Completeness relation for polarization vectors

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I'm reading some quantum optics and I stumbled on the following completeness relation for the polarization vectors of the electromagnetic field.

\sum_{a} (\epsilon_{\vec{k} a } )_i ( \epsilon^*_{ \vec{k} a} )_j = \delta_{ij} -\frac{k_i k_j}{\vec{k}^2}


Does anyone know how to derive this relation?
 
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Check out page 36 of Cohen-Tannoudji's <Introduction to Quantum Electrodynamics>.
 
Thanks! :)
 
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