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PubMed2002

Relative biological effectiveness of boron ions on human melanoma cells.

PURPOSE: To compare the difference in relative biological effectiveness (RBE) between (10)B ions and a (60)Co gamma-ray beam for human melanoma cells using in vitro cell survival based on a clonogenic assay. MATERIALS AND METHODS: Cells were irradiated in vitro under aerobic conditions with (60)Co and (10)B ions with different linear energy transfer (LET) (40, 80 and 160 eV nm(-1)). The dose to the cells was determined using ferrous sulphate dosimetry and an ionisation chamber. The standard linear-quadratic model and the newly proposed repairable conditionally repairable damage (RCR) model were used to calculate the RBE. RESULTS: The RBE at 10% cell survival for 40, 80 and 160 eV nm(-1) boron ions compared with (60)Co were 1.98 (1.83-2.22), 2.85 (2.64-3.11) and 3.37 (3.17-3.58), respectively, of almost independence of the model used in the calculation. CONCLUSIONS: Different cell survival models may generate different RBE, especially at low doses and high cell survival levels.

Apoptosis↗

PubMed2004

Advantage and limitations of weighting factors and weighted dose quantities and their units in boron neutron capture therapy.

Defining the parameters influencing the biological reaction due to absorbed dose is a continuous topic of research. The main goal of radiobiological research is to translate the measurable dose of ionizing radiation to a quantitative expression of biological effect. Mathematical models based on different biological approaches (e.g., skin reaction, cell culture) provide some estimations that are often misleading and, to some extent, dangerous. Conventional radiotherapy is the simplest case because the primary radiation and secondary radiation are both low linear energy transfer (LET) radiation and have about the same relative biological effectiveness (RBE). Nevertheless, for this one-dose-component case, the dose-effect curves are not linear. In fact, the total absorbed dose and the absorbed dose per fraction as well as the time schedule of the fractionation scheme influence the biological effects. Mathematical models such as the linear-quadratic model can only approximate biological effects. With regard to biological effects, fast neutron therapy is more complex than conventional radiotherapy. Fast neutron beams are always contaminated by gamma rays. As a consequence, biological effects are due to two components, a high-LET component (neutrons) and a low-LET component (photons). A straight transfer of knowledge from conventional radiotherapy to fast neutron therapy is, therefore, not possible: RBE depends on the delivered dose and several other parameters. For dose reporting, the European protocol for fast neutron dosimetry recommends that the total absorbed dose with gamma-ray absorbed dose in brackets is stated. However, boron neutron capture therapy (BNCT) is an even more complex case, because the total absorbed dose is due to four dose components with different LET and RBE. In addition, the terminology and units used by the different BNCT groups is confusing: absorbed dose and weighted dose are both to be stated in grays and are never "photon equivalent." The ICRU/IAEA made proposals, which should be followed by all BNCT groups, to report always the four absorbed dose components, boron dose DB, proton dose Dp, gamma-ray dose Dgamma, and neutron dose Dn, as well as the sum DT of all components, as total absorbed dose, together with the total weighted dose Dw (to be used only for internal purposes, indicating the used weighting factors) at all points of interest and the treatment conditions.

Body Burden↗

PubMed1993

Lethality of heavy ion-induced DNA double-strand breaks in mammalian cells.

Cell killing and the production of DNA double-strand breaks (dsbs) were measured in parallel for V79 cells and a human tumour cell line (Caski) following exposure to radiations of differing linear energy transfer (LET) including accelerated heavy ions. Dsb induction was assessed by neutral filter elution (pH 7.4) and elution from agarose plugs in pulsed-field electrophoresis. The elution data were consistent with linear lesion induction and allowed to derive dsb yields or production cross-sections (sigma dsb), respectively. Both cell lines as well as the two elution approaches gave comparable results. sigma dsb was found to rise up to the heaviest ions used (LET = 11,500 keV/microns) but relative biological effectiveness was always smaller than unity. Slopes of the exponential survival curves (final slope with 60Co-radiation) were normalized to the respective dsb yields and allowed to calculate the relative lethality per induced dsb. This parameter increased with LET up to about 300 keV/microns followed by a steep decline for the very heavy ions. The extent of dsb rejoining was concomitantly reduced with ionization density.

