• Title/Summary/Keyword: diode laser

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An Equaivalent Circuit Model for Rquantum Well Laser Diodes (양자우물 레이저 다이오드의 등가회로 모델)

  • 이승우;김대욱;최우영
    • Journal of the Korean Institute of Telematics and Electronics D
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    • v.35D no.1
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    • pp.49-58
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    • 1998
  • In this paper, a new equivalent circuit model for quantum-well laser diode (LD) is proposed. The model includes carrier transport effects in the SCH region, and rprovides, in a stable and accurate manner, large-and small-signal responses of laser diode output power as function of injected currents. SPICE simulation was performed using the circuit model and results are presented for L-I characteristics, pulse and frequency responses under various conditions. It is expencted that the new equaivalent circuit model will find useful applications for designing and analyzing OEIC, LD driver circuits, and LD packaging.

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Novel velocity detection of moving object with rough surface vertically illuminated by self-mixing laser diode

  • Shibata, Takaaki;Shinohara, Shigenobu;Ikeda, Hiroaki;Yoshida, Hirofumi;Sumi, Masao
    • 제어로봇시스템학회:학술대회논문집
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    • 1994.10a
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    • pp.494-497
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    • 1994
  • We propose a novel velocity detection method of moving object based on a speckle pattern on the target surface using a self-mixing laser diode (SMLD). By this measurement, it was confirmed that the speckle signal has its waveform independent of the target velocity, and has its averaged frequency directly proportional to the target velocity. So it will be possible to detect the velocity of the target transversely translating against the laser light beam using a compact measuring system.

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Optical modulation characteristics of resonant tunneling diode oscillator (빛에 의한 공명투과다이오드 진동자의 주파수 변조 특성)

  • 추혜용;이일희
    • Journal of the Korean Institute of Telematics and Electronics A
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    • v.33A no.10
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    • pp.139-143
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    • 1996
  • We report on the static and dynamic characteristics of optically modulated resonant tunneling diode oscillator (RTDO) formed in double-barrier quantum-well structure. Under the illumination of Ti:Sapphire laser, the dc current-voltage (I-V) curves of RTDO shifted towared lower voltages. This characteristic was found to odify the series resistance, negtive differential resistance, capacitance, and the inductance of the RTDO. As a result, the resonant frequency of TRDO centered at 5.302 GHz was found to decrease about 20 MHz under the laser illumination. At a constnat bias voltage, the oscillation frequency decreased linearly as the laser power was increased.

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Second Harmonic Generation and Frequency Stabilization of a Diode Laser Using an External Ring Resonator

  • Kwon, Taeg-Yong;Yang, Sung-Hoon;Lee, Ho-Seong
    • Journal of the Optical Society of Korea
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    • v.2 no.1
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    • pp.1-4
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    • 1998
  • The second harmonic light of an 842 nm diode laser was generated from a KNbO3 crystal in an external ring resonator. The power of the second harmonic light was about 0.8 mV at an input fundamental power of 87 mW. The laser frequency was stabilized to the resonance frequency of the ring resonator, and the frequency fluctuation was measured as about 3 MHz.

A study on the hard surfacing Characteristics of SM45C by using Diode laser (다이오드 레이저를 이용한 SM45C의 표면경화 특성에 관한 연구)

  • Lim, Byung-Chul;Lee, Hong-Sub;Park, Sang-Heup
    • Journal of the Korea Academia-Industrial cooperation Society
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    • v.16 no.3
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    • pp.1620-1625
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    • 2015
  • In this study, a variety of industrial gears, shafts, chains, rollers, mold, etc. are widely used inautomotive steel carbon steel for machine structural SM45C typical material used for the experiments. In order to cure the surface of the test piece after the rough grinding and fine grinding was performed in order polishing. Perform the surface hardening of SM45C lacal area by using a diode laser. The output of the laser diode and the feed rate to the process variable. Micro-hardness testing, microstructure testing, scanning electron microscope testing(SEM), the heat input to the analysis. After analyzing the experiment to compare the mechanical properties of the material. When using a diode laser to assess the soundness of the surface hardening. Accordingly, the process for deriving the optimum demonstrate the feasibility.

