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Consider the space S of incoherent beams. They may be<br />

scaled (e.g, via neutral density filters) and added (e.g., via<br />

superposition of irradiance on a white, <strong>La</strong>mbertian screen).<br />

There is a null element, the “empty beam”, which is<br />

simply no radiation at all.<br />

S would be a linear space were it not for the fact that<br />

the radiance has to be non–negative.<br />

Thus real (actual) beams fill the “positive part” S + of<br />

the linear (infinitely dimensional) “space of beams” S.<br />

“Colors” (to be exp<strong>la</strong>ined!) are elements of a 3 D lin-<br />

ear space C. (The “trichromacy” was first suggested by<br />

Thomas Young.) 7

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