• Title/Summary/Keyword: Hexagonal phase

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A Study on Feasibility of Hexagonal Phase ZnS:$Mn^{2+}$ Phosphor for Low-voltage Display Applications

  • Shin, Sang-Hoon;Lee, Sang-Hyuk;You, Yong-Chan;Jung, Joa-Young;Park, Chang-Won;Chang, Dong-Sik
    • 한국정보디스플레이학회:학술대회논문집
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    • 2002.08a
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    • pp.815-818
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    • 2002
  • Mn doped hexagonal phase of ZnS has been studied as a yellow-orange phosphor for the application to fluorescent displays operated at low voltages. It was found that luminescence from $Mn^{2+}$ was increased as the Mn concentration was increased up to1.2 mol% of host lattice. This study has been attempted by adding trivalent ions such as $Al^{3+}$ or $Bi^{3+}$ to ZnS:Mn as an agent to do the efficient incorporation of Mn ions into ZnS:Mn lattice, resulting in a significant improvement in the phosphor performance, especially at low voltages.

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Electrical Properties of Y-type Hexagonal Ferrite (Y-type hexagonal Ferrite의 전기적 특성)

  • 박영민;최경만
    • Journal of the Korean Ceramic Society
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    • v.30 no.11
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    • pp.962-966
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    • 1993
  • Effect of Fe content on the electrical properties of Zn2Y (Ba2Zn2Fe12O22) was studied by investigating X-ray diffraction patterns, microstructure and resistivity of samples. When x(Ba2Zn2Fe12+xO$\delta$) is between +1 and -1, Zn2Y single phase was obtained and electrical resistivity was inversely proportional to Fe content. The possible defect model of Zn2Y was proposed based on the observation. When x<-1 or x>1, second phase(ZnFe2O4 for x<-1, ZnFe2O4 and Ba3Zn3Fe24O41 for x>1) were observed and the electrical resistivity was inversely proportional to the sample density. The activation energy of electrical conductivity of the stoichiometric Zn2Y was 0.49eV below 20$0^{\circ}C$ and 0.07eV above 50$0^{\circ}C$.

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Structural characteristics of [N(CH3)4]2CdCl4 determined by 1H MAS NMR, 13C CP/ MAS NMR, and 14N NMR

  • Lee, Seung Jin;Lim, Ae Ran
    • Journal of the Korean Magnetic Resonance Society
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    • v.19 no.1
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    • pp.18-22
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    • 2015
  • The structural geometry of $[N(CH_3)_4]_2CdCl_4$ in a hexagonal phase is studied by $^1H$ MAS NMR, $^{13}C$ CP/MAS NMR, and $^{14}N$ NMR. The changes in the chemical shifts for $^{13}C$ and $^{14}N$ in the hexagonal phase are explained by the structural geometry. In addition, the temperature dependencies of the spin-lattice relaxation time in the rotating frame $T_{1{\rho}}$ for $^1H$ MAS NMR and $^{13}C$ CP/MAS NMR are measured.

Crystal and Block Structures of Hexagonal Ferrites (육방정 페라이트의 결정과 Block 구조)

  • Shin, Hyung-Sup
    • Journal of the Korean Ceramic Society
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    • v.49 no.3
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    • pp.205-215
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    • 2012
  • It has been studied the crystal and block structures of the hexagonal ferrites with M, W, Y and Z types prepared by various coprecipitation-oxidation method. The structures have been refined with a Rietveld analysis of the powder X-ray diffraction pattern with high precision ($R_{WP}$ <0.09, $R_I$ <0.03). The density difference between the S-blocks was proportioned to the cobalt contents in hexagonal ferrites, but that between the R or T-blocks was relatively small. Compared with the blocks and cation-oxygen polyhedra in BaM ($BaFe_{12}O_{19}$), those were bulky to the normal direction for the c-axis in $Co_2W$ ($BaCo_2Fe_{16}O_{27}$) and to the parallel direction for the c-axis in $Co_2Y$ ($Ba_2Co_2Fe_{12}O_{22}$) and $Co_2Z$ ($Ba_3Co_2Fe_{24}O_{41}$). The S-blocks of $Co_2W$, $Co_2Y$, and $Co_2Z$ were unstable and distorted. Because the T-block of $Co_2Z$ was unstable, the T-block was decomposed into the Ba-rich phase and $Co_2W$ at high temperatures above $1200^{\circ}C$. A standard powder X-ray diffraction pattern for $Co_2Z$ was proposed as well.

