Materials Science and Engineering B69 – 70 (2000) 182 – 193
Ellipsometric characterization of oxidized porous silicon layer
structures
T. Lohner
a,
*, M. Fried
a
, P. Petrik
a
, O. Polga ´r
a
, J. Gyulai
a
, W. Lehnert
b
a
Research Institute for Technical Physics and Materials Science, P.O. Box 49, H-1525 Budapest, Hungary
b
Fraunhofer -Institut fu ¨r Integrierte Schaltungen, Schottkystrasse 10, D-91058 Erlangen, Germany
Abstract
Electrochemically prepared porous silicon (PS) layers were oxidized thermally and investigated by spectroscopic ellipsometry
(SE). The SE spectra were measured in the range of 270–850 nm with a rotating polarizer ellipsometer. The PS was modelled as
a mixture of void and crystalline silicon or fine-grained polycrystalline silicon with enhanced absorption due to extensive
grain-boundary regions, i.e. the complex refractive index of the layer was calculated by Bruggeman effective medium approxima-
tion. The dielectric function of the fine-grained polycrystalline silicon was taken from the work published by G.E. Jellison, Jr.,
M.F. Chisholm, S.M. Gorbatkin, Appl. Phys. Lett. 62 (1993) 3348. The porosity, the layer thickness and the composition of the
oxidized PS layers were determined. Oxidation at 900°C was performed after a stabilizing heat treatment at 320°C. The oxidation
at 900°C for 10 min generated only a few nm silicon dioxide on single crystalline Si while in the case of PS with 57% porosity
nearly complete oxidation was found. For PS with 68% porosity complete oxidation was observed. © 2000 Elsevier Science S.A.
All rights reserved.
Keywords: Porous silicon; Oxidation; Spectroscopic ellipsometry; Optical modelling; Effective medium approximation
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1. Introduction
The application of porous silicon (PS) requires ap-
propriate control of the electrical and optical proper-
ties, which depend essentially on the morphology, the
porosity and the thickness. Due to the enhanced surface
area PS is a highly reactive material and sensitive to
ageing effects leading to modification of its properties.
The specific surface area of PS is very large: a few
hundred m
2
/cm
3
according to the morphologies
(‘columnar’ vs. ‘spongy’ like) [1].
Spectroscopic ellipsometry (SE) is a widely used non-
destructive method for characterization of PS layers
[2–16]. The depth inhomogeneity of PS layers was
investigated by Tho ¨ nissen et al. by SE, Raman spec-
troscopy and photoluminescence measurements [4].
They established that the thinning of the structure at
the surface is related to the effects of chemical etching
because of the increasing storage time of the topmost
layers in the electrolyte. A porosity graded layer model
was applied for porosity depth profiling of thin PS
layers using variable-angle SE by Pettersson et al. [13].
Krzyzanowska et al. investigated refractive index an-
isotropy of PS layers with columnar structure using
multiple angle of incidence ellipsometry [17]. The illu-
mination assisted formation of PS layers was studied by
Tho ¨ nissen et al. [18]. Molna ´r et al. applied SE for
characterization of PS layer fabricated using illumina-
tion for LED structures [12]. Quantitative adsorption
studies of protein molecules (human serum albumin
and fibrinogen) were performed in thermally oxidized
PS layers using SE [16]. Concerning the morphology
and pore structure of PS ion beam analytical methods
proved to be powerful techniques, for example one can
determine morphological details, as porosity, average
pore diameter and anisotropy of the pore directions by
investigation of the widening of the
16
O(,)
16
O nuclear
resonance peak [19,20].
Surface passivation of PS is an essential issue for
many device application. In PS structures designed to
operate as optical elements the atmospheric oxidation
of the inner surfaces modifies the dielectric function of
the layers. One approach to this is a passivation of PS
layers in rapid thermal oxidation process [6,21]. An-
other approach to this problem is thermal nitridation
* Corresponding author. Fax: +36-1-3959284.
E-mail address: lohner@mfa.kfki.hu (T. Lohner)
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