A N M Nafiul Islam's research while affiliated with Pennsylvania State University and other places

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Publications (15)


Hardware in Loop Learning with Spin Stochastic Neurons
  • Article
  • Full-text available

April 2024

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20 Reads

Advanced Intelligent Systems

Advanced Intelligent Systems

A N M Nafiul Islam

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Amit Kumar Shukla

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Despite the promise of superior efficiency and scalability, real‐world deployment of emerging nanoelectronic platforms for brain‐inspired computing have been limited thus far, primarily because of inter‐device variations and intrinsic non‐idealities. In this work, mitigation of these issues is demonstrated by performing learning directly on practical devices through a hardware‐in‐loop approach, utilizing stochastic neurons based on heavy metal/ferromagnetic spin–orbit torque heterostructures. The probabilistic switching and device‐to‐device variability of the fabricated devices of various sizes is characterized to showcase the effect of device dimension on the neuronal dynamics and its consequent impact on network‐level performance. The efficacy of the hardware‐in‐loop scheme is illustrated in a deep learning scenario achieving equivalent software performance. This work paves the way for future large‐scale implementations of neuromorphic hardware and realization of truly autonomous edge‐intelligent devices.

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Hydrogenated VO2 Bits for Probabilistic Computing

October 2023

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44 Reads

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4 Citations

IEEE Electron Device Letters

The stochastic nature of electronic phase transitions can serve as a random number generating source. This work reports probabilistic bits ( ${p}$ -bits) based on hydrogen-doped vanadium oxide (H-VO2) devices with tunable insulator-metal transition (IMT) characteristics. Hydrogen donor doping reduces ground state resistance and enables control over threshold switching voltage in the post-fabricated devices. Through a paired-pulse scheme, the H-VO2 devices could generate stochastic bit sequences with adjustable switching probabilities. The sequence with a ${p}$ -bit value of 0.488 could pass 14 out of 15 National Institute of Standards and Technology (NIST) random and pseudorandom number generator tests.



Figure 1: Two neurons interacting with a common astrocyte.
Figure 4: Quantitative relationship between self-repair ratio, q, and fault severity, z.
Figure 5: SNN network architecture used for unsupervised learning. Lateral inhibitory connections are only shown for one neuron in the output layer.
Astromorphic Self-Repair of Neuromorphic Hardware Systems

June 2023

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30 Reads

Proceedings of the AAAI Conference on Artificial Intelligence

While neuromorphic computing architectures based on Spiking Neural Networks (SNNs) are increasingly gaining interest as a pathway toward bio-plausible machine learning, attention is still focused on computational units like the neuron and synapse. Shifting from this neuro-synaptic perspective, this paper attempts to explore the self-repair role of glial cells, in particular, astrocytes. The work investigates stronger correlations with astrocyte computational neuroscience models to develop macro-models with a higher degree of bio-fidelity that accurately captures the dynamic behavior of the self-repair process. Hardware-software co-design analysis reveals that bio-morphic astrocytic regulation has the potential to self-repair hardware realistic faults in neuromorphic hardware systems with significantly better accuracy and repair convergence for unsupervised learning tasks on the MNIST and F-MNIST datasets. Our implementation source code and trained models are available at https://github.com/NeuroCompLab-psu/Astromorphic_Self_Repair.


Figures and Tables
Fig. S3. Persistence of neuronal dynamics. The neuronal dynamics of the same device was measured after a week, and it showed similar switching characteristics, with no significant variation (~0.5%) in the bias switching current.
Hardware in Loop Learning with Spin Stochastic Neurons

May 2023

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56 Reads

Despite the promise of superior efficiency and scalability, real-world deployment of emerging nanoelectronic platforms for brain-inspired computing have been limited thus far, primarily because of inter-device variations and intrinsic non-idealities. In this work, we demonstrate mitigating these issues by performing learning directly on practical devices through a hardware-in-loop approach, utilizing stochastic neurons based on heavy metal/ferromagnetic spin-orbit torque heterostructures. We characterize the probabilistic switching and device-to-device variability of our fabricated devices of various sizes to showcase the effect of device dimension on the neuronal dynamics and its consequent impact on network-level performance. The efficacy of the hardware-in-loop scheme is illustrated in a deep learning scenario achieving equivalent software performance. This work paves the way for future large-scale implementations of neuromorphic hardware and realization of truly autonomous edge-intelligent devices.


