- School of Electronic Science & Engineering, Nanjing University, Nanjing, China
Neuromorphic devices that can emulate the bionic sensory and perceptual functions of neural systems have great applications in personal healthcare monitoring, neuro-prosthetics, and human–machine interfaces. In order to realize bionic sensing and perception, it’s crucial to prepare neuromorphic devices with the function of perceiving environment in real-time. Up to now, lots of efforts have been made in the incorporation of the bio-inspired sensing and neuromorphic engineering in the booming artificial intelligence industry. In this review, we first introduce neuromorphic devices based on diverse materials and mechanisms. Then we summarize the progress made in the emulation of biological sensing and perception systems. Finally, the challenges and opportunities in these fields are also discussed.
Introduction
In addition to the achievements of artificial intelligence (AI), the engineering community has been trying to learn and imitate biological neural systems from almost all aspects, such as neural networks and robots, in order to seek artificial general intelligence (AGI). Biological neural systems have the characteristics of in-memory computing structure, large-scale parallel processing and event driven operation (Kuzum et al., 2013; Indiveri and Liu, 2015; Furber, 2016). Such characteristics allow us to perceive and react precisely when confronting to events of the real world in robust, fault tolerant and energy efficient modes (Merolla et al., 2014). Because of these, biological neural systems are more efficient and faster than any hardware/software computing platforms can accomplish for the given scale (Lohman, 1989; Picard et al., 2001). As the solution for efficient processing of enormous dataset sizes, electrical implementation of neural systems has been an important approach for external information acquisition (e.g., sensor), and more significantly, the external information processing and execution through cognitive processes (e.g., neuromorphic computing systems) (Delbruck et al., 2014). Artificial synapses can control information flow, data processing and memory function by modulating the synaptic weight (Voglis and Tavernarakis, 2006; Gkoupidenis et al., 2015). Hardware implementation of synaptic/neuronal functions represents a new-concept paradigm (Park et al., 2020).
The biological neural systems play the leading role in the regulation of physiological functions of vertebrates’ body. Such systems are mainly divided into two parts: central neural system (CNS,
i.e., the brain and spinal cord) and peripheral neural system (PNS, i.e., the sensory and motor nerves) (Lee and Lee, 2019). The CNS conducts high-level activities such as learning, memorizing and planning, and dominates the activities of the body in response to the information received from PNS. The PNS perceives and reacts to stimuli, e.g., light, sound, chemicals and pressure, and transmits this information between CNS and other parts of the body (Anderson, 2010). It’s worth noting that PNS can perform some low-level activities such as reflex and muscle activation directly (Wang et al., 2020). In other words, such sensory signals don’t need to be sent to the brain, and a perceptual decision is made immediately once the sensory signal reaches the spinal cord (Figure 1A). Compared with the brain, PNS processes low-level perceptual activities in a decentralized and localized manner. Localized processing cannot only quickly respond to external stimuli to maintain survival, but also reduce the computational burden of the brain (He K. et al., 2020; Tuchman et al., 2020; Figure 1B). Due to such merits, localized processing has been employed in interactive robotics (Groothuis et al., 2018; Wang et al., 2020).
Figure 1. (A) Biologically neural systems for sensing and perception. (B) Hierarchical functional framework of information processing in neuromorphic neural system (adapted from Wang et al., 2020).
As we know, neuromorphic engineering aims to build bio-inspired cognitive systems to emulate biological neural sensing and processing capabilities; in the meantime, neuromorphic engineering derivates synaptic devices (Field, 1994; Cohen et al., 1997; Kandel, 2001). When performing tasks like pattern classification and feature extraction, artificial neural network based on synaptic devices can effectively implement machine learning algorithms (Lumpkin and Caterina, 2007; Dahiya et al., 2010; Abraira and Ginty, 2013). Inspired by the mentioned above, the incorporation of bio-inspired sensing and neuromorphic engineering technologies for emulating the functions of CNS and PNS may open up a new era for artificial intelligence. In pursuit of mimicking the CNSs and PNSs, two methods have been adopted: the development of synaptic devices with capabilities of information processing and detection of stimuli such as light, sound, chemicals and pressure; the development of artificial synaptic devices integrated with sensing elements (e.g., light, touch) (Park et al., 2020). The approach of device integration has been widely demonstrated for constructing artificial neural systems in recent years, and this method has the potential to be applied on next-generation wearable electronics, robotics, and neuro-prosthetics (Hammock et al., 2013; Wan et al., 2018). For example, artificial neural systems can help to replace damaged neurons, or they can be employed as tools in neuroscience to study sensory/motor neuronal disorders. Furthermore, artificial neural systems can be developed to realize sensory information extraction and analysis, as well as to settle problems in uncertain settings. These systems that able to perceive the environment and react accordingly will cast significant impact on the progress of artificial intelligence.
Here, recent progress in the development of neuromorphic devices for mimicking the bionic sensing and perception functions will be discussed. Firstly, we introduce the properties of the biological synapses and the diverse synaptic characteristics that should be mimicked by neuromorphic devices. Second, we discuss the neuromorphic devices based on various materials and operation mechanisms. Third, bionic sensing and perception for personal healthcare monitoring, robotics and neuro-prosthetics are reviewed. Last, we summarize the review and give a brief outlook. We are looking forward to providing a guideline for the future development of neuromorphic perception systems.
Biological Properties of Synapse
In the biological nervous system, synapses are divided into electrical synapses and chemical synapses; the former commonly exist in fish and amphibians, while the latter are common in mammals (Schmitt et al., 1976; Connors and Long, 2004; Pereda, 2014; Park et al., 2020). The origin and development of synaptic devices are inspired by the human brain, so only chemical synapses will be discussed. Synapses are composed of three parts: presynaptic membrane, synaptic cleft and postsynaptic membrane (Tsodyks et al., 1998; Pereda, 2014). When an action potential is transmitted to the synaptic corpuscle through axons, the permeability of the presynaptic membrane to Ca2+ increases. Then Ca2+ in the synaptic cleft enter the synaptic corpuscle, which promotes the close fusion between synaptic vesicle and presynaptic membrane (Mayford et al., 2012). The neurotransmitters in the vesicle are released into the synaptic cleft (Figure 2). Finally, they reach the postsynaptic membrane through diffusion, and immediately bind to the protein receptors on the postsynaptic membrane, causing excitatory postsynaptic potential/current (EPSP/EPSC) or inhibitory postsynaptic potential/current (IPSP/IPSC) (Neher, 1992; Mayford et al., 2012). The spatial sum of EPSC and IPSC (i.e., the sum of postsynaptic potentials that appear at different positions of the neuron) and the time sum of EPSC and IPSC (i.e., the sum of postsynaptic potentials that occur repeatedly at each synapse) are the criterions to judge whether they can trigger action potentials or not (Ferster and Jagadeesh, 1992; Thomson and Deuchars, 1994; Lewis et al., 2011; Pereda, 2014).
Figure 2. Schematic diagram of chemical synapse, that is composed of presynaptic membrane, synaptic cleft, and postsynaptic membrane.
The efficiency of information transmission between anterior and posterior neurons is defined as synaptic weight (synaptic strength), and the numerous mechanisms in changing the synaptic weight are collectively called synaptic plasticity (Martin et al., 2000; McGaugh, 2000; Mayford et al., 2012; Liao et al., 2014). Synaptic plasticity is grouped into STP (short-term plasticity) and LTP (long-term plasticity) by the retention time, and both of them have potentiation and depression states. The duration of STP occurs between milliseconds and minutes, which is related to the computational functions of neural network and short-term memory (STM) (Morris, 1999). PPF (paired-pulse facilitation), defined as 100% × A2/A1, where A1 and A2 are the amplitudes of the first and the second postsynaptic current corresponding to two consecutive spikes that divided by a time interval Δt, is a form of STP. PPF participates in neuronal tasks, such as simple learning and information processing (Regehr, 2012; Bornschein et al., 2013). LTP can produce plastic changes that last for a few hours even longer; LTP is related to learning and long-term memory (LTM) (Bear and Malenka, 1994; Linden, 1994; Kullmann and Lamsa, 2007; Ho et al., 2011). Hebb hypothesized that continuous and repeated stimulation from presynaptic neurons to postsynaptic neurons could cause an increase in the efficiency of synaptic transmission (Morris, 1999). The concept of STDP (spike-timing-dependent plasticity) further improves Hebb’s theory, pointing out that the time relationship between presynaptic and postsynaptic spikes can modulate the synaptic weight (Bi and Poo, 1998; Dan and Poo, 2006; Caporale and Dan, 2008). SRDP (frequency-dependent-synaptic plasticity) is another basic learning mechanism for LTP in the brain, i.e., synaptic weight can be modulated by controlling the frequency of presynaptic spikes (Bliss and Lomo, 1973; Bear et al., 1987; Dudek and Bear, 1992; Law and Cooper, 1994). For instance, high-frequency (20–100 Hz) trains of presynaptic spikes will generate LTP, whereas low-frequency (1–5 Hz) trains result in LTD (Bear and Malenka, 1994).
The development of “brain-like” computing is inseparable from the exploration of brain functions by neurologists. Synapses serve as functional connections between neurons, thence synaptic devices are essential for the emulation of the neural functions mentioned above. In recent years, circuits based on lots of silicon transistors have been explored to mimic synaptic functions, proving its possibility in the application of neuromorphic engineering (Ramakrishnan et al., 2011; Bamford et al., 2012). In order to reduce hardware cost and power consumption, in this review, we focus on the realization new-concept neuromorphic devices for bionic sensing and perception applications.
Neuromorphic Devices Based on Various Materials and Mechanisms
Numerous materials (e.g., electrochemical metallization materials, phase-change materials, ferroelectric materials, ionic/electronic hybrid materials) have been employed to fabricate artificial synapses for constructing neuromorphic network. To mimic bio-synaptic functions, diverse configurations of synaptic devices have been proposed, including: two-terminal (2-T) devices and three-terminal (3-T) devices. 2-T devices have the advantage of small physical size and easy large-scale integration (Jo et al., 2010; Prezioso et al., 2015; Xu et al., 2016a; Lee et al., 2019). 3-T devices can perform signal transmission and self-learning functions simultaneously (Yuan et al., 2010; Wu et al., 2014; Wan et al., 2015; Kim et al., 2016, 2017; Zhu et al., 2016; Gkoupidenis et al., 2017; Dai et al., 2018; Jerry et al., 2018; He Y. et al., 2020). Multi-terminal synaptic devices with multiple presynaptic terminals can be adopted to emulate information processing (Liu Y.H. et al., 2015; Feng et al., 2017; Jiang et al., 2017). In the section, the recent progresses of the synaptic devices will be introduced. More detailed information will be shown in Tables 1, 2.
Electrochemical Metallization Materials
Electrochemical metallization (ECM) memory composed of top electrode/active layer/bottom electrode sandwiched structure is an important resistive switching memory. ECM memory shows the resistive switching based on the formation/rupture of metallic filament, which generates from the oxidation of active electrode (e.g., Ag, Cu), transport of metal cations through active layer, and reduction at noble metal electrode. The filament dissipates may due to spontaneous diffusion, Joule heating or ionization. Diverse electrochemical metallization materials have been used to fabricate ECM memory, including chalcogenide (Hasegawa et al., 2010; Ohno et al., 2011; Zhang et al., 2013), nitride (Yang et al., 2012), amorphous silicon (Zhang et al., 2017), and polymer (Li et al., 2013; Kim and Lee, 2018).
