 50�m, when one side (with orwithout cells) is irradiated with�-particles, cells onthe other sides will not receive any hits. Becausethere is no cell–cell contact between cells on thetwo sides and the only communication available isthrough the medium, this is a novel approach to inves-tigate the roles of medium in mediating the bystandereffect.

2. Materials and methods

2.1. Cell culture

The human–hamster hybrid (AL) cells that containa standard set of Chinese hamster ovary-K1 chromo-somes and a single copy of human chromosome 11were used in this study. Chromosome 11 encodes cellsurface markers that render AL cells sensitive to killingby a specific monoclonal antibody in the presenceof complement. Rabbit serum complement was fromHPR (Denver, PA). Antibody specific to the CD59antigen was produced from hybridoma culture asdescribed [11,12]. Cells were maintained in Ham’sF-12 medium supplemented with 8% heat-inactivatedfetal bovine serum, 25�g/ml gentamycin and2× 10−4 M glycine at 37◦C in a humidified 5% CO2incubator and passaged as described [13–15].

2.2. Irradiation procedure

Exponentially growing AL cells were plated on oneside or both sides of the double-mylar dishes severaldays before irradiation, depending on the cell densityrequirement of experiments. Mylar (6�m in thick-ness) is epoxied to both sides of 35 mm i.d. stainlesssteel rings (42 mm o.d.). The stainless steel rings haveaccess ports with plugs on opposite sides (Fig. 1) withthe two mylar cell growth surfaces being 9.5 mm apart.Briefly, 1× 105 exponentially growing AL cells wereplated on one side of double-mylar dishes. Two dayslater, the medium was aspirated, the double-mylardishes were turned over and 2× 105 cells were platedon the other side. After cells attached on the bottom(at that time, the cells on the upper layer remainedhydrated), the dish was filled up with 7–8 ml com-pleted medium and kept in an incubator for another2 days before irradiation. One side of dishes with or

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without attached cells (bottom layer) were irradiatedby the 90 keV/�m �-particles ranging in doses from0.1 to 100 Gy using the track segment mode of a4 MeV Van de Graaff accelerator at the RadiologicalResearch Accelerator Facility of Columbia Univer-sity. The linear energy transfer of the�-particles isthe same as that used in bystander microbeam exper-iments [5,14,16]. After irradiation, cells were kept inthe dishes for either 1 or 48 h, then the non-irradiatedcells in the upper layer were collected for thesurvival and the mutation assay as described before[13–15].

2.3. Cytotoxicity of irradiated medium with orwithout cells on non-irradiated cells

Upper mylar sheets containing non-irradiated ALcells were collected either at 1 or 48 h after irradiation.Cultures were trypsinized, counted with a Coultercounter and aliquots of the cells were re-plated into100 mm diameter petri-dishes for colony formation,the others were further incubated for mutation assay.Cultures for clonogenic survival assay were incubatedfor 7–8 days, at which time they were fixed withformaldehyde and stained with Giemsa. The numberof colonies was counted to determine the survivingfraction as described [13–15].

2.4. Quantification of mutations at theCD59 locus

To determine the mutant fraction, after a 7-dayexpression period, 5× 104 cells per dish were platedinto six 60 mm dishes in a total of 2 ml of growthmedium, the cultures were incubated for 2 h to allowfor cell attachment, after which 0.3% CD59 anti-serum and 1.5% (v/v) freshly thawed complementwere added to each dish as described [17]. The cul-tures were further incubated for 7–8 days. At thistime, the cells were fixed and stained and the num-ber of CD59− mutant colonies was scored. Controlsincluded identical sets of dishes containing antiserumalone, complement alone or neither agent. The cul-tures derived from each treatment dose were tested formutant yield for two consecutive weeks to ensure fullexpression of the mutations. The mutant fraction ateach dose was calculated as the number of survivingcolonies divided by the total number of cells plated

after correction for any non-specific killing due tocomplement alone.

2.5. Statistical analysis

All numerical data were calculated as mean andS.D., comparisons of survival fraction (SF) and mu-tation fraction between treatment groups and controlswere made by Student’st-test. A P-value of 0.05 orless between groups was considered to be significanceof the differences.

3. Results

3.1. Effect of irradiated medium alone onthe survival of non-irradiated bystander cells

After �-particles were targeted at the empty, bot-tom mylar layer without attached cells (Fig. 1A), theSFs of non-irradiated AL cells grown on the upperlayer were determined. The normal plating efficiency(PE) of AL cell population used in these experimentsaveraged 0.75± 0.06, a number similar to the PE ofnon-irradiated AL cells cultured in the double-mylarrings. After both 1 and 48 h co-culture, non-irradiatedcells in the 0.1 Gy irradiation group showed a slightdecrease in SF (SF∼ 0.85, Fig. 2). As the doses

Fig. 2. SF of non-irradiated cells in double-mylar dishes wheremedium only was irradiated by�-particles ranging in doses from0.1 to 100 Gy. Data were pooled from three independent experi-ments. Bar represents±S.D.

