Nonlinear optics in the LP(02) higher-order mode of a fiber.

The distinct disperion properties of higher-order modes in optical fibers permit the nonlinear generation of radiation deeper into the ultraviolet than is possible with the fundamental mode. This is exploited using adiabatic, broadband mode convertors to couple light efficiently from an input fundamental mode and also to return the generated light to an output fundamental mode over a broad spectral range. For example, we generate visible and UV supercontinuum light in the LP(02) mode of a photonic crystal fiber from sub-ns pulses with a wavelength of 532 nm.

[1]  J. Siuzdak,et al.  Binary-Phase Spatial Light Filters for Mode-Selective Excitation of Multimode Fibers , 2011, Journal of Lightwave Technology.

[2]  J. Arriaga,et al.  Anomalous dispersion in photonic crystal fiber , 2000, IEEE Photonics Technology Letters.

[3]  J. Knight,et al.  From zero dispersion to group index matching: How tapering fibers offers the best of both worlds for visible supercontinuum generation , 2012 .

[4]  T A Birks,et al.  Wavelength-independent all-fiber mode converters. , 2007, Optics letters.

[5]  R. Cherif,et al.  Supercontinuum generation by higher-order mode excitation in a photonic crystal fiber , 2008, 2009 35th European Conference on Optical Communication.

[6]  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.

[7]  J. Knight,et al.  Reducing spectral attenuation in solid-core photonic crystal fibers , 2010, 2010 Conference on Optical Fiber Communication (OFC/NFOEC), collocated National Fiber Optic Engineers Conference.

[8]  J R Taylor,et al.  Extended blue supercontinuum generation in cascaded holey fibers. , 2005, Optics letters.

[9]  S. Ghalmi,et al.  Soliton self-frequency shift below 1300 nm in higher-order-mode, solid silica-based fiber , 2006, LEOS 2006 - 19th Annual Meeting of the IEEE Lasers and Electro-Optics Society.

[10]  Linards Skuja,et al.  Formation and decay of nonbridging oxygen hole centers in SiO2 glasses induced by F2 laser irradiation: In situ observation using a pump and probe technique , 2001 .

[11]  Siddharth Ramachandran,et al.  Bandwidth control of long-period grating-based mode converters in few-mode fibers. , 2002, Optics letters.

[12]  L. Skuja Optically active oxygen-deficiency-related centers in amorphous silicon dioxide , 1998 .

[13]  J. Dudley,et al.  Supercontinuum generation in photonic crystal fiber , 2006 .

[14]  P. Petropoulos,et al.  Mid-IR Supercontinuum Generation From Nonsilica Microstructured Optical Fibers , 2007, IEEE Journal of Selected Topics in Quantum Electronics.

[15]  J. Knight,et al.  Dispersion compensation using single-material fibers , 1999, IEEE Photonics Technology Letters.

[16]  Yoshimichi Ohki,et al.  Improvement of Radiation Resistance of Pure Silica Core Fibers by Hydrogen Treatment , 1985 .

[17]  Purnananda Nandi,et al.  Characterization of a photonic crystal fiber mode converter using low coherence interferometry. , 2009, Optics letters.

[18]  P. Russell,et al.  Supercontinuum and four-wave mixing with Q-switched pulses in endlessly single-mode photonic crystal fibres. , 2004, Optics express.

[19]  P. Kumar,et al.  Four-wave mixing in microstructure fiber. , 2001, Optics letters.

[20]  S. Leon-Saval,et al.  Supercontinuum generation in submicron fibre waveguides. , 2004, Optics express.

[21]  Andrey V. Gorbach,et al.  Light trapping in gravity-like potentials and expansion of supercontinuum spectra in photonic-crystal fibres , 2007 .

[22]  J. Carpenter,et al.  Characterization of Multimode Fiber by Selective Mode Excitation , 2012, Journal of Lightwave Technology.

[23]  Nori Shibata,et al.  Interferometric method for chromatic dispersion measurement in a single-mode optical fiber , 1981 .

[24]  Ashish M. Vengsarkar,et al.  Optical fiber-based dispersion compensation using higher order modes near cutoff , 1994 .

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

[26]  D. Bird,et al.  Adaptive curvilinear coordinates in a plane-wave solution of Maxwell’s equations in photonic crystals , 2005 .

[27]  A Tonello,et al.  Visible supercontinuum generation controlled by intermodal four-wave mixing in microstructured fiber. , 2007, Optics letters.

[28]  J. Clowes,et al.  Visibly “White” light generation in uniform photonic crystal fiber using a microchip laser , 2008, 2008 Conference on Lasers and Electro-Optics and 2008 Conference on Quantum Electronics and Laser Science.

[29]  D V Skryabin,et al.  Four-wave mixing of linear waves and solitons in fibers with higher-order dispersion. , 2004, Optics letters.

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