• 한국자기학회지
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• 제4권2호
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• pp.160-167
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• 1994

고보자력의 새로운 수평자기기록용 매체를 개발하기위해서 Co-P/Cr과 Co-P-Cr/Cr박막의 자기적 특성을 연구함였다. 상온데서 성막된 Co-P 이원합금의 경우 P의 함량이 9-12 at.%에서 835 Oe의 보자력을 나타내었다. Co-P 이원합금의 경우 P의 함량이 9-12 at.%에서 기판온도가 높을수록 보자력은 오히려 감소하였으며, 이것은 Co-P단일상이 Co와 $Co_{2}P$상으로의 분해에 기인하는 것으로 판단되낟. 그러나 P을 12 at.%이상으로 첨가하면 비정질상의 형성으로 보자력은 급격히 감소하였다. Co-P-Cr 삼원합금박막의 보자력은 Cr 함량이 증가함에 따라 증가하여 상온에서 성장한 $Co_{84}P_{10}Cr_{6}$의 박막에서 1020 Oe의 높은 보자력을 얻을 수 있었다.

• 한국자기학회지
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• 제9권4호
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• pp.203-209
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• 1999

CoCrTa/Cr 자성박막의 Cr 하지층에 Mo와 Si을 첨가하여 제조한 박막의 자기적 성질에 미치는 Mo와 Si의 영향에 대하여 조사하였다. 증착시 사용된 장비는 DC magnetron sputtering system이었고, CoCrTa 자성층의 두께는 30.0$\AA$으로 Cr 하지층의 두께는 700$\AA$으로 고정하였으며 기판의 가열온도는 26$0^{\circ}C$이었다. CrMo 하지층의 박막이 순수한 Cr 하지층에 비하여 약 200 Oe의 보자력 증가를 나타내었다. 하지만 Si을 첨가하였을 경우엔 첨가량의 증가에 따라 보자력이 점차 감소하는 것으로 나타났다. CrMo 하지층에서는Mo를 첨가함에 따라 Cr 하지츠의 (200)면의 결정배향성이 증가하였고, Mo를 첨가한 Cr(200)과 CoCrTa(110)의lattice misfit가 Si을 첨가한 경우보다 작았고, 이것이 보자력 증가의 원인이었다.

• 한국자기학회지
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• 제9권6호
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• pp.312-320
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• 1999

RF 마그네트론 스퍼터링으로 제조한 SmCo/Cr 박막의 스퍼터 제조조건에 따르는 자기적 특성에 관하여 연구하였다. Sm 조성이 약 20 at %이고 Cr(50 nm)/SmCo(40 nm, 50W, 20mT)/Cr(150 nm, 100W, 30 mT)인 조건에서 제조한 시편에서 3.2 kOe의 최대 보자력을 얻었다. SmCo/Cr의 보자력은 하지층 표면거칠기와 SmCo의 조성에 크게 영향을 받았다. Cr 하지층의 거칠기는 Ar 분압과 두께가 증가할수록 증가하고 이는 SmCo 입자의 고립을 증가시켜 보자력이 증가된다. 본 SmCo 박막 증착시 사용한 RF 투입전력 및 Ar 분압은 SmCo의 조성을 변화시키며 최적의 조성(약 20 at.%Sm)에서 최대 보자력을 보인다. 또한 RF 파워 증가나 Ar 분압 증가에 의해 생긴 Cr 하지층의 표면거칠기, 치밀하지 않은 주상 계면구조등의 결함이 자구벽 이동을 방해하여 보자력 증가에 영향을 끼친다.

• 산업기술연구
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• 제21권A호
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• pp.221-229
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• 2001

The effect of Mo underlayer on the magnetic properties of CoCrTa/Cr films deposited on glass substrates were investigated. The coercivity increased and the coercivity squareness decreased by introducing Mo underlayer. The coercivity increase was attributed to the increase of in-plane c-axis orientation and magnetic isolation of Co grains deposited on Cr/Mo underlayer. The decrease of coercivity squarenesses seemed to be caused by the increase of magnetic isolation. The increase of magnetic isolation of Co grains was attributed to the diffusion of Mo atoms into grain boundaries of Co films and the physical isolation of Co grains. The coercivity of CoCrTa/Cr/Mo showed maximum values at Mo thickness of $400{\AA}$. The appearance of the maximum coercivity at that thickness was attributed to the development of strong $Co(10{\bar{1}}0)$ and $Co(10{\bar{1}}1)$ preferred orientation.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2001년도 하계학술대회 논문집
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• pp.100-103
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• 2001

In order to investigate the magnetic properties of CoCr-based bilayered thin films on kind of underlayer, we introduced amorphous Si layer to Co-Cr(-Ta) magnetic layer as underlayer. With the thickness of CoCr, CoCrTa single layer, crystalline orientation and perpendicular coercivity was improved. It was revealed that by introducing the Si underlayer, the c-axis orientation of CoCr, CoCrTa magnetic layer was improved largely. However, with increasing Si film thickness, perpendicular coercivity and saturation magnetization of Cocr/si, CoCrTa/Si bilayered thin films was decreased. Grain size of bilayered thin films became larger.

