Artificial synapses based on memristors are used in emulating the synaptic plasticity behavior of a human brain. Here, we have proposed a transparent memristor based on aluminum zinc oxide (AZO) on a flexible substrate—polyethylene naphthalate. We have analyzed the elemental composition of the gadget subjected to the optimized flow rate of Ar/O2 = 2/1 by x-ray photoelectron spectroscopy. The prepared AZO/ZnO/indium-doped tin oxide memristor exhibits a bipolar switching behavior with Vset/Vreset of 1.4/−2.0 V. The results reflect an acceptable endurance of >500 cycles and retention of 104 s. The optimized device shows an improvement in the non-linearity of potentiation—2.31/depression—3.05 and has more than 25 cycles of stability. The transparency is checked using a UV-visible spectrophotometer showing 90% transparency in the visible region making the device suitable for applications in invisible electronics. Our results reflect that the proposed device can be used as a transparent electrode in making artificial synapses for neuromorphic applications.

Modern electronic equipment, including computer systems, are built using the traditional von Neumann computing architecture, which has its computational constraints. The conventional CMOS transistors used in these systems make it power consuming, with slower speed of operation for solving complex tasks. Even downscaling of transistors to follow Moore's law1 is found to be not a solution. To remove the von Neumann bottlenecks and solve the issues of downscaling of devices, research is on the way for making the latest technologies to fulfill the requirement of fast operational speed and economical and minimal power consumption. Also, as the idea of big data advances and vast volume of formulated and unformulated data becomes more complicated, the limit of processing capacity causes high manufacturing cost and degraded power efficiency, with enhanced other costs. An engineering technique called “Neuromorphic Computing (NC)” aims to solve the current computing system's bottlenecks by mimicking the human brain's function with computer processors.2 

NC technique got the inspiration by looking at how the human brain works. There are roughly 1011 neurons in the human brain, and each neuron is connected by synapses. When a signal travels from a pre-synaptic neuron to a post-synaptic neuron, it typically involves the release of neurotransmitters from the pre-synaptic neuron into the synaptic cleft. These neurotransmitters then bind to receptors on the post-synaptic neuron, leading to changes in the post-synaptic neuron's membrane potential and resulting in the generation of an action potential. The process by which the strength of synaptic transmission is altered is called synaptic plasticity. There are two forms of synaptic plasticity—long-term potentiation/depression (LTP/D)—that result in an increase/decrease in the number or sensitivity of neurotransmitter receptors, respectively. To develop NC hardware, a suitable device is needed that can emulate the biological synapse and perform analog computation efficiently. Given this, the memristor is found to be a suitable candidate that plays a fundamental role in NC applications.

After the development of a memristor in the HP laboratory in 2008, many researchers used their ideas to fabricate different memristive devices and proved that the devices fabricated have great potential for applications in various engineering domains. Memristors have a simple structure with an insulator/semiconductor sandwiched between two metal electrodes. By choosing the proper materials for metal electrodes and insulator/semiconductor layer (active layer), it is aimed to have memristive properties such as low set/reset voltages, fast switching speed, high endurance characteristics (LTP/LTD), long retention, paired-pulse facilitation (PPF), and less power consumption. Now, among the different memristors, oxide-based memristors are best fitted in the framework of NC applications. Metallic oxides, namely, ZnO, TiO2, HfO2, NiO, TaOx, SnOx, WO3, and SrTiO3, are commonly taken for the manufacturing of memristors.3–9 Also, widely used chalcogenide substances like Ag2S, Cu2S,10,11 and ferroelectric materials like Pb0.8Ba0.2ZrO3, La2O3,12,13 have been investigated in fabricating memristors. The switching operation and synaptic behavior in WO3/NiO/FTO composite structures are successfully illustrated.14 ZnO-based memristor is fabricated, which can play the role of artificial synapse and along with synaptic functions such as short- and long-term plasticity.15 Photoelectric plasticity such as electrical resistive switching and photonic response in the ZnO1−x/AlOy hetero-structure has been demonstrated by Hu et al.16 In a study, Lee et al. grew IZO (indium gallium zinc oxide) on SiO2 and Si substrates and demonstrated how the apparatus replicated a key synaptic performance.17 He et al. accomplished electrical habituation and photonic potentiation using a single-layer MOS2.18 

Also, transparent memristors or transristors have wide applications in non-volatile memory, optoelectronic devices, neuromorphic systems, artificial synapses, neural networks, and human visual systems, making them popular at present. Park et al.19 have developed an organic memristor that is flexible and transparent showing a high optical transparency and can be used as non-volatile memory. Saleem et al.20 have presented a transparent bilayer memristor using indium-doped tin oxide (ITO)/ZnO/HfOx/ITO, which can be used in an optically synaptic device. Yan et al.21 fabricated a flexible egg albumen-based memristor that can act as an artificial synapse. Such bio-based memristors are suffering with their degradable stability with time. Zinc oxide (ZnO) is a multifunctional material with a wide range of applications due to its unique properties, including a wide bandgap (3.37 eV), high exciton binding energy (60 meV), and diverse morphologies. In electronics and optoelectronics,22,23 ZnO is employed in light-emitting diodes (LEDs), laser diodes, and photodetectors, leveraging its semiconducting properties and efficient ultraviolet (UV) light emission. Its high transparency and conductivity make it an excellent candidate for transparent conducting oxides (TCOs) in photovoltaic cells and display technologies. The diverse applications of ZnO across various fields underscore its significance and the incessant interest in exploring and optimizing its properties for advanced technological applications.

