• 제목/요약/키워드: nano powder

검색결과 1,133건 처리시간 0.033초

유기 첨가제 및 NH4Cl 융제를 함유하는 분무용액으로부터 합성된 BaMgAl10O17:Eu 형광체의 특성 (Characteristics of BaMgAl10O17:Eu Phosphor Powders Prepared from Spray Solution with Organic Additives and NH4Cl Flux)

  • 이상호;구혜영;고다래;이수민;강윤찬
    • Korean Chemical Engineering Research
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    • 제48권1호
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    • pp.75-79
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    • 2010
  • 에틸렌디아민테트라아세트산, 구연산 및 $NH_4Cl$ 융제가 첨가된 분무용액으로부터 분무열분해법에 의해 얇은 막 구조의 전구체 분말들을 합성하였다. $1,200^{\circ}C$에서 소성 과정을 거친 유기 첨가제와 융제를 사용하지 않은 $BaMgAl_{10}O_{17}:Eu$ 형광체는 $1{\sim}5{\mu}m$ 크기의 구형이며, 두꺼운 막 형태의 속이 빈 구조를 가졌다. 반면에 에틸렌디아민아세트산과 구연산을 첨가하여 합성된 BAM:Eu 형광체는 판상 구조의 미세한 크기를 가졌다.$NH_4Cl$ 융제의 첨가량이 0, 6, 35 wt%일때 합성된 미세 형광체들의 결정자 크기는 각각 23, 35, 33 nm였다. 최대의 발광 세기를 나타내는 최적의 융제 첨가량은 형광체의 35 wt%였으며, 융제를 첨가하지 않은 분무용액으로부터 합성된 형광체의 발광 세기의 215%였다.

기계적합금화에 의한 $Fe/Al_2O_3$$Fe/TiO_2$계 나노복합분말의 제조 (Synthesis of $Fe/Al_2O_3$ and $Fe/TiO_2$ nanocomposite powder by mechanical alloying)

  • 이성희;이충효
    • 한국결정성장학회지
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    • 제19권4호
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    • pp.202-207
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    • 2009
  • 본 연구에서는 $Fe/Al_2O_3$$Fe/TiO_2$계 나노복합분말을 제조하기 위하여 실온 기계적 합금화법(MA)을 적용하였다. $Fe_3O_4-M$(M= AI, Ti)이고 여기서 순금속 Al 및 Ti은 고상반응 시 환원제로서 선택하였다. $Fe_3O_4$-순금속의 각각 25시간 및 75시간 MA 처리한 결과 $Fe/Al_2O_3$$Fe/TiO_2$ 나노복합분발이 얻어졌으며, 이것은 나노결정립의 ${\alpha}$-Fe 기지에 $Al_2O_3$$TiO_2$가 각각 미세하게 분산된 나노복합분말임을 알 수 있었다. 또한 Fe$_3$O$_4$-AI계에서 보다 짧은 반응 시간에 복합분말이 생성되는 것은 $Fe_3O_4$의 Al에 의한 환원반응 시 큰 반응열에 기인하는 것으로 사료된다. MA법으로 제조된 $Fe/TiO_2$ 복합분말의 X선 회절분석으로부터 ${\alpha}$-Fe 결정립 크기는 30 nm 임을 알 수 있었다. 또한 MA 과정 중 시료의 자기 측정으로부터 $Fe_3O_4$의 순금속 Al 및 Ti 에 의한 고상환원반응 과정을 자세히 관찰할 수 있었다.

