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The resistive switching (RS) is a physical phenomenon where an insulating material changes its state of resistance from high resistance state (HRS) to low resistance state (LRS) and vice versa with the application of the external electric field. Many materials has been investigated as an active material for the resistive switching based device but still lots of research is still going on in the finding of better one. Among all the existing materials, oxide materials have proven itself a best candidate for the application of the memory-based device due to its robust nature. The oxygen vacancies play a very crucial role in the oxide materials for the initiation of the resistive switching phenomena. ZnO is a semiconducting material having wide bandgap. Various attempts have been reported to improve the ZnO as a switching layer, like stacking of ZnO with different electrodes, changing the deposition parameters, doping with various elements, post thermal treating and by controlling its growth deposition. The presence of interstitial layer also play important role to enhance the RS switching characteristics. Therefore, based on above discussion, a comprehensive study has done in the resistive switching behavior of the Ag/LSMO/ZnO/ITO device to observe the effect of LSMO as an interfacial layer. The device shows bipolar RS switching type behavior with stability in the operating voltages up to 80 cycles of testing. The ION/IOFF ratio is observed around 102. The LSMO can be act as the reservoir for the oxygen vacancies, which attracts oxygen ions from the ZnO to form the conducting filament type structure by the application of positive voltage. Thus, the formation/rupture of the oxygen vacancies based conducting filament structure in the active materials helps to switch the state of resistance. The introduction of oxygen vacancies in the ZnO leads to the shifting of energy states towards the Fermi level and introducing the metallic characteristic in it. From the density functional theory (DFT) calculation, the role of oxygen vacancies is further confirmed and claimed that, it is highly responsible behind the resistive switching behavior of ZnO.

Materials Challenges for Memory

Resistive Switching behavior of ZnO in the presence of La0.7Sr0.3MnO3 as an Interfacial layer

conducting filament

interfacial layer


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The energy cost of storing and moving data is enormous, and is growing at such a rapid pace that within a few years the power demand may overwhelm some developed nations. Non-volatile memory (NVM) and neuromorphic computing are enabling critical advances in this area, but there are many scientific and technological challenges. This conference will cover the materials challenges of different memory technologies, from the fundamental processes and mechanisms, to industry perspectives on materials specifications and manufacturing.

poster

Magnetic nanofibers can be applied for data transport and storage and are highly interesting in basic research. One of the reasons for their broad investigation is that can be produced by electrospinning [1]. Such bent nanofibers, however, show a broad spectrum of possible magnetization reversal processes and magnetization dynamics, dependent on their bending radius and diameter, the magnetic field orientation relative to the fiber axis, etc. [2].
Besides quasistatic processes, dynamic investigations are used to evaluate the possible data transport through such magnetic nanofibers. Here we report on domain wall nucleation and propagation through nanowires with different bending radii, from single nanowires to networks with multiple data inputs and outputs. In these simulations, diverse phenomena occur which have to be taken into account during these dynamic processes, like domain wall instabilities or interference between converging signals, resulting in a spectrum of possible architectures for nanowire-based logics.

[1] C. Döpke, T. Grothe, P. Steblinski, M. Klöcker, L. Sabantina, D. Kosmalska, T. Blachowicz, A. Ehrmann, Magnetic nanofiber mats for data storage and transfer, Nanomaterials 9, 92 (2019).
[2] T. Blachowicz, A. Ehrmann, Magnetization reversal in bent nanofibers of different cross-sections, J. Appl. Phys. 124, 152112 (2018).


Micromagnetic simulation of magnetization dynamics in nanofiber networks

The development of alternative brain-inspired neuromorphic computing architectures is anticipated to play a key role in addressing the strict requirements of the artificial intelligence (AI) era. In order to obtain a high degree of learning accuracy within an artificial neural network (ANN) that operates with the backpropagation algorithm, a highly symmetric synaptic weight distribution is desired. Along these lines, we present here a detailed device engineering approach that enables analog synaptic properties in completely forming free SiO2-conductive bridge memories (CBRAM). This is achieved, by either incorporating a dense layer of Pt nanoparticles (NPs) as a bottom electrode (BE) or by fabricating bilayer structures using a second switching layer of VOx. Interestingly, compared with the reference sample that manifests both threshold and bipolar switching modes, the Pt NCs sample exhibits only the threshold switching pattern whereas the bilayer configuration operates only under the bipolar switching mode as illustrated by direct current (DC) measurements. These characteristics have a direct, while different impact, on the conductance modulation pattern and determine the analog nature of the synaptic weight distribution. 


