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Physics And Chemistry Basis Of Biotechnology - De Cuyper - tiera.ru

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Urs Häfeli<br />

high energy g-rays. This led to higher than necessary radiation doses to the other<br />

organs as well as to hospital personnel. To avoid this exposure, the pure b-emitters 32 P<br />

and 90 Y have been favoured during the last decade and have become the predominant<br />

radioactive isotopes for many therapeutic applications. Recently, however, it has been<br />

shown that a certain amount of low-energy g-radiation can actually be useful for<br />

imaging, either during or after the application of the radioactive microspheres [27].<br />

During infusion, with the help of a g -camera or g-detector, the surgeons are able to a)<br />

direct the radioactive microspheres and b) adjust the necessary amounts of<br />

radioactivity.<br />

Short-lived radioisotopes (Table 3) can be used to optimise radiobiological aspects<br />

of therapy. Specifically, it has been shown that not only the total dose, but the dose-rate<br />

is very important for the treatment outcome in radiotherapy [28]. Short-lived<br />

radioisotopes such as 165 Dy or 188 Re pack the "punch" into a much shorter time-period,<br />

allowing less time for tumours to recover and grow back. Although much more<br />

research is required in this area, many of the radioactive b-emitting lanthanides are seen<br />

as promising candidates for local or directed radiotherapy, with microspheres serving as<br />

the delivery system. The dosimetry of b-emitting radioactive microspheres depends on<br />

the application. In the simplest case, when the radiopharmaceutical is distributed<br />

homogeneously throughout the target (tumour) area, the MIRD scheme is used [3 1,321.<br />

MIRD calculations can be done on a PC [using a program provided free to the<br />

interested user] [33]. Harbert's calculations are used when the radiopharmaceutical is in<br />

a plane from which it irradiates the tissue [34] (Appendix K). This approach is, for<br />

example, appropriate in the treatment of cystic brain tumours or in radiosynovectomy<br />

(see below). Dosimetric modelling using Monte Carlo simulations can be used for<br />

microspheres of different sizes and different β-emitters [3 5-37].<br />

3.3. GAMMA-EMITTERS<br />

A large group of radioisotopes emits g-rays during decay. Gamma rays represent excess<br />

energy that is given off as the unstable nucleus breaks up and decays in its efforts to<br />

reach a stable form. The energy is emitted in the form of electromagnetic radiation<br />

(photons), with a radioisotope-characteristic photon energy typically expressed in kiloelectronvolt<br />

(keV). Photons are absorbed in biological material by both the<br />

photoelectric and Compton process, and then indirectly ionise the surrounding atoms,<br />

producing chemical and biological changes. Most g-emitters are used primarily for<br />

diagnostic purposes and those used in nuclear medicine (Table 4) were chosen so that<br />

a) their g-ray energy is not too high (radiation safety concerns) and matches the gcamera,<br />

b) their half-life is practical and logistically feasible, c) they are easily<br />

available and inexpensive, and d) they can be bound to microspheres in an easy (kit)<br />

and stable fashion.<br />

220

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