• Proceedings of the Korean Vacuum Society Conference
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• 2010.02a
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• pp.475-475
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• 2010

We have generated Ar plasma in dense plasma focus device with coaxial electrodes for extreme ultraviolet (EUV) lithography and investigated an emitted visible light for electro-optical plasma diagnostics. We have applied an input voltage 4.5 kV to the capacitor bank of 1.53 uF and the diode chamber has been filled with Ar gas of pressure 8 mTorr. The inner surface of the cylindrical cathode has been attatched by an acetal insulator. Also, the anode made of tin metal. If we assumed that the focused plasma regions satisfy the local thermodynamic equilibrium (LTE) conditions, the electron temperature and density of the coaxial plasma focus could be obtained by Stark broadening of optical emission spectroscopy (OES). The Lorentzian profile for emission lines of Ar I of 426.629 nm and Ar II of 487.99 nm were measured with a visible monochromator. And the electron density has been estimated by FWHM (Full Width Half Maximum) of its profile. To find the exact value of FWHM, we observed the instrument line broadening of the monochromator with a Hg-Ar reference lamp. The electron temperature has been calculated using the two relative electron density ratios of the Stark profiles. In case of electron density, it has been observed by the Stark broadening method. This experiment result shows the temporal behavior of the electron temperature and density characteristics for the focused plasma. The EUV emission signal whose wavelength is about 6 ~ 16 nm has been detected by using a photo-detector (AXUV-100 Zr/C, IRD). The result compared the electron temperature and density with the temporal EUV signal. The electron density and temperature were observed to be $10^{16}\;cm^{-3}$ and 20 ~ 30 eV, respectively.

• Journal of the Korea Academia-Industrial cooperation Society
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• v.5 no.3
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• pp.223-226
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• 2004

Injection molding using plastic materials was expected to mass production of structure with nano pattern for low cost phase. The PDMS mold was produced easily and uniformly by using thermal embossing. Quartz master for embossing method was made using electron beam lithography it had 100-500 nm size of line and dot type. The PDMS mold was produced after a brief hardening process and the master removal. The results show that various patterns are successfully fabricated the nano scale.. The replicated mold would be useful a stamper fabrication for injection molding.

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 1999.05a
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• pp.575-577
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• 1999

In this study, the PPPI(Plasma Polymerized Phenyl Isothiocyanate) resist thin film was manufactured in accordance with the plasma polymerization method and after exposing it to an electron beam, a pattern was formed by plasma etching. With the FT-IR(Fourier transform-infrared spectrometry) analysis, it was confirmed that the PI(Phenl Isothiocyanate) monomer was successsfully produced into a thin film by the plasma. The polymerization rate of the thin film was 450~ 1012($\AA$/min) to 100-200(W) discharge power and 120-12($\AA$/min) to 0.1 ~0.4[torr] system pressure.

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 2004.07a
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• pp.44-47
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• 2004

단일 나노선 연구에 있어서 나노선에 원하는 패턴을 선택적으로 구현하는 새로운 방법을 소개한다. 기존에 많이 쓰였던 SEM(Scanning Electron Microscope) 사진을 통한 나노선의 위치를 찾는 방법은 전자빔에 의해 유도되는 비결정성 탄소입자 등으로 인해 측정하고자하는 나노선의 전기적 특성을 왜곡시킬 수 있다. 이러한 점을 예방하고 작업의 편리성을 위하여 ER(E-beam Resist)이 코팅된 상태에서 바로 SEM을 이용해 패터닝하는 방법을 고안하였다. 또 다른 방법으로 기존의 AFM(Atomic Force Microscope) 사진으로 위치를 찾는 방식의 단점인 긴 작업시간을 개선하기 위해 광학현미경 사진을 이용해 패터닝하는 방법을 고안하였다. 이러한 방법들은 작업의 편리성이나 패턴의 정확도면에서 서로 보완적인 성격을 가지고 있어 필요에 따라 방법을 선택할 수 있다.

