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Artificial spin ice (ASI) structures, consisting of arrays of interacting, single domain nanomagnets (NMs) are promising model systems to explore microscopic features of geometrical frustration [1]. While the structural geometry is responsible for tuning the shape anisotropy and the configurational anisotropy of the system, the strength of dipolar coupling can be modified by the film thickness. In the present work, we achieved magnetic tunability for Ni80Fe20 (Py) ASI structures by three distinct methods namely, the geometrical arrangements of the nanomagnets, the variation in film thickness (20 nm, 30 nm and 50 nm) for each geometry and the applied field orientation [2]. The different ASI geometries such as square spin ice (SSI), kagome spin ice (KSI) and comparatively newer triangular spin ice (TSI) structures are shown in Fig. 1 (a), (b) and (c) respectively. The corresponding hysteresis loops in Fig. 1 (d) depict a marked difference in magnetization reversal mechanism with the variation in film thickness which indicates a possible transition from single domain nanostructure to the formation of vortex states with increasing thickness. The ferromagnetic resonance (FMR) spectra, shown in Fig. 2 explain the dependence of various spin wave modes and their spatial localization on the structural symmetry, film thickness and applied field (Happ) orientation. Micromagnetic simulations are in good agreement with the experimental data and shows the space-frequency resolved localization of the spin wave modes. The results show a great potential towards designing reconfigurable magnonic crystals for microwave filter applications.References: [1] R. F. Wang, C. Nisoli, R. S. Freitas, J. Li, W. McConville, B. J. Cooley, M. S. Lund, N. Samarth, C. Leighton, V. H. Crespi and P. Schiffer, Nature 439, 303-306 (2006). [2] A. Talapatra, N. Singh and A. O. Adeyeye, Physical Review Applied 13, 014034 (2020).

MMM 2020

Magnetic Tunability of Permalloy Artificial Spin Ice Structures

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Magnetic materials are already widely used for long-term data storage, but ongoing work seeks to use them as both working memory and computing architectures. Particularly, devices based on magnetic domain walls (DWs) can perform logic operations and can readily store information [1]. However, the stochasticity of DW pinning limits the feasibility of creating technologically viable devices. Here, we demonstrate how stochasticity can be changed from a technologically inhibitive behaviour into an integral property of machine learning algorithms for specialised neuromorphic devices. We first present experimental measurements that demonstrate the tunability of stochastic processes by applying external stimuli. Focused magneto-optic Kerr effect measurements were used to probe the pinning of DWs at notch-shaped defect sites in 400 nm wide Permalloy nanowires (Fig. 1). DWs were injected into the nanowires and propagated to the defect sites using a field parallel to the nanowire (Hx). The probability of the DWs being pinned at the defect sites was found to depend sigmoidally on the magnitude of a field transverse to the nanowires (Hy). The stochastic behaviour of the nanowire were then integrated into machine learning models. We have developed feedforward neural networks with the nanowires acted as binary stochastic synapses (BSS) that can be sampled by repeating the network. It is found that for a single cycle of the network it can be trained to recognise handwritten digits with an error rate of 19%. Repeated sampling of the network decreases the error rate to 9% for 128 cycles - close to mean field performance (Fig. 2). Adding a hidden layer improves performance with extra pathways for the stochastic behaviour to be averaged over. Our work illustrates how the stochasticity of DW devices can be harnessed to provide tunable bespoke hardware for machine learning tasks.References: [1] R. L. Stamps et al., J. Phys. D. Appl. Phys. Vol. 47, p. 333001 (2014)

