46 research outputs found

    Resonate and Fire Neuron with Fixed Magnetic Skyrmions

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    In the brain, the membrane potential of many neurons oscillates in a subthreshold damped fashion and fire when excited by an input frequency that nearly equals their eigen frequency. In this work, we investigate theoretically the artificial implementation of such "resonate-and-fire" neurons by utilizing the magnetization dynamics of a fixed magnetic skyrmion in the free layer of a magnetic tunnel junction (MTJ). To realize firing of this nanomagnetic implementation of an artificial neuron, we propose to employ voltage control of magnetic anisotropy or voltage generated strain as an input (spike or sinusoidal) signal, which modulates the perpendicular magnetic anisotropy (PMA). This results in continual expansion and shrinking (i.e. breathing) of a skyrmion core that mimics the subthreshold oscillation. Any subsequent input pulse having an interval close to the breathing period or a sinusoidal input close to the eigen frequency drives the magnetization dynamics of the fixed skyrmion in a resonant manner. The time varying electrical resistance of the MTJ layer due to this resonant oscillation of the skyrmion core is used to drive a Complementary Metal Oxide Semiconductor (CMOS) buffer circuit, which produces spike outputs. By rigorous micromagnetic simulation, we investigate the interspike timing dependence and response to different excitatory and inhibitory incoming input pulses. Finally, we show that such resonate and fire neurons have potential application in coupled nanomagnetic oscillator based associative memory arrays

    Energy Efficient Spintronic Device for Neuromorphic Computation

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    Future computing will require significant development in new computing device paradigms. This is motivated by CMOS devices reaching their technological limits, the need for non-Von Neumann architectures as well as the energy constraints of wearable technologies and embedded processors. The first device proposal, an energy-efficient voltage-controlled domain wall device for implementing an artificial neuron and synapse is analyzed using