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increased, the SF of unirradiated cells did not showany further decrease, but a gradual increase instead.However, in no instance was there a significant dif-ference in survival between or among these groups(Fig. 2). As shown in Fig. 2, after 10 or 100 Gy irra-diation, the SFs of the non-irradiated cells in the 48 hco-culture group were 1.19 ± 0.23 and 1.13 ± 0.20,respectively,<20% higher than control levels, thoughthe difference was not significant.

3.2. Effect ofα-particle-irradiated medium withcells on the survival of non-irradiated cells

One hour after the bottom layer with AL cellswere irradiated by�-particles ranging in doses from0.1 to 100 Gy, there were no significant differencesin survival between the upper non-irradiated layerof cells and control, where no�-particles weredelivered (Fig. 3). However, if the cells were contin-uously co-cultured for a period of 48 h, the SF of thenon-irradiated, upper layer of cells decreased signif-icantly at doses between 1 and 100 Gy (P < 0.05),but there was no clear response as dose increased.It should be noted that if these values are contrastedagainst the values of medium alone irradiation ratherthan no irradiation, these significant differences arefurther enhanced. These data suggest that irradiatedcells released certain cytotoxic factor(s) into the cul-ture medium that were toxic to the non-irradiated cells.

Fig. 3. SF of non-irradiated cells in double-mylar dishes wherethe bottom layer of cells were irradiated with graded doses of�-particles from 0.1 to 100 Gy. Data were pooled from threeindependent experiments. Bar represents±S.D.

Fig. 4. Mutation fraction of the upper, non-irradiated layer of AL

cells in double-mylar dishes where only media were irradiated by�-particles ranging in doses from 0.1 to 100 Gy. Data were pooledfrom three independent experiments. Bar represents±S.D.

3.3. Effects of irradiated medium with or withoutcells on induction of bystander mutagenesis

Figs. 4 and 5 show the CD59 mutant yield of theupper non-irradiated layer of AL cells induced bygraded doses of the�-particles delivered at the bottomlayer of mylar without and with an attached mono-

Fig. 5. Mutation fraction of the upper, non-irradiated layer of AL

cells in double-mylar dishes where the bottom layer of cells wereirradiated with graded doses of�-particles from 0.1 to 100 Gy. Datawere pooled from three independent experiments. Bar represents±S.D.

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layer of cells, respectively. The spontaneous mutantfraction of AL cells used in this study was 52±10 per105 survivors. Compared to non-irradiated controls,irradiated medium without cells, when co-culturedwith an upper layer of non-hit cells for either 1 or48 h, had no significant effect on the spontaneousCD59 mutation incidence of the latter over a range of�-particle doses from 0.1 to 100 Gy (Fig. 4). Similarly,when a monolayer of cells attached to the bottomlayer of the mylar were irradiated and co-cultured foreither 1 or 48 h with the upper layer of non-irradiatedcells, the mutant fractions of the latter were not signif-icantly different from the controls (Fig. 5). It shouldbe noted that mutation levels for cells assayed after48 h exposure were consistently greater than thosefound after 1 h exposure, though the differences werenot statistically significant. A persistent, non-dosedependent increase in mutant fraction of 20–25%above the background level was seen in the bystandercells following exposure to irradiated medium for 48 h.However, this induction level was not significantlydifferent from the background level. These resultssuggested that the cytotoxic factor(s) that was releasedfrom irradiated cells into the culture medium had littleeffect on the mutagenic response of the non-irradiatedcells exposed to the same culture medium.

4. Discussion

It has long been accepted that the important geneticeffects of radiation in mammalian cells, such as muta-tion and carcinogenesis are attributable mainly to thedirect result of DNA damage. However, recent investi-gations have indicated that�-particles can cause DNAalterations by a mechanism(s) that is independent ofnuclear or even whole-cell traversals [1–10]. Such aphenomenon has been observed with both high andlow LET irradiations. For example, very low dosesof �-particles can induce sister chromatid exchangesin both Chinese hamster ovary and human fibroblastcultures at levels significantly higher than expectedbased on microdosimetric calculation of the numberof cells estimated to have been traversed by a parti-cle [1,2]. These studies suggest that bystander effectsmight be induced by damage signals transmitted fromirradiated to neighboring non-irradiated cells [5,7] orbe mediated by soluble extracellular factors [8,18,19].

However, the mechanism(s) of the bystander effectsis unclear. It was found, for example, that conditionedmedium from�-irradiated epithelial cells reduced thePE and increased the incidence of apoptosis of unir-radiated epithelial cells, but that this effect was notobserved in similarly treated fibroblasts. This effectwas found to be dependent on cell number present atthe time of irradiation, suggesting the production ofsoluble factor(s) by the irradiated cells [8].

