• Title/Summary/Keyword: Silicon substrate

Search Result 1,271, Processing Time 0.03 seconds

Deposition of diamond film at low pressure using the RF plasma CVD (고주파 플라즈마 CVD에 의한 저 압력에서의 다이아몬드 막의 성장)

  • Koo, Hyo-Geun;Park Sang-Hyun;Park Jae-Yoon;Kim Kyoung-Hwan
    • The Transactions of the Korean Institute of Electrical Engineers C
    • /
    • v.50 no.2
    • /
    • pp.49-56
    • /
    • 2001
  • Diamond thin films have been deposited on the silicon substrate by inductively coupled radio frequency plasma enhanced chemical vapor deposition system. The morphological features of thin films depending on methane concentration and deposition time have been studied by scanning electron microscopy and Raman spectroscopy. The diamond particles deposited uniformly on silicon substrate($10{\times}10[mm^2]$) at the pressure of 1[torr], a methane concentration of 1[%], a hydrogen flow rate of 60[sccm], a substrate temperature of $840\{sim}870[^{\circ}C]$, an input power of 1[kw], and a deposition time of 1[hour]. With increasing deposition time, the diamond particles grew, and than about 3 hours have passed, the graphitic phase carbon thin film with "cauliflower-like" morphology deposited on the diamond thin films.

  • PDF

Influence of Substrate Thermal Conductivity on OLED Lifetime

  • Chung, Seung-Jun;Lee, Jae-Hyun;Jeong, Jae-Wook;Kim, Jang-Joo;Hong, Yong-Taek
    • 한국정보디스플레이학회:학술대회논문집
    • /
    • 2008.10a
    • /
    • pp.1026-1029
    • /
    • 2008
  • Temperature increase during OLED operation can significantly degrade the device lifetime. By using top-emission OLEDs fabricated on glass and silicon substrates that have different thermal conductivities, we found that efficient heat dissipation and corresponding lifetime improvement can be obtained by making a direct contact between the OLED anode and the high thermally-conductive silicon substrate. We describe substrate-dependent OLED heat dissipation behavior and OLED lifetime improvement by using infrared camera images and constant current stress test methods.

  • PDF

Characterizations of Interface-state Density between Top Silicon and Buried Oxide on Nano-SOI Substrate by using Pseudo-MOSFETs

  • Cho, Won-Ju
    • JSTS:Journal of Semiconductor Technology and Science
    • /
    • v.5 no.2
    • /
    • pp.83-88
    • /
    • 2005
  • The interface-states between the top silicon layer and buried oxide layer of nano-SOI substrate were developed. Also, the effects of thermal treatment processes on the interface-state distributions were investigated for the first time by using pseudo-MOSFETs. We found that the interface-state distributions were strongly influenced by the thermal treatment processes. The interface-states were generated by the rapid thermal annealing (RTA) process. Increasing the RTA temperature over $800^{\circ}C$, the interface-state density considerably increased. Especially, a peak of interface-states distribution that contributes a hump phenomenon of subthreshold curve in the inversion mode operation of pseudo-MOSFETs was observed at the conduction band side of the energy gap, hut it was not observed in the accumulation mode operation. On the other hand, the increased interface-state density by the RTA process was effectively reduced by the relatively low temperature annealing process in a conventional thermal annealing (CTA) process.

The Effect of Nitric Acid Catalyst on the Properties of Lead Titanate Thin Films by Sol Gel Spin Coating (졸겔 스핀 코팅에서 질산촉매가 티탄산연 박막의 물성에 미치는 영향)

  • 이전국;정형진;김종희
    • Journal of the Korean Ceramic Society
    • /
    • v.28 no.11
    • /
    • pp.859-864
    • /
    • 1991
  • High quality lead titanate thin films were fabricated by spin coating on a silicon substrate. The resulting dried gel layers were uniform in thickness through 2$\times$2 $\textrm{cm}^2$ area, and polycrystalline perovskite structures developed almost crack free with a heat treatment above 50$0^{\circ}C$ in films with thickness above 360 nm. Metastable pyrochlore structures were observed in films with thickness of 160 nm when heat treated at 500 and $600^{\circ}C$, but these structure did not appear in films with thickness of 360 nm. The thickness dependence in crystal structure of films was studied. by varying the substrate condition and analyzing the interface between the film and substrate. In native oxide films on silicon stbstrates, amorphous dried gel layers were heterogeneously nucleated. Metastable cubic pyrochlore structure could be crystallized in amorphous native oxide.

  • PDF

Surface Micromachining of TEOS Sacrificial Layers by HF Gas Phase Etching (HF 기상식각에 의한 TEOS 희생층의 표면 미세가공)

  • 장원익;이창승;이종현;유형준
    • Proceedings of the Korean Society of Precision Engineering Conference
    • /
    • 1996.11a
    • /
    • pp.725-730
    • /
    • 1996
  • The key process in silicon surface micromachining is the selective etching of a sacrificial layer to release the silicon microstructure. The newly developed anhydrous HF/$CH_3$OH gas phase etching of TEOS (teraethylorthosilicate) sacrificial layers onto the polysilicon and the nitride substrates was employed to release the polysilicon microstructures. A residual product after TEOS etching onto the nitride substrate was observed on the surface, since a SiOxNy layer is formed on the TEOS/nitride interface. The polysilicon microstructures are stuck to the underlying substrate because SiOxNy layer does not vaporize. We found that the only sacrificial etching without any residual product and stiction is TEOS etching onto the polysilicon substrate.

