Passive Q-switching of diode pumped Nd: KGd(WO4)(2) lasers by V3+: Y3Al5O12 crystal with anisotropy of nonlinear absorption

Vasili G. Savitski; Igor A. Denisov; Alexander M. Malyarevich; Konstantin V. Yumashev; Alexander V. Sandulenko

doi:10.1364/AO.46.005732

Passive Q-switching of diode pumped Nd: KGd(WO4)(2) lasers by V3+: Y3Al5O12 crystal with anisotropy of nonlinear absorption

Vasili G. Savitski, Igor A. Denisov, Alexander M. Malyarevich, Konstantin V. Yumashev, Alexander V. Sandulenko

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6 Citations (Scopus)

Abstract

Use of a V3+:y(3)Al(5)O(12) crystal as a saturable absorber Q-switch for 1.07 and 1.35 mu m Nd:KGd(WO4)(2) diode pumped lasers shows a considerable dependence of output characteristics on the orientation of the intracavity field polarization vector regarding V3+:y(3)Al(5)O(12) crystallographic axes. Anisotropy of nonlinear absorption of V3+ ions in a Y3Al5O12 single crystal at wavelengths of 1.08 and 1.35 mu m has been experimentally studied. The experimental data are analyzed within the framework of a phenomenological model when the V3+ ions are described as three sets of linear dipoles oriented along the crystallographic axes. Ground-state and excited-state absorption cross sections at 1.08 and 1.35 mu m are evaluated to be sigma(gsa) = 3.4 x 10(-18) cm(2), sigma(esa) = 3.0 x 10(-19) cm(2) and sigma(gsa) = 5.4 x 10(-18) cm(2), sigma esa = 4.8 x 10(-19) cm(2), respectively. Saturation fluence and intensity at 1.08 and 1.35 mu m are estimated as 55 mJ/cm(2) and 1.1 MW/cm(2), respectively. (C) 2007 Optical Society of America.

Original language	English
Pages (from-to)	5732-5737
Number of pages	6
Journal	Applied Optics
Volume	46
Issue number	23
DOIs	https://doi.org/10.1364/AO.46.005732
Publication status	Published - 10 Aug 2007

Keywords

Yttrium aluminum garnet
YAG saturable absorber
V-YAG

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Savitski, V. G., Denisov, I. A., Malyarevich, A. M., Yumashev, K. V., & Sandulenko, A. V. (2007). Passive Q-switching of diode pumped Nd: KGd(WO4)(2) lasers by V3+: Y3Al5O12 crystal with anisotropy of nonlinear absorption. Applied Optics, 46(23), 5732-5737. https://doi.org/10.1364/AO.46.005732

@article{8dbacfb418e5405395a43f5a056e8c49,

title = "Passive Q-switching of diode pumped Nd: KGd(WO4)(2) lasers by V3+: Y3Al5O12 crystal with anisotropy of nonlinear absorption",

abstract = "Use of a V3+:y(3)Al(5)O(12) crystal as a saturable absorber Q-switch for 1.07 and 1.35 mu m Nd:KGd(WO4)(2) diode pumped lasers shows a considerable dependence of output characteristics on the orientation of the intracavity field polarization vector regarding V3+:y(3)Al(5)O(12) crystallographic axes. Anisotropy of nonlinear absorption of V3+ ions in a Y3Al5O12 single crystal at wavelengths of 1.08 and 1.35 mu m has been experimentally studied. The experimental data are analyzed within the framework of a phenomenological model when the V3+ ions are described as three sets of linear dipoles oriented along the crystallographic axes. Ground-state and excited-state absorption cross sections at 1.08 and 1.35 mu m are evaluated to be sigma(gsa) = 3.4 x 10(-18) cm(2), sigma(esa) = 3.0 x 10(-19) cm(2) and sigma(gsa) = 5.4 x 10(-18) cm(2), sigma esa = 4.8 x 10(-19) cm(2), respectively. Saturation fluence and intensity at 1.08 and 1.35 mu m are estimated as 55 mJ/cm(2) and 1.1 MW/cm(2), respectively. (C) 2007 Optical Society of America.",

keywords = "Yttrium aluminum garnet, YAG saturable absorber, V-YAG",

author = "Savitski, {Vasili G.} and Denisov, {Igor A.} and Malyarevich, {Alexander M.} and Yumashev, {Konstantin V.} and Sandulenko, {Alexander V.}",

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doi = "10.1364/AO.46.005732",

language = "English",

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journal = "Applied Optics",

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T1 - Passive Q-switching of diode pumped Nd

T2 - KGd(WO4)(2) lasers by V3+: Y3Al5O12 crystal with anisotropy of nonlinear absorption

AU - Savitski, Vasili G.

AU - Denisov, Igor A.

AU - Malyarevich, Alexander M.

AU - Yumashev, Konstantin V.

AU - Sandulenko, Alexander V.

PY - 2007/8/10

Y1 - 2007/8/10

N2 - Use of a V3+:y(3)Al(5)O(12) crystal as a saturable absorber Q-switch for 1.07 and 1.35 mu m Nd:KGd(WO4)(2) diode pumped lasers shows a considerable dependence of output characteristics on the orientation of the intracavity field polarization vector regarding V3+:y(3)Al(5)O(12) crystallographic axes. Anisotropy of nonlinear absorption of V3+ ions in a Y3Al5O12 single crystal at wavelengths of 1.08 and 1.35 mu m has been experimentally studied. The experimental data are analyzed within the framework of a phenomenological model when the V3+ ions are described as three sets of linear dipoles oriented along the crystallographic axes. Ground-state and excited-state absorption cross sections at 1.08 and 1.35 mu m are evaluated to be sigma(gsa) = 3.4 x 10(-18) cm(2), sigma(esa) = 3.0 x 10(-19) cm(2) and sigma(gsa) = 5.4 x 10(-18) cm(2), sigma esa = 4.8 x 10(-19) cm(2), respectively. Saturation fluence and intensity at 1.08 and 1.35 mu m are estimated as 55 mJ/cm(2) and 1.1 MW/cm(2), respectively. (C) 2007 Optical Society of America.

AB - Use of a V3+:y(3)Al(5)O(12) crystal as a saturable absorber Q-switch for 1.07 and 1.35 mu m Nd:KGd(WO4)(2) diode pumped lasers shows a considerable dependence of output characteristics on the orientation of the intracavity field polarization vector regarding V3+:y(3)Al(5)O(12) crystallographic axes. Anisotropy of nonlinear absorption of V3+ ions in a Y3Al5O12 single crystal at wavelengths of 1.08 and 1.35 mu m has been experimentally studied. The experimental data are analyzed within the framework of a phenomenological model when the V3+ ions are described as three sets of linear dipoles oriented along the crystallographic axes. Ground-state and excited-state absorption cross sections at 1.08 and 1.35 mu m are evaluated to be sigma(gsa) = 3.4 x 10(-18) cm(2), sigma(esa) = 3.0 x 10(-19) cm(2) and sigma(gsa) = 5.4 x 10(-18) cm(2), sigma esa = 4.8 x 10(-19) cm(2), respectively. Saturation fluence and intensity at 1.08 and 1.35 mu m are estimated as 55 mJ/cm(2) and 1.1 MW/cm(2), respectively. (C) 2007 Optical Society of America.

KW - Yttrium aluminum garnet

KW - YAG saturable absorber

KW - V-YAG

U2 - 10.1364/AO.46.005732

DO - 10.1364/AO.46.005732

M3 - Article

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SP - 5732

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JO - Applied Optics

JF - Applied Optics

SN - 1559-128X

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