Research ArticleAPPLIED PHYSICS

Spin-orbit torque manipulated by fine-tuning of oxygen-induced orbital hybridization

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Science Advances  01 Nov 2019:
Vol. 5, no. 11, eaax4278
DOI: 10.1126/sciadv.aax4278

Abstract

Current-induced spin-orbit torques provide an effective way to manipulate magnetization in spintronic devices, promising for fast switching applications in nonvolatile memory and logic units. Recent studies have revealed that the spin-orbit torque is strongly altered by the oxidation of heterostructures with broken inversion symmetry. Although this finding opens a new field of metal-oxide spin-orbitronics, the role of the oxidation in the spin-orbit physics is still unclear. Here, we demonstrate a marked enhancement of the spin-orbit torque induced by a fine-tuning of oxygen-induced modification of orbital hybridization. This is evidenced by a concomitant enhancement of the interface spin-orbit torque, interface spin loss, and interface perpendicular magnetic anisotropy within a narrow range of the oxidation level of metallic heterostructures. This result reveals the crucial role of the atomic-scale effects in the generation of the spin-orbit torques, opening the door to atomic-level engineering of the spin-orbit physics.

INTRODUCTION

Oxide electronic materials promise a wide range of applications, such as transparent electronics, optoelectronics, and power harvesting (1). Among this class of materials, Cu oxide is one of the first semiconducting materials to be investigated as early as the 1920s (2). Because of its low cost, good carrier mobility, and direct energy gap, Cu oxide has been used in the fabrication of a variety of electronic devices, including solar cells, resistive switching memories, and transistors (3).

Recently, Cu oxide has become attractive in spin-orbitronics, which aims to discover novel phenomena and functionalities arising from spin-orbit coupling (SOC) (4). The fundamental building block of spin-orbitronics is the generation of spin-orbit torques (SOTs), which enable electric manipulation of magnetization (5–11). Although Cu has been believed to generate negligible SOTs because of the weak SOC, a recent study has shown that Cu becomes an efficient SOT generator through oxidation (12). The oxidation-induced enhancement of the SOTs has been observed in various systems recently (13–16). These findings illustrate the essential role of the oxidation effect in exploring the physics and technology of spin-orbitronics. However, a fundamental understanding of the oxidation effect on the spin-orbit physics is still unclear. The great flexibility of the oxidation level of Cu makes it a model system to study the physics behind the generation of the SOTs manipulated by oxidation.

In this work, we demonstrate that the SOT in spin-orbitronic heterostructures is markedly enhanced through a fine-tuning of oxygen-induced orbital hybridization. By measuring the SOTs for Ni81Fe19/CuOx bilayers with various oxidation levels, we found that the magnitude of the damping-like (DL) SOT is substantially enhanced, whereas the sign of the field-like (FL) SOT is reversed, only within a narrow range of the oxidation level of CuOx. We show that this anomaly appears concomitantly with the enhancement of the effective spin-mixing conductance and interface perpendicular magnetic anisotropy (PMA). These results demonstrate the essential role of the atomic-scale and chemical bonding effects in the interface spin-orbit physics, providing a crucial piece of information for a fundamental understanding of the SOT generation.

RESULTS

Spin-torque ferromagnetic resonance

We used the spin-torque ferromagnetic resonance (ST-FMR) to quantify the SOTs generated by CuOx films with various oxidation levels. A schematic illustration of the device structure is shown in Fig. 1A. We deposited a Ni81Fe19(10 nm)/CuOx(10 nm) bilayer, covered by a SiO2(4 nm) capping layer, on a SiO2 substrate by radio frequency (RF) magnetron sputtering, where the numbers in parentheses represent the thickness. For the sputtering of the CuOx film, we introduced the mixture of argon and oxygen gas into the chamber. The amount of the oxygen gas flow Q in the reactive mixture varied between 0 and 1.5% (see Materials and Methods). As shown in Fig. 1B, the electrical resistivity ρ of the CuOx film increases markedly with Q, showing that the oxidation level of the CuOx film is controlled by the oxygen gas flow. The bilayer films were patterned into rectangular strips with a width of 20 μm and length of 150 μm using the photolithography and lift-off techniques. For the ST-FMR measurements, an RF charge current was applied along the longitudinal direction of the device, and an in-plane external magnetic field H was applied with an angle of 45∘ from the longitudinal direction of the device. In the bilayer, the RF current generates the DL- and FL-SOTs, as well as an Oersted field, driving magnetization precession in the adjacent ferromagnetic Ni81Fe19 layer (17). The magnetization precession induces an oscillation of the resistance in the ferromagnetic layer by the anisotropic magnetoresistance, resulting in the generation of a direct current (DC) voltage Vmix through the mixing of the RF charge current and oscillating resistance (18, 19): Vmix = VsymW2/[(μ0H − μ0HFMR)2 + W2] + VantiW(μ0H − μ0HFMR)/[(μ0H − μ0HFMR)2 + W2], where Vsym, Vanti, and W are the magnitude of the symmetric component, the magnitude of the antisymmetric component, and the spectral width, respectively. HFMR is the ferromagnetic resonance field. Here, in the Vmix signal, the symmetric part is proportional to the DL spin-orbit effective field HDL, and the antisymmetric part is due to the sum of the Oersted field HOe and FL spin-orbit effective field HFL (17). In Fig. 1C, we show the Vmix signal for the Ni81Fe19/CuOx bilayers with Q = 0.5, 1.0, and 1.25%, measured by using a bias tee at room temperature. This result shows that the sign of Vmix is reversed by reversing the external magnetic field direction, as expected for the voltage generation induced by the ST-FMR.

