On the repair of sub-lethal damage in V79 Chinease hamster cells resulting from irradiation with fast neutrons or fast neutrons combined with X-rays.
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Animals↗
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Study on the biological effect of fast neutrons 1. Effect of fast neutrons on germinability of barley seeds and on the chlorophyll content of the seedlings according to the dose used.
Barley seeds were irradiated in the active zone of the reactor at 500 watt, at favourable flux of fast neutrons in the dose interval of 823--2144 rad. Seeds after irradiation were "cooled" for 48 hours, then germinated, and the length of shoots of the seven days old seedings was measured. The value of the half lethal dose is 1130 rad, estimated from the growth curve. There is a well-defined relation of chlorophyll content (calculated for fresh weight unit) to the dose used. It was concluded from the phenotype of the leaves that the decrease of chlorophyll content was due first of all to the presence of chlorophyll-less cells and cell lines and not to the decrease of chlorophyll content of the individual cells. Irradiation yielded genetically defected cells.
Chlorophyll↗
DNA radiolysis by fast neutrons.
The effects of fast neutron irradiation on DNA were studied using DNA of the pBR322 plasmid (4362 base pairs), and the results compared to those obtained with 60Co gamma rays. Irradiation of the plasmid DNA in solution with a neutrons beam (p34+Be) of the CERI (CNRS Orléans) cyclotron (with a flat energy spectrum from 34 MeV to low energies) results in half the yield of single-strand breaks (ssb), and 1.5 times higher yield of double-strand breaks (dsb) for neutrons as compared to gamma-rays. Possible specificity of the neutron-induced breaks was examined: the scavenging of OH. radicals by 0.1 mol dm-3 ethanol inhibits all neutron-induced ssb, but only 85 per cent of the dsb. For gamma-irradiation, both ssb and dsb are completely inhibited in these conditions. These results suggest at least three different origins for neutron-induced dsb. The occurrence of around 30 per cent of dsb can be explained by a radical transfer mechanism (proposed by Siddiqi and Bothe (1987) for gamma-irradiation). Around 55 per cent of dsb may be due to the non-random distribution of radicals in high-density tracks of the secondary particles of neutrons, which results in a simultaneous attack of the two strands by OH. radicals. These first two processes are both OH.-mediated and thus are sensitive to ethanol. The direct effect of fast neutrons and their secondaries (recoil protons, alpha-particles and recoil nuclei) can account for the remaining 15 per cent of dsb, not inhibited by 0.1 mol dm-3 ethanol.
Cobalt Radioisotopes↗
An historical survey of radiobiology and radiotherapy with fast neutrons.
The treatment of cancer using fast neutrons was first attempted from 1938 to 1942, only a few years after the identification of the particle in 1932. The radiobiological information which was available at that time was both inadequate and contradictory, and provided no definite rationale for using neutrons in preference to X-rays. The doses given were often too high, causing many patients to suffer severe late reactions. As a result, further attempts to use fast neutrons in radiotherapy were abandoned for nearly 30 years. Interest in the use of fast neutrons was stimulated again by the elucidation of the oxygen effect and the discovery that it was less for neutrons than for X-rays. Thus tumours containing hypoxic cells would be less protected against neutrons. Also the reduced repair of sublethal damage with neutrons provided at least a partial explanation of the miscalculation of dose in the early trial. This was confirmed by means of a series of experiments on pig skin, from which it was also concluded that late damage was not more severe after neutrons, compared with X-rays for a given degree of early damage. A new clinical trial began in 1966, and the results so far are encouraging. In order to relate radiotherapy experience with X-rays to neutrons, it is necessary to measure the relative biological effectiveness (RBE) of neutrons. This has been done for skin of man, pig, mouse and rat. Because of the smaller recovery from sublethal damage after neutrons, the RBE increases as the dose per fraction decreases, but the relationship between RBE and dose per fraction is the same for all four species. Similar information, but only for rodents, has been obtained for a variety of other normal tissues with both cyclotron-produced and monoenergetic 14 or 15 meV neutrons. Experiments with animal tumours have indicated that there might be a wide variation in RBE from tumour to tumour due both to the presence of hypoxic cells and to differences in their capacities to recover from sublethal damage after X-rays and neutrons. The largest series of experiments on one tumour shows that whereas certain fractionation techniques with X-rays may produce a poor tumour response for a given level of normal tissue damage, all the neutron regimes produced a similar, close to optimum result. There is no evidence from which to expect any special dangers from neutron irradiation, and their likely advantage is that they may provide a more reliable method of radiotherapy as well as sterilizing some tumours which are normally resistant to X-rays.