• Proceedings of the Korean Vacuum Society Conference
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• 2011.08a
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• pp.332-332
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• 2011

The extreme ultraviolet (EUV) radiation, whose wavelength is from 120 nm down to 10 nm, and the energy from 10 eV up to 124 eV, is widely utilized such as in photoelectron spectroscopy, solar imaging, especially in lithography and soft x-ray microscopy. In this study, we have investigated the plasma diagnostics as well as the debris characteristics between the two types of dense plasma focusing devices with coaxial electrodes of Mather and hypocycloidal pinch (HCP), respectively. The EUV emission intensity, electron temperature and plasma density have been investigated in these cylindrical focused plasma along with the debris characteristics. An input voltage of 5 kV has been applied to the capacitor bank of 1.53 uF and the diode chamber has been filled with Ar gas at pressure ranged from 1 mTorr and 180 mTorr. The inner surface of the cathode was covered by polyacetal insulator. The central anode electrode has been made of tin. The wavelength of the EUV emission has been measured to be in the range of 6~16 nm by a photo-detector (AXUV-100 Zr/C, IRD). The visible emission has also been measured by the spectrometer with the wavelength range of 200~1,100 nm. The electron temperature and plasma density have been measured by the Boltzmann plot and Stark broadening methods, respectively, under the assumption of local thermodynamic equilibrium (LTE).

• Korean Journal of Optics and Photonics
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• v.19 no.1
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• pp.20-24
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• 2008

A color filter was proposed and demonstrated by incorporating a subwavelength patterned 1-dimensional grating in poly silicon. It was produced by employing the laser interference lithography method, providing much wider effective area compared to the conventional e-beam lithography. A $SiO_2$ layer was introduced on top of the silicon grating layer as a mask for the etching of the silicon, facilitating the etching of the silicon layer. It was theoretically found that the selectivity of the filter was also improved thanks to the oxide layer. The parameters for the designed device include the grating pitch of 450 nm, the grating height of 100 nm and the oxide-layer height of 200 nm. As for the fabricated filter, the spectral pass band corresponded to the blue color centered at 470 nm and the peak transmission was about 40%. Within the effective area of $3{\times}3mm^2$, the variation in the relative transmission efficiency and in the center wavelength was less than 10% and 2 nm respectively. Finally, the influence of the angle of the incident beam upon the transfer characteristics of the device was investigated in terms of the rate of the relative transmission efficiency, which was found to be equivalent to 1.5%/degree.

• Proceedings of the Korean Institute of Surface Engineering Conference
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• 2018.06a
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• pp.85.2-85.2
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• 2018

금속 나노구조체에서의 localized surface plasmon resonance와 surface-enhanced Raman scattering 현상은 센서를 비롯한 다양한 응용분야를 가지고 있다. 나노구조체 array 형성을 위한 대표적인 top-down 방식인 e-beam lithography 공정은 제조비용이 매우 높고 대량생산 및 대면적화에도 한계가 있기에 polystyrene(PS) bead의 self-assembly를 이용한 nanosphere lithography와 같은 bottom-up 방식이 폭넓게 연구되고 있다. Closed-packing된 PS bead의 monolayer를 얻기 위해서는 기판의 친수성 처리가 필요한데, 기존의 많은 연구에서는 기판의 표면개질에 화학적 공정을 이용하고 있다. 하지만 이는 기판 선택의 자유도를 떨어뜨리는 원인이 된다. 금속이나 실리콘 기판에서는 산성 용액을 이용한 화학적 처리방법을 적용할 수 있지만 SU-8과 같은 감광액 및 폴리머 기판에서는 산에 대한 내구성이 떨어져 화학적 공정의 도입이 불가능 하기 때문이다. 본 연구에서는 이러한 한계점을 극복하기 위해 $UV-O_3$ 공정으로 친수성 처리된 다양한 기판에서 spin coating을 통한 PS monolayer를 제조하였는데, UV 램프의 에너지 조절을 통해 기판에 붙어있는 유기물들을 효과적으로 제거할 수 있었고 $O_3$ 생성 및 분해 과정에서 기판 표면에 친수성 화학 작용기를 생성시킬 수 있었다. 제조된 PS layer를 mask로 사용하여 Ag, Al, Au 등 다양한 나노구조체 array를 형성하여 array 주기에 따른 플라즈몬 공명 특성을 분석하였다. 레이저 조사로 나노구조체의 형상을 변화시킴으로써 동일한 물질과 주기를 가진 array에서도 플라즈몬 특성의 변조가 가능함을 확인하였는데, 이는 금속 나노구조체의 응용측면에서 매우 고무적인 발견이다.

