By Bahaa E. A. Saleh, Malvin Carl Teich
Now in a brand new full-color variation, basics of Photonics, moment variation is a self-contained and up to date introductory-level textbook that completely surveys this speedily increasing quarter of engineering and utilized physics. that includes a logical mixture of conception and functions, insurance comprises unique money owed of the first theories of sunshine, together with ray optics, wave optics, electromagnetic optics, and photon optics, in addition to the interplay of photons and atoms, and semiconductor optics. offered at expanding degrees of complexity, initial sections construct towards extra complex issues, resembling Fourier optics and holography, guided-wave and fiber optics, semiconductor resources and detectors, electro-optic and acousto-optic units, nonlinear optical units, optical interconnects and switches, and optical fiber communications.
Each of the twenty-two chapters of the 1st version has been completely up-to-date. the second one version additionally gains fullyyt new chapters on photonic-crystal optics (including multilayer and periodic media, waveguides, holey fibers, and resonators) and ultrafast optics (including femtosecond optical pulses, ultrafast nonlinear optics, and optical solitons). The chapters on optical interconnects and switches and optical fiber communications were thoroughly rewritten to deal with present technology.
Each bankruptcy comprises summaries, highlighted equations, routines, difficulties, and chosen analyzing lists. Examples of genuine platforms are incorporated to stress the suggestions governing functions of present curiosity.
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Extra resources for Fundamental of Photonics (2nd Edition)
P == cos - 1 1 - ) d 2f . 4-7 A periodic sequence of lenses. 4 MATRIX OPTICS 33 When d == 2/, cp == 1r /2, and cp /27r == � , so that the trajectory of an arbitrary ray is periodic with period equal to four stages. When d == f, cp == 1f /3, and cp/27r == �, so that the ray trajectory is periodic and retraces itself each six stages. These cases are illustrated in Fig. 4-8. 4-8 l� d �l Examples of stable ray trajectories in a periodic lens system: (a) d == 2/; (b) d == f . 4-6 Examine the trajectories of paraxial rays through a periodic system comprising a sequence of lens pairs with alternating focal lengths f1 and f2 , as shown in Fig.
Regardless of 81) as long as the approxima tion is valid. This means that all paraxial rays originating from point P1 arrive at P2 . The distances z1 and z2 are measured in a coordinate system in which the z axis points to the left. Points of negative z therefore lie to the right of the mirror. 2-2), rays that are emitted from a point very far out on the z axis ( z1 == oo) are focused to a point F at a distance z2 == ( - R) /2. 2-4) f' - Imaging Equation ( Paraxial Rays) which is known as the imaging equation.
A ray crossing the transverse plane at z is completely characterized by the coordinate of y of its crossing point and the angle () (Fig. 41). An optical system is a set of optical components placed between two transverse planes at z1 and z2 , referred to as the input and output planes, respectively. 4-1 A ray is charac terized by its coordinate y and its angle B. 4-2 A ray enters an optical system at location z1 with position y1 and angle B1 and leaves at position y2 and angle B2 . direction (YI , ()I ) .
Fundamental of Photonics (2nd Edition) by Bahaa E. A. Saleh, Malvin Carl Teich