• 제목/요약/키워드: magnetic moment

검색결과 325건 처리시간 0.024초

W(110)위에 성장한 Fe 웃층의 전자 및 자기적 성질 (The Electronic and Magnetic Properties of Fe Overlayers on W(110))

  • 홍순철;이재일
    • 한국자기학회지
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    • 제1권2호
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    • pp.1-8
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    • 1991
  • 비자성 천이금속인 W의 (110)표면 위에 성장한 강자성 Fe 원자층의 전자적 성질 및 자기적 성질을 국소밀도근사 범위 내의 Full Potential Linearized Augmented Plane Wave (FLAPW) 방법을 이용하여 계산하였다. 이 계산에서 W, Fe의 층간 거리는 bull값을 이용하였으며 표면이완 및 계면이완은 고려하지 않았다. 전하밀도, 스핀밀도, 자기 모멘트, 접촉 초미세장, 2차원 띠구조, 각층의 상태밀도 등의 계산결과를 제시하였다. Fe 웃층이 1층인 경우, Fe의 자기모멘트는 2.56 ${\mu}_B$로 bulk에 비해 16% 증가하였고, Fe 웃층이 2층인 경우 표면 및 계면을 이루는 Fe층의 자기 모멘트는 각각 2.90과 2.30 ${\mu}_B$로 평균 자기모멘트는 bulk에 비해 약 18% 증가한 것으로 나타났다. Fe 층수가 1층일 때 자기초미세장의 크기는 2층일 때와는 큰 차이를 보여주고 있다. 깨끗한 Fe(110)의 결과와 비교함으로써 W과의 띠혼합 효과와 격자상수 확장 효과에 대해 논의하고 실험결과의 계산결과를 비교 검토하여 보았다.

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The Enhanced Magnetic Transition Temperature in Double Perovskites A2FeMoO6 (A=Ca, Sr and Ba) : Electron Doping Effects

  • Kim J.;Yang H. M.;Lee B. W.
    • Journal of Magnetics
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    • 제10권1호
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    • pp.10-13
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    • 2005
  • We have studied effects of the partial substitution of $La^{3+}$ for $A^{2+}$ on the magnetic properties of double perovskites $A_2FeMoO_6$ (A=Ca, Sr and Ba). Polycrystalline $A_{2-x}La_xFeMoO_6(0{\leq}x{\leq}0.2)$ samples have been prepared by the conventional solid-state reaction in a stream of 5% $H_2$/Ar gas. The x-ray data indicate that A=Ca is monoclinic with the space group P$2_1$/n, A=Sr is tetragonal with the space group I4/mmm, and A=Ba is cubic with the space group Fm3m. The substitution of $La^{3+}$ for $A^{2+}$ results in a cell volume increase for A=Ca and a cell volume reduction for A=Ba. The decrease of saturation magnetization with increasing x arises from the reduction of magnetic moment associated with the electron doping and the disorder at the Fe and Mo sites. The partial substitution of magnetic $La^{3+}$ for $A^{2+}$ considerably enhances the Curie temperature $T_c$ from 316 K for x = 0 to 334 K for x = 0.2. This enhancement of $T_c$ with $La^{3+}$ doping originates from electron doping effects in addition to ionic size ones.

전기자 형태의 회전자를 갖는 하이브리드 마그네틱 기어의 구조에 관한 연구 (A Study on the Structure of Hybrid Magnetic Gear with Armature Type Rotor)

  • 김찬승;박의종;김용재
    • 한국전자통신학회논문지
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    • 제13권6호
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    • pp.1235-1242
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    • 2018
  • 풍속이 급변할 경우 전력계통 시스템과 기계시스템의 안전을 위해 풍력발전기를 제동시킨다. 이 때, 풍력발전기 내부의 기어박스에서 기어 이의 접촉하중으로 인한 기어의 손상 및 파손이 발생하며, 브레이크를 이용한 제동 시 블레이드의 동력을 그대로 전달받아 마찰열 상승, 브레이크의 성능 저하 등의 문제가 있다. 본 논문은 풍력 발전 시스템의 동력전달장치인 기계식 기어의 접촉에 의한 문제를 해결하기 위해 동력 차단 시스템을 결합시킨 하이브리드 마그네틱 기어의 형상을 제안한다. 이차원 유한해석법을 활용하여 하이브리드 마그네틱 기어의 형상에 따른 토크와 손실 분석을 통해 풍력발전 시스템에 적합한 하이브리드 마그네틱 기어의 형상을 도출하였다.