Harnessing Stochastic Domain Wall Pinning for Machine Learning

Lateral inhibition (LI) is an important neuromorphic network functionality, modeled after the biological neuron behavior that a firing neuron deactivates its neighbors and prevents their firing. In most neuromorphic hardware platforms LI is implemented by external circuitry, thereby decreasing the energy efficiency and increasing the area overhead. Recently, the domain wall – magnetic tunnel junction (DW-MTJ) neuron is shown in modeling to be intrinsically inhibitory1. LI in DW-MTJ neurons results from magnetostatic interaction between adjacent neurons (Fig.1): the two DWs, DWN and DWI, are driven by electrical current of densities JeI<JeN, so that the DW velocities vDWI<vDWN and the active Neuron N fires first. DWI falls behind DWN and is subjected to the stray field of Neuron N in the −z direction. It is demonstrated that such stray field can decrease DWI velocity and prevent Neuron I from firing, thus emulating LI. However, the LI mechanism in DW-MTJ neurons has not been studied thoroughly, leading to weak inhibition only in very closely spaced devices. In our work2 we model the current- and field-driven DW motion in two adjacent DW-MTJ neurons to approach these problems. LI is maximized by an optimal magnetic interaction strength, determined by tuning the spacing between the two neurons (Fig.2). The results are explained by the current- and field-driven DW velocity characteristics and are quantified by an analytical model. We further study the influence of device parameters and demonstrate the LI behavior in an array of 1000 neurons, which renders our proposed DW-MTJ array promising for implementing a k-winner-take-all layer. With strong LI achieved, a path towards competitive learning algorithms are made possible on the DW-MTJ neurons. This work is funded by Sandia National Lab. Sandia National Lab (SNL) is managed and operated by NTESS under DOE NNSA contract DE-NA0003525References: 1. N. Hassan et al. Journal of Applied Physics, Vol.124, p.152127 (2018) 2. C. Cui et al. Nanotechnology, Vol.31(29), p.294001 (2020)

Maximized Lateral Inhibition in Paired Magnetic Domain Wall Racetracks for Neuromorphic Computing

Neuromorphic computing attempts to mimic the neurons and synapses in a human brain in order to provide significant improvements in the computation of unstructured, real-world data. In past research, we have proposed three separate leaky integrate-and-fire (LIF) neurons that provide the leaking, integrating, and firing characteristics without the use of any additional circuitry [1]-[3]. These neurons are therefore able to significantly reduce the area and energy overhead of neuromorphic circuits. To increase the biological accuracy of these neurons and to better match the neurons to different neuromorphic schema and algorithms, it is desirable for neuron leaking to implement specific mathematical functions in addition to exhibiting the three basic LIF neuronal functionalities. By varying the shape of the devices, it is possible to implement a variety of leaking characteristics. In this work, we discuss the implementation of linear leaking characteristics. In the neurons of [1]-[3], the leaking DWs accelerate towards the ends of the tracks. To counter this, it is necessary to alter these devices. In fact, by simply introducing slight exponential variations in the sides of the neuron from [3], as in Figure 1, we are capable of constructing neurons with considerably more linear leaking characteristics than those discussed in [1]-[3]. As the exponential variations become more pronounced, the linearity of the neuron’s leaking increases as well. Beyond a certain point, however, continued increases in the curvature causes a regression in the leaking functionality’s linearity. Figure 2 demonstrates the effect of the curvature of the DW track on the device’s leaking functionality, starting with no curvature and progressing to more pronounced curvature.References: [1] N. Hassan, X. Hu, L. Jiang-Wei et al., “Magnetic domain wall neuron with lateral inhibition,” J. Appl. Phys., vol. 124, no. 15, p. 152127, 2018. [2] W. H. Brigner, X. Hu, N. Hassan, et al., “Graded-Anisotropy-Induced Magnetic Domain Wall Drift for an Artificial Spintronic Leaky Integrate-and-Fire Neuron,” IEEE Journal on Exploratory Solid-State Computational Devices and Circuits, vol. 5, no. 1, pp. 19–24, 2019. [3] W. H. Brigner, N. Hassan, L. Jiang-Wei, et al., “Shape-Based Magnetic Domain Wall Drift for an Artificial Spintronic Leaky Integrate-and-Fire Neuron,” IEEE Transactions on Electron Devices, vol. 66, no. 11, pp. 4970-4975, 2019.

