Solid-state, Nd:YAG laser-based source at 580 nm

H. M. Pask; J. A. Piper

Solid-state, Nd:YAG laser-based source at 580 nm

H. M. Pask^*, J. A. Piper

^*Corresponding author for this work

Research output: Contribution to journal › Article › peer-review

2 Citations (Scopus)

Abstract

An experiment was carried out utilizing an arclamp-pumped Quantronix 114 Nd:YAG laser as the initial pump source. The solid-state Nd:YAG laser was Q-switched at repetition rates from 1-100 kHz. The resonator was modified using intracavity configuration to study the stimulated Raman scattering (SRS) and second-harmonic generation (SHG) in the laser. Intracavity SRS was found to be a function of lamp current, pulse repetition frequency, and output coupling. On the other hand, the Raman shift and threshold were dependent on crystal length, cut, and orientation relative to the pump polarization.

Original language	English
Pages (from-to)	88
Number of pages	1
Journal	Conference Proceedings - Lasers and Electro-Optics Society Annual Meeting-LEOS
Volume	11
Publication status	Published - 1997

Cite this

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abstract = "An experiment was carried out utilizing an arclamp-pumped Quantronix 114 Nd:YAG laser as the initial pump source. The solid-state Nd:YAG laser was Q-switched at repetition rates from 1-100 kHz. The resonator was modified using intracavity configuration to study the stimulated Raman scattering (SRS) and second-harmonic generation (SHG) in the laser. Intracavity SRS was found to be a function of lamp current, pulse repetition frequency, and output coupling. On the other hand, the Raman shift and threshold were dependent on crystal length, cut, and orientation relative to the pump polarization.",

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AU - Pask, H. M.

AU - Piper, J. A.

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N2 - An experiment was carried out utilizing an arclamp-pumped Quantronix 114 Nd:YAG laser as the initial pump source. The solid-state Nd:YAG laser was Q-switched at repetition rates from 1-100 kHz. The resonator was modified using intracavity configuration to study the stimulated Raman scattering (SRS) and second-harmonic generation (SHG) in the laser. Intracavity SRS was found to be a function of lamp current, pulse repetition frequency, and output coupling. On the other hand, the Raman shift and threshold were dependent on crystal length, cut, and orientation relative to the pump polarization.

AB - An experiment was carried out utilizing an arclamp-pumped Quantronix 114 Nd:YAG laser as the initial pump source. The solid-state Nd:YAG laser was Q-switched at repetition rates from 1-100 kHz. The resonator was modified using intracavity configuration to study the stimulated Raman scattering (SRS) and second-harmonic generation (SHG) in the laser. Intracavity SRS was found to be a function of lamp current, pulse repetition frequency, and output coupling. On the other hand, the Raman shift and threshold were dependent on crystal length, cut, and orientation relative to the pump polarization.

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M3 - Article

AN - SCOPUS:0030710020

VL - 11

SP - 88

JO - Conference Proceedings - Lasers and Electro-Optics Society Annual Meeting-LEOS

JF - Conference Proceedings - Lasers and Electro-Optics Society Annual Meeting-LEOS

SN - 1092-8081

ER -

Solid-state, Nd:YAG laser-based source at 580 nm

Abstract

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