The wide band gap semiconductor, GaN, has emerged as an important host for rare earth-electroluminescence. The annealing behaviour and lattice site location of Er implanted into GaN were studied with the Rutherford Backscattering Spectrometry (RBS)/channelling and photoluminescence (PL) techniques. Also Er site dependence on the annealing temperature and implantation dose has been studied in detail. The optical properties of the Er-doped GaN system, evidencing their dependence on the parameters adopted during the synthesis procedure (Er implantation dose, annealing temperature) have been discussed. RBS/channelling measurements suggested that mostly Er occupy substitutional site and depends on the Er concentration. The main result is the activation of a typical Er giving rise to PL emission in the 1450-1650nm range, related to radiative 4I 13/2→ 4I 15/2 transitions. Depending on the Er dose, we observe a specific behaviour linked to variation of the annealing temperature that strongly determines PL emission band. We observed a PL spectral shape with the main peak located at 1542nm and shoulder peak at 1558nm (and full width at half maximum (FWHM) of 33nm) with a series of weaker PL structures at 1519, 1572 and 1591nm, due to the Stark sub-level splitting. © 2012 Copyright Taylor and Francis Group, LLC.

Effects of concentration and thermal annealing on the optical activation of Er implanted into GaN layers

TRAVE, Enrico;
2012-01-01

Abstract

The wide band gap semiconductor, GaN, has emerged as an important host for rare earth-electroluminescence. The annealing behaviour and lattice site location of Er implanted into GaN were studied with the Rutherford Backscattering Spectrometry (RBS)/channelling and photoluminescence (PL) techniques. Also Er site dependence on the annealing temperature and implantation dose has been studied in detail. The optical properties of the Er-doped GaN system, evidencing their dependence on the parameters adopted during the synthesis procedure (Er implantation dose, annealing temperature) have been discussed. RBS/channelling measurements suggested that mostly Er occupy substitutional site and depends on the Er concentration. The main result is the activation of a typical Er giving rise to PL emission in the 1450-1650nm range, related to radiative 4I 13/2→ 4I 15/2 transitions. Depending on the Er dose, we observe a specific behaviour linked to variation of the annealing temperature that strongly determines PL emission band. We observed a PL spectral shape with the main peak located at 1542nm and shoulder peak at 1558nm (and full width at half maximum (FWHM) of 33nm) with a series of weaker PL structures at 1519, 1572 and 1591nm, due to the Stark sub-level splitting. © 2012 Copyright Taylor and Francis Group, LLC.
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/10278/38820
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