Download e-book for kindle: Advanced Fiber Optics by Luc Thévenaz

By Luc Thévenaz

ISBN-10: 1439835179

ISBN-13: 9781439835173

ISBN-10: 1482247038

ISBN-13: 9781482247039

ISBN-10: 2940222436

ISBN-13: 9782940222438

This booklet presents a finished therapy of the sphere of recent fiber optics, starting with the fundamentals of the sector summarized in an introductory bankruptcy. professional participants then issues resembling polarization results in optical fibers photonic crystal fibers highly-doped optical fibers non-linear results amplification and lasing in optical fibers supercontinuum iteration, Rayleigh and inelastic scattering with functions to sensing optical fiber element sensors, and polymer optical-fiber-based sensors.

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14 A fiber-drawing tower: The preform is heated in a furnace and a thin fiber is drawn with tight diameter control. On its way to the take-up drum, the fiber is coated by a thermocuring plastic jacket for mechanical protection and the stripping of cladding modes. 16 Advanced Fiber Optics Before concluding this section we note that several more preform ­manufacturing techniques are in use today, including OVD (outside vapor deposition) and VAD (vapor axial deposition) [26]. Also, dopants other than germanium have been used to increase the core refractive index, such as boron and phosphorus.

Zero dispersion means that very narrow pulses can propagate undistorted for many tens of kilometers before higher-order dispersion terms ({bi, i ≥ 3} in equation (12) become important. , Fabry-Perot multimode lasers) having up to a few nanometers of spectral width. Finally, a slightly different (cf. 19) 20 Advanced Fiber Optics Dwaveguide [ps/(nm·km)] −1 −2 −3 −4 −5 −6 1200 1250 1300 1350 1400 1450 Wavelength (nm) 1500 1550 1600 Fig. 16 Much weaker than material dispersion and opposite in sign, waveguide dispersion has only a small effect on the wavelength of zero dispersion for a standard step-index fiber.

Jones has proven the following important theorem: every linear medium with no polarization-dependent loss can be represented by a concatenation of a linear waveplate and a rotator (see Fig. 8). The concept of reciprocity will be described later in this book (when studying the polarization properties of Rayleigh scattering, see Sect. 3). For a rotator, it means that the rotation angle induced in the backward direction is the opposite of the rotation angle in the forward direction. This is not the case for the Faraday rotator described in the next Section.

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Advanced Fiber Optics by Luc Thévenaz

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