• 제목/요약/키워드: Ultra-shallow junction

검색결과 37건 처리시간 0.028초

레이저 유도 원자층 도핑(Ll-ALD)법으로 성장시킨 SiGe 소스/드레인 얕은 접합 형성 (Ultra-shallow Junction with Elevated SiCe Source/ Drain fabricated by Laser Induced Atomic Layer Doping)

  • 장원수;정은식;배지철;이용재
    • 대한전자공학회:학술대회논문집
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    • 대한전자공학회 2002년도 하계종합학술대회 논문집(2)
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    • pp.29-32
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    • 2002
  • This paper describes a novel structure of NMOSFET with elevated SiGe source/drain region and ultra-shallow source/drain extension(SDE)region. A new ultra-shallow junction formation technology. Which is based on damage-free process for rcplacing of low energy ion implantation, is realized using ultra-high vacuum chemical vapor deposition(UHVCVD) and excimer laser annealing(ELA).

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엑시머 레이져를 이용한 극히 얕은 접합과 소스, 드레인의 형성과 50nm 이하의 극미세 n-MOSFET의 제작 (Ultra Shallow Junction wish Source/Drain Fabricated by Excimer Laser Annealing and realized sub-50nm n-MOSFET)

  • 정은식;배지철;이용재
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 2001년도 하계학술대회 논문집
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    • pp.562-565
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    • 2001
  • In this paper, novel device structures in order to realize ultra fast and ultra small silicon devices are investigated using ultra-high vacuum chemical vapor deposition(UHVCVD) and Excimer Laser Annealing (ELA). Based on these fundamental technologies for the deep sub-micron device, high speed and low power devices can be fabricated. These junction formation technologies based on damage-free process for replacing of low energy ion implantation involve solid phase diffusion and vapor phase diffusion. As a result, ultra shallow junction depths by ELA are analyzed to 10~20nm for arsenic dosage(2${\times}$10$\_$14//$\textrm{cm}^2$), exciter laser source(λ=248nm) is KrF, and sheet resistances are measured to 1k$\Omega$/$\square$ at junction depth of 15nm and realized sub-50nm n-MOSFET.

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레이져 어닐링을 이용한 낮은 면저항의 극히 얕은 접합 형성 (Ultra shallow function Formation of Low Sheet Resistance Using by Laser Annealing)

  • 정은식;배지철;이용재
    • 한국정보통신학회:학술대회논문집
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    • 한국해양정보통신학회 2001년도 춘계종합학술대회
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    • pp.349-352
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    • 2001
  • 본 논문은 기가 SRAM급 이상의 초고집적을- 위한 0.1$\mu\textrm{m}$의 설계치수를 갖는 MOSFET의 게이트 영역에서 활성 부분의 면저항을 감소시키기 위해 n영역으로 비소를 이온 주입하였다. 어닐링은 급속 열처리 공정 방법과 엑시머 레이져 어닐링 방법을 이용하였으며, 극히 얕은 접합의 형성이 가능하였다. 얕은 접합 형성 깊이는 10~20nm이며, 비소의 주입량은 2$\times$$10^{14}$ $\textrm{cm}^2$이고, 레이져는 엑시머이며 소스는 KrF로 파장은 248mm로 어닐링 하였다. 극히 얕은 P/N$^{+}$ 접합 깊이가 15nm이며, 이때 1k$\Omega$/$\square$의 낮은 면저항 특성을 갖는 결과가 나타났다.

