Frequency tunable polarization and intermodal modulation instability in high birefringence holey fiber.

We present an experimental analysis of polarization and intermodal noise-seeded parametric amplification, in which dispersion is phase matched by group velocity mismatch between either polarization or spatial modes in birefringent holey fiber with elliptical core composed of a triple defect. By injecting quasi-CW intense linearly polarized pump pulses either parallel or at 45 degrees with respect to the fiber polarization axes, we observed the simultaneous generation of polarization or intermodal modulation instability sidebands. Furthermore, by shifting the pump wavelength from 532 to 625 nm, we observed a shift of polarization sidebands from 3 to 8 THz, whereas intermodal sidebands shifted from 33 to 63 THz. These observations are in excellent agreement with the experimental characterization and theoretical estimates of phase and group velocities for the respective fiber modes.

[1]  Thibaut Sylvestre,et al.  Generation of a broadband single-mode supercontinuum in a conventional dispersion-shifted fiber by use of a subnanosecond microchip laser. , 2003, Optics letters.

[2]  R. Leonhardt,et al.  Widely tunable optical parametric generation in a photonic crystal fiber. , 2005, Optics letters.

[3]  Réal Vallée,et al.  Intensity and polarization dependences of the supercontinuum generation in birefringent and highly nonlinear microstructured fibers. , 2003, Optics express.

[4]  M S Demokan,et al.  Broadband wavelength converter based on four-wave mixing in a highly nonlinear photonic crystal fiber. , 2005, Optics letters.

[5]  G. Millot,et al.  Observation of modulational instability induced by velocity-matched cross-phase modulation in a normally dispersive bimodal fiber. , 1997, Optics letters.

[6]  Angelika Unterhuber,et al.  Spectral shaping of supercontinuum in a cobweb photonic-crystal fiber with sub-20-fs pulses , 2002 .

[7]  Zhaoming Zhu,et al.  Polarization properties of supercontinuum spectra generated in birefringent photonic crystal fibers , 2004 .

[8]  A. J. Taylor,et al.  Transformation and control of ultra-short pulses in dispersion-engineered photonic crystal fibres , 2003, Nature.

[9]  R. Stolen Phase-matched-stimulated four-photon mixing in silica-fiber waveguides , 1975 .

[10]  M. Lehtonen,et al.  Supercontinuum generation in a highly biréfringent microstructured fiber , 2003 .

[11]  Tadeusz Martynkien,et al.  Measurements of modal birefringence and polarimetric sensitivity of the birefringent holey fiber to hydrostatic pressure and strain , 2004 .

[12]  G. Millot,et al.  Polarization mode dispersion and vectorial modulational instability in air–silica microstructure fiber , 2002 .

[13]  Rothenberg,et al.  Modulational instability for normal dispersion. , 1990, Physical review. A, Atomic, molecular, and optical physics.

[14]  Wabnitz,et al.  Modulational polarization instability of light in a nonlinear birefringent dispersive medium. , 1988, Physical review. A, General physics.

[15]  R. Leonhardt,et al.  Polarization modulation instability in weakly birefringent fibers. , 1995, Optics letters.

[16]  A. Stentz,et al.  Visible continuum generation in air–silica microstructure optical fibers with anomalous dispersion at 800 nm , 2000 .

[17]  Hugo Thienpont,et al.  Experimental and theoretical investigations of birefringent holey fibers with a triple defect. , 2005, Applied optics.

[18]  J R Taylor,et al.  Continuous-wave, totally fiber integrated optical parametric oscillator using holey fiber. , 2004, Optics letters.

[19]  Keith J. Blow,et al.  Theoretical description of transient stimulated Raman scattering in optical fibers , 1989 .

[20]  R. Leonhardt,et al.  Cross-phase modulational instability in high-birefringence fibers , 1990 .

[21]  L. Provino,et al.  Supercontinuum generation in air–silica microstructured fibers with nanosecond and femtosecond pulse pumping , 2002 .