High brightness, quantum-defect-limited conversion efficiency in cladding-pumped Raman fiber amplifiers and oscillators.

We present a detailed theoretical investigation of cladding-pumped Raman fiber amplification in an unexplored parameter space of high conversion efficiency (> 60%) and high brightness enhancement (> 1000). Fibers with large clad-to-core diameter ratios can provide a promising means for Raman-based brightness enhancement of diode pump sources. Unfortunately, the diameter ratio cannot be extended indefinitely since the intensity generated in the core can greatly exceed that in the cladding long before the pump is fully depleted. If left uncontrolled, this leads to the generation of parasitic second-order Stokes wavelengths in the core, limiting the conversion efficiency and as we will show, clamping the achievable brightness enhancement. Using a coupled-wave formalism, we present the upper limit on brightness enhancement as a function of diameter ratio for conventionally guided fibers. We further present strategies for overcoming this limit based upon depressed well core designs. We consider two configurations: 1) pulsed cladding-pumped Raman fiber amplifier (CPRFA) and 2) cw cladding-pumped Raman fiber laser (CPRFL).

[1]  M Ibsen,et al.  High-power continuous-wave cladding-pumped Raman fiber laser. , 2006, Optics letters.

[2]  Moty Heiblum,et al.  Analysis of curved optical waveguides by conformal transformation , 1975 .

[3]  M. Feit,et al.  Computation of mode properties in optical fiber waveguides by a propagating beam method. , 1980, Applied optics.

[4]  R. Beach,et al.  Analysis of the scalability of diffraction-limited fiber lasers and amplifiers to high average power. , 2008, Optics express.

[5]  S. Namiki,et al.  100 nm bandwidth flat gain Raman amplifiers pumped and gain-equalized by 12-wavelength-channel WDM high power laser diodes , 1999, OFC/IOOC . Technical Digest. Optical Fiber Communication Conference, 1999, and the International Conference on Integrated Optics and Optical Fiber Communication.

[6]  P. Pax,et al.  High-gain photonic crystal fiber regenerative amplifier. , 2009, Optics letters.

[7]  Y. Jeong,et al.  High power continuous-wave Yb-doped fiber laser with true single-mode output using W-type structure. , 2006, 2006 Conference on Lasers and Electro-Optics and 2006 Quantum Electronics and Laser Science Conference.

[8]  M. Ibsen,et al.  Analysis of the Conversion to the First Stokes in Cladding-Pumped Fiber Raman Amplifiers , 2009, IEEE Journal of Selected Topics in Quantum Electronics.

[9]  Raymond J Beach,et al.  Brightness enhancement in a high-peak-power cladding-pumped Raman fiber amplifier. , 2009, Optics letters.

[10]  J K Sahu,et al.  Suppression of stimulated Raman scattering in a high power Yb-doped fiber amplifier using a W-type core with fundamental mode cut-off. , 2006, Optics express.

[11]  Amnon Yariv,et al.  Theory of cw Raman oscillation in optical fibers , 1979 .

[12]  J. Nilsson,et al.  Cladding-pumped Raman fiber amplifier for high-gain, high-energy single-stage amplification , 2005, OFC/NFOEC Technical Digest. Optical Fiber Communication Conference, 2005..

[13]  J. Nilsson,et al.  High-brightness, pulsed, cladding-pumped Raman fiber source at 1660 nm , 2007, 2007 Conference on Lasers and Electro-Optics (CLEO).

[14]  Dietrich Marcuse,et al.  Field deformation and loss caused by curvature of optical fibers , 1976 .

[15]  R. Smith Optical power handling capacity of low loss optical fibers as determined by stimulated Raman and brillouin scattering. , 1972, Applied optics.