• Title/Summary/Keyword: Al films

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Microwave Annealing in Ag/HfO2/Pt Structured ReRAM Device

  • Kim, Jang-Han;Kim, Hong-Ki;Jang, Ki-Hyun;Bae, Tae-Eon;Cho, Won-Ju;Chung, Hong-Bay
    • Proceedings of the Korean Vacuum Society Conference
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    • 2014.02a
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    • pp.373-373
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    • 2014
  • Resistive-change random access memory (ReRAM) device is one of the promising candidates owing to its simple structure, high scalability potential and low power operation. Many resistive switching devices using transition metal oxides materials such as NiO, Al2O3, ZnO, HfO2, $TiO_2$, have attracting increased attention in recent years as the next-generation nonvolatile memory. Among various transition metal oxides materials, HfO2 has been adopted as the gate dielectric in advanced Si devices. For this reason, it is advantageous to develop an HfO2-based ReRAM devices to leverage its compatibility with Si. However, the annealing temperature of these high-k thin films for a suitable resistive memory switching is high, so there are several reports for low temperature process including microwave irradiation. In this paper, we demonstrate the bipolar resistive switching characteristics in the microwave irradiation annealing processed Ag/HfO2/Pt ReRAM device. Compared to the as-deposited Ag/HfO2/Pt device, highly improved uniformity of resistance values and operating voltage were obtained from the micro wave annealing processed HfO2 ReRAM device. In addition, a stable DC endurance (>100 cycles) and a high data retention (>104 sec) were achieved.

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The electronic structure of the ion-beam-mixed Pt-Cu alloys by XPS and XANES

  • Lim, K.Y.;Lee, Y.S.;Chung, Y.D.;Lee, K.M.;Jeon, Y.;Whang, C.N.
    • Proceedings of the Korean Vacuum Society Conference
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    • 1998.02a
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    • pp.133-133
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    • 1998
  • In the thin film alloy formation of the transition metals ion-beam-mixing technique forms a metastable structure which cannot be found in the arc-melted metal alloys. Sppecifically it is well known that the studies about the electronic structure of ion-beam-mixed alloys pprovide the useful information in understanding the metastable structures in the metal alloy. We studied the electronic change in the ion-beam-mixed ppt-Ct alloys by XppS and XANES. These analysis tools pprovide us information about the charge transfer in the valence band of intermetallic bonding. The multi-layered films were depposited on the SiO2 substrate by the sequential electron beam evapporation at a ppressure of less than 5$\times$10-7 Torr. These compprise of 4 ppairs of ppt and Cu layers where thicknesses of each layer were varied in order to change the alloy compposition. Ion-beam-mixing pprocess was carried out with 80 keV Ae+ ions with a dose of $1.5\times$ 1016 Ar+/cm2 at room tempperature. The core and valence level energy shift in these system were investigated by x-ray pphotoelectron sppectroscoppy(XppS) pphotoelectrons were excited by monochromatized Al K a(1486.6 eV) The ppass energy of the hemisppherical analyzer was 23.5 eV. Core-level binding energies were calibrated with the Fermi level edge. ppt L3-edge and Cu K-edge XANES sppectra were measured with the flourescence mode detector at the 3C1 beam line of the ppLS (ppohang light source). By using the change of White line(WL) area of the each metal sites and the core level shift we can obtain the information about the electrons pparticippating in the intermetallic bonding of the ion-beam-mixed alloys.

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Low-k plasma polymerized methyl-cyclohexane thin films deposited by inductively coupled plasma chemical vapor deposition

