Iodine-125 decay in a synthetic oligodeoxynucleotide. I. Fragment size distribution and evaluation of breakage probability

Lobachevsky, P. N. and Martin, R. F. Iodine-125 Decay in a Synthetic Oligodeoxynucleotide. I. Fragment Size Distribution and Evaluation of Breakage Probability. Incorporation of (125)I-dC into a defined location of a double-stranded oligodeoxynucleotide was used to investigate DNA breaks arising from decay of the Auger electron-emitting isotope. Samples of the oligodeoxynucleotide were also labeled with (32)P at either the 5' or 3' end of either the (125)I-dC-containing (so-called top) or opposite (bottom) strand and incubated in 20 mM phosphate buffer or the same buffer plus 2 M dimethylsulfoxide at 4 degrees C during 18-20 days. The (32)P-end-labeled fragments produced by (125)I decays were separated on denaturing polyacrylamide gels, and the (32)P activity in each fragment was determined by scintillation counting after elution of fragments from the gel. The relative fragment size distributions were then normalized on a per decay basis and converted to a distribution of single-strand break probabilities as a function of distance from the (125)I-dC. The results of three to five experiments for each of eight possible combinations of labels and incubation conditions are presented as a table showing the relative numbers of (32)P counts in different fragments as well as graphs of normalized fragment size distributions and probabilities of breakage. The average numbers of single-strand breaks per (125)I decay are 3. 3 and 3.7 in the top strand and 1.3 and 1.5 in the bottom strand with and without dimethylsulfoxide, respectively. Every (125)I decay event produces a break in the top strand, and breakage of the bottom strand occurs in 75-80% of the events. Thus a double-strand break is produced by (125)I decay with a probability of approximately 0.8.     

DNA breakage by decay of Auger electron emitters: experiments with 123I-iodoHoechst 33258 and plasmid DNA

The Auger electron-emitting isotope 123I is of interest in the context of potential exploitation of Auger electron emitters in radioimmunotherapy. The efficiency of induction of cytotoxic lesions by decay of DNA-associated 125I, the prototype Auger electron emitter, is well established, but its long half-life (60 days) is a limitation. However, the advantage of the much shorter half-life of 123I (13.2 h) might be outweighed by its "weaker" Auger electron cascade with an average of 8-11 Auger electrons, compared to about 15-21 electrons for 125I. Accordingly, the efficiency of DNA breakage for DNA-associated 123I was investigated by incubation of 123I-iodoHoechst 33258 with plasmid DNA. The efficiency of double-strand break induction by decay of 123I was 0.62 compared to 0.82 per decay of 125I in the same experimental system. In the presence of dimethylsulfoxide, the values were 0.54 and 0.65 for decay of 123I and 125I, respectively. The results also showed that at a very low ligand/plasmid molar ratio (<1), the majority of cleavage seemed to occur at a particular site on the plasmid molecule, indicating preferential binding of the 123I-ligand to a unique site or a cluster of neighboring sites.     

Plasmid DNA breakage by decay of DNA-associated Auger electron emitters: approaches to analysis of experimental data

Plasmid DNA is a popular substrate for the assay of DNA strand breakage by a variety of agents. The use of the plasmid assay relies on the assumption that individual damaging events occur at random, which allows the application of Poisson statistics. This assumption is not valid in the case of damage arising from decay of DNA-associated Auger electron emitters, since a single decay event can generate a few breaks in the same DNA strand, which is indistinguishable from a single break in the assay. The consequent analytical difficulties are overcome by considering relaxation events rather than single-strand breaks, and linearization events rather than double-strand breaks. A further consideration is that apart from damage at the site of DNA-associated decay, which is the principal interest of the analysis, some DNA damage also arises from the radiation field created by all decay events. These two components of damage are referred to as internal and external breakage, respectively, and they can be separated in the analysis since their contribution depends on the experimental conditions. The DNA-binding ligand Hoechst 33258 labeled with 125I was used in our experiments to study breakage in pBR322 plasmid DNA arising from the decay of this Auger electron emitter. The values obtained for the efficiency (per decay) of plasmid relaxation and linearization by the 125I-labeled ligand were 0.090 +/- 0.035 and 0.82 +/- 0.04, respectively. When dimethylsulfoxide was included as a radical scavenger, the efficiency values for relaxation and linearization were 0.15 +/- 0.02 and 0.65 +/- 0.05, respectively.     

