• Proceedings of the Korean Institute of Surface Engineering Conference
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• 2012.11a
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• pp.158-158
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• 2012

급속 열처리 온도의 변화가 라디오파 마그네트론 스퍼터링 방법으로 석영 기판 위에 증착된 $CaMoO_4:Tb$ 형광체 박막의 특성에 미치는 효과를 조사하였다. 형광체 박막의 결정 구조와 발광 특성은 각각 X-선 회절법과 광여기 발광 장치로 측정하였다. $500^{\circ}C$에서 열처리한 박막은 파장 영역 400-1100 nm에서 69%의 평균 투과율을 나타내었고, 열처리 온도가 증가함에 따라 박막의 평균 투과율은 감소하는 경향을 나타내었다.

• Proceedings of the Korean Institute of Surface Engineering Conference
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• 2012.05a
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• pp.195-195
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• 2012

$Eu^{3+}$ 이온의 농도비를 변화시키면서 고상 반응법을 사용하여 적색 형광체 $Sr_{1-1.5x}MoO_4:Eu_x{^{3+}}$ 분말을 합성하였다. 제조한 형광체의 결정 구조는 X-선 회절 장치를 사용하여 정방정계임을 확인하였고, 광학 특성은 형광 광도계를 사용하여 상온에서 측정하였다. $Eu^{3+}$ 이온의 농도비가 0.01 mol인 형광체의 경우에, 파장 295 nm로 여기시켰을 때 주된 발광은 파장 619 nm에 최대 세기를 갖는 적색 형광을 나타내었으며, 최대 흡수 스펙트럼은 넓은 밴드를 갖고 파장 302 nm에서 관측되었다.

• Electrical & Electronic Materials
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• v.9 no.3
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• pp.270-276
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• 1996

As methane concentration was varied, the textures of diamond films deposited on Si(100)substrate were observed by XRD,SEM and Raman spectroscope. As a result, $O_{2}$ plasma etching has been useful to observe microscopic structure of diamond films by SEM. The cross section of diamond films deposited on Si(100)substrate with 4% concentration of methane to hydrogen was a polycrystal like a pillar. The diamond crystal like a pillar has been oriented to (110)surface and the high quality diamond film with FWHM of Raman spectra being 3.8 $cm^{-1}$ / has been grown. As time goes by deposition time, the preferred orientation increases

• Journal of the Korean Vacuum Society
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• v.20 no.3
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• pp.176-181
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• 2011

$Y_{1-x}BO_3:Ce_x^{3+}$ ceramic phosphors were synthesized with changing the concentration of $Ce^{3+}$ ion by using a solid-state reaction method. The crystal structure, surface morphology, and optical properties of the blue phosphors were investigated by using X-ray diffractometer (XRD), scanning electron microscopy, and photoluminescence and photoluminescence excitation spectrophotometry, respectively. The XRD results showed that the main peak of the phosphor powders occurs at (401)와 ($31\bar{2}$) planes. As for the optical properties, the excitation spectrum occurred at 243 nm and the value of blue emission intensity peaking at 469 nm reached the maximum when the concentration of $Ce^{3+}$ ion was 0.10 mol.

• Proceedings of the Korean Vacuum Society Conference
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• 2015.08a
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• pp.185.1-185.1
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• 2015