초미세 나노분말 γ-Fe2O3의 초상자성 특성연구 (Superparamagnetic Properties of γ-Fe2O3 Nanoparticles)

  • 이승화;이재광;채광표;안성용
    • 한국자기학회지
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    • 제20권5호
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    • pp.196-200
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    • 2010
  • Sol-gel 법을 이용하여 초상자성 나노 입자 $\gamma-Fe_2O_3$를 제조하였다. 입자의 크기 및 자기적 성질을 x-선 회절법(XRD), Mossbauer 분광법, 진동시료 자화율 측정기(VSM)를 이용하여 연구하였다. x-선 회절 실험결과 150 이상에서 열처리한 입자는 순수한 cubic spinel 구조를 가지며, $150^{\circ}C$에서 열처리한 $\gamma-Fe_2O_3$의 평균입자 크기는 7 nm로다. Mossbauer 분광실험으로 $150^{\circ}C$에서 열처리한 입자는 상온에서 초상자성의 특성을 가지고 있음을 알 수 있었으며 초상자성의 특성을 잃어버리는 차단온도 $T_B$$183^{\circ}C$로 결정하였으며, 또한 자기이방성상수 K = $1.6{\times}10^6erg/cm^3$의 값을 얻었다. $150^{\circ}C$에서 열처리한 $\gamma-Fe_2O_3$의 VSM 측정 결과로부터 $150^{\circ}C$에서 열처리한 $\gamma-Fe_2O_3$의 경우 상온에서 초상자성의 특성을 확인 할 수 있었다.

Structure and Magnetic Properties of Ho and Ni Co-doped BiFeO3 Ceramics

  • Hwang, J.S.;Yoo, Y.J.;Park, J.S.;Kang, J.H.;Lee, K.H.;Lee, B.W.;Kim, K.W.;Lee, Y.P.
    • 한국진공학회:학술대회논문집
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    • 한국진공학회 2014년도 제46회 동계 정기학술대회 초록집
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    • pp.183-183
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    • 2014
  • Recently, multiferroic materials gain much attention due to their fascinating fundamental physical properties. These materials offer wide range of potential applications such as data storage, spintronic devices and sensors, where both electronic and magnetic polarizations can be coupled. Among single-phase multiferroic materials, $BiFeO_3$ is typical because of the room-temperature magnetoelectric coupling in view of long-range magnetic- and ferroelectric-ordering temperatures. However, $BiFeO_3$ is well known to have large leakage current and small spontaneous polarization due to the existence of oxygen vacancies and other defects. Furthermore the magnetic moment of pure $BiFeO_3$ is very weak owing to its antiferromagnetic nature. Recently, various attempts have been performed to improve the multiferroic properties of $BiFeO_3$ through the co-doping at the A and the B sites, by making use of the fact that the intrinsic polarization and magnetization are associated with the lone pair of $Bi^{3+}$ ions at the A sites and the partially-filled 3d orbitals of $Fe^{3+}$ ions at the B sites, respectively. In this study, $BiFeO_3$, $Bi_{0.9}Ho_{0.1}FeO_3$, $BiFe_{0.97}Ni_{0.03}O_3$ and $Bi_{0.9}Ho_{0.1}Fe_{0.97}Ni_{0.03}O_3$ bulk compounds were prepared by solid-state reaction and rapid sintering. High-purity $Bi_2O_3$, $Ho_2O_3$, $Fe_2O_3$ and $NiO_2$ powders with the stoichiometric proportions were mixed, and calcined at $500^{\circ}C$ for 24 h to produce the samples. The samples were immediately put into an oven, which was heated up to $800^{\circ}C$ and sintered in air for 1 h. The crystalline structure of samples was investigated at room temperature by using a Rigaku Miniflex powder diffractometer. The field-dependent and temperature-dependent magnetization measurements were performed with a vibrating-sample magnetometer and superconducting quantum-interference device.

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TiCl4를 출발원료로한 구형 Li4Ti5O12 분말합성 및 리튬이차 전지특성 (Electrochemical Properties of Lithium Secondary Battery and the Synthesis of Spherical Li4Ti5O12 Powder by Using TiCl4 As a Starting Material)

