37 research outputs found

    The 2020 magnetism roadmap

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    Following the success and relevance of the 2014 and 2017 Magnetism Roadmap articles, this 2020 Magnetism Roadmap edition takes yet another timely look at newly relevant and highly active areas in magnetism research. The overall layout of this article is unchanged, given that it has proved the most appropriate way to convey the most relevant aspects of today's magnetism research in a wide variety of sub-fields to a broad readership. A different group of experts has again been selected for this article, representing both the breadth of new research areas, and the desire to incorporate different voices and viewpoints. The latter is especially relevant for thistype of article, in which one's field of expertise has to be accommodated on two printed pages only, so that personal selection preferences are naturally rather more visible than in other types of articles. Most importantly, the very relevant advances in the field of magnetism research in recent years make the publication of yet another Magnetism Roadmap a very sensible and timely endeavour, allowing its authors and readers to take another broad-based, but concise look at the most significant developments in magnetism, their precise status, their challenges, and their anticipated future developments. While many of the contributions in this 2020 Magnetism Roadmap edition have significant associations with different aspects of magnetism, the general layout can nonetheless be classified in terms of three main themes: (i) phenomena, (ii) materials and characterization, and (iii) applications and devices. While these categories are unsurprisingly rather similar to the 2017 Roadmap, the order is different, in that the 2020 Roadmap considers phenomena first, even if their occurrences are naturally very difficult to separate from the materials exhibiting such phenomena. Nonetheless, the specifically selected topics seemed to be best displayed in the order presented here, in particular, because many of the phenomena or geometries discussed in (i) can be found or designed into a large variety of materials, so that the progression of the article embarks from more general concepts to more specific classes of materials in the selected order. Given that applications and devices are based on both phenomena and materials, it seemed most appropriate to close the article with the application and devices section (iii) once again. The 2020 Magnetism Roadmap article contains 14 sections, all of which were written by individual authors and experts, specifically addressing a subject in terms of its status, advances, challenges and perspectives in just two pages. Evidently, this two-page format limits the depth to which each subject can be described. Nonetheless, the most relevant and key aspects of each field are touched upon, which enables the Roadmap as whole to give its readership an initial overview of and outlook into a wide variety of topics and fields in a fairly condensed format. Correspondingly, the Roadmap pursues the goal of giving each reader a brief reference frame of relevant and current topics in modern applied magnetism research, even if not all sub-fields can be represented here. The first block of this 2020 Magnetism Roadmap, which is focussed on (i) phenomena, contains five contributions, which address the areas of interfacial Dzyaloshinskii-Moriya interactions, and two-dimensional and curvilinear magnetism, as well as spin-orbit torque phenomena and all optical magnetization reversal. All of these contributions describe cutting edge aspects of rather fundamental physical processes and properties, associated with new and improved magnetic materials' properties, together with potential developments in terms of future devices and technology. As such, they form part of a widening magnetism 'phenomena reservoir' for utilization in applied magnetism and related device technology. The final block (iii) of this article focuses on such applications and device-related fields in four contributions relating to currently active areas of research, which are of course utilizing magnetic phenomena to enable specific functions. These contributions highlight the role of magnetism or spintronics in the field of neuromorphic and reservoir computing, terahertz technology, and domain wall-based logic. One aspect common to all of these application-related contributions is that they are not yet being utilized in commercially available technology; it is currently still an open question, whether or not such technological applications will be magnetism-based at all in the future, or if other types of materials and phenomena will yet outperform magnetism. This last point is actually a very good indication of the vibrancy of applied magnetism research today, given that it demonstrates that magnetism research is able to venture into novel application fields, based upon its portfolio of phenomena, effects and materials. This materials portfolio in particular defines the central block (ii) of this article, with its five contributions interconnecting phenomena with devices, for which materials and the characterization of their properties is the decisive discriminator between purely academically interesting aspects and the true viability of real-life devices, because only available materials and their associated fabrication and characterization methods permit reliable technological implementation. These five contributions specifically address magnetic films and multiferroic heterostructures for the purpose of spin electronic utilization, multi-scale materials modelling, and magnetic materials design based upon machine-learning, as well as materials characterization via polarized neutron measurements. As such, these contributions illustrate the balanced relevance of research into experimental and modelling magnetic materials, as well the importance of sophisticated characterization methods that allow for an ever-more refined understanding of materials. As a combined and integrated article, this 2020 Magnetism Roadmap is intended to be a reference point for current, novel and emerging research directions in modern magnetism, just as its 2014 and 2017 predecessors have been in previous years

