Positron motion in an electric field is studied experimentally by measuring the drift length of positrons in the space-charge region of a Au-Si surface-barrier diode. An electric field of the order of 10⁴ V/cm gives rise to a drift length from 2 to 3 {μ}m. The drift-diffusion approximation can explain positron transport up to an electric-field strength of 3×{}10⁴ V/cm. At 300 K we get a positron mobility of 120±{}10 cm²/V s in Czochralski-grown Si ([P]=7.4×{}10¹⁴ cm^-3), and the diffusion coefficient calculated from the Einstein relation is 3.0±{}0.25 cm²/s. Positron diffusion was measured without preparing a metal-semiconductor contact in high-purity floating-zone Si (10⁴ {Ω} cm) assuming the electric field can be neglected. The diffusion coefficient is 3.10±{}0.20 cm²/s, in good agreement with that based upon the positron mobility measured under an electric field.
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Mäkinen et al. (1990) studied this question.
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