ZnO is generally chosen as the active layer in the memristor because of its high electron mobility and high binding energy, thereby resulting in good transparency. As a result, it is a popular material for transparent devices and widely employed for memristive applications and synapses. So, in our current research, we have created and examined a flexible transristor, taking ZnO as the intermediate layer between the electrodes of indium-doped tin oxide (ITO) and aluminum-doped zinc oxide (AZO). We have analyzed the switching mechanism and other synaptic characteristics of the proposed fabricated device. There are currently limited reports on the study of synaptic characteristics for this transparent and flexible device at varying concentrations of oxygen, which enhances the scope of this work.

Figures 1(a) and 1(b) depict the three-dimensional representation view of the flexible transristor device based on AZO/ZnO/ITO/PEN and its biological synapse counterpart, respectively. The devices are fabricated on the cleaned flexible PEN substrate using conventional RF sputtering techniques. Before being loaded into the chamber, the substrate covered with indium-tin-oxide (ITO) that is about 300 nm thick is first sonicated and cleaned for about 10 min using ethanol and de-ionized (DI) water. It is then dried by purging nitrogen gas. ITO is utilized as a transparent bottom electrode (BE) because of its high transmittance and low resistance. Zinc oxide (ZnO) layers are applied onto ITO/PEN substrates using magnetron sputtering, with adjustments made to the Ar/O2 gas ratios to control the deposition. At this stage, the Ar/O2 ratios being used have flow rates of 3/0, 2/1, and 1/1. During all depositions, the working pressure of 20 mTorr and an operating power of 50 W are sternly maintained. Using the shadow mask, a 60 nm thick layer of AZO as a top electrode is also sputtered after the deposition of a 50 nm ZnO layer on the ITO bottom electrode. The AZO film acts as a top electrode having an area of 17.67 μcm2.

FIG. 1.

(a) Three-dimensional view of the AZO/ZnO/ITO flexible transristor. (b) Biological synapse with pre-neuron and post-neuron.

FIG. 1.

(a) Three-dimensional view of the AZO/ZnO/ITO flexible transristor. (b) Biological synapse with pre-neuron and post-neuron.

Close modal

X-ray photoelectron spectra (XPS) are used to investigate the device composition. The electrical properties of the transristor have been analyzed using an Agilent B1500A semiconductor parameter analyzer at room temperature. During electrical measurements of the device, the direction of the current flow between the top and bottom electrodes is indicative of whether a positive or negative bias is applied. The fabricated device's optical transparency is measured with a UV-vis spectrometer.

Depth profile analysis has been conducted using XPS on the optimized device to examine the composition at different depths. Figure 2(a) illustrates the atomic concentration of the elements O 1s, Zn 2p3, Al 2p, and In 3d5 over sputtering time. From the XPS depth profile, it is observed that during the 157–202 s sputtering period, the concentration of zinc is 55% and the rest is oxygen. It is shown that while the concentrations of indium (In) and aluminum (Al) roughly stay constant, the concentration of zinc (Zn) gradually drops as the sputtering time increases. Zn can, therefore, be discovered from the film's surface. Since AZO is our top electrode, a slight reduction in the atomic concentration of Al with respect to sputtering time is anticipated.24 According to our artificial structure, the presence of various elements at various depths is confirmed by other elements. Figure 2(b) displays the deconvolution of Zn-2p3/2 of the ZnO film formed at a gas flow ratio of Ar/O2 = 2/1. The presence of an energy peak of Zn 2p3/2 at 1022.6 eV suggests that the majority of zinc atoms within the oxygen-deficient region retain the Zn2+ valence state. A Gaussian fit technique is used for the simulation of the peak energy and also to find out the different energy levels of the material. The deconvoluted XPS spectra of O 1s at depth 1 (ZnO: D1), which have been fitted with a Gaussian fit, are shown in Fig. 2(c). The O 1s spectra are well fitted with the three energy levels of O 1s, indicating the O 1s is the combination of three energy peaks. These three sub-peaks correspond to OI (530.3 eV), OII (531.05 eV), and OIII (532.25 eV). OI stands for oxygen ions that are closest to ZnO links, OII for oxygen ions that are in a deficient area, and OIII for adsorbed oxygen ions that are weakly bound. The proportionate area of OII/Ototal[Ototal = OI + OII + OIII] ratio is used to estimate the oxygen vacancy-mediated defects, and it is determined to be 77.0%. The process of synaptic conduction is aided by these oxygen vacancy-mediated defects. The sandwiched layer ZnO, at depth 2 (ZnO: D2), is shown in Fig. 2(d). The OII/Ototal at this particular depth is 56.39%. Figure 2(e) represents the O 1s spectra of AZO, which was Gaussian deconvoluted into three peaks. The two peaks that appear at OI (530.15 eV) and OII (531.25 eV) are related to the oxygen bounded as (Al–O and Zn–O) and oxygen vacancies, respectively. The third peak at OIII (532.4 eV) is the loosely bound chemisorbed oxygen. Consequently, the ratio OII/Ototal for the AZO top layer is found to be 74.82%. For the bottom layer ITO, O 1s spectra analysis has been done as shown in Fig. 2(f), and deconvoluted peaks are found to be at OI (530.02 eV), OII (531.38 eV), and OIII (532.78 eV). The OII/Ototal in this layer results as 27.87%.