micromagnetic modeling. By controlling the domain wall motion utilizing spin transfer or spin orbit torques in association with voltage generated strain control of perpendicular magnetic anisotropy in the presence of Dzyaloshinskii-Moriya interaction (DMI), different positions of the domain wall are realized in the free layer of a magnetic tunnel junction to program different synaptic weights. Additionally, an artificial neuron can be realized by combining this DW device with a CMOS buffer. The second neuromorphic device proposal is inspired by the brain. Membrane potential of many neurons oscillate in a subthreshold damped fashion and fire when excited by an input frequency that nearly equals their Eigen frequency. We investigate theoretical implementation of such โ€œresonate-and-fireโ€ neurons by utilizing the magnetization dynamics of a fixed magnetic skyrmion based free layer of a magnetic tunnel junction (MTJ). Voltage control of magnetic anisotropy or voltage generated strain results in expansion and shrinking of a skyrmion core that mimics the subthreshold oscillation. Finally, we show that such resonate and fire neurons have potential application in coupled nanomagnetic oscillator based associative memory arrays

    Neuromorphic weighted sum with magnetic skyrmions

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    Integrating magnetic skyrmion properties into neuromorphic computing promises advancements in hardware efficiency and computational power. However, a scalable implementation of the weighted sum of neuron signals, a core operation in neural networks, has yet to be demonstrated. In this study, we exploit the non-volatile and particle-like characteristics of magnetic skyrmions, akin to synaptic vesicles and neurotransmitters, to perform this weighted sum operation in a compact, biologically-inspired manner. To this aim, skyrmions are electrically generated in numbers proportional to the input with an efficiency given by a non-volatile weight. These chiral particles are then directed using localized current injections to a location where their presence is quantified through non-perturbative electrical measurements. Our experimental demonstration, currently with two inputs, can be scaled to accommodate multiple inputs and outputs using a crossbar array design, potentially nearing the energy efficiency observed in biological systems.Comment: 12 pages, 5 figure

