• Title/Summary/Keyword: 터널링 자기저항

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Large Magneto-Resistance in Magnetite Nanoparticles (마그네타이트 극미세 나노입자의 자기저항 현상)

  • Jang, Eun-Young;Lee, Nyun-Jong;Choi, Deung-Jang;Kim, Tae-Hee
    • Journal of the Korean Magnetics Society
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    • v.18 no.4
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    • pp.154-158
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    • 2008
  • Magnetite($Fe_3O_4$) is currently one of key materials for applications in magnetic storage and many bioinspired applications because bulk $Fe_3O_4$ has a high Curie temperature($Tc={\sim}850K$) and nearly full spin polarization at room temperature(RT). In this work, $Fe_3O_4$ nanoparticles with different sizes of 12 to 15 nm were prepared in a well-controlled manner by a nonhydrolytic synthetic method. Here, we report the significant intergrain magneto-resistance(MR) of ${\sim}2%$ at RT in $Fe_3O_4$ nanoparticle pellets. The tunneling conductance was also investigated based on the Brinkman model, as well. Our results show clearly that the surface or interfacial property of the particles plays a crucial role in the MR effect.

Magnetoresistance and Structural Properties of the Magnetic Tunnel Junction with Ternary Oxide Barrier (삼원계 산화 절연층을 가진 자기터널접합의 자기·구조적 특성에 관한 연구)

  • Park, Sung-Min;Lee, Seong-Rae
    • Journal of the Korean Magnetics Society
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    • v.15 no.4
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    • pp.231-235
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    • 2005
  • We studied the microstructural evolution of ZrTM-Al (TM=Nb and Ti) alloy films, MR and electrical properties of the MTJ with $ZrTM-AlO_x$ barrier as a function of Zr/TM ratio. We observed that the ternary-oxide barrier reduced the TMR ratio due mainly to the structural defects such as the surface roughness. The change in TMR ratio and $V_h$ with Zr/TM ratio exactly corresponds to the systematic changes in the microstructural variation. Although the MTJ with ternary oxide reduced the TMR and the electrical stabilities, the junction resistances decreased as the Ti and Nb concentration increased due to the band-gap reduction caused by the formation of extra bands

Electrostatic discharge simulation of tunneling magnetoresistance devices (터널링 자기저항 소자의 정전기 방전 시뮬레이션)

  • Park, S.Y.;Choi, Y.B.;Jo, S.C.
    • Journal of the Korean Magnetics Society
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    • v.12 no.5
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    • pp.168-173
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    • 2002
  • Electrostatic discharge characteristics were studied by connecting human body model (HBM) with tunneling magnetoresistance (TMR) device in this research. TMR samples were converted into electrical equivalent circuit with HBM and it was simulated utilizing PSPICE. Discharge characteristics were observed by changing the component values of the junction model in this equivalent circuit. The results show that resistance and capacitance of the TMR junction were determinative components that dominate the sensitivity of the electrostatic discharge(ESD). Reducing the resistance oi the junction area and lead line is more profitable to increase the recording density rather than increasing the capacitance to improve the endurance for ESD events. Endurance at DC state was performed by checking breakdown and failure voltages for applied DC voltage. HBM voltage that a TMR device could endure was estimated when the DC failure voltage was regarded as the HBM failure voltage.

Junction Capacitance Dependence of Response Time for Magnetic Tunnel Junction (터널링 자기저항 소자의 접합면 정전용량에 따른 전기적 응답특성)

  • Park, S.Y.;Choi, Y.B.;Jo, S.C.
    • Journal of the Korean Magnetics Society
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    • v.12 no.2
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    • pp.68-72
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    • 2002
  • In this research, the effects of capacitance to the access time were studied at the junction area of tunneling magnetoresistance when these were used as memory devices. These results were obtained by applying electric signal input and magnetic field was not used. We applied bipolar square waves of 1MHz to the MTJ samples to obtain the results and time constant ($\tau$) calculated by observing wave responses utilizing an oscilloscope. And time constant was compared with junction area. Each part of MTJ sample, such as electrical pad, lead and contact area, was modeled as an electrical equivalent circuit based on experimental results. For the 200㎛$\times$200㎛ cell, junction capacitance was 90 pF. Also, measurement and simulation results were compared, which showed those similarity.

Magnetic Characteristics and Annealing Effects of $NiFe/FeMn/NiFe/CoFe/Al_2O_3/CoFe/NiFe$Spin Tunneling Junctions ($NiFe/FeMn/NiFe/CoFe/Al_2O_3/CoFe/NiFe$ 스핀 터널링 접합의 자기적 특성과 열처리 효과)

  • 최연봉;박승영;강재구;조순철
    • Journal of the Korean Magnetics Society
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    • v.9 no.6
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    • pp.296-300
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    • 1999
  • Cross-shape structures of spin tunneling junctions were fabricated using DC magnetron sputtering and metal masks. The film structures were $substrate/Ta/NiFe/FeMn/NiFe/CoFe/Al_2O_3/CoFe/NiFe$ and $substrate/Ta/NiFe/CoFe/ Al_2O_3/CoFe/NiFe/FeMn/NiFe$. Fabrication conditions of insulating layer ($Al_2O_3$) and thickness and sputtering power of each film layer were varied, and maximum magnetoresistance ratio of 24.3 % was obtained. Magnetic characteristic variations in the above mentioned two structures and two types of substrates (Corning glass 7059 and Si(111)) were compared. Annealing of the junctions was performed to find out magnetic characteristic variations expected from the device fabrication. Magneoresistance Ratio were observed to maintain as-deposited value up to 150 $^{\circ}C$ annealing and then to drop rapidly after 180 $^{\circ}C$ annealing.

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Microstructural and Magnetic Properties of CoFeB/MgO/CoFeB Based Magnetic Tunnel Junction Depending on Capping Layer Materials (Capping층 재료에 따른 CoFeB/MgO/CoFeB 자기터널접합의 미세구조와 자기저항 특성)

  • Chung, Ha-Chang;Lee, Seong-Rae
    • Journal of the Korean Magnetics Society
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    • v.17 no.4
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    • pp.162-165
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    • 2007
  • We investigated the effects of the capping layer materials on the crystallization of the amorphous top-CoFeB (t-CoFeB) electrode and the magnetoresistance properties of the magnetic tunnel junctions (MTJs). When the hcp(002)-textured Ru capping layer was used, the amorphous t-CoFeB was crystallized to bcc-CoFe(110). The CoFe(110)/Ru(002) texture relation can be minimized the lattice mismatch down to 5.6%. However, when the fine polycrystalline but almost amorphous TiAl or amorphous ZrAl were used, the amorphous t-CoFeB was crystallized to bcc-CoFe(002). When the amorphous capping materials were used, the evolution of the t-CoFeB texture was affected mainly by the MgO(001) texture. Consequently, the M ratios of the annealed MTJ capped with the ZrAl and TiAl (72.7 and 71.8%) are relatively higher than that of the MTJ with Ru capping layer (46.7%). In conclusions, the texture evolution of the amorphous t-CoFeB during the post deposition annealing could be controlled by the crystallinity of the adjacent capping layer and in turn, it affects the TMR ratio of MTJs.