• Title/Summary/Keyword: Vapor growth

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Study on the Coupled Effects of Process Parameters on Silicon Growth Using Chemical Vapor Deposition

  • Ramadan, Zaher;Ko, Dong Kuk;Im, Ik-Tae
    • Journal of the Semiconductor & Display Technology
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    • v.18 no.3
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    • pp.115-121
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    • 2019
  • Response surface methodology (RSM) is used to investigate the complex coupling effects of different operating parameters on silicon growth rate in planetary CVD reactor. Based on the computational fluid dynamics (CFD) model, an accurate RSM model is obtained to predict the growth rate with different parameters, including temperature, pressure, rotation speed of the wafer, and the mole fraction of dichlorosilane (DCS). Analysis of variance is used to estimate the contributions of process parameters and their interactions. Among the four operating parameters that have been studied, the influences of susceptor temperature and the operating pressure were the most significant factors that affect silicon growth rate, followed by the mole fraction of DCS. The influence of wafer rotation is the least. The validation tests show that the results of silicon deposition rate obtained from the regression model are in good agreement with those from CFD model and the maximum deviations is 2.15%.

Investigation of Synthesis Yield and Diameter Distribution of Single-Walled Carbon Nanotubes Grown at Different Positions in a Horizontal CVD Chamber (수평형 CVD 장치에서 기판 위치에 따른 단일벽 탄소나노튜브의 합성 수율 및 직경 분포 고찰)

  • Jo, Sung-Il;Jeong, Goo-Hwan
    • Journal of the Korean institute of surface engineering
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    • v.52 no.6
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    • pp.357-363
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    • 2019
  • We investigated a synthesis yield and diameter distribution of single-walled carbon nanotubes (SWNTs) with respect to the growth position in a horizontal chemical vapor deposition (CVD) chamber. Thin films and line-patterned Fe films (0.1 nm thickness) were prepared onto ST-cut quartz substrates as catalyst to compare the growth behavior. The line-patterned samples showed higher growth density and parallel alignment than those of the thin film catalyst samples. In addition, line density of the aligned SWNTs at central region of the chamber was 7.7 tubes/㎛ and increased to 13.9 tubes/㎛ at rear region of the CVD chamber. We expect that the enhanced amount of thermally decomposed feedstock gas may contribute to the growth yield enhancement at the rear region. In addition, the lamina flow in the chamber also contribute to the perfect alignment of the SWNTs based on the value of gas velocity, Reynold number, and Knudsen coefficient we employed.

Fabrication of High Tc Superconducting Films by CVD Process

  • Lee, Sang-Heon
    • Transactions on Electrical and Electronic Materials
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    • v.5 no.3
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    • pp.120-121
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    • 2004
  • YBaCuO thick films were fabricated by plasma enhanced chemical vapor deposition, and the crystallinity and the superconducting properties were investigated. The growth temperature to obtain the thick films was decreased by around 150$^{\circ}C$ due to plasma enhancement. The zero resistivity temperatures for films grown at 590$^{\circ}C$ and 620$^{\circ}C$ were 55 and 80 K, respectively.

Crystal Structure Ana1ysis of the Diamond Films Grown by MPCVD (MPCVD에 의한 다이아몬드 박막의 결정구조 해석)

  • 원종각;김종성;흥근조;권상직
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 1999.11a
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    • pp.391-394
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    • 1999
  • The diamond thin films are deposited on silicon using MPCVD(Microwave Plasma Chemical Vapor Deposition) method at various deposition microwave power and time. Diamond is deposited with 100 sccm H$_2$ and 2 sccm CH$_4$ by MPCVD. The crystallinity of diamond thin films were increased with increase of microwave power. The growth rate of diamond thin films were increased with increase of time.

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Thin Film Vacuum Process Technology via Chemical Vapor Deposition Methods (화학기상증착법(CVD)을 이용한 진공 박막 공정기술)

  • Hong, Wan-Shick
    • Vacuum Magazine
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    • v.1 no.3
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    • pp.9-13
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    • 2014
  • Vacuum growth of thin films via chemical vapor deposition (CVD) methods has been extensively used in modern semiconductor and flat panel display industries. The CVD processes have a wide range of variation and are categorized according to their working conditions, power sources, precursor materials, and so forth. Basic components and process steps common to all CVD branches are discussed. In addition, characteristics and applications of two major CVD techniques - LPCVD and PECVD - are reviewed briefly.

