\( \newcommand{\d}{\mathrm{d}} \newcommand{\bomega}{\vec\omega} \newcommand{\half}{ {1\over 2} } \def\mathnot#1{\text{"$#1$"}} %operators \newcommand{\diag}{\mathrm{diag}} \newcommand{\sinc}{\mathrm{sinc}} \newcommand{\Sh}{ {\large\style{font-family:Times}{\text{Ш}}} } \newcommand{\res}{\mathrm{Res}} \)

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  • 5. Classical Electromagnetism

5. Classical Electromagnetism¶

  • 5.1. Maxwell’s Equations
    • 5.1.1. Electromagnetic Field
    • 5.1.2. Maxwell’s Equations
    • 5.1.3. Lorentz Force
    • 5.1.4. Hamiltonian
    • 5.1.5. Electromagnetic Stress Tensor
    • 5.1.6. Examples
  • 5.2. Semiconductor Device Physics
    • 5.2.1. Equations
    • 5.2.2. Example 3

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