Materials Chemistry and Physics 77 (2002) 826–830
Spectroscopic characterization of chromium in sol–gel derived silica
Vinoy Thomas, Gin Jose, Gijo Jose, P.I. Paulose, N.V. Unnikrishnan
∗
School of Pure and Applied Physics, Mahatma Gandhi University, Priyadarsini Hills P.O., Kottayam 686 560, Kerala, India
Received 11 September 2001; received in revised form 18 March 2002; accepted 26 March 2002
Abstract
Trivalent chromium was introduced into silica gel monoliths, prepared via sols obtained from tetraethylorthosilicate and metal salts at
constant pH (pH = 3). Gels were heat-treated up to 900
◦
C. The optical properties of the silica glass and its in-process gel, including the
ultraviolet–visible (UV–VIS) absorption spectra, Fourier transform infrared (FTIR) spectra, fluorescence emission spectra were measured
and analyzed. The UV visible spectra of the gels dried at 60
◦
C indicated only the presence of Cr
3+
ions and no Cr
6+
(∼345 nm) ion was
observed. Electron spin resonance studies showed that concentration of Cr
5+
increased with increasing heat treatment temperatures. The
FTIR spectra showed that high temperature heat treatment can greatly reduce the amount of OH groups and organic residues in the silica.
It was also observed that a high OH content contributes to the fluorescence inefficiency of the gels as well as porous glass.
© 2002 Elsevier Science B.V. All rights reserved.
Keywords: Sol–gel; Optical materials; FTIR spectroscopy
1. Introduction
Sol–gel methods are extensively used for preparation
of optical materials by incorporating different cations or
molecules in a silica host [1,2]. First row transition metal
ions [3,4] and rare-earth ions [5,6] have been utilised for this
purpose. The chromium ion is likely to play a central role in
the development of new solid state laser materials because
of its favourable absorption and emission properties [7]. In
recent years study of the optical properties of crystals and
glasses containing trivalent chromium has received a new
impulse connected both to the exploitation of these materials
as active media for infrared tunable laser, luminescent solar
concentrators and to the fundamental understanding of the
interaction between impurity and host lattice [8–10]. Doped
glasses obtained via thermal densification of the correspond-
ing gels show similar properties with that of the melt route
glasses [11]. Thermal treatment of the doped gels changes
the local environment of the metal ions due to various rea-
sons resulting in fluorescence spectra. Though this behavior
is common for most of the modifier ions doped gels studied,
a detailed study of the incorporation of Cr
3+
ions in sol–gel
silica host is yet to be well established. Since the optical
properties of the doped silica systems depend on the local
structure and bonding of the dopant cations [11], a detailed
understanding of the structural evolution during the gel to
∗
Corresponding author. Tel.: +91-481-597923; fax: +91-481-597731.
E-mail address: spapf@sancharnet.in (N.V. Unnikrishnan).
glass conversion of Cr
3+
doped silica gels is very important
to fabricate the material for optical applications. This short
communication focuses on the spectroscopic properties of
the gel derived monolithic Cr
3+
doped silica glasses.
2. Experimental
Silica sols containing 0.1, 0.2 and 0.5 equivalent mol%
Cr
2
O
3
were prepared from tetraethylorthosilicate (TEOS)
(Fluka purum grade), Cr(NO
3
)
3
·9H
2
O (Merck, India),
doubly distilled deionised water and high purity HNO
3
and NH
4
OH. The desired amount of Cr(NO
3
)
3
·9H
2
O dis-
solved in deionised water in the presence of HNO
3
was
poured in TEOS under stirring at room temperature. The
TEOS/H
2
O/HNO
3
molar ratio was 1:14:0.01. The pH of the
sols was adjusted to a value of 3 by adding NH
4
OH. The
sols were cast in petridishes. The gels were aged for 1 week
at room temperature. Transparent crack-free dried mono-
lithic gels were obtained after drying for 14 days in air oven
at 60 ± 2
◦
C. The gels were heated at different temperatures
ranging from 200 to 900
◦
C in a programmable furnace with
the rate of 3
◦
C/h. (The gel with 0.5 mol% became opaque on
heat treatment and was not taken for further studies). Trans-
parent crack free and bubble free gels (diameter 30–35 mm,
thickness 2–2.5 mm) were reproducibly obtained. Optical
spectra of the gels and heat treated samples were recorded
with UV–VIS (Shimadzu-UVPC2401) and spectrophotoflu-
orimeter (Shimadzu-RFPC 5301). Thermogravimetric curve
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