    A Survey on Reservoir Computing and its Interdisciplinary Applications Beyond Traditional Machine Learning

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    Reservoir computing (RC), first applied to temporal signal processing, is a recurrent neural network in which neurons are randomly connected. Once initialized, the connection strengths remain unchanged. Such a simple structure turns RC into a non-linear dynamical system that maps low-dimensional inputs into a high-dimensional space. The model's rich dynamics, linear separability, and memory capacity then enable a simple linear readout to generate adequate responses for various applications. RC spans areas far beyond machine learning, since it has been shown that the complex dynamics can be realized in various physical hardware implementations and biological devices. This yields greater flexibility and shorter computation time. Moreover, the neuronal responses triggered by the model's dynamics shed light on understanding brain mechanisms that also exploit similar dynamical processes. While the literature on RC is vast and fragmented, here we conduct a unified review of RC's recent developments from machine learning to physics, biology, and neuroscience. We first review the early RC models, and then survey the state-of-the-art models and their applications. We further introduce studies on modeling the brain's mechanisms by RC. Finally, we offer new perspectives on RC development, including reservoir design, coding frameworks unification, physical RC implementations, and interaction between RC, cognitive neuroscience and evolution.Comment: 51 pages, 19 figures, IEEE Acces

    Spin dynamics under spin Hall effect modulation: Skyrmion oscillator

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    ํ•™์œ„๋…ผ๋ฌธ(๋ฐ•์‚ฌ)--์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› :์ž์—ฐ๊ณผํ•™๋Œ€ํ•™ ๋ฌผ๋ฆฌยท์ฒœ๋ฌธํ•™๋ถ€(๋ฌผ๋ฆฌํ•™์ „๊ณต),2019. 