Design of a cylindrical brachytherapy implant applicator for the irradiation of an intestinal segment in mice

YingExperimental determination of the RBE of new isotopes for brachytherapy implants (e.g. iodine-125 and palladium-103) remains a very difficult problem, especially in small animals, where the seeds cannot be implanted easily in the planned geometry in a reproducible way. This technical note describes an original device that makes it possible to irradiate a segment of the intestine in mice for the purpose of determining the RBE for crypt regeneration. The device is a length of tube (3.4 mm and 7 mm internal and external diameter, respectively) whose external surface has been longitudinally grooved and into which the seeds can be squeezed (each groove holds either one or two seeds). The tube is composed of two sections. This seed container can be surgically positioned around an intestinal ansa while the mice are anesthetized. The mean dose rates in the intestine (for eight seeds) were found to be 86.3 +/- 5.9 and 79.0 +/- 5.4 cGy/h for 29.2 MBq (1 U) iodine and 28.6 MBq (1 U) palladium seeds, respectively. So far, more than 100 mice have been irradiated successfully. Full dose-effect relationships can be obtained using the same seeds and applying them successively in different groups of animals (which ensured the accuracy of the relative doses).     

Effects of exposure to low-dose-rate (60)co gamma rays on human tumor cells in vitro

Cells of three asynchronously growing human tumor cell lines, PC3 (human prostate carcinoma), T98G and A7 (human glioblastomas), which have been shown previously to demonstrate low-dose hyper-radiosensitivity to low acute single doses, were irradiated with (60)Co gamma rays at low dose rates (2 cGy-1 Gy h(-1)). Instead of a dose-rate sparing response, these cell lines demonstrated an inverse dose-rate effect on cell survival at dose rates below 1 Gy h(-1), whereby a decrease in dose rate resulted in an increase in cell killing per unit dose. A hyper-radiosensitivity-negative cell line, U373MG, did not demonstrate an inverse dose-rate effect. Analysis of the cell cycle indicated that this inverse dose-rate effect was not due to accumulation of cells in G(2)/M phase or to other cell cycle perturbations. T98G cells in reversible G(1)-phase arrest also showed an inverse dose-rate effect at dose rates below 30 cGy h(-1) but a sparing effect as the dose rate was reduced from 60 to 30 cGy h(-1). We conclude that this inverse dose-rate effect in continuous exposures reflects the hyper-radiosensitivity seen in the same cell lines in response to very small acute single doses.     

Relative biological effectiveness and dose rate effect of tritiated water on chromosomes in human lymphocytes and bone marrow cells

Tritriated water (HTO) is a major toxic effluent from the nuclear power industry, that is released into the environment in large quantities. The low dose radiation effect and dose rate effect of HTO on human lymphocytes and bone marrow cells have not been well studied. The present study was therefore undertaken to investigate the HTO dose-response relationship for chromosomal aberrations in human lymphocytes and bone marrow cells at low in vitro radiation doses ranging from 0.1 to 1 Gy. Lymphocytes (G₀ stage) and bone marrow cells were incubated for 10–150 min with HTO at a dose rate of 2cGy/min (555 MBq/ml). The relative biological effectiveness (RBE) of HTO was calculated with respect to ₆₀Co γ-rays for the induction of dicentric and centric ring chromosomes at low radiation doses. The RBE value for HTO β-rays relative to ⁶⁰Co γ-rays was 2.7 for lymphocytes and 3.1 for chromatid aberrations in bone marrow cells. Lymphocytes were also chronically exposed to HTO for 6.7–80 h at dose rates of 0.5 cGy/min (138.5 MBq/ml) and 0.02 cGy/min (5.6 MBq/ml). There was a 71.5% decrease in the yield of dicentrics and centric rings at the dose rate of 0.02 cGy/min, indicating a clear dose rate effect of HTO. The RBE value for HTO relative to ¹³⁷Cs γ-rays was 2.0 at a dose rate of 0.02 cGy/min, suggesting that low HTO dose rates produce no increase of the RBE values and that the values may be constant between 2 and 3 within these dose rates. These results should prove useful in assessment of the health risk for humans exposed to low levels of HTO.     

