Understanding Nano Photonics and Wave Equations

Aug 22, 2024

Lecture Notes: Nano Photonics and Wave Equations

Recap of Previous Lecture

  • Discussed scientific problems in nano photonics.
  • Focused on solving electromagnetic responses with varying permittivities.

Maxwell's Equations and Wave Equation

  • Solving for electromagnetic response involves Maxwell's equations.
  • Two curl equations from Maxwell's equations lead to the wave equation for free space.

Wave Equation Derivation

  • The wave equation is a second-order partial differential equation relating time and space derivatives.
    • Form: ( \frac{\partial^2 E}{\partial t^2} = v^2 \nabla^2 E )
    • ( \nabla^2 ) is the Laplacian operator (( \frac{\partial^2}{\partial x^2} + \frac{\partial^2}{\partial y^2} + \frac{\partial^2}{\partial z^2} )).

Steps to Derive Wave Equation

  1. Start with curl of electric field (E) and magnetic field (H).
  2. Assume magnetization is zero: ( B = \mu H ).
  3. Apply curl to the first equation to yield wave equation terms:
    • Include terms for displacement (D), polarization (P), and current density (J).
  4. Simplify using vector calculus identities.
  5. In free space (no charges, no currents), equation reduces to:
    • ( \nabla^2 E = \mu_0 \epsilon_0 \frac{\partial^2 E}{\partial t^2} )

Solutions to Wave Equation

  • Solutions are plane waves where:
    • Electric and magnetic fields oscillate perpendicularly to each other and to the direction of propagation.
  • Wave speed in vacuum is defined as:
    • ( v = \frac{1}{\sqrt{\mu_0 \epsilon_0}} = c \approx 3 \times 10^8 m/s )

Electromagnetic Waves in Mediums

  • For a dielectric medium (e.g., glass):
    • No current (J = 0).
    • Polarization (P) is non-zero and related to susceptibility (( \chi )).
    • Wave equation becomes:
      • ( \nabla^2 E = \mu_0 \epsilon_0 (1 + \chi) \frac{\partial^2 E}{\partial t^2} )
  • Velocity of wave in a medium is modified:
    • ( v = \frac{c}{\sqrt{\epsilon_r}} )
    • Refractive index ( n = \sqrt{\epsilon_r} ).

Nonlinear Optics

  • Assumptions made include linear polarization.
  • Non-linear responses can occur, leading to phenomena like harmonic generation.

Refractive Index and Dispersion

  • Refractive index varies with wavelength (dispersion).
  • Example materials and their band gaps:
    • Germanium: 0.8 eV
    • Gallium Arsenide: 1.42 eV
    • Gallium Nitride: 3.4 eV
    • Silicon Dioxide: 9 eV

Relation Between Photons and Electrons

  • Electromagnetic waves are generated by moving charges (e.g., antennas).
  • Electric fields induce charge movement (light detection).
  • Key similarities include:
    • Wave-particle duality of electrons and photons.
    • Electron energy: ( \frac{p^2}{2m} ) (parabolic dispersion).
    • Photon energy: linear relation (energy proportional to momentum).

Conclusion and Questions

  • Discussed implications of different energy levels for electrons and photons.
  • Questions about parameter comparisons between electrons and photons.
  • Importance of understanding both fields as they are interconnected.

Note: The lecture emphasizes the fundamental connections between optics, electromagnetics, and electronics, highlighting the physical laws governing the behavior of light and electrons.