Analysis of Ultra-Broadband Amplified Spontaneous Emissions Generated by ${\rm Cr}^{4+}{:}{\rm YAG}$ Single and Glass-Clad Crystal Fibers

Numerical analysis and experimental verification of the ultra-broadband amplified spontaneous emissions (ASEs) generated by Cr4+:YAG crystal fibers are presented. Milliwatt ASE was obtained from a double-clad 25-mum-core fiber. Results of the experimental ASE power measurements and the composition analysis using electron probe micro-analyzer were used to determine the absorption, emission, and excited-state absorption cross sections of pump and signal of the crystal fibers. The numerical analysis showed that the ASE output power is improved by reducing the fiber core diameter down to several micrometers despite of the increased consumption in excited-state absorption of pump. A comparison of the cross sections between those in literature and this work indicates that the crystal fiber has good crystal and optical qualities using the laser heated pedestal growth method. The large pump absorption of the Cr4+:YAG crystal fiber limits its useful length. With such short fiber length, the ASE lights can not acquire enough gain. The ASE efficiency can be further improved by using bi-direction and cladding pump structure to increase the crystal fiber length and incorporating a high ASE reflector at the input end of the crystal fiber. The Cr4+:YAG crystal fiber has a potential for applying to ultra-broadband ASE light source in wavelength division multiplexing network.

[1]  S. M. Jacobsen,et al.  Saturation of 1.064 μm absorption in Cr,Ca:Y3Al5O12 crystals , 1992 .

[2]  J. F. Massicott,et al.  High gain, broadband, 1.6 mu m Er/sup 3+/ doped silica fibre amplifier , 1990 .

[3]  A. V. Shestakov,et al.  Absorption saturation mechanism for Y A G : C r 4 + crystals , 2000 .

[4]  Walter Koechner,et al.  Solid-State Laser Engineering , 1976 .

[5]  Huber,et al.  Near-infrared emission of Cr4+-doped garnets: Lifetimes, quantum efficiencies, and emission cross sections. , 1995, Physical review. B, Condensed matter.

[6]  Yehoshua Kalisky,et al.  Excited-state absorption studies of Cr/sup 4+/ ions in several garnet host crystals , 1998 .

[7]  C Y Lo,et al.  Double-clad Cr4+:YAG crystal fiber amplifier. , 2005, Optics letters.

[8]  Y. Miyajima,et al.  1.47 mu m band Tm/sup 3+/ doped fluoride fibre amplifier usimg a 1-064 /spl mu/m upconversion pumping scheme , 1993 .

[9]  Max Ming-Kang Liu Principles and Applications of Optical Communications , 1996 .

[10]  R. Feldman,et al.  Dynamics of chromium ion valence transformations in Cr, Ca: YAG crystals used as laser gain and passive Q-switching media , 2003 .

[11]  A. Sennaroğlu Broadly tunable Cr4+-doped solid-state lasers in the near infrared and visible , 2002 .

[12]  N. A. Olsson,et al.  Erbium-Doped Fiber Amplifiers—Amplifier Basics , 1999 .

[13]  F. Di Pasquale,et al.  Improved Gain Performance In Yb -Sensitized Er -Doped Alumina (Al O ) Channel Optical Waveguide Amplifiers , 2001 .

[14]  M Birnbaum,et al.  Dual Q switching and laser action at 1.06 and 1.44 microm in a Nd(3+):YAG-Cr(4+):YAG oscillator at 300 K. , 1993, Optics letters.

[15]  M. Kavehrad,et al.  Analytical model for rare-earth-doped fiber amplifiers and lasers , 1994 .

[16]  N. Olsson,et al.  Erbium-Doped Fiber Amplifiers: Fundamentals and Technology , 1999 .

[17]  Sheng-Lung Huang,et al.  Glass-clad Cr4+:YAG crystal fiber for the generation of superwideband amplified spontaneous emission. , 2004, Optics letters.

[18]  Iain T. McKinnie,et al.  The influence of active ion concentration and crystal parameters on pulsed Cr :YAG laser performance , 1999 .

[19]  Hoffman,et al.  Spectroscopy and dynamics of Cr4+:Y3Al5O12. , 1994, Physical review. B, Condensed matter.

[20]  Robert S. Feigelson,et al.  Pulling optical fibers , 1986 .

[21]  T. Ono,et al.  Key technologies for terabit/second WDM systems with high spectral efficiency of over 1 bit/s/Hz , 1998 .

[22]  Chien-Chih Lai,et al.  Nanostructure formation of double-clad Cr4+:YAG crystal fiber grown by co-drawing laser-heated pedestal , 2006 .

[23]  Zeev Burshtein,et al.  Cr/sup 4+/:YAG as passive Q-switch and Brewster plate in a pulsed Nd:YAG laser , 1995 .

[24]  M. Potenza,et al.  Thulium-doped tellurite fiber amplifier , 2004, IEEE Photonics Technology Letters.

[25]  F. Di Pasquale,et al.  Improved gain performance in Yb/sup 3+/-sensitized Er/sup 3+/-doped alumina (Al/sub 2/O/sub 3/) channel optical waveguide amplifiers , 2001 .

[26]  Santiago Camacho-López,et al.  Intensity-induced birefringence in Cr4+: YAG , 1997 .

[27]  I. M. Jauncey,et al.  Low-noise erbium-doped fibre amplifier operating at 1.54μm , 1987 .

[28]  A Mori,et al.  Gain characteristics of tellurite-based erbium-doped fiber amplifiers for 1.5-microm broadband amplification. , 1998, Optics letters.

[29]  A. Galvanauskas,et al.  Low-noise amplification of high-power pulses in multimode fibers , 1999, IEEE Photonics Technology Letters.

[30]  E. Snitzer,et al.  Pr(3+)-doped fluoride fiber amplifier operating at 1.31 microm. , 1991, Optics letters.

[31]  Michael Bass,et al.  Z-scan measurement of the ground and excited state absorption cross sections of Cr/sup 4+/ in yttrium aluminum garnet , 1999 .

[32]  C. A. Millar Diode-laser pumped erbium-doped fluorozirconate fibre amplifier for the 1530 nm communications window , 1990 .