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Enhancement of ferromagnetic resonance damping due to spin pumping from a ferromagnetic insulator (FI) into adjacent heavy metal (HM) is well-known. The less known phenomenon of a substantial magnetic anisotropy induced in FI at the interface with an HM overlay has not been fully studied. Here, we report a microscopic study of the HF/FI interfacial spin interaction in thin films using scanned ferromagnetic resonance force microscopy (sFMRFM). HM nanostructures, such as 5nm-thick Au pads, are patterned onto 20nm-thick Y3Fe5O12 (YIG) grown on Gd3Ga5O12 substrate using off-axis sputtering technique. Scanning the sFMRFM probe across the boundary separating the bare YIG and YIG/Au bilayer reveals a substantial, 32 Gauss, change of resonance field in the magnetic field out-of-plane geometry. Detailed micromagnetic simulation accurately reproduces the experimental result, demonstrating that a sharp change of uniaxial anisotropy across the boundary induces the observed resonance field shift in YIG/Au. This sharp variation of magnetic anisotropy creates a drastic change of internal field over a short spatial distance, can be highly useful in designing nanoscale spintronic devices. The modification of magnetic properties at the nanoscale is usually achieved by modifying the shape or crystal structure of the FI thin film, such as etching or ion irradiation. Notably, we achieve this modification of magnetic anisotropy by a heavy metal pattern overlayer, thus opening a novel path to fabricate nanoscale magnetic structure with minimal disturbance to the material properties of the FI thin film. Utilizing the ability to vary the magnetic anisotropy in nanometer scale, we propose spintronic devices based on the integration of heavy metal nanostructures on YIG thin films.References: G. Wu, S. P. White, W. T. Ruane Physical Review B, 101(18), 184409. (2020)

MMM 2020

Microscopic Study of Magnetic Anisotropy Modification in Nanoscale Heavy Metal/Ferromagnetic Insulator Heterostructures

The 65th Annual Conference on Magnetism and Magnetic Materials (MMM 2020) was held in a virtual form. The COVID-19 pandemic, with its associated uncertainty about international travel and the ability to gather in large groups, meant that the Steering Committee decided to cancel the face-to-face meeting that had been planned in Palm Beach, Florida November 2-6, 2020.

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technical paper

Recently, the formation of a magnon Bose-Einstein Condensate (BEC) triggered by the rapid cooling of magnonic nano-structures was reported [1]. A rapid decrease in the phonon temperature achieved by the application of DC pulses to a nano-sized YIG/Pt sample leads to a non-equilibrium between the phononic and the magnonic system. This results in a redistribution of magnons to the lowest frequencies of the spectrum. Here we report on the application of such a non-equilibrium, showing the possibiltiy to amplify coherently excited spin waves. The structures under investigation (see Fig. 1) consist of a 34 nm thin and 2 µm broad YIG-waveguide. A 3 µm long area is covered with a 7 nm thin layer of platinum, and an antenna allows for the excitation of a propagating spin-wave packet. The magnetization dynamics is investigated using time-resolved micro-focussed Brillouin light scattering spectroscopy. After the applied DC pulse is switched off, a spin wave pulse excited by the antenna is propagating in the waveguide region below the Pt covered area during rapid cooling. Depending on the time-delay between the DC-pulse and the spin-wave package, an amplification of the propagating spin wave is observed (see Fig. 2). This research does not only show the applicability of the phenomenon of rapid cooling to compensate the intrinsic damping in spintronic devices [2], but also gives insight to new physics, namely the interaction of a prepared coherent state with the rapid cooling induced quantum state of the magnon BEC. This research has been supported by ERC StG 678309 MagnonCircuits, ERC ADG 694709 SuperMagnonics and DFU Grant DU 1427/2-1.References: [1] M. Schneider, T. Brächer, D. Breitbach, et. al., Bose-Einstein Condensation of Quasi-Particles by Rapid Cooling, Nat. Nanotechnol. 15, 457–461 (2020) [2] Q. Wang, M. Kewenig, M. Schneider, et. al., Realization of a nanoscale magnonic directional coupler for all-magnon circuits, arXiv:1905.12353