In 2011, an inorganic synapse with the Pt/Ag2S/Ag structure was fabricated to emulate the synaptic functions of STP and LTP, see Figure 3A (Ohno et al., 2011). In such synaptic device, the temporal enhancement of conductance occurred before the entire formation of a metallic bridge, and the reduction of the conductance is due to the deformation of instable metallic bridge (Figure 3B). When a robust metallic bridge was formed, a non-volatile conductance enhancement can be obtained, which corresponds to LTP (Figure 3C). In 2017, an ECM memory with Cu/ZnS/Pt structure was fabricated for artificial synapse application, and STP and LTP functions were successfully emulated (Hu et al., 2017). In 2018, single-crystalline SiGe epitaxial random-access memory (epiRAM) exhibited superior spatial/temporal uniformity, and linear weight update based on the confinement of conductive filaments (Ag) into dislocations in SiGe was also observed (Choi et al., 2018).
Figure 3. (A) Schematic diagram of Ag2S inorganic synapse and the formation mechanism for STP and LTP. Right side: The signal transmission of biological synapse. (B,C) STP and LTP characteristics of the Ag2S inorganic synapse when input pulses were applied with the intervals of 20 and 2 s (adapted from Ohno et al., 2011).
Phase-Change Materials
Phase-change materials have been widely explored for memory application (PCM: phase-change memory) because of its scalability, controllable multi-level resistance states and fast read/write speed (Ovshinsky, 1968; Lankhorst et al., 2005; Bichler et al., 2012; Suri et al., 2012; Ambrogio et al., 2016, 2018; Boybat et al., 2018). PCM can be switched from amorphous phase [i.e., high-resistance state (HRS)] to crystalline phase [i.e., low-resistance state (LRS)] by Joule heat (Burr et al., 2016). The application of SET voltage on the PCM causes Joule heating, subsequently raises the material temperature to crystal transition temperature but below melting temperature. As for the RESET operation, material temperature is raised above the melting temperature and then quickly quenched to room temperature; the material solidifies into amorphous phase. By precisely controlling the transition process between amorphous and crystalline states, multi-level intermediate states can be generated to emulate biological synapses (Ielmini et al., 2004; Nakayama et al., 2007; Nirschl et al., 2007). Chalcogenide glass such as Ge2Sb2Te5 (GST) (Ambrogio et al., 2016) and GeTe (Bichler et al., 2012) are commonly applied in phase change memory.
Nanoscale electronic synapses based on GST active layers were fabricated (Figure 4A; Kuzum et al., 2012). Different from biological action potentials, the pre-spike was composed of potentiation (set) pulses with decreasing amplitude and depression (reset) pulses with increasing amplitudes; the post-spike was a continuous pulse with 120 ms duration and with a low negative amplitude pulse of 8 ms in the center. The difference between the pre- and post-spike (Vpre − Vpost) decided the programming voltage applied on the synaptic device at each point. By controlling the time interval in the −50 to 50 ms range, the STDP curve was obtained, which matched with the data measured by Bi and Poo (1998). In addition, the time constant of STDP could be changed by adjusting the amplitude and time spacing of the pulses in the pre-spike. Various STDP characteristics were also demonstrated via swapping the order of depression and potentiation pulses in the pre-spike (Figure 4B). All the synaptic functions displayed by the PCM synapse benefitted from the consecutive transition between intermediate resistance states. Such nanoscale device showed picojoule level energy consumption, making a significant step toward achieving the compactness and energy efficiency traits of brain for future neuromorphic system.
Figure 4. (A) Schematic diagram of the crossbar array architecture of the PCM synapses. (B) Different forms of STDP learning rules (adapted from Kuzum et al., 2012).
Ferroelectric Materials
Ferroelectric materials have the properties of high dielectric constant and spontaneous polarization (Chanthbouala et al., 2012; Boyn et al., 2017; Shin et al., 2017; Tu et al., 2018). The polarization states of the ferroelectric materials can be modulated by the applied voltage, so these materials can be used as the active layer in synaptic devices. What’s more, a certain pulse sequence causes the fine polarization states of the ferroelectric material, so multiple conductance states can be obtained in these synaptic devices. The multilevel changes of channel conductance will meet the emulation of various synapse functions. Ferroelectric materials could help synaptic devices improve ON/OFF ratio and linearity of weight updates (Kim and Lee, 2019).
An inorganic memristor based on ferroelectric tunnel junctions was constructed to harness the STDP (Boyn et al., 2017). The super-tetragonal BiFeO3 (BFO) active layer was sandwiched between Co top and (Ca,Ce)MnO3 (CCMO) bottom electrodes, composing the ferroelectric artificial synapse (Figure 5A). As sketched in Figure 5B, well-defined voltage thresholds were shown in the hysteresis loop due to the inherent inhomogeneous polarization switching in the BFO. That made it possible for implementing STDP. By applying various voltage waveforms on the artificial synaptic device, various types of activities between the pre- and post-neuron were realized (Figure 5C).
Figure 5. (A) Schematic diagram of the ferroelectric memristor. (B) The single pulse hysteresis loop of the memristor shows clear voltage thresholds. (C) STDP learning curves of different shapes (adapted from Boyn et al., 2017).
Transistor with ferroelectric material as the gate insulator could be applied as a 3-T memristor device (Yoon et al., 2011; Nishitani et al., 2013). An organic synaptic transistor with ferroelectric poly (vinylidene fluoride/trifluoro ethylene) [P(VDF-TrFE)] was fabricated to mimic synaptic functions (Figure 6A; Tian et al., 2019). The conductance of the device could be modulated alternately between decrement and increment by adjusting the polarity of applied voltages. Thus, the potentiation and depression of synaptic weight could be realized in the device (Figure 6B). STDP was demonstrated by designing the waveforms. The combined waveform temporarily exceeded the threshold voltage, engendering the strengthening (△G > 0) or weakening (△G < 0), depending on the time interval between the pre- and postsynaptic signals (Figure 6C). As shown in Figure 6D, after 107cycles of stimulation of high voltage pulse (± 20 V, 1 ms), the channel conductance could still be modulated to the same highest/lowest states under similar positive voltage and a little increased negative voltage. That organic ferroelectric synaptic transistor has relatively good endurance properties.
Figure 6. (A) Schematic diagram of the organic ferroelectric synaptic device. (B) Change of the channel conductance with the different voltage pulse sequences. (C) Measurement of STDP in the transistor. (D) Change of the channel conductance with various gate voltage pulse amplitude after 107 cycles of total polarization switching (adapted from Tian et al., 2019).
Other ferroelectric materials are also utilized as the gate insulator in synaptic devices. For example, Kaneko et al. (2014) used inorganic Pb(Zr,Ti)O3 (PZT) ferroelectric film to construct synaptic device for realizing STDP function. Although PZT based ferroelectric transistor exhibits great plasticity in emulating synapses, their inherent Pb content will inevitably bring harm to human beings and environment. HfO2 is another feasible candidate for non-volatile memory because of its ferroelectricity and anti-ferroelectricity (Boescke et al., 2011; Park et al., 2015). Recently, ferroelectric material HfZrOx was employed in a synaptic transistor, the ferroelectric transistor exhibited excellent plasticity potentiation and depression (Kim and Lee, 2019).
Ionic/Electronic Hybrid Materials
Ionic/electronic hybrid materials are utilized in field-effect transistors (FETs). Gate dielectric (electrolyte) and channel materials constitute the ionic/electronic hybrid materials. Gate electrolytes have been acted as by diverse materials, such as polyelectrolytes (Yu et al., 2018; He et al., 2019), ion gel (Qian et al., 2016; Xu et al., 2016b), ion liquid (Yang et al., 2017; Yang J.T. et al., 2018), and inorganic oxide (Wan et al., 2013, 2016a). Channel materials can be served as by both inorganic and organic materials, such as IZO (Wan et al., 2016a), IGZO (Zhou et al., 2015), and MoO3 (Yang et al., 2017); carbon nanotubes (CNTs) (Kim et al., 2013; Feng et al., 2017); graphene (Tian et al., 2015; Sharbati et al., 2018), MoS2 (Jiang et al., 2017; John et al., 2018), and PEDOT:PSS (Gkoupidenis et al., 2015, 2017; van de Burgt et al., 2017). For synaptic FETs, gate electrolytes have good ionic conductivity, in which ions can move randomly, but electrons are not allowed. Synaptic FETs with such gate electrolytes can form electric-double-layer (EDL) at the interface of the channel layer and gate electrolyte. The EDL has a large capacitance value (∼μFcm–2 magnitude), so the conductance of the channel layer can be modulated by a small gate voltage, indicating that the FETs could work at a low voltage.
In 2013, a carbon nanotube (CNT) synaptic transistor with poly (ethylene glycol) monomethyl ether (PEG) gate dielectric was proposed (Figure 7A; Kim et al., 2013). In the initial state, the hydrogen ions in the polymer were randomly distributed. When a positive voltage pulse was applied on the gate, the hydrogen ions began to move toward the CNTs channel, and an EDL was formed due to the electrostatic coupling effect, causing the channel current increased (Figure 7B). The transistor successfully emulated typical synaptic function PPF (Figure 7C). Other typical synaptic characteristics such as LTP and LTD were also demonstrated (Figure 7D). The CNT synapse had the potential that was integrated in large-scale circuit to emulate the parallel signal processing and learning features of biological neural network.
Figure 7. (A) The schematic diagram of a carbon nanotube (CNT) synapse, which shows the transistor-like structure of the CNT synapse with a cell containing hydrogen ions in the electrolyte integrated in its gate. Inset is the AFM of a random CNT network. (B) EPSC triggered by the pre-synaptic spikes. (C) EPSCs triggered by a pair of pre-synaptic spikes. (D) The changes of EPSC amplitudes in the synaptic device with Δtpre and Δtpost under the LTP and LTD imitations. Insets illustrate the CNT hydrogenation after the LTD imitation (bottom, left), the dehydrogenation after the LTP imitation (top), and no remarkable change after the LTP or LTD imitations (bottom, right) (adapted from Kim et al., 2013).
Wan group invented oxide-based electronic/protonic hybrid transistors with in-plane gate configuration. As shown in Figure 8A, an indium-zinc-oxide (IZO) based electronic/protonic hybrid transistor was self-assembled on phosphorus (P)-doped nanogranular SiO2 proton conductive films (Zhu et al., 2014). No bottom conductive layer was needed, and the gate voltage could be directly coupled to the IZO channel laterally through only one lateral EDL capacitor. When the in-plane gate was utilized as the presynaptic terminal and the IZO channel with S/D electrodes was acted as the postsynaptic terminal, an artificial synaptic transistor was proposed. The device was employed to imitate a series of short-term plasticity behaviors, including PPF, high-pass filtering behavior and the spatiotemporal correlation dynamic logic (Figures 8B–D). In addition, the laterally coupled synaptic transistor can be easily extended to multiple input gates to realize the function of synaptic interaction. The laterally coupled IZO transistor based on proton conducting electrolyte is of great significance to synaptic electronics and neuromorphic engineering.
Figure 8. (A) Illustration of a laterally coupled IZO synaptic device with two in-plane gates. (B) PPF behavior of the IZO synaptic transistor. (C) EPSCs triggered by the stimulus trains with different frequencies. (D) Dynamic logic testing of the IZO synaptic transistor (adapted from Zhu et al., 2014).