  • 조현욱;권영춘;양재영;정동근
    • Proceedings of the Korean Vacuum Society Conference
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    • 2000.02a
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    • pp.98-98
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    • 2000
  • 초고집적(ULSI) 반도체 소자의 multilevel metalization을 위한 중간 유저네로서 저 유전상수(k<)와 높은 열적안정성(>45$0^{\circ}C$)을 갖는 새로운 물질을 도입하는 것이 필요하다. 중합체 박막은 낮은 유전상수와 높은 열적 안정성으로 인하여 low-k 물질로 적당하다고 여겨진다. PECVD에 의한 plasma polymer 박막의 증착은 많이 보고되어 왔으마 고밀도 플라즈마 형성이 가능하고 기판으로 유입되는 ion의 energy 조절이 가능한 inductively coupled plasma(ICP) CVD에 의한 plasma polymer 박막에 대한 연구는 보고된 바 없다. 본 연구에서는 Mtehyl-cyclohexane precusor를 사용하여 substrate에 bias를 주면서 inductively coupled plasma(ICP)를 이용하여 플라즈마 폴리머 박막(plasma polymerized methyl-cyclohexane : 이하^g , pp MCH라 칭함)을 증착하였으며 ICP power와 substrate bias(SB) power가 증착된 박막의 특성에 어떠한 영향을 미치는지 알아보았다. 증착된 박막의 유전상 수 및 열적 안정성은 ICP power의 변화에 비해 SB power의 변화에 더 크게 영향을 받았다.^g , pp MCH 박막은 platinum(Pt) 기판과 silicon 기판위에서 같이 증착되었다. Methyl-cyclohexane precursor는 4$0^{\circ}C$로 유지된 bubbler에 담겨지고 carrier 가스 (H2:10%, He:90%)에 의해 reactor 내부로 유입된다.^g , pp MCH 박막은 증착압력 350 mTorr, 증착온도 6$0^{\circ}C$에서 \circled1SB power를 10W에 고정시키고 ICP power를 5W부터 70W까지, \circled2ICP power를 10W에 고정시키고 SB power를 5W부터 70W까지 변화하면서 증착하였다. 유전 상수 및 절연성은 Al/PPMCH//Pt 구조의 capacitor를 만들어서 측정하였으며, 열적 안정성은 Ar 분위기에서 30분간의 열처리 전후의 두께 변화를 측정함으로써 분석하였다. SB power 10W에서 ICP power가 5W에서 70w로 증가함에 따라 유전상수는 2.65에서 3.14로 증가하였다. 열적 안정성은 ICP power의 증가에 따라서는 크게 향상되지 않은 것으로 나타났다. ICP power 10W에서 SB power가 5W에서 70W로 증가함에 따라 유전상수는 2.63에서 3.46으로 증가하였다. 열적 안정성은 SB power의 증가에 따라 현저하게 향상되었으며 30W 이상에서 증착된 박막은 45$0^{\circ}C$까지 안정하였고, 70W에서 증착된 박막은 50$0^{\circ}C$까지 안정하였다. 열적 안정성은 ICP power의 증가에 따라서는 현저하게 향상되었다. 그 원인은 SB power의 인가에 의해 활성화된 precursor 분자들이 큰 에너지를 가지고 기판에 유입되어 치밀한 박막이 형성되었기 때문으로 사료된다.

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The temperature effect on the electrical properties of W /Ta$_2$O$_5$/ Si structures (온도가 W /Ta$_2$O$_5$ 5/ Si 구조의 전기적 특성에 미치는 영향)

  • 장영돈;박인철;김홍배
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 1996.11a
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    • pp.71-74
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    • 1996
  • Ta$_2$O$_{5}$ film ale recognized as promising capacitor dielectric for future DRAM\`s. The electrical properties of Ta$_2$O$_{5}$films greatly depend on the heating condition. In the practical fabrication process, several annealing process, such as the annealing of Al in H$_2$(about 40$0^{\circ}C$) and reflow of BPSG (borophosphosilicate glass) film in $N_2$(about 80$0^{\circ}C$), exist after deposition of Ta$_2$O$_{5}$ film. In this paper, we describe the temperature effect on the electrical properties of W/Ta$_2$O$_{5}$/Si structure. The thin film of Ta$_2$O$_{5}$ and tungsten have been deposited on p-si(100) wafer using the sputtering system. The heating temperature was varied from 500 to 90$0^{\circ}C$ in $N_2$for 30min and The degree of temperature is 100\`C. In a log(J/E$^2$) Vs 1/E plot of typical I-V data, we find a linear relationship for the temperature of 500, $600^{\circ}C$ and as deposition. This could indicate Fowler-Nordheim tunneling as the dominant mode of current transports. However, we can not find a linear relationship for the temperature above $700^{\circ}C$. This could not indicate Fowler-Nordheim tunneling as the dominant mode of current transport. The high frequency (1MHz) capacitance-voltage (C-V) of W/Ta$_2$O$_{5}$/Si Capacitor were investigated on the basis of shift in the threshold voltage and dielectric constant. The magnitude of the threshold voltage and dielectric constant depends on the heating temperature, and increases with heating temperature.temperature.

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A unhomogeneity of critical current at the long length coated conductors (Coated conductor에서 임계전류의 불균일)

  • Lee, Nam-Jin;Oh, Sang-Soo;Kim, Ho-Sup;Ha, Dong-Woo;Ha, Hong-Soo;Ko, Rock-Kil;Kim, Tae-Hyung;Moon, Seung-Hyun;Youm, Do-Jun
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2009.05a
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    • pp.1-2
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    • 2009
  • The high critical current ($I_c$, A) of SmBCO coated conductor in a magnetic field, the high production rate and the high material yield are promising for applications. The inhomogeneity of Ie at the long length coated conduct is very important problem for electric application. So we researched the reason of inhomogeneity of $I_c$ at long length tape prepared by batch type co-evaporation system called by EDDC. The long length SmBCO coated conductors were developed on $LaMnO_3/IBAD-MgO/Y_2O_3/Al_2O_3$/Hastelloy C276 template. The distribution of $I_c$ are from 0 to 397 A/cm at 77 K and self field. We have studied the microstructures of these films by using SEM, EDS and X-ray diffraction. The XRD and composition by EDS results of SmBCO film reveals subtle difference. But, the microscopic observation by SEM show the microcrack at the sample with low $I_c$.

