If I accelerate a charge, EM radiation is emitted. For a simple dipole model, the radiation propagates outward along a torus shape (see Griffiths, Intro to ED, 3ed., fig 11.4) - the acceleration field, with power according to Larmor formula.(adsbygoogle = window.adsbygoogle || []).push({});

Since EMR is quantized, in what way is the described dipole radiation quantized?

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# Quantization of EMR in charge acceleration

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