An Ion-Activated Molecular Electronic Device
R. B. Dabke,
†
G. D. Singh,
‡
A. Dhanabalan,
†
R. Lal,
‡
and A. Q. Contractor*
,†
Departments of Chemistry and Electrical Engineering, Indian Institute of Technology, Powai, Bombay 400 076, India
Several molecular devices based on the electronic switch-
ing properties of conducting polymers have been de-
scribed previously and involve an addition/ removal of a
proton/ electron to/ from the polymer chain. This “dop-
ing” process creates charged topological defects such as
polarons or bipolarons, which act as charge carriers. In
the device presented here, we have attempted to produce
a topological defect without effecting an electron/ proton
transfer. Such a topological defect has been produced by
incorporating an ion-binding cavity in the polymer phase,
which undergoes a conformational change on occupation
of the cavity by the appropriate ion. Thus, anchoring 1 8 -
crown-6 in polyaniline results in the electronic switching
of the polymer device in the presence of as low as 10
-7
M K
+
ion concentration. That this switching is ac-
companied by a conformational change was confirmed by
measuring the mean molecular area of a Langmuir mono-
layer of polyaniline-crown film in the presence and
absence of K
+
. It was found that there is an increase and
then a saturation in the mean molecular area in response
to increasing concentrations of K
+
ions in the subphase,
a trend which is similar to the electronic conductivity
changes in the polymer film. This mechanism of switching
makes it possible to design molecular devices that re-
spond to a wide class of ionic species which need not
undergo electron transfer to trigger the device.
One of the goals in the area of molecular devices is to realize
an electronic gate that can be activated by a specific chemical
species.
1
A class of molecular devices based on the electronic
switching properties of conducting polymers was first described
by Wrighton et al.
2
A number of devices have since been
described,
3-5
in which the device responds to the presence of a
specific chemical species. The switching, in these cases, is a
consequence of the production/ consumption of protons or elec-
trons. We describe here an electronic switch which is activated
by the presence of a specific metal ion. The switching in the
present case is a consequence of binding of the metal ion to its
specific receptor, which is anchored in the polymer phase, and
the resultant conformational changes in the polymer system.
It is now well known that the electronic conductivity of
“conducting polymers” is sensitive to the chemical state of the
polymer. The electronic properties of such a polymer chain can
be described in terms of a band structure analogous to that of a
solid.
6
Changes in electronic conductivity can, in general, be
explained in terms of changes in the band structure caused by
local conformational defects in the polymer backbone. These may
be associated with a charge (polarons or bipolarons) or may be
uncharged (e.g., neutral solitons, in polymers with a degenerate
ground state). Charged distortions, polarons or bipolarons, may
be caused by the removal/ addition of one or two electrons,
respectively, from/ to the polymer chain (oxidation/ reduction),
resulting in so-called p-type/ n-type conductivity. It may also be
possible to create a conformational change in the polymer
backbone by causing a local perturbation by polarizing the
π-electron system without effecting a complete removal/ addition
of an electron. One way of doing this could be to bring a charged
species (a cation or an anion) in close proximity to the polymer
chain without actually effecting electron transfer from or to the
polymer chain. This can be done by incorporating within the
polymer matrix an ion-binding species such as, for example, a
crown ether. If the crown ether has a preferentially high binding
constant for a certain ionic species as compared to others, the
polymer would respond preferentially to that ion. In this context,
the recent reports on “secondary”, doping by MacDiarmid et al.
7,8
are relevant and will be discussed later.
There have been attempts at imparting ion specificity by
covalent linking of azacrown ethers to polypyrrole,
9
pseudorotax-
anes to polythiophene,
10
and, very recently, functionalization of
polythiophenes with calix[4]arene-based ion receptors.
11
These
systems do show an ion-specific response but at concentrations
as high as 10
-1
M of the metal ion in nonaqueous media. We
describe here a system that shows a response at concentrations
as low as 10
-8
M of the concerned metal ion in aqueous media.
In the present case, the system 18-crown-6/ K
+
has been
chosen for study in polyaniline. The occupation of the crown
cavity by the metal ion results in a local electrostatic field, which
causes a perturbation in the polymer backbone and a change in
the density of states in the band gap. These changes are observed
even at concentrations as low as 1 × 10
-8
M K
+
. This is
manifested at the macroscopic level as a change in the electronic
†
Department of Chemistry.
‡
Department of Electrical Engineering.
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Anal. Chem. 1997, 69, 724-727
724 Analytical Chemistry, Vol. 69, No. 4, February 15, 1997 S0003-2700(96)00487-8 CCC: $14.00 © 1997 American Chemical Society