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Fabrication and Thermophysical Properties of Nickel-coated Aluminum Powder by Electroless Plating (비전해 방법을 이용한 니켈 코팅 알루미늄 분말 제조 및 열물성 평가)

  • Lee, Sanghyup;Lim, Jihwan;Noh, Kwanyoung;Yoon, Woongsup
    • Journal of the Korean Society of Propulsion Engineers
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    • v.18 no.4
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    • pp.9-17
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    • 2014
  • In this study, in order to improve the ignitability of high energy aluminum powder, natural oxide films (alumina) were chemically removed, and instead nickel coat was applied. We used an electroless plating for nickel coating and confirmed quantitatively and qualitatively a time-dependent degree of nickel coating through analysis of surface by SEM/EDS. We also conducted element analysis by XRD and thermal properties by TGA/DSC in air oxidizer environment. There results explained the ignition enhancement mechanism of the nickel-coated aluminum powder in air. The difference between coated and un-coated aluminum powder, the effectiveness of coated powder has better ignitability.

Gas Sensing Characteristics of Nano Sized SnO2 Sensors for Various Co and Ni Concentration (Co, Ni 농도 변화에 따른 나노 SnO2 센서의 감응 특성)

  • Lee, Ji-Young;Yu, Yoon-Sic;Yu, Il
    • Korean Journal of Materials Research
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    • v.21 no.10
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    • pp.546-549
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    • 2011
  • Nano-sized $SnO_2$ thick films were prepared by a screen-printing method onto $Al_2O_3$ substrates. The sensing characteristics were investigated by measuring the electrical resistance of each sensor in a test box as a function of the detection gas. The nano-sized $SnO_2$ thick film sensors were treated in a $N_2$ atmosphere. The structural properties of the nano $SnO_2$with a rutile structure according to XRD showed a (110) dominant $SnO_2$ peak. The particle size of $SnO_2$:Ni nano powders at Ni 8 wt% was about 45 nm, and the $SnO_2$ particles were found to contain many pores according to the SEM analysis. The sensitivity of the nano $SnO_2$-based sensors was measured for 5 ppm $CH_4$ gas and $CH_3CH_2CH_3$ gas at room temperature by comparing the resistance in air with that in the target gases. The results showed that the best sensitivity of $SnO_2$:Ni and $SnO_2$:Co sensors for $CH_4$ gas and $CH_3CH_2CH_3$ gas at room temperature was observed in $SnO_2$:Ni sensors doped with 8 wt% Ni. The response time of the $SnO_2$:Ni gas sensors was 10 seconds and recovery time was 15 seconds for the $CH_4$ and $CH_3CH_2CH_3$ gases.

Thickness Measurement of Nanogate Oxide Films by Spectroscopic Ellipsometry (SE를 사용한 나노게이트 산화막의 두께측정)

  • 조현모;조용재;이윤우;이인원;김현종;김상열
    • Proceedings of the Korea Crystallographic Association Conference
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    • 2002.11a
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    • pp.40-41
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    • 2002
  • 차세대 반도체 및 나노소자 산업에 대한 국제적 기술은 고밀도 직접화의 추세에 따라서 .게이트 산화막의 두께가 급속히 작아지는 추세이다. 지금까지 이산화규소(A1₂O₃)가 게이트 산화막으로 주로 사용되어 왔으나 점차 SiON 혹은 high k 박막으로 바뀌고 있다. 본 연구에서는 차세대 반도체 소자에 사용될 게이트 산화막 물질인 SiON 박막과 Al₂O₃박막에 대한 SE(Spectroscopic Ellipsometry)분석 모델을 확립하였고, SE 측정결과를 TEM, MEIS, XRR의 결과들과 비교하였다. SiON 박막의 굴절률 값은 Si₃N₄와 SiO₂가 물리적으로 혼합되어 있다고 가정하여 Bruggeman effective medium approximation을 사용하여 구하였다. 동일한 시료를 절단하여 TEM, MEIS, 그리고 XRR에 의하여 SiON 박막의 두께를 측정하였으며, 그 결과 SE와 XRR에 의해 얻어진 박막두께가 TEM과 MEIS의 결과 값보다 약 0.5 nm 크게 주어짐을 알 수 있었다(Table 1 참조). 본 연구결과는 비파괴적이며 비접촉식 측정방법인 SE가 2~4nm 두께의 초미세 SiON 박막의 두께와 N 농도의 상대적 값을 빠르고 쉽게 구할 수 있는 유용한 측정방법 임을 보여주었다. 기존의 게이트 산화물인 SiO₂를 대체할 후보 물질들 중의 하나인 A1₂O₃의 유전함수를 구하기 위하여 8 inch, p-type 실리콘 기판 위에 성장된 5 nm, 10 nm, 및 20 nm 두께의 A1₂O₃ 박막의 유전함수와 두께를 측정하였다. 이 시료들에 대한 SE data는 vacuum-UV spectroscopic ellipsometer를 사용하여 세 개의 입사각에서 0.75 eV에서 8.75 eV까지 0.05 eV 간격으로 측정되었다. A1₂O₃ 박막의 유전함수와 두께를 얻기 위하여 공기층/A1₂O₃ 박막/Si 기판으로 구성된 3상계 모델을 사용하였다. Si 기판에 대한 복소 유전함수는 문헌상의 값(1)을 사용하였고, A1₂O₃ 박막의 유전함수는 5개의 미지상수를 갖는 Tauc- Lorentz(TL) 분산함수(2)를 사용하였다. A1₂O₃ 박막의 경우 두께가 증가함에 따라서 굴절률이 커짐을 알 수 있었다.

