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Article

Multi-Channel Sensing System Utilizing Mott Memristors for Single-Wire Data Fusion and Back-End Greedy Strategy Data Recovery

1
School of Microelectronics, Xi’an Jiaotong University, Xi’an 710049, China
2
Aerial Photogrammetry and Remote Sensing Group Co., Ltd. of CNACG (ARSC), Xi’an 710199, China
*
Authors to whom correspondence should be addressed.
Electronics 2024, 13(2), 345; https://doi.org/10.3390/electronics13020345
Submission received: 26 November 2023 / Revised: 2 January 2024 / Accepted: 11 January 2024 / Published: 13 January 2024
(This article belongs to the Special Issue Advances in Analog and Mixed-Signal Integrated Circuits)

Abstract

:
This paper presents a novel Mott memristor-based multi-channel sensing system designed for the simultaneous processing of multiple sensing channels, employing single-wire data fusion and a greedy search strategy for back-end data recovery. Multiple channels of external stimulus information are simultaneously encoded into analog signals with varying frequencies, utilizing a Mott memristor array. Auxiliary circuits then convert the analog sensing signals into square wave signals which are further transformed into narrow (100 ns) pulse signals through pulse generation circuitry. Subsequently, these narrow pulse signals are fused into a single-wire signal by using an OR gate. At the back-end of the system, a greedy searching strategy is applied to accurately identify all frequencies within the fused pulse signal, enabling seamless analog-to-frequency conversion across multiple channels. The system is suitable for a wide range of sensors and can be directly connected to FPGAs for data processing, eliminating the need for traditional analogue front-end and ADC circuits and greatly reducing circuit complexity and power consumption. By leveraging the innovative capabilities of Mott memristors, the proposed system achieves precise analog-to-frequency conversion with significantly reduced power consumption.

1. Introduction

In recent years, there has been a growing demand for high-performance, low-power sensing systems capable of efficiently converting analog signals from multiple sensors into a digital format for further processing [1,2,3,4,5]. Traditional approaches often rely on complex analog front-end circuits and analog-to-digital converters (ADCs), which not only consume significant power but also introduce design complexities. To address these challenges, researchers have been exploring alternative solutions that offer improved efficiency and reduced power consumption [6,7,8,9,10]. One such innovative solution is the integration of Mott memristors into multi-channel sensing systems [11]. Mott memristors, with their unique characteristics such as non-volatile resistance switching behavior and low power consumption, have emerged as promising devices for analog signal processing. They enable multi-channel analog-to-frequency conversion, making them ideal for applications with a large number of sensors.
This work introduces a novel approach that leverages a Mott memristor array integrated with auxiliary circuits to convert analog signals into square wave signals with varying frequencies. The square wave signals are then transformed into pulse signals through dedicated pulse generation circuitry and integrated using an OR gate to achieve data fusion. At the backend of the system, a greedy search algorithm accurately identifies all frequencies present in the fused pulse signal, enabling multi-channel analog-to-frequency conversion.
Compared to traditional approaches, the Mott memristor-based multi-channel sensing system offers several advantages [12,13,14,15,16,17]. Firstly, it significantly reduces power consumption while simplifying circuit design. By leveraging Mott memristors for efficient analog-to-frequency conversion, the system eliminates the need for power-hungry ADCs, resulting in substantial power savings. Additionally, the seamless integration of the system with FPGA platforms enables efficient data processing, further enhancing overall system performance.
The implications of this research are wide-ranging, with potential applications in environmental monitoring, health tracking, and industrial automation, among others [16]. By providing an efficient and reliable solution for multi-channel analog-to-frequency conversion, the proposed system holds great promise for advancing sensing technologies in various domains.
Given the limitations of traditional analog front-end circuits and the increasing demand for low-power, high-performance sensing systems, this study aims to make a significant contribution to the field of integrated circuits by introducing a novel Mott memristor-based approach for multi-channel analog-to-frequency conversion. The designed system effectively addresses the limitations of traditional analog front-end circuits, offering a high-performance, low-power solution that is particularly relevant in the context of modern integrated circuit design. By seamlessly integrating Mott memristors with auxiliary circuits and advanced signal processing techniques, this research presents a comprehensive framework for efficient multi-channel analog-to-frequency conversion, potentially impacting a broad spectrum of applications.
The subsequent sections will delve into the design and implementation details of the proposed multi-channel sensing system, followed by experimental results and discussions on its performance metrics. Finally, conclusions will be drawn, highlighting the significance of this research and outlining potential avenues for future work. By shedding light on the practical aspects and demonstrating the effectiveness of the proposed approach, we aim to not only enrich the understanding of Mott memristor-based systems but also pave the way for future innovations in the field of integrated circuits and sensor technologies.

