• Title/Summary/Keyword: SmCo

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Magnetic Properties of SmCo Thin Films Grown by Using a Nd-YAG Pulsed Laser Ablation Method (Nd-YAG Pulsed Laser Ablation법으로 제작한 SmCo계 박막의 자기특성)

  • 김상원;양충진
    • Journal of the Korean Magnetics Society
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    • v.10 no.1
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    • pp.30-36
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    • 2000
  • SmCo films were deposited on Si(100) substrate by a Nd-YAG pulsed laser ablation of the targets of Sm$\_$100-x/Co$\_$x/ (73$\leq$x$\leq$93) at the substrate temperature of 600∼700$\^{C}$ and the laser beam energy density of Q switching mode or fixed Q mode. The magnetic properties of the films obtained from the Q switching mode exhibited a 4 $\pi$ Ms of 5200∼7700 Gauss, iHc of 190-250 Oe, and 4$\pi$M$\_$r//4$\pi$M$\_$s/ of 0.4∼0.74, respectively, while the fixed Q mode gave the magnetic properties of corresponding films of a 4$\pi$M$\_$r//4$\pi$M$\_$s/ = 0.32∼0.91 and iHc of 430-6290 Oe, respectively. The fixed Q mode gave the better magnetic properties of the SmCo films which seems to be due to a formation of magnetically hard minor phases in droplet of Sm-rich intermetallics. However, the resultant rough surface of the SmCo films is a problem to be solved by a continued study.

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The effect of Thin Film magnet on soft magnetic thin film (박막자석이 연자성박막에 미치는 바이어스 효과)

  • Kim, Young-Hak;Shin, Kwang-Ho
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2003.05a
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    • pp.101-104
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    • 2003
  • The maximum coercive force of SmCo thin film was obtained at the Sm=28.2% and dc bias field was generated to CoZrNb, soft magnetic thin film, deposited on the SmCo thin film. DC field point having the maximum permeability for CoZrNb was shifted to higher dc field. DC field strength increased as the length of easy direction of magnetization decreased and 60Oe was measured for $3mm{\times}0.5mm$ sample.

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Magnetic Layer Thickness Dependence on Magnetic Switching volume of CoSm/Cr Thin Films (CoSm/Cr 박막의 자성층 두께에 따른 자기역전부피)

  • 정순영;김현수
    • Journal of the Korean Magnetics Society
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    • v.11 no.6
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    • pp.262-266
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    • 2001
  • The magnetic switching volume is known as an important parameter to understand the magnetization reversal process, thermal stability of the written information and media noise. This parameter is influenced significantly by the microstructure of the magnetic layer as well as underlayer. Therefore, we fabricated CoSm/Cr thin films with varying magnetic layer thickness under constant sputtering by using a dc magnetic sputtering machine. The magnetic layer thickness effect on the magnetic switching volume have been studied by the means of magnetic viscosity and dc demagnetization remanence curve mesurements. From these measurements, we found that the switching volumes increased with increasing the magnetic layer thickness, whereas the coercivity showed different behavior. These may be a result of the increased intergranular coupling and the larger volume fraction of the magnetic layer.

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Effects of Ag Seed Layer on the Magnetic Properties and the Microstructural Evolution of SmCo/Cr Thin Films (Ag 씨앗층이 SmCo/Cr 박막의 자기적 특성과 미세구조에 미치는 영향)

  • 이성래;고광식;김영근
    • Journal of the Korean Magnetics Society
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    • v.11 no.2
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    • pp.63-71
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    • 2001
  • The effects of an Ag seed layer on the magnetic properties and the microstructural evolution of SmCo/Cr thin films deposited on glass substrates were investigated. Coercivity of the films is 2.0 kOe when the thickness of Ag seed layer was 1nm thick, but it increased to 2.7 kOe when the Ag seed layer thickness is 3 nm. The increase of coercivity for film with 3 nm-thick Ag is due to roughness of Cr and grain size of Cr by the Ag microbumps. Ar partial pressure influenced on the formation of Ag microbumps, for example, they were formed at 5 mTorr when Ag thickness was 1 nm. The mechanism of magnetization reversal of the SmCo films changed from domain wall motion to domain rotation as the Ag inserted. This was thought to be due to inhibition of domain wall motion by the reduction of Cr grain size and the increase of roughness.

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Optimum Condition of Micro Fuse Fusing as a Function Changed Thickness of Thermosetting Ink Epoxy (열경화성 잉크 에폭시의 두께 변화에 따른 마이크로 퓨즈 용단의 최적 조건)

  • Kim, Do-Kyeong;Hwang, Neung-Hwan;Kil, Tae-Hong;Lee, Soo-Hwa;Seo, Dae-Man;Kim, Min-Ho;Kim, Jong-Sick
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.27 no.10
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    • pp.623-629
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    • 2014
  • For the semiconductor device safety from over current in the digital electronic circuit system must be surely designed that it's surface mount type micro fuse device. In this paper, We has analysed to the fusing character of micro fuse as a function changed thickness of thermosetting ink epoxy. To the change of thermosetting ink epoxy thickness with in production lot, in the electrically character (fusing test in the 2 multiple over current and 10 multiple over current, surface temperature test in the 1.25 multiple over current) of micro fuse has been tested. According to the electrically character result, changed thickness of thermosetting ink epoxy in designed micro fuse withheld direct effect in both end resistance changes. Also, because high thermal energy in the micro fuse test of over current was occurred to effect such as thermal runaway and explosion. Therefore, screen printing process in the design of micro fuse using thermosetting ink epoxy is very important for production quality improvement.

Effect of Magnetic Properties on the Zr contents of Sm(CO.688-xFe.242Cu.07Zr x)7.404 Sintered Magnets (Sm(CO.688-xFe.242Cu.07Zr x)7.404소결자석의 자기적 특성에 미치는 Zr의 영향)

  • Jung, Woo-Sang;Kim, Yoon-Bae;Jeung, Won-Young
    • Journal of the Korean Magnetics Society
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    • v.12 no.5
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    • pp.189-194
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    • 2002
  • Microstructure and magnetic properties of Sm-Co sintered magnet were investigated with the variation of Zr content and their solution treatment and aging temperatures. The fraction of eutectic structure and the size of eutectic area decreased with increasing x value of cast Sm(C $O_{.688-x}$F $e_{.242}$C $u_{.07}$Z $r_{x}$)$_{7.404}$ alloys. On the other hand, x=0.022 ingot had finer dendritic structure compared to the other alloys. The sintered magnet of Sm(C $O_{.688-x}$F $e_{.242}$C $u_{.07}$Z $r_{x}$)$_{7.404}$ had well defined cell structure which is composed of cell boundary Sm $Co_{5}$ and cell interior S $m_2$Co/ssub 17/ phase. Cell boundary Sm $Co_{5}$ phase has 20nm thickness and its relative angle was 120$^{\circ}$ in x=0.018 and 0.022 alloys. Cell size was decreased with increasing Zr contents. But, x=0.026 alloy has diffuse cell boundary and irregular shape compared to x=0.022 and 0.018 alloys. Maximum value of coercive force and maximum energy Product were obtained from x=0.022 alloys. Optimum solution treatment temperature of Sm(C $O_{.688-x}$F $e_{.242}$C $u_{.07}$Z $r_{x}$)$_{7.404}$ alloy was 1170 $^{\circ}C$ and 1st aging temperature of two step aging process for higher coercivity was 850 $^{\circ}C$.