• 제목/요약/키워드: Focal length

검색결과 377건 처리시간 0.028초

Ordered Micropatterns by Confined Dewetting of an Imprinted Polymer Thin Film and Their Microlens Application

  • Lee, Geun-Tak;Yoon, Bo-Kyung;Acharya, Himadri;Park, Cheol-Min;Huh, June
    • Macromolecular Research
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    • 제17권3호
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    • pp.181-186
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    • 2009
  • We fabricated ordered micro/nano patterns induced by controlled dewetting on the topographically patterned PS/P4VP bilayer thin film. The method is based on utilizing microimprinting lithography to induce a topographically heterogeneous bilayer film that allows the controlled dewetting upon subsequent thermal annealing. The dewetting that was initiated strictly at the boundary of the thicker and thinner regions was guided by the presence of the topographic structure. The dewetting front velocity of the microdomains in the confined regions was linearly proportional to the measurement time, which enabled us to control the size of the dewet domain with annealing time. In particular, the submicron sized dot arrays between lines were generated with ease when the dewetting was confined into geometry with a few microns in size. The kinetically driven, non-lithographical pattern structures accompanied the pattern reduction to 400%. The pattern arrays on a transparent glass substrate were especially useful for non-circular microlens arrays where the focal length of the lens was easily tunable by controlling the thermal annealing.

Zoom Lens Design for a 10x Slim Camera using Successive Procedures

  • Park, Sung-Chan;Lee, Sang-Hun
    • Journal of the Optical Society of Korea
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    • 제17권6호
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    • pp.518-524
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    • 2013
  • This study presents a new design method for a zoom lens, in which real lens groups are designed successively to combine to form a lens modules zoom system. The lens modules and aberrations are applied to the initial design for a four-group inner-focus zoom system. An initial design with a focal length range of 4.2 to 39.9 mm is derived by assigning the first-order quantities and third-order aberrations to each module along with the constraints required for optimum solutions. After obtaining the lens module zoom system, the real lens groups are successively, not separately, designed to get a zoom lens system. Compared to the separately designed real lens groups, this approach can give a better starting zoom lens and save time. The successively designed groups result in a zoom system that satisfies the basic properties of the zoom system consisting of the original lens modules. In order to have a slim system, we directly inserted the right-angle prism in front of the first group. This configuration resulted in a compact zoom system with a depth of 12 mm. The finally designed zoom lens has an f-number of 3.5 to 4.5 and is expected to fulfill the requirements for a mobile zoom camera having high zoom ratio of 10x.

강체 이동타겟 추적을 위한 일괄처리방법을 이용한 로봇비젼 제어기법 개발 (Development of Robot Vision Control Schemes based on Batch Method for Tracking of Moving Rigid Body Target)

  • 김재명;최철웅;장완식
    • 한국기계가공학회지
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    • 제17권5호
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    • pp.161-172
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    • 2018
  • This paper proposed the robot vision control method to track a moving rigid body target using the vision system model that can actively control camera parameters even if the relative position between the camera and the robot and the focal length and posture of the camera change. The proposed robotic vision control scheme uses a batch method that uses all the vision data acquired from each moving point of the robot. To process all acquired data, this robot vision control scheme is divided into two cases. One is to give an equal weight for all acquired data, the other is to give weighting for the recent data acquired near the target. Finally, using the two proposed robot vision control schemes, experiments were performed to estimate the positions of a moving rigid body target whose spatial positions are unknown but only the vision data values are known. The efficiency of each control scheme is evaluated by comparing the accuracy through the experimental results of each control scheme.

고체 전기활성 고분자 기반 가변 렌즈의 연구동향 (A Review: All Solid-state Electroactive Polymer-based Tunable Lens)