Relative biological effectiveness of fission neutrons for induction of micronucleus formation in mouse reticulocytes in vivo

Following whole-body irradiation of ICR mice with various doses of fission neutrons or X-rays, the frequency of micronuclei (MNs) in peripheral blood reticulocytes was measured at 12 h intervals beginning immediately after irradiation and ending at 72 h after irradiation. The resulting time-course curve of MN frequency had a clear peak 36 h after irradiation, irrespective of the type of radiation applied and the dose used. The MN frequency, averaged as the unweighted mean over the experimental time course, showed a linear increase with increasing dose of either fission neutrons or X-rays. The linear response to X-rays supports reported conclusion that induction of MN formation in reticulocytes is a dose-rate independent phenomenon. The relative biological effectiveness (RBE) of fission neutrons to X-rays for MN induction was estimated to be 1.9 +/- 0.3. This value is considerably lower than the RBE value of 4.6 +/- 0.5 reported for the same fission neutrons for induction of lymphocyte apoptosis in the thymus of ICR mice that represents dose-rate independent, one-track event. Based on these results, we propose that MNs increased in reticulocytes after irradiation mostly represent acentric fragments caused by single chromosome breaks, and that some confounding factor is operating in erythroblasts for the formation of aberrations from non-rejoining DNA double-strand breaks more severely after high-LET radiation than after low-LET radiation.     

Response of a brachytherapy model using 125I in a murine tumor system

The effects of low-dose-rate irradiation (brachytherapy) were investigated in vivo using a murine mammary adenocarcinoma (MTG-B) growing in the flank of C3H mice. For local tumor irradiations, a noninvasive cap was devised to cover the tumor and house three 125I seeds (average apparent activity 5.2 mCi each) located at 120 degree intervals around the circumference of the hemispherical cap (13 mm i.d.). Mice were secured during treatment in a tube allowing limited mobility while restricting access to the seeds. Tumors were exposed to a series of dose rates ranging from 14-40 cGy/h, and the total dose over the treatment interval (48 or 72 h) ranged from 830 to 2378 cGy. A total of nine experiments were conducted using the caps over a 10-week interval. In each experiment three groups (irradiated tumors, sham controls, and untreated controls) were analyzed, each containing 8-15 mice (N = 34, untreated control; N = 46, sham control; N = 91, brachytherapy irradiation). The brachytherapy results are compared to the effects of external beam irradiation in the same tumor system. A linear relationship was observed between the total radiation dose and doubling volume growth delay (GDDV) or treatment volume growth delay (GDTV) for the brachytherapy and external beam irradiation. The slopes of the dose-response curves are steeper for the acute dose (517 cGy/min) external beam irradiation (0.0072 day/cGy, GDDV; 0.00695 day/cGy, GDTV) than for the brachytherapy (0.0050 day/cGy, GDDV; 0.0057 day/cGy, GDTV) using both GDTV and GDDV end points. Comparison of the tumor volume regrowth slopes indicates that the tumor bed effect is larger for external beam irradiation than for brachytherapy, suggesting that the tumor bed effect may be dose-rate dependent.     

