• 제목/요약/키워드: dopants

검색결과 288건 처리시간 0.029초

화염분무열분해법을 이용한 이산화세륨 나노분말 제조 (Preparation of CeO2 Nanoparticles using Flame Spray Pyrolysis)

  • 김선경;박수련;장한권;장희동
    • 한국입자에어로졸학회지
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    • 제12권2호
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    • pp.37-42
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    • 2016
  • $CeO_2$ nanoparticles were prepared by a flame spray pyrolysis from aqueous solution of cerium nitrate. The morphology, structure crystallinity and specific surface area of as-prepared nanoparticles were characterized by transmission electron microscopy (TEM), X-ray diffraction (XRD), and Brunauer-Emmett-Telle (BET). The $CeO_2$ nanoparticles about 5 nm in diameter showed a cubic fluorite structure and polyhedral morphology. The average particle size increased as the cerium nitrate concentration increased. UV absorption performance of the as-prepared nanoparticles was measured by UV-visible spectroscopy. UV absorption of $CeO_2$ nanoparticles was more effective than that of commercial $TiO_2$ nanoparticles. Effect of dopants such as Ti and Zn to $CeO_2$ nanoparticles on UV absorption properties was also investigated. In case of $Ti/CeO_2$, and $Zn/CeO_2$ nanoparticles, they showed a little higher UV absorption values compared with $CeO_2$ nanoparticles. The as-prepared nanoparticles can be promising materials with high UV absorption value.

Novel Synthesis and Nanocharacterization of Graphene and Related 2D Nanomaterials Formed by Surface Segregation

  • Fujita, Daisuke
    • 한국진공학회:학술대회논문집
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    • 한국진공학회 2015년도 제49회 하계 정기학술대회 초록집
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    • pp.60-60
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    • 2015
  • Nanosheets of graphene and related 2D materials have attracted much attention due to excellent physical, chemical and mechanical properties. Single-layer graphene (SLG) was first synthesized by Blakely et al in 1974 [1]. Following his achievements, we initiated the growth and characterization of graphene and h-BN on metal substrates using surface segregation and precipitation in 1980s [2,3]. There are three important steps for nanosheet growth; surface segregation of dopants, surface reaction for monolayer phase, and subsequent 3-D growth (surface precipitation). Surface phase transition was clearly demonstrated on C-doped Ni(111) by in situ XPS at elevated temperatures [4]. The growth mode was clarified by inelastic background analysis [5]. The surface segregation approach has been applied to C-doped Pt(111) and Pd(111), and controllable growth of SLG has been demonstrated successfully [6]. Recently we proposed a promising method for producing SLG fully covering an entire substrate using Ni films deposited on graphite substrates [7]. A universal method for layer counting has been proposed [8]. In this paper, we will focus on the effect of competitive surface-site occupation between carbon and other surface-active impurities on the graphene growth. It is known that S is a typical impurity of metals and the most surface-active element. The surface sites shall be occupied by S through surface segregation. In the case of Ni(110), it is confirmed by AES and STM that the available surface sites is nearly occupied by S with a centered $2{\times}2$ arrangement. When Ni(110) is doped with C, surface segregation of C may be interfered by surface active elements like S. In this case, nanoscopic characterization has discovered a preferred directional growth of SLG, exhibiting a square-like shape (Fig. 1). Also the detailed characterization methodologies for graphene and h-BN nanosheets, including AFM, STM, KPFM, AES, HIM and XPS shall be discussed.

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스퍼터링 방법으로 성장시킨 나노구조의 Ga 농도 변화에 따른 형상 변화