2. Sensing System Architecture

The development of the Mott memristor-based multi-channel sensing system represents a significant breakthrough in the field of electronic sensing technologies. The architecture of the proposed sensing system is illustrated in Figure 1, showcasing its unique features and operational principles.
The front-end sensing module comprises a 3 × 3 sensor array, a Mott memristor array, a narrow pulse generator, and an OR gate for data fusion. The sensor array is responsible for converting the external stimuli into changes in resistance and capacitance, while the Mott memristor array generates rate-coded spikes based on the changes in the sensor array [18,19,20,21]. These spikes are then shaped into a square wave and transformed into a narrow pulse wave, which is subsequently transmitted to the FPGA board for data fusion.
To enable efficient data recovery, the single-wire output generated by the FPGA board is processed using the greedy strategy. This approach involves iteratively selecting the most significant features from the input signal, thus enabling the recovery of high-quality data with a minimal loss of information.
Overall, the proposed Mott memristor-based sensing system presents a novel and innovative approach to multi-channel electronic sensing. The combination of the sensor array and Mott memristor array facilitates the generation of rate-coded spikes, which can be efficiently processed and fused using the narrow pulse generator circuit and FPGA. The implementation of the greedy strategy for data recovery further enhances the performance and reliability of the proposed sensing system, thus establishing a solid foundation for its potential utilization across diverse electronic applications.

3. Mott Memristor

3.1. Fabrication of the Mott Memristor

The successful fabrication of the Mott memristor is essential for its potential application in electronic devices and systems. The structure of the Mott memristor is depicted in Figure 2a, while a more detailed illustration is presented in Figure 2b.
To fabricate the Mott memristor, a via hole (~10 µm) structure of Ti/W/NbOx/Nb/Pt crossbar is utilized on a silicon wafer with 300 nm SiO2. The bottom electrode (BE) and insulating layer are deposited using radio frequency (RF) magnetron sputtering, with Ti/W (~10 nm/80 nm) and Al2O3 (~30 nm), respectively. These layers are then patterned in a lift-off process. Subsequently, a NbOx (~50 nm) film is prepared as the switching layer using RF magnetron sputtering and a Nb target in an Ar:O2 = 30:2 sccm ambient at room temperature. Finally, the top electrode (TE) consisting of Nb/Pt (~50 nm/100 nm) is sputtered and patterned [22,23].
The utilization of this specific fabrication process ensures the creation of a high-quality Mott memristor with excellent performance characteristics. The precision of the fabrication process is critical to achieving optimal device performance and reliability. Furthermore, the use of a via hole structure helps to minimize the size of the device, thus enabling its integration into small-scale electronic devices.
Overall, the successful fabrication of the Mott memristor through this specific process, together with its unique structural features, underpins its potential utilization across diverse electronic applications. Further research in this field could potentially result in the development of more advanced and efficient memristive devices.

