37 research outputs found

    Two-channel anomalous Hall effect in SrRuO3

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    The Hall effect in SrRuO3_3 thin-films near the thickness limit for ferromagnetism shows an extra peak in addition to the ordinary and anomalous Hall effects. This extra peak has been attributed to a topological Hall effect due to two-dimensional skyrmions in the film around the coercive field; however, the sign of the anomalous Hall effect in SrRuO3_3 can change as a function of saturation magnetization. Here we report Hall peaks in SrRuO3_3 in which volumetric magnetometry measurements and magnetic force microscopy indicate that the peaks result from the superposition of two anomalous Hall channels with opposite sign. These channels likely form due to thickness variations in SrRuO3_3, creating two spatially separated magnetic regions with different saturation magnetizations and coercive fields. The results are central to the development of strongly correlated materials for spintronics.This work is supported by the EPSRC through the Core-to-Core International Network โ€œOxide Superspinโ€ (EP/P026311/1) and the Doctoral Training Partnership Grant (EP/N509620/1). Additional support from the Office of Basic Energy Sciences Division of Materials Sciences and Engineering, US Department of Energy under Award numbers de-sc0018153, and the Research Center Program of IBS (Institute for Basic Science) in Korea (IBS-R009-D1)

    Honeycomb oxide heterostructure: a new platform for Kitaev quantum spin liquid

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    Kitaev quantum spin liquid, massively quantum entangled states, is so scarce in nature that searching for new candidate systems remains a great challenge. Honeycomb heterostructure could be a promising route to realize and utilize such an exotic quantum phase by providing additional controllability of Hamiltonian and device compatibility, respectively. Here, we provide epitaxial honeycomb oxide thin film Na3Co2SbO6, a candidate of Kitaev quantum spin liquid proposed recently. We found a spin glass and antiferromagnetic ground states depending on Na stoichiometry, signifying not only the importance of Na vacancy control but also strong frustration in Na3Co2SbO6. Despite its classical ground state, the field-dependent magnetic susceptibility shows remarkable scaling collapse with a single critical exponent, which can be interpreted as evidence of quantum criticality. Its electronic ground state and derived spin Hamiltonian from spectroscopies are consistent with the predicted Kitaev model. Our work provides a unique route to the realization and utilization of Kitaev quantum spin liquid

    Barrier protection via Toll-like receptor 2 signaling in porcine intestinal epithelial cells damaged by deoxynivalnol

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    Additional file 2. IPEC-J2 cells pretreated with TLR2 ligand maintained the expression of MCP-1, GM-CSF and TLR2 against DON exposure. IPEC-J2 cells pretreated with or without TLR2 ligand for 24ย h were exposed to DON. (A) The bar graph showed the mRNA levels of porcine mcp-1, gm-csf measured using real time-PCR at 1 and 6ย h after DON exposure (nย =ย 3). (B) The mRNA levels of porcine tlr2 were measured using real-time quantitative PCR analysis at 6ย h. NT represents no treatment. Expression of each mRNA was presented relative to the expression of housekeeping gene, gapdh (nย =ย 3). *Pย <ย 0.05; **Pย <ย 0.01; ***Pย <ย 0.001, determined by one-way ANOVA with Tukeyโ€™s posttest

    Tuning orbital-selective phase transitions in a two-dimensional Hund's correlated system

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    Hund's rule coupling (J\textit{J}) has attracted much attention recently for its role in the description of the novel quantum phases of multi orbital materials. Depending on the orbital occupancy, J\textit{J} can lead to various intriguing phases. However, experimental confirmation of the orbital occupancy dependency has been difficult as controlling the orbital degrees of freedom normally accompanies chemical inhomogeneities. Here, we demonstrate a method to investigate the role of orbital occupancy in J\textit{J} related phenomena without inducing inhomogeneities. By growing SrRuO3_3 monolayers on various substrates with symmetry-preserving interlayers, we gradually tune the crystal field splitting and thus the orbital degeneracy of the Ru \textit{t_2_g$}$ orbitals. It effectively varies the orbital occupancies of two-dimensional (2D) ruthenates. Via in-situ angle-resolved photoemission spectroscopy, we observe a progressive metal-insulator transition (MIT). It is found that the MIT occurs with orbital differentiation: concurrent opening of a band insulating gap in the $\textit{d$_x_y} band and a Mott gap in the \textit{d_xz_z_/y_y_z} bands. Our study provides an effective experimental method for investigation of orbital-selective phenomena in multi-orbital materials

