Page 31 - Organic Electronics in Sensors and Biotechnology
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8    Chapter  One

               for these devices with such small dimensions at different tempera-
               tures down to 4.2 K. On the other hand, there have been many reports
               on the transport of various organic semiconductor materials with
               large channel length transistors at low temperatures with different
               measurement techniques. 41–45  To investigate the possible transport
               mechanisms which become dominant when scaling the device size
               from micron-scale down to nanoscale, we systematically fabricated
               thin-film field-effect transistors of a series of channel lengths from 5 μm
               down to 80 nm, with pentacene as the active organic semiconductor
               layer.  All the investigated transistors of different channel lengths
               were fabricated by the same nominal geometry ratio W/L = 10, for
               the purpose of consistent scaling.
                   Bottom-contact structures are preferred in the fabrication of
               nanoscale organic/polymeric thin-film field-effect transistors. To fab-
               ricate submicron devices, e-beam lithography is a commonly used
               tool in defining the electrode pattern. For top-contact structures,
               however, the lithography step has to be performed on top of the pre-
               deposited active organic layer, which can degrade the organic material
               upon immersion in solvent solutions during developing and liftoff
               steps, or damage the organic material while evaporating metal
               atoms onto it. Hence, the bottom-contact configuration is chosen over
               the top-contact one. A heavily doped n-type silicon wafer serves as
               the mechanical substrate and the gate. The single-crystal silicon sub-
               strate was heavily doped by n-type dopants (phosphorous or arsenic)
               so that the depletion in the silicon as a gate was minimized. To serve
               as conductive gate, the doping concentration of the Si substrate
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               needs to be higher than 3.74 × 10 /cm  for phosphorous dopant or
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                      18
               8.5 × 10 /cm  for arsenic dopant.  A SiO  layer that serves as the gate
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               dielectric was then thermally grown on the substrate. Transistors of
               channel length greater than 1 μm utilize a 100 nm thermally grown
               SiO  layer as the gate dielectric, whereas for nanoscale transistors, a
                  2
               5 nm SiO  layer as the gate dielectric was grown by rapid thermal
                        2
               annealing in dry oxygen. The electrode patterns were made by e-beam
               lithography. Metal electrodes with an adhesive layer (Ti was chosen)
               that improves sticking to SiO  were then deposited by e-beam evapo-
                                        2
               ration in high vacuum, followed by a liftoff process. If the Ti layer is
               thinner than the accumulation channel depth, then carriers are
               injected directly from the high work function metal layer atop the Ti
               layer, which remarkably reduces the series resistance. Therefore the
               Ti layer was chosen to be 1 to 3 nm thick. Gold was chosen as the
               electrode material, due to its high work function aiding the injec-
               tion of holes into organic material, its air stability, and its ability to
               form an ohmic contact with organic materials under certain optimal
               conditions.
                   Device fabrication was completed by subliming small organic
               molecules (e.g., pentacene) at different growth rates and different
               substrate temperatures for different grain sizes. Slower growth rates
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