FIG. 2.

(a) Depth profile spectra analysis performed for the optimized sample deposited at Ar/O2 = 2/1. XPS results from deconvolution of (b) Zn 2p3/2 spectra. O 1s spectra at different depths (c), ZnO (depth D1), (d) ZnO (depth D2), (e) AZO, the top layer, and (f) ITO, the bottom layer.

FIG. 2.

(a) Depth profile spectra analysis performed for the optimized sample deposited at Ar/O2 = 2/1. XPS results from deconvolution of (b) Zn 2p3/2 spectra. O 1s spectra at different depths (c), ZnO (depth D1), (d) ZnO (depth D2), (e) AZO, the top layer, and (f) ITO, the bottom layer.

Close modal

The characterization of the constructed devices using their current–voltage (I–V) characteristics is depicted in Fig. 3(a), with +5 and −2 V biases applied for set and reset operations, respectively. In the transristor's operation, the redox process leads to the generation of an electric field. This electric field, in turn, plays a vital role in modulating the transristor's conductivity and thereby controlling its switching behavior. The presence of oxygen vacancies created is confirmed through XPS analysis of the oxide layer. These vacancies then migrate toward the switching zinc oxide upon applying a positive bias to the AZO top electrode (TE) and a negative bias to the indium-doped tin oxide (ITO) bottom electrode (BE). As the concentration of oxygen vacancies in the ZnO layer increases, a conducting filament (CF) develops between the top and bottom electrodes creating a low resistance state (LRS). This phenomenon leads to the transition of the devices from a high-resistance state (HRS), representing the off-state, to an LRS, indicating the on-state. Additionally, the device is switched from an on position, i.e., from LRS to HRS by the re-ionized oxygen ions filling the voids that cause the filament to rupture. First, the switching procedure needs to be started by applying higher positive voltage by forming an initial filament from the pristine state. About +5 V is required as a forming voltage for all the devices. When a positive voltage is applied to the TE, the current flowing through the device gradually rises until it reaches the 1 mA compliance current (CC). Concurrently, the stated device undergoes a transition in resistance level, shifting from an HRS to an LRS. This process is commonly referred to as the “set procedure,” characterized by the formation of a CF. During the reset process, initiated by applying −2 V, the current flowing through the device gradually decreases as the CF is disrupted. Consequently, the device changes its state from set to reset (i.e., LRS to HRS).25,26 When a positive voltage ranging from 0 to 5 V is applied to the device, a moderate increase in current is observed, particularly for the Ar/O2 ratio of 2/1, as depicted in Fig. 3(b). However, the current spikes up to the specified CC at 5 V. The device deposited with a gas ratio of 3/0 exhibits an abrupt increase in current upon applying a voltage between 0 and +5 V, as demonstrated in Fig. 3(c). This abrupt current leads to poor synaptic properties. According to the I–V characteristics, bipolar resistive switching can be achieved through conductivity modulation with the application of either a positive or negative voltage for all the devices. The switching curves confirm that current levels vary proportionally to voltage and polarity due to charge trapping and de-trapping processes. This state demonstrates the device's synaptic behavior of LTP and LTD.

FIG. 3.

Current–voltage switching characteristics of the transristors at different Ar/O2 ratios at (a) 1/1, (b) 2/1, and (c) 3/0.

FIG. 3.

Current–voltage switching characteristics of the transristors at different Ar/O2 ratios at (a) 1/1, (b) 2/1, and (c) 3/0.