Amplification of Propagating Spin Waves by Rapid Cooling

Magnonic computing (MC) architectures based on spin waves are increasingly of interest for special-purpose computing applications [1]. MC offers advantages over conventional charge-based computing [2-5], including low power dissipation (magnon propagation does not require charge transfer), and incorporation of phase information in addition to amplitude, reducing the component count needed for certain logic operations [6]. One of the challenges in the realization of most MC concepts is that they require an efficient means for routing magnons in complex networks. In particular, a scalable, nonvolatile, and reconfigurable mechanism to do so is currently lacking [6,7]. Here we address this challenge by utilizing a Néel skyrmion as a programmable scattering center to route magnons. The skyrmion is stabilized by the interfacial Dzyaloshinskii-Moriya Interaction (DMI) and perpendicular magnetic anisotropy (PMA), which itself can be controlled by electric fields via the voltage-controlled magnetic anisotropy (VCMA) effect, making the magnon-skyrmion interaction tunable by voltage. We investigate the interaction of exchange spin waves with wavelength of 26 to 190 nm, with skyrmions having diameters from 9 to 74 nm. Our micromagnetic simulations show that the propagation, scattering angle, and energy transmission of spin waves can be effectively controlled by tuning the ratio of magnon wavelength to the skyrmion diameter, which depends strongly on PMA and DMI. Based on this approach, we propose a new skyrmionic magnon switch (SMS) device, which provides voltage-controlled routing of spin waves in a magnetic wire and can be applied to build basic logic circuits. We simulate the SMS performance using typical material parameters for thin ferromagnetic films supporting skyrmions, and assess the requirements for its experimental realization.References: [1]. Khalili P, Wang K L. IEEE Spectrum, Vol.52(7), p.30-56(2015) [2]. Wang, K.L. and P. Khalili Amiri, SPIN, Vol.02(02), p.1250009(2012) [3]. Khitun, A., D.E. Nikonov, and K.L. Wang, Journal of Applied Physics, Vol.106(12), p.123909(2009) [4]. Dutta, S., et al., Scientific Reports, Vol.5, p.9861(2015) [5]. Cherepov, S., et al., Applied Physics Letters, Vol.104(8), p.082403(2014) [6]. Shabadi, P., et al., SPIN, Vol.02(03), p.1240006(2012) [7]. Vogt, K., et al., Applied Physics Letters, Vol.101(4), p.042410(2012)

Investigation of spin wave - skyrmion interactions for magnonic information processing

The spin Seebeck effect (SSE) is defined as the generation of a pure spin current (Js) when a magnetised material is subjected to a temperature gradient .[1] To detect Js, a thin non-magnetic [NM] layer such as Pt, is deposited on top of the material of interest. This converts Js into an observable thermoelectric voltage (VSSE) by way of the Inverse Spin Hall Effect (ISHE). It is of interest for thermoelectric and spintronic applications where it could be used to harvest electricity, or produce a pure spin current, respectively. The spin Seebeck effect can be phonon or magnon driven, therefore investigating the thermomagnetic voltage VSSE as a function of temperature can enable separation of these contributions – particularly in non-insulating materials such as Fe3O4 which undergoes a semiconductor-insulator phase transition at approximately 120 K.[2],[3] We have developed a measurement of VSSE as a function of temperature using the heat flux method [4][5], which enables accurate measurement of thin film samples. We will show how this technique can be used to investigate subtle changes in the SSE as a function of temperature and correlate this with measurement of the magnon dispersion in single crystal Fe3O4 using time of flight (TOF) inelastic neutron scattering (INS). We find an upper limit of the magnon diffusion length (MDL) of 34 ± 7 nm determined from bulk INS (Figure 1). Corresponding SSE measurements of Fe3O4 thin films as a function of thickness indicate an MDL of 19 ± 2 nm, which does not change significantly between 300 and 50 K.[6] We also find that the low energy magnon modes are steeper than previously reported[7] and broaden with increasing temperature (Figure 2).References: [1] K. Uchida et al., Nature, 455, 778 (2008) [2] A. Caruana et al., Phys. Status Solidi: RRL, 10, 613-617 (2016) [3] E. J. W. Verwey, Nature, 144, 327 (1939) [4] A. Sola et al., Sci. Rep. 7 46752 (2017) [5] G. Venkat et al., arXiv:2003.07925, submitted to Rev. Sci. Instrum. [6] G. Venkat et al., arXiv:2001.03738, accepted to Phys. Rev. Mat. (2020) [7] R. J. McQueeney et al., Phys. Rev. B 73 174409 (2006)

Magnon Diffusion Lengths in Bulk and Thin Film Fe3O4 for Spin Seebeck Applications

