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At least 19 recordsLinked to original sources
PubMed1995

On the revised concept of linear energy transfer.

The quantities linear energy transfer or restricted linear energy transfer are utilized in calculations that link absorbed dose to the fluence distribution of a radiation field. The computations provide approximations to absorbed dose in terms of the intermediate quantity cema or reduced cema. With the definition of the restricted linear energy transfer, L delta, given in ICRU Report 33, the approximation remains imperfect. This study deals with the resulting need for a modified definition of L delta, as proposed in a draft report of ICRU. Essential differences between the old and the new definitions are demonstrated. The changed definition permits a rigorous formulation of the dependence between fluence and absorbed dose.

Dose-Response Relationship, Radiation↗
PubMed2004

Passive spectrometry of linear energy transfer: development and use.

A linear energy transfer (LET) spectrometer based on the evaluation of particle track parameters in a chemically etched polyallyldiglycolcarbonate (PADC) track detector has been developed at our laboratory. It permits us to determine LET spectra between 10 and 700 keV microm(-1) in tissues. The LET spectra obtained permit us to calculate total dose and dose equivalent corresponding to particles with etchable tracks also. We have recently been able to verify the calibration curves used by using C, Mg, Ne, Si and Fe ion beams with different energies. The calibration curves obtained are presented and compared with those originally used, and a good correlation is found. The LET spectrometer with new calibration was used to analyse the radiation quality of the radiotherapy proton beam at the Joint Institute for Nuclear Research (JINR). The radiation quality was studied along the proton's range, particular attention being devoted to the region of the Bragg peak. It was found that the biologically weighted effective dose (BWE) reaches a value of about 1.25 at the Bragg peak region. At the beam entrance this value increases to about 1.02 due to secondary particles created through primary proton nuclear reactions in tissues.

Algorithms↗
PubMed2006

Internal high linear energy transfer (LET) targeted radiotherapy for cancer.

High linear energy transfer (LET) radiation for internal targeted therapy has been a long time coming on to the medical therapy scene. While fundamental principles were established many decades ago, the clinical implementation has been slow. Localized neutron capture therapy, and more recently systemic targeted alpha therapy, are at the clinical trial stage. What are the attributes of these therapies that have led a band of scientists and clinicians to dedicate so much of their careers? High LET means high energy density, causing double strand breaks in DNA, and short-range radiation, sparing adjacent normal tissues. This targeted approach complements conventional radiotherapy and chemotherapy. Such therapies fail on several fronts. Foremost is the complete lack of progress for the control of primary GBM, the holy grail for cancer therapies. Next is the inability to regress metastatic cancer on a systemic basis. This has been the task of chemotherapy, but palliation is the major application. Finally, there is the inability to inhibit the development of lethal metastatic cancer after successful treatment of the primary cancer. This review charts, from an Australian perspective, the developing role of local and systemic high LET, internal radiation therapy.

Animals↗
PubMed2002

Reduction of survival and induction of chromosome aberrations in tobacco irradiated by carbon ions with different linear energy transfers.

PURPOSE: To determine the relationship between linear energy transfer (LET) and the relative biological effectiveness (RBE) for survival reduction and chromosome aberration induction in plants. MATERIALS AND METHODS: Tobacco seeds were exposed to carbon ions having LET ranging from 92 to 260 keV microm(-1). Survival ratc was determined at 7 weeks after sowing. Chromosome aberrations were observed when the root length reached about 0.5 mm (immediately after radicle emergence), 3 and 10 mm. RESULTS: The RBE for both endpoints increased with increasing LET and showed the highest value at 230 keV um(-1). The highest RBE was 65.0 for survival reduction and 52.5 for chromosome aberration induction. The types and yield ratio of chromosome aberrations such as fragments and bridges were not affected by radiation type at 0.5mm root length. As the roots elongated from 0.5 to 10 mm, the frequency of aberrant cells gradually decreased. The number of cells with fragments decreased faster than the number of cells with bridges. The decrement of chromosome aberrations appeared to be slower in roots irradiated by carbon ions than in roots irradiated by gamma-rays. CONCLUSIONS: The results show a close relationship between survival reduction and chromosome aberration induction in plants. The types and yield ratio of initial chromosome aberrations did not differ among gamma-rays and carbon ions with different LET.

