• 대한교통학회지
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• 제27권1호
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• pp.169-177
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• 2009

본 연구에서는 SLM(Square Lattice Model)과 HLM(Hexagonal Lattice Model)을 개선하여 만든 RHLM(Rotated Hexagonal Model)을 제시하고, 이를 이용하여 양방향 보행 교통류의 시뮬레이션 모형을 개발하였다. $20{\times}20$의 400개 셀에서 진행되었으며, 시간의 변화에 따른 속도, 밀도, 교통류율로 평가하였다. 본 모형을 같은 조건에서 SLM과 비교해본 결과, 기존의 모형이 보행자의 움직임이 불필요한 동작과 비논리적 방향으로 이동하는 것을 모형에 반영하였다면, 본 모형은 보행자의 직진 움직임과 자연스러운 회피 방법을 통해 보행교통류의 최단경로 움직임을 표현할 수 있었다. 또한 보행교통류의 더 높은 곳에서 용량을 가지고 보행을 할 수 있는 현상을 반영할 수 있었고, 보행교통류의 경우 밀도가 높아지더라도 속도가 0이 되는 상황은 잘 일어나지 않는 것을 반영할 수 있음을 알 수 있었다.

• 한국재료학회지
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• 제21권12호
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• pp.697-702
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• 2011

Two-dimensional (2D) nano patterns including a two-dimensional Bravais lattice were fabricated by laser interference lithography using a two step exposure process. After the first exposure, the substrate itself was rotated by a certain angle, $90^{\circ}$ for a square or rectangular lattice, $75^{\circ}$ for an oblique lattice, and $60^{\circ}$ for a hexagonal lattice, and the $90^{\circ}$ and laser incident angle changed for rectangular and the $45^{\circ}$ and laser incident angle changed for a centered rectangular; we then carried out a second exposure process to form 2D bravais lattices. The band structure of five different 2D nano patterns was simulated by a beam propagation program. The presence of the band-gap effect was shown in an oblique and hexagonal structure. The oblique latticed ZnO nano-photonic crystal array had a pseudo-bandgap at a frequency of 0.337-0.375, 0.575-0.596 and 0.858-0.870. The hexagonal latticed ZnO nano-crystallite array had a pseudo-bandgap at a frequency of 0.335-0.384 and 0.585-0.645. The ZnO nano structure with an oblique and hexagonal structure was grown through the patterned opening window area by a hydrothermal method. The morphology of 2D nano patterns and ZnO nano structures were investigated by atomic force microscopy and scanning electron microscopy. The diameter of the opening window was approximately 250 nm. The height and width of ZnO nano-photonic crystals were 380 nm and 250 nm, respectively.