What is the Inverse of Momentum Operator in One Dimensional Problems?

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Homework Help Overview

The discussion revolves around finding the inverse of the momentum operator in one-dimensional quantum mechanics. Participants are exploring the mathematical implications and properties of this operator.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants are considering the action of the momentum operator on wavefunctions and discussing how to derive the inverse operator. There are questions about the notation and the implications of using certain representations.

Discussion Status

Some guidance has been offered regarding the action of the momentum operator and its relationship to the fundamental theorem of calculus. Participants are actively engaging with each other's ideas, but there is no explicit consensus on the final form of the inverse operator.

Contextual Notes

There are indications of potential confusion regarding notation, particularly the use of 1/p to represent the inverse of the momentum operator, which some participants suggest may not be appropriate.

ghazal-sh
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hi every body!
I'm looking for inverse of momentum operator in one dimensional problem.I have no idea to solve it!please help me!
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so sorry about my bad speaking!
 
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Welcome to PF!

ghazal-sh said:
hi every body!
I'm looking for inverse of momentum operator in one dimensional problem.I have no idea to solve it!please help me!

hi ghazal-sh! Welcome to PF! :smile:

Thankyou for the PM.

Can you show us the whole problem? :smile:
 
Can you show us the whole problem?
thanks for your attention!::smile:
the problem is just finding inverse of P!
 
Start by considering the action of the momentum operator [itex]P[/itex] on an arbitrary wavefunction [itex]\psi(x)[/itex]...What is that?
 
Start by considering the action of the momentum operator LaTeX Code: P on an arbitrary wavefunction LaTeX Code: \\psi(x) ...What is that?
thanks!how can you reach to 1/p with this approach?
of course I found the answer.start by calculating expectation value of 1/p in momentum space (so easy)and then use Fourier transform of the wave functions.after so simple calculation you can see that:1/p =integral of dx
 
Last edited:
ghazal-sh said:
thanks!how can you reach to 1/p with this approach?
of course I found the answer.start by calculating expectation value of 1/p in momentum space (so easy)and then use Fourier transform of the wave functions.after so simple calculation you can see that:1/p =integral of dx

Well, the action of [itex]P[/itex] on [itex]\psi(x)[/itex] is of course just [itex]P\psi(x)=-i\hbar \frac{d}{dx} \psi(x)[/itex]...what do you get when you multiply both sides of this equation by the inverse of P (from the left), [itex]P^{-1}[/itex]?... compare that to the fundamental theorem of calculus and it should be apparent what [itex]P^{-1}[/itex] is.

P.S. using 1/p to represent the inverse is usually bad notation when dealing with operators.
 

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