A wave function can be written in a variety of bases. Do you know what a basis is? When I say a wave function is continuous, I am of course referring to it being continuous in some basis. For the particle in a box, the wave function in position space is continuous, and in energy space is discrete. The energy eigenvalues are discrete. The position eigenvalues are continuous.
It really seems to me that you might not have a full grasp of quantum mechanics.
You should really provide a cite, or at least an argument, for this statement. What makes it so that out of a continuous energy spectrum, only a discrete set of values is observable in an experiment? Why is some value E observable, but E + e for arbitrarily small e not? You may not be able to distinguish them in a measurement, but this a) has nothing to do with quantum mechanics, b) does not change the fact that the set of possible values is continuous, not discrete.
How do you tell, for a single measurement, whether it came from a continuous or discrete set? Could you create, in a purely classical world, an instrument that could return a value from a continuous set?
No. If the eigenvalues of the original system are continuous, then the eigenvalues of the system+measurement device after measurement will be continuous, and the eigenvalues of the system+measurement device+experimenter after looking at the measurement device will be continuous and so on, until eventually you end up with a universal wavefunction with continuous eigenvalues.
What do you expect when your retorts are as incoherent/irrelevant as:
“The representation of the wave function is independent of the eigenvalues.”
So? The point is that the wave function can have both continuous and discontinuous eigenvalues. Your continuing to harp on the fact that the energy eigenvalues are discrete is totally irrelevant.