• 제목/요약/키워드: ferromagnetic resonance

검색결과 123건 처리시간 0.023초

Gd3Ga5O12 기판위에 성장된 Y3Fe5O12 박막의 열처리 조건에 따른 강자성 공명 특성 연구 (Effect of the Annealing Conditions on the Ferromagnetic Resonance of YIG Thin Film Prepared on GGG Substrate)

  • 이예림;;박승영;정종율
    • 한국재료학회지
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    • 제25권12호
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    • pp.703-707
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    • 2015
  • In this study, we investigated the effect of annealing conditions on the ferromagnetic resonance(FMR) of yttrium iron garnet ($Y_3Fe_5O_{12}$, YIG) thin film prepared on gadolinium gallium garnet ($Gd_3Ga_5O_{12}$, GGG) substrate. The YIG thin films were grown by rf magnetron sputtering at room temperature and were annealed at various temperatures from 700 to $1000^{\circ}C$. FMR characteristics of the YIG thin films were investigated with a coplanar waveguide FMR measurement system in a frequency range from 5 to 20 GHz. X-ray diffraction(XRD) and X-ray photoelectron spectroscopy(XPS) were used to characterize the phase formation, crystal structure and composition of the YIG thin films. Field dependent magnetization curves at room temperature were obtained by using a vibrating sample magnetometer(VSM). The FMR measurements revealed that the resonance magnetic field was highly dependent on the annealing condition: the lowest FMR linewidth can be observed for the $800^{\circ}C$ annealed sample, which agrees with the VSM results. We also found that the Fe and O composition changes during the annealing process play important roles in the observed magnetic properties.

Dynamic Magneto-mechanical Behavior of Magnetization-graded Ferromagnetic Materials

  • Chen, Lei;Wang, Yao
    • Journal of Magnetics
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    • 제19권3호
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    • pp.215-220
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    • 2014
  • This study investigates the dynamic magneto-mechanical behavior of magnetization-graded ferromagnetic materials Terfenol-D/FeCuNbSiB (MF). We measure the dynamic magneto-mechanical properties as a function of the DC bias magnetic field ($H_{dc}$). Our experimental results show that these dynamic magneto-mechanical properties are strongly dependent on the DC bias magnetic field. Furthermore, the dynamic strain coefficient, electromechanical resonance frequency, Young's moduli, and mechanical quality factor of Terfenol-D/FeCuNbSiB are greater than those of Terfenol-D under a lower DC bias magnetic field. The dynamic strain coefficient increases by a factor of between one and three, under the same DC bias magnetic field. In particular, the dynamic strain coefficient of Terfenol-D/FeCuNbSiB at zero bias achieves 48.6 nm/A, which is about 3.05 times larger than that of Terfenol-D. These good performances indicate that magnetization-graded ferromagnetic materials show promise for application in magnetic sensors.

교환 바이어스 인위적 준강자성 기준층을 포함한 자기 터널 접합의 강자성 공명 (Ferromagnetic Resonance of Magnetic Tunnel Junctions with an Exchange Biased Synthetic Ferrimagnetic Reference Layer)

