Electrochemical Transistor Based on Tungsten Oxide
with Optoelectronic Properties

Paul Grey, Luís Pereira, Sónia Pereira, Pedro Barquinha, Inês Cunha, Rodrigo

Martins, Elvira Fortunato

► To cite this version:

Paul Grey, Luís Pereira, Sónia Pereira, Pedro Barquinha, Inês Cunha, et al. Electrochemical Transistor Based on Tungsten Oxide with Optoelectronic Properties. 7th Doctoral Conference on Computing, Electrical and Industrial Systems (DoCEIS), Apr 2016, Costa de Caparica, Portugal. pp.542-550, 10.1007/978-3-319-31165-4_51. hal-01438282

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Distributed under a Creative Commons CC BY 4.0 - Attribution - International License
Electrochemical Transistor Based on Tungsten Oxide
with Optoelectronic Properties

Paul Grey¹, Luís Pereira¹, Sónia Pereira¹, Pedro Barquinha¹, Inês Cunha¹, Rodrigo Martins¹ and Elvira Fortunato¹

¹CENIMAT/i3N, Departamento de Ciência dos Materiais, Faculdade de Ciências e Tecnologia, FCT, Universidade Nova de Lisboa and CEMOP-UNINOVA
Campus da Caparica
2829-516 Caparica, Portugal
lmnp@fct.unl.pt, emf@fct.unl.pt

**Abstract.** This paper reports the integration of an electrochromic inorganic oxide semiconductor (WO₃) into an electrolyte gated transistor device. The resulting electrochromic transistor (EC-T) is a novel optoelectronic device, exhibiting simultaneous optical and electrical modulation. These devices show an On-Off ratio of 5×10⁶ and a transconductance (g_m) of 3.59 mS, for gate voltages (V_G) between -2 and 2 V, which, to the authors knowledge, are one of the best values ever reported for this type of electrochemical transistors. The simple and low-cost processing together with the electrical/optical performances, well supported into a comprehensive analysis of device physics, opens doors for a wide range of new applications in display technologies, biosensors, fuel cells or electrochemical logic circuits.

**Keywords:** tungsten oxides (VI); electrochromism; thin films; electrolyte-gated transistors; polymer electrolytes.

# 1 Introduction

Electrolyte-gated transistors (EGTs) and electrochemical transistors (ECTs) have received special attention over the last decade due to their advantages, mainly deriving from the use of solid electrolytes as gate dielectrics. These include low operating voltages, printability and solution processability, low contact resistances, the possibility to fabricate new device architectures, and high driving currents.[1] The understanding of the involved phenomena in electrolyte-gated transistor (EGT) operation is an important aspect to enable their integration in applications like biosensors,[2] microelectronics [3] or even the emergent area of textronics.[4]

EGTs using electrochromic (EC) semiconductors are particularly interesting as they combine electrical/ electrochemical effects with a simultaneous optical modulation.

The optical absorption of an EC material can be modified through double insertion of electrons and charge compensating ions,[5] which can be easily achieved by the gate field in an EGT structure. Being a reversible process, this gives an EC material the capability of transiting between two distinct oxidation states: colored and bleached.
During the electrochemical reaction WO₃ also undergoes a change in its electrical properties, namely in its conductivity, making it a candidate for implementation as the semiconductor layer in transistors, as initially demonstrated by Natan *et al.* [6] Furthermore, inorganic oxide semiconductors as WO₃ possess higher chemical stability and higher conductance modulation than the organic semiconductors that compose most of the reported EGTs to date, which are great advantages for digital and analog circuit design with improved longevity.

The combination of both optoelectronic properties of EC-T opens possibilities in a wide range of applications and shows the value of the integration of smart materials into electronic circuitry.

## 2 Relationship to Cyber-Physical Systems

The use of electrolytes in active electronic components will be one of the fundamental building blocks of the interaction between common solid-state devices and ionic charge carriers. Figure 1 exemplifies the proposed interaction between an electrolyte and an ion permeable semiconductor.

