• Title/Summary/Keyword: Line Laser

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Tunable Photonic Microwave Delay Line Filter Based on Fabry-Perot Laser Diode

  • Heo, Sang-Hu;Kim, Junsu;Lee, Chung Ghiu;Park, Chang-Soo
    • Current Optics and Photonics
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    • v.2 no.1
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    • pp.27-33
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    • 2018
  • We report the physical implementation of a tunable photonic microwave delay line filter based on injection locking of a single Fabry-Perot laser diode (FP-LD) to a reflective semiconductor optical amplifier (RSOA). The laser generates equally spaced multiple wavelengths and a single tapped-delay line can be obtained with a dispersive single mode fiber. The filter frequency response depends on the wavelength spacing and can be tuned by the temperature of the FP-LD varying lasing wavelength. For amplitude control of the wavelengths, we use gain saturation of the RSOA and the offset between the peak wavelengths of the FP-LD and the RSOA to decrease the amplitude difference in the wavelengths. From the temperature change of total $15^{\circ}C$, the filter, consisting of four flat wavelengths and two wavelengths with slightly lower amplitudes on both sides, has shown tunability of about 390 MHz.

A Study on Segmentation of Building Points Utilizing Scan-line Characteristic of Airborne Laser Scanner (항공레이저측량 자료의 스캔라인 특성을 활용한 건물 포인트 분리에 관한 연구)

  • Han, Su-Hee;Lee, Jeong-Ho;Yu, Ki-Yun;Kim, Yong-Il;Lee, Byung-Kil
    • Journal of Korean Society for Geospatial Information Science
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    • v.13 no.4 s.34
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    • pp.33-38
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    • 2005
  • The goal of this study is to segment building points effectively utilizing scan-line characteristics of airborne laser scanner. Points are classified as to their altitude similarity and adjacency with other classified points, and point searching range for the classification is restricted within some number of scan-lines, preventing classification speed from lowering as the process goes on. Besides, we detected wrong discrimination of one object into more than two classes, then integrated them into a single class. Consequently we could discriminate points of each building from others, its annexes and none building points simultaneously.

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Synthesis of an On-Line 5 Degrees of Freedom Error Measurement System for Translational Motion Rigid Bodies (병진운동 강체의 온라인 5자유도 운동오차 측정시스템 설계 및 해석)

  • 김진상;정성종
    • Journal of the Korean Society for Precision Engineering
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    • v.15 no.5
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    • pp.93-99
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    • 1998
  • Although laser interferometer measurement system has advantages of measurement range and accuracy, it has some disadvantages when measurement of multi degrees of freedom of motion are required. Because the traditional error measurement methods for geometric errors (two straightness and three angular errors) of a slide of machine tools measures error components one at a time. It may also create an optical path difference and affect the measurement accuracy. In order to identify and compensate for geometric errors of a moving rigid body in real time processes, an on-line error measurement system for simultaneous detection of the five error components of a moving object is required. Using laser alignment technique and some optoelectronic components, an on-line measurement system with 5 degrees of freedom was developed for the geometric error detection in this study Performance verification of the system has been performed on an error generating mechanism. Experimental results show the feasibility of this system for identifying geometric errors of a slide of machine tools.

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Compensations of Polarization Mode Dispersion and Thermal Drift in Optical Coherence Tomography with PZT Optical Delay Lines (광간섭 단층촬영(OCT)용 PZT 광경로 지연기에서의 편광모드 분산 및 열요동 보상)

  • Kim, Young-Kwan;Park, Sung-Jin;Kim, Yong-Pyung
    • Korean Journal of Optics and Photonics
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    • v.16 no.6
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    • pp.547-552
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    • 2005
  • We have fabricated and characterized optical delay lines for optical coherence tomography, which is composed of cylindrical PZT(piezoelectric transducer) and single mode optical fiber. The polarization mode dispersion from the optical delay lines was compensated by the polarization controllers. By applying the duplex optical delay line, we minimized the thermal drift due to optical delay lines and obtained the scan range of 2 times that of a single optical delay line. The OCT system showed resolution of $18.6\pm0.5{\mu}m$, scanning range of 1.68mm, and scanning speed of 360.4mm/s.

Fabrication of an On System based on an Optical Delay line with Cylindrical PZT (실린더형 압전소자 광지연선을 이용한 광 간섭형 단층촬영(OCT) 시스템 제작)

  • Park, Sung-Jin;Kim, Young-Kwan;Kim, Yong-Pyung
    • Korean Journal of Optics and Photonics
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    • v.17 no.2
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    • pp.159-164
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    • 2006
  • We demonstrate a compact optical coherence tomography(OCT) system based on the optical fiber delay line controlled by a cylindrical piezo-electric transducer(PZT). An 18-m length of single mode fiber is wrapped under constant tension around a PZT. Approximately 134 windings are used. Wraps of the long length of fiber allow the small expansion of the PZT to be magnified to an optical path length delay of 0.78 m. The OCT system shows characteristics for 2-dimensional imaging, exhibiting 96.9dB of signal-to-noise ratio(SNR), $18.6{\pm}0.5\;{\mu}m$ of axial resolution, and $5\;{\mu}m$ of lateral resolution with samples.

