• Title/Summary/Keyword: Magnetoresistance(MR)

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Magnetoresistive heads with dual exchange bias using $NiFe/TbCo/Si_3N_4$ thin films (자기 저항 헤드의 이중 자기 교환 바이어스를 위한 $NiFe/TbCo/Si_3N_4$ 박막제조)

  • 김영채;오장근;조순철
    • Journal of the Korean Magnetics Society
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    • v.4 no.3
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    • pp.239-243
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    • 1994
  • $NiFe/TbCo/Si_3N_4$ thin films were fabricated, which can be employed as dualOongitudinal and transverse) biased magnetoresistive elements utilizing surface magnetic exchange at the interface of NiFe/TbCo films. When Tb area percent was 36 % and substrate bias was not applied, magnetic exchange fields of 100~180 Oe were obtained. The thicknesses of NiFe, TbCo and $Si_3N_4$(Protective layer) were $470\;{\AA},\;2400\;{\AA}\;and\;600\;{\AA}$, respectively. Magnetoresistance ratio of 1.45 % was obtained using NiFe films fabricated with 1000 W power and 2.5 mTorr of Ar pressure. The MR ratio of microstructured elements was reduced to 1.31 % and the MR response curves were shown not to saturate due to demagnetizing fields of the elements. When elements were fabricated with $36^{\circ}$ of misalignment with respect to the exchange field direction using films having 150 Oe exchange field, MR response curve was shifted by 85 Oe, and the operating point of the device shifted to the linear region of the response. Also, the Barkhausen noise was eiminated due to longitudinal bias field originating from the exchange field.

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Temperature dependence of exchange bias in Co/Ni anti-dot arrays

  • Seo, M.S.;Deshpande, N.G.;Lee, S.J.;Lee, Y.P.;Rhee, J.Y.;Kim, K.W.
    • Proceedings of the Korean Vacuum Society Conference
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    • 2011.02a
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    • pp.436-436
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    • 2011
  • Recently, spintronic devices with submicron structures are widely investigated to take advantage of their unique micromagnetic properties. In this work, we study the temperature dependence of exchange bias in bilayer anti-dot arrays made by depositing Co (40 nm)/Ni (5 nm) ferromagnetic bilayer on Si substrate to form anti-dot arrays with a diameter $1{\mu}m$. The anti-dot patterning was done only for the upper Co layer, while the Ni underlayer was kept unperforated. The temperature dependences of magnetoresistance (MR) and exchange bias were studied along magnetic easy and hard axes. The in-plane MR measurements were performed using a physical-property measurement system (PPMS ; Quantum Design Inc.) at various temperatures. The standard in-line four-point probe configuration was used for the electrical contacts. As temperature was varied, the MR data were obtained in which in-plane field (H=3 kOe) was applied in the directions along the hard and the easy axes with respect to the lattice plane. The temperature dependences of magnetic anisotropy and exchange bias were also studied along the magnetic easy and hard axes. As temperature decreases, the single peak splits into two peaks. While no exchange bias was observed along the magnetic easy axis, the exchange bias field steadily increased with decreasing temperature along the magnetic hard axis. These results were interpreted in connection with the magnetic anisotropy and the effect of the anti-dots in pinning domain wall motion along the respective direction.

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Magnetic Domain Structure in Laser-Annealed NiFe/FeMn Bilayers (FeMn/NiFe에서 Laser 열처리에 의한 자구연구)

  • Choi, S.D.;Kim, S.W.;Jin, D.H.;Lee, M.S.;Ahn, J.H.;Joo, H.W.;Kim, Y.S.;Lee, K.A.;Lee, S.S.;Hwang, D.G.
    • Journal of the Korean Magnetics Society
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    • v.14 no.6
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    • pp.224-227
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    • 2004
  • We have studied local magnetization reversal by laser annealing in exchange biased NiFe/FeMn bilayer. Local magnetization reversal was performed by using the DPSS laser under external magnetic field of 600G. When the laser illuminated the patterned film with the power of above 300 mW during 15 min, a magnetoresistance (MR) curve with symmetric peaks at the opposite field was obtained due to the local reversal of exchange biasing. The direction of exchange anisotropy in the locally reversed region can be restored by local laser annealing under alternating magnetic field, even if its MR peak was reduced by the damage and interdiffusion. The magnetic domain structure of the locally reversed region was measured by MFM. The new domains were generated by laser annealing near the exposed area.