<figure><img src="image_2.png" /><figcaption>**Fig. 1.** Schematic representation of the interaction between an ion permeable semiconductor and an electrolyte in a transistor setup with source, drain and gate (S, D and G, respectively). In the present paper WO₃ not only generates an electric response (conductivity change), but also an optical one (transmittance change), turning the system double redundant.</figcaption></figure>

Electrolytes are a big part of modern society and naturally occur throughout the whole spectrum of science. For instance solely in physiological systems there exist a plethora of electrolytes, responsible for intra- and extracellular interactions as well as nerve and muscle function control, blood pressure and pH. Consequently, reliable readout and double redundant values (electrical and optical) for electrolyte interpretation is crucial. Thus, creating a consistent interface between semiconductors and such electrolytes potentiates a main challenge for the development and study of EGTs. The technology of EGTs is therefore capable of adding gross value to a diverse range of cyber-physical systems (CPS), such as in chemical processes, healthcare and bio sensing schemes.
## 3 Results and Discussion

The complete device structure is depicted in Figure 2. An interdigital source and drain titanium contact architecture was chosen in order to increase channel width (3000 µm) and consequently the reached drain current of the devices. Furthermore an encapsulated device was fabricated, where the gate electrode (in this case an ITO coated PET foil) was extended over the electrolyte, resulting, not only, in a vertical architecture, but also in a self-passivation effect (Fig. 2 b and d).

<figure><img src="image_3.png" /><figcaption>**Fig. 2.** Schematic device representation, where a) represents the planar and b) the vertical and encapsulated architecture and c) and d) show a longitudinal cross-section representation of both of the device architectures. The PET/ITO foil is kept in place by capillary forces of the electrolyte and a silver glue (Ag) on the gate electrode.</figcaption></figure>

Subsequent characterization of the most crucial layers of the device was carried out. This includes electro-optical characterization of the sputtered WO₃ thin-films (100 nm), Electrochemical impedance spectroscopy (EIS) of the drop-casted electrolyte (a thermosetting composite solid electrolyte - TCSE) and lastly electrical characterization of the final devices.

### 3.1 Electro-Optical Measurements

Electrochromism for WO₃ is commonly introduced by reference to the following simplified redox reaction, also known as the double-injection model:[7]
$$WO_3(\text{transparent}) + xe^- + xM^+ \leftrightarrow M_xWO_3(\text{dark blue}) \quad (1)$$

where $M^+$ is an ion of the alkali metal group (e.g. H+, Li+, Na+ or K+), provided by the electrolyte, $e^-$ represents electrons and parameter $x$, designated as the insertion coefficient, represents the proportion of electro-reduced tungsten sites. Following Equation 1, the pristine $WO_3$ is transparent and the resulting tungsten bronze ($M_xWO_3$), for low $x$, exhibits its characteristic blue coloration due to photo-intervalence charge transfer (CT) between adjacent $W^V$ and $W^{VI}$ sites.[8]

It is widely accepted that the electro-optical centers are activated by the insertion of electrons and charge compensating ions, which distort and expand the lattice of the guest oxide, resulting in an overall modification of the optical properties and electronic structure of $WO_3$. Charge carriers are trapped by $W^{6+}$ octahedra, reducing them to $W^{5+}$, while the alkali metals remain ionized in the interstitial space.[9] This results in a delocalization of electrons in the lattice and a charge carrier concentration increase of several orders of magnitude from the pristine oxide. This consequently increases the conductivity, which in terms of transistor operation is reflected in the transition between the Off- and On-states (oxidized and reduced states, respectively).

The $WO_3$ film was deposited on an ITO coated glass substrate, which was submersed in a $Li^+$ rich liquid electrolyte in a conventional three-electrode setup. By applying a potential of 1 and -1 V to the ITO film it is possible to influence the oxidation states (oxidized and reduced, respectively) and consequently monitor the change in transmittance at a specific wavelength ($\lambda = 633$ nm), as well as the inserted charges into the $WO_3$ film (Fig. 3). The wavelength corresponds to the transmittance of the characteristic blue coloration of reduced $WO_3$ and it can be observed that a transmittance variation of over 90% is achieved. The inserted charges during reduction (-1 V) remain as free available charge carriers in the film and are extracted upon oxidation (1 V). A maximum of 26 mC of charge induction was achieved, yielding (with a contact area of 0.833 cm²) a charge density of about $2 \times 10^{17}$ cm⁻². However the process showed to be not completely reversible as charges might remain in the film after the reduction reaction (charge does not reach 0 mC at 90 s, see Fig. 3). Nonetheless sputtered $WO_3$ films from previous works are capable of reaching very high lifetimes with more than 1000 cycles.[10]
<figure><img src="image_4.png" /><figcaption>Fig. 3. Electro-optical measurements of a 100 nm thick WO₃ film on ITO/Glass Substrate in a Li⁺ rich electrolyte. Transmittance was measured during a full bleaching/coloration/bleaching cycle (30 s each) for the characteristic wavelength of reduced WO₃ (633 nm). The inserted and extracted available charge-carriers were also measured as a function of the duration of the applied potential.</figcaption></figure>