Fig. 1 Spin-torque ferromagnetic resonance.

(A) Schematic of the SiO2/Ni81Fe19/CuOx device used for the ST-FMR measurements. To avoid the oxidation of the surface of the Ni81Fe19 layer, the CuOx layer was first deposited on a SiO2 substrate. After the CuOx deposition, the chamber was evacuated to 1 × 10−6 Pa, and then the Ni81Fe19 layer was sputtered on top of the CuOx layer in an Ar atmosphere. Without breaking the vacuum, the surface of the Ni81Fe19 layer was covered by the SiO2 capping layer, which was sputtered from a SiO2 target in an Ar atmosphere. (B) The oxygen flow rate Q dependence of the electrical resistivity ρ, measured by the four-probe method, of the CuOx films. (C) The magnetic field H dependence of the DC voltage Vmix for the Ni81Fe19/CuOx bilayers with Q = 0.5, 1.0, and 1.25% measured at the RF frequencies from 4 to 10 GHz.

Spin-torque generation efficiency

To quantitatively evaluate the influence of the oxidation level of the CuOx layer on the DL and FL spin-torque efficiencies, we measured the ST-FMR for the Ni81Fe19(dF)/CuOx(10 nm) bilayers with various Ni81Fe19 layer thicknesses dF as shown in Fig. 2A. For the bilayers, the FMR spin-torque generation efficiency, ξFMR=(Vsym/Vanti)(eμ0MsdFdN/ℏ)1+Meff/HFMR, is related to the DL and FL spin-torque efficiencies, ξDL and ξFL, as (17)1ξFMR=1ξDL(1+ћeξFLμ0MsdFdN)(1)where ξDL(FL)=(2e/ћ)μ0MsdFHDL(FL)/jcN (see the Supplementary Materials). Here, jcN is the charge current density in the CuOx layer and dN is the thickness of the CuOx layer. Ms and Meff are the saturation magnetization and effective demagnetization field of the Ni81Fe19 layer, respectively. Using Eq. 1, ξDL(FL) can be determined by measuring dF dependence of ξFMR under the assumption that ξDL(FL) does not have a strong dependence on dF in the range examined. In Fig. 2B, we show 1/ξFMR as a function of 1/dF for different Q.

Fig. 2 Thickness dependence of ST-FMR.

(A) The ST-FMR spectra for the Ni81Fe19(dF)/CuOx (10 nm) bilayer with Q = 0.5, 1.0, and 1.25% at 7 GHz, where dF is the thickness of the Ni81Fe19 layer and HFMR is the ferromagnetic resonance field. The solid circles are the experimental data and the solid curves are the fitting results using the sum of the symmetric and antisymmetric functions. (B) 1/dF dependence of 1/ξFMR for the devices with different Q. The open circles are the experimental data. The solid lines are the linear fitting results using Eq. 1.

Figure 2B demonstrates that only the bilayer with Q = 1% shows a different trend in the SOT generation; 1/ξFMR increases linearly with 1/dF for Q = 1%, whereas 1/ξFMR decreases linearly with 1/dF for Q = 0.5, 0.75, and 1.25%. The opposite sign of the slope in the linear relation between 1/ξFMR and 1/dF indicates that the direction of the FL-SOT generated in the bilayer with Q = 1% is opposite to that in the bilayer with Q = 0.5, 0.75, and 1.25% (see Eq. 1). We also note that the intercept of the linear fitting of 1/ξFMR for the bilayer with Q = 1% is smaller than that for the bilayer with Q = 0.5, 0.75, and 1.25%, indicating a larger DL-SOT generation efficiency when Q = 1%. To study the SOT generation around Q = 1%, we further measured the SOTs by slightly changing Q around 1%. In the following, we discuss the ST-FMR results with respect to the electrical resistivity ρ of the CuOx layer because ρ changes sensitively and monotonically with Q as shown in Fig. 1B, enabling the characterization of the oxidation level of the CuOx films.

The drastic change of the SOTs observed in the Ni81Fe19/CuOx bilayer appears only within a narrow range of the oxidation level. In Fig. 3A, we show the DL and FL spin-torque efficiencies, ξDL and ξFL, determined from the 1/dF dependence of 1/ξFMR, as a function of ρ. Figure 3A shows that ξDL is substantially enhanced only around ρ = 9 × 10−5 Ω cm, which is concomitant with the sign reversal of ξFL. ξDL ∼ 0.05 at ρ ∼ 9 × 10−5 Ω cm is comparable to ξDL for a Ni81Fe19/Pt bilayer, demonstrating efficient SOT generation using CuOx. Here, the drastic change of the SOTs is irrelevant to phase transformation in the CuOx layer. The principal phases of Cu oxide are cuprous oxide (Cu2O) and cupric oxide (CuO). However, from x-ray diffraction and x-ray photoelectron measurements, we found that all the CuOx films with Q = 0.50, 0.75, 1.00, and 1.25% are a mixture of Cu and Cu2O; the CuO phase is absent (see the Supplementary Materials).