Dependence of Magnetoresistance on the Underlayer Thickness for Top-type Spin Valve (Top형 스핀밸브 구조의 Si 기판에서의 하지층 두께에 따른 자기저항 특성 연구)

  • Ko, Hoon;Kim, Sang-Yoon;Kim, Soo-In;Lee, Chang-Woo;Kim, Ji-Won;Jo, Soon-Chul
    • Journal of the Korean Magnetics Society
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    • v.17 no.2
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    • pp.95-98
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    • 2007
  • In this paper, the magnetic properties and the annealing behavior of spin valve structures with Mo(MoN) underlayers were studied for various underlayer thickness. The spin valve structure was Si substrate/Mo(MoN)$(t{\AA})/NiFe(21{\AA})/CoFe(28{\AA})/Cu(22{\AA})/CoFe(18{\AA})/IrMn(65{\AA})/Ta(25 {\AA})$. Mo and MoN films were deposited on Si substrates and their thermal annealing behavior was analyzed. The deposition rate of the MoN thin film was decreased and tile resistivity of the MoN thin films were increased as the $N_2$ gas flow was increased. The variations of MR ratio and magnetic exchange coupling field of spin valve structure were smaller with MoN underlayers than that with Mo underlayers up to thickness of $51{\AA}$. MR ratio of spin valves with Mo underlayers was 2.86% at room temperature and increased up to 2.91 % after annealing at $200^{\circ}C$. Upon annealing at $300^{\circ}C$, the MR ratio decreased about 2.16%. The MR ratio of spin valves structure with MoN underlayers for $N_2$ gas flow 1 sccm was 5.27% at room temperature and increased up to 5.56% after annealing at $200^{\circ}C$. Upon annealing at $300^{\circ}C$, the MR ratio decreased about 4.9%.

Effect of Doubly Plasma Oxidation Time on TMR Devices (이중절연층 산화공정에서 플라즈마 산화시간에 따른 터널자기저항 효과)

  • Lee, Ki-Yung;Song, Oh-Sung
    • Journal of the Korean Magnetics Society
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    • v.12 no.4
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    • pp.127-131
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    • 2002
  • We fabricated MTJ devices that have doubly oxidized tunnel barrier using plasma oxidation method to from oxidized AlO$\sub$x/ tunnel barrier. Doubly oxidation I, which sputtered 10 ${\AA}$-bottom Al layer and oxidized it with oxidation time of 10 s. Subsequent sputtering of 13 ${\AA}$-Al was performed and the metallic layer was oxidized for 50, 80 and 120 s., respectively. Doubly oxidation II, which sputtered 10 ${\AA}$-bottom Al layer and oxidized it varying oxidation time for 30∼120 s. Subsequent sputtering of 13 ${\AA}$-Al was performed and the metallic layer was oxidized for 210 sec. Double oxidation process specimen showed MR ratio of above 27% in all experiment range. Singly oxidation process. 13 ${\AA}$-Al layer and oxidized up to 210 s, showed less MR ratio and more narrow process window than those of doubly oxidation. Cross-sectional TEM images would that doubly oxidized barrowers were thinner and denser than singly oxidized ones. XPS characterization confirmed that doubly oxidation of Fe with bottom insulating layer. As a result, doubly oxidation could have superior MR ratio in process extent during long oxidation time because of preventing oxidation of bottom magnetic layer than singly oxidation.

Fabrication of Thin film Magnetoresistive Device and the Dependency of Applied Manetic Field Direction (박막 자기저항 소자 제작 및 출력의 인가자장 각도 의존성)

  • Min, Bok-Ki;Lee, Won-Jae;Jeong, Soon-Jong;Song, Jae-Sung
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2003.05a
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    • pp.50-54
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    • 2003
  • The output characteristics of thin film NiO/NiFe bilayered magnetoresistive device have been measured as a function of the direction of external magnetic field. Each layer was fabricated by rf magnetron sputtering method, and especially, the under layer, NiO, was fabricated under the in-situmagnetic field of about 1000Oe. The magnetoresistive devices were designed with the angle of 45degree between the direction of current of the device pattern and the induces magnetic field in the NiO film layer. The output of the devices had a good linearity when the devices were placed on the external magnetic field perpendicular to induced field direction and also 45 degree with the currenr path direction.