RBE of the MIT epithermal neutron beam for crypt cell regeneration in mice

The RBE of the new MIT fission converter epithermal neutron capture therapy (NCT) beam has been determined using intestinal crypt regeneration in mice as the reference biological system. Female BALB/c mice were positioned separately at depths of 2.5 and 9.7 cm in a Lucite phantom where the measured total absorbed dose rates were 0.45 and 0.17 Gy/ min, respectively, and irradiated to the whole body with no boron present. The gamma-ray (low-LET) contributions to the total absorbed dose (low- + high-LET dose components) were 77% (2.5 cm) and 90% (9.7 cm), respectively. Control irradiations were performed with the same batch of animals using 6 MV photons at a dose rate of 0.83 Gy/min as the reference radiation. The data were consistent with there being a single RBE for each NCT beam relative to the reference 6 MV photon beam. Fitting the data according to the LQ model, the RBEs of the NCT beams were estimated as 1.50 +/- 0.04 and 1.03 +/- 0.03 at depths of 2.5 and 9.7 cm, respectively. An alternative parameterization of the LQ model considering the proportion of the high- and low-LET dose components yielded RBE values at a survival level corresponding to 20 crypts (16.7%) of 5.2 +/- 0.6 and 4.0 +/- 0.7 for the high-LET component (neutrons) at 2.5 and 9.7 cm, respectively. The two estimates are significantly different (P = 0.016). There was also some evidence to suggest that the shapes of the curves do differ somewhat for the different radiation sources. These discrepancies could be ascribed to differences in the mechanism of action, to dose-rate effects, or, more likely, to differential sampling of a more complex dose-response relationship.     

Effects of Continuous Low Dose-Rate Irradiation: Computer Simulations

Abstract. The effects of continuous low dose-rate irradiation are studied with a computer model that incorporates cell kinetics and the accumulation and repair of radiation damage. This theoretical approach independently explores the effects on survival curves of a phase block, inherited damage and proliferation by dying cells. the computer model is a Monte Carlo simulation which follows the evolution in time of the family trees of a growing cell population under continuous irradiation. the model uses as input the measured phase-specific survival curves for acute exposures and the cell kinetic parameters to generate survival curves for continous low dose-rate irradiations. Cell survival curves for Chinese hamster lung cells (V79) for dose rates ranging from 15 to 500 cGy/h have been generated using various model assumptions. the model shows that for these cells a G₂ block will maximize cell killing for an optimum dose rate near 75 cGy/h. the effect on survival curves of inherited damage, as well as that of the proliferation by dying cells, is shown to increase monotonically with decreasing dose rates, and to be quite large at low dose rates.     

Dose-rate effect on transgenerational mutation frequencies in spermatogonial stem cells of the medaka fish

The estimation of transgenerational genetic risk of radiation exposure to non-human species is crucial for the protection of ecosystems. Here we determined the frequency of specific-locus mutations at the five pigmentation loci in medaka spermatogonial stem cells after gamma irradiation at 0.03 cGy/min and 95 cGy/min. At each total dose, the mutation frequency was significantly lower in the 0.03-cGy/min group than in the 95-cGy/min group, suggesting a dose-rate effect. The ratio of the induced mutation frequency at 0.03 cGy/min to that at 95 cGy/min was approximately 0.42 from 0 to 1.9 Gy and approximately 0.33 from 1.9 to 4.75 cGy. In the mouse, this ratio is estimated to be 0.33 (Russell and Kelly, Proc. Natl. Acad. Sci. USA 79, 542-544, 1982). It is thus possible that the magnitude of the dose-rate effect on transgenerational mutation frequencies is comparable between mouse and medaka spermatogonia, suggesting similar dose-rate effects among vertebrates.     

Effects of continuous low dose-rate irradiation: computer simulations

The effects of continuous low dose-rate irradiation are studied with a computer model that incorporates cell kinetics and the accumulation and repair of radiation damage. This theoretical approach independently explores the effects on survival curves of a phase block, inherited damage and proliferation by dying cells. The computer model is a Monte Carlo simulation which follows the evolution in time of the family trees of a growing cell population under continuous irradiation. The model uses as input the measured phase-specific survival curves for acute exposures and the cell kinetic parameters to generate survival curves for continuous low dose-rate irradiations. Cell survival curves for Chinese hamster lung cells (V79) for dose rates ranging from 15 to 500 cGy/h have been generated using various model assumptions. The model shows that for these cells a G2 block will maximize cell killing for an optimum dose rate near 75 cGy/h. The effect on survival curves of inherited damage, as well as that of the proliferation by dying cells, is shown to increase monotonically with decreasing dose rates, and to be quite large at low dose rates.     