Hybrid stochastic synapses enabled by scaled ferroelectric field-effect transistors

March 2023

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24 Reads

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5 Citations

Applied Physics Letters

Achieving brain-like density and performance in neuromorphic computers necessitates scaling down the size of nanodevices emulating neuro-synaptic functionalities. However, scaling nanodevices results in reduction of programming resolution and emergence of stochastic non-idealities. While prior work has mainly focused on binary transitions, in this work, we leverage the stochastic switching of a three-state ferroelectric field-effect transistor to implement a long-term and short-term two-tier stochastic synaptic memory with a single device. Experimental measurements are performed on a scaled 28 nm high- k metal gate technology-based device to develop a probabilistic model of the hybrid stochastic synapse. In addition to the advantage of ultra-low programming energies afforded by scaling, our hardware–algorithm co-design analysis reveals the efficacy of the two-tier memory in comparison to binary stochastic synapses in on-chip learning tasks—paving the way for algorithms exploiting multi-state devices with probabilistic transitions beyond deterministic ones.


Fig. 1. Homotypic Mott neuromorphic platform. (A) Schematic of biological neurons and synapses. Neurons serve as processing units connected through synapses. (B) Schematic of two-terminal volatile and nonvolatile (H x )VO 2 devices integrated on a single sapphire substrate. The volatilities in the (H x )VO 2 material system can be controlled by selective hydrogenation. Pristine vanadium dioxide (VO 2 ) devices can be used as spiking neurons, and nonvolatile H x VO 2 devices can serve as analog synaptic components. (C) Network architecture for the (H x )VO 2 spiking neural network (SNN) proposed in this work. An example input is from the Fashion-MNIST (Modified National Institute of Standards and Technology) dataset, and it goes through Sobel filtering and Poisson spike encoding before being fed into the network. For MNIST, only the spike encoding is performed before being input to the network. The input layer size is 784, followed by 400 excitatory and inhibitory neurons (1600 for MNIST). (D) Weight evolution during training on Fashion-MNIST of nine representative neurons of the network. The weights are modulated according to the spike timing-dependent plasticity (STDP) rule and approximate different patterns in the training set.
Fig. 2. Selective area carrier doping. (A) Crystal structures of VO 2 and H x VO 2 . Gray, orange, and purple spheres stand for vanadium, oxygen, and hydrogen atoms, respectively. The pristine VO 2 has a monoclinic structure at room temperature. In H x VO 2 , hydrogen atoms tend to occupy interstitial sites among VO 2 lattices. Density functional calculations show that H x VO 2 stays in a pseudorutile phase when the hydrogenation level (x) is >0.25. (B) Averaged electron energy-loss spectroscopy spectra from a VO 2 and a H x VO 2 region centered on the vanadium (V) L 2,3 and oxygen (O) K-edges. The spectra were normalized using the averaged intensity level between 640 and 660 eV (see fig. S3). a.u., arbitrary units. (C) X-ray diffraction (XRD) spectra of the VO 2 thin film (black line) grown on c-plane sapphire substrate, the H x VO 2 with Pd electrodes (red line), and VO 2 with TiAu electrodes (blue line) after the hydrogenation. The out-of-plane lattice of VO 2 after the hydrogenation is expanded. (D) Optical microscope image of pristine and H-doped VO 2 devices was fabricated on a single substrate. The channel region is noted with a down pointing arrow. (E) Conductive atomic force microscope (C-AFM) images of the (H x )VO 2 channels with different electrode combinations after the hydrogenation. Bright conductivity contrast appears near the Pd electrode of TiAu + Pd device, indicating the hydrogenated VO 2 . (F) Spatial Raman mapping in the (H x )VO 2 channel of TiAu + Pd device (top panel). The Raman peak of VO 2 at 615 cm −1 was fixed for this mapping. This characteristic peak exists in VO 2 but disappears in H x VO 2 . Raman spectra measured at points A, B, and C (bottom panel). The Raman spectrum of monoclinic VO 2 is plotted as a reference. (G) Temperature-dependent resistance of the TiAu + Pd device was annealed at different annealing conditions. (H) Current-voltage relation (I-V ) curves of the TiAu + Pd device for different hydrogenation levels. Hydrogenation can effectively create intermediate resistance states in VO 2 .