The temperature dependence of magnetic properties in thin films are important for understanding the underlying physics and enabling the creation of novel devices. Whilst the temperature dependence of saturation magnetization Ms, exchange stiffness A and anisotropy K have been widely investigated [1, 2, 3], research on the interfacial Dzyaloshinskii–Moriya interaction (DMI) remains limited [4]. The DMI exists in perpendicularly magnetized ultrathin films with interfaces to heavy metals and is critical to the formation of magnetic skyrmions. We present a study of the temperature dependence of DMI in a Ta/Pt/CoFeB/Ru/Pt/CoFeb/Ru/Pt heterostructure hosting skyrmions, based on extensive characterization by bulk magnetometry and x-ray magnetic circular dichroism photoemission electron microscopy (XMCD-PEEM). Ms, anisotropy field Hk, zero-field domain width W and skyrmion radius R are extracted directly from the measurements. Through Ms and Hk, the strength of uniaxial anisotropy Ku is determined. Then, we adapt the bulk Bloch law to the thin film geometry to extract A from the temperature dependence of Ms (Fig. 1). Furthermore, we combine Ms, W, R, Ku and A in the static multilayer domain energy model [5] and the static skyrmion size model [6], where the DMI values are calculated at different temperatures (Fig. 2). We find a large spatial variation of the DMI strength between the one derived by the spatial domains and that at skyrmion sites. Besides, the DMI value shows a linear correlation with A and Ku. The possible physical origins are discussed. Finally, according to our results, we argue that the skyrmion size should remain constant over an extensive temperature range [7].References: [1] Atxitia, U., et al., Phys. Rev. B 82, 134440 (2010) [2] Moreno, R., et al., Phys. Rev. B 94, 104433 (2016) [3] Sato, H., et al., Phys. Rev. B 98, 214428 (2018) [4] Schlotter, Sarah, Parnika Agrawal, and Geoffrey SD Beach, Appl. Phys. Lett. 113, 092402 (2018) [5] Lemesh, Ivan, Felix Büttner, and Geoffrey SD Beach, Phys. Rev. B 95, 174423 (2017) [6] Wang, X. S., H. Y. Yuan, and X. R. Wang, Commun Phys 1, 31 (2018) [7] Zhou, Yifan, et al., Phys. Rev. B 101, 054433 (2020)

Temperature dependence of the Dzyaloshinskii-Moriya interaction in ultrathin films

The magnetic proximity effect (MPE) in nonmagnetic heavy metal/magnetic heterostructures has received much recent attention. The MPE is believed to play a role in the spin Hall magnetoresistance (SMR) and may also be leveraged to control the emerging phenomena associated with topological insulators. Pt is most commonly used due to its vicinity to the Stoner criterion, and its use as a source of spin-orbit torques in spintronic measurements. However, much is still unknown about the properties of the MPE, such as the temperature dependence and the coupling to magnetic layers when multiple magnetic sublattices are present. To explore this, we examined pulsed laser deposited 25 nm thick dysprosium iron garnet (DyIG)/sputtered 10 nm Pt heterostructures using polarized neutron reflectometry (PNR), above (200K) and below (15 K) the magnetic compensation temperature (Tcomp = 190 K)1. Below Tcomp, the Dy3+ sublattice dominates the net moment, and above Tcomp, the net Fe3+ dominates. The MPE magnetization has only small effects on the fit to the data, but the results are consistent with a small Pt moment antiparallel to the net DyIG moment at 15 K, i.e. the Pt moment is parallel to the net Fe3+ moment, whereas at 200 K the Pt magnetization is negligible. The MS obtained from the PNR fits is 605 kA/m at 15 K (literature value = 622 kA/m) and 10 kA/m at 200 K (VSM value = 10 kA/m) 1. The scattering length density profile suggests interdiffusion at the GGG substrate interface over a 2-3 nm region, consistent with previous studies. This is accounted for with a layer of composition intermediate between DyIG and GGG. A dip in density at the DyIG/Pt interface is also present, indicating the presence of surface contamination due to the ex situ Pt deposition, or a translational growth region.References: J.J. Bauer, E.R. Rosenberg, S. Kundu, K.A. Mkhoyan, P. Quarterman, A.J. Grutter, B.J. Kirby, J.A. Borchers, and C.A. Ross, Adv. Electron. Mater., Vol. 6, 1900820 (2020).