Cell Death↗

PubMed1994

Clonogenic cell survival and rejoining of DNA double-strand breaks: comparisons between three cell lines after photon or He ion irradiation.

Three cell lines, human glioma U-343MG, Chinese hamster V79-379A and human colon carcinoma LS-174T, were analysed for clonogenic survival and with pulsed-field gel electrophoresis regarding induction and rejoining of double-strand breaks (dsb) in DNA. The cells were irradiated with either intermediate linear energy transfer (LET approximately 55 keV/microns) He ions or with 60Co photons and showed cell type-specific variations in their survival curves. The induction of dsb, per DNA unit, increased linearly with dose for both radiation qualities, and there were no cell type-dependent differences. However, the dsb induction frequency increased for all three cell lines with an RBE of 1.31 +/- 0.08 (SD) after He ion irradiation. All three cell lines showed biphasic dsb rejoining patterns with cell type-specific differences. The differences between the cell lines were somewhat smaller after irradiation with He ions, although the patterns were very similar to those seen after photon irradiation. The shoulders in the survival curves disappeared after He ion irradiations, however the cells retained the capacity to rejoin dsb. After 8-h rejoining the increase of LET to intermediate values did not give a higher fraction of residual dsb.

Animals↗

PubMed1994

A new model of shouldered survival curves.

Recently, the linear-quadratic equation has been used to construct the dose-response relationships of ionizing radiation. The radiobiological theory on which this relationship is based indicates that at low doses, the risk of a biological lesion being formed should depend linearly on dose if a single event is required or quadratically on dose if two events are required. The same approach has also been used to construct the shouldered survival curves, which indicate a lower response of cell killing at low doses of low linear energy transfer (LET) radiation than at high doses because of repair. However, a different approach is possible, derived from the concept of generating the hybrid lognormal distribution, in which the hybrid form of linear and logarithmic components of a random variable is used. The hybrid form is a formulation of the phenomenon in which there is a feedback mechanism against the large change in the random variable. This paper presents a new model of shouldered survival curves, called a hybrid scale model, which has two parameters: the inactivation constant and the protective factor. In the model, the surviving fraction, normalized by a protective factor plotted in a hybrid scale, is assumed to be linear against the dose. This simple model provides an implication of the shoulder of survival curve and the effect of recovery time of radiation damage, as well as giving a good to the well-known data of split-dose experiments with mammalian cells.

Animals↗

PubMed1997

Health impacts of large releases of radionuclides. Cytogenetic effects as quantitative indicators of radiation exposure.

Scoring of dicentrics in metaphase preparations of human T lymphocytes is the method of choice for estimating individual whole-body doses of radiation exposure. A quantification of partial-body exposures or non-uniform distribution of the dose is more complicated but it can be achieved by using specific mathematical approaches. For retrospective biodosimetry, conventional scoring of dicentrics is less precise because these unstable aberrations are eliminated with time post-exposure. Symmetrical translocations are not selected against during mitotic division in the haematopoietic cell reproductive centres, so the frequencies of these stable aberrations are generally assumed to remain constant even for decades. They can now be analysed precisely by fluorescence in situ hybridization using whole chromosome-specific DNA probes (chromosome painting) with an alpha-satellite DNA probe for centromere detection. Based on in vitro calibration curves established with single or multicolour paints covering 4-22% of the total human genomic DNA content, scoring of translocations has been applied for dose reconstruction in smaller groups of atomic bomb survivors and victims of the Chernobyl and Goiania radiation accidents. However, prior to routine use, the method requires further validation. Such work includes the precise evaluation of the unexpectedly high frequency of complex exchanges (> or = 3 breaks in > or = 2 chromosomes) found both at > 2 Gy doses of low linear energy transfer (LET) radiation and generally for high LET alpha-particles. Data on the long-term stability of translocations and the appearance of clonal abberrations, as well as improved measurements of the linear coefficient of standard calibration curves, are also required.