Lung tumour induction in mice after X-rays and neutrons

Dose-response curves were determined for pulmonary adenomas and adenocarcinomas in mice after single acute doses of 200 kVp X-rays and cyclotron neutrons (E = 7.5 MeV). A serial-killing experiment established that the radiation induces the tumours and does not merely accelerate the appearance of spontanoeus cancers [corrected]. The dose versus incidence (I) of tumours in male and female mice for X-ray doses between 0.25 and 7.5 Gy is 'bell-shaped' and best fitted with a purely quadratic induction and exponential inactivation terms, i.e. I = A + BD2e-alpha D. In contrast, the tumour dose-response after 0.1-4.0 Gy of neutrons is best fitted by I = A + BDe-alpha D and is steeply linear less than or equal to 1 Gy, peaks between 1 and 3 Gy and sharply declines at 4.0 Gy. The data for the female mice less than or equal to 1 Gy neutrons are best fitted to the square root of the dose. A major objective of the experiments was to derive neutron RBE values. Because of the differences between the X-ray (quadratic) and neutron (linear) curves, the RBEn will vary inversely with decreasing X-ray dose. The RBE values at 1 Gy of X-rays derived from the B coefficients in the above equations are 7.4 +/- 3.2 (male and female); 8.6 +/- 3.6 (female) and 4.7 +/- 1.8 (male). These are high values and imply even higher values at the doses of interest to radiation protection. If, however, one restricts the analysis to the initial, induction side of the response (less than or equal to 1 Gy neutrons, less than or equal to 3 Gy X-rays) then good linear fits are obtainable for both radiations and indicate neutron RBE values of 7.4 +/- 2.3 for female mice and 4.5 +/- 1.8 for males, and these are independent of dose level.     

A systemic model of the reproductive death of mammalian cells. The effect of radiation dose rate and fractionation

On the basis of the previously developed systemic model a study was made of the effect of dose rate on the survival of mammalian cells, RBE of small doses of heavy ions, and fractionation of radiation. There was a good agreement between theoretical and experimental results. The calculations showed that D10 (10% survival dose) is a function of dose rate P even for such ions as helium and boron which, however, exhibited an insignificant dependence of D10 on P (within the range from (10(-1) to 1 cGy/min). The influence of repair and the rate of cell division on RBE of radiation was determined.     

A linear analog of atrial natriuretic peptide (ANP) discriminates guanylate cyclase-coupled ANP receptors from non-coupled receptors

Atrial natriuretic peptide (ANP) contains a disulfide which is generally considered to be required for biological activity. A truncated linear ANP analog, des-Cys105,Cys121-ANP-(104-126) (referred to as analog I), that lacks the 2 cysteine residues of the parent peptide was synthesized. In competition binding studies using rabbit lung membranes, ANP-(103-126) and analog I displaced bound 125I-ANP-(103-126) from specific ANP binding sites 100 and 73%, respectively. The concentrations of ANP-(103-126) and analog I that produced 50% inhibition of radioligand binding to the membranes were 0.26 +/- 0.07 and 0.31 +/- 0.09 nM, respectively. Radioiodinated ANP-(103-126) and analog I were chemically cross-linked to binding sites on rabbit lung membranes, and the labeled membrane proteins were analyzed by sodium dodecyl sulfate-polyacrylamide gel electrophoresis and autoradiography. 125I-Analog I specifically labeled a 65,000-dalton protein and a 135,000-dalton protein which, under reducing conditions, dissociated into 65,000-dalton subunits. In contrast, 125I-ANP-(103-126) labeled specifically a nonreducible 135,000-dalton protein, in addition to the 65,000-dalton species and the reducible 135,000-dalton species. ANP-(103-126) (100 nM) stimulated rabbit lung particulate guanylate cyclase activity, whereas analog I, at the same concentration, had no effect on cyclic GMP production and did not antagonize the effect of ANP-(103-126). From these observations, we conclude that analog I is a selective ligand which binds to approximately 73% of the total ANP binding sites present in rabbit lung membranes. Unlike ANP-(103-126), analog I does not bind to the remaining 27% of the binding sites and does not activate guanylate cyclase. Binding to the cyclase-linked ANP receptor correlates with the specific labeling by 125I-ANP-(103-126) of the nonreducible 135,000-dalton membrane protein.     

