• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2009년도 하계학술대회 논문집
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• pp.199-200
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• 2009

This paper describes the electrical properties of polycrystalline (poly) 3C-SiC thin films with different nitrogen doping concentrations. The in-situ-doped poly 3C-SiC thin films were deposited by using atmospheric-pressure chemical vapor deposition (APCVD) at $1200^{\circ}C$ with hexamethyldisilane (HMDS: $Si_2$ $(CH_3)_6)$ as a single precursor and 0 ~ 100 sccm of $N_2$ as the dopant source gas. The peaks of the SiC (111) and the Si-C bonding were observed for the poly 3C-SiC thin films grown on $SiO_2/Si$ substrates by using X-ray diffraction (XRD) and Fourier transform infrared spectroscopy (FT-IR) analyses, respectively. The resistivity of the poly 3C-SiC thin films decreased from $8.35\;{\Omega}{\cdot}cm$ for $N_2$ of 0 sccm to $0.014\;{\Omega}{\cdot}cm$ with $N_2$ of 100 sccm. The carrier concentration of the poly 3C-SiC films increased with doping from $3.0819\;{\times}\;10^{17}$ to $2.2994\;{\times}\;10^{19}\;cm^{-3}$, and their electronic mobilities increased from 2.433 to $29.299\;cm^2/V{\cdot}S$.

• 센서학회지
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• 제17권5호
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• pp.325-328
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• 2008

This paper describes the electrical properties of poly (polycrystalline) 3C-SiC thin films with different nitrogen doping concentrations. In-situ doped poly 3C-SiC thin films were deposited by APCVD at $1200^{\circ}C$ using HMDS (hexamethyildisilane: $Si_2(CH_3)_6)$) as Si and C precursor, and $0{\sim}100$ sccm $N_2$ as the dopant source gas. The peak of SiC is appeared in poly 3C-SiC thin films grown on $SiO_2/Si$ substrates in XRD(X-ray diffraction) and FT-IR(Fourier transform infrared spectroscopy) analyses. The resistivity of poly 3C-SiC thin films decreased from $8.35{\Omega}{\cdot}cm$ with $N_2$ of 0 sccm to $0.014{\Omega}{\cdot}cm$ with 100 sccm. The carrier concentration of poly 3C-SiC films increased with doping from $3.0819{\times}10^{17}$ to $2.2994{\times}10^{19}cm^{-3}$ and their electronic mobilities increased from 2.433 to $29.299cm^2/V{\cdot}S$, respectively.

• 한국재료학회지
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• 제9권11호
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• pp.1129-1136
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• 1999

TEMAT precursor를 사용하여 다양한 증착 조건으로 ICP-CVD 방법으로 Si(100) 기판 위에 TiN 박막을 형성하였다. 형성된 TiN 박막의 결정상, 미세구조, 그리고 전기적 특성은 XRD, XPS, HRTEM, 그리고 전기적 측정으로 특성을 조사하였다. BI 구조를 갖는 다결정 TiN 박막은 기판의 온도가 $200^{\circ}C$ 이상의 온도에서 형성되었다. TiN(111) 박막은 기판의 온도가 $300^{\circ}C$에서 TEMAT, $\textrm{N}_{2}$, 그리고 Ar 가스의 유량이 10, 5, 그리고 5sccm으로 반응로에 주입할 때 형성되었다. TiN/Si(100) 계면은 TiN과 $\textrm{SiO}_2$사이에 계면반응이 없었으며 평탄하였다. 기판의 온도가 $500^{\circ}C$에서 형성된 TiN 박막의 비저항, carrier 농도와 이동도는 21 $\mu\Omega$cm, 9.5$\times\textrm{10}^{18}\textrm{cm}^{-3}$와 $462.6\textrm{cm}^{2}$/Vs으로 주어졌다.

• 대한전자공학회:학술대회논문집
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• 대한전자공학회 1998년도 추계종합학술대회 논문집
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• pp.581-584
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• 1998

TiN thin films were grown on (100) Si substrate by atomic layer epitaxy at 130 - $240^{\circ}C$ using TEMAT and NH3 as precursors. Reactants were injected into the reactor in sequence of TEMAT precursor vapor pulse, N2 purging gas pulse, NH3 gas pulse and N2 purging gas pulse so that gas-phase reactions could be removed. The films were characterized by means of x-ray diffraction(XRD), 4-point probe, atomic force microscopy(AFM) and auger electron spectroscopy(AES).

• 한국진공학회:학술대회논문집
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• 한국진공학회 2013년도 제44회 동계 정기학술대회 초록집
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• pp.350-350
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• 2013

Sol-gel법을 이용하여 p-Si 기판위에 yttrium이 도핑된 ZnO (YZO)를 성장하였다. ZnO의 precursor로는 zinc acetate dihydrate를, yttrium의 source로는 yttrium acetate hydrate를 사용하였으며, 용매와 안정제로는 각각 2-methoxy ethanol과 monoethanolamine (MEA)를 사용하였다. yttrium의 doping 농도에 따른 영향을 알아보기 위하여 1~4 at.%로 제작된 YZO sol을 각각 p-type Si 기판에 성장하였으며, 이 후 furnace를 이용하여 500oC에서 1시간 동안 열처리하였다. 성장된 YZO 박막의 표면과 두께를 SEM을 통하여 확인하였으며, XRD를 통한 구조적인 특성을 분석한 결과 모든 박막에서 뚜렷한 c-축 배양성을 갖는 ZnO (0002)피크를 확인하였다. Hall effect를 통하여 YZO는 모두 n-type 특성을 나타낸다는 것을 확인하였으며, 광학적인 특성은 PL을 통해서 분석하였다. n-YZO/p-Si 이종접합의 전류-전압 특성을 분석한 결과 뚜렷한 정류특성을 나타내었다.

