• Title/Summary/Keyword: surface magneto-optic Kerr effect

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표면 자기광 커 효과의 이해 (Understanding the Surface Magneto-optic Kerr Effect)

  • 황찬용
    • 한국자기학회지
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    • 제21권4호
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    • pp.141-146
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    • 2011
  • 지난 20여년간 표면자성 현상의 연구에 가장 도움이 많이 되었던 실험방법중 하나인 표면 자기광 커효과(Surface magneto-optic Kerr effect, SMOKE) 실험 방법을 소개하고자 한다. 예를 들어 단일층의 철막이 강자성이 되는지, 또 큐리(Curie)온도는 bulk와 비교하여 얼마나 떨어져 있는지, 자화 용이축(easy-axis)은 어느 방향인지 등 매우 기본적인 자성박막의 특성은 스핀트로닉스(spintronics) 분야의 연구에 가장 기본적인 정보이다. 표면 자기광 커 효과(SMOKE)는 이러한 물음에 대한 답을 줄 수 있는 매우 효율적인 방법이다.

Magnetic and structural properties of ultrathin magnetic films: Ni/Pt(111)

  • Nahm, T.U.;Oh, S.J.
    • 한국진공학회지
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    • 제12권S1호
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    • pp.17-20
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    • 2003
  • We have studied magnetic and structural properties of ultrathin Ni films grown on PI(lII) surface using in situ surface magneto-optic Kerr effect and X-ray photoelectron spectroscopy. Perpendicular magnetic anisotropy was absent, and longitudinal Kerr signal was only detectable for Ni films thicker than 6 monolayers. Enhancement in longitudinal Kerr signal by 30% was achieved by post-annealing at temperatures below 800K, but upon annealing at 820K, surface alloy was formed. By using core-level binding-energy shifts, the composition was determined to be Ni 70 at. %.

Morphology and Surface Magnetism of Ultrathin Fe Films on Pd(111)

  • Park, Jae-Hoon;Kim, Wookje;Kim, Wondong;Kim, Jae-Young;Hoon Koh;S.J. Oh
    • 한국진공학회:학술대회논문집
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    • 한국진공학회 2000년도 제18회 학술발표회 논문개요집
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    • pp.141-141
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    • 2000
  • In situ surface magneto-optic Kerr effect(SMOKE), X-ray photoelectron spectroscopy(XPS) and low energy electron diffraction(LEED) were used to study magnetic and structural properties of ultrathin Fe films grown on the Pd(111) surface. The SMOKE measurement showed strong enhancement of ferromagnetism after proper annealing process. Simultaneous changes in morphology was checked by LEED and XPS. After room temperature Fe deposition. longitudinal magnetization appeared above a critical thickness between 2.0 and 2.5 monolayers. When annealed at 450K, 2.0 monolayer Fe film exhibited boty longitudinal and polar magnetizations while 3.0 and 5.5 monolayer films showed little changes. After annealing at 600K, both magnetizations were totally destroyed in 2.0 monolayer film, but longitudinal magnetization was enhanced in 3.0 monolayer film. In the case of 5.5 monolayer film, it was only after 660K annealing that the enhancement of the longitudinal magnetization was observed. It was concluded that the surface flatness and the amount of intermixing were critical in the development of surface magnetism of this system.

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ARPES study of Ultrathin Fe Grown on Cu (001) surface

  • Poornima, L.;Oh, Y.R.;Park, Y.S.;Kim, W.;Kim, C.G.;Hong, J.;Hwang, Chan-Yong
    • 한국진공학회:학술대회논문집
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    • 한국진공학회 2011년도 제40회 동계학술대회 초록집
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    • pp.350-350
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    • 2011
  • The spin structure of Fe over layers on Cu (001), especially in region II is one of the unsolved problem for many years. We study the out - of - plane (OP) Fermi surfaces (FSs) of 7 monolayer Fe/Cu (001) films using angle resolved photo emission spectroscopy (ARPES). Ultrathin Fe was grown on Cu (001) substrate at room temperature and the experimental measurements were carried out at room temperature and low temperature. Fermi surfaces measured about $\frac{1}{4}$ of the Brillouin Zone (BZ) using photon energies ranging from 170 eV to 280 eV. Our results confirmed that ferromagnetic signal at 7 ML Fe on Cu (001) is nearly zero. These results are consistent with our recent x-ray magnetic circular dichroism (XMCD) and surface magneto - optic Kerr effect (SMOKE) experiments. Based on our observations we have made a simple model of this system, which explains all the experimental results.

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The Effect of Cr Dosage on FePt Nanoparticle Formation

  • Won, C.;Keavney, D.J.;Divan, R.;Bader, S.D.
    • Journal of Magnetics
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    • 제11권4호
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    • pp.182-188
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    • 2006
  • The search for high-density recording materials has been one of most active and vigorous field in the field of magnetism. $FePt-L1_{0}$ nanoparticle has emerged as a potential candidate because of its high anisotropy. In this paper, we provide an overview of recent work at Argonne National Laboratory that contributes to the ongoing dialogue concerning the relation between structure and properties of the FePt nanoparticle system. In particular we discuss the ability to control structure and properties via dosing with Cr. Cr-dosed FePt films were grown via molecular beam epitaxy and annealed at $550^{\circ}C$ in an ultrahigh vacuum chamber, and were studied with the surface magneto-optic Kerr effect (SMOKE), scanning electron microscopy (SEM) and x-ray magnetic circular dichroism (XMCD). We found that small dosage of Cr helps to generate $L1_{0}$ phase FePt magnetic nanoparticles with small size, defined shape and regular spatial distribution on MgO (001) substrate. The nanostructures are ferromagnetic with high magnetic coercivity (${\sim}0.9T$) and magnetic easy axis in the desired out-of-plane orientation. We also show that controlling the lateral region where nanostructures exist is possible via artificial patterning with Cr.

자기터널절합에서 자기 및 자기저항의 접합크기 의존성 (Junction Size Dependence of Magnetic and Magnetotransport Properties in MTJs)

  • 상카라나라얀;호영강;김철기;김종오;이의복
    • 한국재료학회지
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    • 제13권6호
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    • pp.369-373
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    • 2003
  • Magneto-optic Kerr Effect(MOKE), AFM and magnetoresistance measurements have been carried out on as-deposited and annealed Magnetic Tunnel Junctions(MTJs) with junction sizes 180, 250, 320 and 380 $\mu\textrm{m}$ in order to investigate the correlation among interlayer exchange coupling, surface roughness and junction size. Relatively irregular variations of coercivity $H_{c}$ (∼17.5 Oe) and interlayer exchange coupling $H_{E}$ (∼17.5 Oe) are observed over the junction in as-deposited sample prepared by DC magnetron sputtering. After annealing at $200^{\circ}C$, $H_{c}$ decreases to 15 Oe, while $H_{ E}$ increases to 20 Oe with smooth local variation. $H_{E}$ shows very good correlation with surface roughness across the junction in agreement with Neel's orange peel coupling. The increasing slope per $\mu\textrm{m}$ of normalized $H_{c}$ and $H_{E}$ are same near junction edge along free-layer direction irrespective of junction size, giving relatively uniform $H_{c}$ and $H_{ E}$ for wider junction size. Thickness profiles of the junctions measured with $\alpha$-step show increasingly flat top surface for larger junctions, indicating better uniformity for large. junctions in agreement with the normalized$ H_{c}$ and H$/_{E}$ curves. TMR ratios also increase with increasing junction size, indicating improvement for larger uniform junctions.