• Title/Summary/Keyword: C60 doping

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Effect of GaGe Sputtering Power on Ga Doping in Phase Change Memory Materials (상 변화 메모리 재료 내의 Ga 주입에 미치는 GaGe 스퍼터링 전력의 영향)

  • Jung, Soon-Won;Lee, Seung-Yun
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.28 no.5
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    • pp.285-290
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    • 2015
  • The phase change memory material is an active element in phase change memory and exhibits reversible phase transition behavior by thermal energy input. The doping of the phase change memory material with Ga leads to the increase of its crystallization temperature and the improvement of its amorphous stability. In this study, we investigated the effect of GaGe sputtering power on the formation of the phase change memory material including Ga. The deposition rate linearly increased to a maximum of 127 nm and the surface roughness remained uniform as the GaGe sputtering power increased in the range from 0 to 75 W. The Ga concentration in the thin film material abruptly increased at the critical sputtering power of 60 W. This influence of GaGe sputtering power was confirmed to result from a combined sputtering-evaporation process of Ga occurring due to the low melting point of Ga ($29.77^{\circ}C$).

플라즈마 도핑 후 급속열처리법을 이용한 n+/p 얕은 접합 형성

  • Do, Seung-U;Seo, Yeong-Ho;Lee, Jae-Seong;Lee, Yong-Hyeon
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2009.11a
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    • pp.50-50
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    • 2009
  • In this paper, the plasma doping is performed on p-type wafers using $PH_3$ gas(10 %) diluted with He gas(90 %). The wafer is placed in the plasma generated with 200 W and a negative DC bias (1 kV) is applied to the substrate for 60 sec under no substrate heating. the flow rate of the diluted $PH_3$ gas and the process pressure are 100 sccm and 10 mTorr, respectively. In order to diffuse and activate the dopant, annealing process such as rapid thermal annealing (RTA) is performed. RTA process is performed either in $N_2$, $O_2$ or $O_2+N_2$ ambient at $900{\sim}950^{\circ}C$ for 10 sec. The sheet resistance is measured using four point probe. The shallow n+/p doping profiles are investigated using secondary ion mass spectromtry (SIMS). The analysis of crystalline defect is also done using transmission electron microscopy (TEM) and double crystal X-ray diffraction (DXRD).

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Thermal and Mechanical Properties of a N2 Doped Porous 3C-SiC Thin Film (질소가 도핑된 다공질 3C-SiC 박막의 열적, 기계적 특성)

  • Kim, Kang-San;Chung, Gwiy-Sang
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.23 no.8
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    • pp.651-654
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    • 2010
  • This paper describes the thermal and mechanical properties of doped thin film 3C-SiC and porous 3C-SiC. In this work, the in-situ doped thin film 3C-SiC was deposited by using atmospheric pressure chemical vapor deposition (APCVD) method at $120^{\circ}C$ using single-precursor hexamethyildisilane: $Si_2(CH_3)_6$ (HMDS) as Si and C precursors. 0~40 sccm $N_2$ gas was used as doping source. After growing of doped thin film 3C-SiC, porous structure was achieved by anodization process with 380 nm UV-LED. Anodization time and current density were fixed at 60 sec and 7.1 mA/$cm^2$, respectively. The thermal and mechanical properties of the $N_2$ doped porous 3C-SiC was measured by temperature coefficient of resistance (TCR) and nano-indentation, respectively. In the case of 0 sccm, the variations of TCR of thin film and porous 3C-SiC are similar, but TCR conversely changed with increase of $N_2$ flow rate. Maximum young's modulus and hardness of porous 3C-SiC films were measured to be 276 GPa and 32 Gpa at 0 sccm $N_2$, respectively.

Characteristics of Contact resistivity on RTP annealing temperature and time after Plasma ion implant (플라즈마 이온주입 후 RTP 열처리 온도와 시간에 따른 접촉저항 특성)

  • Choi, Jang-Hun;Do, Seung-Woo;Lee, Yong-Hyun
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2009.06a
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    • pp.5-6
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    • 2009
  • In this paper, plasma ion implant is performed with $PH_3$ gas diluted by helium gas on P-type Si wafer (100). Spike Rapid Thermal Processing(RTP) annealing performed for 30~60 sec from $800\;^{\circ}C$ to $1000\;^{\circ}C$ in $N_2+O_2$ ambient. Crystalline defect is analyzed by Transmission Electron Microscope(TEM) and Double crystal X-ray Diffraction(DXRD). Contact resistivity($\rho c$), contact resistance(Rc) and sheet resistance(Rs) are analyzed by measuring Transfer Length Method(TLM) using 4155C analysis. As annealing temperature increase, Rs decrease and ${\rho}c$ and Rc increase at temperature higher than $850\;^{\circ}C$. We achieve low Rs, ${\rho}c$ and Rc with Plasma ion implant and spike RTP.