Close modal

Figures 4(a)4(c) show the device's endurance characteristics at +0.1 V read voltage. The device with a 2/1 gas ratio maintains stability and a comparable ratio throughout set/reset operation over 500 cycles, with no degradation between LRS and HRS, as shown in Fig. 4(b). In contrast, the other two devices experience poor ratio compared to the device fabricated at the gas ratio of 2/1 and suffer with resistance state stability after only 100 cycles when using a sample that is not deposited without oxygen atmosphere, i.e., the gas ratio of 3/0, as illustrated in Fig. 4(c). The I–V characteristics for all cycles of the devices of (a) Ar/O2 = 1/1, (b) Ar/O2 = 2/1, and (c) Ar/O2 = 3/0 are shown in Fig. S1 in the supplementary material. The stability of the states from low resistance and high resistance over time is utilized to determine the retention characteristics of the transristor. Retention is measured by applying the read voltage and recording the corresponding current response from the device for both resistive states. When the Ar/O2 gas ratio of 1/1 is used in the deposition process, as shown in Fig. 4(a), a significant difference is observed between the two resistance states in the resistive switching devices. On the other hand, Ar/O2 having 2/1 flow ratio exhibits an excellent retention of 104 s for non-volatile memory and neuromorphic computing, as shown in Fig. 4(d).

FIG. 4.

Endurance characteristics of the different transristors operated at a read voltage of 0.1 V for 500 cycles for Ar/O2 at (a) 1/1, (b) 2/1, and (c) 3/0. (d) Retention test of the transristor fabricated at Ar/O2 = 2/1.

FIG. 4.

Endurance characteristics of the different transristors operated at a read voltage of 0.1 V for 500 cycles for Ar/O2 at (a) 1/1, (b) 2/1, and (c) 3/0. (d) Retention test of the transristor fabricated at Ar/O2 = 2/1.

Close modal

Various pulse signals are applied at varying Ar/O2 ratios to examine the synaptic behavior of the transristor. The reaction of the transristor to applying positive and negative pulses is depicted in Fig. 5 in terms of potentiation and depression. For the synaptic measurement of Ar/O2 = 1/1, as shown in Fig. 5(a), an optimized pulse train is applied with a 10 μs width and +0.92 V amplitude for potentiation/−0.96 V amplitude for depression. The device with Ar/O2 = 2/1 is subjected to an optimized pulse train with a 10 μs pulse width and +0.72 V amplitude for potentiation/−0.81 V amplitude for depression, as depicted in Fig. 5(b). For Ar/O2 = 3/0, a pulse train with 10 μs width and +0.8 V amplitude for potentiation/−0.72 V amplitude for depression is energized, as illustrated in Fig. 5(c). To achieve both depression and potentiation during the read condition, a consistent 0.1 V amplitude and 1 ms pulse width is applied to each device. Ar/O2 = 2/1 improves the potentiation and depression linearity values, competing with the sample for a better fit for neuromorphic application than the other prepared devices. Moreover, by energizing a sequence of pulses, the device replicates potentiation and depression cycles and maintains a stable conductance ratio over multiple cycles (>25 cycles).

FIG. 5.

Potentiation/depression curves along with linearity calculation and respective pulses scheme applied to the transristor fabricated at Ar/O2 ratios (a) 1/1, (b) 2/1, and (c) 3/0. Nonlinearity value calculation for the optimized device at (d) first cycle, (e) middle cycle, and (f) last cycle.

FIG. 5.

Potentiation/depression curves along with linearity calculation and respective pulses scheme applied to the transristor fabricated at Ar/O2 ratios (a) 1/1, (b) 2/1, and (c) 3/0. Nonlinearity value calculation for the optimized device at (d) first cycle, (e) middle cycle, and (f) last cycle.

Close modal
The following specific equations are simulated to evaluate the nonlinearity in the potentiation and depression cycles of the prepared transristors:
(1)
(2)
where
(3)

The conductance values for the LTD and LTP are shown by GLTD and GLTP, respectively. Maximum conductance (Gmax), minimum conductance (Gmin), maximum pulse number (Pmax), controllable variable (A) that provides information on nonlinear behavior, and dependent parameter (B) on variable (A). Equations (1)–(3) are utilized to determine the non-linearity of the transristors in terms of αp/αd (potentiation/depression). The results show that for Ar/O2 with 1/1, 2/1, and 3/0 gas flow ratios, αp/αd is 4.11/4.74, 2.31/3.05, and 3.20/4.50, respectively. According to the aforementioned findings, the transristor with an Ar/O2 = 2/1 gas flow ratio has improved non-linearity for both potentiation and depression, making the device appropriate for neuromorphic computing applications. Such improvements in non-linearity in the device prepared at Ar/O2 = 2/1 gas flow ratio may be due to the controlled growth and rupture of filaments formed by oxygen vacancies. The non-linearity value of the optimized device is calculated for three cycles—first, middle, and the last cycles, as shown in Figs. 5(d)5(f), which is found to be consistent as 2.42/3.07, 2.51/3.15, and 2.42/3.07, respectively.

