Optical Transitions of Tm3+ Ions for Amplifiers: How the Local Structure Works in (1−x) TeO2+(x) M (where M = LiCI, CdCl2, WO3) Glass

A. Aydinli; F. Ay; A. Sennaroğlu; S. Cenk; G. Özen

Conference on Lasers and Electro-Optics
OSA Technical Digest (Optica Publishing Group, 2002),
paper CTuK55

Optical Transitions of Tm³⁺ Ions for Amplifiers: How the Local Structure Works in (1−x) TeO₂+(x) M (where M = LiCI, CdCl₂, WO₃) Glass

A. Aydinli, F. Ay, A. Sennaroğlu, S. Cenk, and G. Özen

Conference on Lasers and Electro-Optics 2002

Long Beach, California United States
19–22 May 2002
ISBN: 1-55752-706-7

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Poster Session: 1 (CTuK)

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A. Aydinli, F. Ay, A. Sennaroğlu, S. Cenk, and G. Özen, "Optical Transitions of Tm3+ Ions for Amplifiers: How the Local Structure Works in (1−x) TeO2+(x) M (where M = LiCI, CdCl2, WO3) Glass," in Conference on Lasers and Electro-Optics, M. Fejer, F. Leonberger, J. Fujimoto, and S. Newton, eds., OSA Technical Digest (Optica Publishing Group, 2002), paper CTuK55.

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Abstract

Tm³⁺ doped glass is one of the most studied systems towards the achievement of compact blue upconversion lasers as well as fiber amplifiers in the telecommunication networks both at 1.5 μm and 1.8 μm due to its radiative emissions at 470 nm, 1.45 μm and 1.8 μm.^1,2 These emissions corresponds to the ¹G₄ ≥ ³H₆, ³f₄ ≥ ³H₄ and, ³H₄ ≥ ³h₆, transitions upon excitation into either ³F₃ or ³F₄ levels, respectively.

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