Effect of Phase Change of $MoO_3$ on $H_2$ Spillover Kinetics over Pt/$MoO_3$ (Pt/$MoO_3$ 촉매에서 $MoO_3$ 상변화가 수소 spillover에 미치는 효과)

  • Kim, Jin-Gul;Kim, Seong-Soo;Yoo, Seung-Joon
    • Transactions of the Korean hydrogen and new energy society
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    • v.20 no.4
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    • pp.331-336
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    • 2009
  • 수소가 Pt/$MoO_3$로 흡장되는 현상을 XRD, TEM, CO 화학흡착 분석방법을 사용하여 조사하였다. 소성과정은 Pt/$MoO_3$ 촉매의 Chlorine 함유량을 감소하며 박막을 형성하였다. 소성전과 비교하여 수소 흡장량은 소성 후에 증가하였다. Orthorhombic Pt/$MoO_3$은 Hexagonal Pt/$MoO_3$보다 항상 수소 흡장량이 증가하였다. 상대적으로 Hexagonal Pt/$MoO_3$에서 수소 흡장량이 감소하는 이유는 Hexagonal 결정격자 내에 존재하는 $NH_4^+$ 이온에 기인하는 것으로 판단된다. 결정격자 내부로의 수소 침투시 암모니움 이온이 수소내부 기공에 장애물 역할을 하므로, 수소 흡장량이 감소하는 것으로 판단된다.

Effect of Oxygen Addition on Residual Stress Formation of Cubic Boron Nitride Thin Films (입방정 질화붕소 박막의 잔류응력 형성에 미치는 산소 첨가 효과)

  • Jang, Hee-Yeon;Park, Jong-Keuk;Lee, Wook-Seong;Baik, Young-Joon;Lim, Dae-Soon;Jeong, Jeung-Hyun
    • Journal of the Korean institute of surface engineering
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    • v.40 no.2
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    • pp.91-97
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    • 2007
  • In this study we investigated the oxygen effect on the nucleation and its residual stress during unbalanced magnetron sputtering. Up to 0.5% in oxygen flow rate, cubic phase (c-BN) was dominated with extremely small fraction of Hexagonal phase (h-BN) of increasing trend with oxygen concentration, whereas hexagonal phase is dominated beyond 0.75% flow rate. Interestingly, the residual stress in cubic-phase-dominated films was substantially reduced with small amount of oxygen (${\sim}0.5%$) down to a low value comparable to the h-BN case. This may be because oxygen atoms break B-N $sp^3$ bonds and make B-O bonds more favorably, increasing $sp^2$ bonds preference, as revealed by FTIR and NEXAFS. It was confirmed by experimental facts that the threshold bias voltage for nucleation and growth of cubic phase were increased from -55 V to -70 V and from -50 V to -60 V respectively. The reduction of residual stress in O-added c-BN films is seemingly resulting from the microstructure of the films. The oxygen tends to increase slightly the amount of h-BN phase in the grain boundary of c-BN and the soft h-BN phase of 3D network including surrounding nano grains of cubic phase may relax the residual stress of cubic phase.

Investigations of the Phase Behavior of N-dodecanocyl-N-methyl amido polyol carboxyl alkyl ether/N-dodecanocyl-N-alkyl Glucamine/Water System (N-도데카노실-N-메틸 아미도 폴리올 카르복시 알킬 에테르/(N-도데카노실-N-알킬 글루카민)/물계에서의 상거동 관찰)