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Co/Ti 이중막 실리사이드 접촉을 갖는 p$^{+}$-n 극저접합의 형성 (Formation of p$^{+}$-n ultra shallow junction with Co/Ti bilayer silicide contact)

  • 장지근;엄우용;신철상;장호정
    • 전자공학회논문지D
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    • 제35D권5호
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    • pp.87-92
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    • 1998
  • Ultr shallow p$^{+}$-n junction with Co/Ti bilayer silicidde contact was formed by ion implantation of BF$_{2}$ [energy : (30, 50)keV, dose:($5{\times}10^{14}$, $5{\times}10^{15}$/$\textrm{cm}^2$] onto the n-well Si(100) region and by RTA-silicidation and post annealing of the evaporated Co(120.angs., 170.angs.)/Ti(40~50.angs.) double layer. The sheet resistance of the silicided p$^{+}$ region of the p$^{+}$-n junction formed by BF2 implantation with energy of 30keV and dose of $5{\times}10^{15}$/$\textrm{cm}^2$ and Co/Ti thickness of $120{\AA}$/(40~$50{\AA}$) was about $8{\Omega}$/${\box}$. The junction depth including silicide thickness of about $500{\AA}$ was 0.14${\mu}$. The fabricated p$^{+}$ -n ultra shallow junction depth including silicide thickness of about $500{\AA}$ was 0.14${\mu}$. The fabricated p$^{+}$-n ultra shallow junction with Co/Ti bilayer silicide contact did not show any agglomeration or variation of sheet resistance value after post annealing at $850^{\circ}C$ for 30 minutes. The boron concentration at the epitaxial CoSi$_{2}$/Si interface of the fabricated junction was about 6*10$6{\times}10^{19}$ / $\textrm{cm}^2$./TEX>.

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Ulra shallow Junctions을 위한 플라즈마 이온주입 공정 연구 (The study of plasma source ion implantation process for ultra shallow junctions)

  • 이상욱;정진열;박찬석;황인욱;김정희;지종열;최준영;이영종;한승희;김기만;이원준;나사균
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 2007년도 하계학술대회 논문집 Vol.8
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    • pp.111-111
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    • 2007
  • Further scaling the semiconductor devices down to low dozens of nanometer needs the extremely shallow depth in junction and the intentional counter-doping in the silicon gate. Conventional ion beam ion implantation has some disadvantages and limitations for the future applications. In order to solve them, therefore, plasma source ion implantation technique has been considered as a promising new method for the high throughputs at low energy and the fabrication of the ultra-shallow junctions. In this paper, we study about the effects of DC bias and base pressure as a process parameter. The diluted mixture gas (5% $PH_3/H_2$) was used as a precursor source and chamber is used for vacuum pressure conditions. After ion doping into the Si wafer(100), the samples were annealed via rapid thermal annealing, of which annealed temperature ranges above the $950^{\circ}C$. The junction depth, calculated at dose level of $1{\times}10^{18}/cm^3$, was measured by secondary ion mass spectroscopy(SIMS) and sheet resistance by contact and non-contact mode. Surface morphology of samples was analyzed by scanning electron microscopy. As a result, we could accomplish the process conditions better than in advance.

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초 저 에너지 이온주입으로 고 조사량 B 이온 주입된 실리콘의 Deactivation 현상 (Deactivation Kinetics in Heavily Boron Doped Silicon Using Ultra Low Energy Ion Implantation)

  • 유승한;노재상
    • 한국재료학회지
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    • 제13권6호
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    • pp.398-403
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    • 2003
  • Shallow $p^{+}$ n junction was formed using a ULE(ultra low energy) implanter. Deactivation phenomena were investigated for the shallow source/drain junction based on measurements of post-annealing time and temperature following the rapid thermal annealing(RTA) treatments. We found that deactivation kinetics has two regimes such that the amount of deactivation increases exponentially with annealing temperature up to $850^{\circ}C$ and that it decreases linearly with the annealing temperature beyond that temperature. We believe that the first regime is kinetically limited while the second one is thermodynamically limited. We also observed "transient enhanced deactivation", an anomalous increase in sheet resistance during the early stage of annealing at temperatures higher than X$/^{\circ}C$. Activation energy for transient enhanced deactivation was measured to be 1.75-1.87 eV range, while that for normal deactivation was found to be between 3.49-3.69 eV.