Enhancing the analog synaptic properties of forming free SiO2 memristors by materials engineering approach

We grew La2NiMnO6 (LNMO) films by radiofrequency off-axis magnetron sputtering on a variety of oxide perovskite substrates. Structural characterization indicates high crystalline quality, absence of parasitic defects and rock-salt ordering of the NiO 6 and MnO 6 octahedra with only minimal degree of antisite disorder. 
X-ray absorption spectroscopy (XAS) and confirms the stabilization of Ni 2+ and Mn 4+ valence states. When lowering the thickness of LNMO films grown on SrTiO 3 (STO) we observe a degradation of the ferromagnetic properties that is accompanied by an increase of antisite disorder at the interface between LNMO and STO. Moreover, the polarity mismatch between the film and the substrate triggers an electronic reconstruction that results in additional Mn 3+ states at the LNMO//STO interface.
Despite this occurrence, films as thin as 2 pseudocubic unit cells (0.8 nm) are still ferromagnetic, as verified by x-ray magnetic circular dichroism (XMCD). Capping the LNMO films with a LaNiO 3 layer results in the disappearing of the Mn 3+ content that is supplemented by a restoration of the Curie temperature. 
Considering the scarcity of ferromagnetic insulators, LNMO shows great potential to become a significant element for both fundamental research and promising spintronic applications.

Electronic reconstruction in ferromagnetic insulating double perovskite heterointerfaces

We report a novel delayed-electroforming process in Metal-Insulator-Metal Au/Ti/SiOx/Mo ReRAM devices; this new process allows more energy-efficient switching. For this novel process to occur, a highly resistive pristine device must be stressed under a fixed high voltage for a varying amount of time. The stress time of a device is determined by the amount of charge going through the oxide during stressing. Once a fixed amount of charge has gone through the device, a small detection voltage of 10mV is applied. The device continues to show high resistance (~MΩ) after stressing, and abruptly reaches a low resistance state (~100Ω) after a delay. We investigated the effect of charge injection during stressing, and found good correlation between charge injected during stressing and the delay time after stressing. Additionally, we found that we can modulate conductance of the formed devices by varying amount of charge injection. Based on these results, we propose a charge assisted electroforming model to explain this novel phenomenon.

A Charge-Assisted Delayed-Electroforming Phenomenon in Silicon Oxide

Logic-in-memory architectures based on resistive random access memory (RRAM) technology and the material implication (IMPLY) logic are a promising solution for the development of energy efficient computing hardware for edge computing applications. However, RRAM devices nonidealities, such as cycle-to-cycle variability and random telegraph noise, and circuit-related issues such as logic state degradation, strongly affect the reliability of these circuits and complicate their design. In this, work we use a physics-based RRAM compact model which reproduces the effect of device nonidealities (i.e., variability, Random Telegraph Noise, self-heating) and that was calibrated on three RRAM technologies from the literature to study the reliability and performance of a conventional and a recently proposed smart IMPLY architectures. Finally, we underline the importance of the physics-based RRAM compact model as a tool for implementing device-circuit co-design strategies.

Device-circuit co-design of logic-in-memory circuits using a physics-based RRAM compact model

Electrospinning can be used to produce nanofibers from magnetic materials, forming a magnetic network which may be applied in neuromorphic computing. Besides the influence of the bending radii on the magnetization reversal in such nanofibers [1], the often occurring beads along the fibers have not yet been investigated in detail. Such beads can be assumed to support domain wall formation due to a reduction of the relative impact of the shape anisotropy, in this way influencing magnetization reversal along the fiber. 
Here, we show results of simulations of magnetization reversal processes in iron, nickel, cobalt and magnetite fibers with a bead in the middle, produced in three typical dimensions gained by electrospinning [2]. Mostly, magnetization reversal occurs via a vortex state, for all materials and dimensions. Only some angular orientations of the external magnetic field result in double-vortex or meander states, usually followed by a vortex state. The simulations emphasize the impact of beads along electrospun magnetic nanofibers, making magnetization reversal highly reliable and thus such structures useful for data storage and transport in neuromorphic computing and other applications.

References
[1] T. Blachowicz, A. Ehrmann, Magnetization reversal in bent nanofibers of different cross-sections, J. Appl. Phys. 124, 152112 (2018).
[2] F. Amini, T. Blachowicz, A. Ehrmann, Systematic study of magnetization reversal in beaded fibers from different magnetic materials, J. Magn. Magn. Mater. 529, 167855 (2021)

Magnetization reversal in nanofibers with beads from different magnetic materials

Real-time tracking of high-speed objects in cognitive tasks is challenging in the present artificial intelligence techniques because the data processing and computation are time consuming, resulting in impeditive time delays. A brain-inspired continuous attractor neural network (CANN) can be used to track fast moving targets, where the time delays are intrinsically compensated if the dynamical synapses in the network have short-term plasticity. Here, we show that synapses with short-term depression can be realized by a magnetic tunnel junction, which perfectly reproduces the dynamics of the synaptic weight in a widely applied mathematical model. Then, these dynamical synapses are incorporated into one-dimensional and two-dimensional CANNs, which are demonstrated to have the ability to predict a moving object via micromagnetic simulations. This portable spintronics-based hardware for neuromorphic computing needs no training and is therefore very promising for the tracking technology of moving targets. [1]
[1] Q. Zheng, X. Zhu, Y. Mi, Z. Yuan, and K. Xia, Physical Review Applied 14, 044060 (2020).

