2005 APS March Meeting
Monday–Friday, March 21–25, 2005;
Los Angeles, CA
Session P29: Transport and Electronic Structure of Organic Electronic Materials
11:15 AM–1:39 PM,
Wednesday, March 23, 2005
LACC
Room: 504
Sponsoring
Units:
DPOLY FIAP
Chair: Arthur Epstein, Ohio State University
Abstract ID: BAPS.2005.MAR.P29.1
Abstract: P29.00001 : Theory of Quantum Hopping In Metallic Polymers and Applications in Electronics*
11:15 AM–11:51 AM
Preview Abstract
Abstract
Author:
Vladimir Prigodin
(Department of Physics, The Ohio State University, Columbus, OH 43210-1106)
The low frequency electromagnetic response of highly conducting
polymers
(e.g., polyaniline and polypyrrole) in a metallic state$^{1}$,
when analyzed
within the standard theory of metals, is provided by an extremely
small
fraction of the total number of available electrons $\sim $ 0.1
{\%} (in
contrast to $\sim $ 100 {\%} for common metals such as Cu, Ag, or
Ni) but
with anomalous long scattering time $>$ 10$^{-13}$ s ($\sim $ 100
times
longer than for common metals). We show that a chain-linked
network of
metallic grains (the polymer's crystalline domains) connected by
resonance
quantum tunneling through strongly localized states in surrounding
disordered medium produces this behavior. The small fraction of
electrons is
assigned to the low density of resonance states and the long
scattering time
is related to the narrow width of energy levels in resonance.
Recently a new interesting phenomenon, an electric field effect, was
reported for the doped highly conducting polymers. Upon applying
the gate
voltage of a few volts the conductivity of the polymer film drops
by a
several orders of magnitude$^{2}$. This observation is in
conflict with the
fact that the electric field cannot penetrate into a conductor
further that
the `lattice constant', and therefore its effect on the polymer
film of
$\sim $ 100 nm thickness should be negligible. We suggest that
the field
effect in doped conducting polymers is an electric field induced
conductor-nonconductor transition described by the chain-linked
granular
model in the presence of mobile ions. The ion motion under the
gate voltage
is breaking the interdot percolation network by removing critical
hoping
sites and as a result producing the conductor-nonconductor
transition. The
experimental evidences for the present mechanism of field effect in
conducting polymers are presented.
\begin{enumerate}
\item R.S. Kohlman \textit{et al}.,\textit{ Phys. Rev. Lett}.
\textbf{78}, 3915 (1997).
\item A.J. Epstein \textit{et al}., \textit{Curr. Appl.
Phys.}\textbf{ 2}, 339 (2002).
\end{enumerate}
*Supported in part by ONR
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2005.MAR.P29.1