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Effect of $Al_2O_3$ Additives on Microwave Dielectric Properties of (Ba,Ca,Mg)-$Nd_2O_3-TiO_2+10wt%Bi_2O_3$ Ceramics ($Al_2O_3$ 첨가가 (Ba,Ca,Mg)-$Nd_2O_3-TiO_2+10wt%Bi_2O_3$ 세라믹의 마이크로파 유전특성에 미치는 영향)

  • 최지원;강종윤;하종윤;윤석진;김현재;정현진;윤기현
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 1999.05a
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    • pp.653-656
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    • 1999
  • Effect of $Al_2O_3$ Additives on Microwave Dielectric Properties of $0.15(Ba_{0.85}Ca_{(0.15-y)}Mg_y)$-0.125 $Nd_2O_3-0.60TiO_2+10wt%Bi_zO_3$ (y=0.05, 0.08) Ceramics was investigated. To control of $\tau\;{f}$ on microwave dielectric properties of $0.15(Ba_{0.85}Ca_{(0.15-y)}Mg_y)$-0.125 $Nd_2O_3-0.60TiO_2+10wt%Bi_zO_3$ ceramics $Al_2O_3$ was doped in the composition range of 0 to 0.15 wt%. As a result, dielectric constant was decreased from 94 to 80 but $Q\cdot{f}_0$ value was increased from 4980 to 5210 GHz and temperature coefficient of resonant frequency can be controlled from +9 to -10$ppm^\circ{C}$ as an increase of$Al_2O_3$ doping concentration. Especially, a new microwave dielectric material having $\varepsilon\;_r=84,\;Q\cdot{f}_0=5120\;GHz\;and\;\tau_f=0\;ppm/^\circ{C}$ was obtained at $Al_2O_3$ doping concentration of 0.08 wt%.

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Fabrication and Evaluation of NMOS Devices (NMOS 소자의 제작 및 평가)

  • 이종덕
    • Journal of the Korean Institute of Telematics and Electronics
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    • v.16 no.4
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    • pp.36-46
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    • 1979
  • Using N_ Ch silicon gate technology . the capacitors and transistors with various dimenssion were fabricated. Although the applied process was somewhat standard the conditions of ion implantation for the gate were varied by changing the implant energies from 30keV to 60keV for B and from 100 keV to 175keV for P . The doses of the implant also changed from 3 $\times$ 10 /$\textrm{cm}^2$ to 5 $\times$ 10 /$\textrm{cm}^2$ for B and from 4$\times$ 10 /$\textrm{cm}^2$ to 7 $\times$ 10 /$\textrm{cm}^2$ for P . The D. C. parameters such as threshold voltage. substrate doping level, the degree of inversion, capacitance. flat band voltage, depletion layer width, gate oxide thickless, surface states, motile charge density, electron mobility. leakage current were evaluated and also compared with the corresponing theoretical values and / or good numbers for application. The threshold voltages measured using curve tracer and C-V plot gave good agreements with the values calculated from SUPREM II which has been developed by Stanford University process group. The threshold vol tapes with back gate bias were used to calculate the change of the substrate doping level. The measured subthreshold slope enabled the prediction of the degree of inversion The D. C. testing results suggest the realized capacitors and transistors are suited for the memory applications.

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Effect of Electric Field Frequency on the AC Electrical Treeing Phenomena in an Epoxy/Reactive Diluent/Layered Silicate Nanocomposite

  • Park, Jae-Jun
    • Transactions on Electrical and Electronic Materials
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    • v.15 no.2
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    • pp.87-90
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    • 2014
  • The effects of electric field frequency on the ac electrical treeing phenomena in an epoxy/reactive diluent/layered silicate (1.5 wt%) were carried out, in needle-plate electrode arrangement. A layered silicate was exfoliated in an epoxy base resin, by using our ac electric field apparatus. To measure the treeing propagation rate, constant alternating current (AC) of 10 kV with three different electric field frequencies (60, 500 and 1,000 Hz) was applied to the specimen, in needle-plate electrode arrangement, at $30^{\circ}C$ of insulating oil bath. As the electric field frequency increased, the treeing propagation rate increased. At 500 Hz, the treeing propagation rate of the epoxy/PG/nanosilicate system was $0.41{\times}10^{-3}$ mm/min, which was 3.4 times slower than that of the epoxy/PG system. The electrical treeing morphology was dense bush type at 60 Hz; however, as the frequency increased, the bush type was changed to branch type, having few branches, with very slow propagation rate.