Biological damage from the Auger effect,possible benefits

Summary Decay of radioactive isotopes by K-capture leads to the Auger effect and results in the loss of several orbital electrons and the emission of X-rays. Whereas radiation effects are produced from the emitted electrons, the consequences of the Auger effect are strictly localized to the site of the decaying nuclide.The paper reviews the biological consequences of the decay of¹²⁵I which produces the Auger effect. Nearly all data were obtained from DNA labeled with¹²⁵I-5-iodo-2-deoxyuridine (IUdR) in bacteria and mammalian cells. Parameters of effects were cell death, DNA strand breaks, and mutation induction. In order to recognize in a cell the contribution from the Auger effect and that of absorbed radiation, experimental data are analysed in terms of the specific energy for the nuclear volume which contains the isotope.The data indicate that decay of¹²⁵I is far more toxic than is expected on the basis of absorbed dose to the labeled nucleus. Moreover, it is emphasized that the toxicity of the¹²⁵I decay is largely determined by events immediately localized to the site of decay.Because the consequences of the Auger effect are strictly localized to the molecular site of the decay,¹²⁵I and perhaps other nuclides decaying by K-capture promise to be interesting tools in cell biology and molecular biology. First data on the Auger effect as a tool are summarized.It appears that recognizable biological damage is only observed when the Auger effect takes place in vitally important molecules, an example of which is DNA.Dedicated to Prof. Dr. H. Muth on the occasion of his 60th birthday.     

A Monte Carlo simulation of Auger cascades

The energy imparted to biological tissue after the decay of incorporated Auger emitters stems from two sources: (a) energy deposition by the Auger and Coster-Kronig electrons and (b) the charge potential which remains on the multiple ionized atom after the end of the cascade. For the numerical assessment of both the kinetic energy of the released electrons and the charge potential, a new and--for purposes of microdosimetry--precise method is presented. Based on relativistic Dirac-Fock calculations and a rigorous bookkeeping, this method provides a perfect energy balance of the considered atomic system when applied to Monte Carlo simulations of Auger cascades. By comparing the results for charge distribution for krypton and iodine with experimental data and the electron spectrum of 125I with theoretical data, it can be shown that the approach followed in this work is reasonable and appropriate for the determination of the energy deposited by incorporated Auger emitters in small volumes of condensed matter. The total energy deposited by 125I in a volume of 20-nm diameter is 2.03 keV which is made up by multiple ionization (1.07 keV) and energy deposition by the emitted Auger electrons (0.96 keV).     

Auger electron-induced double-strand breaks depend on DNA topology

From a structural perspective, the factors controlling and the mechanisms underlying the toxic effects of ionizing radiation remain elusive. We have studied the consequences of superhelical/torsional stress on the magnitude and mechanism of DSBs induced by low-energy, short-range, high-LET Auger electrons emitted by (125)I, targeted to plasmid DNA by m-[(125)I]iodo-p-ethoxyHoechst 33342 ((125)IEH). DSB yields per (125)I decay for torsionally relaxed nicked (relaxed circular) and linear DNA (1.74+/-0.11 and 1.62+/-0.07, respectively) are approximately threefold higher than that for torsionally strained supercoiled DNA (0.52+/-0.02), despite the same affinity of all forms for (125)IEH. In the presence of DMSO, the DSB yield for the supercoiled form remains unchanged, whereas that for nicked and linear forms decreases to 1.05+/-0.07 and 0.76+/-0.03 per (125)I decay, respectively. DSBs in supercoiled DNA therefore result exclusively from direct mechanisms, and those in nicked and linear DNA, additionally, from hydroxyl radical-mediated indirect effects. Iodine-125 decays produce hydroxyl radicals along the tracks of Auger electrons in small isolated pockets around the decay site. We propose that relaxation of superhelical stress after radical attack could move a single-strand break lesion away from these pockets, thereby preventing further breaks in the complementary strand that could lead to DSBs.     