Recently, Wan group demonstrated a multiterminal IGZO-based neuro-transistor for dendritic discrimination of different spatiotemporal input modes (Figure 9A; He et al., 2019). Chitosan electrolyte was used as the gate dielectric. The IGZO channel layer, multiple in-plane ITO gate, and ITO source/drain electrodes were deposited by different metal shadow masks. In such neuro-transistor, the synaptic weight can be tuned by the modulatory gate due to the strong lateral electric-double-layer capacitive coupling effect in the electrolyte film. PPF and EPSC behaviors were successfully mimicked in the multiterminal synaptic transistor (Figures 9B,C). In the nervous system, STP contributes to temporal filtering by facilitating or inhibiting the synaptic transmission. Since a larger PPF ratio was obtained with shorter time interval, high-pass temporal filtering could be realized in the transistor (Figure 9D). Various temporal and spatial input patterns of dendrite recognition were also achieved in such multi-terminal neuro-transistor. This kind neuro-transistor can be used as the temporal and spatial information processing unit of basic cortex computing, greatly improving the efficiency of artificial neural network.
Figure 9. (A) Schematic diagram of the multiterminal artificial synaptic device. (B) EPSCs triggered by G1 with different Gm. (C) PPF ratio plotted as the function of time interval between a pair of pulses under different Gm. Inset: EPSCs triggered by a pair of pulses with time interval of 50 ms when there is no Gm bias. (D) EPSCs triggered by spike trains containing 10 spikes with different frequencies when there is no Gm bias. Inset: EPSC amplitude gain (A10/A1) changes with presynaptic spike frequency under different Gm (adapted from He et al., 2019).
Sensory Applications of Neuromorphic Devices
With the improved understanding of biological sensing process and the development of neuromorphic devices, the application of neuromorphic devices in bionic sensing and perception comes naturally. In the section, we will first introduce synaptic devices that can sense external stimuli: light (Li et al., 2016; Lee et al., 2017; Qian et al., 2018; Wang et al., 2018c,d; Ahmed et al., 2019), sound (He et al., 2019), chemicals (Giordani et al., 2017; Song et al., 2019), and PH (Liu N. et al., 2015; Liu et al., 2019). Such devices can convert the external stimuli to the electrical signals, which can play a monitoring role for human to avoid being hurt. Then the incorporation of synaptic and sensing devices is displayed. Finally, the artificial sensory neuron systems are shown.
Synaptic Devices With Sensing Capabilities
The employ of light-sensitive materials in neuromorphic devices is favorable for artificial sensory neuron, because photonic synapses have the merits of large bandwidths and no electrical energy loss at interconnections (Sun et al., 2018; Dai et al., 2019; Wang et al., 2019). Yang Y. et al. (2018) proposed an IGZO-based synaptic transistor in series with a 10 MΩ resistor to realize photo-sensing application (Figure 10A). The light pulse, the output potential (VOUT) and conductance of the channel were regarded as input, post-synaptic potential (PSP) and synaptic weight, respectively. When incident light illuminated the IGZO channel layer, the channel conductance was reduced, and photocurrent could be generated. Two successive light spikes (405 nm, 232 mW cm–2, 20 ms) were applied on the channel, PPF characteristic was mimicked (Figure 10B). The PPF index gradually decreased with the increasing inter-spike interval (Figure 10C). Figure 10D displayed EPSP triggered by light pulse could be modulated by gate voltage. Besides, depression to potentiation mode transition was also displayed by gate voltage modulation.
Figure 10. (A) Schematic diagram of the photonic neuromorphic transistor loaded with a resistor. (B) PPF realized in the synaptic transistor with light input pulses. (C) PPF index decreases with increased ΔT under various VG. (D) EPSPs triggered by a series of 50 light pulses under different VG (adapted from Yang Y. et al., 2018).
Except for artificial synaptic functions, biological behaviors at sensory receptors are highly demanded on synaptic devices. A synaptic phototransistor based on the hybrid structure of transition-metal dichalcogenide (TMD) and mixed halide perovskite [CsPb(Br0.5I0.5)3] emulated the human sensory adaptation to constant light (Figure 11A; Hong et al., 2020). The lessening in the sensitivity of sensory system toward a constant stimulus over time was called sensory adaptation. The combination of TMDs and perovskite overcame the weak light absorption of TMDs, because the photoexcited charges transferred from the perovskite to the MoS2 channel via the differences in band edge. As time went by, the photocurrent of the synaptic device under red light illumination degraded drastically within 3 min (Figure 11B). The phenomenon indicated the device could be applied for sensory-adaptation; the time-resolved photo-response of the device under continuous red-light illumination (Figure 11C) confirmed this. The synaptic device could also mimic the reversibility behavior of sensory-adaptation (Figure 11D), even though the recovery rate dropped slightly as the sequence repeated. The photosensory adaptation behavior of the device with selective light can be applied to intelligent sensors, and biomedical imaging.
Figure 11. (A) Phototransistor under illumination of blue, green, and red light. (B) Variation trend of photocurrent in the phototransistor under RGB light illumination time. (C) Distinction of the photocurrents in the phototransistor under constant red light illumination with respect to time in four measurement. (D) Photosensitivity of the device during emulating sensory adaptation (adapted from Hong et al., 2020).
The sound location function of human brain was mimicked by artificial neural network based on a multi-terminal IGZO neuromorphic transistor (He et al., 2019). The schematic diagram of locating sound was shown in the Figure 12A. Sound azimuth detecting function was realized by a neural system that was consisted of two gate electrodes (PREN1 and PREN2) and two pairs of S/D terminals (POSTN1 and POSTN2). PREN1 and PREN2 were regarded as the left and right ears, respectively, and were fully connected to POSTN1 and POSTN2 (Figure 12B). The connection strength between PREN and two POSTNs were diagonal, implying that one POSTN processed spikes transmitted by the synapses in a strong/weak order while the other processed information in the opposite sequence. When the sound was from the right direction, POSTN1 first processed the signal transmitted by a weak synapse and then processed the signal transmitted by a strong synapse. While POSTN2 processed information in the opposite. Consequently, the amplitude of IPOST1 was larger than that IPOST2 (Figure 12C). The ratio of the amplitude of IPOST2/IPOST1 as the function of (tPREN2 − tPREN1) and the sound azimuth was shown in Figure 12D. This time-dependent recognition shows the potential that the artificial neural network can detect the sound azimuth.
Figure 12. (A) Schematic diagram of sound location by binaural effect in human brain. (B) Sound location in artificial neural network based on the transistor. (C) Postsynaptic currents of POSTN2 and POSTN1 when sound comes from right direction. (D) IPOST2/IPOST1 changes with time interval and sound azimuth (adapted from He et al., 2019).
An organic transistor which had the function of detecting hazardous gas (NO2) leakage paved the way of human health monitoring (Song et al., 2019). As depicted in the Figure 13A, human organs would be damaged under the influence of toxic gas. A large number of studies have shown that prolonged exposure to toxic gas environments could have varying degrees of health effects: respiratory diseases and even lung cancer (Ezratty et al., 2014; Hettfleisch et al., 2017; Mentz et al., 2018). The flexible toxic gas detection device was fabricated with PVA dielectric, PCDTPT channel, gold back-gate and source/drain electrodes (Figure 13B). Hazardous gas acted as the input pulse, PCDTPT channel layer was used as the gas sensing and storage layer. NO2 molecules had the property of withdrawing electron. When there was 20 ppm NO2, the captured NO2 remained on the surface of the channel, acting as electron trapping centers, contributed to the increase of holes in the channel, and resulted in the mounting of Ids. After removing the pulse for 600 s, Ids had a greatly slow decay process, and did not restore to the original value (Figure 13C). That was the reason of the absence of external energy such as thermal/photo energy at room temperature. The PPF was demonstrated in Figure 13D. The functions implemented by the device provide great potential for human health monitoring and non-invasive diagnosis.
Figure 13. (A) Schematic image that shows different injuries of hazardous gas on human and organs and olfactory. (B) Schematic of the operation concept of the artificial organ-damage device. (C) Typical response/recovery characteristics of the device to 20 ppm NO2. (D) Real-time IDS to two successive 20 ppm NO2 pulses at time interval 1,000 and 300 s, respectively, and the PPF index as the function of pulse interval (adapted from Song et al., 2019).
As shown in Figure 14A, a pH-sensing IZO-based synaptic transistor with multiple gate electrode was demonstrated. An Ag/AgCl reference electrode immersed into a pH buffer solution droplet acted as the sensing gate (G1). In-plane Al gate electrodes were used as control gates (Liu N. et al., 2015). The IZO channel could be efficiently tuned by the sensing and control gates, because of the electric field that was coupled by sensing and control gates. As the pH increased, the magnitude of EPSC decreased (Figure 14B). Since the hydrogen ions in the solution would generate a charge repulsion reaction with the protons at the electrolyte interface, and more protons accumulated in the area below the channel, the EPSC was relatively increased. It could be inferred that an appropriate negative bias applied on the sensing gate would increase the sensitivity of the device (Figure 14C) and lessen the energy dissipation (Figure 14D).
Figure 14. (A) Schematic of the pH-sensing IZO-based synaptic transistor. (B) The change of current with pH value. (C) The change of sensitivity with VG1 bias (pH = 10). (D) The change of energy dissipation with VG1 bias (pH = 10) (adapted from Liu N. et al., 2015).
Artificial Synapses Combined With Sensors
The achievable functions of sensory synaptic devices under limited material selection are relatively simple and cannot show diverse synaptic characteristics. Hence, higher level of device structures needs to be designed to make up for this shortcoming (Chen et al., 2018; Seo et al., 2018; Wang et al., 2018a). By integrating with various sensors, the external stimuli can be utilized as the inputs of synaptic devices to realize the emulation of more complex biological functions. The combination of the two parts promotes the development of neuromorphic engineering in the direction of sensory applications.
Human visual system is essential for the knowledge acquisition, which via eyes to sense light and brain to storage image information. Herein, structure of the device that integrated image sensor and memory to emulate visual memory was shown in the Figure 15A (Chen et al., 2018). In2O3 was chosen for the functional material to detect UV light, for it was light-sensitive; Al2O3 was exploited as the memory material on account of the excellent bipolar resistive switching feature. When In2O3 was irradiated with UV light, the charge carrier concentration in In2O3 increased. So, resistance state of the image sensor was transformed from high resistance to low resistance, due to the connection with the image sensor, the resistance switching state of the memory from OFF to ON. Even after the UV was removed, the state of the memory remained until the application of the reset potential, implying that the lighting information was stored in the memory. Visual memory arrays composed of 10 × 10 pixels were fabricated to exhibit imaging and memorizing a butterfly-like pattern (Figure 15B), each pixel was formed by image sensor and memory to compose a visual unit. Only the pixels exposed to the patterned UV light worked normally, and ultimately form the targeted pattern which could retain for 1 week (Figure 15C).
Figure 15. (A) Schematic diagram of the bio-inspired visual memory unit integrated by resistive switching memory device and image sensor. (B) Schematic diagram of detecting and memorizing the light distribution which generated from patterned diffraction optical element (DOE). (C) Schematic of the resistance states between memory device and image sensor (adapted from Chen et al., 2018).
Wang and co-workers presented a light-triggered organic neuromorphic device (LOND) to emulate the retinal functionalities (Wang et al., 2018a). A flexible array was composed of 5 × 6 pixels then were curved into hemispheric surface to imitate the retinal functions. The NIR and green light with the identical frequency (64 Hz) and intensity (10.80 mW cm–2) were shed on the array. In contrast, green light evoked a higher current level, even after 1,800 s, still had 65% of original signals. As mentioned above, the LONDs could achieve the goal of wavelength-recognition, that was expressed by the degree of non-volatility.