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Magnetic Properties of MTJ by Capping Material & External Field Intensity (Capping Material & External Field Intensity에 따른 자기 저항 특성 연구)

  • 이계남;장인우;박영진;박상용;이재형;전경인;신경호
    • Proceedings of the Korean Magnestics Society Conference
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    • 2002.12a
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    • pp.50-51
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    • 2002
  • 최근 실온에서 약 40% 이상의 높은 자기저항(magnetoresistance, MR)을 나타내는 자기 터널 접합(magnetic tunnel junction, MTJ)이 보고되면서 비휘발성 자기메모리로의 응용을 눈앞에 두고 있다.[1]. 이에 본 실험에서는 Substrate / Ta (base electrode) / NiFe / PtMn (AF pinning layer) / CoFe (pinned) / Ru / CoFe (fixed) / Al-O/ CoFe (free) / NiFe (free) / Ta & Ru (Capping Layer)과 같은 MTJ 증착 구조를 사용하여, MTJ의 보다 향상된 특성을 확보하기 위한 노력으로서 Al-O 두께, 어닐링 조건(Field Intensity & Sequence)변화 등을 시도하였다. (중략)

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BOTTOM IrMn-BASED SPIN VALVES BY USING OXYGEN SURFACTANT

  • J. Y. Hwang;Kim, M. Y.;K. I. Jun;J. R. Rhee;Lee, S. S.;D. G. Hwang;S. C. Yu;Lee, S. H.
    • Proceedings of the Korean Magnestics Society Conference
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    • 2002.12a
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    • pp.62-63
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    • 2002
  • To reach 100 Gbit/in$^2$ magnetic recording densities in hard disk drives specular enhancement of giant magnetoresistance (GMR) effect in spin valve (SV) films has become one of the indispensable means for application as read elements in recording heads [1]. More recently specular spin valve (SSV) structure containing nano-oxides layers (NOL) were reported [2], where MR enhancement is caused to extended mean free path of majority spin polarized electrons through specular reflection at metal/insulator interfaces [3] in the SV films. (omitted)

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Magnetotransport Properties of Co-Fe/Al-O/Co-Fe Tunnel Junctions Oxidized with Microwave Excited Plasma

  • Nishikawa, Kazuhiro;Orata, Satoshi;Shoyama, Toshihiro;Cho, Wan-Sick;Yoon, Tae-Sick;Tsunoda, Masakiyo;Takahashi, Migaku
    • Journal of Magnetics
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    • v.7 no.3
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    • pp.63-71
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    • 2002
  • Three fabrication techniques for forming thin barrier layer with uniform thickness and large barrier height in magnetic tunnel junction (MTJ) are discussed. First, the effect of immiscible element addition to Cu layer, a high conducting layer generally placed under the MTJ, is investigated in order to reduce the surface roughness of the bottom ferromagnetic layer, on which the barrier is formed. The Ag addition to the Cu layer successfully realizes the smooth surface of the ferromagnetic layer because of the suppression of the grain growth of Cu. Second, a new plasma source, characterized as low electron energy of 1 eV and high density of $10^{12}$ $cm^{-3}$, is introduced to the Al oxidation process in MTJ fabrication in order to reduce damages to the barrier layer by the ion-bombardment. The magnetotransport properties of the MTJs are investigated as a function of the annealing temperature. As a peculiar feature, the monotonous decrease of resistance area product (RA) is observed with increasing the annealing temperature. The decrease of the RA is due to the decrease of the effective barrier width. Third, the influence of the mixed inert gas species for plasma oxidization process of metallic Al layer on the tunnel magnetoresistance (TMR) was investigated. By the use of Kr-O$_2$ plasma for Al oxidation process, a 58.8 % of MR ratio was obtained at room temperature after annealing the junction at $300{^{\circ}C}$, while the achieved TMR ratio of the MTJ fabricated with usual Ar-$0_2$ plasma remained 48.4%. A faster oxidization rate of the Al layer by using Kr-O$_2$ plasma is a possible cause to prevent the over oxidization of Al layer and to realize a large magnetoresistance.

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