Abstract
As technologies for dispersion compensation in optical fiber communication systems becoming matured, one of the impairments on future high bit-rate systems no doubt is due to the optical fiber dispersion slope (DS). The performance of future high-speed systems rely on the capability of compensators to map the total transmission DS. Nonlinear-chirped fiber Bragg gratings (NCFBGs) which possess quadratic delay, have been demonstrated for DS compensation.1,2 The quadratic chirp in the FBGs can be inscribed permanently during fabrication3 or induced by imparting either mechanical or temperature effect to transform it into a NCFBG.4,5
© 2002 Optical Society of America
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