• 한국재료학회지
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• 제9권6호
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• pp.599-603
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• 1999

AIN과 저온 GaN 완충충율 이용하여 Si 기판 위의 후막 GaN의 성장특성을 조샤하였다. Si과 GaN의 격자부정합도와 열팽창계수의 차이를 줄이기 위해 AIN과 저온 GaN를 완충충으로 사용하였다. AIN은 RF sputter를 이용하여 중착온도와 증착시간 및 RF power에 따른 표면 거칠기를 AFM으로 조사하여 최척조건을 확립하여 사용하였다. 또한 저온에서 GaN를 성장시켜 이를 완충충으로 이용하여 후막 GaN의 성장시 미치는 영향을 살펴보았다. 성장온도와 V/III 비율이 후막 성장시 표면특성과 결정성 및 성장속도에 미치는 영향을 조사하였다. 후막 GaN의 표연특성 및 막의 두께는 SEM과 $\alpha-step$을 이용하여 측정하였으며 결정성은 X-ray Diffractometer를 이용하여 조사하였다.

• 한국재료학회지
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• 제22권4호
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• pp.202-206
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• 2012

$CoSi_2$ was formed through annealing of atomic layer deposition Co thin films. Co ALD was carried out using bis(N,N'-diisopropylacetamidinato) cobalt ($Co(iPr-AMD)_2$) as a precursor and $NH_3$ as a reactant; this reaction produced a highly conformal Co film with low resistivity ($50\;{\mu}{\Omega}cm$). To prevent oxygen contamination, $ex-situ$ sputtered Ti and $in-situ$ ALD Ru were used as capping layers, and the silicide formation prepared by rapid thermal annealing (RTA) was used for comparison. Ru ALD was carried out with (Dimethylcyclopendienyl)(Ethylcyclopentadienyl) Ruthenium ((DMPD)(EtCp)Ru) and $O_2$ as a precursor and reactant, respectively; the resulting material has good conformality of as much as 90% in structure of high aspect ratio. X-ray diffraction showed that $CoSi_2$ was in a poly-crystalline state and formed at over $800^{\circ}C$ of annealing temperature for both cases. To investigate the as-deposited and annealed sample with each capping layer, high resolution scanning transmission electron microscopy (STEM) was employed with electron energy loss spectroscopy (EELS). After annealing, in the case of the Ti capping layer, $CoSi_2$ about 40 nm thick was formed while the $SiO_x$ interlayer, which is the native oxide, became thinner due to oxygen scavenging property of Ti. Although Si diffusion toward the outside occurred in the Ru capping layer case, and the Ru layer was not as good as the sputtered Ti layer, in terms of the lack of scavenging oxygen, the Ru layer prepared by the ALD process, with high conformality, acted as a capping layer, resulting in the prevention of oxidation and the formation of $CoSi_2$.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2008년도 추계학술대회 논문집 Vol.21
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• pp.137-137
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• 2008

In-situ doped polycrystalline 3C-SiC thin films were deposited by APCVD at $1200^{\circ}C$ using HMDS(hexamethyildisilane: $Si_2(CH_3)_6)$) as Si and C precursor, and 0 ~ 100 sccm $N_2$ as the dopant source gas. The peak of SiC is appeared in polycrystalline 3C-SiC thin films grown on $SiO_2$/Si substrates in XRD(X-ray diffraction) and FT-IR(Fourier transform infrared spectroscopy) analyses. The resistivity of polycrystalline 3C-SiC thin films decreased from 8.35 $\Omega{\cdot}cm$ with $N_2$ of 0 sccm to 0.014 $\Omega{\cdot}cm$ with 100 sccm. The carrier concentration of poly 3C-SiC films increased with doping from $3.0819\times10^{17}$ to $2.2994\times10^{19}cm^{-3}$ and their electronic mobilities increased from 2.433 to 29.299 $cm^2/V{\cdot}S$, respectively.

• 연구논문집
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• 통권34호
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• pp.131-138
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• 2004

Porous silicon nitride ceramics were prepared by Self-propagating High Temperature Synthesis from silicon powder, silicon nitride powder and the pore-forming precursor. The microstructure, porosity and the flexural strength of the porous silicon nitride ceramics were varied according to the Si/$Si_3N_4$ ratio, size and amount of the pore-forming precursors. Some samples exhibited as high flexural strength as $162\pm24$ MPa. The high strength is considered to result from the fine pore size and the strong bonding among the silicon nitrid particles.

• 한국전기전자재료학회논문지
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• 제23권8호
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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.