This characterization technique proves the inherent optoelectronic behavior of WO₃ and reveals its potential application in semiconducting devices, owing to reversible insulator-to-metal transitions, resulting from the electrochemical reaction.

## 3.2 Electrochemical Impedance Spectroscopy (EIS)

EIS is a well-known technique to determine the electrical properties of ionic materials, where an *ac* potential at different frequencies (f) is applied to an electrochemical cell, so the total capacitor impedance (Z) can be measured as a function of the frequency. This gives valuable information about ion migration, electric double layer (EDL) formation and its capacitance (C<sub>DL</sub>).

The electrochemical cell prepared for EIS is, as shown in Figure 4 a), composed of 3 distinct layers. Explicitly two ITO coated glass substrates and, sandwiched in between, the TCSE. The behavior and the obtained data of this cell can be described by an equivalent circuit model (ECM) for parameter determination (see Fig. 4 b).

This ECM (describing an ideally polarizable electrochemical cell), is composed of a resistance (R<sub>ext</sub>), associated to contact resistances (ITO), in series with a parallel R<sub>b</sub>C<sub>b</sub> circuit and a constant phase element (CPE). The R<sub>b</sub>C<sub>b</sub> circuit is associated to bulk properties of the electrolyte, namely the bulk resistance and capacitance, respectively. Whereas R<sub>b</sub> gives information about σ<sub>i</sub>, C<sub>b</sub> accounts for the dipolar relaxation of electrolyte solvent molecules at higher frequencies. The CPE mimics a
non-ideal capacitive behavior of the electric double layer, associated to interface inhomogeneities.[11]

Upon polarization of the electrochemical cell, ions migrate from one electrode to the other, causing charge built-ups and EDL formation. As can be observed in Figure 4 c) the ECM describes well the behavior of the cell throughout the whole frequency spectrum and serves for the determination of C<sub>DL</sub> and the ionic conductivity (σ<sub>i</sub>).

Here, as we are dealing with an electrochemical transistor (ECT), σᵢ will be the parameter of interest. This parameter will determine how pronounced the effective net ion diffusion into the semiconductor will be and how fast the insulator-to-metal transition occurs. However, from an electrochemical point-of-view it is also important to determine the amount of accumulated charges at the interfaces (C<sub>DL</sub>), which, in terms of transistor characterization, accounts for charge induction (field-effect) into the semiconductor. It was shown that both effects (electrochemical reaction and field-effect) can contribute to the drain current.[12]

<figure><img src="image_5.png" /><figcaption>**Fig. 4.** Electrochemical Impedance Spectroscopy of the used Thermosetting Composite Solid-Electrolyte (TCSE). Where a) shows the electrochemical cell (TCSE sandwiched in between two ITO (contact) coated glass substrates), b) represents the equivalent circuit model (ECM) used for the fittings and c) depicts the effective capacitance and the phase of the electrochemical cell in a frequency range between 10⁻² and 10⁶ Hz.</figcaption></figure>

The ionic conductivity (for cell dimensions: A = 5 cm² and d = 0.1 mm) and R<sub>b</sub> = 87.34 Ω from the fitting, σ<sub>i</sub> of the electrolyte was determined as 2.29×10<sup>-5</sup> Scm<sup>-1</sup>, using the standard resistivity equation. For C<sub>DL</sub> we considered the approach taken by Jović *et al.* [13] to empirically determine this value by using the fit for the CPE, yielding C<sub>DL</sub> = 5.10 μFcm<sup>-2</sup>.

