Optoelectronics And Photonics Kasap Pdf


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optoelectronics and photonics kasap pdf

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For one-semester, undergraduate-level courses in Optoelectronics and Photonics, in the departments of electrical engineering, engineering physics, and materials science and engineering. An introductory up-to-date textbook in optoelectronic and photonic devices suitable for half- or one-semester courses at the undergraduate level in electrical engineering, engineering physics and materials science and engineering departments. Although written for undergraduate students, it can also be used at the graduate level as an introductory course by incorporating some of the selected topics included on the accompanying CD-ROM.

Kasap - Optoelectronics And Photonics.pdf

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Solutions manual for optoelectronics and photonics principles and practices 2nd edition by kasap 1. Word format may be available from the author. Please check the above website. Report errors and corrections directly to the author at safa. Solutions Manual Preliminary 11 December Chapter 2 2. Currently none reported. In addition, there is a phase difference between the two due to the different paths taken to reach point P.

Show that the superposition of E1 and E2 at P is given by E y, z,t 2Eo cos m y 2 cos t m z 2 1 1 What do the two cosine terms represent? The planar waveguide is symmetric, which means that the intensity, E2 , must be either maximum even m or minimum odd m at the center of the guide. The field distributions are shown in Figure 2Q Allowed upward and downward traveling waves inside the core of the planar waveguide set-up a standing wave along y.

The standing wave can only exist if the wave can be replicated after it has traveled along the y-direction over one round trip. Put differently, a wave starting at A in Figure 2. At this point, it must have an identical phase to its starting phase so that it can replicate itself and not destroy itself.

Given that the wavevector along y is m, derive the waveguide condition. Figure 2. The condition for setting-up a standing wave is that the wave must be identical, able to replicate itself, after one round trip along y. Solution From Figure 2. What is your conclusion?

Ray 1 experiences total internal reflection at A. There is a phase difference between the two waves. See Figure 2Q Given the phase difference y m y m m m a m between the waves at C, distance y above the guide center, find the electric field pattern E y in the guide. Recall that the field at C can be written as E y Acos t Acos[t m y ].

There is a phase difference between the two Solution The two waves interfering at C are out phase by , E y Acos t Acos[t m y ] where A is an arbitrary amplitude. From Example 2. Alternatively one can use a computer program for finding the roots of a function. The above equations are functions of m only for each m. This is shown in Figure 2Q The following intuitive calculation shows how the small difference between the TE and TM waves can lead to dispersion that is time spread in the arrival times of the TE and TM optical signals.

One should be cautioned that we calculated dispersion using the phase velocity whereas we should have used the group velocity. It is assumed that the math-software package can carry out symbolic algebra such as partial differentiation the author used Livemath, , though others can also be used.

The objective is to express and in terms of. Then the group velocity is found by differentiating Eqs 1 and 2 with respect to i. For a given m value, Eqs 2 and 3 can be plotted parametrically, that is, for each value we can calculate and vg and plot vg vs. Using a convenient math-software package, or by other means, obtain the same vg vs. Obviously other math software packages can also be used. The important conclusion from Figure 2.

Equation 2. Thus, it is only approximate. Figure 2Q Group velocity vs. LiveMath used 2. The refractive index of GaAs is 3. What is the cut-off wavelength beyond which only a single mode can propagate in the waveguide, assuming that the refractive index does not vary greatly with the wavelength?

If a What is the mode field width MFW of this radiation? For a rectangular waveguide, the fundamental mode has a mode field width 2w MFW 2a V 1 0. The penetration depth is half the core thickness. Solution of the waveguide condition in Eq. For each wavelength calculate and m and then plot vs. Compare your plot with the dispersion diagram in Figure 2. The propagation constant along the guide, along z is given by Eq.

Propagation constants at other wavelengths and hence frequencies can be similarly calculated. The results are listed in Table 2Q and plotted in Figure 2Q This is the dispersion diagram.

For comparison the dispersion vs for the core and the cladding are also shown. Thus, the solutions of the waveguide condition as in Example 2. Black, TE0 mode. Purple: TE1 mode. Blue: Propagation along the cladding. Red: Propagation along the core. Author's Note: Remember that the slope at a particular frequency is the group velocity at that frequency.

The calculation of the penetration depth requires the calculation of the incidence angle and. Material dispersion and modal dispersion must be combined by 2 2 2 total intermode material The refractive index of water is 1. Consider a water jet of diameter 3 mm that is illuminated by green light of wavelength nm. What is the V-number, numerical aperture, total acceptance angle of the jet? How many modes are there?

What is the cut-off wavelength? The diameter of the jet increases slowly as the jet flows away from the original spout. However, the light is still guided. Light guided along a thin water jet.

Optoelectronics and photonics kasap solution manual pdf chapter 3

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Skip to search form Skip to main content You are currently offline. Some features of the site may not work correctly. Kasap Published Materials Science. Wave Nature of Light. Light Waves in a Homogeneous Medium.

Copyright , by Pearson Education, Inc. Printed in the United States of America. This publication is protected by Copyright and permission should be obtained from the publisher prior to any prohibited reproduction, storage in a retrieval system, or transmission in any form or by any means, electronic, mechanical, photocopying, recording, or likewise. For information regarding permission s , write to: Rights and Permissions Department. Safa O. Includes bibliographical references and index. So there isn t any place to publish, in a dignified manner, what you actually did in order to get to do the work.

Optoelectronics and Photonics: Principles and Practices: United States Edition

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Kasap - Optoelectronics And Photonics.pdf

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The second, updated edition of this essential reference book provides a wealth of detail on a wide range of electronic and photonic materials, starting from fundamentals and building up to advanced topics and applications. Its extensive coverage, with clear illustrations and applications, carefully selected chapter sequencing and logical flow, makes it very different from other electronic materials handbooks. It has been written by professionals in the field and instructors who teach the subject at a university or in corporate laboratories. The Springer Handbook of Electronic and Photonic Materials, second edition, includes practical applications used as examples, details of experimental techniques, useful tables that summarize equations, and, most importantly, properties of various materials, as well as an extensive glossary. Along with significant updates to the content and the references, the second edition includes a number of new chapters such as those covering novel materials and selected applications. This handbook is a valuable resource for graduate students, researchers and practicing professionals working in the area of electronic, optoelectronic and photonic materials.


Kasap, Optoelectronics and Photonics - Principles and Practices, 2nd Ed(​Pearson, )rethinkingafricancollections.org Pages · · MB ·.


Optoelectronics & Photonics: Principles & Practices

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