3.2. Operating Principle of Mott Memristor

Figure 3 illustrates the current-voltage (I-V) DC sweep characteristic of the Mott memristor, showcasing its ability to undergo stable bidirectional transitions between low and high resistance states. As the applied voltage progressively increases from zero to approximately 1.57 V, a notable surge in current is observed, signifying a transition from the high-resistance state to the low-resistance state. This particular voltage level is commonly referred to as the threshold voltage (Vth). Conversely, when the voltage declines from 2 V to around 1.17 V, a sharp decline in current occurs, indicating a transition from the low-resistance state back to the high-resistance state. This specific voltage value is known as the hold voltage (Vhold).
The schematics depicted in Figure 4 present two variations of the spike generation circuits based on the Mott memristor: one driven by a voltage source and another driven by a current source [24,25], denoted as Figure 4a and Figure 4b respectively. To enable oscillation, the Mott memristor necessitates the presence of a capacitor (CP). The distinctive spike waveform, with an amplitude ranging between Vth and Vhold, is generated by the charge and discharge operations of the capacitor CP.
The frequency of the generated spikes is closely related to the Cp and connected resistor Rs in the circuits. When CP and Rs are replaced with capacitive sensors or resistive sensors, the stimuli applied to the sensors are then encoded into the spike rates.
The spike rate f, is expressed by
f = 1 t r + t f
where tr and tf are the rise time and fall time of the output voltage spikes.
As for the circuit in Figure 4a,
t r = R H C P ln V t h V i n R H R S V h o l d V i n R H R S
t f = R L C P ln V h o l d V i n R L R S V t h V i n R L R S
where RH and RL are the high resistance and low resistance of the Mott memristor.
As for the circuit in Figure 4b,
t r = R H C P ln I i n R H V h o l d I i n R H V t h
t f = R L C P ln V t h I i n R L V h o l d I i n R L
The recorded I-V DC sweep characteristics, together with the accompanying schematic diagrams, effectively elucidate the fundamental characteristics and operating principles of the spike generation circuit-based Mott memristor. These significant findings provide valuable insights into the behavior and functionality of the Mott memristor, thus providing a solid foundation for its potential integration and application in various electronic devices and systems.

4. Circuit and Back-End Implementation

4.1. Narrow Pulse Generator

The narrow generator circuit is shown in Figure 5 and Figure 6. To simplify data processing, conversion of the spike wave from the Mott memristor array into a pulse wave is necessary. Initially, this is accomplished by shaping it into a square wave through the use of a comparator. The traditional scheme uses a reference voltage, as shown in Figure 5a, which means that additional voltage reference circuits are required, usually the bandgap voltage reference circuits with trimming, which apparently increases the complexity of the scheme. In addition, each Mott memristor requires a different reference voltage if the DC value of the spike wave is not fixed. Therefore, this scheme is not suitable for large sensor arrays due to inefficiency as well as inconvenience.
The method used in this paper differs from the conventional approach which involves a reference voltage, as shown in Figure 5b. Instead, it involves comparing the original spike wave with the spike wave after RC low-pass filtering. This can prevent the need for varying reference voltages in the array due to the Mott memristor’s non-uniformity and DC drift.
Generating a pulse wave from a square wave requires a delay unit made up of buffers and an adjustable resistor as shown in Figure 6a [26]. And the waveform diagram is shown in Figure 6b. The square wave is split into two signals, one of which is added to an inverter and the other to the delay unit. As a result, when the square wave signal turns to “0”, the inverted signal then turns to “1” and the delayed signal briefly remains “1”, the output of the AND gate is pulled up, generating a narrow pulse at the falling edge of the square wave.

4.2. Rail-to-Rail Input Comparator

Figure 7, shows the schematic of the comparator. A rail-to-rail symmetrical amplifier is used to achieve a wide input voltage range, with transistors MN1, MN2, MP4, and MP6 forming the input stage. A buffer is also required to shape the output and improve the comparator’s drive capability.

