IOP PUBLISHING SEMICONDUCTOR SCIENCE AND TECHNOLOGY
Semicond. Sci. Technol. 23 (2008) 045005 (6pp) doi:10.1088/0268-1242/23/4/045005
Barrier inhomogeneities of tungsten
Schottky diodes on 4H-SiC
A Ferhat Hamida
1
, Z Ouennoughi
1
, A Sellai
2
, R Weiss
3
and H Ryssel
3
1
Laboratoire Opto´ electronique et Composants, D´ epartement de Physique, UFAS S´ etif, Algeria
2
Physics Department, PO Box 36, Sultan Qaboos University 123, Oman
3
University Erlangen-Nurnberg, Chair of Electron Devices, Cauerstrasse 6, 91058 Erlangen, Germany
E-mail: ouennoughi@gmail.com
Received 26 December 2007, in final form 29 January 2008
Published 26 February 2008
Online at stacks.iop.org/SST/23/045005
Abstract
Electrical properties of tungsten on silicon carbide (4H-SiC) Schottky diodes are investigated
through the analysis of the forward current–voltage (I–V) characteristics measured at elevated
temperatures within the range of 303–448 K. The subsequently derived Schottky barrier
heights (SBHs) and ideality factors are found to be temperature dependent with distributions
that are adequately explained within the framework of the model proposed by Tung in which
he considers the barrier at a metal–semiconductor interface as consisting of locally
non-uniform but interacting patches of different barrier heights embedded in a background of
uniform barrier height. A uniform barrier height of 1.248 eV, a Richardson’s constant of
129.95 A cm
−2
K
2
and a factor T
o
of 23.92 K obtained agree very well with values published
previously for similar Schottky barrier systems. Therefore, it has been concluded that the
temperature-dependent I–V characteristics of the device can be successfully explained with
lateral inhomogeneities distribution of the SBH.
(Some figures in this article are in colour only in the electronic version)
1. Introduction
Due to its physical and electronic properties, silicon carbide
(SiC) has demonstrated a better performance compared to Si
or GaAs when operating at high temperatures and/or high
level voltage bias. The promising properties of SiC for the
fabrication of high quality devices depend to a large degree on
the quality of the metal–SiC contact. Although most of the
devices are usually made using Si-face 4H-SiC substrates due
to good surface morphology and the possibility of having low
doping concentrations required for high power applications,
C-face 4H-SiC has recently been the focus of much attention
due to its different properties. The advantages of C-face
4H-SiC include high channel mobility [1], low leakage
current [2], low dislocation densities, less susceptibility to
the formation of bunching steps, superior forward voltage
stability and suitability for epitaxial growth on low off-cut
angles or on-axis substrates [3]. It has been reported, in the
same context, that the Schottky contact on the C-face crystal
gives, in general, a significantly higher barrier height compared
to Si-face contacts. This is particularly true for Pt, Mo, Ti, Au
and Ni [4–6].
Studying the properties of this contact for different
metals and under various conditions is essential to a
clearer understanding and, eventually, better control of these
properties. Although several studies concerning Schottky
contacts have been carried out during the last few decades
[6–16], the current transport and the temperature dependence
of the barrier height (BH) in Schottky diodes formed on high
band-gap semiconductors, in particular, remain a topic of
current interest. SiC Schottky diodes often exhibit non-ideal
current–voltage–temperature (I–V–T) characteristics and
reveal an abnormal variation of barrier height
B
and ideality
factor (n) with temperature. This behaviour is generally
explained by inhomgeneities at the interface of the junction.
Broadly, two approaches have been used in recent years
to explain the experimental data and model the I–V–T
characteristics of Schottky barrier (SB) contacts. These are
based, namely, on models proposed by Tung [17] and Werner
and G¨ uttler [18]. In Werner’s model, the BH is supposed to
be distributed according to a Gaussian-type function which
will usually lead to an apparent BH that is both temperature
and bias dependent. To explain departures from ideality, Tung
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