Top left: A fragment of the cross section of
a "grid-electrode" organic
FET. The organic material in this study is poly(3-hexylthiophene)
and the insulator is a high-dielectric-constant material, TiO2.
Bottom: A photograph of an actual device with dimensions 10 x 14
mm2. Inset: Closeup of the area to be studied.
Arguably, one of the main challenges in achieving these goals
is finding a means of investigating the intrinsic electronic properties
of the charge carriers in organic FETs without the need for metallic
contacts that could interfere with the properties under study.
In FETs, the charge carriers are confined to a nanometer-thick
layer at the semiconductor–insulator interface, buried under
several layers of the device. This makes it difficult to experimentally
study injected charge carriers using some of the most informative
experimental techniques in the arsenal of physicists and chemsists,
including scanning tunneling microscopy, photoemission spectroscopy,
and inelastic x-ray and neutron scattering.
In this research, the scientists instead employed infrared light
to study the electronic processes in organic FETs that are based
on poly(3-hexylthiophene), a semiconducting polymer featuring exceptionally
high charge-carrier mobility. In such materials, charge carriers
can induce infrared vibrations of the polymer chain. In addition,
when these charges are displaced under the influence of an electric
field, they drag the local polarization cloud of the molecular
chains with them, forming so-called polarons. The scientists have
been able to employ infrared spectroscopy to directly probe the
vibrational modes and polarons in a functional organic FET device.
This information is difficult or impossible to obtain using other
experimental techniques.
The voltage-induced infrared absorption spectra
(Δαd) of the device. Employing infrared spectroscopy, the researchers
were able to directly probe the electronic excitations associated
with the injected carriers in a functional organic FET device:
infrared active vibrational modes of the polymer chain (sharp
resonances in the 1,000–1,500 cm-1 range) and polarons
(broad absorption band centered at 3,500 cm-1).
Furthermore, infrared spectromicroscopy can also be used to explore
the distribution of charges in the conducting channel of the FETs
with high spatial resolution, made possible by the exceptionally
high brightness and small focal-spot size of the infrared beams
at the ALS. Using the infrared Beamline
1.4.3, the researchers were able to acquire infrared spectra
from individual spots less than 10 microns in diameter. By scanning
the beam over the conducting channel of the device and measuring
the infrared spectra in different areas, they were able to map
out the density of the charge carriers in different regions and
examine its evolution as the applied voltage is increased. Comparisons
were made between FETs having insulating layers of either SiO2
or TiO2. The latter, having a high dielectric constant,
are much desired in FETs because they allow for a much higher density
of charge carriers in their channels than SiO2-based
FETs.
The variation of carrier density away from the injection contacts
in the area shown by the blue square in the figure at top, obtained
by spatially monitoring the spectroscopic fingerprints of the injected
charges using infrared microspectroscopy.
However, the measurements revealed severe restrictions of the
charge-carrier channel length for TiO2-based devices,
a significant departure from the behavior expected for an "ideal" FET,
in which the charge density increases linearly with voltage and
is uniform in the channel. This is particularly important if one
wants to use these insulators in chemical or biological sensors.
In general, these experiments indicate that infrared spectroscopy
and spectromicroscopy offer researchers unique tools to explore
physical phenomena at the nanoscale occurring at the semiconductor–insulator
interface in organic FETs. The team hopes to employ the same techniques
in the study of other materials in FET devices, including polymers,
organic molecular crystals, and transition-metal oxides.
Research conducted by Z.Q. Li, N. Sai, M. Di Ventra, and D.N.
Basov (University of California, San Diego); G.M. Wang, D. Moses,
and A.J. Heeger (University of California, Sant Barbara); and M.C.
Martin (ALS).
Research funding: National Science Foundation, Petroleum Research
Fund, and U.S. Department of Energy, Office of Basic Energy Sciences
(BES). Operation of the ALS is supported by BES.
Publication about this research: Z.Q. Li, G.M. Wang, N. Sai, D.
Moses, M.C. Martin, M. Di Ventra, A.J. Heeger, and D.N. Basov, "Infrared
imaging of the nanometer-thick accumulation layer in organic field-effect
transistors," Nano Letters 6, 224
(2006).
ALSNews Vol. 267, July 26, 2006 |