8. ์ตœ์„๋ด‰.A magnet exhibits semi-permanent magnetic field, unless the ordering of magnetic moments does not break by external factors. This so-called non-volatility of magnetization can be harnessed to realize a power-efficient data storage, provided with proper mechanisms to modify the magnetization. These mechanisms were established by the discovery of giant magnetoresistance and spin-polarized current in the 1980s, which enabled the electric detection and control of magnetization, respectively. The concept of spin finally entered the field of electronics, which consecutively led to successful applications in the logic and memory devices. This associated field of study is called the spintronics, also known as the spin electronics. Since the spintronics is involved deeply with the collective ordering of the spins, the constraints bestowed upon the system not only expand the phenomena toward exotic dynamics but also provide design rules to achieve desirable properties. Among various possible constraints, a simple tri-layered system of a ferromagnetic thin film sandwiched between two nonmagnetic layers, exhibit surprisingly complex spin dynamics depending on the choice of the materials and their respective thicknesses. As a result, the current-induced spin dynamics in this tri-layered magnetic system is mainly studied throughout the thesis. Amid the various interesting dynamics of a tri-layered film, the spin-Hall effect (SHE) in the sandwiching heavy metal layers that transfer spin polarized current into the ferromagnetic layer, stands out with its design capabilities. Since the magnitude and sign of the spin polarized current by SHE depends on the material and its thickness, one can manipulate the transferred spin torque by modulating the thickness of the sandwiching layers. This technique is called the spin-Hall-effect modulation and exhibits some interesting features. The thesis is mainly directed on searching what and how exotic spin dynamics happen at the wires with laterally modulated SHE, via micromagnetic simulations and analytic equation analysis. Chapter 2 shows how the current-driven domain wall (DW) pins and depins from various types of spin-Hall-effect-modulation boundaries. The method of unidirectional depinning from given modulation boundaries are investigated. This unidirectional depinning behavior provides a systematic mechanism to precisely move a DW step-by-step toward