    Original Article

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    99 cases were operated while we could not use antibiotics. The author traced X-ray photos on paper and measured areas of the peeled cavities with a planimeter. Results were as follows. 1) 66 cases had increasing stage and the rates were more than 30 %. 2) Cases with good developments showed larger original areas (50ใ€œ100cm^2) and smaller increasing rates (less than 30 %). 3) Also their X-ray photos showed coinciding or almost coinciding lines of the apices of lungs and the bases of cavities, but we had to take precautions against suppuration when they showed a horizontal line several days after operation. 4) Most of too high degree of adhesion or thickning of pleura did not show good results. When we found a cord which we must manage with some procedures by pneumolysis we must attend to suppuration too. 5)We ought to resect 4th or 5th rib more than 20 cm and 5th or 4th several cm supplementary. 6) As a method of constriction we commend the INVAGI.NATION method. 7) The author noticed in a considerable number of cases that the areas of cavities increased again after they kept long balanced stages

    Atherosclerosis V, Proceeding of the Fifth International Symposium, A.M. Gotto, L.C. Smith, B. Allen, Spring Verlag, 1979(BOOK REVIEW)

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    Antiviral effect of micafungin on three strains of human rhinoviruses. H1HeLa cells were infected with human rhinovirus type 14 (A), 21 (B), or 71 (C) (100 CCID50) and immediately treated with indicated concentrations of micafungin. Three days after compound treatment antiviral activity was determined by the reduction of cytopathic effect using MTT assay. Cell viability of DMSO-treated cells was set to 0 % and that of uninfected cells was set to 100 %. (TIF 100 kb

    ํŽ˜๋กœ๋ธŒ์Šค์นด์ดํŠธ ์ดˆ๋ฐ•๋ง‰ ๋ฃจํ…Œ๋Š„์—์„œ์˜ ์ „์ž ๊ตฌ์กฐ์— ๋Œ€ํ•œ ๊ณ„๋ฉด ์ œ์–ด

