• 한국자기학회지
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• 제11권4호
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• pp.163-167
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• 2001

DC 마그네트론 스퍼터링법으로 증착된 700 $\AA$의 NiFe 박막을 박막 증착시 형성시킨 자화용이축에 수직한 자기장을 인가하여 열처리한 후 일축 이방성 자기장의 회전을 조사하였다. NiFe 박막은 열처리온도 160 $^{\circ}C$에서 자화용이축과 자화곤란축을 구분할 수 없는 등방적인 상태가 되었고, 열처리온도가 증가함에 따라 다시 일축 이방성을 갖는 상태가 되었다. 열처리 온도가 400 $^{\circ}C$ 이상인 경우에 급격한 보자력의 증가를 보였다. 열처리 온도가 400 $^{\circ}C$인 경우에 XRD 분석과 AES depth profile은 NiFe 박막 내에서 (111) 방향으로 결정성장이 활발히 일어나며 인접한 전극 Au와 상호화산 현상도 광범위하게 일어남을 보여주었다.

• 한국자기학회지
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• 제7권5호
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• pp.243-248
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• 1997

Ar+ $O_{2}$ 혼합가스 중에서 반응성 스퍼터링을 통해 직접 Fe-Hf-O계 초미세결정 연자성 박막을 제조하였으며, 이때 산소분압비의 변화가 Fe-Hf-O 박막의 미세구조 및 자기적 특성에 미치는 영향을 조사하였다. 산소분압이 증가함에 따라 박막의 포화자속밀도는 점차적으로 감소하며 연자기특성이 10%까지는 향상되다가 다시 열화되는 경향을 나타내었다. 최적조건인 10%의 산소분압에서 증착한 F $e_{82}$H $f_{3.4}$ $O_{14.6}$ 초미세결정 박막은 열처리 없이 증착한 상태에서 우수한 연자기 특성을 나타내었으며, 이때의 자기적 특성은 각각 포화자속밀도 17.7 kG, 보자력 0.7 Oe 및 실효투자율 2,500(100 MHz)의 값을 나타내었다. 산소분압이 증가함에 따라 결정립 크기가 감소하며 15% 이상의 산소분압에서는 F $e_{3}$ $O_{4}$가 생성되었다. 따라서 10%에서 가장 우수한 연자기 특성을 나타내는 것은 결정립 크기와 산화물 생성에 의해 설명될 수 있다. Fe-Hf-O계 초미세결정 박막의 전기비저항은 산소분압이 증가함에 따라 증가하는 경향을 나타내었다. 우수한 연자기 특성을 나타내는 F $e_{82}$H $f_{3.4}$ $O_{14.6}$ 박막의 경우, 약 150 .mu. .ohm.cm로 산소를 첨가하지 않은 경우의 30 .mu. .ohm. cm에 비하여 약 5배 증가된 값을 나타내었다. 따라서 F $e_{82}$H $f_{3.4}$ $O_{14.6}$초미세결정 박막이 고주파에서 우수한 연자기 특성을 나타내는 원인은 주로 높은 전기비저항과 미세하게 형성된 결정립에 기이한 것으로 생각된다.

• 한국통신학회논문지
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• 제19권10호
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• pp.1849-1860
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• 1994

본 논문은 비정질 회토류 천이 급속 박막내에서의 자벽 역학(Magnetic domain wall dynamics)을 란다우 리프쉬츠 길버트 (Landau Lifshitz Gilbert) 방정식을 이용한 수치적 해석을 수행하여 연구하였다. 박막을 이차원 정방형 격자($30\times30$)로 나누고, 각 격자 셀(Cell)에 쌍극자간 존재한다고 상정하여, 이들 쌍극자간의 상호 교환 작용과 자기 이방성, 외부 인가 자계, 그리고 감자계의 영향이 고려되었다. 단축 자기 이방성이 존재하고 역방향의 자화가 존재한다고 가정된 상태에서 자벽이 형성되는 시간과 자벽의 두께를 알아보았다. 또한 외부 자계의 인가에 따른 자벽 이동을 연구하였다. 시뮬레이션 결과, 감자계를 고려했을 때 자벽 형성 시간이 상당히 빨라졌고, 평균 자벽의 이동도(Mobility)는 약간 증가되었다.

• 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.

• Journal of Magnetics
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• 제5권2호
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• pp.44-49
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• 2000

Computer simulation of sensing current effects on the magnetic and magnetoresistance properties of a crossed spin-valve head is carried out. The spin-valve head has the following layer structure: Ta (8.0 nm)/NiMn (25 nm)/NiFe (2.5 nm)/Cu (3.0 nm)/NiFe (5.5 nm)/Ta (3.0 nm), and it is 1500 nm long and 600 nm wide. Even with a high pinning field of 300 Oe and a high hard-biased field of 50 Oe, the ideal crossed spin-valve structure, which is essential to the symmetry of the output signal and hence high density recording, is not realized mainly due to large interlayer magnetostatic interactions. This problem is solved by applying a suitable magnitude of sensing currents along the length direction generating magnetic fields in the width direction. The ideal spin-valve head is expected to show good symmetry of the output signal. This has not been shown explicitly in the present simulation, however, The reason for this is possibly related to the simple assumption used in this calculation that each magnetic layer consists of a single domain.