Fig. 3. Threshold switching and learning in (H x )VO 2 devices. (A) I-V curves of the TiAu + TiAu device in the 1st, 500th, and 1000th sweep cycle with a compliance current (I cc ) of 1 mA. The TiAu + TiAu device clearly demonstrates volatile threshold switching. (B) Schematic of neuronal component composed of the volatile VO 2 device, a load resistor, and a capacitor. (C) Measured output voltage waveforms of the neuron. Amplitutde (A p ), capacitor (C M ), pulse width (t p ), and duty ratio (D p ) are set at 0.8 mA, 4.4 nF, 7 μs, and 50%, respectively. (D) I-V curves of the TiAu + Pd device in the 1st, 500th, and 1000th sweep cycle with an I cc of 5 mA in the positive polarity and 1 mA in the negative polarity. The TiAu + Pd device exhibits a combination of nonvolatile resistive switching and threshold switching. (E) Potentiation and depression of the TiAu + Pd device upon different applied pulses. The pulse widths are 1 μs. (F) First-principles calculation of relative stabilities of H x VO 2 (M1) and H x VO 2 (R) phases across different levels of H concentrations. For the sake of clarity, H x VO 2 (M1) and H x VO 2 (R) are in pseudomonoclinic and pseudorutile phases, respectively, since the presence of protons alters the ideal lattice parameters and bond distances of both the pristine monoclinic and rutile phases. The light sea green region describes the zone where H x VO 2 (M1) is more favorable, whereas the light magenta regime indicates that H x VO 2 (R) is more stable. Insets (i), (ii), (iii), and (iv) are the total density of states (DOS) of the lowenergy phases of 0.0, 0.03, 0.25, and 0.50 atomic fraction of H levels in H x VO 2 , respectively. With increasing H dopant level, the semiconducting monoclinic H x VO 2 phase (i) narrows its bandgap from ~0.61 to 0.5 eV as seen in (ii). Upon further doping, it changes to metallic (iii) in its pseudomonoclinic phases and its pseudorutile phases (iv).
Fig. 4. (H x )VO 2 neural circuits and SNNs. (A) Schematic of a connected neural circuit for the feedforward excitation and inhibition motifs. A presynaptic neuron (N1), a synapse, and a postsynaptic neuron (N2) are connected in series with two isolators inserted between them. (B) Photograph of the neural circuit hardware. Inset: Neuromorphic chip with both volatile neuron-like and nonvolatile synapse-like (H x )VO 2 devices. GND stands for ground. A voltage-to-current converter is used to convert voltage pulses (V in ) from an arbitrary function generator into current pulses (I in ) as the circuit input. (C) Simulated and (D) measured output voltage waveforms of N1 and N2 for different synaptic weights. The current pulse train injecting into N1 has an A p of 2.1 mA, a t p of 7 μs, and a D p of 50%. (E) Measured input-current-dependent firing probability (defined by the output spike number per 30 input current pulses) of N2 under different synaptic weights. (F) Cumulative switching dynamics of the volatile VO 2 neurons, which are fitted into sigmoidal stochastic switching neurons used in the network simulation. Training accuracy for (G) Fashion-MNIST and (H) MNIST over 3 and 10 training epochs, respectively. For Fashion-MNIST, we have a batch size of 16, while it is 32 for MNIST. For both datasets, each epoch consists of 60,000 training images. We obtained a final test accuracy of 73.22% on Fashion-MNIST and 92.1% on MNIST. Inset of (G) is the trained weight pattern for Fashion-MNIST. The network of 400 excitatory neurons was trained over the 60,000 training images for three epochs. Inset of (H) is the trained weight pattern for MNIST. The network of 1600 excitatory neurons was trained over the 60,000 training images for 10 epochs.
Selective area doping for Mott neuromorphic electronics

