GaN thin films have been doped with varying Er concentrations (0.01-10 at.
%) during molecular-beam-epitaxy growth. As expected, the visible and infra
red (IR) emissions, from photoluminescence (PL) and electroluminescence (EL
), are a strong function of Er concentration. We report on the determinatio
n of an optimum Er doping level for PL and EL intensity. Secondary ion mass
spectroscopy and Rutherford backscattering measurements showed that the Er
concentration in GaN increased exponentially with Er cell temperature. PL
and EL intensity of green emission at 537 and 558 nm, due to Er 4f-4f inner
shell transitions, exhibited a maximum at similar to1 at. % Er. IR PL inte
nsity at 1.54 mum, due to another Er transition, revealed the same maximum
for similar to1 at. % Er concentration. PL lifetime measurements at 537 nm
showed that samples with Er concentration <1 at. % had a lifetime of simila
r to5 mus. For Er concentration greater than or equal to1 at. %, the lifeti
me decreased rapidly to values below 1 mus. This concentration quenching is
believed to be due to a combination of Er cross relaxation and energy tran
sfer to GaN defects, eventually followed by precipitation. This conclusion
is supported by x-ray diffraction measurements. As a result, we have determ
ined that the optimum Er doping concentration into GaN is similar to1 at. %
. (C) 2001 American Institute of Physics.