Figure 6 illustrates the conductance values of the fabricated transristors for different ratios of Ar/O2. Notably, in Fig. 6(a), the sample with Ar/O2 = 1/1 demonstrates minimal alteration in conductance values for up to six cycles when subjected to consecutive potentiation and depression cycles. On the contrary, while the cycle number increases for Ar/O2 = 3/0, as shown in Fig. 6(b), the conductance value falls. For depression and potentiation, superior 200 pules are administered to each Ar/O2 = 2/1 pair, as depicted in Fig. 6(c). It is evident that for more than 25 cycles, the conductance states remain stable, indicating suitability for synaptic applications. The electrical characteristics of the manufactured gadget are compiled in Table I.

FIG. 6.

Illustrates the long-term potentiation/depression (LTP/LTD) cycles with different pulse schemes applied to the AZO/ZnO/ITO transristor for (a) Ar/O2 = 1/1 (+0.92 V for potentiation and −0.96 V for depression), (b) Ar/O2 = 3/0 (+0.72 V for potentiation and −0.81 V for depression), and (c) Ar/O2 = 2/1 (+0.8 V for potentiation and −0.72 V for depression).

FIG. 6.

Illustrates the long-term potentiation/depression (LTP/LTD) cycles with different pulse schemes applied to the AZO/ZnO/ITO transristor for (a) Ar/O2 = 1/1 (+0.92 V for potentiation and −0.96 V for depression), (b) Ar/O2 = 3/0 (+0.72 V for potentiation and −0.81 V for depression), and (c) Ar/O2 = 2/1 (+0.8 V for potentiation and −0.72 V for depression).

Close modal
TABLE I.

Summary of the electrical characteristics of the AZO/ZnO/ITO transristor.

Characteristics AZO/ZnO/ITO transristorFor different Ar/O2 flow rates (ZnO film)
1/12/13/0
Resistance switching, set/reset voltages, in Volt, V 1.5/−2.5 1.4/−2 1.7/−2 
Endurance (in cycles) 500 500 200 
Potentiation/depression linearity (αpd4.11/4.74 2.31/3.05 3.2/4.5 
Stability (in cycles) 25 
Characteristics AZO/ZnO/ITO transristorFor different Ar/O2 flow rates (ZnO film)
1/12/13/0
Resistance switching, set/reset voltages, in Volt, V 1.5/−2.5 1.4/−2 1.7/−2 
Endurance (in cycles) 500 500 200 
Potentiation/depression linearity (αpd4.11/4.74 2.31/3.05 3.2/4.5 
Stability (in cycles) 25 
To explore the potential applications of the memristors for transparent electronics, the optimized device's transparency is evaluated utilizing a UV-visible spectrophotometer. The transparency characteristics are depicted in Fig. 7(a). The device's transmittance is greater than 90% in the visible range, making it a potential candidate for the applications. It is evident from the inset of Fig. 7(a), the manufactured transristor is nearly diaphanous, as it supports the UV-visible spectra. The following Tauc's formula is used to determine the device's optical bandgap (Eg):
(4)
where h is Planck's constant, K is the energy-independent constant, α is the absorption coefficient, ν is the incident photon's frequency, n is the nature of transmission, and Eg is the optical bandgap. The calculated optical bandgap that refers to the energy difference between the highest occupied and lowest unoccupied energy level of the optimized transristor is given by 3.22 eV, as in Fig. 7(b). We have compared our results with other reported results as depicted in Table II.
FIG. 7.

(a) UV-visible transmittance spectra of the optimized transristor in the visible region. The inset shows the photograph of the transparent device. (b) Calculation of optical bandgap using Tauc's plot.

FIG. 7.

(a) UV-visible transmittance spectra of the optimized transristor in the visible region. The inset shows the photograph of the transparent device. (b) Calculation of optical bandgap using Tauc's plot.

Close modal
TABLE II.

Performance comparative table of the transristor with other reported results of transparent ZnO-based memristors.