Tactile sense is indispensable for normal human activities. It has the functions of protecting the human body from injury and diagnosing diseases. In recent years, there have been an amount of studies on emulating haptic function. Yet the single function imitations of synaptic devices lack the functional memory of tactile, such devices are awkward when reacting to the same motion (Tabot et al., 2013; Foley, 2016). Therefore, the development of tactile-sensing system is of great significance for prosthetics and robotics (Zang et al., 2017; Kim et al., 2018; Zhang C. et al., 2019; Zhang et al., 2020).
In 2016, Zang et al. (2017) demonstrated a dual-organic-transistor (DOT) based tactile perception element (TPE) to achieve the goal that dynamic signal transduction and information processing work in a device. A suspended-gate organic field-effect transistor was employed as the pressure sensing element, and integrated with a synaptic device, forming a prototype DOT-TPE (Figure 16A). The equivalent electrical circuit of the DOT-TPE was exhibited in Figure 16B. When there was an external pressure on the sensor, causing a change in capacitance of the dielectric. Consequently, the conductivity of the sensor was tuned, resulting in the transport of presynaptic spike to the synaptic transistor. Tactile information was collected by monitoring the EPSC of synaptic transistor. A 3 × 3 pixels DOT-TPE array was constructed to emulated the perception of dynamic mechanical pressure, and four bias cycles of retentive pressure at mounting frequencies were applied on pixel 1–9 (Figure 16C). Figure 16D showed a falling EPSC of the first press action (A1) from pixel 1–9, because the increased frequency made the contact time shorter. To the opposite, the gain A4/A1 of every pixel grew from 1.2 to 1.8, indicating the high-pass temporal filtering feature of the tactile-perception system.
Figure 16. (A) Schematic illustration of the DOT-TPS. (B) Equivalent electrical circuit of the DOT-TPS. (C) Four continuous and repeated touch cycles applied to the nine pixel. (D) The EPSC (A1) and the gain A4/A1 for each pixel (adapted from Zang et al., 2017).
The movement of human limbs benefits from the movement of muscles contracting and pulling bones to produce joints, and also requires the adjustment of the nervous system (Graziano, 2006; Urgesi et al., 2006; Stefan et al., 2008). Integrating motion sensor and memory had great significance for robotics and health monitoring systems (Figure 17A; Liu et al., 2017). A hybrid substrate that was spatially separated into different mechanical properties was introduced. Therefore, both fragile memory device and flexible sensor could be combined as a uniform unit (Figure 17B). The memory was based on ZIF-8, and gold film with microcrack morphology/Ag worked as the B/T electrode. It was worth noting that gold film with microcrack morphology had a good ductility under stretching (Lacour et al., 2003; Graudejus et al., 2012; Liu et al., 2014). The I-V characteristic curves of the memory showed typical resistance switching property, which implied its non-volatile feature (Figure 17C). For the purpose of monitoring and storing the information of the elbow telescopic state, a simple circuit was built as shown in Figure 17D. The strain sensor and memory device were fabricated on the mechanical hybrid substrate, and the LED connected with the memory was adopted to observe the state of HRS and LRS. The circuit chip was attached onto the arm near the elbow. When elbow was in the extension state, the telescopic state of the sensor had not changed, i.e., the conductance remained original, so the memory showed HRS and the LED was dark. Correspondingly, the flexing of elbow caused the elongation of the sensor, which switched the memory to the “on” state, and lighted the LED until a reset voltage was applied.
Figure 17. (A) Explanation of the biological concept of motions (left) and the corresponding bionic motion memory device (right). (B) Schematic diagram of the specific structure of the device. (C) I–V curve of the Ag/ZIF-8/Au device (insert: structure of the device). (D) The equivalent electrical circuit of the motion memory system (left), and the detecting and storing information function of the system on elbow flexion (right) (adapted from Liu et al., 2017).
Integration for Constructing Artificial Neural Systems
The previous section introduced the combination of sensors and synaptic devices to achieve more complex functionalities. Nevertheless, the postsynaptic signals of the synaptic devices have not been employed to display practical functions such as motor behavior, distinguishing and identifying tasks. This section will introduce artificial neurons that are constructed by sensors, synaptic devices and proper electric elements. Such artificial neurons can utilize their postsynaptic signals to achieve some sophisticated bionics functions. The artificial neural systems play the key role in the field of artificial intelligence to mimic the “cognitive” function of human (Langley, 2011; Jordan and Mitchell, 2015; Zhang C. et al., 2019).
A neuromorphic tactile processing (NeuTap) system composed of resistive pressure sensor, ductile ionic cable and synaptic transistor was exerted to mimic the sensory neuron (Figures 18A,B; Wan et al., 2018). The applied voltage on VDD generated a voltage drop on PVA wires/pressure sensor/semiconducting channel. Once pressure was applied to the sensor, the resistance decreased rapidly to produce a voltage drop via the PVA wires, that was equivalent to applying a voltage on the PVA wires. The voltage created an EDL at the IWO/PVA interface, tuning the IWO channel conductance. A NeuTap with two sensing terminals was fabricated to mimic the integrated functions for spatiotemporal correlated sensory stimulation. As a proof-of-concept, tactile pattern recognition was completed via one sensing terminal in the NeuTap neuron, the neuron was attached to a finger for the experiment. Two patterns in a row were used for recognition; the convex pattern was marked as “1” and the flat patterns was as “0,” so that each set of patterns could be labeled as “00,” “01,” “10,” and “11” in the form of binary code (Figure 18C). The typical current responses of the NeuTap with three various pattern pairs were depicted in Figure 18D. Supervised learning method was employed in NeuTap to imitate the perceptual learning process. The change in channel conductance was defined as the recognition index (RI) (Figure 18E). RI data and their corresponding labels were employed as the training data, which were imported into the computer program to partition the boundaries for each pattern. The unlabeled RI data were inputted into the computer, then the computer compared the values with “learned” boundaries to infer the labels of the patterns. The 44% error rate could be decreased to 0.4% after six learning times, that resembled the perceptual learning process.
Figure 18. (A) Sensory neuron compared to the NeuTap. (B) Schematic of the details of the NeuTap. (C) Digital image of the NeuTap on one finger and the pattern pairs as well as the corresponding two-bit binary code labels. (D) The responses of the NeuTap to three pattern pairs. (E) The machine learning method for the perceptual learning emulation (adapted from Wan et al., 2018).
An optoelectronic spiking sensory neuron system with pressure sensing, perceptual learning and memory ability has been reported recently (Tan et al., 2020). The system was operated by MXene-based flexible receptors, analogy to E-skin, to detect the external pressure and convert it to voltage signal. Subsequently, the signal was transmitted to the (analog-to-digital) ADC&LED section, and finally integrated into the synaptic photo-memristors in the form of optical spikes (Figures 19A,B). The reason of the receptors and the synaptic photo-memristors were connected in the form of optical was that spike coding was more robust than voltage coding (Burke and Ivory, 2008; Kim et al., 2018). A 5 × 5 sensors array was connected with an ADC-LED and a synaptic photo-memristor in order to recognize handwriting through training (Figure 19C). To simplify the handling of information, instead of processing the 25 data streams, the spiking proportions(P), defined as P = tspiking/twriting, of the five synaptic photo-memristors was extracted as a five-dimensional (5D) feature for the recognition and learning processes. The PSCs of the five photo-memristors corresponding to the input of the alphabet (Figure 19D). The recognition accuracy was improved from ∼58% after the first training cycle to 84% after 10 training cycles. The successful implementations of the functions in the above work provide great examples of brain-like learning and promote the development of artificial intelligence.
Figure 19. (A) The biological afferent nerve. (B) The corresponding artificial afferent nerve. (C) Schematic of handwriting recognition with trait extraction and learning. (D) structure and working principle of the artificial neural network (adapted from Tan et al., 2020).
An artificial afferent nerve based on flexible organic electronics was demonstrated and used to emulate the function of slowly adapting type I (SA-I) sensory neurons (Pruszynski and Johansson, 2014; Kim et al., 2018). The artificial afferent nerve achieved the imitation of biological afferent nerves by the components of resistive pressure sensors/organic ring oscillators/a synaptic transistor corresponding to the receptor, nerve fiber, biological synapse, respectively. The pressure sensors were connected to a ring oscillator to convert external tactile stimulation into voltage pulses, then the electrical signals were integrated and transformed to the synaptic transistor by multiple electrodes. Ultimately, by the process above, the pressure stimuli were output in the form of postsynaptic currents. The highlight of this work was that a discoid cockroach was connected with the artificial afferent nerve to constitute a monosynaptic reflex arc (Figure 20A). The applied pressure information was collected, converted by the artificial afferent nerve, and finally outputted to a detached cockroach leg in the form of post-synaptic current. The post-synaptic current would actuate the tibial extensor muscle of cockroach leg (Figure 20B). The successful application of the artificial afferent nerve on the legs of cockroaches is of great significance for prosthetics and neurorobotics, and sets a solid foundation for the construction of neural networks.
Figure 20. (A) Schematic diagram of the hybrid reflex. (B) Force measured from the tibial extensor muscle when pressure is applied on the hybrid reflex arc (adapted from Kim et al., 2018).
Similarly, an artificial sensorimotor nervous system was constructed (Figure 21A; Lee et al., 2018). In the system, photodetector converted optical signals to voltage spikes that were applied to a synaptic transistor as the presynaptic input signals to trigger EPSCs, and a polymer actuator was connected with the above synaptic transistor via a transimpedance circuit; the polymer actuator was controlled by the EPSCs of the synaptic transistor (Figure 21C). Therefore, the artificial nervous system could achieve biomimetic natural motion. The electrical characteristics of the stretchable synaptic transistor under 0 and 100% strains were almost the same (Figure 21B), indicating the transistor was stable even under strain. The sensorimotor synaptic system would promote the development of next-generation bioinspired soft electronics, neural prostheses, and neurologically inspired robotics.
Figure 21. (A) The structure diagram of artificial sensorimotor nervous system. (B) SDDP from 120 to 960 ms under 0 and 100% strains. (C) Digital images of polymer actuator controlled by various spikes with 0 or 100% strain (adapted from Lee et al., 2018).
Summary and Perspectives
In this review, we have introduced various neuromorphic devices based on various materials, such as electrochemical metallized materials, phase-change materials, ferroelectric materials and ionic/electronic hybrid materials. 2-terminal devices have the merits of simple structure, small physical size, and easily to be integrated on a large scale. three-terminal (3-T) devices have the merits of relatively controllable test parameters, clear operating mechanism. Through appropriate material optimization and structural design, 3-T neuromorphic transistors can convert external stimuli (light, pressure, PH, etc.) into electrical signals efficiently. Multi-terminal neuromorphic transistors can spatiotemporally integrate input signals from multi-presynaptic terminals and facilitate synergistical sensing and perception.
For mimicking the functions of neural perception, neuromorphic devices that can sense the external environment accurately (light, sound, chemical, PH) are essential. Afterward, in order to meet the sensing and learning capabilities of neural systems, the integration of sensory and neuromorphic devices is particularly necessary, by which can make the systems sense external stimulus and store the relevant information. Such systems finally can be employed in humanoid robotic applications. What’s more, the monosynaptic reflex arc assembled by sensory and motor neuron has the potential to replace damaged nerves, and being used as a tackle in neuroscience for studying sensory and motor neuron diseases.
