- 1Department of Chemical Engineering, Polytechnique Montréal, Montreal, QC, Canada
- 2Department of Chemistry, University of Technology Malaysia, Johor Bahru, Malaysia
- 3Department of Engineering Physics, Polytechnique Montréal, Montreal, QC, Canada
Titanium dioxide (TiO2) is an abundant metal oxide, widely used in food industry, cosmetics, medicine, water treatment and electronic devices. TiO2 is of interest for next-generation indium-free thin-film transistors and ion-gated transistors due to its tunable optoelectronic properties, ambient stability, and solution processability. In this work, we fabricated TiO2 films using a wet chemical approach and demonstrated their transistor behavior with room temperature ionic liquids and aqueous electrolytes. In addition, we demonstrated the pH sensing behavior of the TiO2 IGTs with a sensitivity of ∼48 mV/pH. Furthermore, we demonstrated a low temperature (120°C), solution processed TiO2-based IGTs on flexible polyethylene terephthalate (PET) substrates, which were stable under moderate tensile bending.
Introduction
Oxide semiconductors are commonly used in display technologies, energy conversion as well as chemo- and bio-sensing, due to their remarkable physicochemical properties, tunable optoelectronic behavior and mixed ionic-electronic conductivities (Manjakkal et al., 2020; Rim, 2020; Wager, 2020; Papac et al., 2021; Shi et al., 2021; Yoo et al., 2021). They are cost-effective, transparent to visible light, stable in ambient conditions and solution-processable at low temperatures in ambient air (Park et al., 2020; Tiwari et al., 2020). Oxide semiconductors are extensively studied as active channel materials for field-effect transistors (FETs) and ion-gated transistors (IGTs) (Wager, 2016; Cadilha Marques et al., 2019; Leighton, 2019), where charge carrier mobility, ON/OFF current ratio, operating voltage and switching speed are key parameters for determining device performance. Amorphous indium gallium zinc oxide (IGZO), showing a mobility above 10 cm2/Vs, is already used in organic light emitting diode (OLED) display backplanes (Nomura et al., 2004; Wager, 2016; Ji et al., 2021; Song et al., 2021). However, due to the scarcity of indium in the earth’s crust, several alternative oxide semiconductors are being explored (Ramarajan et al., 2020). For instance, in addition to display technologies, the earth-abundant materials ZnO, SnO2 and TiO2 are investigated for sensor applications (Nunes et al., 2019; Manjakkal et al., 2020; Şerban and Enesca, 2020; Sedki et al., 2021). To develop sensors for physiological (e.g., point-of-care testing) and environmental monitoring (e.g., water quality monitoring), the semiconductors need to be stable in ambient conditions (Rim, 2020). TiO2 is known for its abundancy, non-toxicity, tunable optoelectronic properties, high stability under ambient conditions and biocompatibility (Chen and Selloni, 2014). Depending on the type of synthesis, thermal treatment temperature, and type of gating media, FETs and IGTs based on TiO2 channels exhibit charge carrier mobility ranging from 0.05 to 10 cm2/Vs (Zhong et al., 2012; Chong and Kim, 2013; Horita et al., 2013; Valitova et al., 2016; Yajima et al., 2016; Tiwale et al., 2020; Zhang et al., 2021).
Various film processing routes lead to different morphologies, crystal structures and chemical compositions of TiO2, resulting in different electrical properties (Anitha et al., 2015). TiO2 can be processed via a variety of sustainable wet chemical approaches, such as spin-coating, dip-coating, spray-coating and printing (Thomas et al., 2013). However, the high processing temperature (>250°C) and brittle nature of metal oxide films limit their applicability in flexible and stretchable electronics (De A. Freire et al., 1999; Zardetto et al., 2011; Moonen et al., 2012; Wang et al., 2019; Asare et al., 2020; Baeg and Lee, 2020; Park et al., 2020).
