• Title/Summary/Keyword: Focused Ion Beam Lithography

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Monte-Carlo Simulation for Exposure and Development of Focused Ion Beam Lithography (집속이온빔 리소그라피 (Focused Ion Beam Lithography)외 노출 및 현상에 대한 몬데칼로 전산 모사)

  • Lee, Hyun-Yong;Kim, Min-Su;Chung, Hong-Bay
    • Proceedings of the KIEE Conference
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    • 1994.07b
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    • pp.1246-1249
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    • 1994
  • Thin amorphous film of $a-Se_{75}Ge_{25}$ acts as a positive resist in ion beam lithography. Previously, we reported the optical characteristics of amorphous $Se_{75}Ge_{25}$ thin film by the low-energy ion beam exposure and presented analytically calculated values such as ion range, ion concentration and ion transmission coefficient, etc. As the calculated results of analytical calculation, the energy loss per unit distance by $Ga^+$ ion is about $10^3[keV/{\mu}m]$ and nearly constant for all energy range. Especially, the projected range and struggling for 80 [KeV] $Ga^+$ ion energy are 0.0425[${\mu}m$] and 0.020[${\mu}m$], respectively. Hear, we present the results of Monte-Carlo computer simulation of Ga ion scattering, exposure and development in $a-Se_{75}Ge_{25}$ resist film for focused ion beam(FIB) lithography. Monte-Carlo method is based on the simulation of individual particles through their successive collisions with resist atoms. By the summation of the scattering events occurring in a large number N(N>10000) of simulated trajectories within the resist, the distribution for the range parameters is obtained. Also, the deposited energy density and the development pattern by a Gaussian or a rectangular ion beam exposure can be obtained.

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Monte-Carlo Simulation of Focused ton Beam Lithography (집속 이온빔 리소그라피의 몬데칼로 전산 모사)

  • 이현용;정홍배
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 1993.11a
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    • pp.134-136
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    • 1993
  • Microelectronic fabrication technology .is based on the use of lithsgraphy to create small linewidths and patterns that make up ULSI. In previous papers, we discussed the theoretically calculated values such as ion range, ion concentration,ion transmission coefficient and the defocused ion beam-induced characteristics in a-Se$_{75}$Ge$_{25}$. In this paper, the typical Monte Carlo (MC) simulation results and p개cedures for the focused ion beam lithography were presented. The interaction and scattering of ions with the resist depend on the beam energy, impact parameter arid resist parameters. For ion exposure simulations, the quantity of interest is the spatial distribution of energy deposited by ions in the resist due to interaction phenomena with resist ions.s.s.

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EUVL Mask Defect Isolation and Repair using Focused Ion Beam (Focused Ion Beam을 이용한 EUVL Mask Defect Isolation 및 Repair)

  • 김석구;백운규;박재근
    • Journal of the Semiconductor & Display Technology
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    • v.3 no.2
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    • pp.5-9
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    • 2004
  • Microcircuit fabrication requires precise control of impurities in tiny regions of the silicon. These regions must be interconnected to create components and VLSI circuits. The patterns to define such regions are created by lithographic processes. In order to image features smaller than 70 nm, it is necessary to employ non-optical technology (or next generation lithography: NGL). One such NGL is extreme ultra-violet lithography (EUVL). EUVL transmits the pattern on the wafer surface after reflecting ultra-violet through mask pattern. If particles exist on the blank mask, it can't transmit the accurate pattern on the wafer and decrease the reflectivity. It is important to care the blank mask. We removed the particles on the wafer using focused ion beam (FIB). During removal, FIB beam caused damage the multi layer mask and it decreased the reflectivity. The relationship between particle removal and reflectivity is examined: i) transmission electron microscope (TEM) observation after particle removal, ii) reflectivity simulation. It is found that the image mode of FIB is more effective for particle removal than spot and bar mode.

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Focused Ion Beam Milling for Nanostencil Lithography (나노스텐실 제작을 위한 집속이온빔 밀링 특성)

  • Kim, Gyu-Man
    • Journal of the Korean Society for Precision Engineering
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    • v.28 no.2
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    • pp.245-250
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    • 2011
  • A high-resolution shadow mask, a nanostencil, is widely used for high resolution lithography. This high-resolution shadowmask is often fabricated by a combination of MEMS processes and focused ion beam (FIB) milling. In this study, FIB milling on 500-nm-thin SiN membrane was tested and characterized. 500 nm thick and $2{\times}2$ mm large membranes were made on a silicon wafer by micro-fabrication processes of LPCVD, photolithography, ICP etching and bulk silicon etching. A subsequent FIB milling enabled local membrane thinning and aperture making into the thinned silicon nitride membrane. Due to the high resolution of the FIB milling process, nanoscale apertures down to 60 nm could be made into the membrane. The nanostencil could be used for nanoscale patterning by local deposition through the apertures.