Pd층의 두께 변화에 따른 [Co/Pd] 다층박막의 연엑스선 방사광 분광 연구 (Soft X-ray Synchrotron-Radiation Spectroscopy Study of [Co/Pd] Multilayers as a Function of the Pd Sublayer Thickness)

  • 김대현;이은숙;김현우;성승호;강정수;양승모;박해수;홍진표
    • 한국자기학회지
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    • 제26권4호
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    • pp.124-128
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    • 2016
  • 이 연구에서는 연 X선 광흡수 분광법(soft X-ray absorption spectroscopy: XAS)과 연 X선 자기 원편광 이색성(soft X-ray magnetic circular dichroism: XMCD)을 이용하여 수직자기이방성을 보이는 [$Co(2{\AA})/Pd(x{\AA})$] 형의 다층박막의 전자구조를 연구하였다(x = $1{\AA}$, $3{\AA}$, $5{\AA}$, $7{\AA}$, $9{\AA}$). Co 2p XAS와 XMCD 스펙트럼은 Pd 층의 두께 변화에 상관없이 서로 매우 유사하였으며, 또한 Co 금속의 Co 2p XAS와 XMCD 스펙트럼과도 매우 유사함이 관찰되었는데, 이러한 결과는 [$Co(2{\AA})/Pd(x{\AA})$] 다층박막에서 Co 이온들이 금속 결합을 하고 있다는 사실을 보여 준다. Co 2p XMCD 스펙트럼을 분석하여 두께에 따른 궤도 자기모멘트(orbital magnetic moment)와 스핀 자기모멘트(spin magnetic moment) 의 크기를 결정하였다. 이 결과에 의하면 Pd 층의 두께(x)가 $1{\AA}$에서 $3{\AA}$으로 증가할 때, 궤도 자기모멘트가 가장 크게 증가하였으며, $x{\geq}3{\AA}$ 이상의 영역에서는 별 다른 변화가 없었다. 이러한 결과는 [$Co(2{\AA})/Pd(x{\AA})$] 다층박막의 계면에서의 스핀-궤도 상호작용이 수직자기 이방성에 매우 중요한 역할을 한다는 사실을 나타낸다.

Synthesis, Spectral, Characterization, DFT and Biological Studies of New 3-[(3-Chlorophenyl)-hydrazono]-pentane-2,4-dione Metal Complexes

  • Sadeek, Sadeek A.;Zordok, Wael A.;El-Farargy, Ahmed F.;El-Desoky, Sameh I.
    • 대한화학회지
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    • 제58권2호
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    • pp.169-178
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    • 2014
  • A new series of metal complexes of V(IV), Pd(II), Pt(IV), Ce(IV) and U(VI) with 3-[(3-chlorophenyl)-hydrazono]-pentane-2,4-dione (Cphpd) were synthesized and characterized by elemental analysis, molar conductivity, magnetic moment measurements, UV-vis, FT-IR and $^1H$ NMR as well as TG-DTG techniques. The data indicated that the Cphpd acts as a bidentate ligand through the hydrazono nitrogen and one keto oxygen. The kinetic parameters have been evaluated by using Coats Redfern (CR) and Horowitz-Metzeger (HM) methods. The thermodynamic data reflected the thermal stability for all complexes. The calculated bond length and the bond stretching force constant, F(U=O), values for $UO_2$ bond are $0.775{\AA}$ and $286.95Nm^{-1}$. The bond lengths, bond angles, dipole moment and the lowest energy model structure of the complexes have been determined with DFT calculations. The antimicrobial activity of the synthesized ligand and its complexes were screened.