  • 최병현;지미정;권용진;김은경;남산
    • 한국재료학회지
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    • 제20권12호
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    • pp.669-675
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    • 2010
  • One of the greatest challenges for our society is providing powerful electrochemical energy conversion and storage devices. Rechargeable lithium-ion batteries and fuel cells are among the most promising candidates in terms of energy and power density. As the starting material, $TiCl_4{\cdot}YCl_3$ solution and dispersing agent (HCP) were mixed and synthesized using ammonia as the precipitation agent, in order to prepare the nano size Y doped spherical $TiO_2$ precursor. Then, the $Li_4Ti_5O_{12}$ was synthesized using solid state reaction method through the stoichiometric mixture of Y doped spherical $TiO_2$ precursor and LiOH. The Ti mole increased the concentration of the spherical particle size due to the addition of HPC with a similar particle size distribution in a well in which $Li_4Ti_5O_{12}$ spherical particles could be obtained. The optimal synthesis conditions and the molar ratio of the Ti 0.05 mol reaction at $50^{\circ}C$ for 30 minutes and at $850^{\circ}C$ for 6 hours heat treatment time were optimized. $Li_4Ti_5O_{12}$ was prepared by the above conditions as a working electrode after generating the Coin cell; then, electrochemical properties were evaluated when the voltage range of 1.5V was flat, the initial capacity was 141 mAh/g, and cycle retention rate was 86%; also, redox reactions between 1.5 and 1.7V, which arose from the insertion and deintercalation of 0.005 mole of Y doping is not a case of doping because the C-rate characteristics were significantly better.

공침법으로 합성한 이트리아 부분안정화 지르코니아 나노분말의 특성 (Properties of Yttria Partially Stabilized Zirconia Nano-Powders Prepared by Coprecipitation Method)

  • 윤혜온;신미영;안중재
    • 한국광물학회지
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    • 제19권2호
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    • pp.81-88
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    • 2006
  • [ $ZrO_2+Y_2O_3$ ] 계 분말결정을 $ZrOCl_2{\cdot}8H_O-YCl_33{\cdot}6H_2O$를 출발물질로 하여 공침법으로 합성하였다. 출발물질의 농도, 용액의 pH, 부분안정화제로 사용된 $Y_2O_3$의 양, 합성 후 소결온도 등 합성에 요구되는 실험변수에 따른 상 변이에 대한 연구결과를 바탕으로 실험조건을 고정시켜 3 mole% $Y_2O_3$를 포함하는 부분안정화 지르코니아 3YSZ를 합성할 수 있었다. 합성된 3YSZ의 소결특성에 따른 $ZrO_2$ 상전이에 대한 연구를 위하여 XRD, Raman, DTA 및 SEM을 사용하였다. 순수한 $ZrO_2$에 비하여 합성된 3YSZ는 $ZrO_2+Y_2O_3$ 계에서 $Y_2O_3$의 함량 면화에 따라 순수한 $ZrO_2$고온상의 단사정상에서 정방정상으로 상전이가 일어나게 되고 이때 Raman 스팩트럼이 낮은 파수쪽에서 현저하게 나타나는 것으로 쉽게 구분이 되었다.