Site-specific strand breaks in RNA produced by (125)I radiodecay

Decay of ¹²⁵I produces a shower of low energy electrons (Auger electrons) that cause strand breaks in DNA in a distance-dependent manner with 90% of the breaks located within 10 bp from the decay site. We studied strand breaks in RNA molecules produced by decay of ¹²⁵I incorporated into complementary DNA oligonucleotides forming RNA/DNA duplexes with the target RNA. The frequencies and distribution of the breaks were unaffected by the presence of the free radical scavenger dimethyl sulfoxide (DMSO) or by freezing of the samples. Therefore, as was the case with DNA, most of the breaks in RNA were direct rather than caused by diffusible free radicals produced in water. The distribution of break frequencies at individual bases in RNA molecules is narrower, with a maximum shifted to the 3′-end with respect to the distribution of breaks in DNA molecules of the same sequence. This correlates with the distances from the radioiodine to the sugars of the corresponding bases in A-form (RNA/DNA duplex) and B-form (DNA/DNA duplex) DNA. Interestingly, when ¹²⁵I was located close to the end of the antisense DNA oligonucleotide, we observed breaks in RNA beyond the RNA/DNA duplex region. This was not the case for a control DNA/DNA hybrid of the same sequence. We assume that for the RNA there is an interaction between the RNA/DNA duplex region and the single-stranded RNA tail, and we propose a model for such an interaction. This report demonstrates that ¹²⁵I radioprobing of RNA could be a powerful method to study both local conformation and global folding of RNA molecules.     

A method of calculating initial DNA strand breakage following the decay of incorporated 125I

Two sources of individual Auger electron spectra and an electron track code were used with a simple model of the DNA to successfully simulate the single-strand DNA breakage measured by Martin and Haseltine (1981). The conditions of the calculation were then extended to examine patterns of single-strand breaks in both strands of the DNA duplex to score double-strand breaks. The occurrences of five types of break were scored. The total number of double-strand breaks (dsb) per decay at the site of the decay was 0.90 and 0.65 for the different Auger electron spectra. It was shown that for mammalian cells an additional source of double-strand breaks from low LET radiation added approximately 0.17 dsb/decay to each, giving a final total of 1.07 and 0.85 dsb/decay for mammalian cells depending on the electron spectrum. Further is is shown that the energy deposition in the DNA from the iodine decay is very complex, with a broad range of energy depositions and products. Even for a particular energy deposited in the DNA different types of strand break are produced. These are identified and their probabilities calculated.     

Strand breaks in plasmid DNA after positional changes of Auger electron-emitting iodine-125: direct compared to indirect effects.

To elucidate the nature and kinetics of DNA strand breaks caused by low-energy Auger electron emitters, we compared the yields of DNA breaks in supercoiled pUC19 DNA in the presence of the (.)OH scavenger dimethyl sulfoxide (DMSO) after the decay of (125)I (1) in proximity to DNA after minor-groove binding ((125)I-iodoHoechst 33342, (125)IH) and (2) at a distance from DNA ((125)I-iodoantipyrine, (125)IAP). DMSO is efficient at protecting supercoiled plasmid DNA from the decay of (125)I free in solution (dose modification factor, DMF = 59 +/- 4) and less effective when the (125)I decays occur close to DNA (DMF = 3.8 +/- 0.3). This difference is due mainly to the inability of DMSO to protect DNA from the double-strand breaks produced by groove-bound (125)I (DMF = 1.0 +/- 0.2). Additionally, the fragmentation of plasmid DNA beyond the production of single-strand and double-strand breaks that is seen after the decay of (125)IH and not (125)IAP (Kassis et al., Radiat. Res. 151, 167-176, 1999) cannot be modified by DMSO. These results demonstrate that the mechanisms underlying double-strand breaks caused by the decay of (125)IH differ in nature from those caused by the decay of (125)IAP.     

