• Journal of the Microelectronics and Packaging Society
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• v.30 no.4
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• pp.8-16
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• 2023

The importance of next-generation packaging technologies is being emphasized as a solution as the miniaturization of devices reaches its limits. To address the bottleneck issue, there is an increasing need for 2.5D and 3D interconnect pitches. This aims to minimize signal delays while meeting requirements such as small size, low power consumption, and a high number of I/Os. Hybrid bonding technology is gaining attention as an alternative to conventional solder bumps due to their limitations such as miniaturization constraints and reliability issues in high-temperature processes. Recently, there has been active research conducted on SiCN to address and enhance the limitations of the Cu/SiO₂ structure. This paper introduces the advantages of Cu/SiCN over the Cu/SiO₂ structure, taking into account various deposition conditions including precursor, deposition temperature, and substrate temperature. Additionally, it provides insights into the core mechanisms of SiCN, such as the role of Dangling bonds and OH groups, and the effects of plasma surface treatment, which explain the differences from SiO₂. Through this discussion, we aim to ultimately present the achievable advantages of applying the Cu/SiCN hybrid bonding structure.

• Journal of Adhesion and Interface
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• v.24 no.3
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• pp.100-104
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• 2023

Van der Waals heterostructures have garnered significant attention in recent research due to their excellent electronic characteristics arising from the absence of dangling bonds and the exclusive reliance on Van der Waals forces for interlayer coupling. However, most studies have been confined to fundamental research employing the Scotch tape (mechanical exfoliation) method. We fabricated Van der Waals vertical heterojunction transistors to advance this field using materials exclusively grown via chemical vapor deposition (CVD). CVDgrown graphene was patterned through photolithography to serve as electrodes, while CVD-grown MoSe₂ was employed as the pickup/transfer material, resulting in the realization of Van der Waals heterojunction transistors with interlayer charge transfer effects. The electrical characteristics of the fabricated devices were thoroughly examined. Additionally, we observed variations in the transistor's performance based on the presence of defects in MoSe₂ layer.

• Proceedings of the Korean Institute of Surface Engineering Conference
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• 2016.11a
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• pp.181-181
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• 2016

Hydrogenated microcrystalline silicon (${\mu}c-Si:H$) films have attracted much attention as materials of the bottom-cells in Si thin film tandem photovoltaics due to their low bandgap and excellent stability against light soaking. However, in PECVD, the source gas $SiH_4$ must be highly diluted by $H_2$, which eventually results in low deposition rate. Moreover, it is known that high-rate ${\mu}c-Si:H$ growth is usually accompanied by a large number of dangling-bond (DB) defects in the resulting films, which act as recombination centers for photoexcited carriers, leading to a deterioration in the device performance. During film deposition, Si nanoparticles generated in $SiH_4$ discharges can be incorporated into films, and such incorporation may have effects on film properties depending on the size, structure, and volume fraction of nanoparticles incorporated into films. Here we report experimental results on the effects of nonoparticles incorporation at the different substrate temperature studied using a multi-hollow discharge plasma CVD method in which such incorporation can be significantly suppressed in upstream region by setting the gas flow velocity high enough to drive nanoparticles toward the downstream region. All experiments were performed with the multi-hollow discharge plasma CVD reactor at RT, 100, and $250^{\circ}C$, respectively. The gas flow rate ratio of $SiH_4$ to $H_2$ was 0.997. The total gas pressure P was kept at 2 Torr. The discharge frequency and power were 60 MHz, 180 W, respectively. Crystallinity Xc of resulting films was evaluated using Raman spectra. The defect densities of the films were measured with electron spin resonance (ESR). The defect density of fims deposited in the downstream region (with nonoparticles) is higher defect density than that in the upstream region (without nanoparticles) at low substrate temperature of RT and $100^{\circ}C$. This result indicates that nanoparticle incorporation can change considerably their film properties depending on the substrate temperature.