March 2023

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197 Reads

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16 Citations

Science Advances

The cointegration of artificial neuronal and synaptic devices with homotypic materials and structures can greatly simplify the fabrication of neuromorphic hardware. We demonstrate experimental realization of vanadium dioxide (VO2) artificial neurons and synapses on the same substrate through selective area carrier doping. By locally configuring pairs of catalytic and inert electrodes that enable nanoscale control over carrier density, volatility or nonvolatility can be appropriately assigned to each two-terminal Mott memory device per lithographic design, and both neuron- and synapse-like devices are successfully integrated on a single chip. Feedforward excitation and inhibition neural motifs are demonstrated at hardware level, followed by simulation of network-level handwritten digit and fashion product recognition tasks with experimental characteristics. Spatially selective electron doping opens up previously unidentified avenues for integration of emerging correlated semiconductors in electronic device technologies.


Complex Oxides for Brain‐Inspired Computing: A Review

November 2022

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649 Reads

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32 Citations

The fields of brain‐inspired computing, robotics, and, more broadly, artificial intelligence (AI) seek to implement knowledge gleaned from the natural world into human‐designed electronics and machines. In this review, the opportunities presented by complex oxides, a class of electronic ceramic materials whose properties can be elegantly tuned by doping, electron interactions, and a variety of external stimuli near room temperature, are discussed. The review begins with a discussion of natural intelligence at the elementary level in the nervous system, followed by collective intelligence and learning at the animal colony level mediated by social interactions. An important aspect highlighted is the vast spatial and temporal scales involved in learning and memory. The focus then turns to collective phenomena, such as metal‐to‐insulator transitions (MITs), ferroelectricity, and related examples, to highlight recent demonstrations of artificial neurons, synapses, and circuits and their learning. First‐principles theoretical treatments of the electronic structure, and in situ synchrotron spectroscopy of operating devices are then discussed. The implementation of the experimental characteristics into neural networks and algorithm design is then revewed. Finally, outstanding materials challenges that require a microscopic understanding of the physical mechanisms, which will be essential for advancing the frontiers of neuromorphic computing, are highlighted.


Fig. 1. (a) TEM cross-section and schematic of the FeFET structure used in this work, with HfO 2 ferroelectric layer. (b) Simulation studies showing conductance of the device with variable programming voltage magnitudes for different number of domains in the FE layer of the device. As the domain number increases, the number of available states (indicated by specific conductances) increases and their transition is no longer abrupt and stochastic.
Hybrid Stochastic Synapses Enabled by Scaled Ferroelectric Field-effect Transistors

September 2022

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73 Reads

Achieving brain-like density and performance in neuromorphic computers necessitates scaling down the size of nanodevices emulating neuro-synaptic functionalities. However, scaling nanodevices results in reduction of programming resolution and emergence of stochastic non-idealities. While prior work has mainly focused on binary transitions, in this work we leverage the stochastic switching of a three-state ferroelectric field effect transistor (FeFET) to implement a long-term and short-term 2-tier stochastic synaptic memory with a single device. Experimental measurements are performed on a scaled 28nm high-$k$ metal gate technology based device to develop a probabilistic model of the hybrid stochastic synapse. In addition to the advantage of ultra-low programming energies afforded by scaling, our hardware-algorithm co-design analysis reveals the efficacy of the 2-tier memory in comparison to binary stochastic synapses in on-chip learning tasks -- paving the way for algorithms exploiting multi-state devices with probabilistic transitions beyond deterministic ones.