Carbon↗
PubMed1996

Cellular and molecular analysis of mutagenesis induced by charged particles of defined linear energy transfer.

Mutation induction by charged particles of defined linear energy transfer (LET) and gamma rays was scored using human-hamster hybrid AL cells. The LET values for charged particles accelerated at the Radiological Research Accelerator Facility ranged from 10 keV/microm protons to 150 keV/microm 4He ions. The induced mutant fractions at both the S1 and HGPRT loci were dependent on the dose and LET. In addition, for each dose examined, the mutant yield at the S1 locus was 30-60 fold higher than at the corresponding HGPRT locus. To determine whether the mutation spectrum was comparably dependent on dose and LET, independent S1- and HGPRT- mutants induced by 150 keV/microm 4He ions and gamma rays were isolated, and their DNA was analyzed by both Southern blotting and multiplex PCR methods. While the majority of radiation-induced mutants showed deletions of varying sizes, the relative percentage of large deletions was found to be related to both the dose and LET of the radiation examined. Using a mutation system that can detect multilocus changes, results of the present study show that radiation-induced chromosomal loss can be in the millions of base pairs.

Animals↗
PubMed1984

Current status of high linear energy transfer irradiation.

Based on laboratory investigations, high linear energy transfer (LET) particle irradiation is capable of more efficient cell kill than that associated with conventional or low LET irradiation. The advantages of high LET irradiation include: (1) a greater ability to damage hypoxic cells; (2) a lesser ability for repair of sublethal and potentially lethal radiation-induced damage; (3) less variation in radiation sensitivity relative to the cell cycle; and (4) a greater ability to deposit the radiation dose in the region of the tumor as opposed to the normal surrounding tissue (neutrons do not have this advantage compared to other particle therapy). Despite these laboratory advantages, it has been difficult to demonstrate any advantage of high LET irradiation in the clinic. A number of new developments have occurred to test the role of high LET: (1) sophisticated technology to enable treatment delivery with higher dose rate and improved depth dose; (2) the construction of hospital-based facilities; and (3) the development of randomized studies involving diseases in which the risk of early metastasis is minimized. It is hoped that careful study in the clinic over the next decade will elucidate the role of high LET particle therapy.

Clinical Trials as Topic↗
PubMed2004

The response of a spherical tissue-equivalent proportional counter to different ions having similar linear energy transfer.

The response of a tissue-equivalent proportional counter (TEPC) to different ions having a similar linear energy transfer (LET) has been studied. Three ions, 14N, 20Ne and 28Si, were investigated using the HIMAC accelerator at the National Institute of Radiological Sciences at Chiba, Japan. The calculated linear energy transfer (LET( infinity )) of all ions was 44 +/- 2 keV/microm at the sensitive volume of the TEPC. A particle spectrometer was used to record the charge and position of each incident beam particle. This enabled reconstruction of the location of the track as it passed though the TEPC and ensured that the particle survived without fragmentation. The spectrum of energy deposition events in the TEPC could be evaluated as a function of trajectory through the TEPC. The data indicated that there are many events from particles that did not pass through the sensitive volume. The fraction of these events increased as the energy of the particle increased due to changes in the maximum energy of the delta rays. Even though the LET of the incident particles was nearly identical, the frequency-averaged lineal energy, y(F), as well as the dose-averaged lineal energy, y(D), varied with the velocity of the incident particle. However, both values were within 15% of LET in all cases.

Computer Simulation↗
PubMed1988

Mutation induction by charged particles of defined linear energy transfer.

The mutagenic potential of charged particles of defined linear energy transfer (LET) was assessed using the hypoxanthine-guanine phosphoribosyl transferase locus (HGPRT) in primary human fibroblasts. Exponentially growing cultures of early passaged fibroblasts were grown as monolayers on thin mylar sheets and were irradiated with accelerated protons, deuterons or helium-3 ions. The mutation rates were compared with those generated by 137Cs gamma-rays. LET values for charged particles accelerated at the Radiological Research Accelerator Facility, using the track segment mode, ranged from 10 to 150 keV/micron. After irradiation, cells were trypsinized, subcultured and assayed for both cytotoxicity and 6-thioguanine resistance. For gamma-rays, and for the charged particles of lower LET, the dose-response curves for cell survival were characterized by a marked initial shoulder, but approximated to an exponential function of dose for higher LETs. Mutation frequencies, likewise, showed a direct correlation to LET over the dose range examined. Relative biological effectiveness (RBE) for mutagenesis, based on the initial slopes of the dose-response curves, ranged from 1.30 for 10 keV/micron protons to 9.40 for 150 keV/micron helium-3 ions. Results of the present studies indicate that high-LET radiations, apart from being efficient inducers of cell lethality, are even more efficient in mutation induction as compared to low-LET ionizing radiation. These data are consistent with results previously obtained with both rodent and human fibroblast cell lines.