Metal oxide-based IGTs employ semiconducting metal oxides as active channel materials and ionic liquids, ion-gels or aqueous saline solutions as the ion-gating media (Kim et al., 2013; Bisri et al., 2017; Cadilha Marques et al., 2019; Huang et al., 2021; Subramanian et al., 2021). Due to its autoionization, deionized (DI) water can also be used as gating medium (Singh et al., 2016). IGTs operate at low voltages, due to the formation of an electrical double layer at the oxide semiconductor/ion-gating medium interface (Bisri et al., 2017; Griffin, 2020). Current modulation in IGTs can be explained by electrostatic (surface) and electrochemical (volumetric) doping. Surface doping is achieved by the migration of ions from the gating medium towards the surface of the semiconductor and subsequent formation of a high-capacitance electrical double layer, whereas volumetric doping is achieved when ions from the gating medium pass through the permeable surface into the bulk of the semiconductor (Laiho et al., 2011; Kim et al., 2013; Bisri et al., 2017; Sood et al., 2021; Torricelli et al., 2021). Horita et al. (2013) fabricated anatase TiO2-based IGTs using ionic liquids, ion-gels and polyvinyl alcohol and investigated the transistor performance with different mobile ions in the ion-gating media. We recently demonstrated that the characteristics of IGTs based on porous and compact TiO2 films gated by pure 1-ethyl-3-methylimidazolium bis(trifluoromethylsulfonyl)imide ([EMIM][TFSI]), and Li+ ions in [EMIM] [TFSI] were significantly affected by the film morphology and the gating medium (Subramanian et al., 2020).
IGTs can be used as chemical sensors and biosensors due to their ability to function as ion/electron converters (Bu et al., 2020; Torricelli et al., 2021). In IGT sensors, the analyte, i.e., substance to be detected, can be included in the gating medium, leading to a change of the electronic signal (Bu et al., 2020; Cea et al., 2020; Rim, 2020). In IGTs, the analyte is in direct contact with semiconductor, while in the case of ion-sensitive field-effect transistor (ISFETs), it is in direct contact with the gate dielectric. The low operating voltage of oxide-based IGTs makes possible the detection of biomolecules that feature undesired redox reactions at high voltages. In addition, surface functionalization of the oxide semiconductor permits functionalization with specific chemical/biological species. As an example, the surface functionalization of ZnO with the glucose oxidase enzyme enabled the specific quantitative detection of d-glucose in IGT configuration (Bandiello et al., 2014). The detection of coronavirus and cancer biomarkers were recently reported using oxide IGTs (Ishikawa et al., 2009; Chang et al., 2011; AlQahtani et al., 2021).
Oxide-based IGTs can be used as pH sensors, exploiting the threshold voltage shift induced by changes in the pH of the gating medium (Kergoat et al., 2010; Bhatt et al., 2020; Lee et al., 2020). Previous reports based on TiO2 extended-gate ISFETs showed a maximum pH sensitivity of 60 mV/pH (Li et al., 2014; Yao et al., 2014; Yusof et al., 2016; Zulkefle et al., 2016). These devices are composed of a FET (transducing unit), a sensing unit and control gate electrode. The sensing unit and the control gate are placed in the environment containing the analyte solution and the sensing unit is remotely connected to the gate terminal of the FET which is placed outside the analyte. (Li et al., 2014).
In this work, we synthesized TiO2 films using a sustainable wet chemical method employing green alcohol solvents (isopropanol and ethanol). We demonstrated the successful operation of TiO2 IGTs at low voltages in an ionic liquid and an aqueous saline solution. TiO2 IGTs were also used as pH sensors with a pH sensitivity of ∼48 mV/pH. Due to the n-type nature of the TiO2 film, the increase of [H]+ (decrease of pH) makes the IGTs turn on at lower voltages. Conversely, the IGTs turn on at higher voltages at higher pH. In addition, we fabricated TiO2 films on flexible PET substrates at the maximum processing temperature of 120°C and showed that their performance was not severely affected under tensile bending state.