Animals↗
[Neutron therapy in the G.D.R. Fundamentals of fast neutron application in radiation treatment (author's transl)].
In 1972 GDR started with the treatment of tumor patients with fast neutrons on the base of oxygen-effect. That means a better sensitivity of radiation of anoxic cells against radiation with high LET in comparison to radiation of thin ionization. Every tumor contains some anoxic cells. Therefore a better effect is possible with doses that are tolerated by normal tissue. In the following the details of the problems are discussed.
Anaerobiosis↗
Transfer dosemeters for fast neutron sources.
The increasing use of fast neutron sources in radiobiology, radiotherapy, etc. makes dosimetry intercomparisons (intercalibrations) by mail desirable. After comparing the relative advantages and disadvantages of the various available integrating fast neutron detectors, fission fragment track etching was chosen because such detectors can be made sufficiently small, rugged, fading resistant, inexpensive and accurate. Using several combinations of 232Th or 237Np as fissile materials, and organic and inorganic track detectors, it was established that both automatic spark counting and visual track counting techniques can be developed to cover the desirable dose range (approximately 50-500 rad) with sufficient accuracy (sigma less than or equal to 5%). One possible source of errors is the overlapping size distributions of fission fragment and recoil particle tracks in organic foils exposed at high neutron energies. Several approaches to reduce this problem are discussed.
Fast Neutrons↗
A new polycarbonate fast neutron personnel dosimeter.
Registration of fast-neutron-induced recoil and (n,alpha) tracks directly in sensitive polymers especially polycarbonate foils when etched by the electrochemical etching (ECE) method provides a simple, sensitive, and inexpensive means of fast neutron dosimetry. The wide dose range and a dose equivalent response, negligible fading rate, and insensitivity to X, beta, and gamma radiations make such a method feasible for many neutron dosimetry applications, especially personnel dosimetry. Due to very large size of the tracks, even the unaided eye can be used as a reading device.
Carbonates↗
Cytogenetic effect of 235U neutrons and d(50)+Be fast neutrons.
Induction of chromosome aberrations in G0 lymphocytes of peripheral human blood exposed to 235U and d(50)+Be neutron radiation was studied. Dose--effect relationships for different types of chromosome aberrations were analyzed. Linear dependence of the effect was established for the studied neutron radiation, except for the yield of dicentrics exposed to d(50)+Be neutrons. Accordingly to the yield of dicentrics, the relative biological efficiency (RBE) of 235U and d(50)+Be neutrons was 19.5 and 4.14, respectively.
Beryllium↗
Accelerated fast neutron therapy: a pilot study.
The clinical role of fast neutron therapy has been limited by excessive late normal tissue damage. A pilot study of accelerated fractionation of fast neutron therapy was performed, based on the rationale that this should result in an increase in the response in acute reacting tissues (normal and malignant), with no change in late damage and a consequent increase in the therapeutic ratio. Further accelerated fractionation should improve the local control of rapidly proliferating tumour, without the potential problem of inadequate reoxygenation inherent in accelerated photon schedules. 6 or 12 fractions of 62 MeV (p-Be) neutrons were given over 12 days to 27 sites in 23 patients with locally advanced tumours. With a dose reduction of 12% (18 Gy), acceptable skin and oral mucosa early reactions were obtained. A larger dose reduction (15%) was required at pelvic sites. The incidence of late EORTC/RTOG grade 4 toxicity was 46%. The overall response rate was 76% with a complete response rate of 16%. For locally advanced breast cancer, the complete response rate was 9%, which compares unfavourably with previous results with conventional neutron fractionation schedules. The combination of a low overall complete response rate and excessive late normal tissue toxicity suggests that accelerated fractionation of fast neutrons does not lead to an improvement in the therapeutic ratio, and that late normal tissue damage will continue to be dose limiting.