Centromere↗

PubMed2004

Analysis of alpha-particle induced chromosome aberrations in human lymphocytes, using pan-centromeric and pan-telomeric probes.

PURPOSE: The aim of the present study has been the evaluation of the incomplete chromosome aberrations induced after alpha-particle irradiation by the simultaneous detection of all centromeres and telomeres present in human lymphocytes. Moreover, a study on the lengths of the different acentric fragments is presented. MATERIALS AND METHODS: Attached lymphocytes were irradiated at doses of 0.2, 0.5, 0.7 and 1 Gy using a 241Am source. Flourescent in-situ hybridization (FISH) techniques were applied using pan-centromeric and pan-telomeric probes. All abnormal cells were digitalised and analysed using a Cytovision FISH workstation. The description of all abnormalities observed, and the length of the acentric fragments was recorded. RESULTS: A total of 378 incomplete chromosomes plus incomplete acentrics was found. Cases with more than 92 telomeres were not detected. The ratio between total incomplete elements and multicentrics was 1.00. The total number of acentric (ace) fragments was 822; 57% of them were complete fragments ace (+,+), 26% incomplete fragments ace (+,-), and 17% interstitial fragments ace(-,-); the mean relative lengths were 2.91 +/- 0.06, 1.91 +/- 0.07 and 1.63 +/- 0.07, respectively. In all three cases a secondary peak in the length distribution was found, corresponding to a relative length between 3.5 and 4. CONCLUSION: The percentage of incomplete rejoinings is higher after alpha-particle exposure than that described previously for low-linear energy transfer (LET) radiation exposures. The results seem to indicate that compared to low-LET radiation, after alpha-particle exposure centromere-containing elements are more likely to be repaired.Many interstitial fragments are large linear forms that cannot be considered as non-distinguishable acentric rings.

Alpha Particles↗

PubMed1995

The effect of dimethyl sulfoxide on the induction of DNA double-strand breaks in V79-4 mammalian cells by alpha particles.

The present study was undertaken to assess the protective effect of dimethyl sulfoxide (DMSO) against the induction and rejoining of DNA double-strand breaks (DSBs) and inactivation of V79-4 Chinese hamster cells by both high- and low-linear energy transfer (LET) radiations. The cells were exposed under aerobic conditions as monolayers to either low-LET photons (60Co gamma rays) or high-LET alpha particles (238Pu) at 277 K. The initial yield of DSBs, determined by elution under nondenaturing conditions, is linearly dependent on dose. When the irradiation was carried out in the presence of DMSO (0-0.6 mol dm-3), the initial yields of DSBs induced by both gamma and alpha-particle irradiation decrease. With gamma irradiation at [DMSO] > 0.6 mol dm-3, a further decrease in the yield of DSBs occurs. DMSO (0.5 mol dm-3) reduces the initial yield of DSBs by 50 +/- 5% and 32 +/- 4% for photons and alpha particles, respectively. DMSO protects more effectively against cellular inactivation and DSB induction at low LET compared with alpha-particle irradiation with protection factors of 1.7 and 1.4, respectively, for survival and 2.0 and 1.5, respectively, for DSBs. After incubation of the irradiated cells for 3 h at 310 K after high-LET irradiation, the residual yield of DSBs is reduced by < 13% when the irradiations were carried out in the presence of 0.5 mol dm-3 DMSO. With gamma irradiation in the presence of 0.5 mol dm-3 DMSO, 90% of the DSBs are rejoined by 3 h incubation at 310 K. Therefore, the nonscavengeable DSBs induced by alpha particles are not significantly rejoined within 3 h, in contrast to rejoining of the majority of the nonscavengeable DSBs induced by gamma irradiation. From comparison of the data on DSBs and survival for alpha-particle irradiation, it is inferred that the severity of damage is reduced by DMSO through minimizing the formation of OH-induced sugar/base modifications in the vicinity of nonscavengeable DSBs.

