• Applied Science and Convergence Technology
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• v.27 no.5
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• pp.95-99
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• 2018

We discuss the structural and optical characteristics of GaN nanowires (NWs) grown on Si(111) substrates by a plasma-assisted molecular-beam epitaxy. The GaN NWs with high crystal quality were formed by adopting a new growth approach, so called Ga pre-deposition (GaPD) method. In the GaPD, only Ga was supplied without nitrogen flux on a SiN/Si surface, resulting in the formation of Ga droplets. The Ga droplets were used as initial nucleation sites for the growth of GaN NWs. The GaN NWs with the average heights of 60.10 to 214.62 nm obtained by increasing growth time. The hexagonal-shaped top surfaces and facets were observed from the field-emission electron microscope images of GaN NWs, indicating that the NWs have the wurtzite (WZ) crystal structure. Strong peaks of GaN (0002) corresponding to WZ structures were also observed from double crystal x-ray diffraction rocking curves of the NW samples. At room temperature, free-exciton emissions were observed from GaN NWs with narrow linewidth broadenings, indicating to the formation of high-quality NWs.

• Korean Journal of Materials Research
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• v.34 no.2
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• pp.111-115
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• 2024

Silicon carbide (SiC) has emerged as a promising material for next-generation power semiconductor materials, due to its high thermal conductivity and high critical electric field (~3 MV/cm) with a wide bandgap of 3.3 eV. This permits SiC devices to operate at lower on-resistance and higher breakdown voltage. However, to improve device performance, advanced research is still needed to reduce point defects in the SiC epitaxial layer. This work investigated the electrical characteristics and defect properties using DLTS analysis. Four deep level defects generated by the implantation process and during epitaxial layer growth were detected. Trap parameters such as energy level, capture-cross section, trap density were obtained from an Arrhenius plot. To investigate the impact of defects on the device, a 2D TCAD simulation was conducted using the same device structure, and the extracted defect parameters were added to confirm electrical characteristics. The degradation of device performance such as an increase in on-resistance by adding trap parameters was confirmed.

• Proceedings of the Korean Vacuum Society Conference
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• 2014.02a
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• pp.327.1-327.1
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• 2014

Nitrides-on-silicon structures are considered to be an excellent candidate for unique design architectures and creating devices for high-power applications. Therefore, a lot of effort has been concentrating on growing high-quality III-nitrides on Si substrates, mostly Si(111) and Si(001) substrates. However, there are several fundamental problems in the growth of nitride compound semiconductors on silicon. First, the large difference in lattice constants and thermal expansion coefficients will lead to misfit dislocation and stress in the epitaxial films. Second, the growth of polar compounds on a non-polar substrate can lead to antiphase domains or other defective structures. Even though the lattice mismatches are reached to 16.9 % to GaN and 19 % to AlN and a number of dislocations are originated, Si(111) has been selected as the substrate for the epitaxial growth of nitrides because it is always favored due to its three-fold symmetry at the surface, which gives a good rotational matching for the six-fold symmetry of the wurtzite structure of nitrides. Also, Si(001) has been used for the growth of nitrides due to a possible integration of nitride devices with silicon technology despite a four-fold symmetry and a surface reconstruction. Moreover, Si(110), one of surface orientations used in the silicon technology, begins to attract attention as a substrate for the epitaxial growth of nitrides due to an interesting interface structure. In this system, the close lattice match along the [-1100]AlN/[001]Si direction promotes the faster growth along a particular crystal orientation. However, there are insufficient until now on the studies for the growth of nitride compound semiconductors on Si(110) substrate from a microstructural point of view. In this work, the microstructural properties of nitride thin layers grown on Si(110) have been characterized using various TEM techniques. The main purpose of this study was to understand the atomic structure and the strain behavior of III-nitrides grown on Si(110) substrate by molecular beam epitaxy (MBE). Insight gained at the microscopic level regarding how thin layer grows at the interface is essential for the growth of high quality thin films for various applications.

• Korean Journal of Materials Research
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• v.11 no.5
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• pp.413-418
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• 2001

We investigated change of crystal structure, surface morphology and crystal orientation of the electrodeposited film from dispersed $SiO_2$ suspensions (colloidal silica) copper sulfate bath and arse corrosion potentials and physical specific properties. As addition of colloidal silica in copper electrolytic hath, the crystal Particles on filial was fined-down, made uniform and account of particles were increased. Hardness of copper electrodeposited film ascended about 15% and (111), (200) and (311) plane of X-ray diffraction patterns were almost swept away, so preferred orientation chanced from (111) to (110) plane. Also, corrosion potential of electrodeposited copper film was noble with colloidal silica addition.