next modulation boundaries only by alternating the direction of electric current, which will assist the realization of a racetrack memory. Chapter 3 is the highlight of this study where we propose a whole new concept of spin-torque oscillator, based on magnetic skyrmion dynamics subject to lateral modulation of the SHE. In the oscillator, a skyrmion circulates around the modulation boundary between opposite SHE-torque regions, where the SHE pushes the skyrmion in the opposite direction, toward the modulation boundary. A micromagnetic simulation confirms such oscillations. This SHE-modulation-based skyrmion oscillator is expected to overcome the troubling issues of conventional spin-torque oscillators. As part of recent approaches to search for possible applications of spintronic devices, neuromorphic engineering is also briefly discussed in Chapter 4. A neuron device with integrate-and-fire feature is realized via current-driven DW motion in a wire with a magnetic tunnel junction at the end. With the already proposed idea of a DW synapse device, all-DW-based artificial neural network can be realized. Additionally, miscellaneous analytic equations were derived to help magnetic-parameter measurement and to offer design rules for certain properties. The depinning current from a triangle notch, the equations to measure spin-orbit torque at any initial angle and the equations to measure anisotropy field from magneto optical Kerr effect setup are derived from associated analytic models and explained in Chapter 5. Findings analyzed in this thesis provide the latest understanding of the spin-Hall effect modulated systems and some others. The explained spin dynamics in these systems not only exhibit properties that can better the state-of-the-art applications, but also triggers new possibilities to design in completely unconventional ways.๊ฐ•์ž์„ฑ ๋ฌผ์งˆ์€ ์ •๋ ฌ๋œ ์žํ™”์˜ ์ƒํƒœ๊ฐ€ ์™ธ๋ถ€ ์š”์ธ์— ์˜ํ•ด ๊นจ์ง€์ง€ ์•Š๋Š” ํ•œ, ๋ฐ˜์˜๊ตฌ์ ์œผ๋กœ ์ž๊ธฐ์žฅ์„ ๊ฐ€์ง„๋‹ค. ์ด๊ฒƒ์€ ์žํ™”๊ฐ€ ์ผ์ข…์˜ ๋น„ํœ˜๋ฐœ์„ฑ์„ ๊ฐ€์ง„๋‹ค๋Š” ๊ฒƒ์„ ์˜๋ฏธํ•˜๋ฉฐ, ์ด๋Š” ์žํ™”๋ฅผ ๋ณ€ํ™”์‹œํ‚ฌ ์ˆ˜ ์žˆ๋Š” ์ ์ ˆํ•œ ๋ฐฉ๋ฒ•์ด ๊ฐ–์ถ”์–ด์ง„๋‹ค๋ฉด, ์ž์„ฑ๋ฌผ์งˆ์„ ์ด์šฉํ•˜์—ฌ ์ €์ „๋ ฅ์˜ ์ €์žฅ์žฅ์น˜๋ฅผ ๊ตฌํ˜„ํ•  ์ˆ˜ ์žˆ๋‹ค๋Š” ๊ฒƒ์„ ์˜๋ฏธํ•œ๋‹ค. ์‹ค์ œ๋กœ 1980 ๋…„๋Œ€๋ถ€ํ„ฐ ๊ฑฐ๋Œ€ ์ž๊ธฐ ์ €ํ•ญ ํšจ๊ณผ (giant magnetoresistance: GMR)์™€ ์Šคํ•€ ํ† ํฌ ํ˜„์ƒ (spin torque)์ด ๋ฐœ๊ฒฌ๋จ์œผ๋กœ์จ, ์žํ™”๊ฐ€ ๊ฐ์ž ์ „๊ธฐ์ ์œผ๋กœ ์ธก์ •๋˜๊ฑฐ๋‚˜, ์ปจํŠธ๋กค ๋  ์ˆ˜ ์žˆ๊ฒŒ ๋˜์—ˆ๊ณ , ์ด๋กœ ์ธํ•ด, ๋ฌผ์งˆ์˜ ์Šคํ•€ ์ƒํƒœ๊ฐ€ ๋ณธ๊ฒฉ์ ์œผ๋กœ ์ „๊ธฐ ์†Œ์ž์— ์‘์šฉ๋˜๊ธฐ ์‹œ์ž‘ํ•˜์˜€๋‹ค. ์ฃผ๋กœ ๋…ผ๋ฆฌ ๋ฐ ๋ฉ”๋ชจ๋ฆฌ ์†Œ์ž์— ์‘์šฉ๋˜๋Š” ๊ด€๋ จ ๋ถ„์•ผ์— ๋Œ€ํ•œ ์ œ๋ฐ˜์˜ ์—ฐ๊ตฌ๋ฅผ ์Šคํ•€ํŠธ๋กœ๋‹‰์Šค (spintronics: spin electronics)๋ผ๊ณ  ๋ถ€๋ฅธ๋‹ค. ์Šคํ•€ํŠธ๋กœ๋‹‰์Šค๋Š” ์–ธ๊ธ‰ํ•˜์˜€๋“ฏ์ด, ์Šคํ•€๋“ค์˜ ์ง‘๋‹จ ํ˜„์ƒ์— ๊นŠ๊ฒŒ ๊ด€๊ณ„๋˜์–ด ์žˆ๊ธฐ ๋•Œ๋ฌธ์—, ์‹œ์Šคํ…œ์— ์ฃผ์–ด์ง„ ์—ฌ๋Ÿฌ ์ œํ•œ ์กฐ๊ฑด๋“ค์— ์˜ํ•ด, ์™„์ „ํžˆ ์ƒˆ๋กœ์šด ํ˜„์ƒ์ด ๋ฐœ๊ฒฌ๋  ๋ฟ๋งŒ์ด ์•„๋‹ˆ๋ผ, ๊ทธ ์กฐ๊ฑด์„ ์ด์šฉํ•จ์œผ๋กœ์จ, ์›ํ•˜๋Š” ํŠน์„ฑ์„ ๋””์ž์ธ ํ•  ์ˆ˜ ์žˆ๋Š” ๊ฐ€๋Šฅ์„ฑ๊นŒ์ง€ ๊ฐ–์ถ”๊ณ  ์žˆ๋‹ค. ์—ฌ๋Ÿฌ ์ œํ•œ์กฐ๊ฑด๋“ค ์ค‘, ๊ฐ„๋‹จํ•œ 3์ธต ๊ตฌ์กฐ์˜ ๊ฐ•์ž์„ฑ ๋ฐ•๋ง‰์ด ๋†€๋ž๋„๋ก ๋ณต์žกํ•œ ์Šคํ•€ ๋™์—ญํ•™์„ ๋ณด์ด๋Š” ๊ฒƒ์ด ์•Œ๋ ค์ ธ ์žˆ๋‹ค. ๊ฐ•์ž์„ฑ ๋ฌผ์งˆ๋งŒ์ด ์•„๋‹Œ, ์ด์›ƒํ•˜๋Š” ์ธต์˜ ๋ฌผ์งˆ๊ณผ ๋‘๊ป˜, ๊ฒฝ๊ณ„๋ฉด์˜ ์กฐ๊ฑด ๋“ฑ์— ์˜ํ•ด ๋‹ค์–‘ํ•œ ์ž์„ฑ ํŠน์ง•์ด ๊ด€์ฐฐ๋˜๊ณ  ์žˆ๊ณ , ์ด ๋…ผ๋ฌธ ๋˜ํ•œ ์ด๋Ÿฌํ•œ 3์ธต ๊ตฌ์กฐ์— ์ „๋ฅ˜๊ฐ€ ์ฃผ์ž…๋˜์—ˆ์„ ๋•Œ ๋‚˜ํƒ€๋‚˜๋Š” ์—ฌ๋Ÿฌ ํ˜„์ƒ์„ ๋ฐํžˆ๊ณ  ์ด์šฉํ•˜๋Š” ๋ฐ ํ•ต์‹ฌ์„ ๋‘๊ณ  ์žˆ๋‹ค. 3์ธต ๊ตฌ์กฐ ํ•„๋ฆ„์˜ ์—ฌ๋Ÿฌ ํฅ๋ฏธ๋กœ์šด ๋™์—ญํ•™ ์ค‘์—์„œ๋„, ์ž์„ฑ์ธต์— ์ด์›ƒํ•œ ๋ฌผ์งˆ์ธต์—์„œ ์ผ์–ด๋‚˜๋Š” ์Šคํ•€ ํ™€ ํšจ๊ณผ (spin-Hall effect: SHE)๋Š” ๋””์ž์ธ์˜ ์šฉ์ดํ•จ์— ์žˆ์–ด ๋›ฐ์–ด๋‚œ ๋ชจ์Šต์„ ๋ณด์ธ๋‹ค. ์Šคํ•€ ํ™€ ํšจ๊ณผ์˜ ํฌ๊ธฐ์™€ ๋ถ€ํ˜ธ๋Š” ์ด์›ƒ์ธต์˜ ๋ฌผ์งˆ๋งŒ์ด ์•„๋‹Œ ๋‘๊ป˜์— ๋”ฐ๋ผ ๋ฐ”๋€Œ๊ธฐ ๋•Œ๋ฌธ์—, ์ด์›ƒ์ธต์˜ ๋‘๊ป˜๋ฅผ ๋ฐ”๊พธ์–ด์ฃผ๋Š” ๊ฒƒ๋งŒ์œผ๋กœ, ์ž์„ฑ์ธต์— ์Šคํ•€ ํ™€ ํšจ๊ณผ๋กœ ์ธํ•ด ์ „๋‹ฌ๋˜๋Š” ์Šคํ•€ ํ† ํฌ์˜ ํฌ๊ธฐ ๋ฐ ๋ถ€ํ˜ธ๋ฅผ ๋งˆ์Œ๋Œ€๋กœ ๋ฐ”๊พธ์–ด ์ค„ ์ˆ˜ ์žˆ๋‹ค. ์ด ๊ธฐ์ˆ ์€ ์Šคํ•€ ํ™€ ํšจ๊ณผ ์กฐ์ • ๊ธฐ์ˆ  (spin-Hall effect modulation)์œผ๋กœ ๋ถˆ๋ฆฌ๋ฉฐ, ์ด ๋…ผ๋ฌธ์€ ์ด ์Šคํ•€ ํ™€ ํšจ๊ณผ ์กฐ์ • ๊ธฐ์ˆ ์„ ์ด์šฉํ•˜์—ฌ ์Šคํ•€ ํ™€ ํšจ๊ณผ์˜ ํฌ๊ธฐ ๋ฐ ๋ถ€ํ˜ธ๊ฐ€ ๋‹ค๋ฅธ ์˜์—ญ์„ ๋งŒ๋“ค์–ด ์ค€ ํŠน์ˆ˜ํ•œ ์‹œ์Šคํ…œ๋“ค์—์„œ ์–ด๋–ค ์ƒˆ๋กœ์šด ์Šคํ•€ ๋™์—ญํ•™์ด ๊ด€์ฐฐ ๋  ์ˆ˜ ์žˆ๋Š”์ง€๋ฅผ ๋ฏธ์†Œ์ž๊ธฐ์‹œ๋ฎฌ๋ ˆ์ด์…˜ (micromagnetic simulation)๊ณผ ์ด๋ก ์  ๋ถ„์„์„ ํ†ตํ•ด ์—ฐ๊ตฌํ•˜์˜€๋‹ค. ์ฑ•ํ„ฐ 2๋Š” ์ „๋ฅ˜๋กœ ๊ตฌ๋™๋˜๋Š” ์ž๊ตฌ๋ฒฝ (domain wall: DW)์ด ์–ด๋–ป๊ฒŒ ์Šคํ•€ ํ™€ ํšจ๊ณผ ์กฐ์ • ๊ฒฝ๊ณ„๋ฉด์—์„œ ํ”ผ๋‹ (pinning) ๋ฐ ๋””ํ”ผ๋‹ (depinning) ๋˜๋Š” ์ง€ ์†Œ๊ฐœํ•œ๋‹ค. ์ฃผ์–ด์ง„ ์กฐ์ • ๊ฒฝ๊ณ„๋ฉด์—์„œ์˜ ํ•œ์ชฝ ๋ฐฉํ–ฅ์œผ๋กœ ์ž๊ตฌ๋ฒฝ์„ ๋””ํ”ผ๋‹ ์‹œํ‚ค๋Š” ๋ฐฉ๋ฒ•์ด ์†Œ๊ฐœ๋˜๋ฉฐ, ์ด๋ฅผ ์ด์šฉํ•˜์—ฌ, ์ž๊ตฌ๋ฒฝ์„ ํ๋ฅด๋Š” ์ „๋ฅ˜์˜ ๋ถ€ํ˜ธ๋ฅผ ๋ฐ”๊พธ์–ด์ฃผ๋Š” ๊ฒƒ๋งŒ์œผ๋กœ ์ˆœ์ฐจ์ ์œผ๋กœ ๋‹ค์Œ ์กฐ์ • ๊ฒฝ๊ณ„๋ฉด์œผ๋กœ ํŒจ์Šคํ•ด๋‚˜๊ฐˆ ์ˆ˜ ์žˆ๋Š” ๊ตฌ์กฐ์ ์ธ ๋ฐฉ๋ฒ•์„ ๊ตฌํ˜„ํ•จ์œผ๋กœ์จ, ํ•™๊ณ„์˜ ์ฃผ์š” ๊ด€์‹ฌ์‚ฌ์ธ ๋ ˆ์ด์ŠคํŠธ๋ž™ ๋ฉ”๋ชจ๋ฆฌ์˜ ์‹คํ˜„์— ํ•œ ๊ฑธ์Œ ๋” ๋‹ค๊ฐ€๊ฐ„๋‹ค. ์ฑ•ํ„ฐ 3๋Š” ๋ณธ ๋…ผ๋ฌธ์˜ ํ•˜์ด๋ผ์ดํŠธ๋กœ์จ, ์Šคํ•€ ํ† ํฌ ์ง„๋™์ž์˜ ์ƒˆ๋กœ์šด ์ปจ์…‰์„ ๊ธฐ์šธ์–ด์ง„ ์Šคํ•€ ํ™€ ํšจ๊ณผ ์กฐ์ • ๊ฒฝ๊ณ„๋ฉด์—์„œ์˜ ์ž์„ฑ ์Šค์ปค๋ฏธ์˜จ (skyrmion)์˜ ๋™์—ญํ•™์„ ์ด์šฉํ•˜์—ฌ ๊ตฌํ˜„ํ•œ ๊ฒฐ๊ณผ๋ฅผ ์†Œ๊ฐœํ•œ๋‹ค. ์ง„๋™์ž ๊ตฌ์กฐ ๋‚ด๋ถ€์—์„œ, ์Šค์ปค๋ฏธ์˜จ์€ ์„œ๋กœ ์Šคํ•€ ํ™€ ํšจ๊ณผ์˜ ๋ถ€ํ˜ธ๊ฐ€ ๋ฐ˜๋Œ€์ธ ์Šคํ•€ ํ™€ ํšจ๊ณผ ์กฐ์ • ์˜์—ญ ์‚ฌ์ด์˜ ๊ฒฝ๊ณ„๋ฉด์„ ๋”ฐ๋ผ ๋Œ๋ฉฐ, ์ด๋Š” ๋ฏธ์†Œ์ž๊ธฐ์‹œ๋ฎฌ๋ ˆ์ด์…˜์„ ํ†ตํ•ด ํ™•์ธ๋˜์—ˆ๋‹ค. ์ƒˆ๋กœ์šด ์ปจ์…‰์ธ ์Šคํ•€ ํ™€ ํšจ๊ณผ ์กฐ์ • ์Šค์ปค๋ฏธ์˜จ ์ง„๋™์ž (spin-Hall-effect-modulation skyrmion oscillator: SHEM-SO)๋Š” ํ˜„์žฌ๊นŒ์ง€ ์ œ์‹œ๋˜์–ด ์žˆ๋Š” ์Šคํ•€ ํ† ํฌ ์ง„๋™์ž๋“ค์˜ ๋ชจ๋“  ๊ฒฐํ•จ์„ ๊ทน๋ณตํ•  ์ˆ˜ ์žˆ์„ ๊ฒƒ์œผ๋กœ ๊ธฐ๋Œ€๋œ๋‹ค. ์ฑ•ํ„ฐ 4์—์„œ๋Š” ํ˜„์žฌ ์Šคํ•€ํŠธ๋กœ๋‹‰์Šค๊ฐ€ ์ƒˆ๋กœ์ด ์—ญํ• ์„ ํ•  ๋ฐ”์ด์˜ค ๋ชจ๋ฐฉ ์‹ ๊ฒฝ ๊ณตํ•™ (neuromorphic engineering)์—์„œ ์–ป์€ ๊ฒฐ๊ณผ๋ฅผ ๊ฐ„๋žตํžˆ ์†Œ๊ฐœํ•œ๋‹ค. ์ „๋ฅ˜ ๊ตฌ๋™ ์ž๊ตฌ๋ฒฝ ์›€์ง์ž„๊ณผ ์ž๊ธฐ ํ„ฐ๋„ ํšจ๊ณผ๋ฅผ ์ด์šฉํ•˜์—ฌ, ์ ๋ถ„ ๋ฐ ๋ฐœ์‚ฌ (integrate and fire) ๊ธฐ๋Šฅ์„ ๊ตฌํ˜„ํ•œ ๋‰ด๋ก  ์žฅ๋น„๊ฐ€ ์ด๋ฏธ ์ œ์‹œ๋˜์–ด ์žˆ๋Š” ์ž๊ตฌ๋ฒฝ ์‹œ๋ƒ…์Šค ๋””๋ฐ”์ด์Šค์™€ ํ•ฉ์ณ์ ธ, ์ž๊ตฌ๋ฒฝ๋งŒ์œผ๋กœ ๊ตฌํ˜„ ๊ฐ€๋Šฅํ•œ ์ธ๊ณต ์‹ ๊ฒฝ๋ง ๊ตฌ์กฐ๊ฐ€ ์†Œ๊ฐœ๋œ๋‹ค. ์ถ”๊ฐ€์ ์œผ๋กœ, ์ž๊ธฐ ํŠน์„ฑ์„ ์ธก์ •ํ•˜๊ฑฐ๋‚˜, ์ƒˆ๋กœ์šด ์žฅ๋น„์˜ ๋””์ž์ธ ๋ฃฐ์„ ์ œ๊ณตํ•˜๋Š” ๋ฐ ๋„์›€์ด ๋  ์ˆ˜ ์žˆ๋Š” ์—ฌ๋Ÿฌ ๋ถ„์„์‹๋“ค์„ ์œ ๋„ํ•œ ๊ฒฐ๊ณผ๋ฅผ ์†Œ๊ฐœํ•œ๋‹ค. ์‚ผ๊ฐ ๋†‹์น˜ ๊ตฌ์กฐ์—์„œ์˜ ๋””ํ”ผ๋‹ ์ „๋ฅ˜์˜ ์‹๊ณผ, ์ž„์˜์˜ ์žํ™” ๊ฐ๋„์—์„œ ์Šคํ•€ ๊ถค๋„ ํ† ํฌ (spin-orbit torque)๋ฅผ ์ธก์ •ํ•˜๋Š” ๋ฐ ํ•„์š”ํ•œ ์‹๊ณผ, ๊ด‘์ž๊ธฐ ์ปฌ ํšจ๊ณผ (magneto optical Kerr effect: MOKE) ์…‹์—… ์ƒ์—์„œ ์ˆ˜์ง ๋น„๋“ฑ๋ฐฉ์„ฑ ์ž๊ธฐ์žฅ (perpendicular magneto anisotropy field)๋ฅผ ์ธก์ •ํ•˜๋Š” ๋ฐ ํ•„์š”ํ•œ ์‹ ๋“ฑ์„ ์œ ๋„ํ•œ ๊ฒฐ๊ณผ๋ฅผ ์ฑ•ํ„ฐ 5์—์„œ ๊ฐ„๋žตํžˆ ๋‹ค๋ฃฌ๋‹ค. ๋ณธ ๋…ผ๋ฌธ์— ๊ธฐ์ˆ ๋˜์–ด ์žˆ๋Š” ๋ฐœ๊ฒฌ๋“ค์€ ์Šคํ•€ ํšฐ ํšจ๊ณผ ์กฐ์ • ์‹œ์Šคํ…œ์— ๋Œ€ํ•œ ์ตœ์‹ ์˜ ์ดํ•ด๋ฅผ ์ œ๊ณตํ•œ๋‹ค. ์ด๋Ÿฐ ์‹œ์Šคํ…œ๋“ค์—์„œ ์„ค๋ช…๋˜๋Š” ์Šคํ•€ ๋™์—ญํ•™์€, ์ตœ์‹  ์Šคํ•€ํŠธ๋กœ๋‹‰์Šค ์žฅ๋น„๋“ค์˜ ๊ธฐ์ค€์„ ํ•œ ๋‹จ๊ณ„ ์—…๊ทธ๋ ˆ์ด๋“œํ•  ๋ฟ๋งŒ์ด ์•„๋‹ˆ๋ผ, ํ‹€์— ๋ฐ•ํžŒ ์Šคํ•€ํŠธ๋กœ๋‹‰์Šค ์†Œ์ž์˜ ๋””์ž์ธ ๋ฃฐ์„ ํƒ€ํŒŒํ•˜๊ณ , ์˜จ์ „ํžˆ ์ƒˆ๋กœ์šด ๋ฐฉ์‹์˜ ์ ‘๊ทผ์„ ๊ฐ€๋Šฅ์ผ€ ํ•œ๋‹ค๋Š” ์ ์—์„œ ์˜์˜๋ฅผ ๊ฐ€์ง„๋‹ค.Contents Abstract 02 List of Figures 08 1. Introduction 11 1.1 Magnetic anisotropy 13 1.2 Spin torque 14 1.2.1 Spin-transfer torque 14 1.2.2 Spin-orbit torque 17 1.2.3 Spin-Hall effect modulation 19 1.3 Magnetic structures 20 1.3.1 Domain wall 20 1.3.2 Dzyaloshinskii-Moriya interaction 22 1.3.3 Skyrmion 23 1.4 Ferrimagnetism 24 1.5 Micromagnetic simulation 26 2. Domain wall pinning/depinning at the spin-Hall-effect-modulation boundary 29 2.1 Introduction 30 2.2 Pinning at the spin-Hall-effect-modulation boundary 31 2.3 Unstable depinning at the spin-Hall-effect-modulation boundary 33 2.4 Unidirectional depinning at three different spin-Hall-effect-modulation boundaries 35 3. Spin-Hall-effect-modulation skyrmion oscillator 44 3.1 Introduction 45 3.2 Skyrmion motion at the tilted spin-Hall-effect-modulation boundary 47 3.3 Properties of the spin-Hall-effect-modulation skyrmion oscillator 51 3.4 Spin-Hall-effect-modulation skyrmion oscillator in the synthetic ferrimagnetic structure 52 3.5 Conclusion 54 3.6 Supplementary analysis 54 3.6.1 Simulation methods 54 3.6.2 Thiele formula for skyrmion motion near modulation boundary 55 3.6.3 Thiele formula for synthetic ferrimagnets 58 3.6.4 Frequency variation with respect to the angle of the modulation boundary 60 4. Domain wall neuron device 62 4.1 Introduction 63 4.2 Synapse device 66 4.3 Neuron device 67 5. Derivation of miscellaneous analytic equations 70 5.1 The analytic formula on depinning current of magnetic domain walls driven by spin-orbit torques from artificial notches 71 5.1.1 Depinning field/current from a notch 72 5.1.2 1st-order approximation for transverse spin-orbit torque 80 5.2 1st-order equation of equilibrium angle under spin-orbit torque from any initial angle 82 5.3 Optical measurement of magnetic anisotropy field in nanostructured-ferromagnetic thin films 86 6. Conclusion 94 References 96 Publication List 107 Abstract in Korean (๊ตญ๋ฌธ ์ดˆ๋ก) 108 Acknowledgments (๊ฐ์‚ฌ์˜ ๊ธ€) 111Docto
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