twofish-quant said:
The other thing to be careful here is "proof by lack of imagination." In order to prove non-existence, you have to show that something really bad happens if something did exist. I can think of a lot of bad things that would happen if you had physical measurements that were none Lorenz invariant, or if quantum observations didn't reduce to a single number.
However, asserting that something is impossible because one can't think of counterexamples is a bad way of showing that something is impossible.
Throughout this thread, we have been discussing the fact that all measured quantities must be scalars with respect to
coordinate transformations of spacetime, a context to which none of your examples has been relevant.
However, this goes beyond merely spacetime scalars.
Any measurement of a vector quantity (in the vector space sense, not in the computer science sense)
must come by choosing a basis and projecting out components, thereby measuring a set of scalars. If you think about it for a moment, you will see that this statement is a trivial tautology. What I'm really saying here is that
every measurement is a comparison.
After all, that is what we really mean, isn't it? When we say something is "2 meters", all we're saying is it's twice as long as a certain metal bar in France. (Or, in modern SI, it's twice the distance light travels during so many oscillations of Cesium 133.)
Color. Color requires three components to be specified, but color is independent of those components. You can specific color in terms of RGB, or CMYK or pantone or color temperature, but color is independent of those measurement. Because you need multiple components to specific color, and the existence of color is *independent* of those components, its a vector field, and more than a collection of measurements.
RGB, HSB, CMYK, and temperature are all
coordinates on color space. They emphatically do
not obey the linear transformation law and axioms of a vector basis. In fact, I'm not convinced color space is a vector space at all, if we mean the color space that is relevant to "perceived color". (Of course, we can
define color spaces that are vector spaces, but these might have nothing to do with actual color perception).
You could probably geometrize the idea of color space if you like, and make it a manifold, possibly with notions of parallel transport. Who knows, maybe there's a useful way to model some psycho-physical process using a color space bundle over spacetime.
At any rate, "color" is measured by first comparing incoming light against certain bands of frequency; i.e., taking an inner product in frequency space against certain basis vectors in order to form a collection of scalars. These scalars can then be used as a coordinate system on color space. This method works for RGB, CMYK, and color temperature type coordinates. Mapping physical observables to HSB coordinates is more complicated, and will require projecting the incoming spectrum onto several bands and doing some analysis with the results.
Since frequency space is infinite-dimensional, there is no real reason for color space to be 3-dimensional; the ultimate reason is that we have 3 kinds of color receptors in our eyes (which project the spectrum onto 3 bands). Other animals have 2-dimensional, or sometimes 4-dimensional color spaces.