4.3. Greedy Strategy Data Recover

The process of the greedy search strategy for data recovery is shown in Figure 8. This operates as follows [27]: when the square wave signal that is generated by the Mott memristor passes through the multi-input OR gate for “fusion”, the pulse generation circuit transforms the different frequencies into pulse signals, significantly boosting the efficiency and success rate of the search algorithm. Subsequently, the specific positions of the rising edges of all pulses are detected and recorded in an array called P[n], where n denotes the nth pulse.
Once the positions of all pulses have been recorded over a period of time, the algorithm calculates and records the distance between P[0] and P[i] (where i = 1 at the beginning of the search) as d0, with P[0] serving as the starting point. The search then proceeds sequentially backwards, with P[i + 1] as the new starting point. It determines whether there exists a P[i + 1 + x] at a distance of d from P[i + 1]. At this juncture, two possible scenarios un-fold:
If such a point exists, it signals the presence of a sequence of period d between P[0] and P[n]. The algorithm removes this sequence from the overall array and verifies whether any remaining recorded pulse positions exist. If there are remaining positions, the search algorithm continues as described above until no more recorded pulse positions remain in the array. If there are no remaining positions, the search algorithm has successfully identified the period information d0~dm represented by all the pulses in the array.
If such a point does not exist, then i is incremented by 1 and the search algorithm continues as described above.
In summary, the greedy search algorithm leverages pulse generation circuitry to transform different frequencies of a square wave signal into pulse signals. These pulse positions are recorded in an array, and the algorithm seeks a sequence of period d between P[0] and P[n]. If such a sequence is found, it is removed from the array and the search algorithm continues. Otherwise, the search algorithm increments i and continues searching until a sequence is found or all recorded positions have been searched.
Compared to other time–frequency conversion techniques, the greedy strategy has the advantage of being intuitive, easy to understand, and simple to implement. Once the algorithm has made a decision, there is no need to go back and check the values calculated in the previous step, eliminating the need for exhaustive operations that may be required to find the optimal solution, which apparently speeds up the time–frequency conversion considerably.

5. Experimental Results and Analysis

The innovative multi-channel sensing system proposed in this study, which leverages Mott memristor technology, demonstrates exceptional capability in efficiently processing multiple streams of sensing information through a single-signal data wire. Rigorous testing and verification procedures have been conducted to thoroughly assess the performance and reliability of the Mott memristor, the multi-channel sensing system, and the back-end greedy strategy data recovery mechanism.
Figure 9 presents an insightful visual depiction of the experimental platform utilized in the validation of the proposed sensing system. This experimental setup encompasses a 3 × 3 piezoresistive sensor array, a Mott memristor array, a narrow pulse generator, and an FPGA. The piezoresistive sensor array serves as the primary interface for converting external stimuli into changes in resistance, while the Mott memristor array is responsible for generating rate-coded spikes based on the detected variations. The integration of the pulse generator and FPGA facilitates the efficient processing, fusion, and transmission of the output signals from the sensor array, demonstrating the comprehensive functionality of the experimental platform.

5.1. Oscillations of Mott

Figure 10 shows the oscillation driven by a voltage source. In this structure, the test conditions are an input voltage of 5 and RS of 20 kΩ. From the oscillation data for the first 20 μs, it can be seen that the oscillation frequency is about 1.15 MHz. In one hundred oscillation cycles, Vth and Vhold remain stable around 1.55 V and 1.20 V, respectively.
Figure 11 shows the oscillation driven by a current source. In this structure, the test conditions are an input current of 0.8 mA and CP of 4.7 nF. From the oscillation data for the first 100 μs, it can be seen that the oscillation frequency is about 210 kHz. In 20 oscillation cycles, Vth and Vhold remain stable around 1.55 V and 1.10 V, respectively. The measured results indicate that the Mott memristor is operating properly and stably.

5.2. Single-Wire Output of Nine-Channel Narrow Pulse Waveforms

The Mott-based sensor interface has been measured in a previous work [11]. After several tests, the results show that at a pressure of 0.5 N, the pressure sensor resistance is 11.5 kΩ and the Mott memristor produces a stable frequency of 27.47 kHz. At pressures of 3.2 N, 4.6 N, and 8.8 N, the Mott memristor produces frequencies of 64.19 kHz, 100.10 kHz, and 137.00 kHz, respectively. In the test, the RC low-pass filter in the pulse generator has a resistance of 4.7 kΩ and a capacitance of 2.2 nF, producing a pole at 15.4 kHz. Applying different pressures to each pressure-sensitive sensor, the measured waveform of the single-wire output of the nine-channel pulse waveforms of the sensing system is shown is shown in Figure 12a. The zoom-in waveforms and the narrow pulses with a width of 100 ns are successfully obtained as shown in Figure 12b, where the Ch-1 is the spike waveform generated by the Mott memristor, Ch-2 is the square waveform after comparator, Ch-3 is the narrow pulse waveform after the pulse generation circuit, and Ch-4 is the fused pulse waveform.