  • 윤정범;유천열;정명화
    • 한국자기학회지
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    • 제21권4호
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    • pp.121-126
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    • 2011
  • 자유층과 고정 기준층으로 이루어진 자기 터널 접합의 스핀 동역학을 강자성 공명 시늉내기로 연구 하였다. 먼저 교환 바이어스 인위적 준강자성 기준층을 포함한 자기 터널 접합에서 DC 자기장에 대한 각 층의 자화 방향을 확인하고 터널 자기저항을 계산하였다. 자기 터널 접합에서 스핀의 들뜸 모드들을 확인하기 위해 DC와 RF 자기장을 함께 인가하여 강자성 공명 주파수 스펙트라를 관찰 하였다. 각 층 별로 들뜸 모드들을 확인하여 자유층과 기준층의 자화 방향의 차이로 계산된 터널 자기저항의 들뜸 모드들을 분석 하였다. 전체적으로 스핀의 들뜸 모드는 자유층이나 기준층의 자화 방향에 관련해서 DC 자기장의 음, 양의 방향에 따라 상이하게 나타났다. 음의 방향 자기장에 대해서 자유층과 기준층의 강자성 공명 주파수 스펙트라는 수정된 Kittel 방정식으로 잘 설명되지만 양의 방향 자기장에 대해서는 예측하기 어려운 들뜸 모드들로 인해 분석적 해답을 찾기 어려웠다. 자기터널 접합의 강자성 층들은 서로 상호 작용을 하기 때문에 이에 대한 스핀 동역학 연구는 자유층 뿐만 아니라 기준층, 고정층과도 밀접하게 연관되어 있다.

Prototype Electromagnetic-Noise Filters Incorporated with Nano-Granular Co41Fe38Al13O8 Soft Ferromagnetic Thin Films on Coplanar Transmission Lines

  • Sohn, Jae-Cheon;Byun, Dong-Jin
    • 한국세라믹학회지
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    • 제43권2호
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    • pp.74-78
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    • 2006
  • A non-integrated type noise filter on a Coplanar Waveguide (CPW) transmission line is demonstrated by using a highly resistive $Co_{41}Fe_{38}Al_{13}O_8$ nanogranular thin film with the dimensions of $4\;mm (\iota)\times4\;mm(\omega)\times0.1\;{\mu}m(t)$. The noise suppression characteristics are evaluated without placing an insulating layer between the CPW line and the magnetic thin film. The insertion loss is very low being less than 0.3 dB and this low value is maintained up to 2 GHz. At a ferromagnetic resonance frequency of 3.3 GHz, the power loss is very large and the degree of noise attenuation is measured to be 3 dB. This level of noise attenuation is still small for real applications; however, considering the small magnetic volume used in this work, further improvement is expected by simply increasing the magnetic volume and by integrating the magnetic thin film into the CPW transmission line.

Magnetic Properties of Fe3-x MnxO4 Thin Films by FMR

  • Kim, Ki-Hyeon;Kim, Young-Ho;Ha, Tae-Wook;Lee, Jeong-Sik;Park, Mann-Jang
    • Journal of Magnetics
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    • 제2권2호
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    • pp.38-41
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    • 1997
  • Spinel ferrite thin films Fe3-x MnxO4 (x=0.000, 0.006, 0.0010, 0.015, 0.023) were prepared on the coverglass by ferrite plating technique. To investigate the uniaxial anisotrpy of the samples, the saturation and effective magnetization of the thin films were measured by VSM(vibrating sample magnetometer) and FMR(ferromagnetic resonance) measurements respectively. The spectroscopic splitting g factor were estimated from the ferromagnetic resonance curves. For x=0.000, 0.006, the effective magnetization was measured of temperatures form T=77 K to T=300 K. The results were analyzed in terms of Bloch's law Ms(T) = Ms(0) (1-BT3/2-CT5/2). The Bloch coefficient B, C were determined by fitting. Ms(0) was obtained by extrapolating Meff to 0 K. From this result, the spin wave stiffness constants D was also determined.

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자성물질을 이용한 나선형 인덕터의 고주파 특성 분석 (Characterization and Analysis of Integrated RF Ferromagnetic Spiral Inductors)

  • 차승용;김경범;정영채;최윤석;조근휘;이재성;황성우;현응경;이성래
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 2006년도 추계학술대회 논문집 광주전남지부
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    • pp.109-111
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    • 2006
  • This paper presents characterization and analysis of integrated ferromagnetic inductors in RF regime. Two different materials (CoFe/NiFe) are used as ferromagnetic material. Systematic studies of the inductance (L), the Q-factor (Q) and the structure of the inductor have been performed.

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