Fig. 3 Spin-torque generation efficiencies.

(A) The DL ξDL and FL ξFL spin-torque generation efficiencies obtained for the Ni81Fe19/CuOx bilayers with 0.25 % ≤ Q ≤ 1.25% as a function of the CuOx layer resistivity ρ. The solid circles are the experimental data, obtained from the 1/dF dependence of 1/ξFMR. The dotted curve is a guide for eyes. (B) The effective spin mixing conductance geff↑↓ for the Ni81Fe19/CuOx bilayers. geff↑↓ was determined from the Ni81Fe19 layer thickness dependence of the magnetic damping constant α. (C) The interface PMA energy density Ks for the Ni81Fe19/CuOx bilayers. The Ks was determined from dF dependence of Meff.

DISCUSSION

The marked change of the SOTs is induced by the interface SOC, which is maximized only within the narrow range of the oxidation level. In the moderately oxidized CuOx (Q ≤ 1.25%), both bulk and interface SOC can generate the SOTs because the applied change current can flow both in the CuOx bulk and in Ni81Fe19/CuOx interface layers. The bulk contribution can be eliminated by further increasing the oxidation level of the CuOx layer because IcN/Ictot decreases with the oxidation, where IcN and Ictot are the charge current flowing in the CuOx layer and the total charge current flowing in the Ni81Fe19/CuOx bilayer, respectively. In the bilayer with ρ ∼ 10−1 Ω cm (Q = 1.5%), the resistance of the CuOx layer is three orders of magnitude larger than that of the Ni81Fe19 layer, and thus the SOTs can only be generated by the interface SOC (see the Supplementary Materials). We note that the sign of the SOTs in the bilayer with ρ ∼ 9 × 10−5 Ω cm, ξDL > 0 and ξFL > 0, is the same as that in the bilayer with ρ ∼ 10−1 Ω cm (Q = 1.5%), where the interface SOC is responsible for the SOTs (see the Supplementary Materials). This indicates that the interface SOC is responsible for the observed anomaly of the SOTs at ρ ∼ 9 × 10−5 Ω cm. This is also supported by the fact that the anomalous SOT disappears by inserting an ultrathin Cu layer between the Ni81Fe19 and CuOx with Q = 1% (see the Supplementary Materials). In contrast to the highly oxidized Ni81Fe19/CuOx bilayer with ρ ∼ 10−1 Ω cm, the dominant mechanism of the SOT generation in the bilayer within the resistivity range studied in Fig. 3 is determined by the competition between the bulk and interface SOT generation efficiencies, rather than the spatial distribution of the applied charge current. The reason for this is that the change of IcN/Ictot is not substantial, IcN/Ictot∼50% for ρ ∼ 9 × 10−5 Ω cm and IcN/Ictot∼30% for ρ ∼ 23 × 10−5 Ω cm, and both bulk and interface SOC can generate sizable SOTs in all the films studied in Fig. 3. This indicates that the SOTs can be dominated by the interface SOC only when the interface SOT generation efficiency is substantially higher than that of the bulk SOT generation efficiency in the bilayers studied in Fig. 3. Thus, the sign reversal of the FL-SOT only at ρ ∼ 9 × 10−5 Ω cm demonstrates that the interface SOT efficiency is markedly enhanced by the oxidation only at ρ ∼ 9 × 10−5 Ω cm, and the dominant mechanism of the SOT generation is changed only around this oxidation level.

The marked enhancement of the interface SOC, within the narrow range of the oxidation level, is further evidenced by angular momentum dissipation from the Ni81Fe19 layer. Figure 3B shows ρ dependence of the effective spin-mixing conductance geff↑↓, which characterizes the angular momentum dissipation (20). Here, geff↑↓ was obtained from dF dependence of the magnetic damping constant α (20)α=α0+γћ4πMsdFgeff↑↓(2)where α0 is the intrinsic magnetic damping of the Ni81Fe19 film and γ is the gyromagnetic ratio. α for the Ni81Fe19/CuOx bilayers was determined by fitting the microwave frequency f dependence of the ST-FMR spectral width W, using W = (2πα/γ)f + Wext, where Wext is the inhomogeneous linewidth broadening of the extrinsic contribution (see the Supplementary Materials). Figure 3B shows that geff↑↓ is also enhanced around the oxidation level where ξDL is maximized and the sign of ξFL is reversed. In the Ni81Fe19/CuOx bilayer, geff↑↓ can be associated with the angular momentum absorbed in the bulk and interface: geff↑↓=geff↑↓,bulk+geff↑↓,int, where the interface contribution, geff↑↓,int, is known as the spin memory loss due to the interface SOC (21). The bulk contribution is expressed as geff↑↓,bulk=g↑↓[1+(2e2/h)(λN/σN)g↑↓coth(dN/λN)]−1, where g↑↓ is the bare spin-mixing conductance, and λN and σN are the spin diffusion length and conductivity of the CuOx layer, respectively (20). geff↑↓,bulk can be changed with the oxidation through the change of g↑↓, λN, and σN. However, the observed change of geff↑↓ can be reproduced by the change of geff↑↓,bulk only when we assume g↑↓ is negative, which is unphysical. This indicates that the observed enhancement of geff↑↓ is dominated by the enhancement of geff↑↓,int or the interface SOC, consistent with the marked change of the interface SOTs.