Cell Survival↗
PubMed1990

Linear energy transfer (LET) spectra of cosmic radiation in low Earth orbit.

Integral linear energy transfer (LET) spectra of cosmic radiation (CR) particles were measured on five Cosmos series spacecraft in low Earth orbit (LEO). Particular emphasis is placed on results of the Cosmos 1887 biosatellite which carried a set of joint U.S.S.R.-U.S.A. radiation experiments involving passive detectors that included thermoluminescent detectors (TLDs), plastic nuclear track detectors (PNTDs), fission foils, nuclear photo-emulsions, etc. which were located both inside and outside the spacecraft. Measured LET spectra are compared with those theoretically calculated. Results show that there is some dependence of LET spectra on orbital parameters. The results are used to estimate the CR quality factor (QF) for the Cosmos 1887 mission.

Cosmic Radiation↗
PubMed1988

Radiosensitization produced by iododeoxyuridine with high linear energy transfer heavy ion beams.

Little is known about radiosensitization produced by iododeoxyuridine (IUDR) with high linear energy transfer radiation. Likewise, the effect of IUDR on repair of sublethal or potentially lethal damage is unclear. A series of in vitro experiments was performed examining these aspects of IUDR radiosensitization. Human T1 cells were grown in the presence of 3.0 micromolar IUDR for 72 hours (approximately three doubling times), an exposure which resulted in minimal cytotoxicity to unirradiated cells. As the cells entered plateau phase they were exposed to X rays and a variety of heavy ion beams. Sensitization was found to decrease as linear energy transfer (LET) increased. No sensitization took place in an extremely high LET Lanthanum ion beam (1000 keV/micrometer). However, IUDR produced significant sensitization in the Neon ion beam currently used to treat cancer patients at Lawrence Berkeley Laboratory. Sensitization enhancement ratios at the 40% cell survival level were found to be 1.8 for X rays, 1.5 for the proximal Bragg peak of the clinical Neon beam, and 1.3 for the distal peak of the clinical Neon beam. Cell survival curves fitted to the linear-quadratic model showed IUDR significantly increased the value of the linear component (alpha) in beams with LETs below 40 keV/micron. The value of the quadratic component (beta) was unaffected by IUDR, regardless of LET. Split-dose experiments with both X rays and proximal peak Neon ions revealed IUDR did not affect sublethal damage repair. Similarly, delayed-plating experiments showed IUDR did not affect repair of potentially lethal damage. In contrast to cells unexposed to IUDR, IUDR-treated cells showed near-equal levels of cell killing throughout the extended Bragg peak of the clinical Neon beam. These findings suggest that the addition of IUDR to Neon ion radiotherapy could enhance the therapeutic ratio of the clinical Neon beam.

Cell Survival↗
PubMed2000

DNA damage induced by radiation of different linear energy transfer: initial fragmentation.

PURPOSE: To investigate DNA fragmentation as a function of linear energy transfer (LET) after exposure to accelerated ions in the LET range 40-225 keV/microm. MATERIALS AND METHODS: Fragmentation patterns of double-stranded DNA in the range 5 kilobasepairs (kbp) to 5.7 megabasepairs (Mbp) were analysed after irradiation of low-passage GM 5758 normal human fibroblast cells with 60Co-photons, helium ions at 40 keV/microm and high-LET nitrogen ions between 80 and 225 keV/microm. Two separate pulsed-field gel electrophoresis protocols were used, optimized for separation of 1-6 Mbp and 5 kbp to 1.5 Mbp fragments. RESULTS: An increased probability of formation of short and medium-sized DNA fragments was revealed following high-LET irradiation. The DNA double-strand break (dsb) induction yields were, respectively, 5.8 and 6.9-8.8 x 10(-9) dsb bp(-1) Gy(-1) for 60Co-photons and ions. The ion yields were some 80-110% higher than those calculated according to a conventional approach, disregarding the fragment distributions. For photons, the yield was 13% higher. The corresponding relative biological effectiveness (RBE) of dsb induction was in the range 1.2-1.5. CONCLUSIONS: A significant non-random contribution to the number of dsb after irradiation with high-LET was confirmed by detailed fragment analysis using pulsed-field gel electrophoresis. The LET had a strong influence on the initial DNA fragment distribution, and hence also on the induction yields measured. However, when the LET was increased to the highest values studied for nitrogen ions, the yield decreased slightly.