Experimental
Film Deposition
The solution for TiO2 sol-gel synthesis on rigid substrates (route I) was prepared by mixing 1.7 ml of titanium butoxide (Alfa Aesar, 99%), 65 µL of concentrated HNO3 (Thermo Fisher Scientific, 70%), 90 µL of deionized water (Milli-Q water purification system, resistivity of 18.2 MΩ cm) and 19.1 ml of isopropyl alcohol (HoneyWell, 99.9%) for 6 h at room temperature (Kajitvichyanukul et al., 2005; Parthiban et al., 2015). This solution was spin-coated on Au/Ti (40 nm/5 nm) pre-patterned SiO2/p-Si (200 nm/500 µm) substrates (Wafer Pro, Santa Clara, CA, United States) at 2,000 rpm for 40 s. The films were heated initially at 100°C for 15 min to evaporate the solvents and subsequently in a tubular furnace in ambient air (Thermolyne 21100) at 450 ± 10°C for 1 h (Parthiban et al., 2015).
TiO2 films on flexible PET substrates were obtained with a different method (route II), which only required a thermal treatment at 120°C. A TiO2 suspension was prepared by mixing 10 g of Aeroxide TiO2 P25 nanoparticles (Photocatalytic standard, particle size ∼21 nm, Millipore Sigma), 107 ml of ethanol (Commercial Alcohols Inc., Canada), 1.4 ml of deionized water and 3.7 ml of titanium tetraisopropoxide (Millipore Sigma) overnight at room temperature. This suspension was spin-coated on Au/Ti (40 nm/5 nm) pre-patterned polyethylene terephthalate (PET) substrates (175 µm thick, antistatic coating on both sides, purchased from Policrom Inc., Bensalem, PA, United States) at 4,000 rpm for 40 s. The films were heated at 120°C for 90 min in ambient air (Kim and Hwang, 2014).
Film Characterization
The topographical characteristics of the TiO2 films were analyzed using tapping-mode atomic force microscopy (AFM) performed with a Digital Instruments Dimension 3100 and JPK NanoWizard 3 equipped with a silicon cantilever (Spring constant: 40 N/m, tip radius: <10 µm and resonance frequency: 300 kHz). The thicknesses of the TiO2 films (∼55 nm for route I films and ∼1.1 µm for route II films) were measured using a profilometer (Dektak 150, Veeco, Plainview, NY, United States). The morphological characteristics of the TiO2 films were analyzed using JEOL JSM-7600F and Hitachi SU8020 field emission scanning electron microscopes (FESEM). The crystal structures of the TiO2 films were analyzed using X-ray diffraction (XRD) performed with Bruker D8 and Rigaku SmartLab diffractometers using CuKα source. The x-rays were scanned (1°/minute) from 2θ = 10° to 2θ = 60°.
Device Fabrication
Photolithographically patterned Au/Ti (40 nm/5 nm) source and drain electrodes (width/length = 4,000 µm/10 µm) on SiO2/p-Si and PET substrates were prepared according to a procedure described previously (Valitova et al., 2016; De Oliveira Silva et al., 2019; Subramanian et al., 2021). The patterned substrates were ultrasonically cleaned using sequential baths of isopropyl alcohol, acetone and isopropyl alcohol and exposure to UV-ozone for 15 min, prior to the deposition of the TiO2 films (Subramanian et al., 2020).
For ionic liquid gating, a PVDF (polyvinylidene fluoride, 220 nm pore size, Millipore Sigma) membrane (9 × 4 mm) soaked with [EMIM] [TFSI] (IoLiTec Ionic Liquids Technologies GmbH, Germany) was placed on the top of the TiO2 layer and served as the ion-gating media. Activated carbon on carbon paper (6 × 3 mm) was used as the gate electrode and manually placed on top of the ion-gating medium to complete the fabrication of the ionic liquid-gated transistor (Subramanian et al., 2020; Azimi et al., 2021; Subramanian et al., 2021).
For aqueous electrolyte gating/pH sensing, a polydimethylsiloxane (PDMS) well (size of inner well ∼2 × 6 × 6 mm) was attached to the substrates to confine the NaCl or the buffer solutions. (De Oliveira Silva et al., 2019). The saline solution was prepared using NaCl (Sigma Aldrich, 0.1 M) in deionized water. The device fabrication was completed by injecting 0.1 M NaCl aqueous solution in the PDMS well and immersing the activated carbon gate electrode on it (Subramanian et al., 2021). The schematic representation of the device fabrication is shown in Supplementary Figure S1. The illustrations of the transistor cross-sections are shown in Scheme 1. For pH sensors, the NaCl solution was replaced by different pH buffer solutions (pH of 1.68, 4.01, 7.00, 10.01, and 12.46, Orion pH buffer solutions, Thermo Scientific).
