What is a 'low dose' of radiation?

Although the expression of radiation-induced biological effects and responses may be at either the cell, organ or organism level, induction of some of these phenomena (e.g. cancer of clastogenic and genetic effects) can have their origin in the interaction of a single charged particle with the target-containing volume (TCV) of the cell, e.g. the cell nucleus. However, the independent variable now used in both organ and cell population studies, the absorbed dose to the organ, provides no information directly on particle-TCV interactions. Even if calculated as a mean to an organized population of cells, the absorbed dose becomes a composite and confounded quantity, (FzN), in which F is the fraction of TCVs 'hit' by a particle during a given exposure, z is the mean value of z1, the energy absorbed in the TCV in a single hit, and N is the mean number of hits per affected TCV. Scientific precepts demand the avoidance of such confounded variables by achieving their isolation. The needed separation can be effected by the use of microdosimetric techniques, which make it possible to hold one component quantity constant while the others are varied. As an example, low-level radiation exposure (LLE) can be used to hold F at a constant value of 0.2 where, on average, there is but one hit per TCV. The probability of a cellular quantal response, as a function of z1 only, can then be determined by use of LLE to radiations covering a wide span of LETs. Conversely, the effect of varying only the fraction of cells hit can be studied by holding z constant. This can be accomplished by working within a narrow band of LET, but only in the LLE range. The effectiveness of preirradiation altering cell sensitivity as a function of the number of hits per TCV can be determined by working within, and somewhat above, the LLE range. In either risk assessment or the application of radiation as a pretreatment, minimal consequences can be assured only if very low-level exposure is employed in order that F will be small, and if the exposure is in a field of radiation of very low LET so that z1 will be as small as possible. That is to say, exposure conditions with low consequences cannot be specified in terms of any single quantity.

A microdosimetric understanding of low-dose radiation effects.

This paper presents a microdosimetric approach to the problem of radiation response by which effects produced at low doses and dose rates can be understood as the consequences of radiation absorption events in the nucleus of a single relevant cell and in its DNA. Radiation absorption at the cellular level, i.e. in the cell nucleus as a whole, is believed to act through radicals. This kind of action is called 'non-specific' and leads to the definition of an 'elemental dose' and the 'integral response probability' of a cell population. Radiation absorption at the molecular level, i.e. in sensitive parts of the DNA, is thought to act through double-strand breaks. This kind of action is called 'specific' and leads to a 'relative local efficiency'. In general, both mechanisms occur for all types of radiation; however, it is the dose contribution of both specific and non-specific effects that determines the radiation quality of a given radiation. The implications of this approach for the specification of low-dose and low dose-rate regions are discussed.

Mailable TLD system for photon and electron therapy beams.

The mailable TLD system developed by the Radiological Physics Center for monitoring calibration of photon beam energies from cobalt 60 to 25 MV and electron beam energies from 6 to 20 MeV has been in use since 1977 for photons and since 1982 for electron beams. Design considerations, proper use of the system and calibration techniques are detailed. The accuracy of the system is comparable to that of ion chamber measurements made in a water phantom, although it shows less precision.

A flatness and calibration monitor for accelerator photon and electron beams.

A flatness monitor has been built to quickly and accurately check accelerator beam flatness and dose calibration. Consisting of a 7 X 7 ion chamber array, the unit operates in photon beams from 60Co energies to 25 MV and electron beams (scattered or scanned) from 6 MeV to 25 MeV.

Rapid computation of diagnostic X-ray bremsstrahlung spectra.

A method is described for rapid and accurate computation of diagnostic x-ray spectra. Accuracy limitations of Kramers' equation are overcome by providing intensity correction factors derived from published measured data. Use of a parameter based on the energy of the Kramers spectrum intensity peak permits deriving master factor curves which are remarkably independent of kVp, waveform and filtration. Computed and measured spectra generally agree to better than +/- 1 keV for beams generated at 100 kVp and below. Possible application of the method to higher energy diagnostic beams is discussed.

Concepts of microdosimetry. I. Quantities.

This is the first part of an investigation of microdosimetric concepts relevant to numerical calculations. The definitions of the microdosimetric quantities are reviewed and formalized, and some additional conventions are adopted. The common interpretation of the quantities in terms of energy imparted to spherical sites is contrasted with their interpretation as the result of a diffusing process applied to the initial spatial pattern of energy transfers in the irradiated medium.

Variations of salivary amylase as a test of internal irradiation in man.

The hypothesis of the parotid gland radiosensitivity has suggested to the authors to follow up the effect of therapeutic internal irradiation on the serum, urine and salivary alpha-amylase activity in man. The assay and visualization of alpha-amylase isoenzymes on agar gel zymograms by using the "Phadebas amylase test" tablets has demonstrated in some cases increases of salivary alpha-amylase activity expressed by the ratio of the optical density after internal irradiation to that before administration of radioisotopes.