Radiotoxicity of 5-[123I]iodo-2'-deoxyuridine in V79 cells: a comparison with 5-[125I]iodo-2'-deoxyuridine

The toxic effects of the short-lived (T 1/2 = 13.2 h) Auger-electron-emitting isotope 123I, incorporated in the form of 123IUdR into the DNA of V79 cells in vitro, have been investigated and compared to those of 125IUdR. For the concentrations tested, the rate of incorporation of 123IUdR at any time is proportional to the concentration of extracellular radioactivity. The curve for survival of clonogenic cells decreases exponentially and exhibits no shoulder at low doses. The mean lethal dose (D37) to the nucleus is 79 +/- 9 cGy and is about the same as that obtained previously with 125IUdR. However, the total number of decays needed to produce this D37 with 123IUdR is about twice that required with 125IUdR, approximately equal to the ratio of the energy deposited in microscopic volumes by 125I and 123I, respectively. This correlation suggests that nuclear recoil, electronic excitation, and chemical transmutation are probably of minor importance to the observed biological toxicity with either isotope. The results also indicate that there are no saturation effects in the decay of 125IUdR in the DNA of V79 cells (i.e., all of the emitted energy is biologically effective) and that each of the two steps involved in the 125I decay is equally effective in causing biological damage.     

Sensitization to radiation from an implanted 125I source by sustained intratumoral release of chemotherapeutic drugs

We have investigated tumor response to low-dose-rate irradiation from an implanted 125I source alone or in conjunction with intratumoral drug administration. The drug (cis-DDP or 5-FU) was incorporated homogeneously into the co-polymer CPP-SA, 20:80, and the polymer/drug rods were implanted in the RIF-1 fibrosarcomas growing subcutaneously in C3H mice. Twenty-four hours later, the tumor was implanted with an 125I seed. Tumor growth time was the end point in these experiments. For implanted 125I sources of different dose rates and implant times giving a range of total doses, a consistent dose-response relationship was shown between tumor growth time and total dose. In other experiments, 125I sources of different specific activities were implanted for periods of time adjusted so that the total dose to the tumor was always the same. When the 125I implant was combined with 5-FU, greater than additive responses were seen for both short (30 h) and long (96 h) 125I treatment times. In contrast, a short-duration (30 h) 125I implant combined with cis-DDP was the least effective treatment, giving a combined response that was no better than additive, whereas 96 h exposure to 125I combined with cis-DDP was the most effective combined treatment. It is conjectured that this inverse dose-rate effect seen when cis-DDP is combined with low-dose rate radiation is related to a cell cycle effect and/or to inhibition of repair of radiation damage by cis-DDP.     

Estimation of genetic effects of chronic exposure to low-dose rate gamma-radiation by cytogenetic methods and DNA-comet assay

The study of genetic effects in CBA/lac mice exposed for 1 year to constant low dose-rate gamma-radiation at a dose-rate 63 cGy/year has been carried out. We have shown the significant increase in the DNA breaks' level in spleen lymphocytes by comet-assay beginning from the total absorbed dose of 20 cGy. It is possible that the DNA breaks' level increase resulted from the structural rearrangement of chromatin or induction of lymphocyte proliferation. The results obtained by micronucleus test have proved that the mutagenic effect of chronic low dose-rate gamma-radiation depends on cell type and respectively on cell proliferation rate, cell differentiation, etc. So, by the end of experiment the significant increase in the frequency of PCE with micronuclei (MN) was observed. However, in contrast, the frequency of NCE with MN was not increased. No significant increase in the percent of lung cells with MN was registered.     

