• Title/Summary/Keyword: Nd:YAG

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Effect of Temperature Gradient on the Defects of Nd;YAG Single Crystal Grown by Czochralski Method (융액인상법에 의한 Nd;YAG 단결정 성장시 온도구배의 변화에 따른 결함거동)

  • 김한태;배소익;이상호;정수진
    • Journal of the Korean Ceramic Society
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    • v.34 no.10
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    • pp.1015-1020
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    • 1997
  • In the Nd;YAG crystal growth by Czochralski method, the relationship between the core formation and the solid-liquid interface was observed by controlling the temperature gradient in the furnace. When the crystal was grown along<111> direction, defects and core area were reduced as the temperature gradient increased. The optimum temperature gradient was found to be higher than 4$0^{\circ}C$/cm. The Nd3+ concentration analysis by ICP-Mass showed that the segregation coefficient was about 20% higher in the core region than core-free region, where the segregation coefficients of core region and core-free region were 0.22 and 0.18, respectively.

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Automatic Diameter Control System for Single Crystal Growth by Czochralski Method; Growth of Nd:YAG Single Crystal (Czochralski법에 의한 단결정 자동직경 제어시스템 개발;Nd:YAG 단결정 성장)

  • Bae, So-Ik;Lee, Sang-Ho;Kim, Han-Tae
    • Korean Journal of Crystallography
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    • v.7 no.1
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    • pp.1-7
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    • 1996
  • We developed an automatic diameter control system to control the diameter of single crystal for Czochralski growth. The system is composed of load cell, software program and data acquisition system connected to computer which controls RF power. This study describes the basic principle, characteristics and components of the system. The diameter of Nd:YAG crystal could be controlled within ±5% tolerance by this system.

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Nd:YAG 레이저 제작 및 응용 기술

  • 김희제;문덕쇠;이홍식
    • 전기의세계
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    • v.42 no.3
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    • pp.19-27
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    • 1993
  • 본고에서는 Nd:YAG 레이저의 구조 및 특성에 대하여 설명한 뒤 그 제작 및 응용기술에 대한 이해를 돕고자 한다. 제2장에서는 일반적으로 레이저에 대하여 잘 모르는 사람이 이해하기 쉽도록 발전원리에 대하여 간략하게 기술한 후, YAG 레이저의 구조 및 특징에 대하여 간략하게 기술하고 YAG레이저의 구조 및 특징에 대하여 설명하고자 한다. 제3장에서는 전기연구소에서 수행한 YAG 레이저의 설계 및 제작기술, 그리고 연구결과에 대하여 간략히 설명하고 제4장에서는 그 응용기술에 대하여 설명한다. 제5장은 본고에서 기술한 내용을 정리함과 동시에 금후의 발전방향에 대하여 이야기 하고자 한다.

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Stabilization of Output Pulses from a Passively Q-switched Nd:YVO4 Laser Pumped by a Continuous-wave Laser Diode (연속 발진 다이오드 레이저로 여기된 수동형 Q-스위치 Nd:YVO4 레이저의 출력 펄스 안정화)

  • Ahn, Seung-In;Park, Yune-Bae;Yeo, Hwan-Seop;Lee, Joon-Ho;Lee, Kang-In;Yi, Jong-Hoon
    • Korean Journal of Optics and Photonics
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    • v.20 no.5
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    • pp.276-280
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    • 2009
  • A Cr:YAG crystal was used as a saturable absorber for passive Q-switching of a Nd:$YVO_4$ laser which was pumped by a 1-W continuous wave laser diode. The first surface of the Cr:YAG was high-reflection coated for the pump wavelength. The high-reflection coating improved the absorption efficiency of the pump beam in the Nd:$YVO_4$ through double pass absorption. It also prevented pump beam induced partial bleaching of the Cr:YAG. The peak-to-peak pulse fluctuation of passively Q-switched laser output was approximately 4 %. The minimum pulse-width was measured to be 7.11 ns. Also, the average pulse repetition rate was 9 kHz and the maximum output power was 16.27 mW.

Formation of PDP cell structure using Nd:YAG laser beam (Nd:YAG 레이저빔에 의한 PDP 방전셀의 구조 형성)

  • Ahn, Min-Young;Lee, Kyoung-Cheol;Lee, Hong-Kyu;Lee, Cheon
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2000.04a
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    • pp.129-132
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    • 2000
  • The PDP(Plasma Display Panel) barrier rib material on the glass substrate was patterned for fabrication of the PDP cell using Nd:YAG laser(1064 nm) which can generate the second(532 nm) and forth(266 nm) harmonic wave by HGM(harmonic generation modules). At a scan speed of 20 ${\mu}m/s$ with the second harmonic wave(532 nm) of Nd:YAG laser, the etching threshold laser fluence of the PDP material was 6.5 $mJ/cm^2$ and a sample(thickness = 180 ${\mu}m$) on the glass substrate was removed clearly at a laser fluence of 19.5 $mJ/cm^2$. In order to increase the throughput of the fabrication we divided a single-beam into multi-beams by using a metal mask between the sample and the focusing lens. As a result, 10 lines of PDP cell were formed by one laser beam scanning at a scan speed of 200 ${\mu}m/s$ and a laser fluence of 2.86 $J/cm^2$.

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Comparison of Welding Characteristics of Austenitic 304 Stainless Steel and SM45C Using a Continuous Wave Nd:YAG Laser (오스테나이트계 스테인리스강과 SM45C의 연속파형 Nd:YAG 레이저 용접특성비교)

  • 유영태;오용석;노경보;임기건
    • Transactions of the Korean Society of Machine Tool Engineers
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    • v.12 no.3
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    • pp.58-67
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    • 2003
  • Welding characteristics of austienite 304 stainless and SM45C using a continuous wave Nd:YAG laser n experimentally investigated Laser beam welding is increasingly being used in welding of structural steels. The laser welding process is one of the most advanced manufacturing technologies owing to its high speed and deep penetration. The thermal cycles associated with laser welding are generally much Inter than those involved in conventional welding processes, leading to a rather small weld zone. Experiments are performed for 304 stainless steel plates changing several process parameter such as laser power, welding speed, shielding gas flow rate, presence of surface pollution, with fixed or variable gap and misalignment between the similar and dissimilar and plates, etc. The Nd:YAG laser welding process is one of the most advanced manufacturing technologies owing to its high speed and penetration. This paper describes the weld ability of SM45C carbon steel for machine structural use by Nd:YAG laser. The follow conclusions can be drawn that laser power and welding speed have a pronounced effect on size and shape of the fusion zone. Increase in welding speed resulted in an increase in weld depth/aspect ratio and hence a decrease in the fusion zone size. The penetration depth increased with the increase in laser power.