New Unsymmetric Dinuclear Copper(II) Complexes of Trans-disubstituted Cyclam Derivatives: Spectral, Electrochemical, Magnetic, Catalytic, Antimicrobial, DNA Binding and Cleavage Studies

  • Prabu, R.;Vijayaraj, A.;Suresh, R.;Jagadish, L.;Kaviyarasan, V.;Narayanan, V.
    • Bulletin of the Korean Chemical Society
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    • 제32권5호
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    • pp.1669-1678
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    • 2011
  • Six new binuclear copper(II) complexes have been prepared by template condensation of the dialdehydes 1,8-[bis(3-formyl-2-hydroxy-5-methyl)benzyl]-l,4,8,11-tetraazacyclotetradecane (PC-a) and 1,8-[bis(3-formyl-2-hydroxy-5-bromo)benzyl]-l,4,8,11-tetraazacyclotetradecane (PC-b) with appropriate aliphatic diamines, and copper(II) perchlorate. The structural features of the complexes have been confirmed by elemental analysis, IR, UV-vis and mass spectra etc. The electrochemical behavior of all the copper(II) complexes show two irreversible one electron reduction process. The room temperature magnetic moment studies depict the presence of an antiferromagnetic interaction in the binuclear complexes. The catechol oxidation and hydrolysis of 4-nitrophenylphosphate were carried out by using the complexes as catalyst. The antimicrobial screening data show good results. The binding of the complexes to calf thymus DNA (CT DNA) has been investigated with absorption and emission spectroscopy. The complex [$Cu_2L^{1a}$] displays significant cleavage property of circular plasmid pBR322 DNA in to linear form. Spectral, electrochemical, magnetic and catalytic studies support the distortion of the copper ion geometry that arises as the macrocyclic ring size increases.

Crystallographic and Magnetic Properties of Nano-sized Nickel Substituted Cobalt Ferrites Synthesized by the Sol-gel Method

  • Choi, Won-Ok;Lee, Jae-Gwang;Kang, Byung-Sub;Chae, Kwang Pyo
    • Journal of Magnetics
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    • 제19권1호
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    • pp.59-63
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    • 2014
  • Nano-sized nickel substituted cobalt ferrite powders, $Ni_xCo_{1-x}Fe_2O_4$ ($0.0{\leq}x{\leq}1.0$), were fabricated by the sol-gel method, and their crystallographic and magnetic properties were studied. All the ferrite powders showed a single spinel structure, and behaved ferrimagnetically. When the nickel substitution was increased, the lattice constants and the sizes of particles of the ferrite powders decreased. The M$\ddot{o}$ssbauer absorption spectra of $Ni_xCo_{1-x}Fe_2O_4$ ferrite powders could be fitted with two six-line subspectra, which were assigned to a tetrahedral A-site and octahedral B-sites of a typical spinel crystal structure. The increase in values of the magnetic hyperfine fields indicated that the superexchange interaction was stronger, with the increased nickel concentration in $Ni_xCo_{1-x}Fe_2O_4$. This could be explained using the cation distribution, which can be written as, $(Co_{0.28-0.28x}Fe_{0.72+0.28x})[Ni_xCo_{0.72-0.72x}Fe_{1.28-0.28x}]O_4$. The two values of the saturation magnetization and the coercivity decreased, as the rate of nickel substitution was increased. These decreases could be explained using the cation distribution, the magnetic moment, and the magneto crystalline anisotropy constant of the substituted ions.

Effect of Ni dopant on the multiferroicity of BiFeO3 ceramic

  • Hwang, J.S.;Yoo, Y.J.;Kang, J.H.;Lee, K.H.;Lee, B.W.;Park, S.Y.;Lee, Y.P.
    • 한국진공학회:학술대회논문집
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    • 한국진공학회 2016년도 제50회 동계 정기학술대회 초록집
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    • pp.139.1-139.1
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    • 2016
  • Multiferroic materials are of great interest because of its potential applications in the design of devices combining magnetic, electronic and optical functionalities. Among various multiferroic materials, $BiFeO_3$(BFO) is known to be one of the intensively focused mainly due to the possibility of multiferroism at device working temperature (> $200^{\circ}C$). However, leakage current and weak polarization resulting from oxygen deficiency and crystalline defect should be resolved. Furthermore the magnetic ordering of pure BFO mainly prefers to have antiferromagnetic coupling. Up to now many attempts have been performed to improve the ferromagnetic and the ferroelectric properties of BFO by doping. In this work, we investigated the effects of Ni substitution on the multiferroism of bulk BFO. Four BFO samples (a pure BFO and three Ni-doped BFO's; $BiFe_{0.99}Ni_{0.01}O_3$, $BiFe_{0.98}Ni_{0.02}O_3$ and $BiFe_{0.97}Ni_{0.03}O_3$) were synthesized by the standard solid-state reaction and rapid sintering technique. The XRD results reveal that Ni atoms are substituted into Fe-sites and give rise to phase transition of cubic to rhombohedal. By using vibrating sample magnetometer and standard ferroelectric tester, the multiferroic properties at room temperature were characterized. We found that the magnetic moment of Ni-doped BFO turned out to be maximized for 3% of Ni dopant.