본 연구에서는 라디오파 마그네트론 스퍼터링 방법을 사용하여 증착 온도를 변화시켜면서 Eu 이온이 도핑된 MgMoO4 적색 형광체 박막을 사파이어 기판 상부에 성장하였다. 타겟은 고상반응법을 사용하여 직접 제작하였다. 형광체 박막의 구조, 표면, 광학적 특성은 X-선 회절장치, 주사전자현미경, 투과도 및 광여기발광 측정장치를 사용하여 측정하였다, 증착 온도는 100, 200, 300, $400^{\circ}C$이었으며, 증착 후 $870^{\circ}C$에서 열처리 공정을 실행하였다. 이와 더불어, $400^{\circ}C$에서 증착한 박막을 다양한 온도 $770-920^{\circ}C$에서 열처리를 수행하여 각각의 특성을 분석하였다. 증착 온도 $200^{\circ}C$에서 성장한 박막의 경우에 614 nm에 피크를 갖는 주 적색 발광 피크가 관측되었으며, 열처리 온도를 달리한 박막의 경우에는 $920^{\circ}C$에서 가장 강한 발광 피크가 나타났다. UV-VIS 분광광도계를 사용하여 박막의 투과도와 흡광도를 측정하였으며, Tauc의 모델을 사용하여 밴드갭 에너지를 계산하였다. 증착 온도 변화에 따라 성장된 박막의 투과도는 평균 82% 이상 이었으며 밴드갭 에너지는 4.1 eV이었다. 박막의 결정 구조는 단사정계임을 확인하였다. 특히, 결정 입자, 발광 피크의 세기와 투과도의 상관 관계를 조사하였다.

• Proceedings of the Materials Research Society of Korea Conference
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• 1994.11a
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• pp.86-86
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• 1994

박막 EL소자의 투명전극으로 제작된 ITO막의 전기적, 광학적 특성을 조사하였다. Plama CVD방법으로 제작된 ITO막은 증착시 산소결핍으로 인한 비 다량결합(non-stochiometry) 에 의해 In이 석출되어 흑화현상이 일어나 전기전도도와 광투과율을 향상을 위해 산소분위기에서 30$0^{\circ}C$로 4분간 열처리를 행하였다. 한편 ITO막의 비저항 $\rho$와 광투과율 T를 Van der pauw법과 단색 분광계로 각각 측정하였다. 그 결과 상온에서 10-15$\Omega$/$\square$의 면저항과 400-1000nm의 파장영역에서 85-95%의 광투과율을 가져 박막 EL소자의 투명전극 조건을 만족하였다. 열처리에 대학 ITO막의 구조적 특성을 알아보기 위해 X-선회절장치(JEOL.JDX-8030)로 조사하였다. Fig.1은 X-선 회절 패턴을 나타낸다. 열처리후 ITO막은 상대적으로 최대 강도(peak intensity) 가 증가함으로써 열처리에 의해 결정성 향상이되었음을 알수 있다. Fig.2는 파장에 따른 ITO막의 광투과도를 나타낸다.

• Journal of the Korean Chemical Society
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• v.38 no.11
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• pp.827-832
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• 1994

The crystal structure of bis(N-methylphenazinium) bis(oxalato)palladate(II) has been determined by X-ray crystallography. Crystal data: ((C_{13}H_{11}N_2)_2[Pd(C_2O_4)_2]) $M_w$ = 672.93, Triclinic, Space Group P1 (No = 2), a = 7.616(8), b = 9.842(3), c = $20.335(7)\AA$, $\alpha$ = 103.53(3), $\beta$ = 90.00(5), $\gamma$ = $112.38(5)^{\circ}$, Z = 2, $V = 1363(2){\AA}^3\;D_c = 1.639\;gcm^{-3},\;{\mu} = 7.3\;cm^{-1},\;F(000) = 680.0$. The intensity data were collected with $Mo-K\alpha$ radiation (${\lambda}$= 0.7107\;\AA)$ on an automatic four-circle diffractometer with a graphite monochromater. The structure was solved by Patterson method and refined by full matrix least-square methods using Killean & Lawrence weights. The final R and S values were $R = 0.069,\;R_w = 0.050,\;R_{all} = 0.069$ and S = 5.45 for 3120 observed reflections. Both cation and anion complexes are essentially planar and have dihedral angles of 6.3(6) and $57.06(6)^{\circ}$ between their planes. The planar complex anions are sandwiched between slightly bent cations. The interplanar separations of two triads are 3.328 and 3.463 $\AA$, respectively. The triads are stacked along b-axis, but their orientations are different based on dihedral angle $59.08(9)^{\circ}$ of two complex anions.