Sl. no.SubstrateDevice structure (TE/active layer/BE)Set/reset voltage (V/V)Retention (s)Endurance (cycles)Transmittance (in %)Reference
Glass ITO/ZnO/PCMO/ITO −2.6/2.3 … 103 84.6 27  
Glass ITO/AZO/ITO 0.5/−0.5 … 300 80 28  
Glass ITO/ZnO:Mg/FTO 1.8/−3 103 105 80 29  
Glass ITO/GZO/ITO 6/−7 … 350 86.5 30  
Glass ITO/IGZO/ITO −1/3.05 104 102 80 31  
Sapphire GZO/ZnO/GZO 2.2/1.6 … 80 32  
Quartz AZO/MZO/AZO 3/−4 105 50 82% 33  
PEN AZO/ZnO/ITO 1.4/−2 104 500 90 Our work 
Sl. no.SubstrateDevice structure (TE/active layer/BE)Set/reset voltage (V/V)Retention (s)Endurance (cycles)Transmittance (in %)Reference
Glass ITO/ZnO/PCMO/ITO −2.6/2.3 … 103 84.6 27  
Glass ITO/AZO/ITO 0.5/−0.5 … 300 80 28  
Glass ITO/ZnO:Mg/FTO 1.8/−3 103 105 80 29  
Glass ITO/GZO/ITO 6/−7 … 350 86.5 30  
Glass ITO/IGZO/ITO −1/3.05 104 102 80 31  
Sapphire GZO/ZnO/GZO 2.2/1.6 … 80 32  
Quartz AZO/MZO/AZO 3/−4 105 50 82% 33  
PEN AZO/ZnO/ITO 1.4/−2 104 500 90 Our work 

In this work, ZnO due to its unique properties is utilized as a switching film with different oxygen concentrations to fabricate the two-terminal transparent memristor-based synapses. The ZnO layer or the film deposited at Ar/O2 = 2/1 significantly enhances the switching mechanism in the device, as confirmed by the XPS result of Zn 2p3/2 and O 1s. The optimized device exhibits significant resistance switching behavior, with the lowest Vset/Vreset voltage of 1.4/−2 V. An acceptable endurance exceeding switching cycles of more than 500 is observed, indicating the device's reliability over repeated switching events. The device demonstrates good retention characteristics, with a retention time of 104 s, ensuring stable performance over time. Enhanced linearity of 2.31/3.05 is achieved for potentiation and depression, respectively, indicating precise control over the resistance switching process. The device maintains stability for 25 cycles without noticeable degradation, ensuring consistent performance over multiple operational cycles. With over 90% transparency, the optimized transristor can be integrated with invisible electronic applications, expanding its potential use cases. Therefore, applications involving invisible synapses are particularly suitable for these devices.

See the supplementary material for the IV characteristics of all cycles obtained for the device with Ar/O2 = 1/1, Ar/O2 = 2/1, and Ar/O2 = 3/0 as shown in Fig. S1.

This work was supported by the Department of Science and Technology (DST), Science and Engineering Research Board (SERB), Government of India, under core Project Grant No. CRG/2023/001265.

The authors have no conflicts to disclose.

Asutosh Patnaik: Data curation (equal); Formal analysis (equal); Methodology (equal); Software (equal); Writing – original draft (equal). Arpan Acharya: Formal analysis (equal); Visualization (equal). Kabin Tiwari: Investigation (equal); Visualization (equal). Priyanka Saha: Formal analysis (equal); Validation (equal). Narayan Sahoo: Supervision (equal); Validation (equal); Writing – review & editing (equal). Debashis Panda: Conceptualization (equal); Data curation (equal); Formal analysis (equal); Funding acquisition (equal); Investigation (equal); Methodology (equal); Project administration (equal); Resources (equal); Supervision (equal); Writing – review & editing (equal).

The datasets generated and/or analyzed during this study are not publicly available due to confidentiality but are available from the corresponding author upon reasonable request.

