PeterDonis
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jlcd said:Is the above statement colored by intepretation?
No.
jlcd said:He thought of classical physics as an approximation derived from quantum physics.
That's how it is viewed now that we know about quantum physics, yes.
jlcd said:This means if for sake of discussion an object had no position basis
A basis is not a property of an object. It's a choice humans make in the math for convenience. It makes no sense to say an object has or doesn't have a position basis or any other basis.
jlcd said:In your case, he thought you answered differently because you thnk of classical physics as independent of quantum physics, is this right?
No.
jlcd said:So for those who think the wave function or state vectors are the objects themselves such as Many worlders, quantum physics is both map and territory?
No. Saying "the wave function is real" does not mean that the mathematical expression you write down on a piece of paper to describe a quantum system (the map) is the same as the system itself (the territory). Quantum objects don't know or care what math you use.
jlcd said:So when you believe positon basis has nothing to do with classical positions of objects. You were thinking in terms of the latter or Copenhagen context.
No. As I said above, what I said is independent of any particular interpretation.
jlcd said:While the Ph.D. expert was thinking of the former where the state vectors are the objects themselves hence the classical positions are the actual position basis themselves?
I don't know what your Ph. D. expert was thinking.
However, perhaps I can help by expanding a bit on what I said about classical positions. Consider a macroscopic object like a baseball. What is its "classical position"? Mathematically, it is the expectation value of the center of mass position of the baseball. In other words, there is a "center of mass position" operator ##\hat{P}_{\text{CM}}## which, given the quantum state ##| \psi \rangle## of the ball, has an expectation value. ##\langle \psi | \hat{P}_{\text{CM}} | \psi \rangle##. The Ehrenfest theorem, which @Mentz114 mentioned, shows that this expectation value obeys the classical equations of motion for the center of mass of the ball; that's what justifies interpreting it as the "classical position" of the ball.
Now, what does this operator have to do with the "position basis" at the quantum level? Nothing. Saying that the center of mass of the ball is at some particular position tells you nothing at all about the position of any of the individual atoms in the ball. (More precisely, nothing at all beyond that it's within some spatial region around the center of mass.) It doesn't even tell you that any of the atoms in the ball even has a particular position. All of them can be fluctuating at the quantum level and never be in a position eigenstate at all. In fact, all of the atoms in the ball are entangled with each other, so none of them even has a well-defined wave function by itself, much less a wave function that is in a position eigenstate. (Strictly speaking, exact position eigenstates can't exist physically, but we can read "wave function with a sufficiently narrow spread in position" for "position eigenstate" above and it won't change any of what I said.) And, as I said before, the wave function of the ball as a whole, i.e., the ##| \psi \rangle## that appears in the expectation value above, is a function on a space with ##3 \times 10^{25}## dimensions or so (even more if we include spin degrees of freedom), not a function on ordinary 3-dimensional space.