Using the microbeam facility at Columbia Univer-sity, our laboratory reported that cytoplasmic traversalby �-particles resulted in a mutagenic response in thenucleus of the target cells at a frequency that was threetimes higher than background, while inflicting mini-mal toxicity and that free radicals mediated the muta-genic process [16]. Furthermore, we found that cellslethally irradiated with�-particles induced a bystandermutagenic response in neighboring non-irradiatedcells at a level that was two–three-fold higher thanexpected in the absence of bystander modulationand that cell–cell communication process played acritical role in mediating the process [5]. Herein,using double-mylar technique, we found that whenthe lower layer of attached cells were irradiated with�-particles, the SF among the non-irradiated upperlayer of cells was significantly lower than that of con-trol after 48 h of co-culture and that no dose–responserelationship was observed. However, no change insurvival was detected in the 1 h co-culture group orin groups where only medium was irradiated. Thesesurvival data suggested that irradiated cells releasedcertain cytotoxic factor(s) into the culture medium thatwere toxic to the non-irradiated cells. Recently, usingnormal human fibroblasts, Lehnert and co-workersreported [9,10] that an increase in cell growth inducedby very low doses (<0.2 Gy) of�-particles correlatedwith intracellular increase in reactive oxygen species(ROS) along with a decreased in TP53 and CDKN1Aand that these cellular responses were mechanis-tically coupled. In these processes, it seemed thatROS caused a prompt increase in the availability ofextracellular TGF-� that might additionally activatecell surface membrane-associated NADH oxidaseand a release of H2O2 as a subsequent and perhapssustaining event. In the present studies, irradiatingmedium alone at doses of 10 or 100 Gy, the survivingfraction of non-irradiated upper layer bystander cellsincreased, although the difference is not significant.

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It is then possible that irradiating complete mediummay produce changes that can stimulate cell growth.However, this effect (if active) is counter-acted whencells are present, since doses from 1 to 100 Gy initiateproduction of factors in hit cells which are toxic tonon-hit cells.

Co-cultivation with irradiated cells had little effecton the mutagenic yield of cells on the non-irradiatedhalf of the double-mylar dishes. These results sug-gested that the cytotoxic factor(s) that was releasedfrom irradiated cells into the culture medium had littleeffect on the mutagenic response of the non-irradiatedcells exposed to the same culture medium. These dataare in contrast with our microbeam-based bystanderstudies. In non-hit bystander cells, mutant fractionswere elevated (∼three-fold greater than expectation).In the presence of the gap junction inhibitor (lin-dane), the mutation levels were significantly reduced.Hence, intercellular communication plays a highlysignificant role in mediating the bystander mutageniceffect [5]. However, these results are also consistentwith those reported here in that a small (∼1.2-fold)non-significant increase in mutant fraction wasrecorded from cells exposed to irradiated mediumboth with and without cells. That is, it appears thatcell communication plays a much more dramatic rolethan cellular release of medium soluble factors ininitiating the mutagenic bystander response. Clearlythen, multiple mechanisms are involved in mediatingbystander responsiveness. These results are also con-sistent with data obtained in dilution experiments inwhich cells irradiated with�-particles are mixed witha fixed proportion of control cultures to achieve 20%irradiated population. No significant enhancementin bystander mutagenic effect was detected in thesemixing studies [20], again suggesting that cell–cellcontact was a principal requirement and that labilemediator(s) was much less likely to be involved inthe bystander mutagenesis, at least in the cell lineused in this study. In contrast, there is recent evidencethat irradiated cells produce an apoptosis inducingmolecular(s) into the culture medium and initiateapoptosis in the non-irradiated, bystander cells [19].More recently, Mothersill et al. founded that mediumfrom irradiated E89 cells (glucose-6-phosphate de-hydrogenase (G6PD) null CHO-K1 cell line) andE89t cells (null CHO-K1 cell line with the G6PDgene transfected back in) both produced a bystander

survival effect when irradiated conditioned-mediumwas transferred to unirradiated HPV 16-immortalizedhuman keratinocytes. However, such an effect wasnot found when the non-irradiated E89 cells receivedmedium from irradiated E89 cells, which clearly in-dicated that the response of E89 cells to the signalwas compromised by the lack of G6PD although thesignal production was present. These data suggestedthat generation of ATP or reduced NAD/NADP maybe critical to the production of a bystander effect,further implicating that signal production and cellularresponse involves different mechanisms [18]. Combin-ing our recent findings that cell–cell communicationprocess played a crucial role in mediating bystandermutagenesis [5], the present studies provide clear evi-dence that different bystander end points may involvedifferent mechanisms with different cell types.

Acknowledgements

We thank Mr. Stephen Marino of the RadiologicalResearch Accelerator Facility of Columbia Universityfor his help in performing the dosimetry and irradia-tion. This work was supported in part by NIH GrantsCA49062, CA75384, CA75061, DOE 98ER62687 andNIH Resource Center Grant RR 11623.

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