• Journal of Magnetics
• /
• 제3권1호
• /
• pp.4-8
• /
• 1998

Two different compositions of melt spun magnetic alloys, $ Nd_4Fe_{80}B_{16} and Nd_4Fe_{76}Co}\_3Hf_{0.5}Ga_{0.5}B_{16},$ were characterized in terms of magnetic properties and thermal behaviors. It was found that the addition of Hf and Ga effectively slow down the crystallization rate of the nanocomposite $ Nd_2Fe_{14}B/Fe_3B$ magnet. Coercivity(iHc) changes only slightly with varying the post annealing conditions confirming that iHc is not a sensitive magnetic quantity as a function of grain size and exchange coupled interaction. The experimentally observed behaviors of Mr and Hc do not vary monotonously with in-creasing grain size which is not in agreement with the numerically calculated result near the critical grain size (dc). The plot of the grain size dependence for the remanence and coercivity in isotrop!c nanocomposite magnets has been revised in this study. The maxium energy product, $(B, H)_{max}$ =15.34 MGOe, and a reduced remanence, Mr/Ms=0.84 were obtained, respectively.

• 한국세라믹학회지
• /
• 제29권12호
• /
• pp.942-948
• /
• 1992

Ultrafine iron oxide powder, {{{{ gamma }}-Fe2O3 and $\alpha$-Fe2O3, were prepared by the thermal decomposition of organometallic compounds. The formation process of powder includes the thermal decomposition and oxidation of the organometallic precursors, Fe(N2H3COO)2(N2H4)2 (A) and N2H5Fe(N2H3COO)3.H2O (B). The organometallic precursors, A and B, were synthesized by the reaction of ferrous ion with hydrazinocarboxylic acid, and characterized by quantitative analysis and infrared spectroscopy. The mechanistic study for the thermal decomposition was performed by DAT-TG. The iron oxide powder was obtained by the heat treatment of the precursors at 20$0^{\circ}C$ and $600^{\circ}C$ for half an hour in air. The phases of the resulting product were proved {{{{ gamma }}-Fe2O3 and $\alpha$-Fe2O3 respectively. The particle shape was equiaxial and the particle size was less than 0.1 ${\mu}{\textrm}{m}$. Magnetic properties of the {{{{ gamma }}-Fe2O3 powder obtained from A and B was 234 Oe of coercivity, 64.26 emu/g of saturation magnetization, 23.59 emu/g of remanent magnetization and 24.1 Oe, 47.27 emu/g, 3.118 emu/g respectively. The value of $\alpha$-Fe2O3 powder was 1.494 Oe, 0.4862 emu/g, 0.1832 emu/g and 1,276 Oe, 0.4854 emu/g, 0.1856 emu/g respectively.

• 한국자기학회지
• /
• 제22권3호
• /
• pp.85-90
• /
• 2012

$Nd_2Fe_{14}B$ 화합물 결정의 산화 및 미세 $Nd_2Fe_{14}B$ 결정입자의 보자력에 미치는 산화의 영향을 조사하였다. $Nd_2Fe_{14}B$ 화합물 결정의 산화속도는 $Nd_{15}Fe_{77}B_8$ 합금 잉곳 중의 과잉 성장시킨 $Nd_2Fe_{14}B$ 결정립을 이용하여 조사하였다. $Nd_2Fe_{14}B$ 화합물 결정의 산화는 이 결정상의 ${\alpha}$-Fe, $Fe_3B$, 및 Nd 산화물 복합상으로의 분해에 의해 일어 났다. $Nd_2Fe_{14}B$ 화합물 결정의 산화속도는 결정 방위와는 무관하였다. 산화반응 속도 식은 단순한 직선관계로 나타났다. $Nd_2Fe_{14}B$ 화합물 결정의 산화에 대한 활성화에너지는 약 26.8 kJ/mol로 계산되었다. HDDR 처리한 $Nd_{15}Fe_{77}B_8$ 합금을 볼밀링하여 임계단자구 크기에 유사한 미세한 $Nd_2Fe_{14}B$ 결정입자를 제조하고, 이 입자들을 이용하여 보자력에 미치는 산화의 영향을 조사하였다. 임계단자구 크기에 유사한 미세한 $Nd_2Fe_{14}B$ 결정입자(${\fallingdotseq}0.3\;{\mu}m$)는 9 kOe 이상의 높은 보자력을 가졌다. 그러나, 이 보자력은 공기 중에서 온도 상승에 따라 급격하게 저하하였다($200^{\circ}C$에서 2 kOe 이하). 이러한 급격한 보자력의 감소는 산화에 의해 미세 입자의 표면에 형성된 연자성 ${\alpha}$-Fe 및 $Fe_3B$ 상 때문으로 판단되었다.