A clear advantage for this type of dielectric becomes evident as the achieved dielectric capacitance reaches very high values. However, as both characteristic parameters (σᵢ and C<sub>DL</sub>) are highly frequency-dependent, transistors working with these materials are often restricted to lower frequencies, where complete ionic
relaxation can take place (capacitive regime in Fig. 4 c). Nonetheless, efforts are
made towards an improvement of overall electrolyte behavior in order to augment the
EGTs cut off frequency ($f_{co}$ – frequency where $I_{On}/I_{Off} = 10$).[14]

## 3.3 Electrical Characterization

Electrical characterization of the final devices (as depicted in Fig. 5 a) was conducted
with a drain voltage ($V_D$) as low as 1 V and a voltage sweep at the gate ($V_G$) from -4
to 4 V and back at a scan-rate of 20 mVs$^{-1}$. Low-voltage operation of EGTs were
found to be another strong factor of this type of devices, making their application in
low power consuming applications feasible.

<figure><img src="image_6.png" /><figcaption>Fig. 5. a) Transfer characteristics of the fabricated planar and vertical EC-Ts and b) micrographs of channel region with distinct colorations between the On- and the Off-state. Curves obtained with $V_D$ = 1 V and $V_G$ = (-4, 4, -4) V at a scan-rate of 20 mVs$^{-1}$. The arrow next to the main graphs indicates hysteresis direction.</figcaption></figure>

The applied $V_G$ drives ion migration in the electrolyte (as schematized in Fig. 1) and promotes reversible electrochemical doping (reduction and oxidation) of the channel region. As can be observed in Figure 5 a, the fabricated EC-Ts start to switch close to $V_G$ = 0 V to their respective On-states, remaining however with a normally On characteristic. As the channel reduces (and colors from transparent to blue, as seen in Fig. 5 b) the drain current increases until reaching mA values around $V_G$ = 2 V, with leakage currents ($I_G$) remaining in the order of µA (at most). The obtained On-Off ratios are considerable, reaching almost 7 orders of magnitude (vertical architecture). A hysteresis behavior is observed for both architectures planar and vertical, which is connected to the time-dependency of the electrochemical reaction, as well as ion migration processes. Nevertheless, it is possible to open and close both EC-Ts with symmetric VG (-4 and 4 V and -2 and 2 V for the planar and vertical architecture, respectively).
Table 1 resumes crucial device parameters, evidencing an advantage for the vertical and encapsulated EC-T, reaching higher values in each aspect. Furthermore, the vertical EC-T showed higher lifetimes than the planar one due to the self-passivation effect of the organic electrolyte, which is always subjected to environmental degradation factors.

<table><caption>**Table 1.** Crucial EC-T parameters, comparing the planar with the vertical structure. Values calculated from the curves of Figure 5a.</caption><thead><tr><th></th><th>I<sub>on</sub>/I<sub>off</sub></th><th>V<sub>on</sub> (V)</th><th>S<sub>s</sub> (Vdec<sup>-1</sup>)</th><th>g<sub>m</sub> (mS)</th></tr></thead><tbody><tr><td>Planar</td><td>6.55 × 10<sup>5</sup></td><td>0</td><td>0.28</td><td>2.24</td></tr><tr><td>Vertical</td><td>5.10 × 10<sup>6</sup></td><td>-1</td><td>0.22</td><td>3.59</td></tr></tbody></table>

Analyzing Figure 5 a and b together, the double functionality of the EC-Ts becomes visually clear, as it is possible to obtain a simultaneous electrical and optical response. The obtained information from these devices, regarding, for instance, biosensing applications, is on the one hand quantitative (I<sub>D</sub> output) and on the other hand qualitative (color output). This leads to the above discussed double redundancy outputs, turning these devices highly reliable for sensing applications in healthcare or chemical and biological schemes. The results show how important but also how effective a controlled interaction between semiconductor/electrical components and ionic conductors is. A consistent integration of such devices into cyber-physical systems or as such will be feasible in the near future.