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Mössbauer Study of Ti0.9957Fe0.01O2

  • Kim, Eng-Chan;Moon, S.H.;Woo, S.I.;Kim, H.D.;Kim, B.Y.;Cho, J.H.;Joh, Y.G.;Kim, D.H.
    • 한국자기학회지
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    • 제15권2호
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    • pp.106-108
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    • 2005
  • The rutile polycrystal $Ti_{0.99}\;^{57}Fe_{0.01}O_2$ prepared with $^{57}Fe$ enriched iron have been studied by $M\ddot{o}ssbauer$ spectroscopy, X-ray diffraction and VSM. The $M\ddot{o}ssbauer$ spectrum of $Ti_{0.99}\;^{57}Fe_{0.01}O_2$ consists of a ferromagnetic and a paramagnetic phase over all temperature ranging from 4 to 300 K. Isomer shifts indicate $Fe^{2+}$ for the ferromagnetic phase, but $Fe^{3+}$ for the paramagneic phase of $Ti_{0.99}\;^{57}Fe_{0.01}O_2$ sample. It is noted that the magnetic hyperfine field of ferromagnetic phase had the value about 1.48 times as large as that of $\alpha$-Fe. The XRD data for $Ti_{0.99}\;^{57}Fe_{0.01}O_2$ showed a pure rutile phase with tetragonal structures without any segregation of Fe into particulates within the instrumental resolution limit The magnetic hysteresis (M-H) curve at room temperature showed an obvious ferromagnetic behavior and the magnetic moment per Fe atom under the applied field of 1 T was estimated to be about $0.71{\mu}_B$, suggesting a low spin configuration of Fe ions.

Structural Phase Transition, Electronic Structure, and Magnetic Properties of Sol-gel-prepared Inverse-spinel Nickel-ferrites Thin Films

  • Kim, Kwang Joo;Kim, Min Hwan;Kim, Chul Sung
    • Journal of Magnetics
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    • 제19권2호
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    • pp.111-115
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    • 2014
  • X-ray diffraction (XRD), X-ray photoelectron spectroscopy (XPS), and vibrating sample magnetometry (VSM) were used to investigate the influence of Ni ions on the structural, electronic, and magnetic properties of nickel-ferrites ($Ni_xFe_{3-x}O_4$). Spinel $Ni_xFe_{3-x}O_4$ ($x{\leq}0.96$) samples were prepared as polycrystalline thin films on $Al_2O_3$ (0001) substrates, using a sol-gel method. XRD patterns of the nickel-ferrites indicate that as the Ni composition increases (x > 0.3), a structural phase transition takes place from cubic to tetragonal lattice. The XPS results imply that the Ni ions in $Ni_xFe_{3-x}O_4$ substitute for the octahedral sites of the spinel lattice, mostly with the ionic valence of +2. The minority-spin d-electrons of the $Ni^{2+}$ ions are mainly distributed below the Fermi level ($E_F$), at around 3 eV; while those of the $Fe^{2+}$ ions are distributed closer to $E_F$ (~1 eV below $E_F$). The magnetic hysteresis curves of the $Ni_xFe_{3-x}O_4$ films measured by VSM show that as x increases, the saturation magnetization ($M_s$) linearly decreases. The decreasing trend is primarily attributable to the decrease in net spin magnetic moment, by the $Ni^{2+}$ ($2{\mu}_B$) substitution for octahedral $Fe^{2+}$ ($4{\mu}_B$) site.