• Journal of Magnetics
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• 제17권2호
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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.

• 한국자기학회지
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• 제5권5호
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• pp.528-532
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• 1995

Ferromagnetic resonance experiments have been used to investigate the magnetic properties of amorphous $Co_{89.5}Zr_{10.5}$ thin films deposited by DC magnetron sputtering method. In the thickness range from $350\;{\AA}$ to $3,200\;{\AA}$, measurements were carried out in a static magnetic field perpendicular and parallel to the film plane and in a conventional 9.44 GHz spectrometer at room temperature. The ferromagnetic resonance spectra by the field perpendicular to the film plane showed standing spin wave. The spacing and the relative intensities between the various spin wave resonance peaks are analysed considering surface magnetic anisotropy. The surface magnetic anisotropy constant ($K_{so},\;K_{sd}$) of amorphous $Co_{89.5}Zr_{10.5}$ thin films are $0.02\;erg/\textrm{cm}^2$ and $0.55\;erg/\textrm{cm}^2$ respectively regardless of the film thickness except for $3,200\;{\AA}$ film. In case of $3,200\;{\AA}$ these values are $0.46\;erg/\textrm{cm}^2$ and $0.55\;erg/\textrm{cm}^2$ respectively.

• 한국세라믹학회지
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• 제43권2호
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• pp.79-84
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• 2006

We studied the microstructure and magnetic property of the pulsed DC magnetron sputtered $Zn_{\0.8}Co_{0.2}O$ film as a function of substrate temperatures. The X-ray patterns of the $Zn_{\0.8}Co_{0.2}O$ film showed a strong (002) preferential orientation at $500^{\circ}C$. The films with a crystallite size of 23-35 nm were grown in the form of nano-sized structure and this tendency was remarkable with increasing substrate temperature. The UV-visible result showed that the $Zn_{\0.8}Co_{0.2}O$ film prepared above $300^{\circ}C$ has a high optical transmittance of over $80\%$ in the visible region. The absorption bands were observed due to sp-d interchange action by $Co^{2+}$ complex ion and dd transition in the region from 500 to 700nm. The resistivity of the film was below $10^{-1}\;\Omega-cm\;above\;300^{\circ}C$. The AGM analysis results for the all films showed the magnetic hysteresis curves of ferromagnetic nature. The low electrical resistivity and room temperature ferromagnetism of ZnCoO thin films 'deposited above $300^{\circ}C$ suggested the possibility for the application to Diluted Magnetic Semiconductors (DMSs).

• Journal of Magnetics
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• 제3권2호
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• pp.55-63
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• 1998

Magnetic and magnetostrictive properties of amorphous Sm-Fe and Sm-Fe-B thin films are systematically investigated over a wide composition range from 14.1 to 71.7 at.% Sm. The films were fabricated by rf magnetron sputtering using a composite target composed of an Fe (or Fe-B) plate and Sm chips. The amount of B added ranges from 0.3 to 0.8 at. %. The microstructure, examined by X-ray diffraction, mainly consists of an amorphous phase in the intermediate Sm content range from 20 to 45 at.%. Together with an amorphous phase, crystalline phases of Fe and Sm also exist at low and high ends of the Sm content, respectively. Well-developed in-plane anisotropy is formed over the whole compositionrange, except for the low Sm content below 15 at.% and the high Sm content above 55 at %. As the Sm content increases, the saturation magnetization decreases linearly and the coercive force tends to increase, with the exception of the low Sm content where very large magnitudes of the saturation magnetization and the coercive force are observed due to the existence of the crystalline $\alpha$-Fe phase. The coercive force is affected rather substantially by the B addition, resulting in lower values of the coercive force in the practically important Sm content range of 30 to 40 at.%. Good magnetic softness indicated by well-developed in-plane anisotropy, a square-shaped hysteresis loop and a low magnitude of the coercive force results in good magnetostrictive characteristics in both Sm-Fe-B thin films. The magnetostrictive characteristics, particularly at low magnetic fields, are further improved by the addition of B; for example, at a magnetic field of 100 Oe, the magnitude of magnetostriction is -350 ppm in a Sm-Fe thin film and it is -470 ppm in a B containing Sm-Fe thin film.

• 한국자기학회:학술대회 개요집
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• 한국자기학회 2016년도 임시총회 및 하계학술연구발표회
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• pp.176-176
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• 2016