Abstract
The phase-space representation of electromagnetic radiometry is founded on the electromagnetic generalized radiance tensors, which allow overcoming the limitations due to the scalar electromagnetic generalized radiances. The fundamental quantities of both scalar generalized radiometry and classical radiometry or photometry become particular cases. The transport of measurable radiometric quantities by the electromagnetic field is described in terms of the propagation of the contributions from individual radiators and their redistribution over each wavefront on propagation. A physical meaning is given to the negative values of the generalized radiance, which gives new insights into Poynting's theory of energy transport.
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