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    ํ•™์œ„๋…ผ๋ฌธ(๋ฐ•์‚ฌ) -- ์„œ์šธ๋Œ€ํ•™๊ต๋Œ€ํ•™์› : ์ž์—ฐ๊ณผํ•™๋Œ€ํ•™ ๋ฌผ๋ฆฌยท์ฒœ๋ฌธํ•™๋ถ€(๋ฌผ๋ฆฌํ•™์ „๊ณต), 2022. 8. ๋…ธํƒœ์›.Quantum materials host a variety of phenomena beyond the single-electron band theory. As strongly correlated systems, transition metal oxides (TMOs) exhibit exotic features including ferromagnetism, and unconventional superconductivity. Among TMOs, 4d ruthenates have been extensively studies due to their fine balance between electronic correlations. In such systems, the energy scales of on-site Coulomb interaction (U), Hundโ€™s rule coupling (J), and spin-orbital coupling are comparable, giving rise to a variety of functionalities. In this dissertation, we control the electronic structures of perovskite ruthentates ultrathin films by interfacial engineering. First, we investigate the orbital-selective phases in SrRuO3 (SRO) monolayers via epitaxial strain engineering. Despite vast previous theoretical studies on Hund-driven physics, experimental confirmation has been rare due to experimental difficulties. Here, we demonstrate an experimental method to systematically investigate physics in Hundโ€™s systems. The epitaxial strains modulate tetragonal crystal field, which effectively vary the orbital occupancies. Following the ambient nature of J, we observe a drastic change in electronic sturctures; a metal-insulator transition with an orbital differentiation confirmed by in-situ angle-resolved photoemission spectroscopy. We provide a practical direction for exploring multi-orbital physics as well as device applications in Hundโ€™s systems. Second, we discuss the ferromagnetic properties of ultrathin SRO with oxygen vacancy (VO). In TMOs, control of VO can give rise to many intriguing physical properties. However, inducing VO in SRO has been challenging due to volatility of Ru. Here, we utilize interfacial engineering for VO migration. By changing the growth pressure during the SrTiO3 (STO) capping layer deposition, the kinetic energy of ions arriving to the bottom SRO layer can be controlled. The high kinetic process of pulsed laser deposition (PLD) can overcome the migration energy barrier at STO/SRO and VO can be migrated into SRO. We observe VO in SRO and structural