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Low Voltage
Organic Field Effect Transistors with Solution-Processed,
High-k BTO/Epoxy
Nanocomposite Dielectric Gate Insulator
Abstract
Organic Field Effect Transistors (OFETs), whose
characteristics are modulated by an electric filed, are a prominent constituent
of modern microelectronics. Since they were first introduced by Tsumura et
al. in 1986, they have undergone great progress, especially during the last
several years. Currently, OFETs can rival the performance of Field Effect
Transistors (FETs) based on amorphous silicon (a-Si:H). OFETs are particularly
interesting as their fabrication processes are more cost effective and much less
complex compared with conventional silicon technology, In general,
low-temperature deposition and solution processing can replace the
high-temperature and high-vacuum deposition and sophisticated photolithographic
pattering involved in conventional silicon technology. Additionally, the
mechanical flexibility of organic materials makes them compatible with flexible
substrates for lightweight and foldable products.
In many
practical situations where low cost, “disposable electronics” products may be
applied, cost restrictions will limit the available operational voltage. It is
thus paramount to develop organic electronic circuits that can operate with low
switching voltages. However, traditional OFETs often suffer from high operating
voltage due to the low charge carrier mobilities of organic semiconductors.
Since the field-induced current is proportional to the field-induced charge
density and carrier mobility, one approach to overcome this problem is by using
a high dielectric constant (high-K) gate insulators which can enhance the
field-induced carrier density. However, most high-K materials used for OFETs
fabrication so far are based on ceramics and hence are usually brittle and
expensive to prepare. Additionally, the poor mechanical properties of ceramic
materials makes it significantly challenging to utilize these materials in
flexible electronics. The preparation of these high-K materials requires high
temperature annealing process, which is not compatible with plastics
substrates. Consequently, it is necessary to develop a low cost and solution-processable
method to fabricate gate insulators with a high dielectric constant and
mechanical flexibility.
Traditional OFET research has focused mainly on the development of organic
semiconductor materials. Enhancing the mobility of the semiconductor material
has been achieved through rigorous research carried out by several
organizations. Considering the importance of device stability to the future of
organic electronics and the role that the dielectric must play, there has been a
conspicuous lack of effort devoted to this issue. Research into OFET gate
insulators is beginning to receive increased attention and is rapidly
establishing itself as a line of research equally for organic electronics as the
‘traditional’ OFET research themes that address the organic semiconductor
itself, and circuit engineering.
Research Scope
My
research focuses on the development and characterization of a novel high K
solution-processed nanocomposite dielectric layer for low voltage OFET gate
insulator. This work is protected by a patent disclosure being pursued by
Motorola. The Nanocomposite is a specialty material developed specifically for
this research project by Hutsman of Switzerland.
Bottom contact OFETs (Figure 1) are fabricated using a combination of pad
printing and spray coating technologies. An aluminum coated Mylar film is used
as the gate substrate. A Nanocomposite consisting of cross-linked Propylene
Glycol Methyl Ether Acetate and Barium Titanate (BTO) nanoparticles was
developed as the gate insulator. The bimodal Nanocomposite utilized had two
different filler particle sizes; 200 nm. and 1000 nm. diameter particles. Due
to the nanosize of the BTO, it disperses well in the organic solvent, which
makes it possible to use solution-processable methods, such as pad printing to
fabricate the devices. Various Nanocomposite thicknesses were evaluated.

Figure 1. Bottom Contact OFET Structure
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