An analysis of the ion penetration phenomena in amorphous $Se_{75}Ge_{25}$ thin film (비정질 $Se_{75}Ge_{25}$박막으로의 이온침투 현상 해석)

  • 이현용;정홍배
    • Electrical & Electronic Materials
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    • v.7 no.5
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    • pp.389-396
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    • 1994
  • The bilayer film of Ag/a-S $e_{75.G}$ $e_{25}$ and the monolayer film of a-S $e_{75.G}$ $e_{25}$ act as a negative-type and a positive-type resist in focused ion beam lithography, respectively. Using a model which takes into account the ion stopping power, the ion projected range, the ion concentration implanted into resists and the ion transmission coefficient, etc., the ion resist parameters are calculated for a broad range of ion energies and implanted doses. Ion sources of A $r^{+}$, S $i^{++}$ and G $a^{+}$ are used to expose resists. As the calculated results, the energy loss per unit distance by Ga'$^{+}$ ion is about 10$^{3}$[keV/.mu.M] and nearly constant for all energy range. Especially, the projected range and struggling for 80[keV] G $a^{+}$ ion energy are 0.0425[.mu.m] and 0.020[.mu.m], , respectively and the resist thickness of a-S $e_{75}$ G $e_{25}$ to minimize the ion penetration rate into a substrate is 0.118[.mu.m].u.m]..u.m].

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Ion Beam Induced Micro/Nano Fabrication: Modeling (이온빔을 이용한 마이크로/나노 가공: 모델링)

  • Kim, Heung-Bae;Hobler, Gerhard
    • Journal of the Korean Society for Precision Engineering
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    • v.24 no.8 s.197
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    • pp.108-115
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    • 2007
  • 3D nano-scale manufacturing is an important aspect of advanced manufacturing technology. A key element in ability to view, fabricate, and in some cases operate micro-devices is the availability of tightly focused particle beams, particularly of photons, electrons, and ions. The use of ions is the only way to fabricate directly micro-/ nano-scale structures. It has been utilized as a direct-write method for lithography, implantation, and milling of functional devices. The simulation of ion beam induced physical and chemical phenomena based on sound mathematical models associated with simulation methods is presented for 3D micro-/nanofabrication. The results obtained from experimental investigation and characteristics of ion beam induced direct fabrication will be discussed.

The penetration phenomena of LMIS Ga ion into amorphous Se-Ge thin film (비정질 Se-Ge 박막으로의 LMIS $Ga^+$ 이온 침투현상)

  • Lee, Hyun-Yong;Chung, Hong-Bay
    • Proceedings of the KIEE Conference
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    • 1993.07b
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    • pp.1262-1264
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    • 1993
  • An amorphous $Se_{75}Ge_{25}$ thin film as inorganic resist for the focused ion beam lithography(FIBL) is investigated. This film offers an attractive potential alternative to polymer resists because of a number of advantages, such as the possibility of preparing physically uniform films of thickness as small as 200A and obtaining both positive and negative resist action in the same material, compatibility with dry processing, the sensitivity on optical, e-beam and ion beam exposure, the high-temperature stability, etc. In previous paper, the defocused ion beam-induced characteristics in a-$Se_{75}Ge_{25}$ film has been propose. Practically it is neccesary to know the relation with resist and source ions. For the purpose, the ion stopping power, the ion projected range and ion transmission coefficiency are studied. In this paper, the theoretically calculated values of parameters are presented and compared with theory.

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The ocused Ion Beam Etching Characteristic of Au (집속 이온빔 가공변수에 따른 Au 에칭 특성 연구)

  • Park, J.J.;Kim, S.D.
    • Transactions of the Korean Society of Machine Tool Engineers
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    • v.16 no.5
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    • pp.129-133
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    • 2007
  • Focused Ion Beam(FIB) systems is a useful tool for the fabrication of micro-nano scale structures. In this study, the effects of FIB etching on the Au microstructure are systematically investigated. As the fabrication parameters, ion dose, dwell time and beam overlap ratio are studied. First, the increases of Ga ion dose makes the milling yield higher and the sidewall of milling profile steeper. Dwell time is found to have little effects on the milling profile due to the relatively large milling area of $1\times1{\mu}m^2$ used in this study. However, beam overlap significantly affects not only milling rate but also milling profile. As the beam overlap ratio changes from positive to negative, the development of regular cross-stripe patterns at the bottom with low milling rate is observed.

Fabrication of Movable Nanostructures by Selective Etching of Nanoplates (나노판의 선택적 식각에 의한 이동이 가능한 나노구조체 제작)

  • Yun Yong-Ju;Ah Chil-Seong;Yun Wan-Soo;Ha Dong-Han
    • Transactions of the Korean Society of Mechanical Engineers A
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    • v.30 no.3 s.246
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    • pp.328-333
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    • 2006
  • Movable nanometer-scale structures are fabricated by selective etching of single crystalline Au nanoplates. The nanostructures have arbitrary shapes like gear and alphabet 'A' with in-plane size less than 500 m and thickness of $25\sim60nm$. They could be moved successfully on the substrate using a nanornanipulator installed in a focused ion beam system. Our approach is expected to be useful in fabricating various kinds of nanocomponents which can play a role as building blocks for the sophisticated nanodevices or micromachines.