The carbon ink used in the activated carbon gate electrode for the ionic liquid-gated transistors was prepared using activated carbon (Norit CA1, Sigma-Aldrich, 28 mg ml−1) and PVDF (Sigma Aldrich, 1.4 mg ml−1) in N-methyl pyrrolidone (Sigma Aldrich). The carbon ink used in the activated carbon gate electrode for the aqueous electrolyte-gated transistors was prepared using activated carbon (Norit CA1, Sigma-Aldrich, 28 mg ml−1) and Nafion (Sigma Aldrich, 1.4 mg ml−1) in isopropyl alcohol. The activated carbon gate electrodes were obtained by drop-casting the carbon ink on the carbon paper (Spectracarb 2050A, Fuel cell store, United States) followed by heating at 60°C for 5 h (Tang et al., 2015; Valitova et al., 2016; De Oliveira Silva et al., 2019).
Device Characterization
The transistor characterization of IGTs was performed using an electrical probe station equipped with a micropositioner (Signatone Corporation, Gilroy, CA, United States) and a semiconductor parameter analyzer (Keysight B1500A). The electrochemical characterization of TiO2 films was carried out using a potentiostat (VERSASTAT 4, Princeton Applied Research). The electrical and electrochemical characteristics of the ionic liquid gated transistors were measured in a N2 glove box (H2O <5 ppm and O2 <5 ppm). The electrical and electrochemical characteristics of the aqueous electrolyte-gated transistors were measured in ambient conditions (Subramanian et al., 2021).
Charge Carrier Density and Mobility Calculations
The charge carrier mobility was extracted from the linear transfer characteristics, using the formula
where L is the interelectrode distance (10 µm), Ids,lin is the drain-source current in the linear regime of transfer characteristics, W is the electrode width (4,000 µm), e is the elementary charge (1.6 × 10−19 C), Vds is the drain-source voltage and n is the charge carrier density. The charge carrier density (n) was calculated from the linear transfer characteristics, using the formula
Where Q is the doping charge, Igs is the gate-source current in the forward scan of the linear transfer characteristics, rv is the scan rate of the gate-source voltage (Vgs), and A is the geometric area of the TiO2 films in contact with the ion-gating media (0.36 cm2 for ionic liquid based IGTs and 0.12 cm2 for the aqueous electrolyte-gated IGTs) (Subramanian et al., 2021).
pH Sensitivity Calculations
The pH sensitivity of IGTs was calculated using gate-source voltage shift with respect to the drain-source current (10−5 A) in the forward scan of linear transfer characteristics (Vds = 0.1 V). The gate-source voltage shift (ΔVgs) of IGTs for each pH buffer solution was plotted against the pH value and then the data points were fitted as a straight line by linear regression. The slope (V/pH) of the straight line corresponds to the pH sensitivity (Chou and Liao, 2005; Lee et al., 2020).
Results and Discussion
Film Characterization
Morphological, topographical, and structural properties of TiO2 films were studied before transistor assembly. For films on rigid SiO2/p-Si (route I), SEM images reveal a homogeneous, uniform, and crack-free morphology (Figure 1A). The rms roughness was found to be 1.0 ± 0.2 nm (Figure 1B). XRD patterns show the presence of the anatase phase (diffraction peak at 2θ ∼ 25°, Figure 1C). (Subramanian et al., 2020) The additional peaks ∼39° and ∼45° correspond to metallic gold (originating from the Au patterned electrodes) and aluminum (originating from the substrate holder of the XRD measurement setup). An analogous characterization of TiO2 films on PET (route II) revealed a more granular morphology with a uniform distribution of TiO2 nanoparticles (Figure 1D). The rms roughness was found to be 85.4 ± 4.2 nm (Figure 1E). Due to the response from the PET substrate at 2θ ∼ 25°, the main anatase diffraction peak was not visible in the XRD pattern (Figure 1F). The inset of Figure 1F shows the magnified pattern with 2θ ranging from 35° to 60°, indicating the presence of both anatase and rutile phases. XRD patterns of route I and route II films are different due to different processing temperatures and different Ti sources (See Experimental).
