Memristors are regarded as a key electronic component for non-von Neumann computing, such as neuromorphic networks. Hereby, we report a capacitance-coupled memristor (C-memristor) configured with ITO/Ga2O3/ITO coplanar interdigital structures. Depending on the voltage sweeping directions, the C-memristor exhibits a clear current switching with different polarities, offering an easy-to-readout electronic status. Due to the coupled capacitance, the difference between the currents in forward and reverse scanning strongly depends on the voltage sweeping speed, which was quantitatively studied with an equivalent circuit that we established. A device model based on filamentary conductive paths formed by the electrically driven oxygen vacancies was utilized to explain the working mechanism of the C-memristor, which aligns well with the observed results. Unlike previously reported Ga2O3 memristors that rely only on the status of the resistance, our device also exhibits capacitance variation, offering an additional degree of freedom (e.g., the power nodes) for constructing a neural network.
I. INTRODUCTION
A memristor is a nonlinear resistance switching device, regarded as a promising electronic component for neuromorphic computing as a scheme for realizing artificial intelligence (AI).1 The device was predicted by Leon Chua as the fourth fundamental electronic component in addition to resistor, capacitor, and inductor in 1971, when he investigated the relationship between each two out of the four circuit variables, namely, current i, voltage v, charge q, and magnetic flux φ.2 The first solid-state memristor was realized by Strukov et al. from HP labs in 2008.3 Subsequently, memristors have been developing rapidly, including single devices with various working mechanisms and neuro-network systems.4–8 The typical feature of a memristor is that the device remembers its previous resistance based on the history of the voltage applied,9 reflected by a hysteresis loop in the current–voltage (IV) characteristics.
Many materials have been developed to fabricate memristors, including binary oxides, perovskites, and two-dimensional materials.10 Among them, binary oxides (e.g., TiOx, ZrOx, and ZnOx) are the largest material group due to their easy fabrication and strong current hysteresis.11–13 Ga2O3 as a new binary oxide semiconductor material (fourth-gen semiconductor) demonstrates its great potential in various fields, including power electronics, radiation detectors, and memristors.14–18 So far, nearly all published studies on Ga2O3 memristors focus on the changing of resistivity, while the effects of capacitance have yet to be understood.
In this work, we fabricated an ITO/Ga2O3/ITO coplanar interdigital device, which exhibits current hysteresis assisted with a coupled variable capacitance. By using an equivalent circuit, the behavior of the device can be quantitatively analyzed. Based on this, the device working mechanism can be well explained with a conductive filament model.
II. EXPERIMENTS
A 150 nm undoped Ga2O3 film was deposited on a quartz substrate by radio frequency sputtering with a Ga2O3 target under a power of 60 W. The sputtering pressure was 0.4 Pa, and the substrate was not intentionally heated. Details of growth can be found elsewhere.19–21 The surface of the film shows a mirror-like flatness, with a measured roughness <1 nm in a 3 × 3 μm2 scan area by atomic force microscopy (Fig. S1 of the supplementary material). As indicated by x-ray diffraction measurement (Fig. S2 of the supplementary material), the material is amphoteric Ga2O3 (a-Ga2O3).19,22 The transmittance/reflectance measurements show that the bandgap of the material is around 4.8 eV (Fig. S3 of the supplementary material).22 X-ray photoelectron spectroscopy (XPS) shows oxygen binding energy at 530.8 and 531.7 eV [Fig. 1(a)], corresponding to the lattice oxygen of Ga2O3 and oxygen vacancy (VO) related defects. It should be noted that the peak at 531.7 eV indicates the existence of oxygen vacancies.22 The device was fabricated by depositing ITO interdigital electrodes on the film with standard UV lithography. The gap between two ITO interdigital electrodes is 5 μm, with 75 pairs in total [Fig. 1(b)]. The electronic property of the device was measured using a probe station in an electronically shielded box equipped with a Keithley 2636B source meter (SMU), with a current resolution down to 2 fA. The alternative current (AC) frequency response was measured with a function generator (Rohde and Schwarz HMF2525) and a digital oscilloscope (Rohde and Schwarz RTB2002).
(a) XPS spectrum of the oxygen peaks, (b) zoom-in of the interdigital electrodes (a full image can be found in Fig. S4 of the supplementary material), (c) full-range IV curve from −20 to 20 V, (d) zoom-in IV curve in the highlighted region in (c), (e) current at 6 V in 100 loop measurements, and (f) the proposed equivalent circuit.
(a) XPS spectrum of the oxygen peaks, (b) zoom-in of the interdigital electrodes (a full image can be found in Fig. S4 of the supplementary material), (c) full-range IV curve from −20 to 20 V, (d) zoom-in IV curve in the highlighted region in (c), (e) current at 6 V in 100 loop measurements, and (f) the proposed equivalent circuit.