Radioprobing of DNA: distribution of DNA breaks produced by decay of 125I incorporated into a triplex-forming oligonucleotide correlates with geometry of the triplex.

The distribution of breaks produced in both strands of a DNA duplex by the decay of 125I carried by a triplex-forming DNA oligonucleotide was studied at single nucleotide resolution. The 125I atom was located in the C5 position of a single cytosine residue of an oligonucleotide designed to form a triple helix with the target sequence duplex. The majority of the breaks (90%) are located within 10 bp around the decay site. The addition of the free radical scavenger DMSO produces an insignificant effect on the yield and distribution of the breaks. These results suggest that the majority of these breaks are produced by the direct action of radiation and are not mediated by diffusible free radicals. The frequency of breaks in the purine strand was two times higher that in the pyrimidine strand. This asymmetry in the yield of breaks correlates with the geometry of this type of triplex; the C5 of the cytosine in the third strand is closer to the sugar-phosphate backbone of the purine strand. Moreover, study of molecular models shows that the yield of breaks at individual bases correlates with distance from the 125I decay site. We suggest the possible use of 125I decay as a probe for the structure of nucleic acids and nucleoprotein complexes.     

Simulation of <Superscript>125</Superscript>I decay in a synthetic oligodeoxynucleotide with normal and distorted geometry and the role of radiation and non-radiation actions

Within the track structure code PARTRAC, DNA strand break induction by direct and indirect radiation action was calculated for the E. coli catabolite gene activator protein (CAP) DNA complex with ¹²⁵I located at the position of the H₅ atom of the cytosine near the center. The shape of the resulting DNA fragment size distributions was found to be in reasonable agreement with corresponding experimental results. However, the calculated yield was considerably lower than the measured one. To study possible reasons for this, recently published experimental data on DNA strand breaks in a 41-mer synthetic oligodeoxynucleotide (oligoDNA) with incorporated ¹²⁵I were analyzed aiming at an evaluation of the non-radiation-related component due to the neutralization of the initially highly charged ^125mTe daughter ion. This was done by assuming that the differences between simulated radiation-induced distribution and the measured total fragment size distributions were due to the neutralization process. The neutralization effect defined in this way was found to dominate the strand breakage frequency within a range of 5–7 base pairs around the ¹²⁵I decay site on both strands. After implementing this neutralization effect derived from the oligoDNA analysis into the PARTRAC simulation for the CAP-DNA complex, the agreement of the calculated DNA fragment distributions with the corresponding experimental data was considerably improved. The results indicate that DNA conformation may be explored by incorporation of ¹²⁵I into the DNA, measurement of fragment size distributions, and comparison with simulation calculation for various hypothetical DNA models.     

The radiation dose to cells in vitro from intracellular indium-111

Most of the radionuclides used in nuclear medicine emit low energy Auger electrons following radioactive decay. These emissions, if intracellular, could irreparably damage the radiosensitive structures of the cell. The resulting radiation dose, which is a measure of biological damage in the affected cell, could be many times the average radiation dose to the associated organ. In this series of experiments, the radiation dose to the nucleus of a chinese hamster V79 cell was determined for the intracellular radiopharmaceutical 111indium-oxine. Assuming the cell nucleus to be the radiosensitive volume, the radiation dose would be primarily due to the low energy Auger electrons. A much smaller dose would be absorbed from the penetrating X- and gamma-rays and internal conversion electrons released from other radiolabelled cells in the culture. The radiation dose to the cell from the intranuclear decay of 111In was empirically established from cell survival studies to be 3.5 mGy/decay, using cobalt-60 as a reference radiation. The average dose to V79 cells from extracellular 111In (i.e., from 111In located outside the target cell) was calculated to be 5.8 pGy/decay. This suggests that for an intracellular radiopharmaceutical, the radiation dose of consequence would be delivered by the low energy Auger electrons. In contrast, Auger electrons from an extracellular radiopharmaceutical could not directly damage the cell nucleus and therefore would not contribute to the radiation dose.     

