• Title/Summary/Keyword: magnetic films

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Possibility of Magnetocapacitor for Multilayered Thin Films

  • Hong, Jong-Soo;Yoon, Sung-Wook;Kim, Chul-Sung;Shim, In-Bo
    • Journal of Magnetics
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    • v.17 no.2
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    • pp.78-82
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    • 2012
  • CoNiFe(CNF)/$BaTiO_3(BTO)$/CoNiFe(CNF) multilayered thin films were deposited on Pt/Ti/$SiO_2$/Si substrates by using pulsed laser deposition (PLD) system. We fabricated three different thin films of BTO, BTO/CNF and CNF/BTO/CNF for magneto-capacitor and studied their crystalline structure, surface and interface morphology, and magnetic and electrical properties. When three different structures of multilayered thin film were compared, magnetization of CNF/BTO/CNF thin films was decreased by magnetic and dielectric interaction. Also we confirmed that capacitance of CNF/BTO/CNF multilayered thin film was enhanced as being near tetragonal structure with increasing of c/a ratio because of atomic bonding at interface between BTO dielectric and CNF magnetic materials. Finally, we studied the change of the capacitance of CNF/BTO/CNF multilayered thin film with magnetic field for emergence of magnetocapacitance and suggested a possibility of enhanced capacitance.

High density plasma etching of CoFeB and IrMn magnetic films with Ti hard mask

  • Xiao, Y.B.;Kim, E.H.;Kong, S.M.;Chung, C.W.
    • Proceedings of the Korean Vacuum Society Conference
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    • 2010.02a
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    • pp.233-233
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    • 2010
  • Magnetic random access memory (MRAM), based on magnetic tunnel junction (MTJ) and CMOS, is a prominent candidate among prospective semiconductor memories because it can provide nonvolatility, fast access time, unlimited read/write endurance, low operating voltage and high storage density. The etching of MTJ stack with good properties is one of a key process for the realization of high density MRAM. In order to achieve high quality MTJ stack, the use of CoFeB and IrMn magnetic films as free layers was proposed. In this study, inductively coupled plasma reactive ion etching of CoFeB and IrMn thin films masked with Ti hard mask was investigated in a $Cl_2$/Ar gas mix. The etch rate of CoFeB and IrMn films were examined on varying $Cl_2$ gas concentration. As the $Cl_2$ gas increased, the etch rate monotonously decreased. The effective of etch parameters including coil rf power, dc-bais voltage, and gas pressure on the etch profile of CoFeB and IrMn thin film was explored, At high coil rf power, high dc-bais voltage, low gas pressure, the etching of CoFeB and IrMn displayed better etch profiles. Finally, the clean and vertical etch sidewall of CoFeB and IrMn free layers can be achieved by means of thin Ti hard mask in a $Cl_2$/Ar plasma at the optimized condition.

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Structure and Magnetic Properties of Sm-Co(x nm)/Co(6 nm) Multi-layered Nanocomposite Films

  • Yang, Choong-Jin;You, Cai-Yin;Zhang, Zhi-Dong
    • Proceedings of the Korean Magnestics Society Conference
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    • 2002.12a
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    • pp.24-25
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    • 2002
  • Tthe structure and magnetic properties of Sm-Co/co films treated at various annealing temperatures and times are reported, The effects of an externally applied magnetic field during annealing, were also investigated. These result is discussed in terms of magnetization reversal of nano grains which seems to compete with the exchange interaction occurring between the nano grains. (omitted)

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High Frequency Soft Magnetic Properties of ($Co_{1-x}Fe_x$)-Al-O Granular Films with High Electrical Resistivity

  • Jaecheon Sohn;Dongjin Byun;Limb, Sang-Ho
    • Proceedings of the Korean Magnestics Society Conference
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    • 2002.12a
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    • pp.220-221
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    • 2002
  • There has been a demand for higher frequency operation of magnetic devices. Consideration of the materials that could be applicable to such high frequency applications is the first step when designing magnetic thin films for high-frequency use. Materials suitable for high frequency application should have a larger $M_{S}$ and an appropriate anisotropy field ( $H_{K}$), which increase a resonance frequency, and also a larger $\rho$, which reduces eddy current loss. (omitted)ted)

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The effect of anisotropy field of FeTaN thin films for ultraigh-hfrequency applications (초고주파대역용 소자를 위한 FeTaN 박막의 이방자계의 영향)

  • Ryu, Sung-Ryong;Bae, Seok;Jeong, Jong-Han;Kim, Choong-Sik;Nam, Seoung-Eui;Kim, Hyoung-June
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2000.11a
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    • pp.303-305
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    • 2000
  • The effect of anisotropy field on the high frequency magnetic characteristics of FeTaN films was investigated. Those films show good magnetic properties : 4$\pi$Ms of 13KG, Hc of 0.6 Oe, effective permeability(${\mu}$') of 800 with a stable frequency response up to 800MHz. The films also show a large anisotropy field(Hk) over 21Oe. It result from the increased anisotropy of patterned FeTaN films. The combination of high saturation magnetization and relatively high Hk in these films is believed to the partly responsible for FeTaN for the excellent high-frequency behavior.