• Korean Journal of Optics and Photonics
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• v.21 no.4
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• pp.175-178
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• 2010

A transmission type color filter based on a thin film Ag-$SiO_2$-Ag etalon was proposed and realized in a quartz substrate. The device could acquire infrared suppressed transmission and wide effective area compared to costly e-beam lithography and laser interference lithography. The FDTD method was introduced to take into account the effect of the dispersion characteristics of the silver metal and the thickness thereof. Three different color filters were devised: The cavity length for the red, green and blue filters were 160 nm, 130 nm, and 100 nm respectively, with the metal layer unchanged at 25 nm. The observed center wavelengths were measured at 650 nm, 555 nm, and 480 nm for the red, green, and blue devices; the corresponding bandwidths were about 120 nm, 100 nm, and 120 nm; and the peak transmission for all was ~60%. Finally the relative transmission was measured to decline with the angle of the incident beam with the rate of 1%/degree.

• Journal of the Semiconductor & Display Technology
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• v.20 no.4
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• pp.29-37
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• 2021

A 7 nm technology node using extreme ultraviolet lithography with a wavelength of 13.5 nm has been recently developed and applied to the semiconductor manufacturing process. Furthermore, the development of sub-3 nm technology nodes continues to be required. In this study, design factors of an electrostatic deflector for an ultra-miniaturized microcolumn system that can realize an electron wavelength of below 1.23 nm with an acceleration voltage of above 1 eV were investigated using a three-dimensional simulator. Particularly, the optimal design of the electrostatic octupole floating deflector was derived by optimizing the design elements and improving the driving method of the 1 keV low energy ultra-miniaturized microcolumn deflector. As a result, the entire wide field of view greater than 330 ㎛ at a working distance of 4 mm was realized with an ultra-high-resolution electron beam spot smaller than 10 nm. The results of this study are expected to be a basis technology for realizing a wafer-scale multi-array microcolumn system, which is expected to innovatively improve the throughput per unit time, which is the biggest drawback of electron beam lithography.

• Proceedings of the Korean Vacuum Society Conference
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• 2012.02a
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• pp.436-437
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• 2012

Double patterning technology (DPT) has been suggested as a promising candidates of the next generation lithography technology in FLASH and DRAM manufacturing in sub-40nm technology node. DPT enables to overcome the physical limitation of optical lithography, and it is expected to be continued as long as e-beam lithography takes place in manufacturing. Several different processes for DPT are currently available in practice, and they are litho-litho-etch (LLE), litho-etch-litho-etch (LELE), litho-freeze-litho-etch (LFLE), and self-aligned double patterning (SADP) [1]. The self-aligned approach is regarded as more suitable for mass production, but it requires precise control of sidewall space etch profile for the exact definition of hard mask layer. In this paper, we propose etch end point detection (EPD) in spacer etching to precisely control sidewall profile in SADP. Conventional etch EPD notify the end point after or on-set of a layer being etched is removed, but the EPD in spacer etch should land-off exactly after surface removal while the spacer is still remained. Precise control of real-time in-situ EPD may help to control the size of spacer to realize desired pattern geometry. To demonstrate the capability of spacer-etch EPD, we fabricated metal line structure on silicon dioxide layer and spacer deposition layer with silicon nitride. While blanket etch of the spacer layer takes place in inductively coupled plasma-reactive ion etching (ICP-RIE), in-situ monitoring of plasma chemistry is performed using optical emission spectroscopy (OES), and the acquired data is stored in a local computer. Through offline analysis of the acquired OES data with respect to etch gas and by-product chemistry, a representative EPD time traces signal is derived. We found that the SE-EPD is useful for precise control of spacer etching in DPT, and we are continuously developing real-time SE-EPD methodology employing cumulative sum (CUSUM) control chart [2].