Linear Intrinsic Leaking in a Domain-Wall Magnetic Tunnel Junction Neuron

The relaxation kinetics and emerging correlations of arrays of interacting Ising-like nanomagnets are governed by the switching rates of the individual magnets. These rates depend, via the Arrhenius law, on the energy barrier for moment reversal in the nanomagnets. In this work, we consider how the switching behaviour of a nanomagnet in archetypical artificial square ice is modified by the interaction with its six nearest neighbours. We find that due to two effects the transition barriers can be significantly lowered compared to an approximation commonly used for kinetic Monte Carlo simulations: (1) Based on a simplified point-dipole model, we find that the barriers for clockwise and counter-clockwise uniform rotation can differ significantly due to the interactions with neighbours. For a subset of environmental microstates this leads to a significant enhancement of the switching rate, which is especially marked in the limit of rare events. (2) Micromagnetic simulations employing the string method to model the moment reversal in an extended nanomagnets reveal that, in addition to the clockwise/counter-clockwise splitting, the environments promote non-uniform reversal leading to further reductions of the switching barriers. These results highlight that local microstates can significantly enhance moment reversals already in ideal systems, without defects or additional anisotropies, and are particularly pronounced for fully-magnetised configurations. Thus, we expect that the initial stages of demagnetisation will proceed faster than assumed from previous models. These findings are of integral importance to achieve realistic kinetic Monte Carlo simulations of emergent correlations in extended artificial spin systems or the evolution of small-scale nanomagnetic logic circuits.

Switching barriers in artificial square ice

The dynamics involving directed separation of a monopole-antimonopole pair in two- or three-dimensional spin ices is conventionally defined as magnetic current or magnetricity. While the feasibility of magnetricity in artificial spin ices has been shown theoretically and experimentally [1,2], the controllability of magnetic currents is still under debate. Particularly, it has been theoretically shown that maximization of Dirac string’s tension is a necessary condition for stabilization of directed magnetic currents [1]. Experimentally, however, magnetic currents are often of only short duration, because magnetic monopoles created at one sample edge do not reach the other sample edge, but rather stick in the middle of the sample. Here, we explore theoretically the role of the termination of arrays and the higher order magnetic interactions for the directionality of magnetic currents in two-dimensional artificial spin-ice. Our Monte-Carlo calculations show that arrays of point dipoles and identical array with realistic multipole moments give qualitatively similar results with respect to the end states and with respect to the averaged propagation of the monopoles. However, the Monte-Carlo calculations using the higher order contributions reflect much better formation of domains with phase shifted Dirac strings, found in recent experiments [3]. Our calculations permit us to elaborate a phase diagram predicting the probability of directed propagation of monopole current as a function of termination type of a realistic artificial spin-ice array.References: [1] E. Y. Vedmedenko, Dynamics of Bound Monopoles in Artificial Spin Ice: How to Store Energy in Dirac Strings. Physical Review Letters 116, 077202 (2016). [2] A. Farhan et al., Direct Observation of Thermal Relaxation in Artificial Spin Ice. Phys. Rev. Lett. 111, 057204 (2013). [3] A. Hanu, E. Y. Vedmedenko, J. Cuia, J. Vijayakumard, A. Kleibertd, L.J. Heyderman, Control of emergent magnetic monopole currents in artificial spin ice, submitted.

Role of Higher-Order Magnetostatic Interactions for the Directional Injection of Monopole Currents

1D and 2D arrays of coupled magnetic nanoislands, also known as mesospins, have recently attracted much attention for offering the possibility to mimic exotic physical systems [1]. In analyzing these coupled mesospin arrays, the individual building blocks are often assumed to consist of simple dipoles, where any inner structure is ignored. Such an approximation of a mesospin however, leads to discrepancies when temperature becomes an important parameter [2]. Temperature excites thermal magnons in a ferromagnet, which is the basis for temperature dependence of the magnetization as expressed by the Bloch law. Here, we present a framework for studying temperature induced magnetization fluctuations in terms of magnonic excitations. We use MuMax3 to numerically subject a single stadium shaped mesospin (450 nm x 150 nm x 5 nm) to a highly inhomogeneous stochastic thermal field [3], and study the emerging spectrum by Fourier transforming the magnetization. The length, width and thickness of the mesospin element are varied to study the resulting effect of size variation on the spectra. The spectra are found to be gapped, and the spectral peaks pertain to specific edge- and center oscillation modes. Finally, we study the effect of temperature variation and we find that the magnon density of states plays an important role on the overall shape of the spectra. The results of this study are not only useful from the perspective of thermal switching of nanoislands, but also for the design of magnonic crystals based on mesospins.References: 1. S. H. Skjærvø, et al., Nature Reviews Physics, Vol. 2, p. 13–28 (2020) 2. M. Pohlit, G. Muscas, I. A. Chioar, et al., Physical Review B, Vol. 101, p. 134404 (2020) 3. J. Leliaert, J. Mulkers, J. De Clercq, et al., AIP Advances, Vol. 7, p. 125010 (2017)