Cells, Cultured↗
PubMed1991

Increased nuclear damage by high linear energy transfer radioisotopes applicable for radiodirected therapy against radiologic malignancies.

High linear energy transfer radioisotopes carried by appropriate agents have been proposed for receptor-directed radiotherapy. Two such classes of isotopes are Auger electron and alpha-emitting nuclides. To determine the relative cytotoxicity and nuclear damage to cells produced by these two classes of nuclides, we compared bromine-80m (80mBr), an Auger-electron-emitting radionuclide with a 4.4-hour half-life, with bismuth-212 (212Bi), an alpha-emitter with a 1-hour half-life. Because of the short path length of the Auger electrons, 80mBr was radiotoxic only when incorporated into DNA, such as in the form of [80mBr]bromodeoxyuridine ([80mBr]BrUdR). Both agents induced linear increases in chromosome aberration frequency, however, [80mBr]BrUdR caused multiple aberrations including the shattering of parts of the chromosomes. While, in contrast, a 2-hour exposure of cells to 212Bi, chelated to DTPA, a form which does not enter the cell, induced much less extensive chromosome damage. Exposure to equivalent activities of Auger electrons or alpha-particles results in 5 times more damage in Auger-electron-exposed cells. However, estimates of dose suggest they are equally toxic. Unlike Auger electrons, alpha-particles did not need to be in as close proximity to the DNA to have clastogenic and radiotoxic effects.

Alpha Particles↗
PubMed2001

[Production of superoxide radicals with pulse radiolysis of water with high linear energy transfer].

The radiolysis of water with heavy ions of high linear energy transfer (LET) (-dE/dx) is characterized, in deaerated medium, by the production of superoxide anions, the radiolytic yields of which increase with the LET. Radiobiological interest in such radical species comes from the oxidative stress which may be generated by their dismutation in O2 and H2O2 in anoxic medium (radiotherapy with heavy ions). A brief review of the measurements of superoxide free radicals in aqueous solution by indirect or direct methods is presented. Moreover, some experimental results obtained by pulse radiolysis with Ar18+ ions (TEL = 290 keV x microm(-1)), are described. The interpretation of the kinetics takes into account the superoxide absorbance and that of hydrogen peroxide, which is present at the millisecond time scale.

Algorithms↗
PubMed2003

Analytical linear energy transfer calculations for proton therapy.

As the relative biological effectiveness of protons depends on the linear energy transfer (LET), simple methods for LET calculations are desired for the optimization of proton therapy. This work provides an analytical model for the LET on the central axis of broad proton beams in water, which can also be applied to spread-out Bragg peaks. For realistic treatment situations with polyenergetic beams, the LET is here defined as a local mean of the proton stopping power, weighted by the local energy spectrum. The proposed model considers only Coulomb interactions and neglects nonelastic nuclear interactions. By assuming a Gaussian shape for the energy spectrum and by using a suitable parametrization of the stopping power, analytical expressions for the track averaged and the dose averaged LET are derived, which account for range straggling as well as for the initial width of the energy spectrum. The analytical model was evaluated by Monte Carlo simulations with GEANT 3.21. Local energy spectra were simulated to obtain LET distributions for several cases, using clinical energies between 70 and 250 MeV and varying widths of the initial energy spectrum. Good agreement was found between the analytical model and the Monte Carlo simulations (with maximum deviations of 0.5 keV per micrometer), which justifies the assumptions used in the derivation of the analytical model.

Body Burden↗
PubMed2000

Rejoining of DNA fragments produced by radiations of different linear energy transfer.

