MODELING OF METAL-OXIDE-SEMICONDUCTOR CAPACITOR ON INDIUM GALLIUM
NITRIDE
1- CHANNEL MODEL
Tarik Menkad
1
, student member, IEEE, Dimiter Alexandrov
1,2
, and Kenneth Scott A. Butcher
1,2
1
Semiconductor Laboratory, Department of Electrical Engineering, Lakehead University, 955 Oliver Rd, Thunder Bay P7B 5E1, Ontario,
Canada.
2
Meaglow Ltd, 1294 Balmoral St, Suite 150, Thunder Bay P7B 5Z5, Ontario, Canada
ABSTRACT
A new analytical model for a two terminal metal-oxide-
Gallium Nitride/Indium Gallium Nitride heterojunction structure is
presented. This model characterizes the space charge layer created
by electron tunneling in the structure’s channel which is made of
intrinsic Gallium Nitride. A one dimensional (1-D) analysis is
adopted, and a set of hypotheses is stated to frame the present
work.
Index Terms— Gallium Nitride GaN, Indium Gallium
Nitride In
0.5
Ga
0.5
N, excitons.
1. INTRODUCTION
Excitons found in In
x
Ga
1-x
N alloy are used as a basis for the
design of a high frequency field effect transistor [1]. This transistor
uses excitons as a quantum source of free electrons for its channel
made of intrinsic Gallium Nitride. Electrons, under the influence of
an external electric field, move in an intrinsic material and
experience reduced scattering. The high mobility in the channel
allows low-noise and high-speed performance. The metal- oxide-
semiconductor on In
0.5
Ga
0.5
N capacitor, which forms the core of
this high-frequency field-effect transistor, is the subject of the
present work. Quasi-static C-V characteristic are obtained. For this
purpose, a set of hypotheses are stated in order to set the scope and
the domain for the validity of this model.
Channel conductivity is modulated by the value of the free
electric charge present in the intrinsic GaN material. This charge is
due to electrons of excitons origin, which tunnel through the
i-GaN/p-In
0.5
Ga
0.5
N heterojunction. The determination of the
charge density distribution, the electric field through the channel
thickness, and the potential drop across the channel are essential to
relate the electric charge present on the gate to the corresponding
applied gate voltage. For this purpose, a channel model is
presented. The reader will realize that such a model is a standalone
entity and can be introduced separately from the device model, we
chose to do it the other way to demonstrate the need for such a
channel model in the analysis of the MOS capacitor on In
0.5
Ga
0.5
N.
2. MODEL
2.1. Nomenclature
ࡳࢍ
Front gate to back substrate voltage
ଵ
,
ଶ
Potential drop across In
0.5
Ga
0.5
N pn junction
and across the space-charge layer in p-type
In
0.5
Ga
0.5
N side of the i-GaN/p-In
0.5
Ga
0.5
N
heterojunction
ଷ
,
ସ
Potential drop across i-GaN, oxide layers
ݐ
௫
ݐ,
ே
Oxide and GaN layers thicknesses.
ᇱ
,
ே
ᇱ
Charge per unit area on the gate, in GaN layer
ூ
బ.ఱ
బ.ఱ
ே
ᇱ
Charge per unit area in space charge region
located in p-type In
0.5
Ga
0.5
N
side of the i-GaN/p-In
0.5
Ga
0.5
N heterojunction.
Free electron concentration present in intrinsic
Gallium Nitride layer.
ܨ
Electric field in GaN layer at the i-GaN/p-
In
0.5
Ga
0.5
N heterojunction.
,
Thermal equilibrium hole and electron
concentrations in p-In
0.5
Ga
0.5
N.
ߝ
௫
ߝ,
ே
Relative permittivity of oxide and GaN
ߝ
ூ
బ.ఱ
బ.ఱ
ே
ߝ,
Relative permittivity of In
0.5
Ga
0.5
N, and
permittivity of vacuum.
ݑ
Thermal voltage
q Elementary charge
2.2. Set of hypotheses
1) Consider a 1-D dimension model.
2) The oxide material is considered an ideal insulator, no trapped
charges exist.
3) The GaN surface at the interface oxide/GaN is considered to be
ideal, with no defects or traps or recombination centers near the
surface.
4) All semiconductors are considered to be non degenerate, so that
Boltzmann statistics can be used.
5) No temperature gradient is present. The device dimensions are
small enough, that we assume that heat distributes evenly
throughout the device.
6) Polarization is not considered; so that displacement and electric
vector fields are directly proportional.
2012 25th IEEE Canadian Conference on Electrical and Computer Engineering (CCECE)
978-1-4673-1433-6/12/$31.00 ©2012 IEEE