• Proceedings of the Korean Vacuum Society Conference
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• 2013.02a
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• pp.277-277
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• 2013

The epitaxial graphene on the 4H- or 6H-SiC(0001) surface has been intensively studied due to the possibility of wafer-scale growt. However the existence of interface layer (zero layer graphene) and its influence on the upper graphene layer have been considered as one of the main obstarcles for the industrial application. Among various methods tried to overcome the strong interaction with the substrate through the interface layer, it has been proved that the hydrogen intercalation successfully passivate the Si dangling bond of the substrate and can produce the quasi-free standing epitaxial graphene (QFEG) layers on the siC(0001) surface. In this study, we report the results of the angle-resolved photoemission spectroscopy (ARPES) and Raman spectroscopy for the QFEG layers produced by ex-situ and in-situ hydrogen intercalation.From the ARPES measurement, we confirmed that the Dirac points of QFEG layers exactly coincide with the Fermi level. The band structure of QFEG layer are sustainable upon thermal heating up to 1100 K and robust against the deposition of several metals andmolecular deposition. We also investigated the strain of the QFEG layers by using Raman spectroscopy measurement. From the change of the 2D peak position of graphene Raman spectrum, we found out that unlike the strong compressive strain in the normal epitaxial graphene on the SiC(0001) surface, the strain of the QFEG layer are significantly released and almost similar to that of the mechanically exfoliated graphene on the silicon oxide substrate. These results indicated that various ideas proposed for the ideal free-standing graphene can be tested based on the QFEG graphene layers grown on the SiC(0001) surface.

• Proceedings of the Korean Vacuum Society Conference
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• 2014.02a
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• pp.271-271
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• 2014

본 연구에서는 최근 다양한 전자 소자로써의 연구가 진행되고 있는 그라핀을 SiO2/Si 기판 위에 전자빔 식각(Electron-Beam Lithography)을 이용하여 후면 게이트 전극 구조의 그라핀 채널을 갖는 삼단자 소자를 형성하고 가스 유입이 가능한 진공 Probe Measurement System을 이용하여 금속 전극과 그라핀 간의 접촉저항 (Rc) 및 길이가 다른 채널저항(Rch)를 구하고, 채널 길이, 가스 유량, 온도, 게이트 전압에 따른 I-V 변화를 측정함으로써, 후면 게이트 전극 구조의 그라핀 채널을 갖는 삼단자 소자의 가스 센서로서의 가능성을 연구하였다. 후면 게이트 전극 구조의 그라핀 채널을 갖는 삼단자 소자는 전자빔 식각(Electron-Beam Lithography)에 의해 패턴을 제작하고 Evaporator를 이용하여 전극을 증착 하였다. 소자의 소스 (Source)와 드레인 (Drain)은 TLM (Transfer Length Method)패턴을 이용하여 인접한 두 개의 전극간 범위를 변화시키는 형태로 제작함으로써 소스-드레인간 채널 길이가 다르게 하였다. 이 때 전극의 크기는 가로, 세로 각각 $20{\mu}m$, $40{\mu}m$이며 전극간 간격은 $20/30/40/50/60{\mu}m$로 서로 다르게 배열 하였다. 제작된 그라핀 소자는 진공 Probe Measurement System 내에서 게이트 전압(VG)를 변화시킴으로써 VG 변화에 따른 소자의 특성을 평가하였는데, mTorr 상태의 챔버 내로 O2 가스를 주입하여 그라핀의 Dangling bond 및 Defect site에 결합 된 가스로 인한 전기적 특성의 변화를 측정하고, 이 때 가스의 유량을 50 sccm에서 500 sccm 까지 변화시킴으로써 전기적 특성 변화를 측정하여 센서 소자의 민감도를 평가하였다. 또한, 서로 다르게 배열한 소스-드레인 간의 채널 길이로 인하여 채널과의 접촉 면적에 따른 센서 소자의 민감도 또한 평가할 수 있었다. 그리고 챔버 내 온도를 77 K에서 400 K까지 변화시킴으로써 온도에 따른 소자의 작동 범위를 확인하고 소자의 온도의존성을 평가하였다.

