Advanced Fiber Optics - download pdf or read online

By Luc Thévenaz

ISBN-10: 1439835179

ISBN-13: 9781439835173

ISBN-10: 1482247038

ISBN-13: 9781482247039

ISBN-10: 2940222436

ISBN-13: 9782940222438

This publication presents a entire therapy of the sector of recent fiber optics, starting with the fundamentals of the sphere summarized in an introductory bankruptcy. professional members then themes akin to polarization results in optical fibers photonic crystal fibers highly-doped optical fibers non-linear results amplification and lasing in optical fibers supercontinuum new release, Rayleigh and inelastic scattering with functions to sensing optical fiber element sensors, and polymer optical-fiber-based sensors.

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Extra info for Advanced Fiber Optics

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Lopez-Higuera, Handbook Of Optical Fiber Sensing Technology, WileyBlackwell, 2002. [5] Brian Culshaw and John Dakin, Optical Fiber Sensors, (4 volumes), Artech House, 1988–1997. [6] Govind P. Agrawal, Nonlinear fiber optics, 4th Edition, Elsevier – Academic Press, 2007. [7] John M. : Prentice-Hall, 1992. [8] D. W. Prather, A. Sharkawy, S. Shi, J. , Photonic Crystals, Theory, Applications and Fabrication, Wiley Series in Pure and Applied Optics, 2009. [9] H. Lefevre, Fiber-optic Gyroscope, Artech House, 1993.

While the j value has no consequence to the polarization state, it does carry information about the phase of the wave, so important for interferometry and other phase­dependent interactions. Jones vectors expressed in an arbitrary basis The preceding results were obtained by using the Cartesian x and y axes as the basis states. It is possible to generalize the Jones vector to any other set of two different arbitrary basis states B1 and B2. 27) where the Jones vectors of the new basis (B1 and B2) are expressed in the Cartesian xy basis.

It will later become clear that in linearly birefringent materials, linearly polarized light along any direction other than the x and y directions will not emerge as linearly polarized. 17) with bx ≠ by. 18) If ∆fMAT = p2 , we have what is called a l4 retardation plate (quarter-wave plate). If ∆fMAT = p, we have a l2 retardation plate (half-wave plate). If Polarization Effects in Optical Fibers 35 by > bx, the y axis is the slow axis: light linearly polarized parallel to the y axis travels slower than light linearly polarized parallel to the x axis, which is, therefore, the fast axis.

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Advanced Fiber Optics by Luc Thévenaz


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