III. RESULTS AND DISCUSSION
When V = 0, the current is solely dependent on capacitance and the sweeping speed, which will be reflected by the difference between IF and IR (defined as “opening” in this paper). To prove this prediction, IV measurements with various sweep speeds have been carried out. The near V = 0 IV plots are shown in Fig. 2. Obviously, the opening decreases with decreasing sweeping speed (or increasing step time in the measurement), indicating that the total value of is decreasing. At the same time, an oscillation of current with the applied voltage can be observed, with variable peak-to-peak amplitude and period related to the voltage sweeping speed (Fig. S5 of the supplementary material).
IV curves near V = 0 with various sweeping times (time between each step) from 40 to 500 ms.
IV curves near V = 0 with various sweeping times (time between each step) from 40 to 500 ms.
In order to understand the working mechanism, we further analyzed the capacitance at different sweeping speeds. Figure 3 shows the capacitance obtained at V = 0 from Eq. (1), plotted as a function of . The result indicates that the capacitance is not a constant, with a decreasing value with increasing sweeping speed. A conducting filament model schematically shown in Fig. 3(b) is used to understand our device.24–27 When there is no bias, the oxygen vacancies are distributed randomly inside Ga2O3, where no conductive filament forms. Under an external bias, the oxygen vacancies are driven toward the direction of the electrode, and adjacent vacancies subsequently form a conductive filament. Different from the existing reports where a very thin Ga2O3 film (<100 nm) was employed to facilitate the filament connecting two electrodes,28–30 the distance between two electrodes is 5 μm in our device. Therefore, the conductive filaments do not span the entire device. Instead, only the length of the non-filament region (d) is reduced. As a result, the resistance (R ∝ l − d, where l is the length of the material between two electrodes) will decrease and capacitance will increase (). Regarding the current oscillation, it is attributed to temporal polarization and depolarization processes [Fig. 3(c)].31
(a) Capacitance as a function of sweeping speed, (b) schematic of the conductive filament model, and (c) schematic of polarization and depolarization processes.
(a) Capacitance as a function of sweeping speed, (b) schematic of the conductive filament model, and (c) schematic of polarization and depolarization processes.
Finally, we measured the AC response of our C-memristor. The top panel (black curve) of Fig. 4(a) shows an applied square wave at 7 kHz, while the bottom one (red curve) shows the measured response of the C-memristor. By fitting the time decay into (where A, B, τ are fitting parameters), a time decay of τ = 5.9 μs was obtained (blue curve), corresponding to a maximum working frequency of ∼169 kHz. Figure 4(b) shows the measurements up to 30 kHz with our current setup, exhibiting a stable time constant.
(a) AC response of the C-memristor and (b) extracted time decay measured at different frequencies up to 30 kHz (the inset shows the schematic of the setup).
(a) AC response of the C-memristor and (b) extracted time decay measured at different frequencies up to 30 kHz (the inset shows the schematic of the setup).
IV. CONCLUSION
In summary, we have realized a C-memristor based on a-Ga2O3 film with ITO interdigital electrodes. The device exhibits a clear current hysteresis with coupled capacitance, where the latter decides the current differences between forward and reverse scanning (speed). We established an equivalent circuit for quantitatively studying the details of electrical properties. Together with a conductive filament model, the results and device working mechanism can be well explained. In addition, the device offers facilitated readout binary electronic states (polarity) and a fast-working frequency of up to 169 kHz. We envisage that coupled capacitance will offer an additional degree of freedom for building memristor-based neural networks.1,32,33
SUPPLEMENTARY MATERIAL
See the supplementary material for the surface flatness measured by AFM (Fig. S1), XRD scans (Fig. S2), transmittance/reflectance measurements (Fig. S3), a full-image of the device (Fig. S4), and detailed IV measurements at various voltage sweeping speeds (Fig. S5).
ACKNOWLEDGMENTS
This work was supported by the EPSRC under Grant No. EP/T019085/1, Royal Society under Grant No. IEC\NSFC\242145, and SACEME Seedcorn funding from Swansea University. H.L. and Z.M. thank the National Natural Science Foundation of China for the support under Grant Nos. 12174275 and 62174113.
AUTHOR DECLARATIONS
Conflict of Interest
The authors have no conflicts to disclose.
Author Contributions
Alfred Moore: Formal analysis (equal); Investigation (equal); Methodology (equal); Writing – original draft (equal); Writing – review & editing (equal). Lijie Li: Conceptualization (equal); Formal analysis (equal); Investigation (equal); Methodology (equal); Resources (equal); Supervision (lead); Writing – original draft (equal); Writing – review & editing (equal). Hang Shao: Methodology (equal). Xiaoyan Tang: Methodology (equal). Huili Liang: Funding acquisition (equal); Methodology (equal); Resources (equal); Supervision (equal); Writing – original draft (equal); Writing – review & editing (equal). Zengxia Mei: Funding acquisition (equal); Methodology (equal); Resources (equal); Supervision (equal); Writing – original draft (equal); Writing – review & editing (equal). Yaonan Hou: Conceptualization (lead); Data curation (equal); Formal analysis (lead); Funding acquisition (equal); Methodology (equal); Project administration (lead); Resources (equal); Supervision (equal); Writing – original draft (lead); Writing – review & editing (lead).
DATA AVAILABILITY
The data that support the findings of this study are available from the corresponding author upon reasonable request.