  • Kang, Yun-Seog;Nam, Ki-Dae
    • Journal of the Korean Applied Science and Technology
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    • v.14 no.3
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    • pp.23-28
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    • 1997
  • The phase diagram for the surfactant mixture system of N-dodecanocyl-N-methyl amido polyolcarboxyl alkyl ether(DGC)/N-dodecanocyl-N-alkyl glucamine(DG)/water was studied usingpolarized microscopy, differential scanning calorimetry(DSC) and rheological measurements respectively. Using polarized microscopy, the textures of liquid crystal phases obtained at various surfactantconcentrations were investigated as a function of surfactant concentration and temperature, and phasetransitions between anisotropic liquid crystal phases and isotropic liquid phase were examined usingDSC measurements. Viscoelastic properties of surfactant solutions determined between hexagonal andlamellar liquid crystal phase by rheological measurements were approximately consistent with the resultsobtained by polarized microscopy and DSC. In the study for the phase of DGC/DG(5:5 mol ratio)/water system. It could be found that the hexagonal liquid crystal phase appeared at 25${\sim}$60wt% ofsurfactant, the cubic liquid crystal phase at 50${\sim}$65wt% and the lamellar crystal phase at above 70wt%.

Synthesis of Boron-Nitride Film by Plasma Assisted Chemical Vapor Deposition Using $BCl3-NH3-Ar$ Mixed Gas ($BCl3-NH3-Ar$계의 플라즈마화학증착공정을 이용한 질화붕소막의 합성)

  • 박범수;백영준;은광용
    • Journal of the Korean Ceramic Society
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    • v.34 no.3
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    • pp.249-256
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    • 1997
  • The effect of process parameter of plasma assisted chemical vapor deposition (PACVD) on the variation of the ratio between cubic boron nitride (c-BN) and hexagonal boron nitride (h-BN) in the film was in-vestigated. The plasma was generated by electric power with the frequency between 100 and 500 KHz. BCl3 and NH3 were used as a boron and nitrogen source respectively and Ar and hydrogen were added as a car-rier gas. Films were composed of h-BN and c-BN and its ratio varied with the magnitude of process parameters, voltage of the electric power, substrate bias voltage, reaction pressure, gas composition, sub-strate temperature. TEM observation showed that h-BN phase was amorphous while crystalline c-BN par-ticle was imbedded in h-BN matrix in the case of c-BN and h-BN mixed film.

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Self-Assembled Chiral Structures of Discoid Organic Molecule on Au(111)

  • Kim, Ji-Hoon;Khang, Se-Jong;Kwon, Young-Kyun;Park, Yongsup
    • Proceedings of the Korean Vacuum Society Conference
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    • 2013.02a
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    • pp.280-280
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    • 2013
  • Using both experimentaland theoretical methods, we have investigated the structural and electronic properties of self-assembled two-dimensional organic molecule (hexaaza-triphenylene-hexacarbonitrile, HATCN), which is used as an efficient OLED hole injection material, on Au(111) surfaces. Low-temperature scanning tunneling microscope (STM) measurements revealed that self-assembled linear and hexagonal porous structures are formed at atomic steps and terraces of Au(111), respectively. We also found that the hexagonal porous structure have chirality and forms only small (<1,000 nm2) phase-separated chiral domains that can easily change their chiral phase in subsequence STM images at 80 K. To explain these observations, we calculated the molecular-molecular and molecule-surface interaction energies by using first-principles density functional theory method. We found that the change of their chiral phase resulted from the competition between the two energies. These results have not only verified our experimental observations, but also revealed the delicate balance between different interactions that caused the self-assembed structures at the surface.

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Formation of Ti-B-N-C Ceramic Composite Materials via a Gas-Solid Phase Reaction

  • Yoon, Su-Jong
    • Korean Journal of Materials Research
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    • v.16 no.1
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    • pp.50-57
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    • 2006
  • Phase mixtures of Titanium boride, nitride, and carbide powder were produced by the reduction of a mixture of titanium and boron oxides with carbon via a gas-solid phase reaction. Boron oxides produce a vapour phase or decompose to a metal sub-oxide gaseous species when reduced at elevated temperature. The mechanism of BO sub-oxide gas formation from $B_2O_3$ and its subsequent reduction to titanium diboride for the production of uniform size hexagonal platelets is explained. These gaseous phases are critical for the formation of boride, nitride and carbide ceramics. For the production of ceramic phase composite microstructures, the nitrogen partial pressure was the most critical factor. Some calculated equilibrium phase fields has been verified experimentally. The theoretical approach therefore identifies conditions for the formation of phase mixtures. The thermodynamic and kinetic factors that govern the phase constituents are also discussed.