Position operator in momentum space (and vice-versa)

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SUMMARY

The discussion centers on the transformation of operators between position space and momentum space using Fourier transforms. Specifically, the momentum operator in position space, defined as \( p = -i\hbar \frac{\partial}{\partial x} \), transforms into a multiplication operator in momentum space. Participants emphasize the importance of applying the original definition of the momentum operator to the state vector \( |p\rangle \) and simplifying to understand the transformation process. This leads to a clear understanding of how the position operator also transforms accordingly.

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  • Understanding of Fourier transforms in quantum mechanics
  • Familiarity with quantum operators and their representations
  • Knowledge of the momentum operator definition in position space
  • Basic grasp of commutation relations in quantum mechanics
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smiler2505
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Hi all,

I understand how to transform between position space and momentum space; it's a Fourier transform:
\varphi|p>=\frac{1}sqrt{2\hbar\pi}\int_{\infty}^{\infty} <x|\varphi> exp(-ipx/\hbar)dx

But I can't figure out how to transform the operators. I know what they transform into (e.g., the p operator in position space goes to 'p' in momentum space), but not how.

Any help? Thanks
 
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smiler2505 said:
Hi all,

I understand how to transform between position space and momentum space; it's a Fourier transform:
\varphi|p>=\frac{1}sqrt{2\hbar\pi}\int_{\infty}^{\infty} <x|\varphi> exp(-ipx/\hbar)dx

But I can't figure out how to transform the operators. I know what they transform into (e.g., the p operator in position space goes to 'p' in momentum space), but not how.

Any help? Thanks

Apply the original definition of the momentum operator to the |p> just defined, and simplify, and you'll see that the effect is just multiplication with p. Similarly, you can verify the transformed formula for position.
 
Here is a detailed explanation of why p = -i\hbar \partial / \partial x in position space, starting from the commutators of x and p.
 

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