Temperature Dependence of the Magnetic Proximity Effect in Magnetic Insulator/Platinum Heterostructures by Polarized Neutron Reflectometry

The magnetic proximity effect (MPE) enhances the exchange interaction of nominally non-ferromagnetic materials overcoming the Stoner limit in close contact to ferromagnetic (FM) materials. The paramagnet Pt is a famous example and gets spin polarized by the MPE in Pt/FM bilayers which is of huge importance when studying spin transport phenomena at interfaces such as for the spin Seebeck effect [1], the spin Hall magnetoresistance [2], or spin-orbit torque effects [3]. However, the exact quantitative values for the induced magnetic moment per Pt atom cannot be determined by standard x-ray magnetic circular dichroism (XMCD) experiments on a single thin-film system due to the depth-insensitivity of the XMCD technique at buried interfaces of the sample. Within this contribution, we present the quantitative determination of the Pt magnetic moment induced by the MPE utilizing x-ray resonant magnetic reflectivity (XRMR) [4-6], a favored synchrotron-based technique for spin-depth profiling. Thus, element selectivity and depth resolution can be combined. A detailed data analysis based on asymmetry ratio fits and mapping the goodness of fit parameter Χ2 (see Fig. 1) [3,7] together with an ab-initio factor (conversion from magnetooptic constant Δβ to Pt magnetic moment) [4] provides quantitative reliable results. The obtained quantitative XRMR values are in very good agreement to vibrating sample magnetometry results [3] and XMCD analyses [8] which take the effective magnetic Pt thickness determined by XRMR into account. Therefore, XRMR is a powerful technique to study spin distributions with depth resolution, element selectively and quantitative reliability.References: [1] P. Bougiatioti et al., Phys. Rev. Lett. 119, 227205 (2017) [2] M. Althammer et al., Phys. Rev. B 87, 224401 (2013) [3] A. Moskaltsova et al., AIP Advances 10, 015154 (2020) [4] T. Kuschel et al., Phys. Rev. Lett. 115, 097401 (2015) [5] C. Klewe et al., Phys. Rev. B 93, 214440 (2016) [6] T. Kuschel et al., IEEE Trans. Magn. 52, 4500104 (2016) [7] J. Krieft et al., J. Phys. D: Appl. Phys. 53, 375004 (2020) [8] D. Graulich et al., in preparation

Quantitative determination of the Pt magnetic moment in proximity to ferromagnetic material

Magnetic materials with perpendicular magnetic anisotropy, such as thin films based on CoFeB alloys, are gaining interest and have accelerated the development of high-density non-volatile memories. The requirement of high memory bandwidth for next-generation computing systems moved the attention to the development of devices that can combine storage and logic capabilities. The High Bandwidth Memory interface for 3D-stacks DRAM chips is just one example. Domain wall-based spintronic devices intrinsically combine both these requirements making them suitable both for non-volatile storage and computation. Among all the proposed logics, perpendicular nanomagnetic logic (pNML) takes advantage of magnetic dipole coupling to propagate and elaborate information. The materials explored in literature for its realization such as Co/Pt and Co/Ni were the technology drivers [1], but for power constraints and depinning fields, novel CoFeB/MgO layers are investigated for low power and high-density computing devices. Ta/CoFeB/MgO ultrathin films show significantly lower coercivities, even with high perpendicular anisotropy (PMA) [2], thus becoming very promising candidates for low power pNML devices. In this paper, we investigate different Ta/CoFeB/MgO stacks at the simulation and experimental level, to show their potential for the next generation of magnetic logic devices. The micromagnetic simulations are used to support the experiments. We focus, first, on the magnetostatic analysis of magnetic islands quantifying the stray field that can be achieved with different layout topologies. Then, at the experimental level, we measure the coercivity of films with different thicknesses, Ms from SQUID measurements to estimate the coupling strength achievable between neighboring magnetic islands and measure the domain wall speed on magnetic nanowires. Our results show that the achieved coupling is strong enough to realize logic computation with magnetic islands, moving a step forward in the direction of low power perpendicularly magnetized logic devices.References: [1] S. Breitkreutz et al., in IEEE Transactions on Magnetics, vol. 49, no. 7, pp. 4464-4467 (2013) [2] T Devolder et al. , Journal of Applied Physics, 113(20):203912, (2013).