Adult↗
Basic radiobiological investigations of fast neutrons.
The radiobiological properties of a cyclotron-produced 43-MeV (p----Be) fast-neutron beam relative to gamma rays have been investigated using Chinese hamster V79 cells in culture. As expected, the relative biological effectiveness (RBE) of this neutron beam for cell killing was shown to increase as dose decreased, and the effectiveness per unit dose was slightly less compared to a 25-MeV (d----Be) neutron beam. By tracing single cells that formed microcolonies after irradiation, we found cell proliferation kinetics to be retarded to a greater extent by fast neutrons than by gamma irradiation. Following either neutron or gamma irradiation, a fraction of the irradiated cells failed to divide in the first postirradiation division and another fraction could produce as many as four generations of progeny before proliferation stopped. The properties of these cells presumed to be destined for death suggest that more than one mechanism and/or multistep process underlies the radiation-induced proliferative death. The fast-neutron beam was also found to be more effective quantitatively than gamma rays in producing DNA double-strand breaks (DSBs, measured by nondenaturing filter elution), and G1-phase chromosome fragments (measured by the premature chromosome condensation technique). However, the reverse was observed for DNA single-strand breaks (SSBs, measured by alkaline filter elution or hydroxylapatite uncoiling). Interestingly, both fast neutrons and gamma rays produced a large component of SSBs and DSBs with a fast-rejoining time constant of about 2-5 min, which appears to be independent of dose. The latter results could not resolve the possibility of lengthening the repair-time constant by increasing radiation dose within the range that is reflected by the shoulder of the survival curve, and consequently did not support the idea of repair saturation as a mechanism for the presence of the shoulder. The RBE for the hypoxanthine phosphoribosyl transferase mutation frequency per survivor at the 10% survival level was estimated to be 2.5, a value that is comparable to the RBE (2.1) for cell killing at the same survival level. Although most of the above-mentioned findings are compatible qualitatively with the relatively high-LET (linear energy transfer) nature associated with the fast-neutron beam, the significance of the action attributable to the mixture of LET could not be delineated in these experiments. Further, the biological significance of DSBs and chromosome aberration and the molecular mechanisms responsible for the repair and expression of these damaging processes remain to be elucidated.
Animals↗
The role of fast neutrons in radiooncology--a critical appraisal.
The contribution of fast neutrons to local tumour control has been investigated worldwide since the mid-60's in more than 20 institutions. The high expectations anticipated from the promising results of experimental studies could not be adequately realized in the clinic. The late normal tissue damage was unacceptable due to poor depth dose characteristics and further technical limitations of the first generation low-energy machines. Even with sophisticated therapy planning systems and high-energy cyclotrons as well as comparable late normal tissue damage as witnessed after photons, only a few tumour entities have responded superiorly to fast neutrons. These particularly include macroscopic tumours of the salivary glands, prostate and, potentially, soft and osseous tissues. The role of fast neutrons for head and neck cancer has not yet been definitely proved. For bladder-, cervical- and rectal carcinomas, non-small cell lung-, pancreatic- and breast cancers as well as malignant gliomas, no therapeutic benefit as compared with photons was observed in the case of macroscopic residual or inoperable recurrent tumours.
Aged↗
Morphologic effects of fast neutrons or photons on the canine kidney.
Thirty-nine adult male Beagles received either fast neutron or photon irradiation to the right thorax to determine the relative biological effectiveness of fast neutrons on normal pulmonary tissue. The right anterior abdomen, including the cranial half of the right kidney, was included in the field of irradiation. Twenty-four dogs (six/group) received fast neutrons with an average energy of 15 MeV to total doses of 1000, 1500, 2250, or 3375 cGy in four fractions per week for 6 weeks. Fifteen dogs received 3000, 4500, or 6750 cGy of photons (five/group) in an identical fractionation pattern. All 12 neutron irradiated dogs receiving 3375 and 2250 cGy and 1 of 6 receiving 1500 cGy, developed clinical and clinical pathologic signs of hepatic, pancreatic, and gastrointestinal disturbances, but no signs of renal injury were seen. These 13 dogs died or were euthanatized 47-367 days after irradiation. Only 1 of 5 dogs receiving 6750 cGy of photons developed similar signs and died 708 days post-irradiation. The remaining 11 neutron irradiated dogs and 14 photon irradiated dogs eventually died of other causes. All 39 dogs were necropsied and their kidneys were compared to each other and to control dogs. Radiation induced lesions included hemorrhages, necrosis and disappearance of tubular epithelia, glomerulosclerosis, atrophy and fibrosis. These lesions were associated with degenerative and occlusive vascular changes and were much more severe in the neutron irradiated dogs. The relative biologic effectiveness of fast neutrons for canine kidney assessed by gross and microscopic pathology is approximately 4.5 (6750/1500).