The development of neuromorphic devices for bionic sensing and perception applications has greatly promoted the field of artificial intelligence. First of all, there are still limitations in the selection of materials that respond to external stimuli (PH, sound, chemical, touch). For instance, to monitor toxic chemical, the device must employ materials that react specifically with the target. Secondly, for the construction of the artificial neural systems, there is still huge research space for structural design and optimization. Take pressure sensory neuron as an example, which is composed of three parts: pressure receptor, axon, and synapse. Lots of efforts are needed in the connection between the receptor and the synapse, that is, the afferent nerve part: the conductivity, transmission efficiency and the mechanical flexibility of the connection material must be considered, and the impact of the interference generated by the bionic sensor on the performance of the neuromorphic device needs to be further minimized. The normal maintenance of mammals and even the human body is inseparable from complex physiological adjustments. Insufficient understanding of the mechanism of the biosensing systems is also a major challenge that limits the bionic sensing and perception application of neuromorphic devices. So more interdisciplinary cooperation is needed in the area of neuromorphic devices and bionic sensing and perception application.
Author Contributions
QW and MZ conceptualized the concept and wrote the manuscript. YH and CZ participated in writing the manuscript. All authors contributed to the article and approved the submitted version.
Funding
This work was supported by the National Key Research and Development Program of China under Grant 2019YFB2205400.
Conflict of Interest
The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.
References
Abraira, V. E., and Ginty, D. D. (2013). The sensory neurons of touch. Neuron 79, 618–639. doi: 10.1016/j.neuron.2013.07.051
Ahmed, T., Kuriakose, S., Mayes, E. L. H., Ramanathan, R., Bansal, V., Bhaskaran, M., et al. (2019). Optically stimulated artificial synapse based on layered black phosphorus. Small 15:1900966. doi: 10.1002/smll.201900966
Ambrogio, S., Ciocchini, N., Laudato, M., Milo, V., Pirovano, A., Fantini, P., et al. (2016). Unsupervised learning by spike timing dependent plasticity in phase change memory (PCM) synapses. Front. Neurosci. 10:56. doi: 10.3389/fnins.2016.00056
Ambrogio, S., Narayanan, P., Tsai, H. Y., Shelby, R. M., Boybat, I., di Nolfo, C., et al. (2018). Equivalent-accuracy accelerated neural-network training using analogue memory. Nature 558:60. doi: 10.1038/s41586-018-0180-5
Anderson, M. L. (2010). Neural reuse: a fundamental organizational principle of the brain. Behav. Brain Sci. 33:245. doi: 10.1017/s0140525x10000853
Bamford, S. A., Murray, A. F., and Willshaw, D. J. (2012). Spike-Timing-Dependent plasticity with weight dependence evoked from physical constraints. IEEE Trans. Biomed. Circ. Syst. 6, 385–398. doi: 10.1109/tbcas.2012.2184285
Bear, M. F., and Malenka, R. C. (1994). Synaptic plasticity: LTP and LTD. Curr. Opin. Neurobiol. 4, 389–399. doi: 10.1016/0959-4388(94)90101-5
Bear, M. F., Cooper, L. N., and Ebner, F. F. (1987). A physiological-basis for a theory of synapse modification. Science 237, 42–48. doi: 10.1126/science.3037696
Bi, G. Q., and Poo, M. M. (1998). Synaptic modifications in cultured hippocampal neurons: dependence on spike timing, synaptic strength, and postsynaptic cell type. J. Neurosci. 18, 10464–10472. doi: 10.1523/jneurosci.18-24-10464.1998
Bichler, O., Suri, M., Querlioz, D., Vuillaume, D., DeSalvo, B., and Gamrat, C. (2012). Visual Pattern Extraction Using Energy-Efficient “2-PCM Synapse” Neuromorphic Architecture. IEEE Trans. Electron Dev. 59, 2206–2214. doi: 10.1109/ted.2012.2197951
Bliss, T. V. P., and Lomo, T. (1973). Long-lasting potentiation of synaptic transmission in dentate area of anesthetized rabbit following stimulation of perforant path. J. Physiol. Lond. 232, 331–356. doi: 10.1113/jphysiol.1973.sp010273
Boescke, T. S., Muller, J., Brauhaus, D., Schroder, U., and Bottger, U. (2011). Ferroelectricity in hafnium oxide thin films. Appl. Phys. Lett. 99:102903. doi: 10.1063/1.3634052
Bornschein, G., Arendt, O., Hallermann, S., Brachtendorf, S., Eilers, J., and Schmidt, H. (2013). Paired-pulse facilitation at recurrent Purkinje neuron synapses is independent of calbindin and parvalbumin during high-frequency activation. J. Physiol. Lond. 591, 3355–3370. doi: 10.1113/jphysiol.2013.254128
Boybat, I., Le Gallo, M., Nandakumar, S. R., Moraitis, T., Parnell, T., Tuma, T., et al. (2018). Neuromorphic computing with multi-memristive synapses. Nat. Commun. 9:2514. doi: 10.1038/s41467-018-04933-y
Boyn, S., Grollier, J., Lecerf, G., Xu, B., Locatelli, N., Fusil, S., et al. (2017). Learning through ferroelectric domain dynamics in solid-state synapses. Nat. Commun. 8:14736. doi: 10.1038/ncomms14736
Burke, J. M., and Ivory, C. F. (2008). Characterization of voltage degradation in dynamic field gradient focusing. Electrophoresis 29, 1013–1025. doi: 10.1002/elps.200700447
Burr, G. W., Brightsky, M. J., Sebastian, A., Cheng, H. Y., Wu, J. Y., Kim, S., et al. (2016). Recent progress in phase-change memory technology. IEEE J. Emerg. Sel. Top. Circ. Syst. 6, 146–162. doi: 10.1109/jetcas.2016.2547718
Caporale, N., and Dan, Y. (2008). Spike timing-dependent plasticity: a Hebbian learning rule. Annu. Rev. Neurosci. 31, 25–46.
Chanthbouala, A., Garcia, V., Cherifi, R. O., Bouzehouane, K., Fusil, S., Moya, X., et al. (2012). A ferroelectric memristor. Nat. Mater. 11, 860–864. doi: 10.1038/nmat3415
Chen, S., Lou, Z., Chen, D., and Shen, G. (2018). An artificial flexible visual memory system based on an UV-Motivated memristor. Adv. Mater. 30:1705400. doi: 10.1002/adma.201705400
Choi, S., Tan, S. H., Li, Z. F., Kim, Y., Choi, C., Chen, P. Y., et al. (2018). SiGe epitaxial memory for neuromorphic computing with reproducible high performance based on engineered dislocations. Nat. Mater. 17, 335–340. doi: 10.1038/s41563-017-0001-5
Cohen, J. D., Perlstein, W. M., Braver, T. S., Nystrom, L. E., Noll, D. C., Jonides, J., et al. (1997). Temporal dynamics of brain activation during a working memory task. Nature 386, 604–608. doi: 10.1038/386604a0
Connors, B. W., and Long, M. A. (2004). Electrical synapses in the mammalian brain. Annu. Rev. Neurosci. 27, 393–418. doi: 10.1146/annurev.neuro.26.041002.131128
Dahiya, R. S., Metta, G., Valle, M., and Sandini, G. (2010). Tactile sensing-from humans to humanoids. IEEE Trans. Robot. 26, 1–20. doi: 10.1109/tro.2009.2033627
Dai, S., Wang, Y., Zhang, J., Zhao, Y., Xiao, F., Liu, D., et al. (2018). Wood-derived nanopaper dielectrics for organic synaptic transistors. ACS Appl. Mater. Interfaces 10, 39983–39991. doi: 10.1021/acsami.8b15063
Dai, S., Zhao, Y., Wang, Y., Zhang, J., Fang, L., Jin, S., et al. (2019). Recent advances in transistor-based artificial synapses. Adv. Funct. Mater. 29:1903700. doi: 10.1002/adfm.201903700
Dan, Y., and Poo, M. M. (2006). Spike timing-dependent plasticity: from synapse to perception. Physiol. Rev. 86, 1033–1048. doi: 10.1152/physrev.00030.2005
Dang, B., Wu, Q., Song, F., Sun, J., Yang, M., Ma, X., et al. (2018). A bio-inspired physically transient/biodegradable synapse for security neuromorphic computing based on memristors. Nanoscale 10, 20089–20095. doi: 10.1039/c8nr07442a
Delbruck, T., van Schaik, A., and Hasler, J. (2014). Research topic: neuromorphic engineering systems and applications. A snapshot of neuromorphic systems engineering. Front. Neurosci. 8:424. doi: 10.3389/fnins.2014.00424
Dudek, S. M., and Bear, M. F. (1992). Homosynaptic long-term depression in area Ca1 of hippocampus and effects of N-Methyl-D-Aspartate receptor blockade. Proc. Natl. Acad. Sci. U.S.A. 89, 4363–4367. doi: 10.1073/pnas.89.10.4363
Ezratty, V., Guillossou, G., Neukirch, C., Dehoux, M., Koscielny, S., Bonay, M., et al. (2014). Repeated nitrogen dioxide exposures and eosinophilic airway inflammation in asthmatics: a randomized crossover study. Environ. Health Perspect. 122, 850–855. doi: 10.1289/ehp.1307240
Feng, P., Xu, W. W., Yang, Y., Wan, X., Shi, Y., Wan, Q., et al. (2017). Printed neuromorphic devices based on printed carbon nanotube thin-film transistors. Adv. Funct. Mater. 27:1604447. doi: 10.1002/adfm.201604447
Ferster, D., and Jagadeesh, B. (1992). EPSP-IPSP interactions in cat visual-cortex studied with invivo whole-cell patch recording. J. Neurosci. 12, 1262–1274.