• Journal of the Korean Chemical Society
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• v.37 no.6
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• pp.599-603
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• 1993

Crystal structure of bis(1,2-diaminopropane)palladium(II) bis(oxalato)palladate(II) has been determined by X-ray crystallography. Crystal data: $Pd_2C_{10}H_{10}N_{4}O_{8}$, $M_W$ = 573.09, orthorhombic, space group $P_{ccn}$ (No = 56), a = 16.178(5), b = 16.381(6), c = 6.685(2)$\{AA}$, V = 1771.6 $\{AA}^3$, $M_W$W = 573.09, $D_c$ = 2.014 g${\cdot}c\;m^{-3}$, Z = 4, T = 294K, F(000) = 1056.0 and $\mu$ = 20.466 c$m^{-1}$. The intensity data were collected with $Mo-K\alpha$ radiation (${\lambda}$ = 0.7107 $\AA)$ on an automatic four-circle diffractometer with a graphite monochromater. The structure was solved by Patterson method and refined by full matrix least-squares methods using Pivot weights. The final R and S values were R = 0.065, $R_W = 0.059, R_{all}$ = 0.065 and S = 4.315 for 605 observed reflections. Both cation and anion complexes are essentially planar and have dihedral angle of $18(l)^{\circ}$ between thier planes. In the crystal structure, they do not have the Magnus's salt type mixed stacks; instead, the complex anions form regular stacks along the c-axis with the M-M bond length of $3.343(5)\AA$ and their stacks are surrounded by the complex cations through hydrogen bonds with the nitrogen-oxygen distances of 2.94(3) and $3.31(4)\AA.$

• Korean Journal of Crystallography
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• v.7 no.1
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• pp.36-43
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• 1996

The crystal structure Tris(ethylenediamine)nickel(II)Dichromate has been determined by X-ray crystallography. Crystal data: a=8.268(2), b=13.865(2), c=14.921(2)Å, γ=102.04(2)°, V=1672.9(5)Å3, Z=4, Monocline, P21/b (space group No.=14), Dcalc=1.806 gcm-3, μ=24.05 cm-0.1. The intensity data were collected with Mo-Kα radiation(λ=0.7107Å) on an automatic four-circle diffractometer with a graphite monochromator. The structure was solved by Patterson method and refined by full matrix least-square methods using unit weights. The final R and S values were R=0.045, Rw=0.051, Rall=0.059 and S=2.171for 2248 observed reflections. The two carbon atoms of a ring of Ni(en)-ion were split into crossed four atoms. In consideration of α- and β-angles of two rings of a disordered ethylenediamine of Nien3-ion and the hydrogen bonds between Ni(en)3-cation and Cr2O7-anion, the configuration of Ni(en)3-ion is assumed to be disordered with Λδδδ and Λδδλ.

• Korean Journal of Crystallography
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• v.13 no.1
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• pp.21-24
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• 2002

The crystal structure of cholesteryl crotonate was investigated by X-ray diffraction. Crystallo-graphic data for the title compound: P2₁, a = 13.446(4) , b = 11.802(3) , c = 18.782(5) , β = 103.99(2)°, Z = 4. Reflections were collected with an Enraf-Nonius CAD-4 diffractometer equipped with a graphite monochromator. The structure was solved by direct methods and refined by least-squares analyses. The final R value was 0.092 for 1604 reflections. The cholesterol fragment of the title compound were in good agreement with those for related cholesterol derivatives. The molecules were stacked in clearly separated layers. At the center of the layers, there were cholesterol-cholesteryl interactions between the symmetry-related A molecules and the cholesteryl-C(17) side chain of B molecules. There were also interactions between the C(17) side chain of A molecules and the crotonate chains off and B molecules in the interface region between layers. The crystal structure of the title compound turned out to be isostructural with those of cholesteryl ethylcarbonate, cholesteryl propylcarbonate, and cholesterol crotylcarbonate. The crystals show the liquid crystalline state having the cholesteric phase.