Alpha Particles↗

PubMed1992

Direct comparison between protons and alpha-particles of the same LET: I. Irradiation methods and inactivation of asynchronous V79, HeLa and C3H 10T1/2 cells.

A direct comparison was carried out of the biological effectiveness of protons and alpha-particles of the same linear energy transfer (LET) under identical conditions with a variety of in vitro biological systems. Monolayers of mammalian cells were irradiated with accelerated beams of protons (1.2 and 1.4 MeV) and alpha-particles (30 and 35 MeV) corresponding to LETs of 23 and 20 keV microns-1 for each particle type. For V79-4 cells it was observed that the linear term of the dose-response for cell inactivation by protons was significantly greater than that for alpha-particles of the same LET. For HeLa and HeLa S3 cells, also, the linear term appeared to be greater for protons, but this was not observed with more limited data for C3H 10T1/2 cells. The result for V79 cells is in agreement with the report of Belli et al. (1989) who observed that the biological effectiveness of protons rose sharply between 17 and 30 keV microns-1 in strong contrast to alpha-particles which reached a peak effectiveness at greater than 100 keV microns-1. These results place new constraints on the biologically relevant features of the microscopic structure of radiation tracks, and have implications for the mechanistic and practical comparison between radiations.

Alpha Particles↗

PubMed2006

A semianalytic model to extract differential linear scattering coefficients of breast tissue from energy dispersive x-ray diffraction measurements.

The goal of this work is to develop a technique to measure the x-ray diffraction signals of breast biopsy specimens. A biomedical x-ray diffraction technology capable of measuring such signals may prove to be of diagnostic use to the medical field. Energy dispersive x-ray diffraction measurements coupled with a semianalytical model were used to extract the differential linear scattering coefficients [mus(x)] of breast tissues on absolute scales. The coefficients describe the probabilities of scatter events occuring per unit length of tissue per unit solid angle of detection. They are a function of the momentum transfer argument, x=sin(theta/2)/X, where theta=scatter angle and lambda=incident wavelength. The technique was validated by using a 3 mm diameter 50 kV polychromatic x-ray beam incident on a 5 mm diameter 5 mm thick sample of water. Water was used because good x-ray diffraction data are available in the literature. The scatter profiles from 6 degrees to 15 degrees in increments of 1 degrees were measured with a 3 mm x 3 mm x 2 mm thick cadmium zinc telluride detector. A 2 mm diameter Pb aperture was placed on top of the detector. The target to detector distance was 29 cm and the duration of each measurement was 10 min. Ensemble averages of the results compare well with the gold standard data of A. H. Narten ["X-ray diffraction data on liquid water in the temperature range 4 degrees C-200 degrees C," ORNL Report No. 4578 (1970)]. An average 7.68% difference for which most of the discrepancies can be attributed to the background noise at low angles was obtained. The preliminary measurements of breast tissue are also encouraging.

Breast Neoplasms↗

PubMed1992

Damage to cellular DNA from particulate radiations, the efficacy of its processing and the radiosensitivity of mammalian cells. Emphasis on DNA double strand breaks and chromatin breaks.

