## optical properties of solids

167.86.98.99. Semiconductor quantum wells 7. Part of Springer Nature. VitalSource Bookshelf gives you access to content when, where, and how you want. We cannot process tax exempt orders online. Molecular materials 9. Not affiliated 10.1. Please enter a star rating for this review, Please fill out all of the mandatory (*) fields, One or more of your answers does not meet the required criteria. : 0114/2224527, Fax: 0114/2728079, Email: mark.fox@shef.ac.uk, Department of Physics and Astronomy Mark Fox, B Quantum theory of radiative absorption and emission, Volume 3 van Oxford master series in condensed matter physics, Volume 3 van Oxford master series in physics. The fundamental principles of absorption, reflection, luminescence and light scattering are discussed for a wide range of materials, including crystalline insulators and semiconductors, glasses, metals,and molecular materials. $$, © Springer International Publishing AG, part of Springer Nature 2018, \( \left[ {x,p_{x} } \right] = {\text{i}}\hbar \), \( \hat{\varvec{e}} = \hat{\varvec{i}} \), https://doi.org/10.1007/978-3-319-75322-5_10. Suggested Citation:"ELECTRICAL, OPTICAL, AND THERMAL PROPERTIES OF SOLIDS. Browse door 's werelds grootste eBoekenwinkel en begin vandaag nog met lezen op internet, je tablet, telefoon of eReader. © 2020 Springer Nature Switzerland AG. If you decide to participate, a new browser tab will open so you can complete the survey after you have completed your visit to this website. Sitemap. Share your review so everyone else can enjoy it too. Download Citation | Optical Properties of Solids | Preface 1. To provide all customers with timely access to content, we are offering 50% off Science and Technology Print & eBook bundle options. Examples include semiconductor quantum wells, organic semiconductors, vibronic solid state lasers and nonlinear optics.The book is primarily written for physicists, but it will also be useful for electrical engineers, materials scientists, and physical chemists. The fundamental principles of absorption, reflection, luminescence and light scattering are discussed for a wide range of materials, including crystalline insulators and semiconductors, glasses, metals,and molecular materials. Privacy Policy Easily read copying, pasting, and printing. process to access eBooks; all eBooks are fully searchable, and enabled for Thanks in advance for your time. Classical propagation 3. The innovative text gives an introductory treatment of the optical properties of solids. Softcover available. - Buy once, receive and download all available eBook formats, For intermediate frequencies \( \omega_{T} < \omega < \omega_{L} \), given [by (10.198)]. This is a preview of subscription content, log in to check access. Excitons 5. Luminescence centres 10. Your review was sent successfully and is now waiting for our team to publish it. (b) For \( \hat{\varvec{e}} = \hat{\varvec{i}} \), show the oscillator strength \( f_{ij} \) obeys the sum rule \( \sum\nolimits_{j} {f_{ij} } = 1 \). p Perturbation Theory Nonlinear optics Appendix A: Electromagnetism in dielectrics Appendix B: Quantum theory of radiative absorption and emission Appendix C: Band theory Appendix … Free electrons 8. We would like to ask you for a moment of your time to fill in a short questionnaire, at the end of your visit. p. cm. This is a preview of subscription content, $$ \left[ {\mathcal{H},\hat{\varvec{e}} \cdot \varvec{r}} \right] = - \frac{i\hbar }{m}\hat{\varvec{e}} \cdot \varvec{p} $$, $$ \frac{\varepsilon (\omega )}{\varepsilon_{0} } - \frac{\varepsilon \left( \infty \right)}{\varepsilon_{0} } = \frac{{3B_{\text{ion}} (\omega )}}{{\left[ {1 - B_{\text{el}} - B_{\text{ion}} (\omega )} \right]\left( {1 - B_{\text{el}} } \right)}}, $$, $$ \mu \ddot{v} + Gv = \frac{1}{{3\varepsilon_{0} }}\,\frac{{Ne^{2} }}{{1 - B_{\text{el}} }}v + eE, $$, $$ \omega_{T}^{2} + \frac{{c\varepsilon_{0} }}{\varepsilon (\infty )} = \omega_{L}^{2} , $$, $$ \begin{aligned} & \mu \left( {\omega_{T}^{2} - \omega^{2} } \right)v = eE, \\ & \frac{E}{{E_{\text{loc}} }} = \frac{1}{1 + F}, \\ & \varepsilon (\omega ) = \varepsilon (\infty ) + \frac{{c\varepsilon_{0} }}{{\omega_{T}^{2} - \omega^{2} }}.

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