  • 김영이;우창호;조형균
    • 한국재료학회:학술대회논문집
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    • 한국재료학회 2009년도 추계학술발표대회
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    • pp.23.1-23.1
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    • 2009
  • ZnO is of great interest for various technological applications ranging from optoelectronics to chemical sensors because of its superior emission, electronic, and chemical properties. In addition, vertically well-aligned ZnO nanorods on large areas with good optical and structural properties are of special interest for the fabrication of electronic and optical nanodevices. To date, several approaches have been proposed for the growth of one-dimensional (1D) ZnO nanostructunres. Several groups have been reported the MOCVD growth of ZnO nanorods with no metal catalysts at $400^{\circ}C$, and fabricated a well-aligned ZnO nanorod array on a PLD prepared ZnO film by using a catalyst-free method. It has been suggested that the synthesis of ZnO nanowires using a template-less/surfactant-free aqueous method. However, despite being a well-established and cost-effective method of thin film deposition, the use of magnetrons puttering to grow ZnO nanorods has not been reported yet. Additionally,magnetron sputtering has the dvantage of producing highly oriented ZnO film sat a relatively low process temperature. Currently, more effort has been concentrated on the synthesis of 1D ZnO nanostructures doped with various metal elements (Al, In, Ga, etc.) to obtain nanostructures with high quality,improved emission properties, and high conductance in functional oxide semiconductors. Among these dopants, Ga-doped ZnO has demonstrated substantial advantages over Al-doped ZnO, including greater resistant to oxidation. Since the covalent bond length of Ga-O ($1.92\;{\AA}$) is nearly equal to that of Zn-O ($1.97\;{\AA}$), high electron mobility and low electrical resistivity are also expected in the Ga-doped ZnO. In this article, we report the successful growth of Ga-doped ZnO nanorods on c-Sapphire substrate without metal catalysts by magnetrons puttering and our investigations of their structural, optical, and field emission properties.

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Effect of $ZnCl_2$ on Formation of Carbonized Phenol Resin Anode

  • Kim Han-Joo;Hong Ji-sook;Son Won-Ken;Park Soo-Gil;Oyama Noboru
    • 전기화학회지
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    • 제3권2호
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    • pp.85-89
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    • 2000
  • Lithium ion Battery(LIB)의 음극 활물질로써 리튬을 대체하기 위한 노력으로 phenol resin을 탄화시킨 탄소재료를 사용하였다. Phenol resin을 소성하면 축합반응을 일으키면서 탄화되어 무정형 탄소가 된다. 무정형 탄소는 층간거리가 넓어 리튬의 삽입과 탈리가 용이하지만 탄소간의 결합력이 약하여 구조적 붕괴가 일어난다. 이러한 문제를 해결하기 위해 세공형성제로서 $ZnCl_2$를 사용하였다. $ZnCl_2$는 생성된 물질에서 3차원적 망상구조로 성장하는 개방세공을 형성하는 세공형성제로서 뿐만 아니라, 벌크 첨가제가 도핑된 느슨한 구조를 형성하는 미세세공 형성제로서 작용하였다. SEM을 통해서 구조적 차이를 알 수 있었으며, XRD분석으로 층간의 거리를 알 수 있었다. CV측정을 통해 두 가지 샘플에 대한 산화와 환원 반응의 차이를 알아보았다.

수직경사응고(VGF)법에 의한 Si 도핑 GaAs 단결정 성장시 $B_{2}O_{3}$ 첨가에 따른 캐리어 농도 변화 (Control of carrier concentrations by addition of $B_{2}O_{3}$ in Si-doped vertical gradient freeze (VGF) GaAs single crystal growth)

  • 배소익;한창운
    • 한국결정성장학회지
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    • 제19권2호
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    • pp.75-78
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    • 2009
  • PBN 도가니를 이용하여 Si이 도핑된 GaAs 단결정을 수직경사 응고법으로 성장시켰다. PBN 도가니에 산화막인 $B_{2}O_{3}$의 양을 $0{\sim}0.2wt%$ 범위에서 변화시키면서, 성장 후 캐리어 농도를 측정하였다. $B_{2}O_{3}$ 첨가량이 증가함에 따라, 초기 0.1 정도의 Si 도판트의 편석계수는 0.01 부근까지 급격히 감소하고, 동시에 캐리어 농도도 감소하는 것을 알 수 있었다. 이는 성장도중 도판트인 Si이 $B_{2}O_{3}$과 반응하며 도너인 Si 양을 감소시키며, 동시에 억셉터인 B 양을 증가시키기 때문으로 보인다. 한편 PBN 도가니 내면에 얇은 유리질의 $B_{2}O_{3}$층 형성이 용이한 고온 산화막 처리가 결함감소에 효과적임을 확인하였다.

