• Title/Summary/Keyword: Interlayer exchange coupling

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Reflection-amplitude Approximation for the Interlayer Exchange Coupling in (001) Co/Cu/Co Multilayers

  • Lee, B. C.
    • Proceedings of the Korean Magnestics Society Conference
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    • 2000.09a
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    • pp.191-199
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    • 2000
  • The reflection-amplitude approximation is used to calculate the interlayer exchange coupling in (001) Co/Cu/Co multilayers. The dependence of the phase factor of the reflection amplitude on the energy and wave vector is included. The contribution of each period is calculated and the results are compared with those from the asymptotic behavior. It is shown that the energy and wave-vector dependence of the phase factor may affect the interlayer exchange coupling significantly.

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Effect of the Phase Factor of the Reflection Amplitude on the Interlayer Exchange Coupling in (001) Co/Cu/Co Multilayers

  • Lee, B.C.
    • Journal of Magnetics
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    • v.6 no.2
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    • pp.43-46
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    • 2001
  • The reflection-amplitude approximation is used to calculate the interlayer exchange coupling in (001) Co/Cu/Co multilayers. The dependence of the phase factor of the reflection amplitude on the energy and wave vector is included. The contribution of each period is calculated and the results are compared with those from asymptotic behavior. It is shown that the energy and wave-vector dependence of the phase factor may affect the interlayer exchange coupling significantly.

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Effect of a Ferromagnetic Layer Thickness on a Narrow Domain Wall Width (좁은 자벽의 두께에 강자성층의 두께가 미치는 영향)

  • Lim, Ho-Tack;You, Chun-Yeol
    • Journal of the Korean Magnetics Society
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    • v.15 no.6
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    • pp.303-306
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    • 2005
  • Effect of a ferromagnetic layer thickness on a narrow domain wall width is investigated. It is found that the narrow domain wall is formed in ferromagnetic/nonmagnetic/ferromagnetic multi layer structure with a loc at interlayer exchange coupling, and that the width of the narrow domain wall is affected by the ferromagnetic layer thickness. We performed micromagnetics simulations for the $Fe_1/Cr/Fe_2$ system with the local interlayer exchange coupling, with fixed thickness (20-nm) of $Fe_2$ layer and various $Fe_1$ layer thickness (1, 2, 4, and 6 nm). Consequently, we confirmed that the thinner the $Fe_1$ layer thickness, the thinner the width of the domain wall is formed, because of the surface energy nature of the interlayer exchange coupling.

NiO Thickness Dependences of Perpendicular Magnetic Anisotropy in the [CoFe/Pt] Multilayers

  • Kim, S.W;Lee, J.Y;Lee, S.S;Hahn, E.J;Hwang, D.G
    • Journal of Magnetics
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    • v.9 no.4
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    • pp.121-124
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    • 2004
  • NiO thickness dependences of perpendicular magnetic anisotropy (PMA) in the $NiO/[CoFe/Pt]_5$ multilayers for exchange biasing and $[CoFe/Pt]_4/Pt/[CoFe/Pt]_4$ for interlayer exchange coupling were investigated. Perpendicular magnetization curve was obtained by out-of-plane extraordinary Hall measurement. Magnetic force microscopy (MFM) has been used for the investigation of magnetic domains on thin films. We confirmed that the interlayer exchange coupling (IEC) as a function of NiO thickness at room temperature existed with a period of two monolayers.

Pt Thickness Dependence of Oscillatory Interlayer Exchange Coupling in [CoFe/Pt/CoFe]/IrMn Multilayers with Perpendicular Anisotropy

  • Lee, Sang-Suk;Choi, Jong-Gu;Kim, Sun-Wook;Hwang, Do-Guwn;Rhee, Jang-Roh
    • Journal of Magnetics
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    • v.10 no.2
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    • pp.44-47
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    • 2005
  • The oscillatory interlayer exchange coupling (IEC) has been shown in pinned $[CoFe/Pt(t_{pt})/CoFe]/IrMn$ multi-layers with perpendicular anisotropy. The period of oscillation corresponds to about 2 monolayers of Pt. The oscillatory behavior of IEC depending on the nonmagnetic metallic Pt thickness is thought to be related the antiferromagnetic ordering induced by IrMn layer. Oscillatory IEC as function of insulating NiO thickness has been observed in $[Pt/CoFe]_4/NiO(t_{NiO})/[CoFe/Pt]_4$ multilayers. The effect of N (number of bilayer repeats) upon the magnetic property of [Pt/CoFe]N/IrMn is also studied.

