Articles
Radiative and Nonradiative Excited State Processes for
Studying the Sol to Gel Evolution
M. Claudia Marchi, Sara A. Bilmes, and R. Martı ´n Negri*
Instituto de Quı ´mica Fı ´sica de los Materiales, Medio Ambiente y Energı ´a (INQUIMAE),
Departamento de Quı ´mica Inorga ´ nica, Analı ´tica y Quı ´mica Fı ´sica, Facultad de Ciencias
Exactas y Naturales, Universidad de Buenos Aires, Ciudad Universitaria, Pabello ´ n II,
(C1428EHA) Buenos Aires, Argentina
Received December 5, 2001. In Final Form: May 3, 2002
The sol to gel evolution of systems based on the hydrolysis of titanium n-butoxide, Ti(OBu
n
)4, in 1-butanol
was investigated by monitoring the changes of the radiative and nonradiative electronic excited state
processes of embedded dyes (cresyl violet and 4-(dicyanomethylene)-2-methyl-6(p-dimethylaminostyryl)-
4H-pyran). Fluorescence anisotropy experiments (FA) allow determination of changes in the microviscosity
of the medium surrounding the fluorophore through the sol-gel evolution. The increase of the anisotropy
parameter, 〈r〉, is explained in terms of solvent confinement in cavities enclosed within cross-linked polymeric
chains. The acoustic signal recorded in laser-induced optoacoustics experiments (LIOAS) is attenuated as
the system loses fluidity, with a minimum at t
g, thus providing an alternative method for determining the
gelation point. In addition, within the theoretical approach of percolation theory, the exponent of the
viscosity power law is obtained from the attenuation of the sound wave. Although both FA and LIOAS
provide information on the degree of cross-linking between polymeric chains, there is a clear difference
between the behavior of the macroscopic shear viscosity determined by LIOAS and the local friction or
microviscosity obtained from FA.
Introduction
The sol-gel process is a well-known low-temperature
synthesis method that uses molecular precursors, typically
metal alkoxides or halides,
1
to obtain ceramics, glasses,
and nanocomposites with wide applications in optics,
2,3
optoelectronics,
2,4,5
chemical sensors,
1,6
and matrixes for
molecules, cell and bacteria encapsulation,
7,8
and photo-
catalysts.
9,10
The properties of the final material are related
to the formation of a cross-linked network, which in turn
is determined by the kinetics of hydrolysis and condensa-
tion reactions involved in the sol to gel evolution.
Diverse methods have been employed for the study of
sol-gel materials, such as NMR with different isotopes,
11
small-angle X-ray or neutron scattering (SAXS or
SANS),
12,13
infrared and Raman spectroscopies,
14
and
dynamic rheological measurements.
15
However, these
methods usually report on average properties and are
insensitive to the local microenvironments within a
nanocomposite. We propose here a strategy based on the
radiative and nonradiative electronic excited-state re-
laxation of dyes included in the system, such as steady-
state fluorescence anisotropy (FA) and laser-induced
optoacoustic spectroscopy (LIOAS).
FA of chromophores is a well-known technique for the
study of microenvironments in micelles
16,17
that has also
been employed for monitoring the structure and aging of
sol-gel materials.
18-22
Briefly, the steady-state fluores-
cence anisotropy, 〈r〉, is a measure of the fluorescence
depolarization that is due to the rotation of the dye (as a
rigid body) during its excited-state lifetime. Thus, 〈r〉 gives
direct information on the friction exerted by the environ-
ment on the fluorophore; large values of 〈r〉 are related to
slow rotation of the dye or, in other words, to a high local
friction or microviscosity of the molecular environment
* To whom correspondence should be addressed. Fax: xx54-11-
4576-3341. E-mail: rmn@qi.fcen.uba.ar.
(1) Brinker, C. J.; Scherer, G. W. Sol-Gel Science. The Physics and
Chemistry of Sol-Gel Processing; Academic Press: San Diego, CA, 1990.
(2) Hench, L. L.; West, J. K. Chem. Rev. 1990, 90, 33.
(3) Sanchez, C.; Ribot, F. New J. Chem. 1994, 18, 1007.
(4) Livage, J.; Henry, M.; Sanchez, C. Prog. Solid State Chem. 1988,
18, 259.
(5) Sakka, S. Struct. Bonding 1996, 85, 1.
(6) Bronshtein, A.; Aharonson, N.; Avnir, D.; Turniansky, A.; Altstein,
M. Chem. Mater. 1997, 9, 2632.
(7) Livage, J.; Corandin, T.; Roux, C. J. Phys.: Condens. Matter 2001,
13, 2673.
(8) Avnir, D.; Braun, S.; Lev, O.; Ottolenghi, M. Chem. Mater. 1994,
6, 1605.
(9) Bilmes, S. A.; Mandelbaum, P.; Alvarez, F.; Victoria, N. J. Phys.
Chem. B 2000, 104, 9851.
(10) Calvo, M. E.; Candal, R. J.; Bilmes, S. A.; Environ. Sci. Technol.
2001, 35, 4132.
(11) Blanchard, J.; Ribot, F.; Sanchez, C.; Bellot, P.-V.; Trokiner, A.
J. Non-Cryst. Solids 2000, 265, 83.
(12) Krakovsky, I.; Urakawa, H.; Kajiwara, K.; Kohjiya, S. J. Non-
Cryst. Solids 1998, 231, 31.
(13) Margaca, F. M. A.; Miranda Salvado, I. M.; Teixeira, J. J. Non-
Cryst. Solids 1997, 209, 143.
(14) Schraml-Marth, M.; Walther, K. L.; Wokaun, A.; Handy, B. E.;
Baiker, A. J. Non-Cryst. Solids 1992, 143, 93.
(15) Panton, A.; Barboux-Doeuff, S.; Sanchez, C. Colloids Surf., A
2000, 162, 177.
(16) Laia, C. A. T.; Costa, S. M. B. Langmuir 2002, 18, 1494.
(17) Lakowicz, J. R. Principles of Fluorescence Spectroscopy, 2nd ed.;
Plenum Press: New York, 1999.
(18) Dunn, B.; Zink, J. I. J. Mater. Chem. 1991, 1, 903.
(19) Narang, U.; Wang, R.; Prasad, P. N.; Bright, F. V. J. Phys. Chem.
1994, 98, 17.
(20) Marchi, M. C.; Bilmes, S. A.; Negri, R. M. Langmuir 1997, 13,
3665.
(21) del Monte, F.; Ferrer, M. L.; Levy, D. J. Mater. Chem. 2001, 11,
1745.
(22) Keeling-Tucker, T.; Brennan, J. D. Chem. Mater. 2001, 13, 3331.
6730 Langmuir 2002, 18, 6730-6735
10.1021/la0117597 CCC: $22.00 © 2002 American Chemical Society
Published on Web 08/08/2002