The Effect of Dentin Desensitization Treatment on the Shear Bond Strength of Luting Cements (상아질 지각과민 완화법이 접착용 시멘트의 전단결합강도에 미치는 영향)

  • Park, In-Ho;Lee, Joon-Soek;Cho, In-Ho
    • Journal of Dental Rehabilitation and Applied Science
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    • v.22 no.3
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    • pp.231-242
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    • 2006
  • Statement of problem: The sealing of the opened dentinal tubules that follows the tooth preparation for the prosthodontic restoration is considered as clinical process to reduce postoperative sensitivity. Purpose: This study investigated the effect of desensitization treatment on shear bond strength of luting cements. Materials and Method: Total 80 dentin specimens were divided into two groups according to the kinds of luting cements. Each groups was further divided into 4 subgroups with AQ $bond^{(R)}$, $Saforide^{(R)}$, Diode laser $MDL-10^{(R)}$ application and without desensitization treatment. After desensitization treatment application, Ni-Cr specimens were luted to dentin surface with Fuji $CEM^{(R)}$ and $Panavia-F^{(R)}$. Specimens were placed in distilled water at $37^{\circ}C$ for 24 hours and shear bond strength between metal and dentin was measured by a universal testing machine. Results: 1. In Fuji $CEM^{(R)}$ cemented groups, the combination of AQ $bond^{(R)}$ showed the greatest strength, followed by diode laser, no desensitizer treatment, and $Saforide^{(R)}$. Both AQ $bond^{(R)}$ and Diode laser groups had a significant difference than no desensitization treatment group and $Saforide^{(R)}$ group(p<0.05). 2. In $Panavia-F^{(R)}$ cemented groups, the combination of Diode laser showed the greatest strength, followed by AQ $bond^{(R)}$, $Saforide^{(R)}$, and No desensitization treatment. All desensitization treatment groups had a significant difference than no desensitization treatment group(p<0.05). 3. All $Panavia-F^{(R)}$ groups showed a significant higher shear bond strength than all Fuji $CEM^{(R)}$ groups(p<0.05). Conclusion: The results of this study showed possibility of bond strength increase after desensitization treatment. The application of desensitization treatments like AQ $bond^{(R)}$, $Saforide^{(R)}$, and Diode laser $MDL-10^{(R)}$ have advantages in exposed dentin surface after tooth prep.

Characteristics of the laser brazing on AZ31 magnesium alloy and Zn coated steel dissimilar joint (AZ31 마그네슘합금과 아연도금강판 이종소재의 레이저 브레이징 특성)

  • Lee, Mok-Young;Kim, Sook-Whan;NASIRI, ALI M.;ZHOU, NORMAN Y.
    • Laser Solutions
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    • v.17 no.1
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    • pp.7-12
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    • 2014
  • The dissimilar welding between magnesium alloy and steel sheet was required in automobile industry to increase the strength of the dissimilar joints. Laser brazing is one of the good joining processes for Mg- steel dissimilar joint. In this study, AZ31 magnesium alloy and Zn coated steel dissimilar joint was brazed using diode direct laser with Mg600 filler wire and Superior #21 flux. The wetting of Mg filler wire on Zn coating was very good because of the formation of eutectic phase with low melting temperature. The strength of the brazed joint between AZ31 magnesium alloy and Zn coated steel was 131.3N/mm. The fracture occurred at brazement.

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Implementation of the Variable Output Laser Diode Driver Synchronized with a Pulse Repetition Frequency Code (펄스 반복 주파수 코드에 동기된 출력 가변형 레이저 다이오드 드라이버 구현)

  • Lee, Young-Ju;Kim, Yong-Pyung
    • The Transactions of The Korean Institute of Electrical Engineers
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    • v.64 no.5
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    • pp.746-750
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    • 2015
  • In this paper, we propose a simulator to evaluate the performance of the semi-active laser guidance or the quadrant photodetector and to simulate the laser power reflected from a target. The laser pulse repetition frequency was generated and synchronized with the laser pulse repetition(PRF) code. To evaluate the performances of the proposed methods, we implemented a prototype system and performed experiments. As a result, the generated high voltage was variable in the range of DC 3V to 340V and has the rate of change of 2000 V/s. PRF code can be generated within 50ms ∼ 100ms and the error is implemented within 0.3ns. The laser output is synchronized with the PRF code and has a dynamic range of 23.6dB.