Field, D. J. (1994). What is the goal of sensory coding. Neural Comput. 6, 559–601. doi: 10.1162/neco.1994.6.4.559
Foley, K. E. (2016). Ideas in movement: the next wave of brain-computer interfaces. Nat. Med. 22, 2–5. doi: 10.1038/nm0116-2
Furber, S. (2016). Large-scale neuromorphic computing systems. J. Neural Eng. 13:051001. doi: 10.1088/1741-2560/13/5/051001
Giordani, M., Berto, M., Di Lauro, M., Bortolotti, C. A., Zoli, M., and Biscarini, F. (2017). Specific dopamine sensing based on short-term plasticity behavior of a whole organic artificial synapse. ACS Sens. 2, 1756–1760. doi: 10.1021/acssensors.7b00542
Gkoupidenis, P., Koutsouras, D. A., and Malliaras, G. G. (2017). Neuromorphic device architectures with global connectivity through electrolyte gating. Nat. Commun. 8:15448. doi: 10.1038/ncomms15448
Gkoupidenis, P., Schaefer, N., Garlan, B., and Malliaras, G. G. (2015). Neuromorphic functions in PEDOT:PSS organic electrochemical transistors. Adv. Mater. 27:7176. doi: 10.1002/adma.201503674
Graudejus, O., Jia, Z., Li, T., and Wagner, S. (2012). Size-dependent rupture strain of elastically stretchable metal conductors. Scripta Mater. 66, 919–922. doi: 10.1016/j.scriptamat.2012.02.034
Graziano, M. (2006). The organization of behavioral repertoire in motor cortex. Annu. Rev. Neurosci. 29, 105–134. doi: 10.1146/annurev.neuro.29.051605.112924
Groothuis, S. S., Folkertsma, G. A., and Stramigioli, S. (2018). A general approach to achieving stability and safe behavior in distributed robotic architectures. Front. Robot. AI 5:108. doi: 10.3389/frobt.2018.00108
Hammock, M. L., Chortos, A., Tee, B. C. K., Tok, J. B. H., and Bao, Z. A. (2013). 25th Anniversary Article: the evolution of electronic skin (E-Skin): a brief history, design considerations, and recent progress. Adv. Mater. 25, 5997–6037. doi: 10.1002/adma.201302240
Hasegawa, T., Ohno, T., Terabe, K., Tsuruoka, T., Nakayama, T., Gimzewski, J. K., et al. (2010). Learning abilities achieved by a single solid-state atomic switch. Adv. Mater. 22:1831. doi: 10.1002/adma.200903680
He, K., Liu, Y., Wang, M., Chen, G., Jiang, Y., Yu, J., et al. (2020). An artificial somatic reflex Arc. Adv. Mater. 32:e1905399. doi: 10.1002/adma.201905399
He, Y. L., Nie, S., Liu, R., Jiang, S. S., Shi, Y., and Wan, Q. (2019). Spatiotemporal information processing emulated by multiterminal neuro-transistor networks. Adv. Mater. 31:1900903. doi: 10.1002/adma.201900903
He, Y., Liu, R., Jiang, S., Chen, C., Zhu, L., Shi, Y., et al. (2020). IGZO-based floating-gate synaptic transistors for neuromorphic computing. J. Phys. D Appl. Phys. 53:215106. doi: 10.1088/1361-6463/ab7bb4
Hettfleisch, K., Bernardes, L. S., Carvalho, M. A., Pastro, L. D. M., Vieira, S. E., Saldiva, S., et al. (2017). Short-Term exposure to urban air pollution and influences on placental vascularization indexes. Environ. Health Perspect. 125, 753–759. doi: 10.1289/ehp300
Ho, V. M., Lee, J.-A., and Martin, K. C. (2011). The cell biology of synaptic plasticity. Science 334, 623–628. doi: 10.1126/science.1209236
Hong, S., Choi, S. H., Park, J., Yoo, H., Oh, J. Y., Hwang, E., et al. (2020). Sensory adaptation and neuromorphic phototransistors based on CsPb(Br1-xIx)3 perovskite and MoS2 hybrid structure. ACS Nano 14, 9796–9806. doi: 10.1021/acsnano.0c01689
Hu, L. X., Fu, S., Chen, Y. H., Cao, H. T., Liang, L. Y., Zhang, H. L., et al. (2017). Ultrasensitive memristive synapses based on lightly oxidized sulfide films. Adv. Mater. 29:1606927. doi: 10.1002/adma.201606927
Ielmini, D., Lacaita, A. L., Pirovano, A., Pellizzer, F., and Bez, R. (2004). Analysis of phase distribution in phase-change nonvolatile memories. IEEE Electron Device Lett. 25, 507–509. doi: 10.1109/led.2004.831219
Indiveri, G., and Liu, S. C. (2015). Memory and information processing in neuromorphic systems. Proc. IEEE 103, 1379–1397. doi: 10.1109/jproc.2015.2444094
Jang, S., Jang, S., Lee, E. H., Kang, M., Wang, G., and Kim, T. W. (2019). Ultrathin conformable organic artificial synapse for wearable intelligent device applications. ACS Appl. Mater. Interfaces 11, 1071–1080. doi: 10.1021/acsami.8b12092
Jerry, M., Dutta, S., Kazemi, A., Ni, K., Zhang, J., Chen, P.-Y., et al. (2018). A ferroelectric field effect transistor based synaptic weight cell. J. Phys. D Appl. Phys. 51:434001. doi: 10.1088/1361-6463/aad6f8
Jiang, J., Guo, J. J., Wan, X., Yang, Y., Xie, H. P., Niu, D. M., et al. (2017). 2D MoS2 neuromorphic devices for brain-like computational systems. Small 13:1700933. doi: 10.1002/smll.201700933
Jo, S. H., Chang, T., Ebong, I., Bhadviya, B. B., Mazumder, P., and Lu, W. (2010). Nanoscale memristor device as synapse in neuromorphic systems. Nano Lett. 10, 1297–1301. doi: 10.1021/nl904092h
John, R. A., Liu, F. C., Chien, N. A., Kulkarni, M. R., Zhu, C., Fu, Q. D., et al. (2018). Synergistic gating of electro-iono-photoactive 2D chalcogenide neuristors: coexistence of hebbian and homeostatic synaptic metaplasticity. Adv. Mater. 30:1800220. doi: 10.1002/adma.201800220
Jordan, M. I., and Mitchell, T. M. (2015). Machine learning: trends, perspectives, and prospects. Science 349, 255–260. doi: 10.1126/science.aaa8415
Kandel, E. R. (2001). Neuroscience - The molecular biology of memory storage: a dialogue between genes and synapses. Science 294, 1030–1038. doi: 10.1126/science.1067020
Kaneko, Y., Nishitani, Y., and Ueda, M. (2014). Ferroelectric artificial synapses for recognition of a multishaded image. IEEE Trans. Electron Devices 61, 2827–2833. doi: 10.1109/ted.2014.2331707
Kim, C. H., Sung, S., and Yoon, M. H. (2016). Synaptic organic transistors with a vacuum-deposited charge-trapping nanosheet. Sci. Rep. 6:33355. doi: 10.1038/srep33355
Kim, K., Chen, C. L., Truong, Q., Shen, A. M., and Chen, Y. (2013). A carbon nanotube synapse with dynamic logic and learning. Adv. Mater. 25, 1693–1698. doi: 10.1002/adma.201203116
Kim, M. K., and Lee, J. S. (2018). Short-Term plasticity and long-term potentiation in artificial biosynapses with diffusive dynamics. ACS Nano 12, 1680–1687. doi: 10.1021/acsnano.7b08331
Kim, M. K., and Lee, J. S. (2019). Ferroelectric analog synaptic transistors. Nano Lett. 19, 2044–2050. doi: 10.1021/acs.nanolett.9b00180
Kim, S., Choi, B., Lim, M., Yoon, J., Lee, J., Kim, H. D., et al. (2017). Pattern recognition using carbon nanotube synaptic transistors with an adjustable weight update protocol. ACS Nano 11, 2814–2822. doi: 10.1021/acsnano.6b07894
Kim, Y., Chortos, A., Xu, W. T., Liu, Y. X., Oh, J. Y., Son, D., et al. (2018). A bioinspired flexible organic artificial afferent nerve. Science 360, 998–1003. doi: 10.1126/science.aao0098
Kullmann, D. M., and Lamsa, K. P. (2007). Long-term synaptic plasticity in hippocampal interneurons. Nat. Rev. Neurosci. 8, 687–699. doi: 10.1038/nrn2207
Kuzum, D., Jeyasingh, R. G., Lee, B., and Wong, H. S. (2012). Nanoelectronic programmable synapses based on phase change materials for brain-inspired computing. Nano Lett. 12, 2179–2186. doi: 10.1021/nl201040y
Kuzum, D., Yu, S., and Wong, H. S. P. (2013). Synaptic electronics: materials, devices and applications. Nanotechnology 24:382001. doi: 10.1088/0957-4484/24/38/382001
Lacour, S. P., Wagner, S., Huang, Z. Y., and Suo, Z. (2003). Stretchable gold conductors on elastomeric substrates. Appl. Phys. Lett. 82, 2404–2406. doi: 10.1063/1.1565683
Langley, P. (2011). The changing science of machine learning. Mach. Learn. 82, 275–279. doi: 10.1007/s10994-011-5242-y
Lankhorst, M. H. R., Ketelaars, B., and Wolters, R. A. M. (2005). Low-cost and nanoscale non-volatile memory concept for future silicon chips. Nat. Mater. 4, 347–352. doi: 10.1038/nmat1350
Law, C. C., and Cooper, L. N. (1994). Formation of receptive-fields in realistic visual environments according to the bienenstock, cooper, and Munro (BCM) theory. Proc. Natl. Acad. Sci. U.S.A. 91, 7797–7801. doi: 10.1073/pnas.91.16.7797
Lee, M., Lee, W., Choi, S., Jo, J. W., Kim, J., Park, S. K., et al. (2017). Brain-Inspired photonic neuromorphic devices using photodynamic amorphous oxide semiconductors and their persistent photoconductivity. Adv. Mater. 29:1700951. doi: 10.1002/adma.201700951
Lee, S. H., Park, H. L., Keum, C. M., Lee, I. H., Kim, M. H., and Lee, S. D. (2019). Organic flexible memristor with reduced operating voltage and high stability by interfacial control of conductive filament growth. physica status solidi (RRL). Rapid Res. Lett. 13:1900044. doi: 10.1002/pssr.201900044
Lee, Y., and Lee, T. W. (2019). Organic synapses for neuromorphic electronics: from brain-inspired computing to sensorimotor nervetronics. Acc. Chem. Res. 52, 964–974. doi: 10.1021/acs.accounts.8b00553
Lee, Y., Oh, J. Y., Xu, W., Kim, O., Kim, T. R., Kang, J., et al. (2018). Stretchable organic optoelectronic sensorimotor synapse. Sci. Adv. 4:eaat7387. doi: 10.1126/sciadv.aat7387
Lewis, R., Asplin, K. E., Bruce, G., Dart, C., Mobasheri, A., and Barrett-Jolley, R. (2011). The role of the membrane potential in chondrocyte volume regulation. J. Cell. Phys. 226, 2979–2986. doi: 10.1002/jcp.22646
Li, H. K., Chen, T. P., Liu, P., Hu, S. G., Liu, Y., Zhang, Q., et al. (2016). A light-stimulated synaptic transistor with synaptic plasticity and memory functions based on InGaZnOx-Al2O3 thin film structure. J. Appl. Phys. 119:244505. doi: 10.1063/1.4955042
Li, S. Z., Zeng, F., Chen, C., Liu, H. Y., Tang, G. S., Gao, S., et al. (2013). Synaptic plasticity and learning behaviours mimicked through Ag interface movement in an Ag/conducting polymer/Ta memristive system. J. Mater. Chem. C 1, 5292–5298. doi: 10.1039/c3tc30575a
Liao, X. K., Xiao, L. Q., Yang, C. Q., and Lu, Y. T. (2014). MilkyWay-2 supercomputer: system and application. Front. Comput. Sci. 8:345–356. doi: 10.1007/s11704-014-3501-3
Lin, Y., Zeng, T., Xu, H., Wang, Z., Zhao, X., Liu, W., et al. (2018). Transferable and flexible artificial memristive synapse based on WOx schottky junction on arbitrary substrates. Adv. Electron. Mater. 4:1800373. doi: 10.1002/aelm.201800373
Linden, D. J. (1994). Long-Term synaptic depression in the mammalian brain. Neuron 12, 457–472. doi: 10.1016/0896-6273(94)90205-4
Liu, N., Liu, Y., Hu, J., He, Y., Zhang, X., and Wan, Q. (2019). pH-dependent plasticity regulation in proton/electron hybrid oxide-based synaptic transistors. Appl. Surface Sci. 481, 1412–1417. doi: 10.1016/j.apsusc.2019.03.037
Liu, N., Zhu, L. Q., Feng, P., Wan, C. J., Liu, Y. H., Shi, Y., et al. (2015). Flexible sensory platform based on oxide-based neuromorphic transistors. Sci. Rep. 5:18082. doi: 10.1038/srep18082
Liu, Y. H., Zhu, L. Q., Feng, P., Shi, Y., and Wan, Q. (2015). Freestanding artificial synapses based on laterally proton-coupled transistors on chitosan membranes. Adv. Mater. 27, 5599–5604. doi: 10.1002/adma.201502719
Liu, Y., Liu, Z., Zhu, B., Yu, J., He, K., Leow, W. R., et al. (2017). Stretchable motion memory devices based on mechanical hybrid materials. Adv. Mater. 29:1701780. doi: 10.1002/adma.201701780
Liu, Z. Y., Yu, M., Lv, J. H., Li, Y. C., and Yu, Z. (2014). Dispersed, porous nanoislands landing on stretchable nanocrack gold films: maintenance of stretchability and controllable impedance. ACS Appl. Mater. Interfaces 6, 13487–13495. doi: 10.1021/am502454t
Lohman, D. F. (1989). Human intelligence - an introduction to advances in theory and research. Rev. Educ. Res. 59, 333–373. doi: 10.2307/1170203
Lumpkin, E. A., and Caterina, M. J. (2007). Mechanisms of sensory transduction in the skin. Nature 445, 858–865. doi: 10.1038/nature05662
Ma, C., Luo, Z., Huang, W., Zhao, L., Chen, Q., Lin, Y., et al. (2020). Sub-nanosecond memristor based on ferroelectric tunnel junction. Nat. Commun. 11:1439. doi: 10.1038/s41467-020-15249-1
Martin, S. J., Grimwood, P. D., and Morris, R. G. M. (2000). “Synaptic plasticity and memory: an evaluation of the hypothesis,” in Annual Review of Neuroscience, eds W. M. Cowan, E. M. Shooter, C. F. Stevens, and R. F. Thompson (Palo Alto, CA: Annual Reviews), 649–711.
