By Mark Fox

ISBN-10: 0198506120

ISBN-13: 9780198506126

ISBN-10: 0198506139

ISBN-13: 9780198506133

Supplies an advent to the optical homes of solids, together with many new issues that experience no longer been formerly lined in different stable kingdom texts at this point. Softcover. Hardcover to be had.

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The scattering is both coherent and elastic, and each atom behaves like a Huygens point source. However, eachscatteringeventintroducesa phase lag which causesa slowing of the propagation of the phasefront through the a trc oJl tGC tn h ]E rbi bir dd tq rill t dc medium. 2 Vibrational oscillators 2-l- An optical medium may contain other types of dipole oscillators in addition to those originating from the bound electronswithin the atoms. If the medium is ionic, it will contain oppositely charged ions.

The free electron model of metals is attributed to Paul Drude, and so the rpplication of the dipole oscillator model to free electron systemsis generally -'alledthe Drudrlorentz model. The dipole oscillator model is perfectly valid, :rcept that we must set 1116: 0 throughout. The optical properties of free :lectron systemswill be discussedin Chapter 7. 2 The dipole oscillator model In the previous section we introduced the general assumptionsof the dipole oscillator model. We now want to use the model to calculate the frequency dependenceof the refractive index and absorption coefficient.

I1, and recall the definition of e. ed to calculate the full frequency dependenceof the dielectric constant. :e plotted against frequency in Fig. 6. The width of eachabsorption :ne has been set ta l0 Eo of the centre frequency by appropriate choice of :re damping term. The resonancein the infrared is included to representthe . ibrational absorption. In a real solid, we would have to adapt the model :ppropriately to account for the different reduced mass and effective charge 'l the vibrational oscillator.

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Optical properties of solids by Mark Fox


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