Ta/CoFeB/MgO Analysis for Low Power Nanomagnetic Devices

The fluctuation theory of concentration and thermodynamic magnetic phase transitions in chiral helicoidal ferromagnetic binary and quasi-binary alloys with the Dzyaloshinsky-Moriya interaction is being developed. The ground state is described based on the LDA+U+SO approximation with additional allowance for concentration fluctuations associated with the difference in the potentials of intra-atomic Hubbard interaction at the sites. The functional of free energy of electronic and magnetic subsystems with thermodynamic and concentration spin fluctuations is constructed. The equations of magnetic state obtained from the conditions of the saddle point allow us to consider the conditions for the realization of the phases of the helicoidal long-range and short-range orders with right and left magnetic chirality. Solutions of the equations of magnetic state are considered on the example of quasi-binary alloys Fe1-xCoxSi, which are the main prototypes of materials of modern spintronics. h-T diagrams of spin phases arising due to the concentration shift of the chemical potential and concentration magnetic fluctuations with a change in the concentration x were constructed. It was found that, in the concentration range 0.05

Phase transitions induced by concentration and thermodynamic magnetic fluctuations in chiral ferromagnets Fe1-xCoxSi

Magnetic skyrmions are compact spin textures that show remarkably unique, particle-like properties. They are widely regarded as promising candidates for emergent magnetic devices as they are small in size and easily maneuverable [1]. The Dzyaloshinskii-Moriya interaction (DMI) is often critical to the generation and manipulation of skyrmions. However, there has been a fundamental lack of understanding of the microscopic origin of DMI or the mechanisms by which DMI stabilizes skyrmions in magnetic bilayers. Little has been known of the material parameters that determine the value of DMI. This knowledge is critical for rational design of skyrmion-hosting materials and further development of skyrmion technology [2]. Here, we address this knowledge gap and present a model to explain the microscopic origin of DMI in heavy metal/ferromagnet (HM/FM) bilayers. We calculate the DMI values in a series of HM/FM bilayers and explain the trend of DMI values observed [3]. We present a new theoretical model that explains the microscopic origin of DMI in these bilayers. We show that the value of DMI depends on two parameters, namely, interfacial hybridization and orbital contributions of the heavy metal. Using these parameters, we explain the experimentally observed DMI trends. Additionally, we report four new materials systems predicted to demonstrate giant DMI. In HM/FM bilayers, the size and stability of DMI-stabilized-skyrmions is decided by the interplay between the DMI, the exchange constant, the out-of-plane anisotropy and dipolar fields. Due to their giant DMI, our newly discovered materials are promising for hosting small sized skyrmions at room-temperature, enabling ultra-dense, ultra-low power skyrmion devices. Together, our results put forth a new understanding of DMI, discover promising materials and suggest pathways for the controlled generation of skyrmions.References: 1. A. Fert, V. Cros, and J. Sampaio, Nature nanotechnology, Vol. 8, p. 152 (2013) 2. W. Jiang et al., Physics Reports, Vol. 704, p. 1-49 (2017). 3. P. Jadaun, L. F. Register and S. K. Banerjee, npj Computational Materials, Vol. 6, p.88 (2020)

Design of giant DMI and its microscopic origin in magnetic bilayers

Tuning the perpendicular magnetic anisotropy (PMA) in magnetic thin films has been an interest for several decades owing to its potential in magnetic recording applications. For device-level applications, it is preferable to employ a single film layer with PMA instead of a multilayer to evade the complicated fabrication process. Therefore, there is a search for materials exhibiting strong PMA in a single layer. Of the several materials exhibiting PMA, rare-earth transition metal-based Gd-Fe thin films have attracted special attention from both the fundamental and technological viewpoints. Gd-Fe films exhibit tunable magnetic anisotropy that can be tailored by modifying the composition, thickness, ion-irradiation and annealing conditions, etc.[1]. Although substantial work has been carried out in understanding the magnetic anisotropy of these films, studies on magnetic transport are still elusive. In the present study, we have grown 150 nm thick Gd-Fe thin film capped with 5nm Cr on Si and Si/SiO2 substrates by electron-beam evaporation under vacuum. Films were found to be amorphous in nature due to the large difference between the atomic radius of Gd and Fe atoms and high cooling rate attained during the deposition process. Magnetization measurements and domain imaging studies indicated the anisotropy axis is tilted in between in-plane and out-of-plane direction. This inherent tilt anisotropy makes it a unique material for sensing vector fields. Magneto-transport measurement on this film showed positive magneto-resistance along both in-plane (IP) and out-of-plane (OOP) directions. This resistance change was mainly contributed by the scattering at domain walls [2].References: [1] A. Talaptra, J. Arout Chelvane and J. Mohanty, AIP Advances., Vol. 8, p. 056327 (2018) [2] M. Tofizur Rahman, et al, Journal of applied physics., Vol. 97, p. 10C515 (2005)

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Microscopic Study of Magnetic Anisotropy Modification in Nanoscale Heavy Metal/Ferromagnetic Insulator Heterostructures

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