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Classification of Chemical Warfare Agents Using Thick Film Gas Sensor Array (후막 센서 어레이를 이용한 화학 작용제 분류)

  • Kwak Jun-Hyuk;Choi Nak-Jin;Bahn Tae-Hyun;Lim Yeon-Tae;Kim Jae-Chang;Huh Jeung-Soo;Lee Duk-Dong
    • Journal of the Korea Institute of Military Science and Technology
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    • v.7 no.2 s.17
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    • pp.81-87
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    • 2004
  • Semiconductor thick film gas sensors based on tin oxide are fabricated and their gas response characteristics are examined for four simulant gases of chemical warfare agent (CWA)s. The sensing materials are prepared in three different sets. 1) The Pt or Pd $(1,\;2,\;3\;wt.\%)$ as catalyst is impregnated in the base material of $SnO_2$ by impregnation method.2) $Al_2O_3\;(0,\;4,\;12,\;20\;wt.\%),\;In_2O_3\;(1,\;2,\;3\;wt.\%),\;WO_3\;(1,\;2,\;3\;wt.\%),\;TiO_2\;(3,\;5,\;10\;wt.\%)$ or $SiO_2\;(3,\;5,\;10\;wt.\%)$ is added to $SnO_2$ by physical ball milling process. 3) ZnO $(1,\;2,\;3,\;4,\;5\;wt.\%)$ or $ZrO_2\;(1,\;3,\;5\;wt.\%)$ is added to $SnO_2$ by co-precipitation method. Surface morphology, particle size, and specific surface area of fabricated sensing films are performed by the SEM, XRD and BET respectively. Response characteristics are examined for simulant gases with temperature in the range 200 to $400^{\circ}C$, with different gas concentrations. These sensors have high sensitivities more than $50\%$ at 500ppb concentration for test gases and also have shown good repetition tests. Four sensing materials are selected with good sensitivity and stability and are fabricated as a sensor array A sensor array Identities among the four simulant gases through the principal component analysis (PCA). High sensitivity is acquired by using the semiconductor thick film gas sensors and four CWA gases are classified by using a sensor array through PCA.

In-situ Raman Spectroscopic Study of Nickel-base Alloys in Nuclear Power Plants and Its Implications to SCC

  • Kim, Ji Hyun;Bahn, Chi Bum;Hwang, Il Soon
    • Corrosion Science and Technology
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    • v.3 no.5
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    • pp.198-208
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    • 2004
  • Although there has been no general agreement on the mechanism of primary water stress corrosion cracking (PWSCC) as one of major degradation modes of Ni-base alloys in pressurized water reactors (PWR's), common postulation derived from previous studies is that the damage to the alloy substrate can be related to mass transport characteristics and/or repair properties of overlaid oxide film. Recently, it was shown that the oxide film structure and PWSCC initiation time as well as crack growth rate were systematically varied as a function of dissolved hydrogen concentration in high temperature water, supporting the postulation. In order to understand how the oxide film composition can vary with water chemistry, this study was conducted to characterize oxide films on Alloy 600 by an in-situ Raman spectroscopy. Based on both experimental and thermodynamic prediction results, Ni/NiO thermodynamic equilibrium condition was defined as a function of electrochemical potential and temperature. The results agree well with Attanasio et al.'s data by contact electrical resistance measurements. The anomalously high PWSCC growth rate consistently observed in the vicinity of Ni/NiO equilibrium is then attributed to weak thermodynamic stability of NiO. Redox-induced phase transition between Ni metal and NiO may undermine the integrity of NiO and enhance presumably the percolation of oxidizing environment through the oxide film, especially along grain boundaries. The redox-induced grain boundary oxide degradation mechanism has been postulated and will be tested by using the in-situ Raman facility.