For several years, it has been evident that cellular radiation biology is in a necessary period of consolidation and transition (Lett 1987, 1990; Lett et al. 1986, 1987). Both changes are moving apace, and have been stimulated by studies with heavy charged particles. From the standpoint of radiation chemistry, there is now a consensus of opinion that the DNA hydration shell must be distinguished from bulk water in the cell nucleus and treated as an integral part of DNA (chromatin) (Lett 1987). Concomitantly, sentiment is strengthening for the abandonment of the classical notions of "direct" and "indirect" action (Fielden and O'Neill 1991; O'Neill 1991; O'Neill et al. 1991; Schulte-Frohlinde and Bothe 1991 and references therein). A layer of water molecules outside, or in the outer edge of, the DNA (chromatin) hydration shell influences cellular radiosensitivity in ways not fully understood. Charge and energy transfer processes facilitated by, or involving, DNA hydration must be considered in rigorous theories of radiation action on cells. The induction and processing of double stand breaks (DSBs) in DNA (chromatin) seem to be the predominant determinants of the radiotoxicity of normally radioresistant mammalian cells, the survival curves of which reflect the patterns of damage induced and the damage present after processing ceases, and can be modelled in formal terms by the use of reaction (enzyme) kinetics. Incongruities such as sublethal damage are neither scientifically sound nor relevant to cellular radiation biology (Calkins 1991; Lett 1990; Lett et al. 1987a). Increases in linear energy transfer (LET infinity) up to 100-200 keV micron-1 cause increases in the extents of neighboring chemical and physical damage in DNA denoted by the general term DSB. Those changes are accompanied by decreasing abilities of cells normally radioresistant to sparsely ionizing radiations to process DSBs in DNA and chromatin and to recover from radiation exposure, so they make significant contributions to the relative biological effectiveness (RBE) of a given radiation.(ABSTRACT TRUNCATED AT 400 WORDS)

Animals↗

PubMed1998

From chimney sweeps to astronauts: cancer risks in the work place: the 1998 Lauriston Taylor lecture.

Percival Pott, in 1775, was the first to note an association between overt cancer and a carcinogen in the work place when he astutely observed an elevated incidence of scrotal cancer in small boys who assisted chimney sweeps. In their "workplace" astronauts and crew of high altitude jet-liners are exposed, not only to low linear energy transfer (LET) radiation but also to HZE (high energy + high atomic number) particles and to neutrons-for which no human epidemiological data exist. The current system of radiation protection is based on risk estimates from low LET radiations, delivered in large doses and at high dose-rate, coupled with the assumption of a linear no-threshold model. In extrapolating to low doses and dose-rates, and to high LET radiations, it would be helpful if the mechanisms of radiation carcinogenesis were known. Unfortunately that is not the case, though progress has been made toward that end. Many human leukemias and lymphomas appear to be due to specific chromosomal translocations, while solid tumors usually involve multiple mutations in oncogenes, deletions in suppressor genes, and/or chromosomal rearrangements. Genomic instability and immortality are hallmarks of cancer and it is attractive to hypothesize that this is due to a mutation in a gene or genes responsible for the stability of the genome. Examples abound of a small DNA change inactivating a gene and leading to major biological consequences. This could result from a single particle, especially a HZE particle, or a recoil proton from the absorption of a neutron. In this context the assumption of a threshold is hazardous, and the linear no-threshold hypothesis still appears to be prudent and conservative.

Astronauts↗

PubMed2006

Redox changes induced in hippocampal precursor cells by heavy ion irradiation.

Hippocampal precursors retain the capacity to proliferate and differentiate throughout life, and their progeny, immature neurons, can undergo neurogenesis, a process believed to be important in maintaining the cognitive health of an organism. A variety of stresses including irradiation have been shown to deplete neural precursor cells, an effect that inhibits neurogenesis and is associated with the onset of cognitive impairments. Our past work has shown that neural precursor cells exposed to X-rays or protons exhibit a prolonged increase in oxidative stress, a factor we hypothesize to be critical in regulating the function of these cells after irradiation and other stresses. Here we report that irradiation of hippocampal precursor cells with high-linear energy transfer (LET) 1 GeV/nucleon 56Fe ions leads to significantly higher levels of oxidative stress when compared to lower LET radiations (X-rays, protons). Irradiation with 1 Gy of 56Fe ions elicits twofold to fivefold higher levels of reactive oxygen species (ROS) compared to unirradiated controls, and at lower doses (<or=1 Gy) neural precursors exhibit a linear dose response 6 h after heavy ion exposure. The use of the antioxidant lipoic acid (LA) was able to reduce ROS levels below background levels when added before or after 56Fe ion irradiation. These results conclusively show that low doses of 56Fe ions can elicit significant levels of oxidative stress in neural precursor cells. Given the prevalence of heavy ions in space and the duration of interplanetary travel, these data suggest that astronauts are at risk for developing cognitive decrements. However, our results also indicate that antioxidants delivered before as radioprotective agents or after as mitigating agents hold promise as effective countermeasures for ameliorating certain adverse effects of heavy ion exposure to the CNS.

