Parylene-Based Double-Layer Gate Dielectrics for

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Supporting Information Parylene-Based Double-Layer Gate Dielectrics for Organic Field-Effect Transistors Hyunjin Park, Hyungju Ahn, Jimin Kwon, Seongju Kim, and Sungjune Jung *,, Department of Electrical Engineering, Pohang University of Science and Technology (POSTECH), 77 Cheongam-Ro, Nam-Gu, Pohang, 37673, Republic of Korea Pohang Accelerator Laboratory, 77 Cheongam-Ro, Nam-Gu, Pohang, 37673, Republic of Korea Department of Creative IT Engineering, Pohang University of Science and Technology (POSTECH), 77 Cheongam-Ro, Nam-Gu, Pohang, 37673, Republic of Korea Department of Mechanical Engineering, Pohang University of Science and Technology (POSTECH), 77 Cheongam-Ro, Nam-Gu, Pohang, 37673, Republic of Korea S-1

*E-mail: sjjung@postech.ac.kr S-2

Experimental Details Materials: The parylene C (dix-c, Daisankasei Co., Ltd.) and F (VT4, Suzhou Chireach Biomedical Technology Co., LTD.) were prepared as gate dielectric layers. For the bank solution, Cytop (CTL-809M, Asahi Glass) was dissolved in a fluorinate solvent (CT-Solv.180, Asahi Glass) in the volume ratio of 1:2. The semiconductor solution was prepared with a blend of 2.5 mg ml -1 TIPS-pentacene (> 99.9 %, Ossila) and 1.25 mg ml -1 PS (MW ~280,000, Sigma-Aldrich) dissolved in mesitylene (98 %, Sigma-Aldrich). Device Fabrication: The BGTC OFET was fabricated on a glass substrate (Eagle XG, Corning). A 50-nm-thick aluminum gate electrode was thermally evaporated through a shadow mask on the substrate. Parylene films were deposited by means of CVD, using a parylene coater (OBT-PC300, OBANGTECHNOLOGY), at near room temperature. For the DLGD structure, parylene F is deposited and parylene C is deposited. Then, Cytop solution was printed with dispenser equipment (350PC, Musashi Engineering, Inc.) to form the bank layer. The substrate and nozzle temperatures were maintained at 40 C during the dispensing process. After bank layer printing, the device was annealed S-3

on a hotplate at 100 C for 10 min to remove residual solvent. The solution of TIPSpentacene:PS blends was printed in the area defined by the bank layer with dispenser equipment. The substrate and nozzle temperatures were maintained at 30 C during the dispensing process. After semiconducting layer printing, the device was annealed on a hotplate at 70 C for 10 min to remove residual solvent. Finally, a 40-nm-thick silver was thermally evaporated through a shadow mask for the source and drain electrodes with channel width and length of 1000 and 50 μm, respectively. Characterization: The thickness of parylene-based films was measured with a stylus surface profiler (DektakXT, Bruker). The electrical characteristics of OFETs were measured in a dark box using a semiconductor parameter analyzer (4200-SCS, Keithley) under ambient conditions. The V GS was normalized to the thickness of parylene-based dielectrics as 1 MV cm -1. The capacitance of MIM capacitors was measured with a precision LCR meter (ZM2376, NF Corporation) within the frequency range of 1 Hz to 1 MHz. AFM images were recorded in tapping mode using an SPM system (Veeco Dimension 3100 + Nanoscope V, Digital Instruments/Veeco Metrology Group). The crystalline of TIPS-pentacene thin films was observed with a POM (Leica S-4

DM2700M, Leica). The 2D GIXRD was measured at the 3C beamline of the Pohang Acceleration Laboratory in Korea. S-5

Table S1. Device and electrical parameters of OFETs with parylene SLGDs and DLGDs. The dielectric thickness (t d ), dielectric constant (ε r ), characteristics trapping time constant (τ), and dispersion parameter (β) are averaged over five devices. The threshold electric-field (E TH ), field-effect mobility (μ FET ), on/off current ratio (I on /I off ), and subthreshold swing (SS) are averaged over ten devices. X [t C (t C + t F ) -1 ] t d [nm] ε r at 10 Hz E TH [MV cm -1 ] μ FET [cm 2 V -1 s -1 ] I on /I off [ 10 6 ] SS [V decade - 1 ] τ [ 10 4 s] β 1 (C) 168 3.74-0.08 0.12 0.04 10.2 10.1 0.26 0.04 12.9 4.7 0.63 0.05 0.78 216 3.30-0.09 0.13 0.05 4.90 2.34 0.52 0.45 7.8 2.9 0.56 0.05 0.71 238 3.13-0.08 0.14 0.05 3.38 2.67 1.19 1.44 8.6 6.4 0.55 0.04 0.63 265 2.99-0.09 0.15 0.03 7.16 6.72 0.93 0.54 10.1 4.1 0.54 0.01 0.58 291 2.90-0.07 0.13 0.05 9.40 5.60 1.75 1.69 12.3 7.5 0.48 0.03 0.41 241 2.70-0.11 0.03 0.14 1.86 1.79 1.28 1.02 15.8 11.1 0.44 0.03 0.33 211 2.59-0.14 0.07 3.34 1.72 11.3 0.38 S-6

0.03 3.05 1.27 5.3 0.05 0.26 191 2.44-0.14 0.05 2.13 1.83 2.54 2.24 10.0 7.7 0.37 0.05 0 (F) 141 2.17-0.15 0.03 0.09 0.04 3.39 3.03 1.42 1.49 6.3 1.1 0.37 0.02 * V GS = t d [nm] E GS [MV cm -1 ] * V TH = t d [nm] E TH [MV cm -1 ] S-7

Figure S1. Dielectric constants of MIM capacitors with various thickness ratios of parylene DLGDs as a function of frequency. S-8

Figure S2. (a-e) AFM images of parylene-based gate dielectrics, where X is the thickness ratio. S-9

Figure S3. (a-e) DI water CA measurement images of parylene-based gate dielectrics, where X is the thickness ratio. S-10

Figure S4. (a-e) POM images of TIPS-pentacene thin films on parylene-based gate dielectric, where X is the thickness ratio. S-11

Figure S5. (a-e) 2D GIXRD patterns of TIPS-pentacene thin films on parylene-based gate dielectrics, where X is the thickness ratio. S-12

Figure S6. Out-of-plane XRD patterns of TIPS-pentacene thin films on parylene-based gate dielectrics. S-13