Charge carriers of both signs are produced in the bulk of anthracene single crystals by strongly absorbed light of λ < 300 nm. The overlap time of the electron and hole spatial distributions in this case depends on the relative drift velocity in an applied electric field E separating these distributions and on the penetration depth of the light. During this time recombination losses occur. The experimental drift current pulses obtained with λ = 280 nm light are explained quite well by a theory worked out for this model. A bimolecular recombination coefficient γ between 10−5 and 10−6 cm3/s is found, in agreement with results by other methods, depending somewhat on crystal quality and purity. For λ = 250 nm light, which is absorbed stronger than λ = 280 nm by a factor of about 100 and where the charge carriers therefore should be produced in a much narrower region, strange results are obtained (γ ∼ E2), possibly caused by flat traps or by diffusion.
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Karl et al. (1971) studied this question.
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