Animals↗

PubMed1996

Breast cancer mortality between 1950 and 1987 after exposure to fractionated moderate-dose-rate ionizing radiation in the Canadian fluoroscopy cohort study and a comparison with breast cancer mortality in the atomic bomb survivors study.

The relationship between exposure to low-linear energy transfer ionizing radiation and subsequent breast cancer mortality risk is reported based on a further 7 years of follow-up in the Canadian fluoroscopy study. Amongst 31,917 women first treated for tuberculosis in a Canadian institution between 1930 and 1952, a total of 688 breast cancer deaths were observed between 1950 and 1987. There is a strong linear trend of increasing risk with increasing dose (P < 0.0001), with the excess relative risk per sievert decreasing with age at exposure (P = 0.0003). The excess relative risk is approximately constant between 5 and 39 years after exposure, with a suggestion of a decrease between 40 and 57 years after exposure, though this could be a chance effect (P = 0.22). Combined analyses of the Canadian fluoroscopy data and the data for the atomic bomb survivors with respect to breast cancer mortality are also reported. In general the two studies are reasonably consistent, the only distinct difference being the much greater excess relative risk per sievert amongst women exposed to very high doses in the province of Nova Scotia (P, heterogeneity <0.0001). Based on the combined data sets a simple relative risk (RR) model for the effect of a dose of D sieverts at age A years is developed: RR(D) = 1.0 + 0.52D exp[-0.10(A-15)]. This model fits the combined data well, and is used to predict excess lifetime risks of breast cancer mortality after radiation exposure from routine annual mammography.

Adolescent↗

PubMed1994

The depth-dependent radiation response of human melanoma cells exposed to 65 MeV protons.

Radiation therapy with positively charged particles implies that the Bragg peak be spread out to deliver a homogeneous dose to the tumour. The spread-out Bragg peak (SOBP) has a higher linear energy transfer (LET) than the entrance beam. In addition, there is an LET gradient from proximal to distal SOBP. The aim of this study is to find out whether these small LET variations lead to differences in radiation response. Human melanoma cells (CAL4) were exposed to 65 MeV proton beams produced by the cyclotron Medicyc at five different positions: 2 mm depth corresponding to the entrance, 15, 20, 25 and 26.8 mm depth corresponding to four different positions in the half-modulated SOBP. Survival curves were generated using the in vitro colony method and fitted with the linear-quadratic model. Survival differences were observed at high doses; they were statistically significant at a dose of 8 Gy. With respect to the entrance position (2 mm), the relative biological effectiveness (RBE) at 1% survival was 1.09, 1.12, 1.19 and 1.27 at 15, 20, 25 and 26.8 mm in the SOBP, respectively. Whereas RBE values in the SOBP greater than 1.0 relative to the entrance beam represent a small biological advantage to be added to the well-known physical advantage of high energy proton beams; the RBE gradient along the SOBP would imply that the distal end of the tumour would receive a higher biologically equivalent dose than the proximal end, despite a homogeneous physical dose, especially at the high doses per fraction given in ocular melanomas. Although the increase in effectiveness with depth is mild, it should be kept in mind during eye treatment planning, in case a critical target is present at the extreme end of the SOBP.

Cell Survival↗

PubMed1993

Derivations of relative biological effectiveness for the high-let radiations produced during boron neutron capture irradiations of the 9L rat gliosarcoma in vitro and in vivo.

