Nanocrystalline Ceramic Phosphors for High-Power Lasers Operating at 2μm

Rare-earth (RE) doped silica glass optical fibers became a hearth of modern fiber-lasers. Such lasers are fully competitive with conventional solid-state lasers because of their high brightness, high quality beam, high conversion efficiency, good thermal management, tunability, compactness, size and even flexibility. However, a low solubility of RE inside a silica matrix and a high phonon energy of silica glass strongly reduce the luminescence efficiency of incorporated RE elements. Nanoparticle doping represents a powerful method that can eliminate these disadvantages.In this contribution we present an effect of the processing temperature on the luminescence properties of nanocrystalline (Eu<inf>0.05</inf>Y<inf>0.95</inf>)<inf>2</inf>Ti<inf>2</inf>O<inf>7</inf> and (Ho<inf>0.05</inf>Y<inf>0.95</inf>)<inf>2</inf>Ti<inf>2</inf>O<inf>7</inf> phosphors. The luminescence properties of (Ho<inf>0.05</inf>Y<inf>0.95</inf>)<inf>2</inf>Ti<inf>2</inf>O<inf>7</inf> improved with increasing nanocrystal size. The nanocrystals of (Ho<inf>0.05</inf>Y<inf>0.95</inf>)<inf>2</inf>Ti<inf>2</inf>O<inf>7</inf> were successfully incorporated into optical fiber with the outer diameter 125 μm and the core diameter 8 μm. The fiber’s numerical aperture was 0.13 and the background losses at 850 nm were 0.38 dB•m<sup>−1</sup>.The lifetime of the <sup>5</sup>I<inf>7</inf> →<sup>5</sup>I<inf>8</inf> transition at 1.92 μm was 0.72 ± 0.01 ms. The results bring the fundamental information about the effect of the nanocrystal size their luminescence properties of (RE<inf>0.05</inf>Y<inf>0.95</inf>)<inf>2</inf>Ti<inf>2</inf>O<inf>7</inf> and their possible application as phosphors in active optical fibers.

[1]  Pavel Peterka,et al.  Sol-gel route to highly transparent (Ho0.05Y0.95)2Ti2O7 thin films for active optical components operating at 2 μm , 2018 .

[2]  Anirban Dhar,et al.  The mechanism of rare earth incorporation in solution doping process. , 2008, Optics express.

[3]  John Ballato,et al.  Use of thulium-doped LaF 3 nanoparticles to lower the phonon energy of the thulium's environment in silica-based optical fibres , 2017 .

[4]  G. Blasse,et al.  Luminescence and energy transfer in a highly symmetrical system: Eu2Ti2O7 , 1986 .

[5]  Wilfried Blanc,et al.  Fabrication of Rare Earth‐Doped Transparent Glass Ceramic Optical Fibers by Modified Chemical Vapor Deposition , 2011, 1108.3195.

[6]  S. Jackson Towards high-power mid-infrared emission from a fibre laser , 2012, Nature Photonics.

[7]  Kaharudin Dimyati,et al.  An overview on S-band erbium-doped fiber amplifiers , 2006 .

[8]  Simon A. T. Redfern,et al.  Characterisation of the (Y1−xLax)2Ti2O7 system by powder diffraction and nuclear magnetic resonance methods , 2006 .

[9]  Pavel Peterka,et al.  Erbium and Al2O3 nanocrystals-doped silica optical fibers , 2014 .

[10]  Pavel Peterka,et al.  Silica Optical Fibers Doped with Nanoparticles for Fiber Lasers and Broadband Sources , 2016 .

[11]  Michel Langlet,et al.  Up-conversion emission in rare earth-doped Y2Ti2O7 sol–gel thin films , 2005 .

[12]  Snejana Bakardjieva,et al.  Luminescence properties of nanocrystalline europium titanate Eu2Ti2O7 , 2015 .