Mayford, M., Siegelbaum, S. A., and Kandel, E. R. (2012). Synapses and memory storage. Cold Spring Harb. Perspect. Biol. 4:a005751. doi: 10.1101/cshperspect.a005751
McGaugh, J. L. (2000). Neuroscience – Memory – a century of consolidation. Science 287, 248–251. doi: 10.1126/science.287.5451.248
Mentz, G., Robins, T. G., Batterman, S., and Naidoo, R. N. (2018). Acute respiratory symptoms associated with short term fluctuations in ambient pollutants among schoolchildren in Durban, South Africa. Environ. Pollut. 233, 529–539. doi: 10.1016/j.envpol.2017.10.108
Merolla, P. A., Arthur, J. V., Alvarez-Icaza, R., Cassidy, A. S., Sawada, J., Akopyan, F., et al. (2014). A million spiking-neuron integrated circuit with a scalable communication network and interface. Science 345, 668–673. doi: 10.1126/science.1254642
Morris, R. G. M. (1999). D.O. Hebb: the organization of behavior, Wiley: New York; 1949. Brain Res. Bull. 50, 437–437. doi: 10.1016/s0361-9230(99)00182-3
Nakayama, K., Takata, M., Kasai, T., Kitagawa, A., and Akita, J. (2007). Pulse number control of electrical resistance for multi-level storage based on phase change. J. Phys. D Appl. Phys. 40, 5061–5065. doi: 10.1088/0022-3727/40/17/009
Neher, E. (1992). Ion channels for communication between and within cells (nobel lecture). Angew. Chem. Int. Ed. Engl. 31, 824–829. doi: 10.1002/anie.199208241
Nirschl, T., Philipp, J. B., Flapp, T. D., Burr, G. W., Rajendran, B., Leeo, M. H., et al. (2007). “Write strategies for 2 and 4-bit multi-level phase-change memory,” in Proceedings of the 2007 IEEE International Electron Devices Meeting, (New York: IEEE), 461–464.
Nishitani, Y., Kaneko, Y., Ueda, M., Fujii, E., and Tsujimura, A. (2013). Dynamic observation of brain-like learning in a ferroelectric synapse device. Jpn. J. Appl. Phys. 52:04CE06. doi: 10.7567/jjap.52.04ce06
Ohno, T., Hasegawa, T., Tsuruoka, T., Terabe, K., Gimzewski, J. K., and Aono, M. (2011). Short-term plasticity and long-term potentiation mimicked in single inorganic synapses. Nat. Mater. 10, 591–595. doi: 10.1038/nmat3054
Ovshinsky, S. R. (1968). Reversible electrical switching phenomena in disordered structures. Phys. Rev. Lett. 21:1450. doi: 10.1103/PhysRevLett.21.1450
Park, H. L., Lee, Y., Kim, N., Seo, D. G., Go, G. T., and Lee, T. W. (2020). Flexible neuromorphic electronics for computing, soft robotics, and neuroprosthetics. Adv. Mater. 32:e1903558. doi: 10.1002/adma.201903558
Park, M. H., Lee, Y. H., Kim, H. J., Kim, Y. J., Moon, T., Do Kim, K., et al. (2015). Ferroelectricity and antiferroelectricity of doped thin HfO2-Based films. Adv. Mater. 27, 1811–1831. doi: 10.1002/adma.201404531
Park, Y., and Lee, J. S. (2017). Artificial synapses with short- and long-term memory for spiking neural networks based on renewable materials. ACS Nano 11, 8962–8969. doi: 10.1021/acsnano.7b03347
Pereda, A. E. (2014). Electrical synapses and their functional interactions with chemical synapses. Nat. Rev. Neurosci. 15, 250–263. doi: 10.1038/nrn3708
Picard, R. W., Vyzas, E., and Healey, J. (2001). Toward machine emotional intelligence: analysis of affective physiological state. IEEE Trans. Pattern Anal. Mach. Intell. 23, 1175–1191. doi: 10.1109/34.954607
Prezioso, M., Merrikh-Bayat, F., Hoskins, B. D., Adam, G. C., Likharev, K. K., and Strukov, D. B. (2015). Training andoperation of an integrated neuromorphic network based on metal-oxide memristors. Nature 521, 61–64. doi: 10.1038/nature14441
Pruszynski, J. A., and Johansson, R. S. (2014). Edge-orientation processing in first-order tactile neurons. Nat. Neurosci. 17, 1404–1409. doi: 10.1038/nn.3804
Qian, C., Sun, J., Kong, L. A., Gou, G. Y., Yang, J. L., He, J., et al. (2016). Artificial synapses based on in-plane gate organic electrochemical transistors. ACS Appl. Mater. Interfaces 8, 26169–26175. doi: 10.1021/acsami.6b08866
Qian, L., Sun, Y. L., Wu, M. M., Li, C., Xie, D., Ding, L. M., et al. (2018). A lead-free two-dimensional perovskite for a high-performance flexible photoconductor and a light-stimulated synaptic device. Nanoscale 10, 6837–6843. doi: 10.1039/c8nr00914g
Raeis-Hosseini, N., Park, Y., and Lee, J.-S. (2018). Flexible artificial synaptic devices based on collagen from fish protein with spike-timing-dependent plasticity. Adv. Funct. Mater. 28:1800553. doi: 10.1002/adfm.201800553
Ramakrishnan, S., Hasler, P. E., and Gordon, C. (2011). Floating gate synapses with spike-time-dependent plasticity. IEEE Trans. Biomed. Circuits Syst. 5, 244–252. doi: 10.1109/tbcas.2011.2109000
Regehr, W. G. (2012). Short-Term presynaptic plasticity. Cold Spring Harb. Perspect. Biol. 4:a005702. doi: 10.1101/cshperspect.a005702
Ren, Y., Yang, J. Q., Zhou, L., Mao, J. Y., Zhang, S. R., Zhou, Y., et al. (2018). Gate-Tunable synaptic plasticity through controlled polarity of charge trapping in fullerene composites. Adv. Funct. Mater. 28:1805599. doi: 10.1002/adfm.201805599
Schmitt, F. O., Dev, P., and Smith, B. H. (1976). Electrotonic processing of information by brain-cells. Science 193, 114–120.
Seo, S., Jo, S. H., Kim, S., Shim, J., Oh, S., Kim, J. H., et al. (2018). Artificial optic-neural synapse for colored and color-mixed pattern recognition. Nat. Commun. 9:5106. doi: 10.1038/s41467-018-07572-5
Sharbati, M. T., Du, Y., Torres, J., Ardolino, N. D., Yun, M., and Xiong, F. (2018). Low-Power, electrochemically tunable graphene synapses for neuromorphic computing. Adv. Mater. 30:e1802353. doi: 10.1002/adma.201802353
Shin, Y. J., Kim, Y., Kang, S. J., Nahm, H. H., Murugavel, P., Kim, J. R., et al. (2017). Interface control of ferroelectricity in an SrRuO3/BaTiO3/SrRuO3 capacitor and its critical thickness. Adv. Mater. 29:1602795. doi: 10.1002/adma.201602795
Song, Z., Tong, Y., Zhao, X., Ren, H., Tang, Q., and Liu, Y. (2019). A flexible conformable artificial organ-damage memory system towards hazardous gas leakage based on a single organic transistor. Mater. Horizons 6, 717–726. doi: 10.1039/c8mh01577e
Stefan, K., Classen, J., Celnik, P., and Cohen, L. G. (2008). Concurrent action observation modulates practice-induced motor memory formation. Eur. J. Neurosci. 27, 730–738. doi: 10.1111/j.1460-9568.2008.06035.x
Sun, J., Oh, S., Choi, Y., Seo, S., Oh, M. J., Lee, M., et al. (2018). Optoelectronic synapse based on IGZO-Alkylated graphene oxide hybrid structure. Adv. Funct. Mater. 28:1804397. doi: 10.1002/adfm.201804397
Suri, M., Bichler, O., Querlioz, D., Traore, B., Cueto, O., Perniola, L., et al. (2012). Physical aspects of low power synapses based on phase change memory devices. J. Appl. Phys. 112:054904. doi: 10.1063/1.4749411
Tabot, G. A., Dammann, J. F., Berg, J. A., Tenore, F. V., Boback, J. L., Vogelstein, R. J., et al. (2013). Restoring the sense of touch with a prosthetic hand through a brain interface. Proc. Natl. Acad. Sci. U.S.A. 110, 18279–18284. doi: 10.1073/pnas.1221113110
Tan, H., Tao, Q., Pande, I., Majumdar, S., Liu, F., Zhou, Y., et al. (2020). Tactile sensory coding and learning with bio-inspired optoelectronic spiking afferent nerves. Nat. Commun. 11:1369. doi: 10.1038/s41467-020-15105-2
Thomson, A. M., and Deuchars, J. (1994). Temporal and spatial properties of local circuits in neocortex. Trends Neurosci. 17, 119–126. doi: 10.1016/0166-2236(94)90121-x
Tian, B., Liu, L., Yan, M., Wang, J., Zhao, Q., Zhong, N., et al. (2019). A robust artificial synapse based on organic ferroelectric polymer. Adv. Electron. Mater. 5:1800600. doi: 10.1002/aelm.201800600
Tian, H., Mi, W. T., Wang, X. F., Zhao, H. M., Xie, Q. Y., Li, C., et al. (2015). Graphene dynamic synapse with modulatable plasticity. Nano Lett. 15, 8013–8019. doi: 10.1021/acs.nanolett.5b03283
Tiwari, N., Rajput, M., John, R. A., Kulkarni, M. R., Nguyen, A. C., and Mathews, N. (2018). Indium tungsten oxide thin films for flexible high-performance transistors and neuromorphic electronics. ACS Appl. Mater. Interfaces 10, 30506–30513. doi: 10.1021/acsami.8b06956
Tsodyks, M., Pawelzik, K., and Markram, H. (1998). Neural networks with dynamic synapses. Neural Comput. 10, 821–835. doi: 10.1162/089976698300017502
Tu, L., Yuan, S., Xu, J., Yang, K., Wang, P., Cui, X., et al. (2018). A wide-range operating synaptic device based on organic ferroelectricity with low energy consumption. RSC Adv. 8, 26549–26553. doi: 10.1039/c8ra04403a
Tuchman, Y., Mangoma, T. N., Gkoupidenis, P., van de Burgt, Y., John, R. A., Mathews, N., et al. (2020). Organic neuromorphic devices: past, present, and future challenges. MRS Bull. 45, 619–630. doi: 10.1557/mrs.2020.196
Urgesi, C., Moro, V., Candidi, M., and Aglioti, S. M. (2006). Mapping implied body actions in the human motor system. J. Neurosci. 26, 7942–7949. doi: 10.1523/jneurosci.1289-06.2006