  • 신은재;고현우;김상연
    • 로봇학회논문지
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    • 제16권1호
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    • pp.41-48
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    • 2021
  • In this paper, we review papers which report to the all solid-state electroactive polymer-based tunable lens. Since electroactive polymer-based tunable lenses change their focal length by responding to electric stimuli, it can be minimized the size and weight of optical modules. Thus, it has been received attention in the robot, mobile device and display industry. The all solid-state electroactive polymer-based tunable lenses can be classified into two categories depending on the classification of materials: ionic electroactive polymer-based lenses and non-ionic electroactive polymer-based lenses. Most of the ionic electroactive polymer-based tunable lenses are fabricated with ionic polymer-metal composite. So, the ionic electroactive polymer-based tunable lenses can be operated under low electric voltage. But small force, slow recovery time and environmental limitation for operation has been pointed to the disadvantage of the lenses. The non-ionic electroactive polymer-based tunable lenses are classified again into two categories: dielectric polymer-based tunable lenses and polyvinylchloride gel-based tunable lenses. The advantage of the dielectric polymer-based tunable lenses is fast response to electric stimuli. But the essential flexible electrodes degrade performance of the lens. Polyvinylchloride gel-based tunable lens has reported impressive performance without flexible electrodes.

300-W-class Side-pumped Solar Laser

  • Qi, Hongfei;Lan, Lanling;Liu, Yan;Xiang, Pengfei;Tang, Yulong
    • Current Optics and Photonics
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    • 제6권6호
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    • pp.627-633
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    • 2022
  • To realize uniform side pumping of solar lasers and improve their output power, a solar concentrating system based on off-axis parabolic mirrors is proposed. Four identical off-axis parabolic mirrors with focal length of 1,000 mm are toroidally arranged as the primary concentrator. Four two-dimensional compound parabolic concentrators (2D-CPCs) are designed as a secondary concentrator to further compress the focused spot induced by the parabolic mirrors, and the focused light is then homogenized by four rectangular diffusers and provides uniform pumping for a laser-crystal rod to achieve solar laser emission. Simulation results show that the solar power received by the laser rod, uniformity of the light spot, and output power of the solar laser are 7,872.7 W, 98%, and 351.8 W respectively. This uniform pumping configuration and concentrator design thus provide a new means for developing high-power side-pumped solid-state solar lasers.

혈관용해 레이저를 이용한 후두미세수술 최신 지견 (Update on Angiolytic Laser Laryngeal Surgery)

  • 강민석;임재열
    • 대한후두음성언어의학회지
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    • 제32권2호
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    • pp.51-55
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    • 2021
  • There are several lasers available for office-based or suspension microlaryngoscopy laser procedures in the treatment of laryngeal diseases. Each has advantages and disadvantages given the depth of penetration per unit of power, absorption in water, spectral absorption characteristics, mode of delivery, safety, and cost. It is important to note that while the proper selection of indication of treatment based on a laser wavelength is critical, of equal importance is selecting the appropriate power setting, focal length (or spot size), and time of exposure. The photoangiolytic lasers precisely target hemoglobin within the microcirculation of the highly vascularized tissue and may have better hemostatic effects and preservation of surrounding normal tissue than the CO2 laser. Although the choice of laser is purely theoretical and cannot be accurately concluded which parameters of laser (wattage and pulse width) were best to use, photoangiolytic laser surgery is safe and effective for specific laryngeal lesions. In this review, indications for photoangiolytic laser procedures for various laryngeal diseases, laser settings and surgical techniques for specific laryngeal lesions including sulcus vocalis, laryngeal dysplasia, and recurrent respiratory papillomatosis will be introduced. Pros and cons of in-office laser surgery using photoangiolytic laser and flexible CO2 laser will also be addressed.

고배율 줌 광학계의 상면 오차 보정 방법 (Focus-adjustment Method for a High-magnification Zoom-lens System)

  • 유재명
    • 한국광학회지
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    • 제34권2호
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    • pp.66-71
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    • 2023
  • 줌 렌즈는 이제 휴대폰에도 적용되기 시작했다. 휴대폰에 적용되는 줌 렌즈는 주로 망원 영역을 촬영하기 위해 적용되고 있으며, 이러한 광학계는 고배율 줌 광학계와 유사하게 초점거리가 길어서 부품의 제작 오차에 의한 촬상 소자의 위치도 크게 변한다. 이를 보정하기 위해 기존에는 렌즈군 1군과 광학계 전체를 이동해서 촬상 소자의 위치 변화를 보정했으나, 본 논문에서는 이동하는 렌즈군 2개를 임의로 선택해서 촬상 소자의 위치를 보정할 수 있음을 확인했다. 다만, 이를 위해서는 이동하는 렌즈군 앞쪽과 뒤쪽으로 간격을 더 확보해야 함을 알 수 있었다.