Our experimental finding is that the SOT is markedly changed through the enhancement of the SOC at the Ni81Fe19/CuOx interface only within the narrow range of the oxidation level; the interface SOT and SOC are ultrasensitive to the oxidation level of the CuOx layer. The maximization of the interface SOT through the fine-tuning of the oxidation has not been reported previously. Here, the physics behind the interface SOC, or the Bychkov-Rashba SOC, is the orbital hybridization due to the broken inversion symmetry and atomic SOC. Ab initio calculations show that the strength of the interface SOC is dominated by the asymmetry of the interface-state wave function, or the strength of the hybridization, near the position of the nucleus of the interface atoms in conjunction with the atomic SOC (22–29). Because the orbital hybridization plays a key role in the Rashba physics, several experimental and theoretical studies have proposed that the strength of the Rashba splitting can be tuned by adatom adsorption (28–31).

The critical enhancement of the SOC at the Ni81Fe19/CuOx interface can be attributed to oxygen-induced deformations of the interface-state wave functions. Since oxygen is an electronegative atom, the charge transfer toward oxygen atoms should be substantial; although O-2p states are weakly spin-orbit–coupled, they can dramatically modify the hybridization of the Ni, Fe, and Cu orbitals near the interface, resulting in the change of the wave-function asymmetry near the nucleus (32). This oxygen-induced wave-function asymmetry can result in the enhancement of the Rashba effect (28). In the Ni81Fe19/CuOx bilayer, the strength of the atomic SOC of Ni, Fe, and Cu is comparable (33), and thus the wave-function deformation of these atoms near the Ni81Fe19/CuOx interface can contribute to the observed interface SOC (25). In contrast, since the atomic SOC of O is quite small, the primary role of the O incorporation is to control the charge distribution, or the orbital hybridization, near the interface (22). We note that the wave-function deformation near the position of the nucleus of the interface atoms is quite sensitive to the oxygen concentration. An ab initio calculation predicts that the Dzyaloshinskii-Moriya interaction (DMI), which also originates from the interface SOC, is quite sensitive to the atomic-level oxidation; the oxygen incorporation strongly alters the interface DMI through the change of the induced electrostatic dipole moment, or the wave-function asymmetry, which is suppressed by overoxidation (32). Experimentally, the DMI strength in Pt/Co/metal oxide trilayers has been found to be maximized for the optimum oxidation (34). The maximization of the DMI is consistent with our experimental finding of the enhanced interface SOT within the narrow range of the oxidation level. We also note that the amount of the change in the interface oxidation level of the Ni81Fe19/CuOx bilayer is reasonable to markedly alter the interface spin-orbit physics. To characterize the Ni81Fe19/CuOx interface, we have performed x-ray reflectivity (XRR) measurements. The XRR result shows that the thickness dNiFeOx of the oxidized Ni81Fe19 layer changes systematically with Q in the range of 0.5 to 1.0 nm (see the Supplementary Materials). The range of dNiFeOx is comparable to the thickness of the oxidized layer of a Pt/Co/Pt structure where a fourfold (an order of magnitude) increase of the DL (FL) torque efficiency was observed by oxidizing the Co layer around dCoOx = 0.5 nm (15). Here, the anomaly of the SOTs in the Ni81Fe19/CuOx bilayer cannot be attributed to a possible change of the spin-current absorption due to antiferromagnetic properties of the oxidized interface since the Néel temperature for dNiFeOx < 1 nm is far below the room temperature (35).

The essential role of the oxygen-induced modification of the orbital hybridization in the critical enhancement of the interface SOT is further supported by a change of the interface PMA. The interface PMA is also known to be the result of orbital hybridization, in combination with the SOC, and is quite sensitive to the interface oxidation level (36). A previous study demonstrated that the PMA at Co/M interfaces (M = Al, Mg, and Ta) can be optimized through a fine-tuning of the natural oxidation of the interface by controlling the M layer thickness around 0.5 nm (37). To compare the interface SOT and interface PMA, we show the interface PMA energy density Ks for the Ni81Fe19/CuOx bilayer in Fig. 3C. Ks was determined from dF dependence of the effective demagnetization field Meff using μ0Meff = μ0Ms − 2Ks/(MsdF), where Meff was obtained using the Kittel formula: (2πf/γ)=μ0HFMR(μ0HFMR+μ0Heff). Figure 3C shows that the interface PMA is also enhanced at the oxidation level where the anomaly of the SOTs is observed. The concomitant enhancement of the interface SOT and interface PMA demonstrates that the interfacial orbital hybridization, tailored by the oxygen incorporation, governs the spin-orbit physics in the Ni81Fe19/CuOx bilayer.