van de Burgt, Y., Lubberman, E., Fuller, E. J., Keene, S. T., Faria, G. C., Agarwal, S., et al. (2017). A non-volatile organic electrochemical device as a low-voltage artificial synapse for neuromorphic computing. Nat. Mater. 16, 414–418. doi: 10.1038/nmat4856
Voglis, G., and Tavernarakis, N. (2006). The role of synaptic ion channels in synaptic plasticity. EMBO Rep. 7, 1104–1110. doi: 10.1038/sj.embor.7400830
Wan, C. J., Liu, Y. H., Feng, P., Wang, W., Zhu, L. Q., Liu, Z. P., et al. (2016a). Flexible metal oxide/graphene oxide hybrid neuromorphic transistors on flexible conducting graphene substrates. Adv. Mater. 28:5878. doi: 10.1002/adma.201600820
Wan, C. J., Liu, Y. H., Zhu, L. Q., Feng, P., Shi, Y., and Wan, Q. (2016b). Short-Term synaptic plasticity regulation in solution-gated indium-gallium-zinc-oxide electric-double-layer transistors. ACS Appl. Mater. Interfaces 8, 9762–9768. doi: 10.1021/acsami.5b12726
Wan, C. J., Zhu, L. Q., Zhou, J. M., Shi, Y., and Wan, Q. (2013). Memory and learning behaviors mimicked in nanogranular SiO2-based proton conductor gated oxide-based synaptic transistors. Nanoscale 5, 10194–10199. doi: 10.1039/c3nr02987e
Wan, C., Chen, G., Fu, Y., Wang, M., Matsuhisa, N., Pan, S., et al. (2018). An artificial sensory neuron with tactile perceptual learning. Adv. Mater. 30:1801291. doi: 10.1002/adma.201801291
Wan, Q., Zeng, F., Yin, J., Sun, Y., Hu, Y., Liu, J., et al. (2019). Phase-change nanoclusters embedded in a memristor for simulating synaptic learning. Nanoscale 11, 5684–5692. doi: 10.1039/c8nr09765h
Wan, X., Feng, P., Dong, Wu, G., Shi, Y., and Wan, Q. (2015). Simulation of laterally coupled InGaZnO4-Based electric-double-layer transistors for synaptic electronics. IEEE Electron Device Lett. 36, 204–206. doi: 10.1109/led.2015.2388952
Wang, H., Zhao, Q., Ni, Z., Li, Q., Liu, H., Yang, Y., et al. (2018a). A ferroelectric/electrochemical modulated organic synapse for ultraflexible, artificial visual-perception system. Adv. Mater. 30:1803961. doi: 10.1002/adma.201803961
Wang, K., Dai, S. L., Zhao, Y. W., Wang, Y., Liu, C., and Huang, J. (2019). Light-Stimulated synaptic transistors fabricated by a facile solution process based on inorganic perovskite quantum dots and organic semiconductors. Small 15:1900010. doi: 10.1002/smll.201900010
Wang, M., Luo, Y., Wang, T., Wan, C., Pan, L., Pan, S., et al. (2020). Artificial skin perception. Adv. Mater. 33:e2003014. doi: 10.1002/adma.202003014
Wang, T. Y., He, Z. Y., Liu, H., Chen, L., Zhu, H., Sun, Q. Q., et al. (2018b). Flexible electronic synapses for face recognition application with multimodulated conductance states. ACS Appl. Mater. Interfaces 10, 37345–37352. doi: 10.1021/acsami.8b16841
Wang, Y., Lv, Z. Y., Liao, Q. F., Shan, H. Q., Chen, J. R., Zhou, Y., et al. (2018d). Synergies of electrochemical metallization and valance change in all-inorganic perovskite quantum dots for resistive switching. Adv. Mater. 30:1800327. doi: 10.1002/adma.201800327
Wang, Y., Lv, Z., Chen, J., Wang, Z., Zhou, Y., Zhou, L., et al. (2018c). Photonic synapses based on inorganic perovskite quantum dots for neuromorphic computing. Adv. Mater. 30:1802883. doi: 10.1002/adma.201802883
Wu, C., Kim, T. W., Choi, H. Y., Strukov, D. B., and Yang, J. J. (2017). Flexible three-dimensional artificial synapse networks with correlated learning and trainable memory capability. Nat. Commun. 8:752. doi: 10.1038/s41467-017-00803-1
Wu, G., Zhang, J., Wan, X., Yang, Y., and Jiang, S. (2014). Chitosan-based biopolysaccharide proton conductors for synaptic transistors on paper substrates. J. Mater. Chem. C 2, 6249–6255. doi: 10.1039/c4tc00652f
Xu, W., Lee, Y., Min, S. Y., Park, C., and Lee, T. W. (2016a). Simple, inexpensive, and rapid approach to fabricate cross-shaped memristors using an inorganic-nanowire-digital-alignment technique and a one-step reduction process. Adv. Mater. 28, 527–532. doi: 10.1002/adma.201503153
Xu, W., Min, S. Y., Hwang, H., and Lee, T. W. (2016b). Organic core-sheath nanowire artificial synapses with femtojoule energy consumption. Sci. Adv. 2:e1501326. doi: 10.1126/sciadv.1501326
Yang, C. S., Shang, D. S., Liu, N., Shi, G., Shen, X., Yu, R. C., et al. (2017). A synaptic transistor based on quasi-2D molybdenum oxide. Adv. Mater. 29:1700906. doi: 10.1002/adma.201700906
Yang, J. T., Ge, C., Du, J. Y., Huang, H. Y., He, M., Wang, C., et al. (2018). Artificial synapses emulated by an electrolyte-gated tungsten-oxide transistor. Adv. Mater. 30:1801548. doi: 10.1002/adma.201801548
Yang, Y. C., Gao, P., Gaba, S., Chang, T., Pan, X. Q., and Lu, W. (2012). Observation of conducting filament growth in nanoscale resistive memories. Nat. Commun. 3:732. doi: 10.1038/ncomms1737
Yang, Y., He, Y. L., Nie, S., Shi, Y., and Wan, Q. (2018). Light stimulated IGZO-Based electric-double-layer transistors for photoelectric neuromorphic devices. IEEE Electron Device Lett. 39, 897–900. doi: 10.1109/led.2018.2824339
Yoon, J. H., Wang, Z., Kim, K. M., Wu, H., Ravichandran, V., Xia, Q., et al. (2018). An artificial nociceptor based on a diffusive memristor. Nat. Commun. 9:417. doi: 10.1038/s41467-017-02572-3
Yoon, S. M., Yang, S., Jung, S. W., Byun, C. W., Ryu, M. K., Cheong, W. S., et al. (2011). Polymeric ferroelectric and oxide semiconductor-based fully transparent memristor cell. Appl. Phys. A Mater. Sci. Process. 102, 983–990. doi: 10.1007/s00339-011-6280-9
Yu, F., Zhu, L. Q., Xiao, H., Gao, W. T., and Guo, Y. B. (2018). Restickable oxide neuromorphic transistors with spike-timing-dependent plasticity and pavlovian associative learning activities. Adv. Funct. Mater. 28:1804025. doi: 10.1002/adfm.201804025
Yuan, H. T., Shimotani, H., Tsukazaki, A., Ohtomo, A., Kawasaki, M., and Iwasa, Y. (2010). Hydrogenation-Induced surface polarity recognition and proton memory behavior at protic-ionic-liquid/oxide electric-double-layer interfaces. J. Am. Chem. Soc. 132, 6672–6678. doi: 10.1021/ja909110s
Zang, Y., Shen, H., Huang, D., Di, C. A., and Zhu, D. (2017). A dual-organic-transistor-based tactile-perception system with signal-processing functionality. Adv. Mater. 29:1606088. doi: 10.1002/adma.201606088
Zhang, C. X., Li, S., He, Y. L., Chen, C. S., Jiang, S. S., Yang, X. Q., et al. (2020). Oxide synaptic transistors coupled with triboelectric nanogenerators for bio-inspired tactile sensing application. IEEE Electron Device Lett. 41, 617–620. doi: 10.1109/led.2020.2972038
Zhang, C., Ye, W. B., Zhou, K., Chen, H. Y., Yang, J. Q., Ding, G. L., et al. (2019). Bioinspired artificial sensory nerve based on nafion memristor. Adv. Funct. Mater. 29:1808783. doi: 10.1002/adfm.201808783
Zhang, D. M., Zeng, L., Cao, K. H., Wang, M. X., Peng, S. Z., Zhang, Y., et al. (2016). All spin artificial neural networks based on compound spintronic synapse and neuron. IEEE Trans. Biomed. Circuits Syst. 10, 828–836. doi: 10.1109/tbcas.2016.2533798
Zhang, J. J., Sun, H. J., Li, Y., Wang, Q., Xu, X. H., and Miao, X. S. (2013). AgInSbTe memristor with gradual resistance tuning. Appl. Phys. Lett. 102:183513. doi: 10.1063/1.4804983
Zhang, S.-R., Zhou, L., Mao, J.-Y., Ren, Y., Yang, J.-Q., Yang, G.-H., et al. (2019). Artificial synapse emulated by charge trapping-based resistive switching device. Adv. Mater. Technol. 4:1800342. doi: 10.1002/admt.201800342
Zhang, X. M., Liu, S., Zhao, X. L., Wu, F. C., Wu, Q. T., Wang, W., et al. (2017). Emulating short-term and long-term plasticity of bio-synapse based on Cu/a-Si/Pt memristor. IEEE Electron Device Lett. 38, 1208–1211. doi: 10.1109/led.2017.2722463
Zhou, J., Liu, N., Zhu, L., Shi, Y., and Wan, Q. (2015). Energy-Efficient artificial synapses based on flexible IGZO electric-double-layer transistors. IEEE Electron Device Lett. 36, 198–200. doi: 10.1109/led.2014.2381631
Zhu, L. Q., Wan, C. J., Gao, P. Q., Liu, Y. H., Xiao, H., Ye, J. C., et al. (2016). Flexible proton-gated oxide synaptic transistors on SI membrane. ACS Appl. Mater. Interfaces 8, 21770–21775. doi: 10.1021/acsami.6b05167
Keywords: neuromorphic devices, artificial neural systems, artificial intelligence, bionic sensing and perception, neuromorphic engineering
Citation: Zeng M, He Y, Zhang C and Wan Q (2021) Neuromorphic Devices for Bionic Sensing and Perception. Front. Neurosci. 15:690950. doi: 10.3389/fnins.2021.690950
Received: 05 April 2021; Accepted: 07 June 2021;
Published: 29 June 2021.
Edited by:
Yimao Cai, Peking University, ChinaReviewed by:
Simeon A. Bamford, Italian Institute of Technology (IIT), ItalyVassiliy Tsytsarev, University of Maryland, College Park, United States
Copyright © 2021 Zeng, He, Zhang and Wan. This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.
*Correspondence: Qing Wan, d2FucWluZ0BuanUuZWR1LmNu