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- W1996979231 startingPage "11042" @default.
- W1996979231 abstract "Optical capacitance spectroscopy and thermal annealing of defects have been used to study both the electron traps ${mathrm{EP}}_{1}$,${mathrm{E}}_{11}$ and the dominant hole traps (${mathrm{H}}_{3}$-${mathrm{H}}_{4}$-${mathrm{H}}_{4}^{ensuremath{'}}$) produced by low-energy electron irradiation in Zn-doped p-type InP. This shows that the 1.1-eV onset in the photoionization cross sections (PCS's) previously attributed to (${mathrm{H}}_{3}$-${mathrm{H}}_{4}$) is actually due to the unrelated electron trap ${mathrm{EP}}_{1}$. The true PCS's ${mathrm{ensuremath{sigma}}}_{mathrm{p}}^{0}$ of (${mathrm{H}}_{3}$,${mathrm{H}}_{4}$) are compared with PCS tight-binding Green's function calculations to test the earlier proposal that the (${mathrm{H}}_{2}$-${mathrm{H}}_{3}$-${mathrm{H}}_{4}$-${mathrm{H}}_{4}^{ensuremath{'}}$,${mathrm{E}}_{11}$) series might arise from different states of (${mathrm{V}}_{mathrm{P}}$-Zn) complexes. The model yields an effective agreement as concerns both the energy location of the hole-levels series in the forbidden gap and the vanishingly small contribution to the PCS's of the four equivalent L valence-band minima. The proposal that ${mathrm{E}}_{11}$ might correspond to the ionization of an e state of the ${mathrm{V}}_{mathrm{P}}$-Zn complex also agrees with the experimental observation of both optical transitions to the valence band and to the conduction band but cannot account for the midgap position of ${mathrm{E}}_{11}$." @default.
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- W1996979231 date "1990-12-15" @default.
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- W1996979231 title "Optical properties of the main electron-irradiation-induced defects in<i>p</i>-type InP: Comparison with calculations for the isolated and acceptor-paired phosphorus vacancy" @default.
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- W1996979231 doi "https://doi.org/10.1103/physrevb.42.11042" @default.
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