Induction and repair of double- and single-strand DNA breaks in bacteriophage lambda superinfecting Escherichia coli

Induction and repair of double- and single-strand DNA breaks have been measured after decays of 125I and 3H incorporated into the DNA and after external irradiation with 4 MeV electrons. For the decay experiments, cells of wild type Escherichia coli K-12 were superinfected with bacteriophage lambda DNA labelled with 5'-(125I)iodo-2'-deoxyuridine or with (methyl-3H)thymidine and frozen in liquid nitrogen. Aliquots were thawed at intervals and lysed at neutral pH, and the phage DNA was assayed for double- and single-strand breakage by neutral sucrose gradient centrifugation. The gradients used allowed measurements of both kinds of breaks in the same gradient. Decays of 125I induced 0.39 single-strand breaks per double-strand break. No repair of either break type could be detected. Each 3H disintegration caused 0.20 single-strand breaks and very few double-strand breaks. The single-strand breaks were rapidly rejoined after the cells were thawed. For irradiation with 4 MeV electrons, cells of wild type E. coli K-12 were superinfected with phage lambda and suspended in growth medium. Irradiation induced 42 single-strand breaks per double-strand break. The rates of break induction were 6.75 x 10(-14) (double-strand breaks) and 2.82 x 10(-12) (single-strand breaks) per rad and per dalton. The single-strand breaks were rapidly repaired upon incubation whereas the double-strand breaks seemed to remain unrepaired. It is concluded that double-strand breaks in superinfecting bacteriophage lambda DNA are repaired to a very small extent, if at all.     

Efficient mutation induction by 125I and 131I decays in DNA of human cells

To examine the role of radiation energy deposition in DNA on cellular effects, we investigated the ability of 125IdUrd and 131IdUrd to kill cells and induce mutations at the hprt locus. We employed human lymphoblastoid cells proficient (TK6) or deficient (SE30) in the ability to incorporate a thymidine analog into DNA by way of the thymidine kinase (TK) scavenger pathway. Iodine-125 releases a shower of low-energy Auger electrons upon decay which deposit most of their energy within 20 nm of the decay site, whereas 131I is a high-energy beta/gamma emitter that is generally considered to emit sparsely ionizing radiation. Although 125IdUrd incorporated into cellular DNA was very effective at producing toxic and mutagenic effects in TK6 cells, virtually no effect was seen in TK-deficient cells incubated with similar levels of 125IdUrd in the extracellular medium. In response to 131IdUrd treatment, 0.45 X 10(-6) mutants were induced per centigray dose deposited within the nucleus in TK-proficient cells, whereas few mutations were induced in TK-deficient cells at doses up to 38 cGy from 131I decays occurring in the medium. The differences in biological response between TK6 and SE30 cells cannot be explained by differential radiosensitivity or IdUrd sensitization of the cell lines involved. We conclude that both 125I and 131I decays occurring while incorporated into DNA are more effective at inducing cell killing and mutations in human cells than either nonincorporated decays or low-LET radiations. These results suggest that localized energy deposition is an important factor in producing biologically important damage by both of these isotopes, and that residual lesions following the decay of DNA-incorporated radioisotopes may contribute to the toxic and mutagenic effects observed in TK-proficient cells. Furthermore, they emphasize that certain beta/gamma-emitting isotopes such as 131I may be particularly hazardous when incorporated into DNA.     