• 대한치과기공학회지
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• 제40권3호
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• pp.125-131
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• 2018

Purpose: Automatic dental prosthesis manufacturing process was accelerated by the spread of dental CAD / CAM system. The CAD / CAM system with milling alloys were needed supplement. So, sintered alloy blocks were introduced. In this study, we want to study sintered alloy block. And to evaluate the alloy block manufacture and alloy properties. Methods: The alloy powders were prepared by high pressure water dispersion method. The sintered alloy blocks were prepared by low temperature pressing method. Their components observation were EDX, and the alloy structure was observed by XRD. Results: Co-Cr alloy powders were observed to have a circle shape with an average diameter of about $100{\mu}m$ and a Ni-Cr alloy powder had a circle shape with an average diameter of about $50{\mu}m$. The Co-Cr alloy block is composed of Co (34.62 wt%), Cr (17.33 wt%), Mo (2.98 wt%), Si (0.36 wt%) and C (44.17 wt%). The Ni-Cr alloy powder was composed of Ni (40.29 wt%), Cr (19.37 wt%), Mo (3.53 wt%), Si (0.52 wt%) and C (33.18 wt%). The peak of the Co and CoCr peaks were observed in the CoCr alloy body by the means of XRD study. Cr2Ni3 of the peak was observed in the Ni-Cr alloy material. Conclusion : As a result, the following conclusions were obtained. 1. Prepared by high-pressure water-law Co-Cr alloy powder has an average diameter $100{\mu}m$, Ni-Cr alloy powder was found to have the form of sphere having an average diameter $50{\mu}m$. 2. Co-Cr alloy and Ni-Cr alloy block produced by low-temperature processing showed a certain ratio. 3. In the XRD study, Co phase appeared in Co-Cr alloy block after sintering. and Cr2Ni3 phase appeared in Ni-Cr alloy block after sintering.

• 한국주조공학회지
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• 제27권3호
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• pp.120-125
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• 2007

The microstructure, mechanical properties and melting range of Ni-Cr-Mo based alloys were investigated to develop Be-free Ni-Cr-Mo base dental alloys for Porcelain-Fused-to-Metal Firing(PFM). All as-cast alloys showed dendritic structure. Rockwell hardness of 20Cr7Mo was increased with addition of Si and Ti. On the contrary, it was decreased with addition of Co. The duplex alloying elemental addition such as 3Co + xTi, 2Si + xCo and 2Si + xTi to 20Cr7Mo resulted in much increase of hardness. Rockwell hardness and compressive strength for 20Cr3CoSiTi or 17Cr6CoSiTi alloy that add Si-Ti had similar values compared to the commercial alloys. Melting range for 20Cr3CoSiTi and 17Cr6CoSiTi alloy that add Si-Ti showed similar or lower than commercial alloys. In conclusion, 20Cr3CoSiTi and 17Cr6CoSiTi alloys can be applied for commercial use.

• E2M - 전기 전자와 첨단 소재
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• 제11권10호
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• pp.72-77
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• 1998

The effects of Al micro-bumps on the magnetic properties of CoCr(Pt)Ta/Cr films deposited on glass substrates were investigated. The coercivity increased and the coercivity squareness decreased by incorporating Cr/Al underlayers. The cause of the coercivity increase is attributed to the reduction of Co(0002) texture, the increase of magnetic isolation of CoCr(Pt)/Ta grains, and the refinement of CoCr(Pt)/Ta grains deposited on Cr/Al underlayers. The effects of an Al overlayer on the magnetic properties of CoCr(Pt)Ta/Cr films were also studied. The decrease of coercivity squareness is ascribed to the magnetic isolation of CoCr(Pt)Ta grains.

• 한국표면공학회지
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• 제36권5호
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• pp.379-385
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• 2003

The surface morphology, the glossiness and the hardness of Zn-Cr and Zn-Cr-X(X:Co, Mn) alloy electrodeposits were investigated by using chloride bath with EDTA additive and flow cell system. The surface morphology of Zn-Cr alloy and Zn-Cr-Mn alloy changed from fine needle shape crystalline structure to colony structure of fine granular crystallites with increasing current density in the range of 20-100 $A/dm^2$. The surface morphology of Zn-Cr-Co alloy deposited from low Co concentration bath(2.5-10 g/$\ell$) was similar to that of Zn-Cr alloy, while that of Zn-Cr-Co alloy deposited from high cobalt concentration bath was fine granular crystalline structure in the same range of current density. The glossiness of Zn-Cr and Zn-Cr-Mn alloy increased noticeably with increasing current density, while that of Zn-Cr-Mn alloy decreased with increasing Mn concentration of bath in high current density region. The glossiness of Zn-Cr-Co alloy deposited from low Co concentration bath increased with current density while that of the alloy from high Co concentration bath decreased with increasing current density. The hardness of Zn-Cr and Zn-Cr-X alloy increased noticeably with current density.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 1992년도 추계학술대회 논문집
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• pp.7-10
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• 1992

CoNiCr/Cr and CoCrTa/Cr for longitudinal magnetic recording media were. prepared on Coming 7059 glass by RF magnetron sputtering. The thickness of Cr underlayer was varied from 500 to $3000{\AA}$ and. that of magnetic layer was $700{\AA}$. Coercivity and squareness were measured using V.S.M.(vibrating sample magnetometer). The coercivity of films increased with increasing Cr thickness when the films were unannealed. The coercivity of the films annealed in a 10 mtorr vacuum increased initially with annealing time and then saturated with further increase in annealing time. The coercivity value difference between the unannealed and annealed films increased with increasing the thickness of Cr underlayer No significant change was found in squareness after anneal, regardless of Cr underlayer thickness.