FIGURE 1. (A,D) SEM images, (B, E) AFM images and (C, F) XRD patterns of TiO2 films on SiO2/p-Si (A–C) and PET (D–F) substrates prepared by route I and route II. A and R indicate anatase and rutile phases of TiO2.
Electrochemical Characterization
Cyclic voltammetry was measured in a transistor configuration, with the TiO2 active channel functioning as the working electrode and the activated carbon gate (specific capacitance of ∼100 F/g) as the counter and quasi-reference electrode. (Subramanian et al., 2020; Subramanian et al., 2021). The cathodic and anodic signals indicate the doping and dedoping of the TiO2 films. Cyclic voltammograms (CVs) of the route I TiO2 films in [EMIM][TFSI] and 0.1 M NaCl solution, are shown in Figures 2A,B. The electrochemical reduction of TiO2 starts around −0.6 V for both [EMIM] [TFSI] and 0.1 M aqueous NaCl gating (Figures 2A,B). The reduction-oxidation signals are displayed by the wide cathodic and anodic waves. Cyclic voltammograms of route II TiO2 films with [EMIM][TFSI] show that the electrochemical reduction potential of TiO2 starts at ∼-1.1 V (See Supplementary Figure S2 for the cyclic voltammogram in the lower potential window region), which is more cathodic than for route I TiO2 films (∼−0.6 V) (Figure 2C). This information indicates that the route II TiO2 films can be safely operated between Vgs ∼ 1 V and Vgs ∼ 2 V in transistor configuration. As compared to route I TiO2, a higher gate voltage is necessary to activate the channel material, likely due to the lower temperature thermal treatment.
FIGURE 2. Cyclic voltammetry in transistor configuration for route I TiO2 films gated with [EMIM][TFSI] (A) and 0.1 M NaCl (B), and route II TiO2 films gated with [EMIM][TFSI] (C). The scan rates are 10, 50, and 100 mV/s.
Ion-Gated Transistors Based on Route I TiO2 Films on SiO2/Si Substrates
The output and transfer characteristics of route I TiO2 films gated with [EMIM][TFSI], measured in a N2–purged glove box, show n-type enhancement mode of operation (Figures 3A,B). The transfer curve reveals an ON/OFF current ratio of ∼103 (average value of three devices), extracted between Vgs = 0 V and Vgs = 1.1 V. The hysteresis in the transfer curve is attributed to the slow ion transport during forward and reverse scans. The output and transfer characteristics of route I TiO2 films, gated with 0.1 M NaCl, show a higher drain-source current than the [EMIM] [TFSI] counterparts (Figures 3C,D). The transfer curves shows that the ON/OFF current ratio of the transistors, calculated between Vgs = 0 V and Vgs = 1.1 V, is ∼104 (average value of three devices). Compared to the [EMIM][TFSI]-gated devices, NaCl(aq)-gated transistors show a clearer drain current saturation as well as a lower hysteresis, likely due to the faster dedoping. The charge carrier density and charge carrier mobility were ∼1.7 × 1014 cm−2 and ∼3.5 × 10−2 cm2/Vs for [EMIM][TFSI] gated devices and ∼1.5 × 1016 cm−2 and ∼4.5 × 10−3 cm2/Vs for the NaCl gated ones. The obtained mobility values (average values of three devices) are comparable with the previous articles based on metal oxide TFTs and IGTs (Wöbkenberg et al., 2010; Liang et al., 2012; Zhong et al., 2012; De Oliveira Silva et al., 2019).