Monte Carlo simulations and measurement of DNA damage from x-ray-triggered Auger cascades in iododeoxyuridine (IUdR)

We investigated the DNA damage from Auger electrons emitted from incorporated stable iodine (¹²⁷I), following photoelectric absorption of external x-rays. The effectiveness of the Auger electrons in producing DNA double-strand breaks (DSB) was determined theoretically, using Monte Carlo simulations of the radiation physics and chemistry, and was shown to be in reasonable agreement with DNA damage measured using the comet assay. The DSB yields were measured in CHO cells for ⁶⁰Co (as a non-Auger-promoting radiation) and for tungsten-filtered 100 kVp x-rays capable of producing Auger electron emission. The theoretical study showed that on average, 2.5 Auger electrons were emitted for N-shell orbital vacancies and up to 10 Auger electrons were emitted from L₁-shell vacancies. These Auger bursts produced approximately 0.03 DSB per N-shell vacancy and 0.3 DSB per K-shell or L-shell vacancy. The calculated yield of DSB from Auger cascades per unit dose (1 Gy) in water was approximately 1.7 for tungsten-filtered 100 kVp x-rays, assuming 20% IUdR substitution of thymidine. The comet assay yielded an experimental value of 3.6±1.6 per 1 Gy for the same conditions. The Monte Carlo simulations also demonstrated a high complexity of DSB produced by Auger cascades with virtually all DSB from inner shell orbitals (i.e. K, L shells) accompanied by compounded strand breakage and base damage, indicating a difficult lesion to repair. This finding agrees well with comet assay results of DNA repair, where an increase in the DSB yield in IUdR-sensitized cells was shown to persist after a time of 24 h. We conclude that Auger cascades in iodine produce a modest increase in the number of initial strand breaks of the order of 10% but the complex nature of these DSB makes them very difficult to repair or potentially prone to misrepair. The accentuated DNA damage may have major consequences for cell survival and may be exploitable in kilovoltage photon activation therapy (PAT) of tumors sensitized with iodine. Received: 23 October 2000 / Accepted: 26 March 2001     

Strand breaks in whole plasmid dna produced by the decay of (125)I in a triplex-forming oligonucleotide.

DNA strand breaks produced by the decay of (125)I positioned against a specific site in plasmid DNA via a triplex-forming oligonucleotide were studied both in the immediate vicinity of the site of the decay with a single nucleotide resolution and in the whole plasmid by measuring the percentages of supercoiled, open-circular and linear forms. The localized breaks are distributed within 10 bp in each direction from the decay site with maxima in both strands just opposite the (125)I-dC residue in the triplex-forming oligonucleotide. The distributions of breaks in the two DNA strands are almost symmetrical, in agreement with the geometry of the pyrimidine motif triplex. We found that about 25% of the double-strand breaks were located outside the 90-bp fragment containing the triplex-forming oligonucleotide binding sequence. The ratio of single- to double-strand breaks in the whole plasmid was 11 for bound triplex-forming oligonucleotide compared to 26 when the triplex-forming oligonucleotide was free in solution. The number of double-strand breaks per decay of (125)I was 0.46 for bound triplex-forming oligonucleotide and 0.17 for free triplex-forming oligonucleotide. Comparing the data on the localized damage and those for the whole plasmid, we concluded that, in addition to DNA breaks that are confined to a helical turn around the (125)I atom, the decay can produce breaks hundreds of base pairs away in the plasmid molecule. This linear plasmid molecule containing radiation-induced damage at a specific DNA site should be useful in studies of the molecular mechanisms of DNA repair.     

