By Michael E. Thomas
A customary optical procedure consists of 3 simple elements: a resource, a detector, and a medium within which the optical strength propagates. Many textbooks disguise assets and detectors, yet only a few disguise propagation in a finished method, incorporating the newest development in conception and test about the propagating medium. This booklet fulfills that want. it's the first finished and self-contained booklet in this subject. it truly is invaluable reference publication for researchers, and a textbook for classes like Laser mild Propagation, reliable country Optics, and Optical Propagation within the surroundings.
Read or Download Optical Propagation in Linear Media: Atmospheric Gases and Particles, Solid-State Components, and Water (Johns Hopkins University Applied Physics Laboratory Series in Science & Engineering) PDF
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Extra resources for Optical Propagation in Linear Media: Atmospheric Gases and Particles, Solid-State Components, and Water (Johns Hopkins University Applied Physics Laboratory Series in Science & Engineering)
Sample text
C. Teich, Fundamentals of Photonics, Wiley (1991). W. Goodman, Statistical Optics, Wiley-Interscience (1985). W. H. Eberly, Lasers, Wiley (1988). E. C. Sherman, Electromagnetic Pulse propagation in Causal Dielectrics, Springer-Verlag (1994). This page intentionally left blank 2 Optical Electromagnetics II In this chapter the same basic topics are addressed as in the previous chapter, but now in the presence of matter. This greatly complicates the description of optical propagation and continues to be the primary topic of the remaining chapters.
67) 40 OPTICAL PROPAGATION IN LINEAR MEDIA Substituting these definitions into Eq. 64, we obtain i = r + s + a + t. 70c) and finally τ ( i,ω) = t( i,ω) = total integrated transmittance. 70d) Notice that these quantities are functions of angles of incidence and frequency only. 69 is also called the total power law. The sum of total integrated scatterance and total integrated absorptance is generally defined as the total integrated extinctance, αext , αext ( i,ω) = αabs ( i,ω) + α sca ( i,ω). 71) Using this result, the total power law becomes 1 = ρ( i,ω) + αext ( i,ω) + τ ( i,ω).
Only general macroscopic properties of these parameters will be examined at this time. A more detailed microscopic development is presented in Chapter 5. The constitutive relations greatly complicate a time-domain solution of Maxwell’s equations. For this reason, a frequency-domain solution is preferred because the convolution integrals are not needed. 11) ∇ · µ(r,ω)H(r,ω) = 0. 12) and Taking the curl of Faraday’s law, one obtains the frequency-domain wave equation for the electric field, E ∇× 1 ∇×E(r,ω) = (− jωσ + ω2 )E(r,ω).