• 제목/요약/키워드: 200 mm wafer diameter

검색결과 7건 처리시간 0.022초

정전효과가 있는 100mm보다 큰 반도체 웨이퍼로의 입자침착 (Particle deposition on a semiconductor wafer larger than 100 mm with electrostatic effect)

  • 송근수;유경훈;이건형
    • 한국입자에어로졸학회지
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    • 제5권1호
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    • pp.17-27
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    • 2009
  • Particle deposition on a semiconductor wafer larger than 100 mm was studied experimentally and numerically. Particularly the electrostatic effect on particle deposition velocity was investigated. The experimental apparatus consisted of a particle generation system, a particle deposition chamber and a wafer surface scanner. Experimental data of particle deposition velocity were obtained for a semiconductor wafer of 200 mm diameter with the applied voltage of 5,000 V and PSL particles of the sizes between 83 and 495 nm. The experimental data of particle deposition velocity were compared with the present numerical results and the existing experimental data for a 100 mm wafer by Ye et al. (1991) and Opiolka et al. (1994). The present numerical method took into consideration the particle transport mechanisms of convection, Brownian diffusion, gravitational settling and electrostatic attraction in an Eulerian frame of reference. Based on the comparison of the present experimental and numerical results with the existing experimental results the present experimental method for a 200 mm semiconductor wafer was found to be able to present reasonable data.

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스컬법에 의한 루틸 단결정 성장에 관한 연구 (A study on the growth of rutile single crystal by skull melting method)

  • 석정원;최종건
    • 한국결정성장학회지
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    • 제14권6호
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    • pp.262-266
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    • 2004
  • 초기 RF유도가열을 위해 Ti 금속링을 사용하여 스컬법에 의해 루릴 단결정을 성장시켰다. 성장시킨 단결정은 ${\varnothing}55.5{\times}1.0mm$의 wafer로 가공하였으며,$1300^{\circ}C$에서 15시간까지 대기중에서 열처리 하여 $\lambda=200~25000nm$의 범위에서 투광도를 비교하였다.

새로운 기포동력 마이크로펌프 제작 및 실험 (Novel Fabrication and Testing of a Bubble-Powered Micropump)

  • 정정열;곽호영
    • 대한기계학회:학술대회논문집
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    • 대한기계학회 2004년도 추계학술대회
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    • pp.1196-1200
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    • 2004
  • Micropump is very useful component in micro/nano fluidics and bioMEMS applications. In this study, a bubble-powered micropump was fabricated and tested. The micropump consists of two-parallel micro line heaters, a pair of nozzle-diffuser flow controller and a 1 mm in diameter, 400 ${\mu}m$ in depth pumping chamber. The two-parallel micro line heaters with 20 ${\mu}m-width$ and 200 ${\mu}m-length$ were fabricated to be embedded in the silicon dioxide layer of a wafer which serves as a base plate for the micropump. The pumping chamber, the pair of nozzle-diffuser unit and microchannels including the liquid inlet and outlet port were fabricated by etching through another silicon wafer. A glass wafer (thickness of $525{\pm}15$ ${\mu}m$) having two holes of inlet and outlet ports of liquid serve as upper plate of the pump. Finally the silicon wafer of the base plate, the silicon wafer of pumping chamber and the glass wafer were aligned and bonded (Si-Si bonding and anodic bonding). A sequential photograph of bubble nucleation, growth and collapse was visualized by CCD camera. Clearly liquid flow through the nozzle during the period of bubble growth and slight back flow of liquid at the end of collapsing period can be seen. The mass flow rate was found to be dependent on the duty ratio and the operation frequency. As duty ratio increases, flow rate decreases gradually when the duty ratio exceeds 60%. Also as the operation frequency increases, the flow rate of the micropump decreases slightly.

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SEM 단면 시료 제작을 위한 플라즈마 이온원의 구조 (Structure of a Plasma Ion Source for a Cross-Section SEM Sample)

  • 원종한;장동영;박만진
    • 한국생산제조학회지
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    • 제24권4호
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    • pp.400-406
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    • 2015
  • This study researched the structure of the source of an ion milling machine used to fabricate a scanning electron microscope (SEM) sample. An ion source is used to mill out samples of over 1 mm dimension using a broad ion beam to generate plasma between the anode and cathode using a permanent magnet. To mill the sample in the vacuum chamber, the ion source should be greater than 6 kV for a positive ion current over $200{\mu}A$. To discover the optimum operating conditions for the ion miller, the diameter of the extractor, anode shape, and strength of the permanent magnet were varied in the experiments. A silicon wafer was used as the sample. The sputter yield was measured on the milled surface, which was analyzed using the SEM. The wafer was milled by injecting 1 sccm of argon gas into the 0.5 mTorr vacuum chamber.