In summary, we demonstrated the concomitant enhancement of the interface SOT, interface spin loss, and interface PMA, triggered by the fine-tuning of the interface oxidation level of the Ni81Fe19/CuOx bilayer. The underlying physics is the marked enhancement of the interface SOC associated with the oxygen-induced modification of the interface orbital hybridization. This mechanism is clearly different from that of the enhanced SOT generated by naturally oxidized Cu, where the bulk effect plays a key role (12). Our results illustrate the essential role of the atomic-scale and chemical bonding effects in the interface spin-orbit physics, providing a way to tune the SOTs by atomic modification (38–40).

MATERIALS AND METHODS

The films were deposited on thermally oxidized Si substrates by RF magnetron sputtering at room temperature. The base pressure in the chamber before the deposition was lower than 1 ×10−6 Pa, and the deposition pressure was 0.2 Pa. The Ni81Fe19 and SiO2 films were deposited by applying argon gas with a flow rate of 10 standard cubic centimeters per minute (sccm). For the CuOx deposition, a 99.99% purity Cu target was used, argon gas flow rate was fixed with 20 sccm, and the oxygen gas was applied with the reactive mixture ratio Q. The film thicknesses were controlled by the deposition time with a precalibrated deposition rate for each oxidation level. For the fabrication of the devices used for the ST-FMR experiment, the substrates were patterned into a 20 μm × 150 μm rectangular shape by standard photolithography before deposition, and lift-off technique was used to take off the remaining part of the films after deposition. For the Ni81Fe19 layer thickness dependence of the ST-FMR, a linear shutter was used to fabricate the Ni81Fe19 layer with various thicknesses. For the x-ray diffraction and x-ray photoelectron measurements of the CuOx films, the 50-nm-thick films were deposited on glass substrates with different oxygen reactive mixture rates Q by RF magnetron sputtering at room temperature.

SUPPLEMENTARY MATERIALS

Supplementary material for this article is available at http://advances.sciencemag.org/cgi/content/full/5/11/eaax4278/DC1

Section S1. Spin-torque efficiency

Section S2. X-ray diffraction and x-ray photoelectron measurements

Section S3. Interface SOTs

Section S4. Spin-torque ferromagnetic resonance for the Ni81Fe19/Cu/CuOx trilayer

Section S5. Magnetic damping constant

Section S6. Interface oxidation level characterized by x-ray reflectivity

Fig. S1. Characterization of CuOx films.

Fig. S2. Interface SOTs.

Fig. S3. ST-FMR for trilayer.

Fig. S4. Magnetic damping constant.

Fig. S5. X-ray reflectivity.

Fig. S6. Auger electron spectroscopy.

References (41–44)

