Classical Electrodynamics · Problem 11.10

Radiating Systems, Multipole Fields and Radiation — John David Jackson

Physics — E&M · lorentz-group-generators

Problem

(a) For the Lorentz boost and rotation matrices K\mathbf{K} and S\mathbf{S} show that (ϵ⋅S)3=−ϵ⋅S(\boldsymbol{\epsilon} \cdot \mathbf{S})^3 = -\boldsymbol{\epsilon} \cdot \mathbf{S} (ϵ′⋅K)3=ϵ′⋅K(\boldsymbol{\epsilon}' \cdot \mathbf{K})^3 = \boldsymbol{\epsilon}' \cdot \mathbf{K} where ϵ\boldsymbol{\epsilon} and ϵ′\boldsymbol{\epsilon}' are any real unit 3-vectors. (b) Use the results of part a to show that exp⁡(−ζβ^⋅K)=I−β^⋅Ksinh⁡ζ+(β^⋅K)2[cosh⁡ζ−1]\exp(-\zeta\hat{\boldsymbol{\beta}} \cdot \mathbf{K}) = I - \hat{\boldsymbol{\beta}} \cdot \mathbf{K} \sinh \zeta + (\hat{\boldsymbol{\beta}} \cdot \mathbf{K})^2[\cosh \zeta - 1]

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