Nonassociative learning in NiOx. a) Schematic of a gene (DNA). b) Habituation indicates a reduction in the response after repetitive exposure to stimuli. c) Sensitization implies an increase in response with respect to the iterative stimulus. The positive/negative signs represent marked genes with respect to inputs (training). d) Schematic of NiOx device architecture. The input training pulses were applied between the top (Pd) and bottom (Pt) electrode which causes movement of oxygen vacancies depending on the amplitude of the pulses. (inset) Optical image of an array of NiOx test chip. e–f) Relative percentage change in resistance with respect to the training times when each training cycle was performed for 52 s with an interval of T = 8 s. The pulse width was kept constant to 500 ms with the amplitude of input pulses of E1 = 5 mV nm⁻¹ for habituation (e) and 30 mV nm⁻¹ for sensitization (f). (inset) Triangular pulses used for measuring the change in resistance state. (bottom panels) Square‐shaped training pulse series applied to the device for the habituation and sensitization measurement.
Training interval and bias amplitude‐dependent habituation and sensitization. a,b) Habituation and sensitization measurement was executed by following the resting time of 24 h and applying training electric field of 5 and 30 mV nm⁻¹, respectively. The NiOx device returns to the original resistive response after long rest period in normal laboratory environment. c) Training interval (T) dependence of the NiOx device with a constant pulse amplitude E1 = 5 mV nm⁻¹. The arrow indicates habituation in an electric field even after training interval T of 52 s, which is equal to the training time. d) Sensitization of NiOx with E1 = 30 mV nm⁻¹ for different training intervals. The increased response is independent of the training interval. e) Amplitude of training pulse (E1) dependence of NiOx with a constant training interval T = 8 s. The critical electric field between habituation and sensitization is about 20 mV nm⁻¹. (Inset) Movement of oxygen vacancies at different training pulses.
Habituation and sensitization model based on “stimulus model comparator theory.[³⁰]” a) A proposed model on habituation and sensitization based on retraining using weak and strong stimulus (inputs), respectively. b,c) The resistance decay behavior of NiOx has been compared with the decay time constant (τ), extracted from the decay curve by fitting the exponential relation, ΔR(t)/ΔRo=exp[ 1−(t/τ)β ], where, ΔR(t)=R(t)−Rpristine and ΔRo=Ro−Rpristine in which R (t) is the resistance at any specific time t and Ro is the resistance measured immediately after applying b) single and c) 50 training pulses and index β ranging from 0 to 1. (insets) τ representing relaxation time constant with respect to the amplitude of training pulses. d) A statistical distribution of memory window was collected from 65 devices measured immediately after applying the pulses of ±30 mV nm⁻¹ for 500 ms.
Mechanisms enabling cellular‐like learning in oxygen‐deficient NiOx. a) Electrical resistivity with visual color change in NiOx films after annealing at different temperature (Figure S2, Supporting Information). b) (bottom) Optimal resistive switching state in the as‐prepared (AP) NiOx is essential for cellular‐like learning. The resistance increases from 4.7 kΩ (pristine) to 5.2 kΩ for application pulse width of +30 mV nm⁻¹/0.5 s and decreases to 4 kΩ owing to the application of −30 mV nm⁻¹/0.5 s. The simulated curve follows the trends of switching characteristics. (Top) After the heat treatment at 450 °C/1 h, the device does not display any switching behavior due to the annihilation of oxygen vacancies. c) s‐SNOM second‐harmonic amplitude images taken at laser wavelength of λ = 10.5 μm of NiOx samples prepared in 2% oxygen environment and annealed at different temperatures (as prepared, 350 °C, 400 °C, and 450 °C). d) Oxygen peaks in core level measured by XPS for as‐prepared to 450 °C‐annealed NiOx films, respectively. The oxygen peaks fit by three distinct components corresponding to lattice oxygen (OL) are cyan, oxygen vacancies (OV) violet, and hydroxide (OOH) yellow. e) Stoichiometry of NiOx, where x denotes the ratio of oxygen to nickel. f) Synchrotron X‐ray diffraction of NiOx (111) peaks after annealing. Lattice constant expansion of ≈0.19% is observed for AP NiOx over 450 °C NiOx film. g) Ex situ XANES‐measured spectrum for AP NiOx and after annealing. The weight of the O K‐edge peaks reduces (arrow direction) for AP NiOx, indicating a decrease of unoccupied state in O 2p orbital with higher oxygen vacancies. (inset) Zoomed peak intensity variation. h) Normalized Ni K‐edge XANES spectra of AP NiOx and 450 °C NiOx with pre‐edge features in zoomed view (inset).
Proof‐of‐concept learning with NiOx device arrays and implementation of homeostatic regulation. a) The light intensity of letter “P” has been controlled by 6 × 8 of NiOx devices corresponding to change in resistance with respect to the training cycle. b) The training has been performed by applying 50 training pulses amplitude E1 = 5 mV nm⁻¹ and width 500 ms (Video S1, Supporting Information). The delay between training pulses was kept constant to 8 s. c) A systematic change in light intensity is recorded with respect to time demonstrating the occurrence of habituation. The intensity was scaled with respect to the first training cycle. d) Sensitization measurement has been performed by applying a similar number of training pulses of amplitude E1 = 30 mV nm⁻¹ and width 500 ms. The intensity of “P” increases due to the continuous training process after the initial decrease of intensity (Video S2, Supporting Information). Here, the intensity is scaled into tenth training pulse. e) Systematic change in intensity at different training cycles has been recorded. (insets) Change in resistance for X–Y after every training cycle for habituation and sensitization respectively. f) Effect of neuronal adaptive decay realizing homeostasis on a toy network. Without adaptively changing the decay rate (no homeostasis), only a few neurons fire and dominate. In contrast, adaptive decay functionality in the neuronal devices provides an alternate pathway to enable homeostasis in the network, thereby allowing all neurons to competitively learn. g) The network architecture consisting of an input layer of size equal to the dimensionality of the MNIST training images, an excitatory layer of 225 LIF neurons with adaptive decay, and an inhibitory neuron layer for implementing lateral inhibition. h) The final weight patterns after training over the 60 000 training images. The network achieves an accuracy of 84.8% over the test set of 10 000 images.
All‐Electric Nonassociative Learning in Nickel Oxide