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REFERENCES AND NOTES

  1. ↵
    1. M. Lorenz,
    2. M. S. R. Rao,
    3. T. Venkatesan,
    4. E. Fortunato,
    5. P. Barquinha,
    6. R. Branquinho,
    7. D. Salgueiro,
    8. R. Martins,
    9. E. Carlos,
    10. A. Liu,
    11. F. K. Shan,
    12. M. Grundmann,
    13. H. Boschker,
    14. J. Mukherjee,
    15. M. Priyadarshini,
    16. N. DasGupta,
    17. D. J. Rogers,
    18. F. H. Teherani,
    19. E. V. Sandana,
    20. P. Bove,
    21. K. Rietwyk,
    22. A. Zaban,
    23. A. Veziridis,
    24. A. Weidenkaff,
    25. M. Muralidhar,
    26. M. Murakami,
    27. S. Abel,
    28. J. Fompeyrine,
    29. J. Zuniga-Perez,
    30. R. Ramesh,
    31. N. A. Spaldin,
    32. S. Ostanin,
    33. V. Borisov,
    34. I. Mertig,
    35. V. Lazenka,
    36. G. Srinivasan,
    37. W. Prellier,
    38. M. Uchida,
    39. M. Kawasaki,
    40. R. Pentcheva,
    41. P. Gegenwart,
    42. F. M. Granozio,
    43. J. Fontcuberta,
    44. N. Pryds
    , The 2016 oxide electronic materials and oxide interfaces roadmap. J. Phys. D 49, 433001 (2016).
    OpenUrl
  2. ↵
    1. L. O. Grondahl
    , The copper-cuprous-oxide rectifier and photoelectric cell. Rev. Mod. Phys. 5, 141–168 (1933).
    OpenUrlCrossRef
  3. ↵
    1. X. Yu,
    2. T. J. Marks,
    3. A. Facchetti
    , Metal oxides for optoelectronic applications. Nat. Mater. 15, 383–396 (2016).
    OpenUrlCrossRefPubMed
  4. ↵
    1. A. Manchon,
    2. J. Železnỳ,
    3. I. M. Miron,
    4. T. Jungwirth,
    5. J. Sinova,
    6. A. Thiaville,
    7. K. Garello,
    8. P. Gambardella
    , Current-induced spin-orbit torques in ferromagnetic and antiferromagnetic systems. Rev. Mod. Phys. 91, 035004 (2019).
    OpenUrl
  5. ↵
    1. I. M. Miron,
    2. G. Gaudin,
    3. S. Auffret,
    4. B. Rodmacq,
    5. A. Schuhl,
    6. S. Pizzini,
    7. J. Vogel,
    8. P. Gambardella
    , Current-driven spin torque induced by the Rashba effect in a ferromagnetic metal layer. Nat. Mater. 9, 230–234 (2010).
    OpenUrlPubMedWeb of Science
    1. L. Liu,
    2. C.-F. Pai,
    3. Y. Li,
    4. H. W. Tseng,
    5. D. C. Ralph,
    6. R. A. Buhrman
    , Spin-torque switching with the giant spin Hall effect of tantalum. Science 336, 555–558 (2012).
    OpenUrlAbstract/FREE Full Text
    1. J. Kim,
    2. J. Sinha,
    3. M. Hayashi,
    4. M. Yamanouchi,
    5. S. Fukami,
    6. T. Suzuki,
    7. S. Mitani,
    8. H. Ohno
    , Layer thickness dependence of the current-induced effective field vector in Ta|CoFeB|MgO. Nat. Mater. 12, 240–245 (2013).
    OpenUrlPubMed
    1. G. Yu,
    2. P. Upadhyaya,
    3. Y. Fan,
    4. J. G. Alzate,
    5. W. Jiang,
    6. K. L. Wong,
    7. S. Takei,
    8. S. A. Bender,
    9. L.-T. Chang,
    10. Y. Jiang,
    11. M. Lang,
    12. J. Tang,
    13. Y. Wang,
    14. Y. Tserkovnyak,
    15. P. K. Amiri,
    16. K. L. Wang
    , Switching of perpendicular magnetization by spin-orbit torques in the absence of external magnetic fields. Nat. Nanotechnol. 9, 548–554 (2014).
    OpenUrlCrossRefPubMed
    1. Y. Fan,
    2. P. Upadhyaya,
    3. X. Kou,
    4. M. Lang,
    5. S. Takei,
    6. Z. Wang,
    7. J. Tang,
    8. L. He,
    9. L.-T. Chang,
    10. M. Montazeri,
    11. G. Yu,
    12. W. Jiang,
    13. T. Nie,
    14. R. N. Schwartz,
    15. Y. Tserkovnyak,
    16. K. L. Wang
    , Magnetization switching through giant spin–orbit torque in a magnetically doped topological insulator heterostructure. Nat. Mater. 13, 699–704 (2014).
    OpenUrl
    1. X. Fan,
    2. J. Wu,
    3. Y. Chen,
    4. M. J. Jerry,
    5. H. Zhang,
    6. J. Q. Xiao
    , Observation of the nonlocal spin-orbital effective field. Nat. Commun. 4, 1799 (2013).
    OpenUrl
  11. ↵
    1. S. Fukami,
    2. C. Zhang,
    3. S. DuttaGupta,
    4. A. Kurenkov,
    5. H. Ohno
    , Magnetization switching by spin-orbit torque in an antiferromagnet-ferromagnet bilayer system. Nat. Mater. 15, 535–541 (2016).
    OpenUrlCrossRefPubMed
  12. ↵
    1. H. An,
    2. Y. Kageyama,
    3. Y. Kanno,
    4. N. Enishi,
    5. K. Ando
    , Spin-torque generator engineered by natural oxidation of Cu. Nat. Commun. 7, 13069 (2016).
    OpenUrlCrossRefPubMed
  13. ↵
    1. X. Qiu,
    2. K. Narayanapillai,
    3. Y. Wu,
    4. P. Deorani,
    5. D.-H. Yang,
    6. W.-S. Noh,
    7. J.-H. Park,