    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

    Ferrimagnetic rare-earth-transition-metal heterostructures: implications for future data storage, sensors, and unconventional computing

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    In this work, different ferrimagnetic rare-earth-transition-metal heterostructures are investigated. The findings provide implications for future data storage, sensor, and unconventional computing devices. In the first part, ferri- and ferromagnetic films are exchange-coupled and studied as potential composite media for magnetic recording technologies. For this, the underlying individual layers are examined, too. Within this study, the influence of Pd and Pt insertion layers in ferromagnetic Co/Ni multilayers is investigated. In these systems, the maximum effective magnetic anisotropy is more than doubled by the introduced insertion layers, while the initial saturation magnetization and Curie temperature are reduced. Further, amorphous Tb-FeCo alloys and multilayers are studied as the second building block of the desired composite medium. In particular, the structural and magnetic properties are analyzed upon post-annealing. At temperatures above 400 K, irreversible effects on the structural properties are found, which also influence the magnetic properties. It is shown that these changes in properties cannot be prevented by tuning the composition or by a multilayer structure of the film. However, key insights on the structural and magnetic properties upon annealing are provided for future high-temperature devices. Afterward, the exchange-coupled ferrimagnetic/ferromagnetic bilayer is studied. Measurements on the dependency on temperature, the ferrimagnetic composition, and the thickness of the ferromagnet are carried out. Two distinct magnetic reversal mechanisms are revealed. The reversal characteristics depend critically on the thickness of the ferromagnetic layer. The underlying microscopic origin is revealed by high-resolution magnetic force microscopy. Above a certain thickness of the ferromagnet, the switching process is driven by in-plane domain wall propagation. In contrast, thinner ferromagnetic layers exhibit a nucleation-dominated reversal due to grain-to-grain variations in magnetic anisotropy. Although the realization of an exchange-coupled composite medium for magnetic recording can not be achieved, insights for the future realization of sub micron high energy density permanent magnets and spintronic devices are gained. In the second part of this work, topologically protected spin structures, including skyrmions and antiskyrmions, are investigated in Fe/Gd-based multilayers. Particularly in coexisting phases, different topologically protected magnetic quasi-particles may show fascinating physics and potential for spintronic devices. While skyrmions are observed in a wide range of materials, until now, antiskyrmions have been exclusive to materials with D2d or S4 symmetry. In this work, first and second-order antiskyrmions are stabilized for the first time by magnetic dipole-dipole interaction. Using Lorentz transmission electron microscopy imaging, coexisting first- and second-order antiskyrmions, Bloch skyrmions, and type-2 bubbles are observed, and the range of material properties and magnetic fields where the different spin objects form and dissipate is determined. The discovered phase pocket of metastable antiskyrmions for low saturation magnetization and uniaxial magnetic anisotropy values is confirmed by micromagnetic simulations and represents a recipe, which has to be satisfied for the stabilization of antiskyrmions by dipole-dipole interaction in other material systems. Furthermore, the nucleation process of the spin objects and the influence of an in-plane magnetic field are studied. Additionally, post-deposition techniques are employed to locally change the anisotropy of the samples and influence the nucleation and stability range of the spin objects. The gained knowledge significantly simplifies future investigations of antiskyrmions. Moreover, the coexisting phases of different topologically protected spin objects and their controlled nucleation provide great potential for further studies on magnetic quasi-particle interactions, spin dynamics, as well as for possible future applications in spintronics, namely the racetrack memory, skyrmionic interconnections, skyrmion-based unconventional computing, and sensor devices

    Quantum materials for energy-efficient neuromorphic computing

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    Neuromorphic computing approaches become increasingly important as we address future needs for efficiently processing massive amounts of data. The unique attributes of quantum materials can help address these needs by enabling new energy-efficient device concepts that implement neuromorphic ideas at the hardware level. In particular, strong correlations give rise to highly non-linear responses, such as conductive phase transitions that can be harnessed for short and long-term plasticity. Similarly, magnetization dynamics are strongly non-linear and can be utilized for data classification. This paper discusses select examples of these approaches, and provides a perspective for the current opportunities and challenges for assembling quantum-material-based devices for neuromorphic functionalities into larger emergent complex network systems
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