Codoped materials for high power fiber lasers: diffusion behaviour and optical properties

Optical fibers for high power lasers and amplifiers are fabricated on the basis of quartz glass which has outstanding properties concerning high fiber strength, high power hardness and low optical losses compared with other glasses such as heavy metal fluoride or oxide glasses. It is well known, however, that the host properties of pure silica regarding the active rare earth ions are insufficient and the laser medium has to be improved by the incorporation of codopants. Here we present new investigations of material and fiber properties for phosphorus/aluminium codoping, with regard to the realization of efficient rare earth doped cw and pulsed high power fiber devices. The diffusion behaviour in the complex systems shows characteristic interaction effects, which influence the dopant concentration and their spatial distribution. The refractive index in the codoped systems and the basic attenuation deviate remarkably from additivity relations. The absorption spectrum in the VIS/NIR region depends on codopant concentration and on preparation conditions, with influence on the fluorescence properties of the rare earths and the laser efficiency.

[1]  David N. Payne,et al.  Role of Aluminum in Ytterbium–Erbium Codoped Phosphoaluminosilicate Optical Fibers , 1996 .

[2]  J. Broeng,et al.  Large-Mode-Area Erbium-Ytterbium-doped Photonic-Crystal Fiber Amplifier yielding 54-kW Femtosecond Pulses without Chirped-Pulse Amplification , 2005, 2005 Pacific Rim Conference on Lasers & Electro-Optics.

[3]  Johannes Kirchhof,et al.  Diffusion of phosphorus doped silica for active optical fibers , 2004 .

[4]  Johan Nilsson,et al.  High-energy in-fiber pulse amplification for coherent lidar applications. , 2004, Optics letters.

[5]  Johannes Kirchhof,et al.  Dopant interactions in high-power laser fibers , 2005, SPIE OPTO.

[6]  Eugeni M. Dianov,et al.  Phosphosilicate-core single-mode fibers intended for use as active medium of Raman lasers and amplifiers , 2001, SPIE Optics East.

[7]  Johannes Kirchhof,et al.  Fiber lasers: materials, structures and technologies , 2003, SPIE BiOS.

[8]  Rustum Roy,et al.  Revised Phase Diagram for the System Al2O3—SiO2 , 1962 .

[9]  David N. Payne,et al.  Fabrication and characterization of Yb/sup 3+/:Er/sup 3+/ phosphosilicate fibers for lasers , 1998 .

[10]  Johannes Kirchhof,et al.  Spatial distribution effects and laser efficiency in Er/Yb-doped fibers , 2004, SPIE OPTO.

[11]  Jay R. Simpson,et al.  Raman and NMR spectroscopy of SiO2 glasses CO-doped with Al2O3 and P2O5 , 1988 .

[12]  D. J. DiGiovanni,et al.  Structure and properties of silica containing aluminum and phosphorus near the AlPO4 join , 1989 .

[13]  Akira Shirakawa,et al.  Large-mode-area erbium-ytterbium-doped photonic-crystal fiber amplifier for high-energy femtosecond pulses at 1.55 microm. , 2005, Optics express.

[14]  J. Kobelke,et al.  Materials and technologies for microstructured high power laser fibers , 2005, SPIE Optics + Optoelectronics.

[15]  G. G. Stokes "J." , 1890, The New Yale Book of Quotations.

[16]  Eugeni M. Dianov,et al.  Fabrication and investigation of single-mode highly phosphorus-doped fibers for Raman lasers , 2000, Other Conferences.

[17]  U. Röpke,et al.  Preform index profiling with high spatial resolution , 1981 .

[18]  J. Kirchhof,et al.  Er-Yb-doped LMA fiber structures for high energy amplification of narrow linewidth pulses at 1.5μm , 2007, 2007 Conference on Lasers and Electro-Optics (CLEO).

[19]  J K Sahu,et al.  Highly efficient Er,Yb-doped fiber laser with 188W free-running and > 100W tunable output power. , 2005, Optics express.