Interlayer and Interfacial Exchange Coupling of IrMn Based MTJ

  • Wrona, J.;Stobiecki, T.;Czapkiewicz, M.;Kanak, J.;Rak, R.;Tsunoda, M.;Takahashi, M.
    • Journal of Magnetics
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    • v.9 no.2
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    • pp.52-59
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    • 2004
  • As deposited and annealed MTJs with the structure of $Ta(5 nm)/Cu(10 nm)/Ta(5 nm)/Ni_{80}Fe_{20}(2 nm)/Cu(5 nm)/ Ir_{25}Mn_{75}(10 nm)/Co_{70}Fe_{30}(2.5 nm)/Al-O/Co_{70}Fe_{30}(2.5nm)/Ni_{80}Fe_{20}(t)/Ta(5nm)/Ni_{80}Fe_{20}(t)/Ta(5 nm)$, where t=10, 30, 60 and 100 nm were characterized by XRD and magnetic hysteresis loops measurements. The XRD measurements were done in grazing incidence $(GID scan-2{\theta})$ and ${\theta}-2{\theta}$ geometry, by rocking curve $(scan-{\omega})$ and pole figures in order to establish correlation between texture and crystallites size and magnetic parameters of exchange biased and interlayer coupling. The variations of shifting and coercivity field of free and pinned layers after annealing in $300^{\circ}C$ correlate with the improvement of [111] texture and grains size of $Ni_{80}Fe_{20}$ and $Ir_{25}Mn_{75}$ respectively. The exchange biased and the coercivity fields of the pinned layer linearly increased with increasing grain size of $Ir_{25}Mn_{75}$, The reciprocal proportionality between interlayer coupling and coercivity fields of the free layer and grain size of $Ni_{80}Fe_{20}$ was found. The enhancement of interlayer coupling between pinned and free layers, after annealing treatment, indicates on the correlated in-phase roughness of dipolar interacting interfaces due to increase of crystallites size of $Ni_{80}Fe_{20}$.

External Magnetic Field Influence on Exchange Coupling Oscillations in Ultrathin Fe/Au/Tb Film Structures

  • Pogoryelov, Ye.
    • Journal of Magnetics
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    • v.9 no.4
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    • pp.97-100
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    • 2004
  • In the present work exchange coupling between ultrathin Fe ($8{\AA}$) and Tb ($12{\AA}$) layers separated by Au spacer of varied thickness ($3-20{\AA}$) was studied. Anomalous Hall effect measurements showed weakly damped oscillating dependence of the Hall conductivity as a function of Au spacer thickness. Disagreement of the observed damping with the RKKY model of interlayer exchange coupling was explained by the influence of external magnetic field on the behaviour of exchange coupling oscillations. It was confirmed by Hall-like effect measurements at zero applied magnetic field and also illustrated by corresponding estimations.

BEAUTY OF INTERLAYER EXCHANGE COUPLING IN SPINTRONICS DEVICES

  • You, Chun-Yeol
    • Proceedings of the Korean Magnestics Society Conference
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    • 2002.12a
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    • pp.20-21
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    • 2002
  • 최근 자성 박막의 연구에 있어서 이웃한 두 자성체 층 간의 교환 상호 결합 작용(interlayer exchange coupling)은 매우 중요한 연구 분야중 하나이다. 80년대 말 처음 강한 층간 교환 상호 결합 작용이 발견된 이래로, 비자성 사이 층의 두께에 따라서 층간 교환 상호 작용이 요동하는 현상과 더불어서 소위 거대 자기 저항(giant magnetoresistance)이라고 불리는 현상의 발견은 자성 박막의 나노 시대를 열었다고 해도 과언이 아니었다. (중략)

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Monte Carlo Study of Layered Heisenberg Ferromagnet

  • Lee, Kyuwon
    • Journal of Magnetics
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    • v.6 no.4
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    • pp.119-121
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    • 2001
  • Monte Carlo simulation was employed to study the phase transition in the classical Heisenberg ferromagnet with variable interlayer interactions. The measured transition temperatures show a strong logarithmic dependence on J/J'where J and J'are the intralayer and the interlayer exchange interaction, respectively. The results were compared with the theoretical expectations and an empirical formula for the critical coupling was stained.

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Exchange and Interlayer Coupling in NiO Spin Valve Films (NiO 스핀밸브 박막에서 교환결합과 사잇층 결합에 관한 연구)

  • 박창만;고성호;황도근;이상석;이기암
    • Journal of the Korean Magnetics Society
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    • v.7 no.5
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    • pp.258-264
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    • 1997
  • Exchange and interlayer couplings between a NiFe ferromagnetic layer and an antiferromagnetic NiO layer in NiO/NiFe/Cu/NiFe spin-valve films prepared by rf/dc magnetron sputtering were investigated. The interlayer coupling field ($H_{int}$ decreased with the Cu layer thickness, and the exchange coupling field $(H_{ex}$ saturated to 90 Oe. the magnetitudes of $H_{ex}$ and $H_{int}$ decreased with increasing thickness of the pinned NiFe layer. The increase of $H_{int}$ with the free NiFe layer may be due to the increased magnetization.

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