5.3. Greedy Strategy Data Recover

Considering that it is difficult to ensure constant pressures on nine piezoresistive sensors simultaneously and identify the channels, to facilitate verification of the sensing system, different RS, CP are set so that the Mott memristor array can generate spike waves of 10 kHz, 15 kHz, 22 kHz, 35 kHz, 50 kHz, 68 kHz, 90 kHz, 115 kHz, and 150 kHz, simulating the outputs of the piezoresistive sensor array and the Mott memristor array at different pressures. The results of greedy strategy data recovery are shown in Table 1.
The results show that data recovery using the greedy strategy is very accurate. For the actual piezoresistive sensor array, the greedy strategy is still able to recover the nine signals because the frequency of the system sampling clock is much higher than the frequency signals generated by the Mott memristors. Finally, Table 2 summarizes the performance comparison of this work with several state-of-the-art works. The proposed multi-channel sensing system utilizing Mott memristors has a wide range of applicability and can be used with various types of resistive or capacitive sensors such as light, pressure, humidity, and temperature. Multi-channel data transmission over a single wire is also an advantage for large sensor array applications.

6. Conclusions

In summary, we have proposed and validated a multi-channel sensing system based on Mott memristors, featuring single-wire data fusion and a back-end greedy strategy for data recovery. The key advantage of this design lies in the transmission of sensor array data through a single signal wire, and the effective data recovery achieved by the greedy strategy within an error margin of 1.5%. Leveraging Mott’s memristor enables the sensing system to achieve rapid and precise conversion at a remarkably low power consumption of only 13 mW.

Author Contributions

S.F. and P.L. proposed the architecture. S.F., S.Z. and J.X. designed the circuit and performed all of the measurements. Y.S. and C.H. wrote the initial manuscript, G.Z. supervised the manuscript. All authors have read and agreed to the published version of the manuscript.

Funding

This work was supported in part by the National Key R&D Program of China under Grant 2022YFB3203600, in part by the National Natural Science Foundation of China under Grant 62074124, and in part by the Key R&D plan of Shaanxi Province under Grant 2023-YBSF-407, 2022GY-337, and 2021GY-175.

Data Availability Statement

Data are contained within the article.

Acknowledgments

The authors would like to thank all of the editors and reviewers for their valuable comments.

Conflicts of Interest

Author Junyi Xu was employed by the company Aerial Photogrammetry and Remote Sensing Group Co., Ltd. of CNACG (ARSC). The remaining 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.