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Growth and magnetic properties of Tb, Eu, EuTb-substituted garnet single crystal films (Tb, Eu, EuTb가 치환된 가네트 단결정 막의 성장과 자기적 특성)

  • Kim G. Y;Yoon S. G.;Chung I. S;Park S. B;Yoon D. H
    • Journal of the Korean Crystal Growth and Crystal Technology
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    • v.14 no.5
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    • pp.193-198
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    • 2004
  • Using the $PbO-B_2O_3-Bi_2O_3$ flux system, $(TbBi)_3(FeAIGa)_5O_{12}(TbIG)$, $(EuBi)_3(FeAIGa)_5O_{12}(EuIG)$ and $(EuTbBi)_3(FeAIGa)_5O_{12}(EuTbIG)$ films were grown on $(GdCa)_3(GaMgZr)_5O_{12}(SGGG)$ substrates by the liquid phase epitaxy (LPE). The saturation magnetization of the grown TbIG, EuIG and EuTbIG films was about 150, 950 and 125 Oe, respectively. The TbIG films resulted in the single magnetic domain while the EuIG and EuTbIG films were observed to be the multi magnetic domains by magnetic force microscope (MFM).

Magnetic Properties of Fe-Zr-N Soft Magnetic Thin Films (Fe-Zr-N 연자성 박막의 자기적 성질)

  • 김택수;김종오;이중환;윤선진;김좌연
    • Journal of the Korean Magnetics Society
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    • v.6 no.5
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    • pp.317-322
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    • 1996
  • Thin films of Fe-Zr-N were fabricated by rf magnetron reactive sputtering method. The saturation magnetization and coercivity as functions of annealing temperature and partial pressure of nitrogen gas, effective permeability at high frequencies, and thermal stability were investigated. Magnetic softness was exhibited in the composition range of $Fe_{72-78}Zr_{7-10}N_{15-18}$ which was boundary between polycrystalline and amorphous structure. These films exhibited magnetic softness with saturation magentic flux density of 1.55 T and effective permeability of about 3000 at 1 MHz. These films also exhibited thermal stability by sustaining effective permeability of 2500 or above as the temperature was raised to $550^{\circ}C$. It is asswned that good magnetic softness is obtained because grain growth of $\alpha-Fe$ is prohibited due to the precipitation of ZrN nanocrystals. The grain sizes of $\alpha-Fe$ films were $40~50\AA$ and the grain sizes of ZrN nanocrystals were $10~15\AA$.

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Magnetic Properties of FeZrBAg Soft Magnetic Thin Films with High Permeability and High Magnetization (고투자율, 고포화자화 FeZrBAg 연자성 박막의 자기적 특성)

  • 민복기;김현식;송재성
    • Journal of the Korean Magnetics Society
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    • v.9 no.6
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    • pp.285-290
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    • 1999
  • The magnetic properties of sputtered amorphous $Fe_{86.7}Zr_{3.3}B_4Ag_6$ thin films, which contains an additional insoluble element Ag, have been investigated as a function of uniaxal field annealing temperature. The amorphous $Fe_{86.7}Zr_{3.3}B_4Ag_6$ thin films produced by relatively low temperature annealing at 40$0^{\circ}C$ for 1 hour was found to have very high permeability of 7800 at 50 MHz, 0.2 mOe, high magnetization of 1.7 T, low coercivity of 1.0 Oe and very low core loss of 1.4 W/cc at 1 MHz, 0.1 T, respectively. It is notable that the permeability and core loss values for various kinds of the soft magnetic thin films reported up to now. The reason for the appearance for the good soft magnetic properties is presumably due to the homogeneous formation of very fine bcc $\alpha$-Fe clusters with the size in the amorphous $Fe_{86.7}Zr_{3.3}B_4Ag_6$ thin films matrix, which can be deduced from the XRD results.

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$MgB_2$ Thin Films on SiC Buffer Layers with Enhanced Critical Current Density at High Magnetic Fields

  • Putri, W.B.K.;Tran, D.H.;Kang, B.;Lee, N.H.;Kang, W.N.
    • Progress in Superconductivity
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    • v.14 no.1
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    • pp.30-33
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    • 2012
  • We have grown $MgB_2$ superconducting thin films on the SiC buffer layers by means of hybrid physical-chemical vapor deposition (HPCVD) technique. Prior to that, SiC was first deposited on $Al_2O_3$ substrates at various temperatures from room temperature to $600^{\circ}C$ by using the pulsed laser deposition (PLD) method in a vacuum atmosphere of ${\sim}10^{-6}$ Torr pressure. All samples showed a high transition temperature of ~40 K. The grain boundaries of $MgB_2$ samples with SiC layer are greater in amount, compare to that of the pure $MgB_2$ samples. $MgB_2$ with SiC buffer layer samples show interesting change in the critical current density ($J_c$) values. Generally, at both 5 K and 20 K measurements, at lower magnetic field, all $MgB_2$ films deposited on SiC buffer layers have low $J_c$ values, but when they reach higher magnetic fields of nearly 3.5 Tesla, $J_c$ values are enhanced. $MgB_2$ film with SiC grown at $600^{\circ}C$ has the highest $J_c$ enhancement at higher magnetic fields, while all SiC buffer layer samples exhibit higher $J_c$ values than that of the pure $MgB_2$ films. A change in the grain boundary morphologies of $MgB_2$ films due to SiC buffer layer seems to be responsible for $J_c$ enhancements at high magnetic fields.

Increment of the Exchange Coupling in Fe-Ni Alloy Thin Films Deposited with a Bias Magnetic Field

  • Han, Kyung-Hunn;Kim, Jung-Gi;Cho, Jae-Hun;Lee, Suk-Mock
    • Journal of Magnetics
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    • v.11 no.2
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    • pp.77-82
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    • 2006
  • The structure and magnetic properties of Fe-Ni films, deposited by DC magnetron sputtering on Si(111) wafer, have been studied. The spin wave stiffness constant is determined by Brillouin light scattering (BLS) and compared with the value obtained from magnetization measurements. The range of exchange interaction was determined as 0.4 atomic distances in the film deposited in a bias magnetic field, which is 1/2 that in the film grown in no bias magnetic field. The results show that the dimensions of exchange coupling increased by the sputtering in the magnetic field.