Animals↗
Response of the rat Dunning R3327-AT1 prostate tumor to treatment with fractionated fast neutrons.
Reports indicate that cancer of the prostate, soft tissue sarcomas, salivary gland tumors, and melanomas respond well to fast-neutron treatment. To better understand the action of fast neutrons on such tumor tissues, we have begun studies with the versatile Dunning rat prostate tumor system. In our initial studies with the R3327-AT1 subline we observed a relative biological effectiveness (RBE) of approximately 3 for single doses of 14-meV fast neutrons. As a continuation of those studies the present report discusses our findings following fractionated treatments with 10 equal fractions of 14-MeV fast neutrons or 60Co gamma rays at several dose levels per fraction. After either fractionated neutron or photon treatment the volume of the tumors continued to increase for 2 weeks and then reached a plateau, the level of which was dose dependent. Tumor growth resumed and no local control was observed. Analysis of the data using growth delay as biological end point yielded an RBE of approximately 4.2 +/- 1.3.
Animals↗
Fractionated dose of 35-MEV fast neutrons and hypoxic tumor cell survival curve.
The determination of the RBE for the MANTA fast neutrons produced by NRL is inprogress, with the model system using tumor cell population kinetic response patterns assayed in vitro after irradiation in vivo. Ascites tumor cells BW-5147 were irradiated with a clinically usable fast neutron beam from the NRL cyclotron, which is produced by accelrating deuterons to 35 MeV and using htem to bombard a thick berylliumtarget. The comparison of dose-effect relationships was made for doses ranging from30 to 1000 rads. The doses required for an isoeffect on BW-5147 hypoxic tumor cell survival and impairment of its reproductive capacity from fast neutron exposure were not different wheither it was given a single dose or the same dose given in three fractions separated by long recovery periods in situ. No intracellular repair of sublethal injury when the dose was given in three fractions, although the hypoxic BWp5147 tumor cells haveno effective reoxygenation or repopulation in this time interval. The RBE for the fast neutron beam is 4 relative to x rays for fractionated doses at the surviving fractionlevel of 0.6-0.7, while the RBE IS 2.5 FOR SINGLE DOSES. However, at a surviving fraction of 0.1, the RBE is 1.9 for single and 2.8 for fractionated doses. Analysis of thedaily cell population rate or mitotic delay between the two types of radiations at a similiar level of survival.
Animals↗
A thermoluminescent fast-neutron dosemeter based on pellets of CaSO4: Dy mixed with sulphur.
The fast neutron activation reaction 32S(n, p) 32P in CaSO4: Dy has been used in the measurements of fast neutron dose by employing a post-irradiation TL accumulation method. In order to increase the efficiency of the method CaSO4: Dy powder was mixed with sulphur powder in various proportions from which pellets weighing each were made. After neutron irradiation these pellets were each burnt in an aluminium planchette and the phosphor residue with 32P beta activity on it was allowed to undergo self-irradiation for TL accumulation. The fast neutron efficiency of the system employing 10 pellets of 0.1% CaSO4: Dy was found to be about 100 times that of bare CaSO4: Dy powder.
Calcium↗
The relative biological effectiveness of fractionated doses of fast neutrons (42 MeVd----Be) for normal tissues in the pig. IV. Effects on renal function.