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Figure 1. System architecture of the proposed Mott memristor-based multi-channel sensing system with single-wire data fusion and back-end greedy strategy data recovery.
Figure 1. System architecture of the proposed Mott memristor-based multi-channel sensing system with single-wire data fusion and back-end greedy strategy data recovery.
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Figure 2. (a) Microscopic image of the Mott memristor array; (b) structure of the Mott memristor cell.
Figure 2. (a) Microscopic image of the Mott memristor array; (b) structure of the Mott memristor cell.
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Figure 3. I-V DC sweeps of the Mott memristor.
Figure 3. I-V DC sweeps of the Mott memristor.
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Figure 4. Schematic of the spike generation circuits based on Mott memristors: (a) driven by a voltage source and (b) driven by a current source.
Figure 4. Schematic of the spike generation circuits based on Mott memristors: (a) driven by a voltage source and (b) driven by a current source.
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Figure 5. Spike-to-square wave conversion: (a) Comparator with reference Vref. (b) Comparator with a low-pass filter.
Figure 5. Spike-to-square wave conversion: (a) Comparator with reference Vref. (b) Comparator with a low-pass filter.
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Figure 6. Square to narrow pulse wave conversion: (a) Schematic. (b) Waveform diagram.
Figure 6. Square to narrow pulse wave conversion: (a) Schematic. (b) Waveform diagram.
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Figure 7. Schematic of designed rail-to-rail input comparator.
Figure 7. Schematic of designed rail-to-rail input comparator.
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Figure 8. Process of the greedy strategy data recovery.
Figure 8. Process of the greedy strategy data recovery.
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Figure 9. Photo of the experimental platform for the multi-channel sensing system, (a) test platform, (b) sensing system.
Figure 9. Photo of the experimental platform for the multi-channel sensing system, (a) test platform, (b) sensing system.
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Figure 10. Oscillation driven by a voltage source, structure diagram, and the threshold voltage extracted from the oscillation diagram.
Figure 10. Oscillation driven by a voltage source, structure diagram, and the threshold voltage extracted from the oscillation diagram.
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Figure 11. Oscillation driven by a current source, structure diagram, and the threshold voltage extracted from the oscillation diagram.
Figure 11. Oscillation driven by a current source, structure diagram, and the threshold voltage extracted from the oscillation diagram.
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Figure 12. Measured waveforms: (a) single-wire output of the nine-channel narrow pulse waveforms of the sensing system, (b) zoom-in waveforms.
Figure 12. Measured waveforms: (a) single-wire output of the nine-channel narrow pulse waveforms of the sensing system, (b) zoom-in waveforms.
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Table 1. Results of greedy strategy data recovery.
Table 1. Results of greedy strategy data recovery.
ChannelSetting FrequencyRecovered FrequencyError
110 kHz10.005 kHz+0.05%
215 kHz15.023 kHz+0.15%
322 kHz21.952 kHz−0.22%
435 kHz35.061 kHz+0.18%
550 kHz49.751 kHz−0.50%
668 kHz67.541 kHz−0.68%
790 kHz89.597 kHz−0.45%
8115 kHz115.665 kHz+0.58%
9150 kHz147.783 kHz−1.48%
Table 2. Performance summary and comparison with previously state-of-the-art sensing systems.
Table 2. Performance summary and comparison with previously state-of-the-art sensing systems.
JSSC-2019 [2]ISSCC-2019 [7]TCAS-II-2020 [9]JSSC-2020 [15]JSSC-2023 [28]This Work
Syst. ArchitectureSC +
Zoom SAR
WhB +
FIR ADC
CTC + TDCPGA + SAR ADCHBDCMott Memristor
+ FPGA
Process (μm)0.180.180.0650.180.1810 (Mott Memristor Array)
Area (mm2)2.940.120.020.722.520.24
Sensor TypeCapacitive-pressureResistive-
temperature
Capacitive
unlimited
Resistive-
pressure
Resistive-
pressure
Resistive
/Capacitive-
unlimited
Channels111119
Data Trans. Type----Single-WireSingle-Wire--Single-Wire
Real-Time
Data Recover----------Greedy strategy
Supply (V)1.1N/A11.81.81.8–3.3
Conversion (ms)0.85100.005111.5210
Resolution116 aF0.16 mK3.2 ps--0.24 mmHg25 ns @ 40 MHz
Measured range0~18.12 pF−55–125 °C0.82 s--500–1000 mmHgConfigurable
Power (W)3.09 μ79 μ10 μ12.3 μ12.79 μ13.0 m
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Fan, S.; Liu, P.; Shi, Y.; Zhao, S.; Han, C.; Xu, J.; Zhang, G. Multi-Channel Sensing System Utilizing Mott Memristors for Single-Wire Data Fusion and Back-End Greedy Strategy Data Recovery. Electronics 2024, 13, 345. https://doi.org/10.3390/electronics13020345

AMA Style

Fan S, Liu P, Shi Y, Zhao S, Han C, Xu J, Zhang G. Multi-Channel Sensing System Utilizing Mott Memristors for Single-Wire Data Fusion and Back-End Greedy Strategy Data Recovery. Electronics. 2024; 13(2):345. https://doi.org/10.3390/electronics13020345

Chicago/Turabian Style

Fan, Shiquan, Peihao Liu, Yongqiang Shi, Shujing Zhao, Chuanyu Han, Junyi Xu, and Guohe Zhang. 2024. "Multi-Channel Sensing System Utilizing Mott Memristors for Single-Wire Data Fusion and Back-End Greedy Strategy Data Recovery" Electronics 13, no. 2: 345. https://doi.org/10.3390/electronics13020345

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