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Conductivity induced by high LET particles

Radioactive a-sources are usually deposited on one electrode. Due to their high LET values, the range of a-particles in organic liquids is small. Range data which have been verified experimentally are compiled in Table 2. [Pg.186]

Since all of the energy of an a-particle is spent within the liquid, the value can be calculated just as in the case of the low LET radiation (see Equation 21). Values are compiled in Table 3. [Pg.186]

The Gfi(E = 0) values are much smaller than those for low LET radiation. From theoretical considerations it follows that the probability of escape of electrons from a track in the absence of an applied electric field is zero. The low yield observed is attributed to charge separation induced by 8-rays. Electrons with keV energy will become thermalized far away from their parent positive ions. The variation with [Pg.186]

Data from Ramy, J.P., Mesure de I energic moyenne necessaire pour crier une paire d ions dans les liquides dielectriques sous irradiation alpha, PhD Thesis, Uni-versite Paul Sabatier de Toulouse, 1971. [Pg.187]

Fission fragments produce dense ionization tracks from which electron escape is very low. Even at a field strength of 38 kV/cm, only 3% of the initial ionization is collected in liquid argon (Hitachi et al., 1987). [Pg.188]


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