• 한국자기학회:학술대회 개요집
• /
• 한국자기학회 2002년도 동계연구발표회 논문개요집
• /
• pp.214-215
• /
• 2002

High saturation magnetization (B$\_$s/) and excellent high frequency characteristics of magnetic thin films has been recognized as the most important requirement for further miniaturization and higher frequency operation in magnetic devices, such as magnetic heads and magnetic sensors. Up to now, Fe-X-N (X =Ti, Hf, and Al etc.) films with B$\_$s/ of 15 ∼ 19 kG and coercivity (H$\_$c/) of 0.5 ∼ 5.0 Oe have been successfully fabricated and proven to satisfy various requirements as a potential candidate for thin film head materials. (omitted)

• 한국자기학회지
• /
• 제5권5호
• /
• pp.412-415
• /
• 1995

By adding 1wt.% $HfB_{2}$ into $Nd_{3-4}Fe_{77-78.5}B_{18.5}$ alloys, the grain growth of $Fe_{3}B/Nd_{2}Fe_{14}B$ composite phases during annealing was found to be hindered by 40~50%. It is proposed that the addition of $HfB_{2}$ leads to the formation of fine dispersoids of $HfB_{2}$ in the $Fe_{3}B/Nd_{2}Fe_{14}B$ composite magnet. The maximum energy product($(B.H)_{max}$) as well as intrinsic coercivity($_{i}H_{c}$) for the $Nd_{3}Fe_{78.5}B_{18.5}\;+\;1wt.%\;HfB_{2}$ alloy were enhanced by more than 25% $(B.H)_{max}=10\;MGOe,\;_{i}H_{c}=2.5\;kOe)$ due to the addition of $HfB_{2}$ while remanent magntization($B_{r}$) was reduced slightly. Itis deduced that the formation of fine dispersoids will also play a role of magnetic domain pinning.

• 한국전기전자재료학회:학술대회논문집
• /
• 한국전기전자재료학회 2000년도 하계학술대회 논문집
• /
• pp.802-805
• /
• 2000

Anistropic [Ta/NdFeB/Ta] thin film was sputtered on heated Si substrate by Nd$\_$17/Fe$\_$74/B$\_$9/ target. The grain size of the films increased according to the increase of substrate temperature, and the film deposited at 650$^{\circ}C$ showed optimum coercivity. 4$\pi$M$\_$r/, $\_$i/H$\_$c/ and (BH)$\_$max/ measured perpendicular to the film plane of thin film deposited at 650$^{\circ}C$ are 12.3 kG, 9.9 kOe and 37 MGOe, respectivly.

• 한국자기학회지
• /
• 제10권2호
• /
• pp.62-66
• /
• 2000

비자성사이층 Cu 두께(30 $\AA$, 35 $\AA$, 40 $\AA$)를 달리한 glass(7059)/N $i_{81}$$Fe_{19}$(70 $\AA$)/Co(10 $\AA$)/Cu(t $\AA$)/Co(15 $\AA$)/N $i_{81}$$Fe_{19}$(35 $\AA$)N $i_{25}$M $n_{75}$(250 $\AA$)Ta(50 $\AA$) 스핀밸브박막(spin valve film; SVF) 을 dc 스퍼터링으로 제작하였다 이 시편을 진공 열처리 한 후 자유자성층의 상호결합세기(interlayer coupling field; $H_{inf}$ )와 보자력(coercivity; $H_{sf}$ )에 대한 열처리 순환횟수 및 비자성층 두께 의존성에 관련한 자기저항특성을 조사했다. Cu 두께가 35 $\AA$인 SVF의 경우에 교환결합세기(exchange coupling field; $H_{ex}$)가 620 Oe, 보자력( $H_{c}$)이 280 Oe 및 자기저항(magnetoresistance; MR)비가 2.5%를 보였다. $H_{inf}$ 와 $H_{cf}$ 는 모든 SVF가 열처리 순환 횟수에 따라 증가하는 경향을 보이다가 일정한 값으로 안정화되며 Cu 35 $\AA$인 경우는 열처리 순환 횟수 15회 이후에 각각 120 Oe 및 75 Oe를 유지한다. $H_{inf}$ 및 $H_{cf}$ 가 열처리 순환횟수 증가에 따라 증가하는 것은 열처리 효과에 의해 Cu층과 Co층의 계면섞임 증대에 의한 유효한 Cu층 두께 감소에 기인한다. Cu가 적정둘레 35 $\AA$ 보다 더 얇아지거나 두꺼워지면 계면섞임에 의한 효과는 각각 더 증대하거나 둔화되는 것으로 분석된다.으로 분석된다..