• Journal of the Korean Vacuum Society
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• v.5 no.3
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• pp.199-205
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• 1996

InGaAs eqitaxial layers have been selectively grown on patterned GaAs(100) substrates by chemical beam epitaxy (CBE) using triethylgallium (TEGa), trimethylindium (TMIn), and unprecracked monoethylarsine (MEAs). Facet growth of InGaAs epilayers has also been investigated at the various growth temperatures and Si4N4 dielectric pattern directions. In [011] jirection of mask, the change from (311), (377) and (111) facets to (311) facet with increasing growth temperature was observed. In [011] direction, however, the change from (011) and (111) facets to (111) facet with increasing growth temperature was observed. These results are attributed to the sidewall growth caused by different surface migration lengths of reactants. The formation of U-shaped (100) top surface is also discussed in terms of dangling bond model.

• Proceedings of the KIEE Conference
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• 2005.11a
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• pp.12-14
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• 2005

Inductively Coupled Plasma Chemical Vapor Deposition(ICP-CVD)를 이용하여 공정온도 $150^{\circ}C$에서 Nanocrystalline silicon (nc-Si) 박막을 증착하였다. 실험에서 헬륨(He)가스, 수소($H_2$)가스 그리고 헬륨(He)과 수소($H_2$)의 혼합가스로 희석한 사일렌($SiH_4$)을 반응가스로 이용하였다. 이 혼합가스는 3sccm의 사일렌($SiH_4$)에 헬륨(He)과 수소($H_2$)의 주입율을 20sccm에서부터 60sccm까지 변화시켜 조건을 달리하여 사용했다. 증착한 Nc-Si 박막을 X-ray diffraction (XRD)으로 분석하여 각각의 조건에 대한 Nc-Si 박막의 속성을 연구하였다. 헬륨(He) 또는 수소($H_2$) 혼합가스의 주입율이 커지면서 <111>과 <222>의 최고점(peak)이 더 높아졌으며 결정화 되지 않고 비결정질로 남아 있는 성장층(incubation layer)이 얇아졌다. 이 결과는 nc-Si를 증착할 때 사용한 수소($H_2$) 플라즈마와 헬륨(He) 플라즈마의 효과로 설명할 수 있다. 실험을 통해 ICP-CVD로 증착한 nc-Si 박막을 박막 전계효과트랜지스터 (TFT)에서 우수한 특성의 전자수송층(active layer)으로 사용할 수 있는 것을 확인하였다.

• Proceedings of the Materials Research Society of Korea Conference
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• 2009.05a
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• pp.52.2-52.2
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• 2009

Si 박막형 solar cell은 Si 결정형 solar cell대비 cost 및 대면적화 측면에서 장점을 가지고 있다. 그러나 amorphous Si의 경우 light soacking에 의한 열화 문제가 있고, microcrystalline Si의 경우 요구되는 효율 확보를 위하여 $1.5{\mu}m$ 이상 두께가 필요하며, 증착율이 $5{\AA}/sec$.이하인 단점이 있다. 본 연구에서는 high deposition rate로 microcrystalline Si를 증착하기 위하여 high frequency, high power PECVD를 이용하였으며, RF power, 증착온도, H2/SiH4 ratio의 3인자를 3수준으로 변화시킨 완전요인배치 실험을 실시하였다. 실험결과 증착율은 $8.0{\AA}/sec.{\sim}52.8{\AA}/sec$ 범위, crystalline fraction은 0%~83.3% 범위의 결과를 얻었으며, 결정이 형성된 조건에서는 XRD분석결과 $2\theta=28.5$ 및 47.5에서 Si (111), (220) peak을 확인할 수 있었다. Surface Profilometer 를 이용한 surface roughness의 경우 $6.3{\AA}\sim32.4{\AA}$ 범위의 결과를 얻었으며, crystalline Portion이 높을수록 surface roughness가 증가함을 알 수 있었다.

• Journal of the Korean Vacuum Society
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• v.4 no.S2
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• pp.64-68
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• 1995

Silicon films were deposited at $430^{\circ}C$ by remote plasma chemical vapor deposition(RPECVD) with a gas mixture of $Si_2H_6/SiF_4/H_2$. The silicon films deposited without and with $SiF_4$ were characterized using atomic force microscopy(AFM), transmission electron microscopy(TEM) and X-ray diffraction(XRD). Both silicon films have the same rugged surface morphology, but, the silicon film deposited with $SiF_4$ exhibits more rugged. The silicon film deposited without $SiF_4$ is amorphous, whereas the silicon film deposited with $SiF_4$ is polycrystalline with very small needle-like grains which are perpendicular to the substrate and uniformly distributed in the thickness of the film. The silicon film deposited with $SiF_4$ was found to have a preferred orientation along the growth direction with the<110> of the film parallel to the <111> of the substrate. The effect of $SiF_4$ during RPECVD was discussed.

• Proceedings of the Korean Vacuum Society Conference
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• 2001.02a
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• pp.101-101
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• 2001

• Proceedings of the Korean Vacuum Society Conference
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• 2001.02a
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• pp.182-182
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• 2001