  • PDF

A study on the AIN thin films fabricated by RF magnetron sputtering (RF Magnetron Sputtering 법으로 제조된 AIN 박막에 관한 연구)

  • 남창길;최승우;천희곤;조동율
    • Journal of the Korean Vacuum Society
    • /
    • v.6 no.1
    • /
    • pp.44-49
    • /
    • 1997
  • AIN thin films were deposited on silicon and glass substrates by sputtering Al target and introducing mixed gases of argon and nitrogen into reactive RF magnetron sputter. The substrate was not heated to protect the PC (polycarbonate) substrate and the micro-sized pregroove morphology on the surface of PC substrate. But its temperature was around $100^{\circ}C$ due to the self-heating by plasma. The crystallinity, cross-section morphology and refractive index were characterized by changing various deposition parameters.

  • PDF

Enhanced Crystallization of Si at Low Temperature by $O_2$ Flow during Deposition

  • Nam, Hyoung-Gin;Koo, Kyung-Hwan
    • Journal of the Semiconductor & Display Technology
    • /
    • v.6 no.2 s.19
    • /
    • pp.15-18
    • /
    • 2007
  • Effects of $O_2$ flow during deposition on Si crystallization at low substrate temperature were studied. Silicon thin films were prepared on $SiO_2$ substrates in a low-pressure chemical vapor deposition chamber using a mixture of $SiH_4$ and $H_2$. In some cases $O_2$ was intentionally introduced during deposition. Growth of poly silicon was observed at the substrate temperature as low as $480^{\circ}C$ when $O_2$ was flowed during deposition implying that crystallization of Si was enhanced by $O_2$ flow. On the other hand, $O_2$ flow did not show any significant effects at higher substrate temperature, where deposition rate is relatively fast. Enhancement mechanism of Si crystallization by $O_2$ flow was suggested from these results.

  • PDF

Field emission from diamond-like carbon films studied by scanning anode

  • Ahn, S.H.;Jeon, D.;Lee, K.-R.
    • Journal of Korean Vacuum Science & Technology
    • /
    • v.3 no.1
    • /
    • pp.54-58
    • /
    • 1999
  • We deposited diamond-like carbon (DLC) films using ion beam sputtering of a graphite target on flat substrates for use as a thin film field emitter. An n-type silicon wafer, titanium-coated silicon, and indium tin oxide (ITO) coated glass were used as a substrate. All films exhibited a sudden increase in the emission after a breakdown occurred at high voltage. The morphology of the films after the breakdown depended on the substrate. On ITO and Ti substrates, the DLC film peeled off upon breakdown, but on the Si substrate the surface melting due to breakdown resulted in the formation of various structures such as a sharp point, mound, and crater. By scanning the deformed surface with a tip anode, we found that the emission was concentrated at the deformed sites, indicating that the field enhancement due to the morphology change was responsible for the increased emission.

  • PDF

Design of 60-GHz Back-to-back Differential Patch Antenna on Silicon Substrate

  • Deokgi Kim;Juhyeong Seo;Seungmin Ryu;Sangyoon Lee;JaeHyun Noh;Byeongju Kang;Donghyuk Jung;Sarah Eunkyung Kim;Dongha Shim
    • Journal of the Semiconductor & Display Technology
    • /
    • v.22 no.4
    • /
    • pp.142-147
    • /
    • 2023
  • This paper presents a novel design of a differential patch antenna for 60-GHz millimeter-wave applications. The design process of the back-to-back (BTB) patch antenna is based on the conventional single-patch antenna. The initial design of the BTB patch antenna (Type-I) has a patch size of 0.66 × 0.98 mm2 and a substrate size of 0.99 × 1.48 mm2. It has a gain of 1.83 dBi and an efficiency of 94.4% with an omni-directional radiation pattern. A 0.4 mm-thick high-resistivity silicon (HRS) is employed for the substrate of the BTB patch antenna. The proposed antenna is further analyzed to investigate the effect of substrate size and resistivity. As the substrate resistivity decreases, the gain and efficiency degrade due to the substrate loss. As the substrate (HRS) size decreases approaching the patch size, the resonant frequency increases with a higher gain and efficiency. The BTB patch antenna has optimal performances when the substrate size matches the patch size on the HRS substrate (Type-II). The antenna is redesigned to have a patch size of 0.81 × 1.18 mm2 on the HRS substrate in the same size. It has an efficiency of 94.9% and a gain of 1.97 dBi at the resonant frequency of 60 GHz with an omni-directional radiation pattern. Compared to the initial design of the BTB patch antenna (Type-I), the optimal BTB patch antenna (Type-II) has a slightly higher efficiency and gain with a considerable reduction in antenna area by 34.8%.

  • PDF