The effects of fractionated doses of fast neutrons (42 MeVd----Be) on the radiation response of the pig kidney have been assessed and compared with those observed after X irradiation. Following X irradiation there was a marked increase in the total dose at which renal function was preserved with decreasing fraction size. The rate of this increase was dependent on the overall treatment time; for fractionated irradiation given over 18 or 39 days the exponents related to fraction number, N, were 0.36 +/- 0.03 and 0.48 +/- 0.003, respectively. In contrast, there was no significant change in the iso-effect dose for renal injury following fractionated irradiation with fast neutrons where there was also little effect of varying the overall treatment time. Analysing these data by means of the linear-quadratic (LQ) model, using both an Fe-plot and the Tucker test, gave alpha/beta ratios of 2.42 +/- 0.06 Gy and 2.99 +/- 0.16 Gy, respectively, for X-ray doses given in 18 days. For fractionated doses of X rays given in 39 days the alpha/beta ratios were 0.40 +/- 0.01 Gy and 0.47 +/- 0.02 Gy, respectively. The alpha/beta ratios for renal tissue following fast neutron irradiation obtained by the two methods were also similar, i.e. 15.00 +/- 0.60 Gy and 15.72 +/- 3.76 Gy, respectively. The pronounced fractionation effect seen with X irradiation, particularly for doses administered over 39 days as opposed to 18 days, coupled with the absence of any such effect with fast neutrons, resulted in a marked increase in relative biological effectiveness (RBE) with decreasing X-ray dose/fraction. The slopes of the resulting regression lines were -0.73 +/- 0.05 and -0.33 +/- 0.02, respectively. The lack of dose sparing associated with fractionation, or variation of the overall treatment time for fast neutron irradiation, suggests that doses administered to tumours adjacent to the kidney can be given as a few relatively large dose/fractions in a short overall treatment time without an increased risk of complications related to renal tissue. This may be of therapeutic advantage in the treatment of rapidly proliferating tumours where dose may be wasted using more conventional protracted fractionated irradiation schedules.
Animals↗
Preimplantation growth delay and micronucleus formation after in vivo exposure of mouse zygotes to fast neutrons.
Mouse zygotes were irradiated with fast neutrons (0.06 to 1.00 Gy) 1 h after conception and examined at various intervals (24 to 100 h after conception) for embryonic development and micronucleus formation. The frequency of micronuclei per cell increased linearly with dose in 2-cell embryos observed at 24 h after conception and in 4-cell and 8-cell embryos at 48 h after conception. Compared with X rays, the relative biological effectiveness of neutrons for the induction of micronuclei per embryo was 2.5 at 24 h after conception and 3.5 at 48 h after conception. Neutron-induced micronucleus formation was accompanied by morphological growth delay and a significant decrease in the number of cells in the embryos. An inverse relationship was found between the number of cells in embryos and the number of micronuclei when observed at 48 h after conception following irradiation with 0.12 to 1.00 Gy and at 78 h after conception following exposure to 0.50 Gy. The effect of neutron irradiation on embryonic development was likely to be mediated by cell death, as suggested by a significantly increased dead cell index in blastocysts following irradiation of zygotes.
Animals↗
Fast neutrons from a 25-MeV betatron.
Since published results for the fast-neutron dose per x-ray rad from high-energy therapy installations have differed by as much as a factor of 300, we have measured the neutron production from our 25-MeV betatron. Fast-neutron activation of aluminum foils was the method used. The effect of photoneutron production in the detectors, which has affected some past work, has been eliminated. A major source of neutrons in the treatment field was the platinum target. The neutron spectra used in the calculations of fluence were obtained by interpolation between published energies and between neighboring elements. Fluences per rad of x rays without a phantom were largely independent of field size and energy in the range 18-23 MeV. At 100 cm SSD and 23 MeV a large beam flattener contributed 15% of the neutrons, the remainder coming equally from the target and background. A phantom increased the neutron fluence/rad of x rays by 0%-10% depending on the field size. At 23 MeV we estimated the neutron dose to a patient to be 2.2 X 10(-4) rad per rad of x rays inside the treatment field and 3 X 10(-5) at 20 cm outside the field. The uncertainty in these figures is believed to be +/- 50%. In the electron beam the neutron dose per rad was about 50 times smaller than in the x-ray beam. Estimates were made of neutron fluences at other energies and target thicknesses. We discuss our results in comparison with those of others.
Fast Neutrons↗