• 제목/요약/키워드: ${V_2}{O_5}$-doping

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Differences of Structural and Electronic Properties in $Ba_{1-x}K_xBiO_3$ (x=0, 0.04, and 0.4)

  • 정동운;최은국
    • Bulletin of the Korean Chemical Society
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    • 제20권9호
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    • pp.1045-1048
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    • 1999
  • Electronic structures calculated based upon the extended Huckel tight-binding method for Ba1-xKxBiO3 with x = 0, 0.04, and 0.4 are reported. It is noticed that the commensurate ordering of Bi 3+ and Bi 5+ is responsible for the insulating and semiconducting behavior in BaBiO3 and Ba0.96K0.04BiO4. The band gaps of 3.2 eV and 1.4 eV for the former and the latter compounds, respectively, are consistent with the experimental results. Doping in Bi 6s-block band up to x = 0.4 causes the collapse of the ordering of Bi 3+ and Bi 5+, thereby resulting in the superconductivity in the Ba0.6K0.4BiO3 compound. Strikingly, the character of oxygen contributes to the conducting mechanism than that of the bismuth. This is quite different from the cuprate superconductors in which the character of copper dominates that of oxygen.

Electronic and Electrical Properties of Transparent Conducting Nickel Oxide Thin Films

  • Lee, Kang-Il;Kim, Beom-Sik;Kim, Ju-Hwan;Park, Soo-Jeong;Denny, Yus Rama;Kang, Hee-Jae
    • 한국진공학회:학술대회논문집
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    • 한국진공학회 2012년도 제43회 하계 정기 학술대회 초록집
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    • pp.226-226
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    • 2012
  • The electronic and electrical properties of nickel oxide (NiO) thin films were investigated by reflection electron energy loss spectroscopy (REELS), x-ray photoelectron spectroscopy (XPS), and Hall Effect measurements. REELS spectra revealed that the band gap of the NiO thin film was increased from 3.50 eV to 4.02 eV after annealing the sample at $800^{\circ}C$. Our XPS spectra showed that the amount of Ni2O3 decreased after annealing. The Hall Effect results showed that the doping type of the sample changed from n type to p type after annealing. The resistivity decreased drastically from $4.6{\times}10^3$ to $3.5{\times}10^{-2}$ ${\Omega}{\cdot}cm$. The mobility of NiO thin films was changed form $3.29{\times}10^3$ to $3.09{\times}10^5cm^2/V{\cdot}s$. Our results showed that the annealing temperature plays a crucial role in increasing the carrier concentration and the mobility which leads to lowering resistivity of NiO thin films.

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역스피넬 Fe3O4 박막의 바나듐 도핑에 따르는 자기적 성질 변화 (Effects of Vanadium Doping on Magnetic Properties of Inverse Spinel Fe3O4 Thin Films)

  • 김광주;최승리;박영란;박재윤
    • 한국자기학회지
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    • 제16권1호
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    • pp.18-22
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    • 2006
  • 바나듐(V)도핑이 $Fe_3O_4$의 자기적 성질에 미치는 영향을 조사하기 위하여 졸-겔 방법을 이용하여 $V_xFe_{3-x}O_4$ 박막들을 제작하고, x-ray diffraction(XRD), x-ray photoelectron spectroscopy(XPS), conversion electron Mossbauer spectroscopy(CEMS), vibrating sample magnetometry(VSM) 등을 이용하여 그 구조적, 자기적 특성들을 측정 및 분석하였다. XRD 측정 결과에 따르면 $V_xFe_{3-x}O_4$ x=1.0까지 입방(cubic)구조를 유지하며, 그 격자 상수는 거의 변화하지 않았다. 바나듐의 2p 및 철의 2p 준위들에 대한 XPS 측정 및 분석 결과, 바나듐은 화합물 내에서 주로 +3가의 상태로 존재하며, 성분비 x가 증가함에 따라 +2가 이온의 농도가 증가함이 나타났다. CEMS측정 결과 $V^{3+}$이온들은 사면체 $Fe^{3+}$자리를 주로 치환하며, $Fe^{2+}$이온들은 팔면체 $Fe^{2+}$자리를 치환하는 것으로 나타났다. 박막들에 대한 상온에서의 VSM측정 결과, 바나듐을 작은 양 도핑 할 경우(x=0.14) $V_xFe_{3-x}O_4$의 포화자화량(saturation magnetization)은 $Fe_3O_4$ 비하여 증가함이 나타났으며, 다량 도핑 할 경우$(x\geq0.5) Fe_3O_4$에 비하여 점차적으로 감소함이 나타났다. $V_xFe_{3-x}O_4$의 보자력(coercivity)은 x의 증가에 따라 증가함이 나타났는데, $V^{2+}(d^3)$ 이온의 팔면체 자리 치환에 의한 비등방성의 증가에 기인하는 것으로 해석된다.