$CoSi_{2}$ 에피박막을 확산원으로 이용하여 형성한 매우 얇은 접합의 전기적 특성 (Electrical properties of Ultra-Shallow Junction formed by using Epitaxial $CoSi_{2}$ Thin Film as Diffusion Source)

  • 구본철;심현상;정연실;배규식
    • 한국재료학회지
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    • 제8권5호
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    • pp.470-473
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    • 1998
  • Co/Ti 이중막을 급속열처리하여 형성한 $CoSi_{2}$$As^+$을 이온주입한 후, 500~$1000^{\circ}C$에서 drive-in 열처리하여 매우얇은 $n_{+}$ p접합의 다이오드를 제작하고 I-V 특성을 측정하였다. $500^{\circ}C$에서 280초 drive-in 열처리하였을 때, 50nm정도의 매우 얇은접합이 형성되었고, 누설전류가 매우 낮아 가장 우수한 다이오드 특성을 나타내었다. 특히, Co 단일막을 사용한 다이오드에 비해 누설전류는 2order 이상 낮았으며, 이는 $CoSi_{2}$Si의 계면이 균일하였기 때문이다.

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이온 주입 공정시 발생한 실리콘 내 결함의 제어를 통한 $p^+-n$ 초 저접합 형성 방법 (Formation of ultra-shallow $p^+-n$ junction through the control of ion implantation-induced defects in silicon substrate)

  • 이길호;김종철
    • 한국진공학회지
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    • 제6권4호
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    • pp.326-336
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    • 1997
  • 트랜지스터의 소오스/드레인 접합 특성에 가장 큰 영향을 미치는 인자는 이온 주입 시 발생한 실리콘 내에 발생한 결합이라는 사실에 착안하여, 기존 소오스/드레인 접합 형성 공정과 다른 새로운 방식을 도입하여 이온 주입에 의해 생긴 결함의 제어를 통해 고품질 초 저접합 $p^+$-n접합을 형성하였다. 기존의 $p^+$소오스/드레인 접합 형성 공정은 $^{49}BF_2^+$ 이온 주입 후 층간 절연막들인 TEOS(Tetra-Ethyl-Ortho-Silicate)막과 BPSG(Boro-Phospho-Silicate-Glass)막을 증착 후 BPSG막 평탄화를 위한 furnace annealing 공정으로 진행된다. 본 연구에서는 이러한 기존 공정과는 달리 층간 절연막 증착 전 저온 RTA첨가 방법, $^{49}BF_2^+$$^{11}B^+$ 을 혼합하여 이온 주입하는 방법, 그리고 이온 주입 후 잔류 산화막을 제거하고 MTO(Medium temperature CVD oxide)를 증착하는 방법을 제시하 였으며, 각각의 방법은 모두 이온 주입에 의한 실리콘 내 결합 농도를 줄여 기존의 방법보 다 더 우수한 양질의 초 저접합을 형성할 수 있었다.

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향상된 MDRANGE을 사용한 초미세 접합 형성에 관한 연구 (A Study on Ultra-Shallow Junction Formation using Upgraded MDRANGE)

  • 강정원;강유석
    • 대한전자공학회:학술대회논문집
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    • 대한전자공학회 1998년도 추계종합학술대회 논문집
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    • pp.585-588
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    • 1998
  • We investigated the ultra-low energy B, P, and As ion implantation using ungraded MDRANGE code to form nanometer junction depths. Even at the ultra-low energies that were simulated in paper, it was found that channeling cases must be carefully considered. In the cases of B, channeling occurred above 500 eV, in the cases of P, channeling occurred above 1 keV, and in the cases of As, channeling occurred above 2 keV. Comparing 2D dopant profiles of 1 keV B, 2 keV P, and 5 keV As with tilts, we demonstrated that most channeling cases occurred not lateral directions but depth directions. Through thus results, even below 5 keV energy ion implant considered here, it is estimated that channeling effects are important in the formation of nanometer junction depths.

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