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Higher-order mode suppression in twisted single-ring hollow-core photonic crystal fibers

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Edavalath,  N. N.
Russell Division, Max Planck Institute for the Science of Light, Max Planck Society;

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Guenendi,  M. C.
Russell Division, Max Planck Institute for the Science of Light, Max Planck Society;

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Beravat,  R.
Russell Division, Max Planck Institute for the Science of Light, Max Planck Society;
International Max Planck Research School, Max Planck Institute for the Science of Light, Max Planck Society;

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Wong,  G. K. L.
Russell Division, Max Planck Institute for the Science of Light, Max Planck Society;

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Frosz,  M. H.
Russell Division, Max Planck Institute for the Science of Light, Max Planck Society;

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Menard,  J. -M.
Russell Division, Max Planck Institute for the Science of Light, Max Planck Society;

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Russell,  P. St. J.
Russell Division, Max Planck Institute for the Science of Light, Max Planck Society;

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Citation

Edavalath, N. N., Guenendi, M. C., Beravat, R., Wong, G. K. L., Frosz, M. H., Menard, J.-.-M., et al. (2017). Higher-order mode suppression in twisted single-ring hollow-core photonic crystal fibers. OPTICS LETTERS, 42(11), 2074-2077. doi:10.1364/OL.42.002074.


Cite as: https://hdl.handle.net/21.11116/0000-0000-89AA-6
Abstract
A hollow-core single-ring photonic crystal fiber (SR-PCF) consists of a ring of capillaries arranged around a central hollow core. Spinning the preform during drawing introduces a continuous helical twist, offering a novel means of controlling the modal properties of hollow-core SR-PCF. For example, twisting geometrically increases the effective axial propagation constant of the LP01-like modes of the capillaries, providing a means of optimizing the suppression of HOMs, which occurs when the LP11-like core mode phase-matches to the LP01-like modes of the surrounding capillaries. (In a straight fiber, optimum suppression occurs for a capillary-to-core diameter ratio d/D = 0.682.) Twisting also introduces circular birefringence (to be studied in a future Letter) and has a remarkable effect on the transverse intensity profiles of the higher-order core modes, forcing the two-lobed LP11-like mode in the untwisted fiber to become three-fold symmetric in the twisted case. These phenomena are explored by means of extensive numerical modeling, an analytical model, and a series of experiments. Prism-assisted side-coupling is used to measure the losses, refractive indices, and near-field patterns of individual fiber modes in both the straight and twisted cases. (C) 2017 Optical Society of America