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Investigation of self-focusing effects in wurtzite InGaN/GaN quantum dots
H. Kaviani
a
, A. Asgari
a,b,∗
a
Research Institute for Applied Physics, University of Tabriz, Tabriz 51665-163, Iran
b
School of Electrical, Electronic and Computer Engineering, The University of Western Australia, Crawley, WA 6009, Australia
a r t i c l e i n f o
Article history:
Received 5 September 2011
Accepted 11 January 2012
Keywords:
Nonlinear optic
InGaN QDs
Self-focusing effects
a b s t r a c t
The third-order nonlinear optical properties in wurtzite InGaN/GaN pyramid and truncated-pyramid
quantum dots are studied, and the oscillator strength, third-order nonlinear optical susceptibility and
self-focusing effects are analyzed theoretically taken into account the strong built-in electric field effect
due to the piezoelectric and spontaneous polarization in nitride materials. The numerical results clearly
show that the quantum dot (QD) size of InGaN/GaN have a significant influence on the nonlinear optical
properties of wurtzite InGaN/GaN quantum dots. Furthermore, the self-focusing effect increases with
decrease in size of QDs.
© 2012 Elsevier GmbH. All rights reserved.
1. Introduction
In recent years, III-nitride alloys have been the wide research
subjects due to practical applications in the field of optoelectronic
devices, high thermal conductivity, high electron-saturated drift
velocity and small dielectric constant [1,2]. These materials have
direct wide band gaps from 0.7 eV to 3.42 eV at room temperature,
therefore, they are so useful in blue light emitting diodes industrial
[3–5].
III–V nitride materials are founded in two different type struc-
tures: (i) wurtzite (WZ) [6] and, (ii) zinc-blend (ZB) [7]. In wurtzite
structures, electronic states and optical properties are highly
affected by the built-in electric field due to spontaneous (P
s
) and
piezoelectric (P
z
) polarizations. The magnitude of the built-in elec-
tric field is estimated to be in the order of MV/cm. These properties
do not exist in ZB structures, because they have high crystal sym-
metry [8–10]. Among III-nitride quantum dots (QDs) are already
acknowledged as quantum nanostructures with high potentials
in optoelectronic field; for instance, in light emitting diodes
(LEDs), laser diodes (LDs), optical memories and single electron
transistors [11–13].
In this nanometer scale semiconductors, the charge carriers
(electrons and holes) are confined in all three dimensions [14,15]
and due to the modification in the density of states, these quantum
nanostructures are expected to exhibit enhanced optical non-
linearities and enhanced electro-optic effects. Indeed many of
these optical nonlinear properties associated with intersubband
transitions those due to large dipole transition and very large oscil-
∗
Corresponding author at: Research Institute for Applied Physics, University of
Tabriz, Tabriz 51665-163, Iran. Tel.: +98 411 339 3005; fax: +98 411 334 7050.
E-mail address: asgari@tabrizu.ac.ir (A. Asgari).
lator strength, these optical intraband nonlinear are large too. As
the intrasubband dipole length extend over the QDs which are in
nanometer ranges [16,17]. Compare to bulk semiconductors, QD
semiconductors have larger third-order nonlinear susceptibility
[18,19].
One of the most interesting effect associated with third order
susceptibility (
3
) is the self-focusing. It is typical type of nonlinear
wave propagation that depends critically on the transverse profile
of the beam. Self-focusing of the light is the process in which an
intense beam of light modifies the optical properties of a material
medium in such a manner that the beam is caused to come to a
focus within or outside the material [20].
In this paper in order to understand the optical nonlinearity in
QDs and its application as self-focusing effects, first we assume two
different shapes of wurtzite In
x
Ga
1-x
N QDs (pyramid and truncated
pyramid), then we calculated the Schrödinger equation in presence
of the built-in polarization electric field in the framework of the
envelope function, and the effective mass theory. The third-order
nonlinear susceptibility of the taken QDs as function of DQ’s size
is investigated. Finally, the effects of QD size and shape on self-
focusing effects have been analyzed.
2. Theoretical model
To model the device, two pyramid and truncated-pyramid
shaped InGaN wurtzite QDs embedded in GaN material are
assumed. The proposed structure has been shown in Fig. 1.
In order to study the electronic structures, different methods
have been experienced [21–24]. The single band method is used
0030-4026/$ – see front matter © 2012 Elsevier GmbH. All rights reserved.
doi:10.1016/j.ijleo.2012.01.012