PURPOSE: To analyse the rejoining of DNA double-strand breaks (dsb) produced by high-linear energy transfer (LET) ions, with the specific focus on the influence, on the rejoining estimates, of the way dsb are distributed along chromosomes. MATERIAL AND METHODS: Low passages of normal human fibroblasts (GM5758) were irradiated with 60Co photons, 40 keV/microm helium ions or nitrogen ions with LETs of 80, 125, 175 and 225 keV/microm. The double-stranded DNA fragment distributions, ranging from 5 kbp to 5.7 Mbp, were assayed by pulsed-field gel electrophoresis after repair incubation for 0-22 h. RESULTS: The rejoining was biphasic and the half-times of the two phases were 15 min and 2-3h, respectively, and were independent of LET. Although the majority of breaks were rejoined by the fast phase, both the fraction of dsb rejoined by the slow phase and the fraction of unrejoined dsb at 20-22h increased with increasing LET. CONCLUSIONS: DNA fragment analysis detected LET-dependent differences in the amount of rejoining while the half-times were independent of LET. The majority of dsb were rapidly rejoined even after high-LET irradiation. If fragment-size distribution is not taken into account, both the fraction of breaks rejoined by slow kinetics, and the fraction of unrejoined breaks, can be overestimated when the LET is increased.

Cells, Cultured↗
PubMed2006

Human in vivo dose-response to controlled, low-dose low linear energy transfer ionizing radiation exposure.

PURPOSE: The effect of low doses of low-linear energy transfer (photon) ionizing radiation (LDIR, <10 cGy) on human tissue when exposure is under normal physiologic conditions is of significant interest to the medical and scientific community in therapeutic and other contexts. Although, to date, there has been no direct assessment of the response of human tissue to LDIR when exposure is under normal physiologic conditions of intact three-dimensional architecture, vasculature, and cell-cell contacts (between epithelial cells and between epithelial and stromal cells). EXPERIMENTAL DESIGN: In this article, we present the first data on the response of human tissue exposed in vivo to LDIR with precisely controlled and calibrated doses. We evaluated transcriptomic responses to a single exposure of LDIR in the normal skin of men undergoing therapeutic radiation for prostate cancer (research protocol, Health Insurance Portability and Accountability Act-compliant, Institutional Review Board-approved). Using newly developed biostatistical tools that account for individual splice variants and the expected variability of temporal response between humans even when the outcome is measured at a single time, we show a dose-response pattern in gene expression in a number of pathways and gene groups that are biologically plausible responses to LDIR. RESULTS: Examining genes and pathways identified as radiation-responsive in cell culture models, we found seven gene groups and five pathways that were altered in men in this experiment. These included the Akt/phosphoinositide-3-kinase pathway, the growth factor pathway, the stress/apoptosis pathway, and the pathway initiated by transforming growth factor-beta signaling, whereas gene groups with altered expression included the keratins, the zinc finger proteins and signaling molecules in the mitogen-activated protein kinase gene group. We show that there is considerable individual variability in radiation response that makes the detection of effects difficult, but still feasible when analyzed according to gene group and pathway. CONCLUSIONS: These results show for the first time that low doses of radiation have an identifiable biosignature in human tissue, irradiated in vivo with normal intact three-dimensional architecture, vascular supply, and innervation. The genes and pathways show that the tissue (a) does detect the injury, (b) initiates a stress/inflammatory response, (c) undergoes DNA remodeling, as suggested by the significant increase in zinc finger protein gene expression, and (d) initiates a "pro-survival" response. The ability to detect a distinct radiation response pattern following LDIR exposure has important implications for risk assessment in both therapeutic and national defense contexts.

Biopsy↗
PubMed1994

Radially restricted linear energy transfer for high-energy protons: a new analytical approach.

Radially restricted linear energy transfer (LET) is a basic physical parameter relevant to radiation biology and radiation protection. In this report a convenient method is presented for the analytical computation of this quantity without the need for complicated simulation. The method uses the energy-restricted LET L delta, as recently redefined in a 1993 ICRU draft document and supplements it by a relatively simple term that represents the energy of fast delta rays lost within distance r from the track core. The method provides a better fit than other models and is valid over the entire range of radial distance from track center to the maximum radial distance traveled by the most energetic secondary electrons. Lr computed by this approach differs only a few percent from the values obtained from explicit Monte Carlo simulations. The concept applies equally to heavy ions and to electrons.

Linear Energy Transfer↗