직사각형 금속 슬롯을 활용한 이중대역 신호 집중 위상변화 메타표면 (Rectangular Slot based Beam Focusing Dual-Band Phase Gradient Metasurface)

  • 민경수;김성건;홍익표;이경원;정성훈;이명식;육종관
    • 한국군사과학기술학회지
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    • 제27권5호
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    • pp.558-566
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    • 2024
  • This study proposes method for enhancing the performance of previously developed or produced weapon systems without developing new detection equipment by using Phase Gradient Metasurfaces(PGMS). Metasurface has been studied and utilized a lot to improve the detection performance of inorganic systems, but its utilization is low due to its narrow bandwidth and complex structure. To address some of these limitations, dual-band power focusing PGMS is proposed. Its frequency independent unit cell characteristic enables creating metasurface that concentrates signals in dual-band. The designed PGMS was validated through near-field and far-field measurement, confirming signal concentration at the specified focal length and improved gain in the dual bands.

Design of an Asymmetric-custom-surface Imaging Optical System for Two-dimensional Temperature-field Measurement

  • Guanghai Liu;Ming Gao;Jixiang Zhao;Yang Chen
    • Current Optics and Photonics
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    • 제8권5호
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    • pp.484-492
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    • 2024
  • In response to the difficulty of synchronously obtaining multiwavelength images for fast two-dimensional (2D) temperature measurement, a multispectral framing imaging optical system is designed, based on the segmented-aperture imaging method and asymmetric surface shape. The system adopts a common-aperture four-channel array structure to synchronously collect multiwavelength temperature-field images. To solve the problem of asymmetric aberration caused by being off-axis, a model of the relationship between incident and outgoing rays is established to calculate the asymmetric custom surface. The designed focal length of the optical system is 80 mm, the F-number is 1:3.8, and the operating wavelength range is 0.48-0.65 ㎛. The system is divided into four channels, corresponding to wavelengths of 0.48, 0.55, 0.58, and 0.65 ㎛ respectively. The modulation transfer function value of a single channel lens is higher than 0.6 in the full field of view at 35 lp/mm. The experimental results show that the asymmetric-custom-surface imaging system can capture clear multiwavelength images of a temperature field. The framing imaging system can capture clear images of multiwavelength temperature fields, with high consistency in images of different wavelengths. The designed optical system can provide reliable multiwavelength image data for 2D temperature-field measurement.

광 HDMI 인터페이스용 2채널 광송신기 광학 설계 (Optical Design of an Integrated Two-Channel Optical Transmitter for an HDMI interface)

  • 윤현재;강현서
    • 한국광학회지
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    • 제26권5호
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    • pp.269-274
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    • 2015
  • 본 논문에서는 code V 시뮬레이터를 이용하여 광 HDMI 인터페이스에 적용하기 위한 집적형 2채널 TO 구조 광송신기의 광학계 설계를 하였다. 제안된 집적형 2채널 TO 구조 광송신기는 지름의 6.4 mm인 하나의 8 pin TO-CAN 패키지 안에 2개의 VCSEL을 평행하게 부착하고 그 위에 반구(hemisphere) 렌즈가 부착된 직육면체 모양($1mm(H){\times}2mm(W){\times}4mm(D)$)의 렌즈필터 블록 (lens filter block) 을 올려놓은 구조이다. 집적형 2채널 TO 구조 광송신기 제작 시 1060 nm/1270 nm와 1330 nm/1550 nm로 두 개 파장씩 묶어 TO-CAN 형태로 제작하므로, 이들 파장 조합에서 반구 렌즈의 지름은 0.6 mm, 볼 렌즈와 렌즈 필터 간격(L)은 파장 1060 nm/1270 nm 조합의 경우 1.7 mm, 파장 1330 nm/1550 nm 조합의 경우 2.0 mm일 때 최적의 결과를 얻을 수 있었다. 이때 렌즈필터 블록의 초점거리($f_0$)는 1060 nm, 1270 nm, 1330 nm, 1550 nm 파장에 대하여 0.351 mm, 0.354 mm, 0.355 mm, 0.359 mm이었으며 렌즈 필터 블록과 볼 렌즈를 통과한 빛의 초점 위치(F)는 파장 1060 nm/1270 nm 조합의 경우 0.62 mm, 파장 1330 nm/1550 nm 조합의 경우 0.60 mm ~ 0.66 mm이었다.