FIGURE 3. (A,C) Output and (B,D) transfer characteristics of route I TiO2 films on SiO2/p-Si substrates gated with [EMIM][TFSI], measured in a N2-purged glove box (A,B) and with 0.1M NaCl(aq) measured in ambient conditions (C,D). The output characteristics were measured at Vgs = 0.6, 0.7, 0.8, 0.9, 1.0, and 1.1 V and the transfer characteristics at Vds = 0.1 V with a scan rate of 10 mV/s.
pH Sensors Based on Ion-Gated TiO2 Films
Low voltage operation in aqueous media makes TiO2 IGTs suitable for ion-sensing applications. With the aim to demonstrate pH sensing, we used TiO2 IGTs with pH buffer solutions as the ion-gating media.
Figure 4A shows the forward transfer characteristics (Vds = 0.1 V) of the IGT gated with pH buffer solutions (pH from 1.68 to 12.48). Two additional set of data extracted from two other devices are shown in Supplementary Figure S3. The change of pH of the gating media leads to a shift of the gate voltage at a given reference drain-source current point (e.g., Ids = 10−5 A). Being TiO2 an n-type semiconductor, when a positive voltage is applied to the gate electrode of TiO2 IGTs, the positive ions in the gating medium migrate and accumulates on the surface of TiO2 films, leading to an increase in electron density. Therefore, the negative shift in gate voltage observed when lowering the pH of ion-gating media, can be attributed to the increase of the of H3O+ concentration. The gate voltage shift at 10−5 A plotted against pH (Figure 4B) shows a pH sensitivity of TiO2 IGTs of ∼48 mV/pH (average value of 3 devices), which is comparable with the pH sensitivity values of metal oxide IGT based pH sensors (Bhatt et al., 2020; Lee et al., 2020; Woo Son et al., 2020). A larger statistical difference in gate voltage shift is observed for TiO2 IGTs at higher pH levels. The forward and backward scan of transfer characteristics of the TiO2 IGTs with an increasing pH value does not show any significant hysteresis (Supplementary Figure S4). The transfer characteristics of TiO2 IGTs measured with a decreasing pH value shows the same trend in device response with respect to increasing pH (Supplementary Figure S5).
FIGURE 4. (A) Transfer (forward scan) characteristics (Vds = 0.1 V) of route I TiO2 films on SiO2/Si substrates gated with pH buffer (pH 1.68, 4.01, 7.00, 10.01, and 12.46) solutions measured in ambient air. The Vgs scan rate is 10 mV/s. (B) Gate voltage shift corresponding to the reference drain-source current point (ca 10−5 A) versus pH. Each point in Figure 4 (B) corresponds to the average gate voltage shift of 3 devices with respect to pH value. The error bar in the graph indicates the standard deviation of 3 devices.
Ion-Gated Transistors Based on Route II TiO2 Films on PET Substrates
Transistors processed by route II synthesis on flexible PET substrates, characterized under flat and bent state using [EMIM][TFSI] as the gating medium. Figure 5 shows the output (A–C) and transfer (D, E) characteristics. These transistors required a higher voltage compared to the route I ones, in agreement with cyclic voltammetry data discussed above (Figure 2C). For comparison, we prepared similar devices on SiO2/Si substrates, which did not show any significant difference in the transistor characteristics with respect to PET substrates (Supplementary Figure S6). Compared to the route I devices, we observed a higher turn on voltage for route II devices, likely due to the lower processing temperature of TiO2. The linear transfer characteristics from Vgs = −2 V to Vgs = +2 V do not show any p-type transistor behavior (Supplementary Figure S7). Route II TiO2 shows a lower saturation current as compared to the route I TiO2. The charge carrier density and charge carrier mobility, extracted from the linear transfer characteristics (Figure 5D), were ∼1.2 × 1015 cm−2 and 7.5 × 10−3 cm2/Vs (average value of three devices). The ON/OFF ratio, extracted from the saturation transfer characteristics (Figure 5E), extracted between Vgs = 0 V and Vgs = 2 V, was ∼ 102 (average value of three devices). Transistor characterization under tensile bending radii at R ∼ 20 mm (Figure 5B) and at R ∼ 10 mm (Figure 5C) shows a slight decrease in Ids and their ON/OFF ratio (Figure 5E) is not severely affected by the bending. The device characteristics under flat state after bending are shown in Supplementary Figure S8. The drain-source current is slightly recovered after the bending measurements. The saturation transfer characteristics after multiple bending cycles shows no significant change with respect to the unbent state (Supplementary Figure S9). Two additional set of data (saturation transfer characteristics) extracted from two other devices are shown in Supplementary Figure S10.
