Microbeams, microdosimetry and specific dose.
Dose and its usefulness as a single parameter to describe the amount of radiation absorbed are well established for most situations. The conditions where the concept of dose starts to break down are well known, mostly from the study of microdosimetry. For low doses of high LET radiation it is noted that the process of taking the limiting value of the energy absorbed within a test volume divided by the mass within that volume yields either zero or a relatively large value. The problem is further exacerbated with microbeam irradiations where the uniformity of the energy deposition is experimentally manipulated on the spatial scale of cells being irradiated. Booz introduced a quantity to deal with these problems: the unfortunately named 'mean specific energy in affected volumes'. This quantity multiplied by the probability that a test volume has received an energy deposit is equal to dose (in situations where dose can be defined). I propose that Booz's quantity be renamed 'specific dose', that is the mean energy deposited divided by the mass within a specified volume. If we believe for instance that the nucleus of a cell is the critical volume for biological effects, we can refer to the nuclear specific dose. A microbeam experiment wherein 10 per cent of the cell nuclei were targeted with 10 alpha particles would be described as delivering a nuclear specific dose of 1.6 Gy to 10 per cent of the population.
Columbia University, RARAF, PO Box 21, Irvington, NY 10533, USA. gerhard@r-p.net
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Randers-Pehrson
D006801:Humans; D011829:Radiation Dosage; D011868:Radioisotopes / Q000493:pharmacokinetics; D011874:Radiometry / Q000379:methods*; D011878:Radiotherapy / Q000009:adverse effects; D012680:Sensitivity and Specificity; D014018:Tissue Distribution
D011868:Radioisotopes