## 4 Conclusion

With this work we show an approach for a possible integration of ionic conductors (electrolytes) into electronic circuitry. The developed electrolyte-gated transistors (EGTs) based on the semiconductor WO<sub>3</sub> exhibit double functionality (electrical and optical), as the electrochemical reaction of WO<sub>3</sub> not only promotes a change in its coloration, but also a change of conductivity of several orders of magnitude. Characterization goes through electro-optical analysis of the WO<sub>3</sub> film, electrochemical impedance spectroscopy of the electrolyte (a thermosetting composite solid-electrolyte - TCSE) and electrical characterization of the final devices. Two transistor architectures with identical W/L = 12 were implemented (planar and vertical) in order to investigate structure influences and self-passivation effects. The best device (vertical) showed an On-Off ratio of almost 7 orders of magnitude (one of the highest ever reported for EGTs) for very low operation voltages (V<sub>D</sub> = 1 V and V<sub>G</sub> between -4 and 4 V) and additional hysteresis reduction. In future works the dynamical switching of such devices will be in focus, as well as testing and optimizing different types of electrolytes.
The presented research paves the way for sophisticated systems, where the analysis of electrolytes and the interaction of these with semiconductors is crucial. These devices could be integrated into applications as diverse as lab-on-chip, wearable electronics, healthcare monitoring and biosensors.

**Acknowledgments.** This work was supported by the FCT - Portuguese Foundation for Science and Technology, by the project EXCL/CTM-NAN/0201/2012 and by FEDER funds through the COMPETE 2020 Programme and National Funds through FCT under the project UID/CTM/50025/2013. The work was also supported by FP7 APPLE (grant number 262782-2) and SMART EC (grant number 258203) projects.

**5 References**

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[2] Berggren, M., Richter-Dahlfors, A.: Organic bioelectronics. Advanced Materials. 19, 3201-3213 (2007)

[3] Herlogsson, L., Crispin, X., Tierney, S., Berggren, M.: Polyelectrolyte-Gated Organic Complementary Circuits Operating at Low Power and Voltage. Advanced Materials. 23, 4684-+ (2011)

[4] Hamedi, M., Herlogsson, L., Crispin, X., Marcilla, R., Berggren, M., Inganas, O.: Fiber-Embedded Electrolyte-Gated Field-Effect Transistors for e-Textiles. Advanced Materials. 21, 573-+ (2009)

[5] Granqvist, C. G.: Electrochromic tungsten oxide films: Review of progress 1993-1998. Solar Energy Materials and Solar Cells. 60, 201-262 (2000)

[6] Natan, M. J., Mallouk, T. E., Wrighton, M. S.: PH-SENSITIVE WO3-BASED MICROELECTROCHEMICAL TRANSISTORS. Journal of Physical Chemistry. 91, 648-654 (1987)

[7] Granqvist, C. G.: Progress in electrochromics: tungsten oxide revisited. Electrochimica Acta. 44, 3005-3015 (1999)

[8] Somani, P. R., Radhakrishnan, S.: Electrochromic materials and devices: present and future. Materials Chemistry and Physics. 77, 117-133 (2003)

[9] Azens, A., Hjelm, A., LeBellac, D., Granqvist, C. G., Barczynskab, J., Pentjuss, E., Gabrusenoks, J., Wills, J. M.: Electrochromism of W-oxide-based thin films: Recent advances. Solid State Ionics. 86, (2007)

[10] Barquinha, P., Pereira, S., Pereira, L., Wojcik, P. J., Grey, P., Martins, R., Fortunato, E.: Flexible and Transparent WO3 Transistor with Electrical and Optical Modulation. Advanced Electronic Materials. 1, (2015)

[11] Barsoukov, E., Macdonald, J. R.: Impedance Spectroscopy Theory, Experiment, and Applications. John Wiley & Sons, Inc., New Jersey (2005)

[12] Santos, L., Nunes, D., Calmeiro, T., Branquinho, R., Salgueiro, D., Barquinha, P., Pereira, L., Martins, R., Fortunato, E.: Solvothermal Synthesis of Gallium-Indium-Zinc-
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[13] Jovic, V. D., Jovic, B. M.: EIS and differential capacitance measurements onto single crystal faces in different solutions - Part I: Ag(111) in 0.01 M NaCl. Journal of Electroanalytical Chemistry. 541, 1-11 (2003)

[14] Liu, J., Herlogsson, L., Sawatdee, A., Favia, P., Sandberg, M., Crispin, X., Engquist, I., Berggren, M.: Vertical polyelectrolyte-gated organic field-effect transistors. Applied Physics Letters. 97, 3 (2010)