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(R0 embedded in R3)

One may object that by Stavenga's own example of the elementary particle, the current definition of 'content' is failing with regard to R3, as literally all the physical parameters of the particle are directly retrievable by just measuring the relevant analogues in the photograph.

Yet this is allowed for on the assumption that the explicity of the-particle's-parameters-viewed-as-R0-relation is contained in the R3-relation of the photograph by which obviously a typical quale is directly expressed.

Obvious in this respect also is the example of modern art!

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