Solid-State Theory 0260031 Dr. Hongwei Chu Room 139, Building N5 hongwei.chu@sdu.edu.cn 15165199229 Scores Final Examination (50%) + Presentation (50%) Introduction This lecture is mainly about the way light interacts with solids, specially designed for the first year graduate students in Physics, Optical Engineering. At the same time, I hope some of the topics will be of particular interest to students and researchers of other disciplines in chemical, environmental, or material engineering in the campus. Introduction Contents 01 Introduction 02 Classical propagation 03 Interband absorption 04 Excitons 05 Luminescence 06 Nonlinear optics Introduction Overview of optical properties and models Linear optics Nonlinear optics Electronic Physics Vibronic Systems Vibrational Physics Intraband absorption Luminescent defects and impurites Phonons Excitons Intraband emissions … … … Introduction Refraction • Reflection Light waves propagate with a smaller velocity < c. • Some of the light is reflected from the front surfaces Interface refraction: Snell’s Law • If any of the propagation light reaches the back surfaces, the reflection occurs again • • • • Light-mater interactions Absorption in the propagation resonant with ΔE • • Absorption/Luminescence Luminescence: spontaneous emission of light from the excited states to the ground state in solids • • Scattering Light waves change the propagation directions, possibly its frequency after interacting with the medium • • Nonlinear optics Other phenomena when the light propagates through the medium • SHG, SFG, FWM, etc • Propagation • The light enters the medium and propagates through it • Transmission • The amount of light transmitted related to the reflectivity at both faces, along the way the light propagates through the medium Introduction • Reflectivity, R • R=reflected power/ the incident power Optical coefficients • Transmissivity, T • T=transmitted power / the incident power Introduction Excited State Ωs Absorption hv Relaxation Emission hvs Ground State Introduction Scattering Mie Scattering Rayleigh Scattering Raman Scattering elastic scattering of light elastic scattering of light Inelastic scattering of light d~/> λ d<<λ Raman active molecules Mie signal is proportional to d2 is proportional to 1/λ4 Raman shift ~ vibrational mode stronger Normal Weaker (6 order smaller than Mie) strong angular dependency Species non-selective λRa on λl Mie imaging λRL~ λin Raman spectrometer/imaging spontaneous Introduction Example The reflectivity of silicon at 633 nm is 35% and the absorption coefficient is 3.8×105 m-1. There is a silicon wafer with a thickness of 10 µm. Try to calculate the transmission and optical density of this wafer. Introduction Complex refractive index Introduction Complex refractive index Introduction Complex dielectric constant Introduction Example Introduction Optical materials Crystalline Glasses Metals Molecular materials Doped Introduction Characteristic optical physics Crystal symmetry Electronic bands Crystals: long range translational order 32 classes: point group symmetry 230 classes: space group symmetry Vibronic bands Density of stats 7 Crystal systems 14 Bravais Lattices Cubic Primitive I(Body-) Facecentered Tetragonal PI Orthorhombic P I F C(side-centered) Hexagonal P Monoclinic P Triclinic PC Trigonal P Delocalized states and collective excitations Introduction Crystal symmetry Note: the point group symmetry of a crystal is lower than that of an individual atom (highest possible symmetry owing to the spherical invariance). the point group symmetry Optical anisotropy: crystal is anisotropic if the properties are not the same in all direction. Lifting of degeneracies: Free atoms: spherical symmetric, no preferable directions. Zeeman effect can describe the splitting of degenerate magnetic levels when the atom is put in a magnetic field. The same atom in a crystal, owing to the crystal field determined degeneracies can be lifted. by the lattice, some level Introduction Electronic bands Introduction Density of States l Thanks for attention