• Proceedings of the Korean Vacuum Society Conference
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• 2011.08a
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• pp.312-312
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• 2011

In SiH4/H2 discharge for growth process of hydrogenated amorphous silicon (a-Si:H), silane polymers, produced by SiH2 + Sin-1H2n ${\rightarrow}$ SinH2n+2, have no reactivity on the film-growing surface. However, under the SiH2 rich condition, high silane reactive species (HSRS) can be produced by electron collision to silane polymers. HSRS, having relatively strong reactivity on the surface, can react with dangling bond and form Si-H2 networks which have a close correlation with photo-induced degradation of a-Si:H thin film solar cell [1]. To find contributions of suggested several external plasma conditions (pressure, frequency and ratio of mixture gas) [2,3] to suppressing productions of HSRS, some plasma characteristics are studied by numerical methods. For this study, a zero-dimensional global model for SiH4/H2 discharge and a one-dimensional particle-in-cell Monte-Carlo-collision model (PIC-MCC) for pure SiH4 discharge have been developed. Densities of important reactive species of SiH4/H2 discharge are observed by means of the global model, dealing 30 species and 136 reactions, and electron energy probability functions (EEPFs) of pure SiH4 discharge are obtained from the PIC-MCC model, containing 5 charged species and 15 reactions. Using global model, SiH2/SiH3 values were calculated when pressure and driving frequency vary from 0.1 Torr to 10 Torr, from 13.56 MHz to 60 MHz respectively and when the portion of hydrogen changes. Due to the limitation of global model, frequency effects can be explained by PIC-MCC model. Through PIC-MCC model for pure SiH4, EEPFs are obtained in the specific range responsible for forming SiH2 and SiH3: from 8.75 eV to 9.47 eV [4]. Through densities of reactive species and EEPFs, polymerization reactions and production of HSRS are discussed.

• Proceedings of the Korean Vacuum Society Conference
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• 2011.02a
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• pp.254-254
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• 2011

현재 AMLCD(Active Matrix Liquid Crystal Display)는 노트북, 컴퓨터, TV등 여러 영상매체에 있어 가장 많이 활용되고 있는 디스플레이로 손꼽힌다. AMLCD에 구동소자로 사용되는 a-Si:H TFT는 낮은 제조비용과 축적된 기술을 바탕으로 가장 많이 쓰이고 있다. 특히 a-Si이 가지는 소형화나 대형화의 편의성은 모바일 기기, projection TV, 광고용 패널 등 적용분야가 점점 넓어지고 있는 추세이다. 하지만 a-Si라는 물질 자체가 가지는 낮은 이동도는 더 많은 application을 위해 해결되어야 할 과제이다. 낮은 이동도는 a-Si 실리콘 원자간 결합의 불규칙성 및 무질서와 dangling bond에 의한 localize state(deep trap, band tail)의 존재 때문에 발생하며 결과적으로 TFT 소자의 특성의 저하를 가져온다. 앞선 연구에서는 carrier이동도의 개선을 위해서 첫 번째로 insulator층과 active층 사이의 계면 상태를 향상시키기 위해 insulator로 쓰이는 a-SiN층 표면에 0~18 sccm의 유량으로 phosphorus를 주입하였다. AFM분석을 해본 결과 phosphorus를 주입함으로써 계면의 roughness가 줄어드는 것을 확인 할 수 있었다. 이러한 계면의 roughness 감소는 표면 산란(surface scattering)및 전자 포획(trap)의 영향을 줄임으로써 이동도의 향상을 가져왔다. 두 번째로 active층으로 쓰이는 a-Si:H 층의 표면에 phosphorus를 0?9sccm의 유량으로 doping하였다. 이로 인해 channel이 형성되는 active 영역에 직접적으로 불순물을 doping됨으로써 전도도를 증가되어 이동도를 향상시켰다. 하지만 지나친 doping은 불순물 산란(impurity scattering)의 증가로 인해 이동도를 저하시키는 결과를 보여 주었다. 본 연구에서는 TFT의 이동도 향상을 위해 두 가지의 technology를 함께 적용시켜 a-SiN/a-Si:H 계면 각각에 phosphorus를 주입 및 doping을 하였다. 모든 박막은 PECVD로 제작하였으며 각 박막의 두께는 a-SiN/a-SiN(phosphorus)/a-Si:H(doped)/a-Si:H/n+ a-Si($2350{\AA}/150{\AA}/150{\AA}/1850{\AA}/150{\AA}$)으로 고정하고 유량을 변화시키면서 특성을 관찰하였다.

