Buried‐Contact Organic Field‐Effect Transistor: The Way of Alleviating Drawbacks from Interfacial Charge Transfer

Author:

Hwang Taehoon12,Seo Jungyoon12,Tsogbayar Dashdendev12,Ko Eun12,Park Jisu12,Jeong Yujeong3,Han Songyeon3,Kim Hongdeok24,Choi Joonmyung24,Ahn Hyungju5,Lee Jihoon67,Choi Hyun Ho3ORCID,Lee Hwa Sung12ORCID

Affiliation:

1. Department of Materials Science and Chemical Engineering Hanyang University Ansan 15588 Republic of Korea

2. BK21 FOUR ERICA‐ACE Center Hanyang University Ansan 15588 Republic of Korea

3. Department of Materials Engineering and Convergence Technology Gyeongsang National University Jinju 52828 Republic of Korea

4. Department of Mechanical Design Engineering Hanyang University Seoul 04763 Republic of Korea

5. Pohang Accelerator Laboratory Pohang 37673 Republic of Korea

6. Department of IT Convergence Korea National University of Transportation Chungju 27469 Republic of Korea

7. Department of Polymer Science and Engineering Korea National University of Transportation Chungju 27469 Republic of Korea

Abstract

AbstractFacile charge transfer between source/drain (S/D) electrodes and organic semiconductor (OSC) channel is crucial for high‐mobility organic field‐effect transistors (OFETs). Herein, a novel OFET geometry is developed by modifying a top‐contact bottom‐gate device structure, termed a buried‐contact OFET, enabling close proximity between the S/D‐OSC interface and conducting channel, consequently decreasing the access contact resistance (RC,acc) and overall contact resistance (RC). Conventional post‐thermal annealing is combined with a burying pressure (pressure‐thermal annealing (PTA)). The synergistic effect of thermal and pressure annealings leads to the softened OSC layer enabling metal electrodes to bury inward by applied pressure. This process induces structural transitions from a top‐contact to buried‐contact configuration, as verified by atomic force microscopy and finite element simulations. Transfer line method and 4‐probe measurements revealed that PTA reduces the contact by 1/3 (65 kΩ cm) and the source‐to‐drain voltage waste due to charge injection from 52% to 31%. Consequently, the field‐effect mobility is four times higher than that of a conventional thermally annealed top‐contact OFET. The density of deep traps (Ntr) is mainly distributed in the OSC bulk responsible for charge injection. Remarkably, the Ntr decreased 30‐fold using PTA, resulting in a shallow sub‐threshold region and a threshold voltage close to zero.

Publisher

Wiley

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