Dose responses for chromosome aberrations produced in noncycling primary human fibroblasts by alpha particles,and by gamma rays delivered at sublimiting low dose rates

As the total dose of X or gamma rays is delivered at lower and lower rates, the yield of chromosome aberrations progressively diminishes. Simultaneously, the shape of the dose response changes from one exhibiting pronounced upward curvature at high dose rates to one approaching linearity at low dose rates. Although the maximum sparing effect caused by lowering the dose rate can be predicted from classical cytogenetic theory, it has yet to be verified experimentally. Here, noncycling normal human fibroblasts were exposed to graded doses of (137)Cs gamma rays at chronic dose rates of 6.3 and 2.8 cGy h(-1), dose rates that we reasoned should be lower than those required to achieve maximal sparing. This was indeed shown to be the case, after it was determined that the two chronic dose rates produced identical linear dose responses of 0.05 total aberrations per cell Gy(-1). Consistent with cytogenetic theory, this value was statistically indistinguishable from the linear coefficient derived from a fit to aberration frequencies produced by high-dose-rate exposure. Exposure to (238)Pu alpha particles also produced a linear dose response for total aberrations, whose slope-with respect to (137)Cs gamma rays as a reference radiation-implied a maximum RBE of 35 +/- 2.     

Chromosome damage induced by decay of 3H and 125I incorporated into DNA of Chinese hamster cells

The present study was undertaken to compare the frequency of chromatid-type aberrations in Chinese hamster cells with previous results on accumulation of unrepaired DNA-strand breaks after incorporation of 3H-TdR or 125IUdR into DNA. A linear-quadratic function was fitted by the weighted-least-square method to the data on yield of chromatid aberrations at different dpm values. Based on a significant linear response at low doses, RBE for 125I in relation to 3H was calculated for (i) chromatid breaks (17 +/- 6), (ii) the sum of isochromatid breaks and chromatid exchanges (21 +/- 9), and (iii) the total number of chromatid aberrations (18 +/- 5). Analogously, the RBE for accumulation of DNA-strand breaks was determined (13 +/- 6). Our results are consistent with the assumption that chromosomal aberrations mainly originate from unrepaired DNA-strand breaks.     

Modulation of pharmacokinetics of radioiodinated sugar-conjugated somatostatin analogues by variation of peptide net charge and carbohydration chemistry