A Magnon Approach to Thermal Fluctuations in Ising-like Mesospins

The extent of magnetic ordering in highly-frustrated thermally-active artificial kagome spin ice is limited by the lowest achievable blocking temperature, as the moments freeze in before ordering is achieved [1]. A more substantial degree of magnetic ordering can be achieved by lowering the blocking temperature of the individual nanomagnets or by increasing the critical transition temperature for the system. We pursue an original approach of introducing interfacial Dzyaloshinskii-Moriya interactions, which lowers the blocking temperature while keeping the transition temperature unchanged [2]. Using this approach, we demonstrate that a seven-ring kagome structure consisting of 30 nanomagnets can be thermally annealed into its ground state. Furthermore, the spin-ice correlations extracted from extended kagome lattices are found to exhibit the quantitative signatures of long-range charge-order, thereby giving experimental evidence for the theoretically predicted continuous transition to a charge-ordered state. We also find that slight modifications of the nanomagnets at a vertex in the artificial kagome ice lead to an increase in the critical temperatures, and allow us to control the energy landscape. Our results provide the foundations for the tuning of magnetic ordering in several different artificial spin systems.References: [1] S.H. Skjærvø, C.H. Marrows, R.L. Stamps, L.J. Heyderman. “Advances in artificial spin ice.” Nature Reviews Physics 2, 13-28 (2020). [2] K. Hofhuis et al., under review.

Long-range Magnetic Ordering in Artificial Kagome Spin Ice

Artificial spin ices (ASIs) are lithographically patterned arrays of single domain magnetic nanoislands where the dipolar interactions between these Ising-like macrospins have served as the basis for investigating phenomena such as geometric frustration and emergent magnetic monopoles [1]. While the majority of ASI studies have utilized nanoislands composed of soft magnetic metals (e.g. permalloy), the use of complex oxides, such as La0.7Sr0.3MnO3 (LSMO), could permit room temperature studies of thermally-active ASIs (TC ~ 360 K) and serve as a platform for coupling the rich physics of both complex oxide heterostructures and ASI structures. In this work, we utilize x-ray photoemission electron microscopy (X-PEEM) to image LSMO-based brickwork ASI structures where a breakdown of the Ising model of individual nanoislands occurs at a critical coupling strength which balances intra- and inter-island magnetic interactions. For ASI structures with nanoislands of identical dimensions, the ASI lattice parameter controls the inter-island coupling strength, resulting in systems composed solely of single-domain magnetic nanoislands, or a mixture of single-domain and complex spin textures (CST, i.e. single and double vortex states). Analysis of magnetic ordering in X-PEEM images reveals that nucleation of CST in frustrated nanoislands is accompanied by a disruption in long-range ordering. While it is generally assumed that inter-island interactions in ASI systems only influence the ordering of the nanomagnetic ensemble, in this LSMO-based ASI system inter-island coupling can dictate both the spin texture within individual nanoislands and long-range magnetic ordering. These results suggest the potential to create tunable nanoisland domain states, providing a new direction in developing ASI systems with exotic phase transitions as well as novel nanomagnetic logic architectures.References: 1. Skjærvø, S.H., et al., Nature Reviews Physics., Vol. 2, p.13 (2020)

The Formation of Complex Spin Textures in La0.7Sr0.3MnO3 Artificial Spin Ice Arrays