September 2022

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106 Reads

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23 Citations

Advanced Intelligent Systems

Advanced Intelligent Systems

Habituation and sensitization represent nonassociative learning mechanisms in both non‐neural and neural organisms. They are essential for a range of functions from survival to adaptation in dynamic environments. Design of hardware for neuroinspired computing strives to emulate such features driven by electric bias and can also be incorporated into neural network algorithms. Herein, cellular‐like learning in oxygen‐deficient NiOx devices is demonstrated. Both habituation learning and sensitization response can be achieved in a single device by simply controlling the magnitude of the electric field. Spontaneous memory relaxations and dynamic redistribution of oxygen vacancies under electric bias enable such learning behavior of NiOx under sequential training. These characteristics in simple device arrays are implemented to learn alphabets as well as demonstrate simulated algorithmic use cases in digit recognition. Transition metal oxides with carefully prepared defect concentrations can be highly sensitive to electronic structure perturbations under moderate electrical stimulus and serve as building blocks for next‐generation neuroinspired computing hardware. Habituation and sensitization are fundamental forms of learning found in various organisms. Herein, experimental demonstration of all‐electric room‐temperature habituation and sensitization within a single device is presented. The learning behavior demonstrated in a simple two‐terminal crossbar‐type NiO device is readily implementable in resistive random access memory arrays.


