A. Neumaier said:
The electromagnetic field in its Silberstein representation is another, classical complex-valued beable!
I don't think the Silberstein representation should be thought of as fundamental or ontological (even if classical EM would be true of Nature). It is not Lorentz-covariant, and it also does not nicely express the Lorentz force law, which is the main observable effect of the fields.
A. Neumaier said:
But then ##i## appears in the formula for the ##\tilde H## of a harmonic oscillator. So your propsed recipe doesn't help at all.
Indeed, once we start listing Hamiltonians for systems that actually turn up in the world, we quickly see that they look much more natural as operators on complex Hilbert space. That is part of what we wish to explain. However, note that if necessary, was can always do things in real Hilbert space, by having separate dimensions for (what in complex QM we call) the real and imaginary parts of each dimension coefficient. Then the imaginary number ##i## is replaced by the operator ##J## which exchanges them anti-symmetrically.
stevendaryl said:
The ontological question of what the wave function means is independent, it seems to me, of whether or not it uses complex numbers. If you had a physical interpretation that said something like "the wave function is a length of some object" or "the wave function is a probability", then certainly complex values are unphysical. But it seems to me that worrying about whether it's complex prior to coming up with a physical meaning for it is putting the cart before the horse.
I am referring to interpretations like MWI or dBB, or even GRW, where the wavefunction is seen as a fundamental object, like a field. Indeed in may be the
only fundamental object. So that answers what its "meaning" is, and we are free to ruminate on whether complex values seem appropriate.
I do magnanimously allow others to not share my niggling feelings and ruminations.
stevendaryl said:
Certainly, you can always eliminate complex numbers by using matrices instead of numbers, or by using quaternions, or whatever. But I don't see that such a change is anything more than aesthetic.
There is one important difference between complex QM and the real QM generated by thinking of the real and imaginary parts as different dimensions: the question of which operators count as linear. Operations like complex conjugation, or selecting the real or imaginary part, are linear on ##\mathbb R^2## but not on ##\mathbb C##, and similarly for larger Hilbert spaces. When we say that QM is complex rather than real, we are referring to the fact that all of the unitaries and observable operators that show up in QM are complex-linear, rather than merely linear in the corresponding real space. In other words, looking from the real-QM perspective, there is a pairing of dimensions into effective complex dimensions, that is maintained by all physical operators. One effect of this is that the state ends up only being fixed (by physical outcomes) up to a complex phase, or in real-QM terms, up to a 2-D rotation. On the face of it, this seems like good enough reason to conclude that the real-QM description is just unnatural and our world does use complex QM. This is something that could have been otherwise, and we are left to asking God how the choice was made. Perhaps He wants us to be able to do local tomography of states.
But if it turns out that this pairing is actually completely natural and even inevitable, for any real Hilbert space with the right symmetries, then that gives us a different perspective. That would mean there really are not two options that could have been, but only two self-sufficient ways of expressing the same theory. The complex version will be the neater and more convenient one, but God need not commit to it.
And yes, this would explain why actual Hamiltonians like the harmonic oscillator look so ugly in real QM: it is because we are expressing things in terms of an observable position operator, and that operator must comply with the emergent complex structure - meaning it cannot have nondegenerate real-QM eigenstates (I mean in the limiting, rigged-Hilbert-space sense in which the standard non-relativistic position operator does have eigenstates), but only degenerate and indistinguishable pairs of states.