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Materials Challenges for Memory

Industry challenges and outlook for resistive memories


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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.

technical paper

Resistive +PCM

Spin-transfer-torque MRAM

Oxide perovskites have received widespread attention ever since their discovery due to the multiple physical properties they exhibit, including ferroelectricity, multiferroicity, and superconductivity. One prominent absence in this list of properties that oxide perovskites exhibit is electronic topological order. This is a consequence of the large band gaps of oxide perovskites, which make the band inversions necessary for topology impossible. Alternatively, we find that topological phonons – nodal rings, nodal lines, and Weyl points – are ubiquitous in oxide perovskites in terms of structures (tetragonal, orthorhombic, and rhombohedral), compounds (BaTiO3, PbTiO3, and SrTiO3), and external conditions (photoexcitation, strain, and temperature). In particular, in the tetragonal phase of these compounds all types of topological phonons can simultaneously emerge when stabilized by photoexcitation, whereas the tetragonal phase stabilized by thermal fluctuations only hosts a more limited set of topological phonon states. In addition, we find that the photoexcited carrier density can be used to control the emergent topological states, for example driving the creation/annihilation of Weyl points and switching between nodal lines and nodal rings. Overall, we propose oxide perovskites as a versatile platform in which to study topological phonons and their manipulation with light [1]. Topological phonons in oxide perovskites provide a promising platform to study physical phenomena, ranging from the phonon Hall effect to superconductivity, and may also offer new technological opportunities such as the realization of controllable topological quantum states for neuromorphic computing.

Reference:
[1] Bo Peng, Yuchen Hu, Shuichi Murakami, Tiantian Zhang, Bartomeu Monserrat. Topological phonons in oxide perovskites controlled by light. Science Advances 6 (46), eabd1618 (2020).

Topological phonons in oxide perovskites controlled by light

Magneto-ionics, understood as voltage-driven ion transport in magnetic materials, could represent a significant breakthrough in the search for routes to enhance energy efficiency in magnetically-actuated devices. Particularly, magneto-ionics in Co3O4 allows for voltage-controlled ON−OFF ferromagnetism, since Co3O4 (paramagnetic) can be partially reduced to Co (ferromagnetic) by voltage actuation and reversed by applying a voltage of opposite polarity [1]. This could be used to binary encode information: for example, OFF = 0 (paramagnetism) and ON = 1 (ferromagnetism). However, ion motion at room temperature is still too slow for applications. The way to apply electric field (voltage actuation) can have a strong impact on the room temperature magneto-ionic motion. Specifically, in electrolyte-gated paramagnetic Co3O4 films, the oxygen magneto-ionic motion can be increased by more than one order of magnitude by applying the electric field through an electrochemical capacitor configuration (i.e., using, as working electrode, an underlying conducting buffer layer beneath the Co3O4 film) rather than using an electric-double-layer transistor-like configuration (i.e., placing the electric contact at one side of the Co3O4 film as working electrode). This is due to a greater uniformity and strength of the electric field in the capacitor design [1,2].

[1] A. Quintana, E. Menéndez, M. O. Liedke, M. Butterling, A. Wagner, V. Sireus, P. Torruella, S. Estradé, F. Peiró, J. Dendooven, C. Detavernier, P. D. Murray, D. A. Gilbert, K. Liu, E. Pellicer, J. Nogues and J. Sort, Voltage-controlled ON−OFF ferromagnetism at room temperature in a single metal oxide film, ACS Nano 12 (2018) 10291–10300
[2] J. de Rojas, A. Quintana, A. Lopeandía, J. Salguero, J. L. Costa-Krämer, L. Abad, M. O. Liedke, M. Butterling, A. Wagner, L. Henderick, J. Dendooven, C. Detavernier, J. Sort and E. Menéndez, Boosting room-temperature magneto-ionics in a non-magnetic oxide semiconductor, Advanced Functional Materials 30 (2020) 2003704