Non-contact Transportation of Flat Panel Substrate by Combined Ultrasonic Acoustic Viscous and Aerostatic Forces

  • Isobe, Hiromi;Fushimi, Masaaki;Ootsuka, Masami;Kyusojin, Akira
    • International Journal of Precision Engineering and Manufacturing
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    • 제8권2호
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    • pp.44-48
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    • 2007
  • In recent years, the size of plane substrates and semiconductor wafers has increased. As conventional contact transportation systems composed of, for example, carrier rollers, belt conveyers, and robot hands carry these longer and wider substrates, the increased weight results in increased potential for fracture. A noncontact transportation system is required to solve this problem. We propose a new noncontact transportation system combining acoustic viscous and aerostatic forces to provide damage-free transport. In this system, substrates are supported by aerostatic force and transported by acoustic viscous streaming induced by traveling wave deformation of a disk-type stator. A ring-type piezoelectric transducer bonded on the stator excites vibration. A stator with a high Q piezoelectric transducer can generate traveling vibrations with amplitude of $3.2{\mu}m$. Prior to constructing a carrying road for substrates, we clarified the basic properties of this technique and stator vibration characteristics experimentally. We constructed the experimental equipment using a rotational disk with a 95-mm diameter. Electric power was 70 W at an input voltage of 200 Vpp. A rotational torque of $8.5\times10^{-5}Nm$ was obtained when clearance between the stator and disk was $120{\mu}m$. Finally, we constructed a noncontact transport apparatus for polycrystalline silicon wafers $(150(W)\times150(L)\times0.3(t))$, producing a carrying speed of 59.2 mm/s at a clearance of 0.3 mm between the stator and wafer. The carrying force when four stators acted on the wafer was $2\times10^{-3}N$. Thus, the new noncontact transportation system was demonstrated to be effective.

Laser TSV 공정에 있어서 Via 세정에 관한 연구 (Via Cleaning Process for Laser TSV process)

  • 서원;박재현;이지영;조민교;김구성
    • 마이크로전자및패키징학회지
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    • 제16권1호
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    • pp.45-50
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    • 2009
  • 레이저를 이용 실리콘 관통형 접속기술인 TSV(Through-Silicon-Via)를 형성할 경우 Debris(파편물) 및 Particle이 발생되므로 이를 제거하기 위한 세정공정을 연구하였다. 계면활성제를 이용한 화학적 세정과 Brush를 이용한 물리적 세정을 검토하기 위하여 세정기를 제작하고 8인치 CMOS Image Sensor wafer에 직경 $30{\mu}m$, 깊이 $100{\mu}m$를 갖는 Via를 제작하여 두 가지의 세정방법을 연구하였다. 세정액은 DI Water와 계면활성제의 혼합비 2:1에서 Debris 범위가 $73{\mu}m^2$로 희석비가 낮을수록 세정력이 우수하였다. 레이저의 주파수와 속도변위에 따른 가공 조건 변화에는 Debris 분포차가 5% 미만으로 세정력에는 영향이 없었다. Brush를 이용하여 Debris를 제거하는 실험에서 Strip $1000{\sim}3000rpm$, Rinse $50{\sim}3000rpm$, Brush $200{\sim}300rpm$ 으로 증가시켜 세정하였을 때 Crack이나 손상 없이 Debris의 분포가 감소하였다. 따라서 화학적 세정과 물리적 세정으로 Debris를 제거할 수 있다.

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Fabrication of Microwire Arrays for Enhanced Light Trapping Efficiency Using Deep Reactive Ion Etching

  • 황인찬;서관용
    • 한국진공학회:학술대회논문집
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    • 한국진공학회 2014년도 제46회 동계 정기학술대회 초록집
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    • pp.454-454
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    • 2014
  • Silicon microwire array is one of the promising platforms as a means for developing highly efficient solar cells thanks to the enhanced light trapping efficiency. Among the various fabrication methods of microstructures, deep reactive ion etching (DRIE) process has been extensively used in fabrication of high aspect ratio microwire arrays. In this presentation, we show precisely controlled Si microwire arrays by tuning the DRIE process conditions. A periodic microdisk arrays were patterned on 4-inch Si wafer (p-type, $1{\sim}10{\Omega}cm$) using photolithography. After developing the pattern, 150-nm-thick Al was deposited and lifted-off to leave Al microdisk arrays on the starting Si wafer. Periodic Al microdisk arrays (diameter of $2{\mu}m$ and periodic distance of $2{\mu}m$) were used as an etch mask. A DRIE process (Tegal 200) is used for anisotropic deep silicon etching at room temperature. During the process, $SF_6$ and $C_4F_8$ gases were used for the etching and surface passivation, respectively. The length and shape of microwire arrays were controlled by etching time and $SF_6/C_4F_8$ ratio. By adjusting $SF_6/C_4F_8$ gas ratio, the shape of Si microwire can be controlled, resulting in the formation of tapered or vertical microwires. After DRIE process, the residual polymer and etching damage on the surface of the microwires were removed using piranha solution ($H_2SO_4:H_2O_2=4:1$) followed by thermal oxidation ($900^{\circ}C$, 40 min). The oxide layer formed through the thermal oxidation was etched by diluted hydrofluoric acid (1 wt% HF). The surface morphology of a Si microwire arrays was characterized by field-emission scanning electron microscopy (FE-SEM, Hitachi S-4800). Optical reflection measurements were performed over 300~1100 nm wavelengths using a UV-Vis/NIR spectrophotometer (Cary 5000, Agilent) in which a 60 mm integrating sphere (Labsphere) is equipped to account for total light (diffuse and specular) reflected from the samples. The total reflection by the microwire arrays sample was reduced from 20 % to 10 % of the incident light over the visible region when the length of the microwire was increased from $10{\mu}m$ to $30{\mu}m$.

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