Abstract

Measurements have been made of the yield of slow positrons from Ag(100), polycrystalline Au, Pb and Sn, and 8 Å, SiO 2 Si . The measured dependence of the total yields of re-emitted positrons upon incident positron energy indicates that only epithermal positron emission is observed from these samples. By fitting the data using a procedure more commonly applied to the evaluation of thermal diffusion lengths by slow-positron implantation spectroscopy the length L T, over which positrons are reduced in energy from ∼ 10 1 eV to below the positron work function, has been determined. L T is related to the positron thermalisation length. The largest value of L T of 24 ± 3 A ̊ is for the SiO 2 Si structure, attributed to the absence of a strong energy loss mechanism for positrons with energies below the SiO 2 Si bandgap(s). By assuming that the most significant effect on the positron yield at the lowest incident energies is the size of the positive surface potential step, work-function values have been deduced for the polycrystalline metallic samples of 0.9 ± 0.25 eV for Au and Pb, and 0.8 ± 0.25 eV for Sn.

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