1.
G. E.
Moore
, “
Cramming more components onto integrated circuits
,”
Electron. Mag.
38
,
114
117
(
1965
).
2.
D.
Panda
,
C.
Chu
,
A.
Pradhan
,
S.
Chandrasekharan
,
B.
Pattanayak
,
S. M.
Sze
, and
T.
Tseng
, “
Synaptic behaviour of TiO x /HfO2 RRAM enhanced by inserting ultrathin Al2O3 layer for neuromorphic computing
,”
Semicond. Sci. Technol.
36
(
4
),
045002
(
2021
).
3.
S.
Chandrasekaran
,
F. M.
Simanjuntak
,
D.
Panda
, and
T.-Y.
Tseng
, “
Enhanced synaptic linearity in ZNO-based invisible memristive synapse by introducing double pulsing scheme
,”
IEEE Trans. Electron Devices
66
(
11
),
4722
4726
(
2019
).
4.
J.
Wang
,
D.
Ren
,
Z.
Zhang
,
H.
Xiang
,
J.
Zhao
,
Z.
Zhou
,
X.
Li
,
H.
Wang
,
L.
Zhang
,
M.
Zhao
,
Y.
Fang
,
C.
Lu
,
C.
Zhao
,
C. Z.
Zhao
, and
X.
Yan
, “
A radiation-hardening Ta/Ta2O5-x/Al2O3/InGaZnO4 memristor for harsh electronics
,”
Appl. Phys. Lett.
113
(
12
), 122907 (
2018
).
5.
Z.
Peng
,
F.
Wu
,
L.
Jiang
,
G.
Cao
,
B.
Jiang
,
G.
Cheng
,
S.
Ke
,
K.
Chang
,
L.
Li
, and
C.
Ye
, “
Hfo2-based memristor as an artificial synapse for neuromorphic computing with tri-layer HfO2/BiFeO3/HfO2 design
,”
Adv. Funct. Mater.
31
(
48
), 2107131 (
2021
).
6.
T.
Chang
,
S.-H.
Jo
,
K.-H.
Kim
,
P.
Sheridan
,
S.
Gaba
, and
W.
Lu
, “
Synaptic behaviors and modeling of a metal oxide memristive device
,”
Appl. Phys. A
102
(
4
),
857
863
(
2011
).
7.
D.
Panda
and
A.
Patnaik
, “
Novel TiO2-based memristors FET with programmable SET/RESET for neuromorphic computing
,”
Mater. Today Proc.
(
2023
).
8.
J. J.
Yang
,
M. D.
Pickett
,
X.
Li
,
D.
a
.
A.
Ohlberg
,
D. R.
Stewart
, and
R. S.
Williams
, “
Memristive switching mechanism for metal/oxide/metal nanodevices
,”
Nat. Nanotechnol.
3
(
7
),
429
433
(
2008
).
9.
T.
Shi
,
X.-B.
Yin
,
R.
Yang
, and
X.
Guo
, “
Pt/WO3/FTO memristive devices with recoverable pseudo-electroforming for time-delay switches in neuromorphic computing
,”
Phys. Chem. Chem. Phys.
18
(
14
),
9338
9343
(
2016
).
10.
Y.
Zhu
,
J.-S.
Liang
,
X.
Shi
, and
Z.
Zhang
, “
Full-inorganic flexible Ag2S memristor with interface resistance–switching for energy-efficient computing
,”
ACS Appl. Mater. Interfaces
14
(
38
),
43482
43489
(
2022
).
11.
Z.-M.
Liao
,
C.
Hou
,
H.-Z.
Zhang
,
D.-S.
Wang
, and
D.-P.
Yu
, “
Evolution of resistive switching over bias duration of single Ag2S nanowires
,”
Appl. Phys. Lett.
96
(
20
), 203109 (
2010
).
12.
C.
Yang
,
H.
Fan
,
S.
Qiu
,
Y.
Xi
, and
Y.
Fu
, “
Microstructure and dielectric properties of La2O3 films prepared by ion beam assistant electron-beam evaporation
,”
J. Non-Cryst. Solids
355
(
1
),
33
37
(
2009
).
13.
B.
Peng
,
H.
Fan
, and
Q.
Zhang
, “
A giant electrocaloric effect in nanoscale antiferroelectric and ferroelectric phases coexisting in a relaxor PB0.8Ba0.2ZRO3 thin film at room temperature
,”
Adv. Funct. Mater.
23
(
23
),
2987
2992
(
2013
).
14.
R.
Singh
,
M.
Kumar
,
S.
Iqbal
,
H.
Kang
,
J.-Y.
Park
, and
H.
Seo
, “
Highly transparent solid-state artificial synapse based on oxide memristor
,”
Appl. Surf. Sci.
536
,
147738
(
2021
).
15.
M.
Kumar
,
S.
Abbas
, and
J.
Kim
, “
All-oxide-based highly transparent photonic synapse for neuromorphic computing
,”
ACS Appl. Mater. Interfaces
10
(
40
),
34370
34376
(
2018
).
16.
D.-C.
Hu
,
R.
Yang
,
L.
Jiang
, and
X.
Guo
, “
Memristive synapses with photoelectric plasticity realized in ZnO1–x/AlOy heterojunction
,”
ACS Appl. Mater. Interfaces
10
(
7
),
6463
6470
(
2018
).
17.
M.
Lee
,
W.
Lee
,
S.
Choi
,
J.
Jo
,
J.
Kim
,
S. K.
Park
, and
Y.
Kim
, “
Brain-inspired photonic neuromorphic devices using photodynamic amorphous oxide semiconductors and their persistent photoconductivity
,”
Adv. Mater.
29
(
28
), 1700951 (
2017
).
18.
H.
He
,
R.
Yang
,
W.
Zhou
,
H.
Huang
,
J.
Xiong
,
L.
Gan
,
T.
Zhai
, and
X.
Guo
, “
