Telling whether a wave function might have physical graph

AI Thread Summary
The discussion centers on the physical significance of two wave functions, with one being deemed valid and the other not. The wave function on the left is criticized for being unbounded, which implies that it could suggest the object exists at an infinite number of locations simultaneously, contradicting the principles of probability distribution. The requirement for a wave function to represent a probability distribution is that the integral of its square must be normalized. Participants agree that the unbounded nature of the left wave function makes normalization impossible. This highlights the importance of bounded wave functions in quantum mechanics.
Von Neumann
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Problem:

Which of the wave functions shown might conceivably have physical significance?

Solution:

I have attached a drawing of the two wave functions. According to my book, the one on the right could have physical significance, while the one on the left does not. Can anyone explain why not? They are both single valued, differentiable functions, so I don't see why the left one is apparently disqualified. Thanks for any help.
 

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Von Neumann said:
Problem:

Which of the wave functions shown might conceivably have physical significance?

Solution:

I have attached a drawing of the two wave functions. According to my book, the one on the right could have physical significance, while the one on the left does not. Can anyone explain why not? They are both single valued, differentiable functions, so I don't see why the left one is apparently disqualified. Thanks for any help.
attachment.php?attachmentid=56573&d=1362960230.jpg


I assume the graph on the left continues upward toward ∞ without a bound.
 
Hmmm, that never occurred to me. How would that take away from its physical significance?
 
Well, since the wave function is proportional to finding the object at a specific place at a specific time, and unbounded wave function doesn't make sense. Right?
 
Von Neumann said:
Well, since the wave function is proportional to finding the object at a specific place at a specific time, and unbounded wave function doesn't make sense. Right?

Yes.

Why doesn't it make sense?
 
SammyS said:
Yes.

Why doesn't it make sense?

It doesn't make sense logically because, according to the unbounded function, the object described by the wave function is located at an infinite number of places at the same time.
 
Von Neumann said:
It doesn't make sense logically because, according to the unbounded function, the object described by the wave function is located at an infinite number of places at the same time.
In order for the square of the wave function to represent a probability distribution, what has to be true of the integral of the square of the wave function ?
 
SammyS said:
In order for the square of the wave function to represent a probability distribution, what has to be true of the integral of the square of the wave function ?

The integral of the square of the wave function must be normalized, correct? Are you hinting that it is impossible to normalize the diverging function?
 
Von Neumann said:
The integral of the square of the wave function must be normalized, correct? Are you hinting that it is impossible to normalize the diverging function?
It is impossible if the integral diverges.
 
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