Improved Physical Properties of Ni-doped $BiFeO_3$ Ceramic

  • Yoo, Y.J.;Park, J.S.;Kang, J.H.;Kim, J.;Lee, B.W.;Kim, K.W.;Lee, Y.P.
    • 한국진공학회:학술대회논문집
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    • 한국진공학회 2012년도 제42회 동계 정기 학술대회 초록집
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    • pp.250-250
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    • 2012
  • Recently, multiferroic materials have attracted much attention due to their fascinating fundamental physical properties and potential technological applications in magnetic/ferroelectric data storage systems, quantum electromagnets, spintronics, and sensor devices. Among single-phase multiferroic materials, $BiFeO_3$, in particular, has received considerable attention because of its very interesting magnetoelectric properties for application to spintronics. Enhanced ferromagnetism was found by Fe-site ion substitution with magnetic ions. In this study, $BiFe_{1-x}Ni_xO_3$ (x=0 and 0.05) bulk ceramic compounds were prepared by solid-state reaction and rapid sintering. High-purity $Bi_2O_3$, $Fe_3O_4$ and NiO powders were mixed with the stoichiometric proportions, and calcined at $450^{\circ}C$ for 24 h to produce $BiFe_{1-x}Ni_xO_3$. Then, the samples were directly put into the oven, which was heated up to $800^{\circ}C$ and sintered in air for 20 min. The crystalline structure of samples was investigated at room temperature by using a Rigaku Miniflex powder diffractometer. The Raman measurements were carried out with a Raman spectrometer with 514.5-nm-excitation Ar+-laser source under air ambient condition on a focused area of $1-{\mu}m$ diameter. The field-dependent magnetization and the temperature-dependent magnetization measurements were performed with a vibrating-sample magnetometer. The x-ray diffraction study demonstrates the compressive stress due to Ni substitution at the Fe site. $BiFe_{0.95}Ni_{0.05}O_3$ exhibits the rhombohedral perovskite structure R3c, similar to $BiFeO_3$. The lattice constant of $BiFe_{0.95}Ni_{0.05}O_3$ is smaller than of $BiFeO_3$ because of the smaller ionic radius of Ni3+ than that of Fe3+. The field-dependent magnetization of $BiFe_{0.95}Ni_{0.05}O_3$ exhibits a clear hysteresis loop at 300 K. The magnetic properties of $BiFe_{0.95}Ni_{0.05}O_3$ were improved at room temperature because of the existence of structurally compressive stress.

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스피넬 구조를 가지는 전이금속화합물(ZnCo2O4, NiCo2O4)의 열적 분석 및 열역학적 특성 연구 (The Study on Thermal Analysis and Thermodynamic Characteristics of Spinel Compounds(ZnCo2O4, NiCo2O4))

  • 김재욱;지명진;차병관;김철현;장원철;김종규
    • 대한화학회지
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    • 제54권2호
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    • pp.192-197
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    • 2010
  • 형광체나 반도체의 소자로 사용되는 전이금속화합물 중에서 나노(nano) 크기를 가지는 스피넬 화합물을 합성하였다. 스피넬 화합물의 크기, 합성여부, 열적분석과 화합물의 특성을 확인하기 위하여 열 중량 분석기(TGA), X-선 회절 분석기(XRD), 적외선 흡수 분광기(IR)를 사용하였다. Scherrer식을 이용하여 화합물의 평균 입자 크기가 13~16 nm임을 예측할 수 있었다. 본 논문에 사용된 실험방법은 졸-겔(sol-gel)법을 사용하였으며, 소성 온도는 낮은 온도에서 진행 되었다($350^{\circ}C$). Kinetic 함수인 활성화 에너지와 전환인자를 계산하기 위해서 Kissinger방법과 Arrhenius식을 이용하여 계산하였다. $ZnCo_2O_4$$NiCo_2O_4$의 활성화 에너지는 163.42 kJ/mol와 147.01 kJ/mol 값을 가지는 있음을 확인하였다. 그리고 spinel 화합물들의 열역학적 함수(${\Delta}G^{\varphi}$, ${\Delta}H^{\varphi}$, ${\Delta}S^{\varphi}$)를 결정하였다.

Cu2ZnSn(S,Se)4 Thin Film Solar Cells Fabricated by Sulfurization of Stacked Precursors Prepared Using Sputtering Process