BaZrO3계 수소이온 전도체의 제조 및 첨가물에 따른 전기적 특성 (The Fabrication of BaZrO3-based Proton Conductors and their Electrical Properties by Dopants)

  • 권정범;유광수
    • 한국세라믹학회지
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    • 제40권5호
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    • pp.415-422
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    • 2003
  • BaZr $O_3$를 기본으로 첨가제(Ce, Yb)를 넣어 B자리인 Zr을 부분적으로 치환하였고 Ce의 첨가량을 달리하여 4가지의 조성을 갖는 시편을 제조하였다. 제조된 시편을 임피던스 분석 장치를 이용하여 건조공기 분위기와 수증기 분위기에서 전기적 특성을 측정하였다. $600^{\circ}C$ 이하의 낮은 온도 영역에서, 수증기 분위기에서의 전기전도도가 건조공기 분위기에서의 전기전도도 보다 모든 조성에서 높은 값을 나타냈고 Ce의 첨가량이 증가할수록 높은 전도도 값을 보였다. BaZ $r_{0.8}$C $e_{0.15}$Y $b_{0.05}$ $O_3$$_{-{\delta}}$조성을 갖는 시편이 80$0^{\circ}C$에서 가장 높은 1.72$\times$$10^{-3}$ S$cm^{-1}$ / 전기전도도 값을 나타냈다. 낮은 온도영역에서는 수소이온 전도에 의해 건조공기 분위기 보다 수증기 분위기에서 높은 전지전도도를 나타냈지만 온도가 올라갈수록 수소이온 전도도가 줄어들면서 $700^{\circ}C$ 근처에서는 거의 비슷한 값을 보였다.

ZnO thin films with Cu, Ga and Ag dopants prepared by ZnS oxidation in different ambient

  • Herrera, Roberto Benjamin Cortes;Kryshtab, Tetyana;Andraca Adame, Jose Alberto;Kryvko, Andriy
    • Advances in nano research
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    • 제5권3호
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    • pp.193-201
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    • 2017
  • ZnO, ZnO: Cu, Ga, and ZnO: Cu, Ga, Ag thin films were obtained by oxidization of ZnS and ZnS: Cu, Ga films deposited onto glass substrates by electron-beam evaporation from ZnS and ZnS: Cu, Ga targets and from ZnS: Cu, Ga film additionally doped with Ag by the closed space sublimation technique at atmospheric pressure. The film thickness was about $1{\mu}m$. The oxidation was carried out at $600-650^{\circ}C$ in air or in an atmosphere containing water vapor. Structural characteristics were investigated by X-ray diffraction (XRD) and atomic force microscopy (AFM). Photoluminescence (PL) spectra of the films were measured at 30-300 K using the excitation wavelengths of 337, 405 and 457.9 nm. As-deposited ZnS and ZnS: Cu, Ga films had cubic structure. The oxidation of the doped films in air or in water vapors led to complete ZnO phase transition. XRD and AFM studies showed that the grain sizes of oxidized films at wet annealing were larger than of the films after dry annealing. As-deposited doped and undoped ZnS thin films did not emit PL. Shape and intensity of the PL emission depended on doping and oxidation conditions. Emission intensity of the films annealed in water vapors was higher than of the films annealed in the air. PL of ZnO: Cu, Ga films excited by 337 nm wavelength exhibits UV (380 nm) and green emission (500 nm). PL spectra at 300 and 30 K excited by 457.9 and 405 nm wavelengths consisted of two bands - the green band at 500 nm and the red band at 650 nm. Location and intensities ratio depended on the preparation conditions.