Spray 방법을 이용한 결정질 태양전지 Emitter 확산의 최적화 연구

  • Song, Gyu-Wan;Jang, Ju-Yeon;Lee, Jun-Sin
    • Proceedings of the Korean Vacuum Society Conference
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    • 2011.08a
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    • pp.406-406
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    • 2011
  • 결정질 태양전지에서 도핑(Doping)은 반도체(Semiconductor)의 PN 접합(Junction)을 형성하는 중요한 역할을 한다. 도핑은 반도체에 불순물(Dopant)을 주입하는 공정으로 고온에서 진행되며 온도는 중요한 변수(Parameter)로 작용한다. 본 연구에서는 여러 가지 에미터(emitter)층 형성방법 중에 가장 저가이면서 공정과정이 간단하며 대면적 도핑이 용의한 Spray 방법을 통해 효과적인 에미터 층 형성의 최적화를 위해 DI water에 각각 1%, 3%, 5% 7%로 희석된 H3PO4용액 으로 850$^{\circ}C$에서 열처리 시간을 가변해 가며 최적화된 면저항과 표면농도 특성을 분석하였다. 도핑소스가 웨이퍼(wafer) 각각의 표면에 흡착시킨 후 오븐에 넣어 150$^{\circ}C$에서 5분간 건조시킨 후 퍼니스(furance)에 넣어 시간을 가변해 가며 도핑시켰다. Spray 방식은 기존의 방식보다 저렴하고 In-line 공정에 적합하며 대용량으로 전환이 쉽다는 많은 장점을 가지고 있다. 도핑시 먼저 spray를 이용하여 웨이퍼 표면에 균일하게 용액을 흡착시킨 후 오븐에서 150$^{\circ}C$에서 5분간 건조 후 furnace에 넣어 850$^{\circ}C$에서 시간을 가변 해가며 실험하였다. H3PO4용액의 비율이 1%일 때는 2분 이상 열처리를 하였을 때 60${\Omega}/{\Box}$ 이하로 내려가지 않았다. 이는 최초 표면농도가 낮아 더 이상 확산되지 않음을 의미한다. 또한 H3PO4의 비율이 3% 이상일 때는 열처리 시간이 1분 이하일 때 면저항의 변화가 거의 없었으나 2분 이상일 때는 시간에 따라서 점차 낮아졌으며 균일도 역시 좋아졌다. 이는 H3PO4의 비율이 3% 이상일 때는 표면농도가 높아서 1분 이하의 열처리 시간에서는 확산해 들어가는 양이 거의 같음을 알 수 있었다.

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A study on the n-CdS/p-InP solar cells (n-CdS/p-InP 태양전지에 관한 연구)

  • 송복식;최영복;한성준;문동찬;김선태
    • Electrical & Electronic Materials
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    • v.8 no.4
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    • pp.406-412
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    • 1995
  • A n-CdS thin films were evaporated by thermal evaporation method and their structure, optical transmission spectra and electrical characteristics were investigated. The photovoltaic characteristics of solar cells which were fabricated in optimum conditions measured. The evaporated CdS thin films showed in hexagonal structure and above 80% of optical transmission spectra regardless of impurity doping. The high quality thin films could be obtained at 150.deg. C temperature of substrate, which is useful for solar cell window layer with low resistivity of 6*10$\^$-2/(.ohm.-cm) by In doping We measured the electrical and optical characteristics of the n-CdS/p-InP heterojunction solar cells. The most efficient photovoltaic characteristics of heterojunction solar cells had the open circuit voltage of 0.66V, short circuit current density of 13.85mA/cm$\^$2/, fill factor of 0.576 and conversion efficiency of 8.78% under 60mW/cm$\^$2/ illumination.

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A Study on the Characteristics of Ammonia Doped Plasma Polymer Thin Film with a Controlled Plasma Power

  • Seo, Hyeon-Jin;Hwang, Gi-Hwan;Ju, Dong-U;Yu, Jeong-Hun;Lee, Jin-Su;Jeon, So-Hyeon;Nam, Sang-Hun;Yun, Sang-Ho;Bu, Jin-Hyo
    • Proceedings of the Korean Vacuum Society Conference
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    • 2014.02a
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    • pp.242.2-242.2
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    • 2014
  • Plasma-polymer thin films (PPTF) have been deposited on a Si(100) wafer and glass under several conditions such as different RF power by using plasma-enhanced chemical vapor deposition (PECVD) system. Ethylcyclohexane, ammonia gas, hydrogen and argon were utilized as organic precursor, doping gas, bubbler gas and carrier gases, respectively. PPTFs were grown up with RF (ratio frequency using 13.56 MHz) powers in the range of 20~60 watt. PPTFs were characterized by FT-IR (Fourier Transform Infrared), FE-SEM (Scanning Electron Microscope), AFM (Atomic Force Microscope), Contact angle and Probe station. The result of FT-IR measurement showed that the PPTFs have high cross-link density nitrogen doping ratio was also changed with a RF power increasing. AFM and FE-SEM also showed that the PPTFs have smooth surface and thickness. Impedance analyzer was utilized for the measurements of C-V curves having different dielectric constant as RF power.

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