Inhibitory and stimulatory bystander effects are differentially induced by Iodine-125 and Iodine-123

The bystander effect, originating from cells irradiated in vitro, describes responses of surrounding cells not targeted by the radiation. Previously we demonstrated that the subcutaneous injection into nude mice of human adenocarcinoma LS174T cells lethally irradiated by Auger electrons from the decay of DNA-incorporated (125)I inhibits growth of co-injected LS174T cells (inhibitory bystander effect; Proc. Natl. Acad. Sci. USA 99, 13765-13770, 2002). We have repeated these studies using cells exposed to lethal doses of (123)I, an Auger electron emitter whose emission spectrum is identical to that of (125)I, and report herein that the decay of (123)I within tumor cell DNA stimulates the proliferation of neighboring unlabeled tumor cells growing subcutaneously in nude mice (stimulatory bystander effect). Similar inhibitory bystander effects ((125)I) and stimulatory bystander effects ((123)I) are obtained in vitro. Moreover, supernatants from cultures with (125)I-labeled cells are positive for tissue inhibitors of metalloproteinases (TIMP1 and TIMP2), and those from cultures with (123)I-labeled cells are positive for angiogenin. These findings call for the re-evaluation of current dosimetric approaches for the estimation of dose-response relationships in individuals after radiopharmaceutical administration or radiocontamination and demonstrate a need to adjust all "calculated" dose estimates by a dose modification factor (DMF), a radionuclide-specific constant that factors in hitherto not-so-well recognized biophysical processes.     

Detecting the DNA kinks in a DNA-CRP complex in solution with iodine-125 radioprobing.

Auger-electron-emitting radioisotopes such as 125I produce DNA strand breaks within nanometer range of the decay site. Here we analyze these breaks in order to study changes in DNA conformation upon binding with cyclic AMP receptor protein (CRP) in solution. The clear difference we found in break frequency in the CRP-DNA complex, as compared to the naked DNA duplex, correlates with the increased distances between the deoxyriboses and the radioiodine atom caused by the CRP-induced kink observed in the cocrystal. Thus, we demonstrate that 125I radioprobing can be used to study fine conformational changes of DNA within DNA-protein complexes.     

Interaction of measles virus vectors with Auger electron emitting radioisotopes

A recombinant measles virus (MV) expressing the sodium iodide symporter (NIS) is being considered for therapy of advanced multiple myeloma. Auger electrons selectively damage cells in which the isotope decays. We hypothesized that the Auger electron emitting isotope 125I can be used to control viral proliferation. MV was engineered to express both carcinoembryonic antigen and NIS (MV-NICE). Cells were infected with MV-NICE and exposed to 125I with appropriate controls. MV-NICE replication in vitro is inhibited by the selective uptake of 125I by cells expressing NIS. Auger electron damage is partly mediated by free radicals and abrogated by glutathione. In myeloma xenografts, control of MV-NICE with 125I was not possible under the conditions of the experiment. MV-NICE does not replicate faster in the presence of radiation. Auger electron emitting isotopes effectively stop propagation of MV vectors expressing NIS in vitro. Additional work is necessary to translate these observations in vivo.     

125I-induced DNA double strand breaks: use in calibration of the neutral filter elution technique and comparison with X-ray induced breaks

The neutral filter elution assay, for measurement of DNA double strand breakage, has been calibrated using mouse L cells and Chinese hamster V79 cells labelled with [125I]dUrd and then held at liquid nitrogen temperature to accumulate decays. The basis of the calibration is the observation that each 125I decay, occurring in DNA, produces a DNA double strand break. Linear relationships between 125I decays per cell and lethal lesions per cell (minus natural logarithm survival) and the level of elution, were found. Using the calibration data, it was calculated that the yield of DNA double strand breaks after X-irradiation of both cell types was from 6 to 9 X 10(-12) DNA double strand breaks per Gy per dalton of DNA, for doses greater than 6 Gy. Neutral filter elution and survival data for X-irradiated and 125I-labelled cells suggested that the relationships between lethal lesions and DNA double strand breakage were significantly different for both cell types. An attempt was made to study the repair kinetics for 125I-induced DNA double strand breaks, but was frustrated by the rapid DNA degradation which occurs in cells that have been killed by the freezing-thawing process.