Preparation and Properties of Y2O3-Doped ZrO2 Films on Etched Al Foil by Sol-Gel Process

  • Chen, Fei;Park, Sang-Shik
    • 한국재료학회지
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    • 제25권2호
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    • pp.107-112
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    • 2015
  • The oxide films formed on etched aluminum foils play an important role as dielectric layers in aluminum electrolytic capacitors. $Y_2O_3$-doped $ZrO_2$ (YZ) films were coated on the etched aluminum foils by sol-gel dip coating, and the electrical properties of YZ-coated Al foils were characterized. YZ films annealed at $450^{\circ}C$ were crystallized into a cubic phase, and as the $Y_2O_3$ doping content increased, the unit cell of $ZrO_2$ expanded and the grain size decreased. The etch pits of Al foils were filled by YZ sol when it dried at atmospheric pressure after repeating for several times, but this step could essentially be avoided when being dried in a vacuum. YZ-coated foils indicated that the specific capacitance and dissipation factor were $2-2.5{\mu}F/cm^2$ and 2-4 at 1 kHz, respectively, and the leakage current and withstanding voltage of films approximately 200 nm thick were $5{\times}10^{-4}A$ at 21 V and 22 V, respectively. After being anodized at 500 V, the foils exhibited a specific capacitance and dissipation factor of $0.6-0.7{\mu}F/cm^2$ and 0.1-0.2, respectively, at 1 kHz, while the leakage current and withstanding voltage were $2{\times}10^{-4}-3{\times}10^{-5}A$ at 400 V and 420-450 V, respectively. This suggests that YZ film is a promising dielectric that can be used in high voltage Al electrolytic capacitors.

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.

High performance of ZnO thin film transistors using $SiN_x$ and organic PVP gate dielectrics

  • Kim, Young-Woong;Park, In-Sung;Kim, Young-Bae;Choi, Duck-Kyun
    • 한국결정성장학회지
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    • 제17권5호
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    • pp.187-191
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    • 2007
  • The device performance of ZnO-thin film transistors(ZnO-TFTs) with gate dielectrics of $SiO_2,\;SiN_x$ and Polyvinylphenol(PVP) having a bottom gate configuration were investigated. ZnO-TFTs can induce high device performance with low intrinsic carrier concentration of ZnO only by controlling gas flow rates without additional doping or annealing processes. The field effect mobility and on/off ratio of ZnO-TFTs with $SiN_x$ were $20.2cm^2V^{-1}s^{-1}\;and\;5{\times}10^6$ respectively which is higher than those previously reported. The device adoptable values of the mobility of $1.37cm^2V^{-1}s^{-1}$ and the on/off ratio of $6{\times}10^3$ were evaluated from the device with organic PVP dielectric.

충방전 과정중 구조가 안정한 Zr이 도핑된 LiCoO2 분말 (Structural Stability During Charge-Discharge Cycles in Zr-doped LiCoO2 Powders)

  • 김선혜;심광보;안재평;김창삼
    • 한국세라믹학회지
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    • 제45권3호
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    • pp.167-171
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    • 2008
  • Zirconium-doped $Li_{1.1}Co_{1-x}Zr_xO_2(0{\leq}x{\leq}0.05)$ powders as cathode materials for lithium ion batteries were synthesized using an ultrasonic spray pyrolysis method. Cyclic voltammetry and cyclic stability tests were performed, and the changes of microstructure were observed. The solubility limit of zirconium into $Li_{1.1}CoO_2$ was less than 5 mol%, and monoclinic $Li_2ZrO_3$ phase was formed above the limit. The Zr-doping suppressed the grain growth and increased the lattice parameters of the hexagonal $LiCoO_2$ phase. The Zr-dopiong of 1mol% resulted in the best cyclic performance in the range of $3.0{\sim}4.3V$ at 1C rate (140 mA/g); the initial discharge capacity decreased from 158 mAh/g to 60 mAh/g in the undoped powder, while from 154 mAh/g to 135 mAh/g in the Zr-doped powder of 1 mol% after 30 cycles. The excellent cycle stability of Zr-doped powder was due to the low polarization during chargedischarge processes which resulted from the delayed collapse of the crystal structure of the active materials with Zr-doping.

