Flexible low-voltage organic phototransistors based on air-stable dinaphtho[2,3-b:2′,3′-f]thieno[3,2-b]thiophene (DNTT)
Graphical abstract
Introduction
Organic thin-film transistors (OTFTs) and circuits pose a promising way of manufacturing electronic systems with new properties, as they can be fabricated on flexible, large-area substrates [1], [2]. Applications range from organic active-matrix displays [3] and adaptive lighting panels to medical applications [4], wearable devices [5] or packaging [6]. Many of these applications require some sort of sensor, capable of extracting data from the environment, such as pressure, temperature, humidity or light. Imaging capabilities could potentially have the widest range of applications, as they can be used for example for photography, scanning, object or movement detection or range finding. Due to the high spatial resolution of typical image sensors, the required control and read-out logic tends to be sophisticated. Rigid image sensors have made a lot of progress in the past decades, and the majority of mobile consumer devices, such as smartphones and tablets, contain at least one of them. A flexible and printable version would be desirable and open up even more possible applications. Gesture or motion based interactions between humans and almost any surface or large-area scanning of objects are just some of the prospects. In 2005, Someya et al. demonstrated a flexible image sensor on a plastic substrate using organic photodiodes [7]. The fabrication process of organic imagers could, however, be simplified if efficient organic phototransistors (OPT) replaced the photodiodes. In the best case, these phototransistors are fabricated in exactly the same way as the logic transistors surrounding them without adding a substantial number of extra process steps. This would lead to an easy-to-integrate optical and electrical circuit on a common flexible substrate. This work aims to use existing, high-performance OTFTs [8] as photo-sensing elements, i.e., as OPTs, and poses the question if they are viable for a sensor application. In order to answer this question, the effect of illumination on the OTFTs has to be studied thoroughly. Furthermore, proper biasing sequences and read-out techniques have to be developed, which distinguish these opto-electric transducers from memory-type organic transistors [9], [10]. OPTs with various geometries and materials have already been investigated by other research groups within the past years [11], [12], [13], [14], [15], [16], [10]. However, the low-voltage operation of 2–3 V and the large effective mobility greater than 1.2 cm2/Vs at channel lengths as short as demonstrated in [8] encourage further investigation.
Section snippets
Fabrication
All transistors and phototransistors were fabricated in the inverted-staggered (bottom-gate, top-contact) configuration on a flexible polyethylene naphthalate (PEN) substrate using a set of 4 high-resolution silicon stencil masks [17]. First, a thin layer of gold (Au) was deposited by thermal evaporation in vacuum and patterned through a first stencil mask to define the routing (interconnect) layer. In the second step, aluminum (Al) was vacuum-deposited through a second mask to define the gate
Light-induced threshold voltage shift
Under illumination, the p-channel DNTT OPTs show a strong and slow threshold-voltage shift towards more positive values, which is attributed to the formation of an additional charge sheet caused by the trapping of photo-generated electrons. The trap centers are believed to be located either in the bulk of the AlOx (which the electrons can reach by tunneling through the thick SAM) or at the interface between the semiconductor and the SAM (perhaps at grain boundaries or other
Conclusion
The effect of illumination on high-performance, low-voltage, DNTT-based OTFTs was thoroughly investigated. With proper biasing, the absorption of UV/blue light in the p-channel organic semiconductor DNTT leads to a significant increase in the density of free electrons, which can be trapped in the AlOx of the gate dielectric or in the semiconductor, at grain boundaries or structural defects reaching the interface of the SAM. This produces a strong but slow threshold voltage shift that translates
Acknowledgments
The authors gratefully acknowledge Prof. Kazuo Takimiya (Center for Emergent Matter Science, RIKEN, Wako, Saitama, Japan) for providing the organic semiconductor DNTT employed in this study, Harald Richter for his valuable input and Marion Hagel for wire-bonding of the flexible substrates. This work was partially funded by the German Ministry of Education and Research (BMBF) under Grant 1612000463 (KoSiF).
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