    8. K.-J. Lee,
    9. H.-W. Lee,
    10. H. Yang
    , Spin-orbit-torque engineering via oxygen manipulation. Nat. Nanotechnol. 10, 333–338 (2015).
    OpenUrl
    1. K.-U. Demasius,
    2. T. Phung,
    3. W. Zhang,
    4. B. P. Hughes,
    5. S.-H. Yang,
    6. A. Kellock,
    7. W. Han,
    8. A. Pushp,
    9. S. S. P. Parkin
    , Enhanced spin-orbit torques by oxygen incorporation in tungsten films. Nat. Commun. 7, 10644 (2016).
    OpenUrlCrossRefPubMed
  15. ↵
    1. K. Hasegawa,
    2. Y. Hibino,
    3. M. Suzuki,
    4. T. Koyama,
    5. D. Chiba
    , Enhancement of spin-orbit torque by inserting CoOx layer into Co/Pt interface. Phys. Rev. B 98, 020405 (2018).
    OpenUrl
  16. ↵
    1. H. An,
    2. T. Ohno,
    3. Y. Kanno,
    4. Y. Kageyama,
    5. Y. Monnai,
    6. H. Maki,
    7. J. Shi,
    8. K. Ando
    , Current-induced magnetization switching using an electrically insulating spin-torque generator. Sci. Adv. 4, aar2250 (2018).
    OpenUrl
  17. ↵
    1. C.-F. Pai,
    2. Y. Ou,
    3. L. H. Vilela-Leão,
    4. D. C. Ralph,
    5. R. A. Buhrman
    , Dependence of the efficiency of spin Hall torque on the transparency of Pt/ferromagnetic layer interfaces. Phys. Rev. B 92, 064426 (2015).
    OpenUrl
  18. ↵
    1. L. Liu,
    2. T. Moriyama,
    3. D. Ralph,
    4. R. Buhrman
    , Spin-torque ferromagnetic resonance induced by the spin Hall effect. Phys. Rev. Lett. 106, 036601 (2011).
    OpenUrlCrossRefPubMed
  19. ↵
    1. W. Zhang,
    2. W. Han,
    3. X. Jiang,
    4. S.-H. Yang,
    5. S. S. P. Parkin
    , Role of transparency of platinum-ferromagnet interfaces in determining the intrinsic magnitude of the spin Hall effect. Nat. Phys. 11, 496–502 (2015).
    OpenUrl
  20. ↵
    1. Y. Tserkovnyak,
    2. A. Brataas,
    3. G. E. Bauer,
    4. B. I. Halperin
    , Nonlocal magnetization dynamics in ferromagnetic heterostructures. Rev. Mod. Phys. 77, 1375–1421 (2005).
    OpenUrlCrossRefWeb of Science
  21. ↵
    1. J.-C. Rojas-Sánchez,
    2. N. Reyren,
    3. P. Laczkowski,
    4. W. Savero,
    5. J.-P. Attané,
    6. C. Deranlot,
    7. M. Jamet,
    8. J.-M. George,
    9. L. Vila,
    10. H. Jaffrès
    , Spin pumping and inverse spin Hall effect in platinum: The essential role of spin-memory loss at metallic interfaces. Phys. Rev. Lett. 112, 106602 (2014).
    OpenUrl
  22. ↵
    1. K. V. Shanavas,
    2. Z. S. Popović,
    3. S. Satpathy
    , Theoretical model for Rashba spin-orbit interaction in d electrons. Phys. Rev. B 90, 165108 (2014).
    OpenUrl
    1. M. Hortamani,
    2. R. Wiesendanger
    , Role of hybridization in the Rashba splitting of noble metal monolayers on W(110). Phys. Rev. B 86, 235437 (2012).
    OpenUrl
    1. L. Petersen,
    2. P. Hedegård
    , A simple tight-binding model of spin–orbit splitting of sp-derived surface states. Surf. Sci. 459, 49–56 (2000).
    OpenUrlCrossRefWeb of Science
  25. ↵
    1. S. Grytsyuk,
    2. A. Belabbes,
    3. P. M. Haney,
    4. H.-W. Lee,
    5. K.-J. Lee,
    6. M. D. Stiles,
    7. U. Schwingenschlögl,
    8. A. Manchon
    , k-asymmetric spin splitting at the interface between transition metal ferromagnets and heavy metals. Phys. Rev. B 93, 174421 (2016).
    OpenUrl
    1. G. Bihlmayer,
    2. Y. M. Koroteev,
    3. P. Echenique,
    4. E. Chulkov,
    5. S. Blügel
    , The Rashba-effect at metallic surfaces. Surf. Sci. 600, 3888–3891 (2006).
    OpenUrl
    1. S. R. Park,
    2. C. H. Kim,
    3. J. Yu,
    4. J. H. Han,
    5. C. Kim
    , Orbital-angular-momentum based origin of Rashba-type surface band splitting. Phys. Rev. Lett. 107, 156803 (2011).
    OpenUrlCrossRefPubMed
  28. ↵
    1. O. Krupin,
    2. G. Bihlmayer,
    3. K. Starke,
    4. S. Gorovikov,
    5. J. E. Prieto,
    6. K. Döbrich,
    7. S. Blügel,
    8. G. Kaindl
    , Rashba effect at magnetic metal surfaces. Phys. Rev. B 71, 201403 (2005).
    OpenUrl
  29. ↵
    1. H. Tsai,
    2. S. Karube,
    3. K. Kondou,
    4. N. Yamaguchi,
    5. F. Ishii,
    6. Y. Otani
    , Clear variation of spin splitting by changing electron distribution at non-magnetic metal/Bi2O3 interfaces. Sci. Rep. 8, 5564 (2018).
    OpenUrl
    1. E. Rotenberg,
    2. J. W. Chung,
    3. S. D. Kevan
    , Spin-orbit coupling induced surface band splitting in Li/W(110) and Li/Mo(110). Phys. Rev. Lett. 82, 4066–4069 (1999).