  • Gang, Myeng Gil;Shin, Seung Wook;Lee, Jeong Yong;Kim, Jin Hyeok
    • 한국진공학회:학술대회논문집
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    • 한국진공학회 2013년도 제45회 하계 정기학술대회 초록집
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    • pp.97-97
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    • 2013
  • Recently, Cu2ZnSn(S,Se)4 (CZTSS), which is one of the In- and Ga- free absorber materials, has been attracted considerable attention as a new candidate for use as an absorber material in thin film solar cells. The CZTSS-based absorber material has outstanding characteristics such as band gap energy of 1.0 eV to 1.5 eV, high absorption coefficient on the order of 104 cm-1, and high theoretical conversion efficiency of 32.2% in thin film solar cells. Despite these promising characteristics, research into CZTSS based thin film solar cells is still incomprehensive and related reports are quite few compared to those for CIGS thin film solar cells, which show high efficiency of over 20%. I will briefly overview the recent technological development of CZTSS thin film solar cells and then introduce our research results mainly related to sputter based process. CZTSS thin film solar cells are prepared by sulfurization of stacked both metallic and sulfide precursors. Sulfurization process was performed in both furnace annealing system and rapid thermal processing system using S powder as well as 5% diluted H2S gas source at various annealing temperatures ranging from $520^{\circ}C$ to $580^{\circ}C$. Structural, optical, microstructural, and electrical properties of absorber layers were characterized using XRD, SEM, TEM, UV-Vis spectroscopy, Hall-measurement, TRPL, etc. The effects of processing parameters, such as composition ratio, sulfurization pressure, and sulfurization temperature on the properties of CZTSS absorber layers will be discussed in detail. CZTSS thin film solar cell fabricated using metallic precursors shows maximum cell efficiency of 6.9% with Jsc of 25.2 mA/cm2, Voc of 469 mV, and fill factor of 59.1% and CZTS thin film solar cell using sulfide precursors shows that of 4.5% with Jsc of 19.8 mA/cm2, Voc of 492 mV, and fill factor of 46.2%. In addition, other research activities in our lab related to the formation of CZTS absorber layers using solution based processes such as electro-deposition, chemical solution deposition, nano-particle formation will be introduced briefly.

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Effect of Core Morphology on the Decomposition of CCI₄ over the Surface of Core/Shell Structured Fe₂O₃/MgO Composite Metal Oxides

  • 김해진;강진;박동곤;권호진;Kenneth J. Klabunde
    • Bulletin of the Korean Chemical Society
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    • 제18권8호
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    • pp.831-840
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    • 1997
  • Core/shell structured composite metal oxides of Fe2O3/MgO were prepared by thermal decomposition of Fe(acac)3 adsorbed on the surface of MgO cores. The morphology of the composites conformed to that of the MgO used as the cores. Broad powder X-ray diffraction peaks shifted toward larger d, large BET surface area (∼350 m2/g), and the size of crystalline domains in nano range (4 nm), all corroborate to the nanocrystallinity of the Fe2O3/MgO composite which was prepared by using nanocrystalline MgO as the core. By use of microcrystalline MgO as the core, microcrystalline Fe2O3/MgO composite was prepared, and it had small BET surface area of less than 35 m2/g. AFM measurements on nanocrystalline Fe2O3/MgO showed a collection of spherical aggregates (∼80 nm dia) with a very rough surface. On the contrary, microcrystalline Fe2O3/MgO was a collection of plate-like flat crystallites with a smooth surface. The nitrogen adsorption-desorption behavior indicated that microcrystalline Fe2O3/MgO was nonporous, whereas nanocrystalline Fe2O3/MgO was mesoporous. Bimodal distribution of the pore size became unimodal as the layer of Fe2O3 was applied to nanocrystalline MgO. The macropores in a wide distribution which the nanocrystalline MgO had were absent in the nanocrystalline Fe2O3/MgO. The decomposition of CCl4 was largily enhanced by the overlayer of Fe2O3 on nanocrystalline MgO making the reaction between nanocrystalline Fe2O3/MgO and CCl4 be nearly stoichiometric. The reaction products were environmentally benign MgCl2 and CO2. Such an enhancement was not attainable with the microcrystalline samples. Even for the nanocrystalline MgO, the enhancement was not attained, if not with the Fe2O3 layer. Without the layer of Fe2O3, it was observed that the nanocrystalline domain of the MgO transformed into microcrystalline one as the decomposition of CCl4 proceeded on its surface. It appeared that the layer of Fe2O3 on the particles of nanocrystalline Fe2O3/MgO blocked the transformation of the nanocrystalline domain into microcrystalline one. Therefore, in order to attain stoichiometric reaction between CCl4 and Fe2O3/MgO core/shell structured composite metal oxide, the morphology of the core MgO has to be nanocrystalline, and also the nanocrystalline domains has to be sustained until the core was exhausted into MgCl2.