Anticipative Tracking with the Short-Term Synaptic Plasticity of Spintronic Devices

A resistive switching ZnO homojunction diode fabricated with a stack of two dissimilar ZnO thin film shows promising characteristics necessary to address the crosstalk [1] problem in a cross-bar memory array. The device has a characteristic IV-hysteresis loop in forward bias, in conjunction with its pn junction characteristics. In the ac frequency range of 10 Hz to 15 kHz, the area inside the hysteresis loop initially increased, reaching a maximum at 1 kHz, and then decreases with increasing frequency. The maximum in the area of the hysteresis loop corresponds to the accumulation of space charge at the interface. The resistivity of the device was found to vary from 5 kΩ to 100 kΩ in the bias range 0V - 10V and in the range of 106 Ω when reverse biased the ratio of High Resistive State (HRS) to Low Resistive State (LRS) [2] has its maximum (~2.4) at 1 kHz ac signal at 3V.


Addressing crosstalk in cross-bar memory arrays with a resistive switching ZnO homojunction diode

Observing the domain structure of antiferromagnetic materials is notoriously difficult, and in the non-collinear antiferromagnet Mn3NiN eight arrangements of the local magnetic moments are possible in the unit cell. Yet for potential applications in antiferromagnetic spintronics it is essential to prepare known domain structures to control the properties of the devices. We grow Mn3NiN films 50nm thick on STO, pattern the films into Hall bars and cool below TN = 220K into the antiferromagnetic state. We then use a laser to generate a local in-plane heat gradient and detect the voltage generated due to the anomalous Nernst effect (ANE) - a manifestation of the Berry curvature of the material. From the sign of the voltage signal we can distinguish domains 2μm in diameter and can saturate the device to a single state using an applied magnetic field. We also show a form of heat assisted writing - by increasing the laser power and reversing the field we are able to write a domain with opposite sign of the ANE.

Using the anomalous Nernst effect to image domains in non collinear antiferromagnetic Mn3NiN thin films

Wake-up effect is a major issue for ferroelectric HfO2-based memory devices. Here, two TiN/Hf0.5Zr0.5O2/TiN structures deposited by magnetron sputtering on silicon are compared. The maximum remanant polarization is higher than 21µC/cm² for both samples, a strong difference is observed in the electrical behavior. For the mesa sample, the difference between maximal and initial Pr is only 3µC/cm² whereas it is around 14µC/cm² in the non-mesa case. We discuss the root causes of these behaviors in light of structural results. Various applications have been suggested for fluorite-structure ferroelectrics due to their advantages over the conventional perovskite-structure ferroelectrics. In this presentation we will focus on (Hf,Zr)O2 (HZO) thin films deposition for the capacitor of Ferroelectric Random Access Memories (FRAM) in the 1Transitor-1Capacitor (1T-1C) model. (Hf,Zr)O2 thin films are studied to either fully understand the stabilization of the ferroelectric phase (f-phase) or to fit with industrial requirements. Samples are stacks of Si/TiN/Hf0.5Zr0.5O/TiN/Pt. All materials are grown by sputtering at room temperature following by a rapid thermal annealing at 450°C during 30 seconds under N2 atmosphere. The samples are called NM, and M. NM and M refers to two different architectures, respectively non-mesa and mesa structures. The description and size of NM and M samples is given in figure 1 for each sample. We report the fabrication of two samples deposited by magnetron sputtering with excellent performances, quite similar to samples deposited by Atomic Layer Deposition. Pr values are among the highest for samples deposited by sputtering. Although the N-sample and NM-samples show very close Pr values, the two samples show completely different electrical behaviors. During cycling, the increase of Pr value for the NM-sample is more than an order of magnitude higher than the M-sample. It is accompanied by a decrease of the endurance which is two order of magnitude higher for the NM-sample than for the M-sample. As electrical behaviors are not the same, for low stress conditions M-sample has a higher Pr value during cycling whereas for high stress conditions NM-sample has a higher Pr value during cycling. As a matter of fact, it has been proven that maximum Pr values are more sensitive to stress conditions than the structures themselves. The origins of the different electrical behaviors come from the micro-crystalline structures of the two samples, according to GIXRD results. The crystallization takes place during the annealing step. During annealing, M-sample is built with a TiN TE fully covering the HZO layer whereas the TiN covers only partially the HZO layer in case of the NM-sample. It induces different stress states which lead to two different micro-crystalline patterning. The M-sample shows no monoclinic peak, whereas the NM-sample shows many monoclinic orientations. It can explain the huge reduction of the wake-up effect.

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