I How to apply potential operator ##V(\hat{x})##

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The discussion centers on clarifying the action of the potential operator ##V(\hat{x})## on position kets, specifically whether it is defined as ##\hat{V}(x)|x\rangle=V(x)|x\rangle##. It is confirmed that for any ket ##|\psi\rangle##, the expression ##V(\hat{x})|\psi\rangle## can be represented as an integral involving ##V(x)## and position kets. Additionally, the transformation of the operator on negative position kets is explored, leading to the expression ##V(\hat{x}) \int d x|-x\rangle\langle x \mid \psi\rangle## equating to ##\int d x V(-x)|-x\rangle\langle x \mid \psi\rangle##. The participants express uncertainty about the implications of this transformation but agree that the mathematical representations appear correct. Overall, the discussion effectively clarifies the operator's action on position states within quantum mechanics.
Kashmir
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I want some clarification on the potential operator ##V(\hat{x})##. Can you please help me

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Is the action of ##V(\hat{x})## defined by its action on the position kets as ##\hat{V}(x)|x\rangle=V(x)|x\rangle##?

Then we'd have for any ket ##|\psi\rangle## that ##V(\hat{x})|\psi\rangle## ##=V(\hat{x}) \int d x|x\rangle\langle x \mid \psi\rangle####=\int d x V(x)|x\rangle\langle x \mid \psi\rangle##

And ##V(\hat{x}) \int d x|-x\rangle\langle x \mid \psi\rangle## equals ##\int d x V(-x)|-x\rangle\langle x \mid \psi\rangle##
Is that correct?
 
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Kashmir said:
Is the action of ##V(\hat{x})## defined by its action on the position kets as ##\hat{V}(x)|x\rangle=V(x)|x\rangle##?

Then we'd have for any ket ##|\psi\rangle## that ##V(\hat{x})|\psi\rangle## ##=V(\hat{x}) \int d x|x\rangle\langle x \mid \psi\rangle####=\int d x V(x)|x\rangle\langle x \mid \psi\rangle##
This looks right.
Kashmir said:
And ##V(\hat{x}) \int d x|-x\rangle\langle x \mid \psi\rangle## equals ##\int d x V(-x)|-x\rangle\langle x \mid \psi\rangle##
I'm not sure what this means. But, it looks right.
 
I get this expression ##V(\hat{x}) \int d x|-x\rangle\langle x \mid \psi\rangle## while doing another problem ( commutator of parity and V)
 
An antilinear operator ##\hat{A}## can be considered as, ##\hat{A}=\hat{L}\hat{K}##, where ##\hat{L}## is a linear operator and ##\hat{K} c=c^*## (##c## is a complex number). In the Eq. (26) of the text https://bohr.physics.berkeley.edu/classes/221/notes/timerev.pdf the equality ##(\langle \phi |\hat{A})|\psi \rangle=[ \langle \phi|(\hat{A}|\psi \rangle)]^*## is given but I think this equation is not correct within a minus sign. For example, in the Hilbert space of spin up and down, having...

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