FIGURE 5. (A–C) Output and (D,E) transfer characteristics of route II TiO2 films on PET substrates gated with [EMIM] [TFSI] measured in a N2 purged glove box. The output characteristics under (A) flat, (B) bending radius ∼20 mm and (C) bending radius ∼10 mm were measured at Vgs = 0, 1.0, 1.25, 1.5, 1.75, and 2.0 V. The transfer characteristics under flat and bent state were measured in (D) linear (Vds = 0.2 V) and (E) saturation (Vds = 1.75 V) regime. The scan rate is 50 mV/s.
The operating voltage of route II devices lays beyond the thermodynamical stability window of water, therefore preventing their use in the aqueous gating medium, as the high voltage may causes unwanted redox processes.
Conclusion and Perspectives
We fabricated TiO2 films on rigid and flexible substrates using sustainable wet synthesis. We demonstrated the transistor behavior of TiO2 films using room temperature ionic liquid and aqueous saline solution. TiO2 IGTs were successfully used as pH sensors with a sensitivity of ∼48 mV/pH. Furthermore, TiO2 films were deposited on the flexible PET substrates at the maximum processing temperature of 120°C. The transistor behavior of TiO2 IGTs was not severely affected by the tensile bending radii (R ∼ 20 mm and R ∼ 10 mm). In view of the flexibility and low temperature processability, route II TiO2 IGTs pave the way to future low-cost flexible electronics. Currently, work is in progress to fabricate TiO2 thin films on flexible substrates using controlled aqueous growth at lower temperatures for flexible pH sensing applications.
Data Availability Statement
The raw data supporting the conclusion of this article will be made available by the authors, without undue reservation.
Author Contributions
FC and AS designed the experiments. AS performed the transistor and electrochemical characteristics of the devices. FC supervised the experiments. CL did SEM, AFM and XRD characterizations. MA did AFM characterization and pH sensing measurements. SL and CS revised the manuscript.
Conflict of Interest
The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.
Publisher’s Note
All claims expressed in this article are solely those of the authors and do not necessarily represent those of their affiliated organizations, or those of the publisher, the editors and the reviewers. Any product that may be evaluated in this article, or claim that may be made by its manufacturer, is not guaranteed or endorsed by the publisher.
Acknowledgments
The Natural Sciences and Engineering Research Council of Canada (NSERC) is acknowledged for a Discovery Grant (F.C.). Equipment and infrastructure used for this research were acquired and maintained by the Canada Foundation for Innovation and Quebec Strategic Networks (CQMF-QCAM, RQMP, CREPEC, and GCM), respectively. AS and MA are grateful to the Trottier Energy Institute for a doctoral scholarship. AS is grateful to the FRQNT for a doctoral scholarship. CL is grateful to the Polytechnique Montréal for a research internship scholarship.
Supplementary Material
The Supplementary Material for this article can be found online at: https://www.frontiersin.org/articles/10.3389/felec.2022.813535/full#supplementary-material
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Keywords: titanium dioxide, ion-gating, transistors, pH sensors, thin films
Citation: Subramanian A, Azimi M, Leong CY, Lee SL, Santato C and Cicoira F (2022) Solution-Processed Titanium Dioxide Ion-Gated Transistors and Their Application for pH Sensing. Front. Electron. 3:813535. doi: 10.3389/felec.2022.813535
Received: 11 November 2021; Accepted: 02 March 2022;
Published: 22 March 2022.
Edited by:
Luisa Petti, Free University of Bozen-Bolzano, ItalyReviewed by:
Mattia Petrelli, Free University of Bozen-Bolzano, ItalyGiulia Casula, University of Cagliari, Italy
Copyright © 2022 Subramanian, Azimi, Leong, Lee, Santato and Cicoira. This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.
*Correspondence: Fabio Cicoira, fabio.cicoira@polymtl.ca