On Aug 13, 4:38 pm, "Jay R. Yablon"
> "Igor Khavkine"
> news: @ ...
[...examples of quantum Hamilton's principle function observables...]
> Now, how do you go from these examples to S = int_{-oo to +oo} L (t,x)
> d^4x? Is there some general rule here? Do +oo and -oo lend themselves
> to imposing boundary conditions that can give us a general answer?
To answer this question, you first need to find what is the field
theory quantity analogous to x(t) in my earlier examples. Then, follow
the steps I already outlined.
> Also, perhaps as stepping stones to answer this, permit me please to ask
> the following:
>
> 1) can you come up with a classical example that yields a discrete
> spectrum?
No, impossible. Classical observables are either constant or take on
continuous ranges of values.
> 2) can you come up with a quantum theory example that yields a discrete
> spectrum?
Not off hand.
> 3) can you articulate a general rule which will tell us when we will
> obtain a continuous spectrum and when we will obtain a discrete
> spectrum?
Not off hand.
Igor