IOP PUBLISHING SEMICONDUCTOR SCIENCE AND TECHNOLOGY
Semicond. Sci. Technol. 23 (2008) 075028 (5pp) doi:10.1088/0268-1242/23/7/075028
Ion irradiation induced nitrogen mobility
in a GaInNAs quantum well laser
Y N Qiu
1
, G Papaioannou
2
, J Pozo
1
, J M Rorison
1
, M Saarinen
3
,
J Konttinen
3
, J Viheri¨ al¨ a
3
, P Leinonen
3
, T Jouhti
3
and M Pessa
3
1
Room 2.14 Queen’s Building, Department of Electrical Electronic Engineering, University of Bristol,
Bristol, BS8 1TR, UK
2
Solid State Physics Section, Physics Department, University of Athens, Athens 15784, Greece
3
Optoelectronics Research Centre, Tampere University of Technology, Tampere, PO Box 692,
FIN-33101, Finland
E-mail: yingningqiu@yahoo.com
Received 25 January 2008, in final form 17 April 2008
Published 23 May 2008
Online at stacks.iop.org/SST/23/075028
Abstract
Changes in the optical properties in GaInNAs/GaAs quantum wells after alpha particle
bombardment followed by low temperature annealing are reported. Both blue and red shifts of
the lasing wavelength are observed under different annealing conditions. This differs from the
usually observed blue shift which is found after high-temperature post-grown annealing.
Competing processes that result in the lasing wavelength shifts are energetic considerations
which act to increase the number of Ga–N and In–As bonds (maximize the cohesive energy),
minimizing the strain of the system which increases the number of In–N and Ga–As bonds
(large-ion-small-ion links), maximizing the number of N located at lattice sites effective at
shrinking the band-gap and moving the N position within the quantum well. For the case of
high-temperature post-grown annealing the increase of Ga–As and In–N bonding wins,
resulting in the blue shift observed. The wavelength shifts are discussed in terms of these
competing mechanisms.
1. Introduction
Dilute-nitride semiconductors based on GaInNAs/GaAs
quantum well (QW) structures have attracted attention for
their potential applications in optoelectronic devices [1]. Post-
growth annealing has proved to be necessary to obtain high
optical emission intensity, but results in an undesirable blue
shift of the peak emission wavelength. For this reason, much
work has been done to understand the mechanisms responsible
for this blue shift leading to various and conflicting possible
explanations. Amongst these, some support that neither In
nor N diffuse out of the QW [2–4], although others suggest
that both atoms do [5–7]. Other studies appear to show
that only the In diffuses out of the QW [8, 9], while other
observations support that only N diffuses out of the QW
[10]. The diffusion issue led also to an uncertainty as to
whether it occurs entirely within the QW on the order of a few
atomic lengths [11] or through a nearest-neighbour relaxation
involving interstitial–substitutional positions [2, 12]. The
effect of electron radiation induced defects and subsequent
annealing on the blue shift has been also investigated [13].
Monte Carlo simulations [14] show that theoretically the most
stable state is that which increases the number of Ga–As and
In–N bonds and this predicts a blue shift. This results from
a competition of cohesive energy and strain effects. Finally,
theoretical calculations based on the band-anti-crossing (BAC)
model have shown that the blue shift can be also connected to
the redistribution of nitrogen atoms in the QW [15]. Recent
work on bulk GaInNAs annealed at a higher temperature
than reported here, but still low relative to the usual QW
annealing, has reported [16] an observed PL red shift which
has been attributed to N moving from interstitial to site
locations following the irradiation and annealing (There is
no consideration of whether the N becomes bonded to In or
Ga or indeed how this changes with annealing temperature.)
This has been attributed to the N only being able to interact
with the GaInAs conduction band and push it down when the
N is located at a lattice site. These results show that short
range ordering effects within the GaInNAs/GaAs QW can
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