Astigmatically compensated cw Ti:Sapphire laser pumped by $Ar^+$ laser (비점수차가 보상된 $Ar^+$ 레이저로 펌핑하는 cw Ti:Sapphire 레이저)

  • Yoon, Tai-Hyun;Kim, Gyu-Ug;Jo, Jae-Heung;Won, Jong-Wook
    • Proceedings of the KIEE Conference
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    • 1990.07a
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    • pp.451-454
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    • 1990
  • Room temperature cw operations of a standing wave and a unidirectional Ti:Sapphire laser pumped by a $Ar^+$ laser have been demonstrated in the same pumping cavity configuration. Laser emission at 790 nm was excited with all-line $Ar^+$ laser pump for both cavities. The maximum output power was found to be 600 mW in the standing wave cavity and 210 mW in the ring cavity. Values of (83 ${\pm}$ 10) % for the internal quantum efficiency and (3.0 ${\pm}$ 0.5) % for the round-trip cavity loss for standing wave cavity are obtained from the thresholds and slope efficiencies measured with 2.4 and 11.2 % optput couplers. The measured cavity-loss value at 790 nm gives a meterial figure of merit (FOM) to be 146. Unidirectional operation of the ring Ti:Sapphire laser will be discussed.

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T-joint Laser Welding of Circular and Square Pipes Using the Vision Tracking System (용접선 추적 비전장치를 이용한 원형-사각 파이프의 T형 조인트 레이저용접)

  • Son, Yeong-Il;Park, Gi-Yeong;Lee, Gyeong-Don
    • Laser Solutions
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    • v.12 no.1
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    • pp.19-24
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    • 2009
  • Because of its fast and precise welding performance, laser welding is becoming a new excellent welding method. However, the precise focusing and robust seam tracking are required to apply laser welding to the practical fields. In order to laser weld a type of T joint like a circular pipe on a square pipe, which could be met in the three dimensional structure such as an aluminum space frame, a visual sensor system was developed for automation of focusing and seam tracking. The developed sensor system consists of a digital CCD camera, a structured laser, and a vision processor. It is moved and positioned by a 2-axis motorized stage, which is attached to a 6 axis robot manipulator with a laser welding head. After stripe-type structured laser illuminates a target surface, images are captured through the digital CCD camera. From the image, seam error and defocusing error are calculated using image processing algorithms which includes efficient techniques handling continuously changed image patterns. These errors are corrected by the stage off-line during welding or teaching. Laser welding of a circular pipe on a square pipe was successful with the vision tracking system by reducing the path positioning and de focusing errors due to the robot teaching or a geometrical variation of specimens and jig holding.

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Tailoring Surface Properties of Polyimides by Laser Direct Patterning (레이저 직접 패터닝에 의한 폴리이미드의 표면 특성 제어)

  • Yun Chan Hwang;Jeong Min Sohn;Jae Hui Park;Ki-Ho Nam
    • Textile Coloration and Finishing
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    • v.35 no.2
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    • pp.121-127
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    • 2023
  • In this study, a comprehensive investigation was conducted on the morphological and property changes of laser-induced nanocarbon (LINC) as a function of laser process parameters. LINC was formed on the surfaces of polyimide films with different backbone structures under various process conditions, including laser power, scan speed, and resolution. Three different forms of LINC electrodes (i.e., continuous 3D porous graphene, wooly nanocarbon fibers, line cut) were formed depending on the laser power and scan speed. Furthermore, heteroatom doping induced from the chemical structure of the polyimide during laser patterning was found to be effective in modifying the electrical properties of LINC electrodes. The LINC surfaces exhibited different microstructures depending on the laser beam resolution under constant laser power and scan speed, allowing for controllable surface wettability. The correlation between the chemical structure of the polymer substrate, laser process parameters, and carbonized surface properties in this study is expected to be utilized as fundamental understanding for the manufacturing of next-generation carbon-based electronic devices.

Observation of the Preionization effect and Operational Characteristics of a Nitrogen Laser by a Pulse type high Voltage Power Supply (펄스형 고전압 전원에 의한 선전리 현상의 관측과 질소레이저의 동작 특성)

  • Lee, Bong-Yeon
    • Korean Journal of Optics and Photonics
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    • v.17 no.1
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    • pp.60-67
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    • 2006
  • We constructed a TEA $N_2$ laser which consists of spark gap, pulse type high voltage power supply, Blumlein transmission line circuit, laser tube with Ernst electrode. We observed the self-preionization with an optical fiber in the spark gap and laser tube. The higher voltage power supplied to the Blumlein transmission line circuit, the better preionization was. An U-type transformer yielded better stability and output power than an I-type transformer. The discharge time after triggering a spark gap for the U-type transformer was also short. We obtained the stability of $2.7\%$ and output power of $36{\mu}J$ when the optimum conditions of the laser operation were spark gap distance of 6.0 mm, electrode distance in laser tube of 5.0 mm, $N_2$ gas flow rate in spark gap of 1500 cc/min, $N_2$ gas flow rate in laser tube of 4 ${\iota}$/min, output window reflectivity of $40\%$ and repetition rate of 10 Hz.