The magnetic behaviour of ferromagnetic antidot thin films can be tuned by engineering their geometry, such as the hole diameter, inter-hole distance and film thickness [1,2]. Although antidot patterned nanostructures are grown by template-assisted methods mostly using lithographical techniques [1,2], the use of anodic alumina templates has also been checked successfully [3]. However, this latter alternative shows some challenging aspects for the patterning of large areas with sufficiently high ordering and/or complex antidot geometries. These limitations are partly overcome by performing a mechanical nanoimprinting process before a single anodization process [4-6]. This work introduces an easy and less-expensive route to synthesize highly ordered nanoporous alumina templates in large areas and subsequently magnetic antidot arrays with different and complex geometries. The procedure is based on large-scale nanoimprint using patterned commercial disks as a 1-D grating stamp (e.g., CD, DVD and BR disks) followed by single anodization process which allows obtaining 1-D anodic alumina templates (Figure 1a). In addition, complex 2-D patterned nanoporous alumina templates, with square or triangular ordering (Figures 1b and c), were generated using the 1-D grating stamp by multiple imprinting steps at different angles. Afterwards, Co antidot thin films were sputtered onto these templates with different thickness (from 20 to 100 nm) and symmetries. Magnetic studies confirm the presence of in-plane anisotropy with easy axis parallel to the nanostripes in Co antidot films, while a modest in-plane bi-axial magnetic anisotropy with perpendicular magnetization easy axes is concluded in Co squared nanodot arrays. In summary, a non-expensive methodology, combining soft-imprint and single anodization, is introduced for massive mould production and complex pattern generation, avoiding standard lithographical techniques. The magnetic response of the final sputtered antidot films can be engineered by the appropriate nanoimprinted processes.References: 1. R. P. Cowburn, A. O. Adeyeye, and J. A. C. Bland, Appl. Phys. Lett. 70, 2309 (1997). 2. N. G. Deshpande, M. S. Seo, X. R. Jin, S. J. Lee, Y. P. Lee, J. Y. Rhee and K. W. Kim, Appl. Phys. Lett. 96, 122503 (2010). 3. K. J. Merazzo, C. Castán-Guerrero, J. Herrero-Albillos, F. Kronast, F. Bartolomé, J. Sesé, R.P. Del Real, L. M. García and M. Vázquez, Phys. Rev. B. 85, 184427 (2012). 4. W. Lee, R. Ji, C. A. Ross, U. Gosele and K. Nielsch, Small, 2, 978 (2006). 5. J. Choi, R.B. Wehrspohn, and A. Gösele, Adv. Mater., 15, 1531 (2003). 6. J. Um, M. R. Z. Kouhpanji, S. Liu, Z. N. Porshokouh, S.-Y. Sung, J. Kosel and B. Stadler, IEEE Trans. Magn. 56, 6701006 (2020).

Ferromagnetic antidot arrays with complex geometries

Novel computational paradigms in combination with proper hardware solutions are required to overcome the limitations of our state-of-the-art computer technology, in particular regarding energy consumption. Due to the inherent complex and non-linear nature, spintronics offers the possibility towards energy-efficient, non-volatile hardware solutions for various unconventional computing schemes.[1-3] In this talk, I will address the potential of topologically stabilized magnetic whirls – so-called skyrmions – for in particular two unconventional computing schemes – reservoir computing and stochastic computing. Reservoir computing is a computational scheme that allows to drastically simplify spatial-temporal recognition tasks. We have shown that random skyrmion fabrics provide a suitable physical implementation of the reservoir [4,5] and allow to classify patterns via their complex resistance responses either by tracing the signal over time or by a single spatially resolved measurement. [6] Stochastic computing is a computational paradigm that allows to speed up a calculation while trading for numerical precision. Information is encoded in terms of bit-streams as a probability. A key requirement and simultaneously a challenge is that the incoming bitstreams are uncorrelated. The Brownian motion of magnetic skyrmions allows creating a device that reshuffles the bit-streams. [7,8]References: [1] J. Grollier, D. Querlioz, K. Y. Camsari, KES, S. Fukami, M. D. Stiles, Nature Electronics (2020) [2] E. Vedmedenko, R. Kawakami, D. Sheka, ..., KES, et al., J. of Phys. D (2020) [3] G. Finocchio, M. Di Ventra, K.Y. Camsari, KES, P. K. Amiri and Z. Zeng, arXiv:1907.04601 [4] D. Prychynenko, M. Sitte, et al, KES, Phys. Rev. Appl. 9, 014034 (2018) [5] G. Bourianoff, D. Pinna, M. Sitte and KES, AIP Adv. 8, 055602 (2018) [6] D. Pinna, G. Bourianoff and KES, arXiv:1811.12623 [7] D. Pinna, F. Abreu Araujo, J.-V. Kim, et al, Phys. Rev. Appl. 9, 064018 (2018) [8] J. Zazvorka, F. Jakobs, D. Heinze, ..., KES, et al., Nat. Nanotech. 14, 658 (2019)

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