Controlled Growth of Large-area Mono-, Bi-, and Few-layer Graphene by Chemical Vapor Deposition on Copper Substrate

  • Kim, Yooseok;Lee, Su-il;Jung, Dae Sung;Cha, Myoung-Jun;Kim, Ji Sun;Park, Seung-Ho;Park, Chong-Yun
    • Proceedings of the Korean Vacuum Society Conference
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    • 2014.02a
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    • pp.380.2-380.2
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    • 2014
  • Direct synthesis of graphene using a chemical vapor deposition (CVD) has been considered a facile way to produce large-area and uniform graphene film, which is an accessible method from an application standpoint. Hence, their fundamental understanding is highly required. Unfortunately, the CVD growth mechanism of graphene on Cu remains elusive and controversial. Here, we present the effect of graphene growth parameters on the number of graphene layers were systematically studied and growth mechanism on copper substrate was proposed. Parameters that could affect the thickness of graphene growth include the pressure in the system, gas flow rate, growth pressure, growth temperature, and cooling rate. We hypothesis that the partial pressure of both the carbon sources and hydrogen gas in the growth process, which is set by the total pressure and the mole fraction of the feedstock, could be the factor that controls the thickness of the graphene. The graphene on Cu was grown by the diffusion and precipitation mode not by the surface adsorption mode, because similar results were observed in graphene/Ni system. The carbon-diffused Cu layer was also observed after graphene growth under high CH4 pressure. Our findings may facilitate both the large-area synthesis of well-controlled graphene features and wide range of applications of graphene.

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Growth of Highly Purified Carbon Nanotubes by Thermal Chemical Vapor Deposition (열화학기상증착법에 의한 고순도 탄소나노튜브의 성장)

  • Yu, Jae-Geun;Park, Jeong-Hun;Kim, Dae-Un;Lee, Cheol-Jin;Son, Gwon-Hui;Sin, Dong-Hyeok;Mun, In-Gi
    • The Transactions of the Korean Institute of Electrical Engineers C
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    • v.49 no.12
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    • pp.649-653
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    • 2000
  • We have grown carbon nanotubes by thermal chemical vapor deposition of $C_{2}H_{2}$ on catalytic metal deposited on silicon oxide substrates. Highly purified carbon nanotubes are uniformly grown on a large area of the silicon oxide substrates. It is observed that surface modification of catalytic metals deposited on substrates by either etching with dipping in a HF solution and/or $NH_{3}$ pretreatment is a crucial step for the nanotube growth prior to the reaction of $C_{2}H_{2}$ gas. The diameters of carbon naotubes could be controlled by applying the different catalytic metals.

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The Formation of Microcrystalline SiGe Film Using a Remote Plasma Enhanced Chemical Vapor Deposition (원격 플라즈마 화학기상 증착법으로 성장된 미세 결정화된 SiGe 박막 형성)

  • Kim, Doyoung
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.31 no.5
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    • pp.320-323
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    • 2018
  • SiGe thin films were deposited by remote plasma enhanced chemical vapor deposition (RPE-CVD) at $400^{\circ}C$ using $SiH_4$ or $SiCl_4$ and $GeCl_4$ as the source of Si and Ge, respectively. The growth rate and the degree of crystallinity of the fabricated films were characterized by scanning electron microscopy and Raman analysis, respectively. The optical and electrical properties of SiGe films fabricated using $SiCl_4$ and $SiH_4$ source were comparatively studied. SiGe films deposited using $SiCl_4$ source showed a lower growth rate and higher crystallinity than those deposited using $SiH_4$ source. Ultraviolet and visible spectroscopy measurement showed that the optical band gap of SiGe is in the range of 0.88~1.22 eV.

Interplay between Defect Propagation and Surface Hydrogen in Silicon Nanowire Kinking Superstructures

  • Sin, Nae-Cheol
    • Proceedings of the Korean Vacuum Society Conference
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    • 2015.08a
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    • pp.221.1-221.1
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    • 2015
  • The vapor-liquid-solid (VLS) method, where the "liquid" catalytic droplets collecting atoms from vapor precursors build the solid crystal layers via supersaturation, is a ubiquitous technique to synthesize 1-dimensional nanoscale materials. However, the lack of fundamental understanding of chemical information governing the process inhibits the rational route to the structural programming. By combining the in situ or operando IR spectroscopy with post-growth high resolution electron microscopy, we show the strong correlation between the surface chemical species concentration and nanowire structures. More specifically, the critical role of surface adsorbed hydrogen, generated from the decomposition of Si2H6 precursor on the interplay between nanowire / kinking and the defect propagation is demonstrated. Our results show that adsorbed hydrogen atoms are responsible for selecting -oriented growth and indicate that a twin boundary imparts structural coherence. The twin boundary, only continuous at / kinks, reduces the symmetry of the trijunction and limits the number of degenerate directions available to the nanowire. These findings constitute a general approach for rationally engineering kinking superstructures and also provide important insight into the role of surface chemical bonding during VLS synthesis.

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A time dependent thermal and solutal convection problem in physical vapor transport of Hg2Cl2-I2 system

  • Kim, Geug Tae
    • Journal of the Korean Crystal Growth and Crystal Technology
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    • v.27 no.2
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    • pp.80-88
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    • 2017
  • In this research a time dependent thermal and solutal convection was computationally investigated for the physical vapor transport of the mixture of $Hg_2Cl_2-I_2$ system with for the convective regime from thermal Rayleigh number of $2.16{\times}10^6$ up to $1.7{\times}10^7$ with marching time to a steady state problem. With time marching, the convective cells are decreased for the thermal Rayleigh number of $2.16{\times}10^6$, and increased for the thermal Rayleigh number of $1.7{\times}10^7$. The convective flow structures are found to be essentially time independent on the horizontal orientation of the enclosure with respect to the gravity vector, and on the other hand, time dependent on the vertical orientation of the enclosure with respect to the gravity vector.