modification in SRO such as c-lattice expansion near the interface. Following, a continuous control of ferromagnetic coercive field of ultrathin SRO is achieved by controlling the amount of VO migration. We conclude that the large amount of VO induces enhancement of perpendicular magnetic anisotropy, resulting in increasing coercive field. Lastly, we investigate multiple anomalous Hall effect (AHE) interpretation in ultrathin SRO films by inducing different magnetic phases. We control the growth pressure during the LaAlO3 capping layer growth for control of the kinetic process during PLD. According to the growth pressure, two different magnetic phases in ultrathin SRO films are induced, and the composition between them can be systematically controlled. We find that the amplitude and sign of AHE change according to the composition of the magnetic phases. Our results indicate that the Berry curvature-driven AHE in ultrathin SRO films is strongly related to its magnetic properties.๊ฐ•์ƒ๊ด€๊ณ„ ๋ฌผ์งˆ์€ ๋น„ํŽ˜๋ฅด๋ฏธ ์•ก์ฒด์„ฑ, ์ดˆ์ „๋„์™€ ๊ฐ™์€ ๋…ํŠนํ•œ ํ˜„์ƒ์„ ๊ฐ€์ง„๋‹ค. ๋‹จ์ผ ์ „์ž ๋ฐด๋“œ ์ด๋ก ์œผ๋กœ๋Š” ์„ค๋ช…ํ•  ์ˆ˜ ์—†๋Š” ์ด๋Ÿฌํ•œ ํ˜„์ƒ๋“ค์„ ์ดํ•ดํ•˜๊ธฐ ์œ„ํ•ด ์ „์ž ๊ฐ„์˜ ๊ด€๊ณ„์— ๋Œ€ํ•ด ํ™œ๋ฐœํ•˜๊ฒŒ ์กฐ์‚ฌ๋˜์–ด ์™”๋‹ค. ์ „์ด ๊ธˆ์† ์‚ฐํ™”๋ฌผ์€ ๊ฐ•ํ•œ ์ƒ๊ด€๊ด€๊ณ„๊ฐ€ ์žˆ๋Š” ์‹œ์Šคํ…œ ์ค‘ ํ•˜๋‚˜์ด๋ฉฐ ๊ธˆ์†-์ ˆ์—ฐ์ฒด ์ „์ด, ๊ฐ•์ž์„ฑ ๋ฐ ์ดˆ์ „๋„์„ฑ๊ณผ ๊ฐ™์€ ํฅ๋ฏธ๋กœ์šด ํŠน์„ฑ์„ ๋ณด์ธ๋‹ค. ์ด ์ค‘ 4d ๋ฃจํ…Œ๋Š„์€ ์ „์ž์˜ ์ƒ๊ด€๊ด€๊ณ„๋ฅผ ์—ฐ๊ตฌํ•˜๊ธฐ์— ์ ํ•ฉํ•œ ์‹œ์Šคํ…œ์ด๋‹ค. ์ด ์‹œ์Šคํ…œ์—์„œ๋Š” ์ฟจ๋กฑ ์ƒํ˜ธ์ž‘์šฉ (U), ์ „์ž hopping (t), ๊ทธ๋ฆฌ๊ณ  ํ›ˆํŠธ ๋ฒ•์น™ ์ปคํ”Œ๋ง (J) ์˜ ์—๋„ˆ์ง€ ๊ทœ๋ชจ๊ฐ€ ๋น„์Šทํ•  ์ˆ˜ ์žˆ๋‹ค. ๋ณธ ํ•™์œ„ ๋…ผ๋ฌธ์—์„œ๋Š” ํŽ˜๋กœ๋ธŒ์Šค์นด์ดํŠธ ์ดˆ๋ฐ•๋ง‰ ๋ฃจํ…Œ๋Š„ ์‚ฐํ™”๋ฌผ์˜ ์ „์ž ๊ตฌ์กฐ๋ฅผ ๋ฐ•๋ง‰์˜ ๊ณ„๋ฉด ์ œ์–ด๋ฅผ ํ†ตํ•ด ์กฐ์‚ฌํ•˜์˜€๋‹ค. ์ฒซ๋ฒˆ์งธ๋กœ, ์šฐ๋ฆฌ๋Š” ์—ํ”ผํƒ์…œ ์‘๋ ฅ (epitaxial strain) ์ œ์–ด๋ฅผ ํ†ตํ•ด SrRuO3 (SRO) ํ•˜๋‚˜์˜ ์ธต์—์„œ ํ›ˆํŠธ ๋ฒ•์น™์ด ์ด๋„๋Š” ๋ชจํŠธ ์ „์ด๋ฅผ ๋ณด์—ฌ์ค€๋‹ค. ํ›ˆํŠธ ๋ฒ•์น™์ด ์ด๋„๋Š” ์ƒ๊ด€๊ด€๊ณ„์— ๋Œ€ํ•œ ์ด์ „์˜ ๋งŽ์€ ์ด๋ก  ์—ฐ๊ตฌ์—๋„ ๋ถˆ๊ตฌํ•˜๊ณ , J ๊ฐ’ ๋˜๋Š” ์˜ค๋น„ํƒˆ ๊ฐ„์˜ ์ „์ž ๋ถ„ํฌ๋ฅผ ์‹คํ—˜์ ์œผ๋กœ ์กฐ์ ˆํ•˜๊ธฐ ์–ด๋ ค์›Œ์„œ ์‹คํ—˜์  ํ™•์ธ์ด ๊ฑฐ์˜ ์—†์—ˆ๋‹ค. ์—ฌ๊ธฐ์„œ ์šฐ๋ฆฌ๋Š” J ์™€ ๊ฒฐ์ •์žฅ (crystal field) ์˜ ๊ฒฝ์Ÿ ํšจ๊ณผ๋ฅผ ํ™œ์šฉํ•˜์˜€๋‹ค. ์—ํ”ผํƒ์…œ ์‘๋ ฅ ์ œ์–ด๋Š” ์˜ค๋น„ํƒˆ ๊ฐ„์˜ ์ „์ž ๋ถ„ํฌ๋ฅผ ํšจ๊ณผ์ ์œผ๋กœ ์กฐ์ ˆํ•˜์˜€๋‹ค. ๊ทธ๋ฆฌ๊ณ , ๊ฐ๋„๋ถ„ํ•ด ๊ด‘์ „์ž ๋ถ„๊ด‘๋ฒ•์„ ์‚ฌ์šฉํ•˜์—ฌ ๋ชจํŠธ ์ „์ด๋ฅผ ๊ด€์ฐฐํ•˜์˜€๋‹ค. ์šฐ๋ฆฌ๋Š” ๋‹ค์ค‘ ์˜ค๋น„ํƒˆ ์‹œ์Šคํ…œ์—์„œ ํ›ˆํŠธ ๊ธฐ๋ฐ˜ ๋ฌผ๋ฆฌ๋ฅผ ์กฐ์‚ฌํ•˜๋Š” ํšจ๊ณผ์ ์ธ ๋ฐฉ๋ฒ•์„ ์ œ์‹œํ•˜์˜€๋‹ค. โ€ƒ ๋‘๋ฒˆ์งธ๋กœ, ์‚ฐ์†Œ ๊ฒฐ์† (oxygen vacancy) ์ด ์žˆ๋Š” ์ดˆ๋ฐ•๋ง‰ SRO ์˜ ๊ฐ•์ž์„ฑ ํŠน์„ฑ์— ๋Œ€ํ•ด ๋…ผ์˜ํ•œ๋‹ค. ์ „์ด ๊ธˆ์† ์‚ฐํ™”๋ฌผ์—์„œ ์‚ฐ์†Œ ๊ฒฐ์†์˜ ์ œ์–ด๋Š” ํฅ๋ฏธ๋กœ์šด ๋ฌผ๋ฆฌ์  ํŠน์„ฑ์„ ์ผ์œผํ‚ฌ ์ˆ˜ ์žˆ๋‹ค. ํ•˜์ง€๋งŒ SRO ์— ์‚ฐ์†Œ๊ฒฐ์†์„ ์œ ๋„ํ•˜๋Š” ๊ฒƒ์€ ๋ฃจํ…Œ๋Š„์˜ ๋†’์€ ํœ˜๋ฐœ์„ฑ์œผ๋กœ ์ธํ•ด ์–ด๋ ค์› ๋‹ค. ์—ฌ๊ธฐ์—์„œ ์šฐ๋ฆฌ๋Š” ์‚ฐ์†Œ ๊ฒฐ์† ์ด๋™์„ ์œ„ํ•ด ๊ณ„๋ฉด ์ œ์–ด๋ฅผ ํ™œ์šฉํ•˜์˜€๋‹ค. SrTiO3 (STO) ๋ฎ์Œ์ธต ์ฆ์ฐฉ ๋™์•ˆ ์„ฑ์žฅ ์••๋ ฅ์„ ๋ณ€๊ฒฝํ•จ์œผ๋กœ์จ ๋ฐ‘์— SRO ์ธต์— ๋„๋‹ฌํ•˜๋Š” ์ด์˜จ์˜ ์šด๋™ ์—๋„ˆ์ง€๋ฅผ ์ œ์–ดํ•  ์ˆ˜ ์žˆ์—ˆ๋‹ค. ํŽ„์Šค ๋ ˆ์ด์ € ์ฆ์ฐฉ (pulsed laser deposition) ๊ณผ์ • ์ค‘ ๋†’์€ ์šด๋™ ์—๋„ˆ์ง€๋Š” STO/SRO ๊ณ„๋ฉด์—์„œ ์‚ฐ์†Œ๊ฒฐ์† ์ด๋™ ์—๋„ˆ์ง€ ์žฅ๋ฒฝ์„ ๊ทน๋ณตํ•  ์ˆ˜ ์žˆ๋„๋ก ๋„์™€์ฃผ์—ˆ๋‹ค. ์šฐ๋ฆฌ๋Š” SRO ์˜ ์‚ฐ์†Œ๊ฒฐ์†๊ณผ ๊ทธ์— ๋”ฐ๋ฅธ ๊ฒฉ์ž ๋ณ€์ด๋ฅผ ๊ด€์ฐฐํ•˜์˜€๋‹ค. ๊ทธ๋ฆฌ๊ณ  ์ดˆ๋ฐ•๋ง‰ SRO ์˜ ๋ณด์ž๋ ฅ (coercive field) ์˜ ์ง€์†์ ์ธ ์ œ์–ด๋ฅผ ์‚ฐ์†Œ๊ฒฐ์† ์ด๋™๋Ÿ‰์„ ์ œ์–ดํ•˜์—ฌ ๋‹ฌ์„ฑํ•˜์˜€๋‹ค. ๋˜ํ•œ ์šฐ๋ฆฌ๋Š” ๋งŽ์€ ์–‘์˜ ์‚ฐ์†Œ ๊ฒฐ์†์ด ์ˆ˜์ง ์ž๊ธฐ ์ด๋ฐฉ์„ฑ์„ ๋†’์ด๋Š” ๊ฒƒ์„ ํ™•์ธํ•˜์˜€๋‹ค. ๋งˆ์ง€๋ง‰์œผ๋กœ, ์šฐ๋ฆฌ๋Š” ์„œ๋กœ ๋‹ค๋ฅธ ์ž๊ธฐ ์ƒ (phase) ์„ ์œ ๋„ํ•˜์—ฌ ์ดˆ๋ฐ•๋ง‰ SRO ์—์„œ ๋‹ค์ค‘ ๋น„์ •์ƒ ํ™€ ํšจ๊ณผ๋ฅผ ์กฐ์‚ฌํ•˜์˜€๋‹ค. LaAlO3 ๋ฎ์Œ์ธต ์„ฑ์žฅ ๋™์•ˆ ์••๋ ฅ์„ ์ œ์–ดํ•˜์—ฌ ์šด๋™์—๋„ˆ์ง€๋ฅผ ์กฐ์ ˆํ•˜์˜€๋‹ค. ์„ฑ์žฅ ์••๋ ฅ์— ๋”ฐ๋ผ SRO ํ•„๋ฆ„์—์„œ ๋‘ ๊ฐœ์˜ ์„œ๋กœ ๋‹ค๋ฅธ ์ž๊ธฐ ์ƒ์ด ์œ ๋„๋˜์—ˆ๊ณ , ์ด๋“ค ์‚ฌ์ด์˜ ๋น„์œจ์€ ์ฒด๊ณ„์ ์œผ๋กœ ์ œ์–ดํ•  ์ˆ˜ ์žˆ์—ˆ๋‹ค. ์šฐ๋ฆฌ๋Š” ๋น„์ •์ƒ ํ™€ ํšจ๊ณผ์˜ ํฌ๊ธฐ์™€ ๋ถ€ํ˜ธ๊ฐ€ ์ž๊ธฐ ์ƒ์˜ ๊ตฌ์„ฑ์— ๋”ฐ๋ผ ๋ณ€ํ•œ๋‹ค๋Š” ๊ฒƒ์„ ๋ฐœ๊ฒฌํ•˜์˜€๋‹ค. ์ด ๊ฒฐ๊ณผ๋Š” ์ดˆ๋ฐ•๋ง‰ SRO ํ•„๋ฆ„์˜ ๋น„์ •์ƒ ํ™€ ํšจ๊ณผ๊ฐ€ ์ž๊ธฐ ํŠน์„ฑ๊ณผ ๋ฐ€์ ‘ํ•œ ๊ด€๋ จ์ด ์žˆ์Œ์„ ๋‚˜ํƒ€๋‚ธ๋‹ค.Contents List of Figures Abstract Chapter 1. Introduction Chapter 2. Experimental Methods Chapter 3. Orbital-selective phase transition in a two-dimensional correlated system Chapter 4. Hetero-interfacial control for oxygen vacancy migration Chapter 5. Hetero-interfacial control for two-channel anomalous Hall effect Chapter 6. Summary and Outlook List of Publication ๊ตญ๋ฌธ ์ดˆ๋ก (Korean Abstract)๋ฐ•