ON-OFF magneto-ionics in Co3O4

Voltage-controlled magnetism (VCM) utilizes an applied electric field to modulate magnetic properties in a material instead of current, potentially representing a sizable increase in energy savings in next-generation technology and devices. However, VCM still faces several difficult challenges: a scarcity of room-temperature multiferroics, mechanical fatigue and failure in strain-mediated piezoelectric/magnetostrictive devices, and thickness limitations in charged metallic films. Voltage-driven ionic motion (magneto-ionics) presents an alternative which does not suffer from many of these drawbacks, although translating magneto-ionics into real world devices requires significant improvements in magneto-ionic rates, cyclability, and changes in magnetization. Here, we report on room-temperature voltage-driven nitrogen magneto-ionics (via N transport) by electrolyte-gating of a CoN film using a propylene carbonate liquid electrolyte[1]. Nanocrystalline (face-centered cubic structure) CoN and Co3O4 films biased using an electrochemical capacitor configuration are compared. Both materials show reversible voltage-driven ON-OFF ferromagnetism, albeit with CoN displaying a remarkable 6-fold advantage in magneto-ionic rate. Nitrogen transport in CoN is found to occur uniformly throughout the film, creating a plane-wave-like migration front, without assistance of diffusion channels, in sharp contrast with oxygen transport in Co3O4, where ion diffusion is more inhomogeneous and preferentially occurs along grain boundaries. Nitrogen magneto-ionics in CoN is also shown to require lower onset voltages than oxygen magneto-ionics, as well as enhanced rates and cyclability due to the combination of a lower energy barrier for ion diffusion (and, hence, minimum applied voltage) and the lower electronegativity of nitrogen with respect to oxygen, consistent with ab initio calculations of N vs. O ion motion in a cobalt lattice. These promising results suggest nitrogen magneto-ionics can be tantalizing alternative for efficient voltage-driven effects and, alongside oxygen magneto-ionics, may enable the use of magneto-ionics in devices such as brain-inspired/stochastic computing or magnetic micro-electro-mechanical systems.

Nitrogen Magneto-ionics

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.

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

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

Layered magnetic semiconductors are a key resource for next-generation spintronic logic and memory applications [1]. The recent advances in growing 2D magnetic materials provide ease of thickness control, atomistic mechanical stability, measurable spin-mobility, and a practical approach for spintronic research [2]. Here, we have synthesized 2D chromium sulfide (Cr2S3) using chemical vapor deposition (CVD) on a sapphire substrate and carried out transport measurements under an external magnetic field applied out-of-plane (Figure 1). The microscopy and Raman investigations suggest layered non-van der Waal crystal growth along the c-axis (001) direction. The set of investigations suggest that the 2D-Cr2S3 consists of a layered geometry with magnetic behavior similar to that reported in CrI3 [3] i.e., intra-layer ferromagnetic and inter-layer antiferromagnetic ordering along the stacking (c-axis) direction. The Neil temperature (TN) is noted as ~120 K and small magnetic contributions are evident till room temperature (300 K) as shown in Figures 1d and 2a. 
A four-probe device structure with non-magnetic (Al) electrodes was fabricated using standard semiconductor processing[4] to carry out the transport measurements as shown in Fig. 1c. The voltage across the two inner electrodes was measured in response to a constant current of 10 µA injected into the device. The field-induced magnetoresistance (MRH) was calculated as 〖MR〗_H=(R(H)-R(0))/(R(0)), where R(H) is the resistance measured at an applied magnetic field strength of H in Oe. A large MRH of -25% was observed at 100 K, i.e., near TN. Our study shows the change in MRH magnitude from negative to positive below 20 K as shown in Figure 2a. 
To probe the spin induced magnetoresistance (MR_s=(∆R_s)/R_0 where ∆R_s is the difference in resistance between the positive sweep and the negative sweep of the applied magnetic field, as shown in Figure 2b), the resistance versus a dual sweep (0→5T→0→-5T→0→5T) of the magnetic field (Hext), has been investigated at different temperatures. For TN<T≤300 K, a small negative MRs vs. Hext was noticed. This behavior is characteristic of a disordered magnetic state, typically attributed to quenching of spin disorder upon applying a Hext [5]. On the other hand, distinct resistance states (0 and 1) are observed with Rs ≅ 3 kΩ when cooled down to 10 K at ±5 kOe and 10 µA (power = 0.2 watts). Here, MRs of 13% is observed, which has not been shown before in thin-film Cr2S3 systems. The large resistance hysteresis also matches the magnetization hysteresis (not shown here) and can be attributed to the large (2-5 x 108) spins/m3, which get flipped above the threshold magnetic field.[6]
In summary, we have successfully demonstrated the magneto-resistive effect in CVD-grown 2D Cr2S3 thin film, which makes Cr-based 2D materials novel among 2D materials. Furthermore, these Cr2S3 with ferrimagnetic and narrow bandgap characteristics provide an excellent platform for next-generation spintronic applications.

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