Investigation of the Molecular Organization in
Langmuir-Blodgett Films Using Polarized Infrared
Spectra: Comparison of Two Methods
H. Hui-Litwin,
†
L. Servant,*
,‡
M. J. Dignam,
§
and M. Moskovits
Department of Chemistry, University of Toronto, 80 Saint George Street, Toronto,
Ontario M5S 1A1, Canada
Received June 24, 1997
X
We compare two methods for obtaining structural information on Langmuir-Blodgett films from polarized
infrared spectroscopy. For sufficiently uniform films, we have already shown (refs 11 and 12) that all
polarized spectroscopic properties could be characterized by a single quantity that we call the “electrical
surface susceptibility tensor”, γ ˜ . The imaginary parts of the susceptibility tensor could be readily obtained
from reflectance measurements with the electric field parallel (Im(γ
t)) and perpendicular (Im(γn)) to the
plane of the film, independently of any specific properties of the film. This, in turn, could be related to
the characteristics of individual molecules comprising the film, and their geometric disposition if the
molecules are assumed to be interacting dipoles, which corrects, to a large extent, for the local field effects.
We report the results of an infrared study performed on a dipalmitoylphosphatidylethanolamine monolayer.
Attenuated total reflection spectra for both s and p polarization were recorded, and the spectra of Im(γ
t)
and Im(γ
n), as well as those of the imaginary part of the refractive index (kt and kn), are presented. Finally,
the information deduced from the Im(γx) and kx (x ) s, p) are compared, and the molecular orientation
is discussed both in terms of Im(γ
x) and kx. We show that by using this approach one obtains more
truthworthy measurements of the disposition of oriented molecules at surfaces than those obtained from
absorption coefficients.
1. Introduction
Organic thin films offer an attractive method of design-
ing molecular materials for various applications. The
properties of such films arise not only from the specific
characteristics of the molecules but also from their
arrangement within the film.
1,2
Polarized infrared spec-
troscopy has been widely used to obtain information on
molecular organization. Since the infrared (IR) absorption
depends on the relative orientation of the incident electric
field and of the dipole transition moment belonging to the
molecular vibration, it is possible to obtain information
on the orientation of the molecules by using polarized
radiation.
In most studies incorporating this approach, the re-
flectance spectra of a film lying on a substrate are recorded
for the electric field parallel and perpendicular to the
incident plane. The reflectance is defined as the ratio of
the reflected intensity of the film-covered substrate to
that of the bare substrate. The results are then discussed
in terms of a three-phase stratified model, with an
anisotropic film of thickness d, lying between the ambient
and the substrate phase.
3-6
Here, the connection between
the spectroscopic observables and the mean molecular
orientation can be derived in principle, but it is not a simple
one. The problem arises from the contribution of the
radiation-induced dipole moment to the local electric field
experienced by the oscillators. In general, the local electric
field acting on a molecule is modified by the electric field
radiated by all the surrounding induced dipoles. As a
consequence, in an anisotropic medium, the effect of the
local field is to alter the direction of the transition moments
so that they do not correspond with those of an equivalent
set of well-separated molecules. As pointed out by several
authors,
1,2
the problem of taking into account local field
effects in evaluating molecular parameters is not a simple
task.
3-10
The Lorentz-Lorenz local field expressions are
likely to be invalid for ordered Langmuir-Blodgett (LB)
systems, where more detailed calculations are required.
7
With this in mind, we developed a new approach to
evaluate the optical response of an anisotropic molecular
layer, taking into account the local field effect, and directly
connecting it to measurable spectroscopic quantities.
11-15
We show in particular, that the reflectance spectra of a
thin uniaxial film lying on a substrate could be understood
by considering the elements of a single tensor: the electric
surface susceptibility tensor (γ ˜ ), which is related simply
to the density of the induced dipoles per unit area. In
addition, we show that the imaginary parts of the
tangential and normal components of γ ˜ (Im(γ
t
) and Im-
(γ
n
)) could be readily obtained directly from the experi-
mental data, without any assumptions regarding film
†
Now at Centre for Infection and Biomaterials Research, The
Toronto Hospital, Bell Wing, Ground Fl., Rm. 631, 200 Elizabeth
St., Toronto, ON M5G 2C4, Canada.
‡
Now at Laboratoire de Spectroscopie Mole ´ culaire et Cristalline,
URA 124 CNRS, Universite ´ Bordeaux I, 351, Cours de La Libe ´ration,
33405 Talence Cedex, France. Author to whom correspondence
should be sent.
§
Deceased.
X
Abstract published in Advance ACS Abstracts, December 1,
1997.
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7211 Langmuir 1997, 13, 7211-7216
S0743-7463(97)00676-8 CCC: $14.00 © 1997 American Chemical Society