Photonic potentiation and electric habituation in ultrathin memristive synapses based on monolayer MOS2
,”
Small
14
(
15
), 1800079 (
2018
).
19.
H.-L.
Park
and
M.
Choi
, “
Flexible transparent memory systems based on solution-processed organic memristors
,”
J. Korean Phys. Soc.
81
(
3
),
285
289
(
2022
).
20.
A.
Saleem
,
D.
Kumar
,
F.
Wu
,
L. B.
Keong
, and
T.-Y.
Tseng
, “
An opto-electronic HfO x -based transparent memristive synapse for neuromorphic computing system
,”
IEEE Trans. Electron Devices
70
(
3
),
1351
1358
(
2023
).
21.
X.
Yan
,
X.
Li
,
Z.
Zhou
,
J.
Zhao
,
H.
Wang
,
J.
Wang
,
L.
Zhang
,
D.
Ren
,
X.
Zhang
,
J.
Chen
,
C.
Lu
,
P.
Zhou
, and
Q.
Liu
, “
Flexible transparent organic artificial synapse based on the Tungsten/Egg albumen/indium tin oxide/polyethylene terephthalate memristor
,”
ACS Appl. Mater. Interfaces
11
(
20
),
18654
18661
(
2019
).
22.
S.
Dhar
,
T.
Majumder
, and
S. P.
Mondal
, “
Graphene quantum dot-sensitized ZnO nanorod/polymer Schottky junction UV detector with superior external quantum efficiency, detectivity, and responsivity
,”
ACS Appl. Mater. Interfaces
8
(
46
),
31822
31831
(
2016
).
23.
S.
Dhar
,
T.
Majumder
,
P.
Chakraborty
, and
S. P.
Mondal
, “
DMSO modified PEDOT:PSS polymer/ZnO nanorods Schottky junction ultraviolet photodetector: Photoresponse, external quantum efficiency, detectivity, and responsivity augmentation using N doped graphene quantum dots
,”
Org. Electron.
53
,
101
110
(
2018
).
24.
M. M.
Nauman
,
M. Z.
Esa
,
J. H.
Zaini
,
A.
Iqbal
, and
S. A.
Bakar
, “
Zirconium oxide based memristors fabrication via electrohydrodynamic printing
,” in
2020 IEEE 11th International Conference on Mechanical and Intelligent Manufacturing Technologies (ICMIMT)
,
Cape town, South Africa
(
IEEE
, 2020), pp.
167
171
.
25.
C.-L.
Lin
,
C.-C.
Tang
,
S.-C.
Wu
,
P.-C.
Juan
, and
T.-K.
Kang
, “
Impact of oxygen composition of ZnO metal-oxide on unipolar resistive switching characteristics of Al/ZnO/Al resistive RAM (RRAM)
,”
Microelectron. Eng.
136
,
15
21
(
2015
).
26.
F. M.
Simanjuntak
,
S.
Chandrasekaran
,
C.-C.
Lin
, and
T.-Y.
Tseng
, “
Zno2/ZnO bilayer switching film for making fully transparent analog memristor devices
,”
APL Mater.
7
(
5
), 051108 (
2019
).
27.
R.
Zhang
,
J.
Miao
,
F.
Shao
,
W. T.
Huang
,
C.
Dong
,
X. G.
Xu
, and
Y.
Jiang
, “
Transparent amorphous memory cell: A bipolar resistive switching in ZnO/Pr0.7Ca0.3MnO3/ITO for invisible electronics application
,”
J. Non-Cryst. Solids
406
,
102
106
(
2014
).
28.
H.
Yu
,
M.
Kim
,
Y.
Kim
,
J.
Lee
,
K.-K.
Kim
,
S.-J.
Choi
, and
S.
Cho
, “
Al-doped ZnO as a switching layer for transparent bipolar resistive switching memory
,”
Electron. Mater. Lett.
10
(
2
),
321
324
(
2014
).
29.
L.
Shi
,
D.
Shang
,
J.
Sun
, and
B.
Shen
, “
Bipolar resistance switching in fully transparent ZNO:MG-based devices
,”
Appl. Phys. Express
2
(
10
),
101602
(
2009
).
30.
A.
Kim
,
K.
Song
,
Y.
Kim
, and
J.
Moon
, “
All solution-processed, fully transparent resistive memory devices
,”
ACS Appl. Mater. Interfaces
3
(
11
),
4525
4530
(
2011
).
31.
M.-C.
Chen
,
T.-C.
Chang
,
S.-Y.
Huang
,
S.-C.
Chen
,
C.-W.
Hu
,
C.-T.
Tsai
, and
S. M.
Sze
, “
Bipolar resistive switching characteristics of transparent indium gallium zinc oxide resistive random access memory
,”
Electrochem. Solid-State Lett.
13
(
6
),
H191
(
2010
).
32.
P.
Misra
,
A. K.
Das
, and
L. M.
Kukreja
, “
Switching characteristics of ZnO based transparent resistive random access memory devices grown by pulsed laser deposition
,”
Phys. Status Solidi C
7
(
6
),
1718
1720
(
2010
).
33.
X.
Cao
,
X.
Li
,
X.
Gao
,
X.
Liu
,
C.
Yang
,
R.
Yang
, and
P.
Jin
, “
All-ZnO-based transparent resistance random access memory device fully fabricated at room temperature
,”
J. Phys. D: Appl. Phys.
44
(
25
),
255104
(
2011
).