• Journal of Magnetics
• /
• 제4권4호
• /
• pp.119-122
• /
• 1999

Magnetic properties and crystal structures of (Fe1-XCoX) Pt (X = 0, 0.2, 0.4, 0.5, 0.6, 0.8 and 1.0) ternary thin films were investigated. The order-disorder phase transformation of FePt thin films during annealing was also studied by x-ray diffraction and M ssbauer spectroscopy. The magnetic thin films were deposited on glass substrates using a dc sputtering method and were subsequently annealed at 400~$700^{\circ}C$ in a high vacuum. The as-deposited films exhibited a high degree of the <111> preferred orientation and the preferred orientation was not destroyed even after the subsequent post annealing. The coercivity of the ($Fe_xCo_{1-x}$) Pt thin films annealed at $700^{\circ}C$ showed a minimum value at the equiatomic composition of the Fe and Co atoms. The ordered structure of the FePt alloy was thought to have formed from the disordered structure by an inhomogeneous process, which was confirmed by the asymmetric peak shapes and M ssbauer spectra.

• Journal of Magnetics
• /
• 제6권2호
• /
• pp.57-60
• /
• 2001

Mechanically alloyed $TbCu_7 -type \;Sm_{12.5}Fe_{87.5-x}Ti_x$(x=0, 2.5, 5, 7.5),and their nitrides have been studied systematically by X-ray diffraction, A.C. initial susceptibility, and pulsed magnetization measurement. In this series, the volume expansion by nitriding is 5.6%~7.3%, and the increment of the Curie temperature is in the range of 21$0^{\circ}C$~35$0^{\circ}C$. With increasing Ti content, the remanence decreases linearly due to the substitution of non-magnetic Ti, and the coercivity decreases rapidly from 34.6 kA/cm (43.5 kOe) for $\chi$=0 to 14.3 kA/cm (18 kOe) for $\chi$=7.5. In the $Sm_{12.5}Fe_{87.5-x}Ti_xN_y$ series, the best magnetic properties were obtained from .7Ti7Ny series, the best magnetic properties were obtained from $Sm_{12.5}Fe_{87.5}N_y$($\chi$=0) with $_iH_c$=34.6 kA/cm (43.5 kOe), $B_r=0.75 \;T, \;and (BH)_{max}=113.8 kJ/m^3$(10.9 MGOe).

• 전기화학회지
• /
• 제6권4호
• /
• pp.236-241
• /
• 2003

Magnetic CoW thin film alloys were electrodeposited from citrate baths to investigate the resulting microstructure and magnetic properties. Deposit tungsten (W) content in the films electrodeposited at $70^{\circ}C$ were independent of current density, while coercivity decreased from hard $(H_{c,//}\~150\;Oe\;and\;H_{c.{\bot}}\;\~240\;Oe)$ to soft magnetic properties $(H_{c,//}\~20\;Oe\;and\;H_{c.{\bot}}\;\~30\;Oe)$ with increasing current densities from $10\;to\;100mA{\cdot}cm^2$, with deposit W content $(\~40\%)$ relatively unaffected by the applied current density. X-ray diffraction analysis indicated that hcp $Co_3W$ phases [(200), (201) and (220) planes] in the CoW films electrodeposited at $70^{\circ}C\;and\;10mA{\cdot}cm^{-2}$ were dominant, whereas amorphous CoW phases with small amount of hcp $Co_3W$ [(002) planes] were dominant with deposition at $70^{\circ}C\;and\;100mA{\cdot}cm^{-2}$. At intermediate current densities $(25\;and\;50mA{\cdot}cm^{-2}),\;hop\;Co_3W$ phases [(200), (002), (201) and (220)] were observed. The average grain size was measured to be 30 nm from Sheller formula. It is suggested that the change of the deposit coercivities in the CoW thin films electrodeposited at $70^{\circ}C$ is attributed to the change of microstructures with varying the current density. Nanostructured $Co_3W/amorphous-CoW$ multilayers were fabricated by alternating current density between 10 and $100 mA{\cdot}cm^{-2}$, varying the individual layer thickness. The magnetic properties of $Co_3W/amorphous-CoW$ multilayers were strongly dependent on the thickness of the alternating hard and soft magnetic thin films. The nanostructured $Co_3W/amorphous-CoW$ multilayers exhibited a shift from low to high coercivities suggesting a strong coupling effect.