PURPOSE: Relative biological effectiveness (RBE) values for the high linear-energy-transfer particles produced during boron neutron capture therapy have generally been based on theoretical considerations or in vitro experiments. The purpose of this study was to independently determine RBE values for all of the boron neutron capture therapy dose components. METHODS AND MATERIALS: Clonogenic cell survival data were obtained for 9L rat gliosarcoma cells irradiated in the Brookhaven Medical Research Reactor thermal neutron beam both in vitro and as an intracerebral tumor. These data were analyzed using the linear quadratic model for cell survival to derive measured RBE values for all beam components and for a number of different boron compounds. RESULTS: In the absence of boron, the combined effects of the protons from the nitrogen capture, 14N(n,p)14C, and the fast neutron scatter, 1H(n,n')p, reactions generated RBEs of 3.7 in vitro and 3.2 in an in vivo/in vitro excision assay, compared to 250 kVp X rays using an end point of 1% cell survival. Apparent RBEs for the 10B(n,alpha)7Li reaction products were calculated from cell survival data following reactor irradiations in the presence of the amino acid p-boronophenylalanine, the sulfhydryl dodecaborate monomer or dimer, or boric acid. Apparent RBEs for the 10B(n,alpha)7Li reaction ranged from 1.2 to 9.8 depending on which boron compound was used. RBEs from the in vitro studies were consistently higher than from the in vivo/in vitro studies. Under any conditions, the apparent RBE for the 10B(n,alpha)7Li reaction with p-boronophenylalanine was higher than that with any other boron compound tested. CONCLUSIONS: Generally accepted RBE values for the fast neutron and 14N(n,p)14C reaction components of the total dose are too low. The apparent RBEs calculated for the 10B(n,alpha)7Li reaction were compound-dependent and consistent with differences in the distribution of 10B relative to glioma cell nuclei.

Animals↗

PubMed1988

Oncogenic transformation by charged particles of defined LET.

Neoplastic transformation incidence and cytotoxicity were scored in the C3H/10T1/2 cell system following irradiation with charged particles of defined linear energy transfer (LET) produced at the Radiological Research Accelerator Facility of Columbia University. Cells cultured in monolayers, attached to thin Mylar sheets, were irradiated with accelerated protons, deuterons or helium-3 ions, and the results compared with X-rays. Defined LET values obtained by using the track segment mode, ranged from 10 to 120 keV/microns. For X-rays, and for the charged particles of lower LET, the dose-response curves for cell survival have a marked initial shoulder. With increasing LET, there is a progressive decrease in the size of the shoulder and for the highest LETs, survival curves approximate an exponential function of dose. The transformation incidence, likewise, showed a direct correlation to LET over the dose range examined. The efficiencies of transformation, however, appeared to approach a plateau between 80 and 120 keV/micron. Transformation data were analyzed using a linear-quadratic function of dose for the transformation probability. This latter quantity, when analyzed using microdosimetric consideration, suggests that the target volume for this end point is of the order of micrometer.

Animals↗

PubMed2001

Comparison of quality assurance for performance and safety characteristics of the facility for Boron Neutron Capture therapy in Petten/NL with medical electron accelerators.

BACKGROUND AND PURPOSE: The European Council Directive on health protection 97/43/EURATOM requires radiotherapy quality assurance programmes for performance and safety characteristics including acceptance and repeated tests. For Boron Neutron Capture therapy (BNCT) at the High Flux Reactor (HFR) in Petten/NL such a programme has been developed on the basis of IEC publications for medical electron accelerators. RESULTS: The fundamental differences of clinical dosimetry for medical electron accelerators and BNCT are presented and the order of magnitude of dose components and their stability and that of the main other influencing parameter 10B concentration for BNCT patient treatments. A comparison is given for requirements for accelerators and BNCT units indicating items which are not transferable, equal or additional. Preliminary results of in vivo measurements done with a set of 55Mn, 63Cu and 197Au activation foils for all single fields for the four fractions at all 15 treated patients show with < +/- 4% up to now a worse reproducibility than the used dose monitoring systems (+/- 1.5%) caused by influence of hair position on the foil-skull distance. CONCLUSIONS: Despite the more complex clinical dosimetry (because of four relevant dose components, partly of different linear energy transfer (LET)) BNCT can be regulated following the principles of quality assurance procedures for therapy with medical electron accelerators. The reproducibility of applied neutron fluence (proportional to absorbed doses) and the main safety aspects are equal for all teletherapy methods including BNCT.

Acceleration↗