$Ru^{+3}$, $Pt^{+4}$로 표면 처리한 GaSb의 결정 성장과 특성 (Study on the Crystal Growth and Characterization of GaSb treated with $Ru^{+3}$, $Pt^{+4}$)

  • 이재구;오장섭;송복식;정성훈;문동찬;김선태
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 1995년도 추계학술대회 논문집
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    • pp.77-80
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    • 1995
  • GaSb crystals were grown by the vertical Bridgman method. P-type GaSb crystals were grown with Ga:Sb=1:1 at % ratio without dopants and with Te, respectively. Also, GaSb:Te crystals were investigated. Lattice constants were 6.117${\AA}$ for p-type. The carrier concentration, the resistivity, and the carrier mobility measured by the van der Pauw method were p≡8 x $10^{16}$$cm^{-3}$, p≡0.20$\Omega$-cm, ${\mu}$$_{n}$$400\textrm{cm}^2$$V^{-1}$$sec^{-1}$ for p-type, n≡1 x $10^{17}$$cm^{-3}$, p≡0.15 $\Omega$-cm, ${\mu}$$_{n}$$500\textrm{cm}^2$$V^{-1}$$sec^{-1}$ for n-type at 300K. In case of treating with metal ion of $Ru^{+3}$, $Pt^{+1}$, p≡2 x $10^{17}$$cm^{-3}$, p≡0.08$\Omega$-cm, ${\mu}$$_{n}$≡420$\textrm{cm}^2$$V^{-1}$$sec^{-1}$ for p-type, n≡2.5 x $10^{17}$$cm^{-13}$, p≡0.07 $\Omega$-cm, ${\mu}$$_{n}$≡520$\textrm{cm}^2$$V^{-1}$$sec^{-1}$ for n-type were obtained.

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유도용해법으로 제조된 Co1-xNbxSb3의 열전특성 (Thermoelectric Properties of Co1-xNbxSb3 Prepared by Induction Melting)

  • 박종범;유신욱;조경원;장경욱;이정일;어순철;김일호
    • 한국재료학회지
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    • 제15권2호
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    • pp.89-92
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    • 2005
  • The induction melting was employed to prepare Nb-doped $CoSb_3$ skutterudites and their thermoelectric properties were investigated. Single phase $\delta-CoSb_3$ was successfully obtained by induction melting and subsequent annealing at $400^{\circ}C$ for 2 hrs in vacuum. The positive signs of Seebeck coefficients for all the specimens revealed that Nb atoms acted as p-type dopants by substituting Co atoms. Electrical conductivity decreased and then increased with increasing temperature, indicating mixed conduction behavior. Electrical conductivity increased by Nb doping, and it was saturated at high temperature. Maximum value of the thermoelectric power factor was shifted to higher temperature with increasing the amount of Nb doping, mainly originated from the high Seebeck coefficient around mixed conduction temperature and high electrical conductivity.

피롤/퓨란 고분자 복합체 전극의 전기화학적 성질 (Electrochemical Properties of Polypyrrole/Polyfuran Polymer Composite Electrode)

  • 차성극
    • 대한화학회지
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    • 제42권6호
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    • pp.664-671
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    • 1998
  • 유기 전도성 고분자들중 전도성이 뛰어나고 전기화학적으로 중합이 용이하며 안정성이 뛰어난 피로고분자(ppy)는 산화-환원 활성자리에 회합되는 이온종에 따라서 피막의 형태학적 구조가 다양하다. 그러나 공기중에서 쉽게 노화하며 잘 부서지고 물과 친하지 않은 단점이 있다. 이를 개선하기 위하여 이 다공성 ppy 피막에 높은 개시전위를 갖는 퓨란고분자(pfu)를 끼워심기 중합한 Pt/ppy/pfu(x)전극을 제작하여 그 전기화학적 성질들을 순환전압전류법과 전기호학적 임피던스법으로 조사하였다. 이 때 사용된 도판트 이온은 $PF_6^-,\; BF_4^-$, 그리고 $ClO_4^-$이온 이였으며, pfu의 조성은 ppy에 대하여 0∼1.10 범위였는데 그 조성이 0.1∼0.2의 범위에 있을 때 가장 좋은 산화환원 특징을 나타냈다. 또, $PF_6^-$ 이온이 도우핑되었을 때 전하전달 저항은 다른 이온들로 중합된 것에 비하여 40배정도 낮았으며, 이 중층의 용량은 다른 두 종에 비하여 20배정도 큰 값을 보였다. 전하전달은 주파수의 변화에 영향을 받으며 물질전달에 의한 Warburg 임피던스 항이 포함되는 등가회로를 갖는다.

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