• Korean Journal of Materials Research
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• v.28 no.2
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• pp.118-123
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• 2018

5 nm-thick $SiO_2$ layers formed by plasma-enhanced chemical vapor deposition (PECVD) are densified to improve the electrical and interface properties by using nitric acid oxidation of Si (NAOS) method at a low temperature of $121^{\circ}C$. The physical and electrical properties are clearly investigated according to NAOS times and post-metallization annealing (PMA) at $250^{\circ}C$ for 10 min in 5 vol% hydrogen atmosphere. The leakage current density is significantly decreased about three orders of magnitude from $3.110{\times}10^{-5}A/cm^2$ after NAOS 5 hours with PMA treatment, although the $SiO_2$ layers are not changed. These dramatically decreases of leakage current density are resulted from improvement of the interface properties. Concentration of suboxide species ($Si^{1+}$, $Si^{2+}$ and $Si^{3+}$) in $SiO_x$ transition layers as well as the interface state density ($D_{it}$) in $SiO_2/Si$ interface region are critically decreased about 1/3 and one order of magnitude, respectively. The decrease in leakage current density is attributed to improvement of interface properties though chemical method of NAOS with PMA treatment which can perform the oxidation and remove the OH species and dangling bond.

• Journal of Surface Science and Engineering
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• v.42 no.4
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• pp.179-185
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• 2009

Diamond-like carbon(DLC) films were deposited by linear ion source(LIS)-physical vapor deposition method changing the anode voltages from 800 V to 1800 V, and characteristics of the films were investigated using residual stress tester, nano-indentation, micro raman spectroscopy, scratch tester and Field Emission Scanning Electron Microscope(FE-SEM). The results showed that the residual stress and hardness increased with increasing the ion energy up to anode voltage of 1400 V. It was also found that the content of $SP^3$ carbon increased with increasing the anode voltage $SP^3/SP^2$ ratio through investigation of $SP^3/SP^2$ ratio by the micro-raman analysis. From these results, it can be concluded that the physical properties of DLC films such as residual stress and hardness are increased with increasing the anode voltage. These results can be explained that 3-dimensional cross-links between carbon atoms and Dangling bond are enhanced and the internal compressive stress also increased with increasing the anode voltage. The optimal anode voltage is considered to be around 1400 V in these experimental conditions.

• Journal of the Korean Vacuum Society
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• v.6 no.4
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• pp.348-353
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• 1997

Hydrogenated amorphous carbon(a-C:H) films were deposited on p-type Si(100) by DC saddle-field plasma enhanced CVD to investigate the effect of substrate bias on optical properties and structural changes. They were deposited using pure methane gas at a wide range of substrate bias at room temperature and 90 mtorr. The substrate bias voltage ($V_s$) was employed from $V_s=0 V$ to $V_s=400 V$. The information of optical properties was investigated by photoluminescence and transmitance. Chemical bondings of a-C:H have been explored from FT-IR and Raman spectroscopy. The thickness and relative hydrogen content of the films were measured by Rutherford backscattering spectroscopy (RBS) and elastic recoil detection (ERD) technigue. The growth rate of a-C:H film was decreased with the increase of $V_s$, but the hydrogen content of the film was increased with the increase of $V_s$. The a-C:H films deposited at the lowest $V_s$ contain the smallest amount of hydrogen with most of C-H bonds in the of $CH_2$ configuration, whereas the films produced at higher $V_s$ reveal dominant the $CH_3$ bonding structure. The emission of white photoluminescence from the films were observed even with naked eyes at room temperature and the PL intensity of the film has the maximum value at $V_s$=200 V. With $V_s$ lower than 200 V, the PL intensity of the film increased with V, but for V, higher than 200 V, the PL intensity decreased with the increase of $V_s$. The peak energy of the PL spectra slightly shifted to the higher energy with the increase of $V_s$. The optical bandgap of the film, determined by optical transmittance, was increased from 1.5 eV at $V_s$=0V to 2.3 eV at $V_s$=400 V. But there were no obvious relations between the PL peak and the optical gap which were measured by Tauc process.