    In-operando spectroscopic ellipsometry studies of IrO2 dynamic instabilities: Guide to in-situ growth of pyrochlore iridate thin films

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    The instability of iridium oxide at high temperature has long been a bottleneck for in growing pyrochlore iridate thin films in a vacuum chamber. To overcome this problem, we investigated the chemical instability of IrO2 thin films, which are the simplest form of iridate, via in-operando spectroscopic ellipsometry (SE). We observed that IrO2 thin films undergo IrO2 dissociation and IrO3 gas formation depending on the thermodynamic conditions. The chemical kinetics observations of IrO2 were confirmed by ex-situ X-ray diffraction and atomic force microscopy. SE experimental data were compared with models used to describe the evolution of the two chemical reactions. Real-time in-operando SE analysis based on the Maxwell Garnett theory yielded a precise IrO2 dissociation speed for the given thermodynamic conditions. Moreover, the real-time in-operando SE technique allowed us to observe the phase transition from solid IrO2 to gaseous IrO3. This study on the chemical instability of IrO2 at high temperature affords insights into a new method for in-situ pyrochlore iridate and other iridates thin-film growth. ยฉ 2019 Korean Physical Society. Published by Elsevier B.V. All rights reserved

    Controllable Thickness Inhomogeneity and Berry Curvature Engineering of Anomalous Hall Effect in SrRuO3 Ultrathin Films

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    In quantum matters hosting electronโˆ’electron correlation and spinโˆ’orbit coupling, spatial inhomogeneities, arising from competing ground states, can be essential for understanding exotic topological properties. A prominent example is Hall anomalies observed in SrRuO 3 films, which were interpreted in terms of either magnetic skyrmion-induced topological Hall effect or inhomogeneous anomalous Hall effect (AHE). To clarify this ambiguity, we systematically investigated the evolution of AHE with controllable inhomogeneities in SrRuO 3 film thickness (t SRO ). By exploiting the step-flow growth of SrRuO 3 films, we induced a microscopically ordered stripe pattern with one-unit-cell differences in t SRO . The associated spatial distribution of momentum-space Berry curvatures enables a two-channel AHE with hump-like Hall anomalies, which can be continuously engineered according to non-integer t SRO . We further microscopically characterized the stripe-like ferromagnetic domains and two-step magnetic switching behavior in the inhomogeneous SrRuO 3 film. These unique features can be utilized to identify the two-channel AHE model and understand its microscopic origin. ยฉ 2020 American Chemical Society11Nsciescopu
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