    OpenUrlCrossRefWeb of Science
  31. ↵
    1. M. Hochstrasser,
    2. J. G. Tobin,
    3. E. Rotenberg,
    4. S. D. Kevan
    , Spin-resolved photoemission of surface states of W(110)-(1×1)H. Phys. Rev. Lett. 89, 216802 (2002).
    OpenUrlPubMed
  32. ↵
    1. A. Belabbes,
    2. G. Bihlmayer,
    3. S. Blügel,
    4. A. Manchon
    , Oxygen-enabled control of Dzyaloshinskii-Moriya interaction in ultra-thin magnetic films. Sci. Rep. 6, 24634 (2016).
    OpenUrl
  33. ↵
    M. Montalti, A. Credi, L. Prodi, M. T. Gandolfi, Handbook of Photochemistry (CRC Press, Taylor & Francis Group, 2006).
  34. ↵
    1. D. de Souza Chaves,
    2. F. Ajejas,
    3. V. Křižáková,
    4. J. Vogel,
    5. S. Pizzini
    , Oxidation dependence of the Dzyaloshinskii-Moriya interaction in Pt/Co/MOx trilayers (M = Al or Gd). Phys. Rev. B 99, 144404 (2019).
    OpenUrl
  35. ↵
    1. L. Frangou,
    2. G. Forestier,
    3. S. Auffret,
    4. S. Gambarelli,
    5. V. Baltz
    , Relaxation mechanism in NiFe thin films driven by spin angular momentum absorption throughout the antiferromagnetic phase transition in native surface oxides. Phys. Rev. B 95, 054416 (2017).
    OpenUrl
  36. ↵
    1. B. Dieny,
    2. M. Chshiev
    , Perpendicular magnetic anisotropy at transition metal/oxide interfaces and applications. Rev. Mod. Phys. 89, 025008 (2017).
    OpenUrl
  37. ↵
    1. A. Manchon,
    2. C. Ducruet,
    3. L. Lombard,
    4. S. Auffret,
    5. B. Rodmacq,
    6. B. Dieny,
    7. S. Pizzini,
    8. J. Vogel,
    9. V. Uhlíř,
    10. M. Hochstrasser,
    11. G. Panaccione
    , Analysis of oxygen induced anisotropy crossover in Pt/Co/MOx trilayers. J. Appl. Phys. 104, 043914 (2008).
    OpenUrlCrossRef
  38. ↵
    1. A. Bose,
    2. H. Singh,
    3. V. K. Kushwaha,
    4. S. Bhuktare,
    5. S. Dutta,
    6. A. A. Tulapurkar
    , Sign reversal of fieldlike spin-orbit torque in an ultrathin Cr/Ni bilayer. Phys. Rev. Appl. 9, 014022 (2018).
    OpenUrl
    1. M. Mann,
    2. G. S. D. Beach
    , Reduction of in-plane field required for spin-orbit torque magnetization reversal by insertion of Au spacer in Pt/Au/Co/Ni/Co/Ta. APL Mater. 5, 106104 (2017).
    OpenUrl
  40. ↵
    1. S. Shi,
    2. Y. Ou,
    3. S. V. Aradhya,
    4. D. C. Ralph,
    5. R. A. Buhrman
    , Fast low-current spin-orbit-torque switching of magnetic tunnel junctions through atomic modifications of the free-layer interfaces. Phys. Rev. Appl. 9, 011002 (2018).
    OpenUrl
  41. ↵
    1. V. Tshitoyan,
    2. C. Ciccarelli,
    3. A. P. Mihai,
    4. M. Ali,
    5. A. C. Irvine,
    6. T. A. Moore,
    7. T. Jungwirth,
    8. A. J. Ferguson
    , Electrical manipulation of ferromagnetic NiFe by antiferromagnetic IrMn. Phys. Rev. B 92, 214406 (2015).
    OpenUrl
    1. M.-H. Nguyen,
    2. D. C. Ralph,
    3. R. A. Buhrman
    , Spin torque study of the spin Hall conductivity and spin diffusion length in platinum thin films with varying resistivity. Phys. Rev. Lett. 116, 126601 (2016).
    OpenUrl
  43. D. D. Stancil, A. Prabhakar, Spin waves (Springer, 2009).
  44. ↵
    1. S. Hofmann
    , Sputter depth profile analysis of interfaces. Rep. Prog. Phys. 61, 827 (1998).
    OpenUrlCrossRef
Acknowledgments: Funding: This work was supported by JSPS KAKENHI grant numbers 19H00864, 26220604, and 26103004; the Canon Foundation; the Asahi Glass Foundation; the JGC-S Scholarship Foundation; the Kao Foundation for Arts and Sciences; and the Spintronics Research Network of Japan (Spin-RNJ). H.A. acknowledges the support from the JSPS Fellowship (no. P17066). Author contributions: Y.K., Y.T., and H.A. fabricated devices and collected and analyzed the data. T.H., T.G., and J.S. performed the materials characterization. K.A. and Y.K. designed the experiments, developed the explanation, and wrote the manuscript. All authors discussed results and reviewed the manuscript. Y.K. claims the responsibility for all the figures in the main text and the Supplementary Materials. Competing interests: The authors declare that they have no competing interests. Data and materials availability: All data needed to evaluate the conclusions in the paper are present in the paper and/or the Supplementary Materials. Additional data related to this paper may be requested from the authors.
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