Sugar conjugation of biooactive peptides has been shown to be a powerful tool to modulate peptide pharmacokinetics. In the case of radiolabeled somatostatin analogues developed for in vivo scintigraphy of somatostatin receptor (sst) expressing tumors, it generally led to tracers with predominant renal excretion and low uptake in nontarget organs, and in some cases also with enhanced tumor accumulation. Especially with respect to endoradiotherapeutic applicability of these tracers, however, understanding the structural requirements for minimal kidney accumulation and maximal tumor uptake is important. The aim of this study was therefore the evaluation of the potential of specific glycoside structures in combination with reduced peptide net charge to reduce kidney accumulation without affecting tumor accumulation. Three glyco analogues of radioiodinated Tyr(3)-octreotate (TOCA) with z = 0 were evaluated in a comparative study using [(125)I]Mtr-TOCA (z = +1), the maltotriose-Amadori analogue of [(125)I]TOCA, as a reference, [(125)I]Glucuron-TOCA, the Amadori conjugate with glucuronic acid, and [(125)I]Gluc-S- and [(125)I]Gal-S-TOCA, the coupling products with glucosyl- and mannosyl-mercaptopropionate. In cells transfected with sst(1)-sst(5), all three new analogues show sst-subtype binding profiles similar to I-Mtr-TOCA with high, but somewhat reduced, affinity for sst(2). In contrast, internalization into sst(2)-expressing cells (in % of [(125)I]Tyr(3)-octreotide ([(125)I]TOC)) as well as the EC(50,R) of unlabeled TOC for internalization determined in dual-tracer experiments are substantially enhanced for [(123)I]Gal-S-TOCA and [(123)I]Gluc-S-TOCA (internalization, 190% +/- 12% and 265% +/- 20%, respectively, vs 168% +/- 6% of [(125)I]TOC for [(123)I]Mtr-TOCA; EC(50,R), 2.62 +/- 0.07 and 2.96 +/- 0.14, respectively, vs 1.81 +/- 0.07 for [(123)I]Mtr-TOCA). The tumor accumulation of [(125)I]Gal-S-TOCA and [(125)I]Gluc-S-TOCA in AR42J tumor-bearing nude mice 1 h p.i. is consequently very high (22.6 +/- 2.2 and 26.2 +/- 5.6%ID/g) and comparable to that of [(125)I]Mtr-TOCA (25.1 +/- 4.4%ID/g). [(125)I]Glucuron-TOCA showed lower uptake in sst-expressing tissues than did [(125)I]Mtr-TOCA, but considerably enhanced accumulation in nontarget organs such as liver, intestine, and kidney. Due to increased lipophilicity, hepatic and intestinal uptake 1 and 4 h p.i. of [(125)I]Gal-S-TOCA and [(125)I]Gluc-S-TOCA was also slightly higher than that of [(125)I]Mtr-TOCA. Kidney accumulation, however, was reduced by approximately 50% for both compounds (2.6 +/- 0.3 and 2.2 +/- 0.4, respectively, vs 4.0 +/- 0.7%ID/g at 1 h p.i.). Because no sugar-specific effect was detected in the latter case, it is concluded that general ligand pharmacokinetics and especially kidney accumulation of the tracers investigated are mainly determined by physicochemical characteristics such as lipophilicity, net charge, and also charge distribution ([(125)I]Glucuron-TOCA vs [(125)I]Gal-S- and [(125)I]Gluc-S-TOCA). With respect to receptor targeting, however, the structure of the carbohydrate moiety plays an important role, leading to dramatically enhanced ligand internalization, especially in the case of [(123)I]Gluc-S-TOCA. Taking into account the combined effects of the Gluc-S-moiety both on kidney and on tumor accumulation, this group seems to be a promising synthon for the synthesis of other radiolabeled peptide analogues with improved pharmacokinetics.     

Renal damage in the mouse: the effect of d(4)-Be neutrons

A further study on the response of the mouse kidney to d(4)-Be neutrons (EN = 2.3 MeV) is described. The results confirm and augment the work published previously by Stewart et al. [Br. J. Radiol. 57, 1009-1021 (1984)]; the present paper includes the data from a "top-up" design of experiment which extends the measurements of neutron RBE (relative to 240 kVp X rays) down to X-ray doses of 0.75 Gy per fraction. The mean RBE for these neutrons increases from 5.8 to 7.3 as X-ray dose per fraction decreases from 3.0 to 1.5 Gy in the kidney. This agrees with the predictions from the linear quadratic (LQ) model, based on the renal response to X-ray doses above 4 Gy per fraction. The mean RBE estimate from a single dose group at 0.75 Gy per fraction of X rays is, however, 3.9. This is below the LQ prediction and may indicate increasing X-ray sensitivity at low doses. Data from this study and from those published previously have been used to determine more accurately the shape of the underlying response to d(4)-Be neutrons; an alpha/beta ratio of 20.5 +/- 3.7 Gy was found. The best value of alpha/beta for X rays determined from these experiments was 3.04 +/- 0.35 Gy, in agreement with previous values.