Citations (7)


... where, G 0 is the mapped conductance for when the weight is "1". The synapses can be implemented by any memristive technology, including phase change devices, [45,46] spintronic devices, [19] ferroelectric devices, [6,47] among others. Note, the focus of this article is on neurons and compliments works on these synaptic devices. ...

Reference:

Hardware in Loop Learning with Spin Stochastic Neurons
Hybrid stochastic synapses enabled by scaled ferroelectric field-effect transistors
  • Citing Article
  • March 2023

Applied Physics Letters

... Avalanche resistive switching is the fundamental process that triggers the sudden change of the electrical properties in solid-state devices under the action of intense electric fields [1]. Despite its relevance for information processing, ultrafast electronics, neuromorphic devices, resistive memories and brain-inspired computation [1][2][3][4][5][6][7][8][9][10][11][12][13][14], the nature of the local stochastic fluctuations that drive the formation of metallic regions within the insulating state has remained hidden. ...

Selective area doping for Mott neuromorphic electronics

Science Advances

... When proteinoids are subjected to the same stimuli over and over again, a sort of learning known as 'non-associative' learning takes place [21][22][23]. A proteinoid might, for instance, be programmed to lower its resistance in response to particular sounds or frequencies. ...

All‐Electric Nonassociative Learning in Nickel Oxide
Advanced Intelligent Systems

Advanced Intelligent Systems

... There are now several excellent reviews on the importance of ionic defects in oxide materials for device applications such as memristors and neuromorphic computing, and we point to those for further information. [32][33][34][35] We also briefly discuss methods of characterization, with particular attention toward x-ray probes of epitaxial ionotronic materials, and conclude with an outlook. ...

Complex Oxides for Brain‐Inspired Computing: A Review
Advanced Materials

Advanced Materials

... 14,17,18), and the temporal dynamics of the built-in capacitor (defined by the memristor electrodes). It is known that such Mott neurons are highly sensitive to their thermal environment 22,23 and can be manipulated by applying external heat (for example, via a micrometre-scale heater) [24][25][26] . Informed by the foregoing aspects of the thermal behaviour, we uncover a previously unexplored degree of freedom within a single device; dynamical thermal interactions with the substrate. ...

Switching Dynamics in Vanadium Dioxide-Based Stochastic Thermal Neurons
  • Citing Article
  • June 2022

IEEE Transactions on Electron Devices

... For example, the hybrid of the ionic gate with 2D materials enables the modulation of the phase transition 6-8 and band structures [9][10][11] in 2D materials due to the strong gate control ability of the ionic gate. Furthermore, the extrinsic ionic states can be introduced into 2D materials through the pre-treatment, such as the intercalation of external ions 4,12 and plasma treatment 5,13 . Subsequently, employing an electric field to control the migration of ions allows for emulating the function of biological neurons and synapses, showing the vast potential in the field of neuromorphic computing 4,5,13 . ...

Reconfigurable perovskite nickelate electronics for artificial intelligence
  • Citing Article
  • February 2022

Science

... One of the traditional mechanisms of training SNNs is through spike-timing-dependent plasticity (STDP) where the model weights are updated locally based on firing patterns of connecting neurons inspired by biological measurements [9]. STDP based learning rules have been lucrative for the neuromorphic hardware community where various emerging nanoelectronic devices have been demonstrated to mimic STDP based learning rules through their intrinsic physics, thereby leading to compact and resource-efficient on-chip learning platforms [10]. Recent works have also demonstrated that unsupervised STDP can serve as an energy-efficient hardware alternative to conventional clustering algorithms [11]. ...

Intrinsic synaptic plasticity of ferroelectric field effect transistors for online learning
  • Citing Article
  • September 2021

Applied Physics Letters