Photoluminescence property of Al,N-codoped p-type ZnO films by dc magnetron sputtering

  • Jin, Hu-Jie;Liu, Yan-Yan;Park, Bok-Kee;Park, Choon-Bae
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 2008년도 하계학술대회 논문집 Vol.9
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    • pp.419-420
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    • 2008
  • In this study, high quality (Al,N)-codoped p-type ZnO thin films were obtained by DC magnetron sputtering. The film on buffer layer grown in 80% $N_2$ ambient shows highest hole concentration of $2.93\times10^{17}cm^{-3}$. The films show hole concentration in the range of $1.5\times10^{15}$ to $2.93\times10^{17}cm^{-3}$, resistivity of 131.2 to 2.864 $\Omega$cm, mobility of 3.99 to 31.6 $cm^2V^{-1}s^{-1}$. The films on Si show easier p-doping in ZnO than those on buffer layer. The film on Si shows the highest quality of optical photoluminescence (PL) characteristics. The donor energy level $(E_d)$ of (Al,N)-codoped ZnO films is about 50 meV and acceptor energy level $(E_a)$ is in the range of 63 to 71 meV. It will help to improve p-type ZnO films.

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졸-겔법으로 성장시킨 바나듐이 도핑된 ${Bi_4}{Ti_3}{O_{12}}$ 박막의 미세구조 및 전기적 특성 (Microstructure and Electrical Properties of Vanadium-doped ${Bi_4}{Ti_3}{O_{12}}$ Thin Films Prepared by Sol-gel Method)

  • 김종국;김상수;최은경;김진흥;송태권;김인성
    • 한국재료학회지
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    • 제11권11호
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    • pp.960-964
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    • 2001
  • $Bi_{3.99}Ti_{2.97}V_{0.03}O_{12}$ (BTV) thin films with 3 mol% vanadium doping were Prepared on $Pt/Ti/SiO_2/Si$ substrate by sol-gel method. X-ray diffraction analysis indicated that single-phase layered perovskite were obtained and preferred orientation was not observed. Under the annealing temperature at $600^{\circ}C$, the surface morphology of the BTV thin films had fine-rounded particles and then changed plate-like at $650^{\circ}C$ and $700^{\circ}C$. The remanent polarization $(2P_r)$ and coercive field $(2E_c)$ of $700^{\circ}C$ annealed BTV thin film were 25 $\mu$C/cm$^2$ and 116 kV/cm, respectively. In addition, BTV thin film showed little polarization fatigue during $10_9$ switching cycles. These improved ferroelectric properties were attributed to the increased rattling space and reduced oxygen vacancies by substitution $Ti^{4+}$ ion (68 pm) with smaller $V^{5+}$ ion (59 pm). The dielectric constant and loss were measured 130 and 0.03 at 10 kHz, respectively.

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The Structural Investigation for the Enhancement of Electrical Conductivity in Ga-doped ZnO Targets

  • 윤상원;서종현;성태연;안재평;권훈;이건배
    • 한국재료학회:학술대회논문집
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    • 한국재료학회 2011년도 춘계학술발표대회
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    • pp.243.2-243.2
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    • 2011
  • ZnO materials with a wide band gap of approximately 3.3 eV has been used in transparent conducting oxides (TCO) due to exhibitinga high optical transmission, but its low conductivity acts as role of a limitation for conducting applications. Recently, Ga or Al-doped ZnO (GZO, AZO) becomes transparent conducting materials because of high optical transmission and excellent conductivity. However, the fundamental mechanism underlying the improvement of electrical conductivity of the GZO is still the subject of debate. In this study, we have fully investigated the reasons of high conductivity through the characterization of plane defects, crystal orientation, doping contents, crystal structure in Zn1-xGaxO (x=0, 3, 5.1, 5.6, 6.6 wt%). We manufactured Zn1-xGaxO by sintering ZnO and Ga2O3 powers, having a theoretical density of 99.9% and homogeneous Ga-dopant distribution in ZnO grains. The GZO containing 5.6 wt% Ga represents the highest electrical conductivity of $7.5{\times}10^{-4}{\Omega}{\cdot}m$. In particular, many twins and superlattices were induced by doping Ga in ZnO, revealed by X-ray diffraction measurements and TEM (transmission electron microscopy) observations. Twins developed in conventional ZnO crystal are generally formed at (110) and (112) planes, but we have observed the twins at (113) plane only, which is the first report in ZnO material. Interestingly, the superlattice structure was not observed at the grains in which twins are developed and the opposite case was true. This structural change in the GZO resulted in the difference of electrical conductivity. Enhancement of the conductivity was closely related to the extent of Ga ordering in the GZO lattice. Maximum conductivity was obtained at the GZO with a superlattice structure formed ideal ordering of Ga atoms.

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