Eigenvalue of position operator and delta function.

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SUMMARY

The discussion centers on the eigenvalue of the position operator \(\overset {\wedge}{x}\) in quantum mechanics, specifically addressing the relationship between the delta function and the position operator. The conclusion drawn is that \(\langle x|\overset {\wedge}{x}|x'\rangle = x\delta(x-x')\), which leads to the assertion that \(\overset {\wedge}{x}|x\rangle = x|x\rangle\). The confusion arises from the definition of the delta function, with participants questioning whether \(\delta(x-x')\) equals \(\langle x|x'\rangle\) or \(\langle x'|x\rangle\). The discussion also highlights the lack of clarity regarding hermitian operators in the referenced literature.

PREREQUISITES
  • Understanding of quantum mechanics principles, particularly operators and eigenvalues.
  • Familiarity with the Dirac delta function and its properties.
  • Knowledge of bra-ket notation in quantum mechanics.
  • Basic concepts of hermitian operators and their significance in quantum theory.
NEXT STEPS
  • Research the properties of the Dirac delta function in quantum mechanics.
  • Study the implications of hermitian operators on eigenvalues and eigenstates.
  • Explore the mathematical derivation of position operators in quantum mechanics.
  • Investigate the relationship between \(\delta(x-x')\) and \(\delta(x'-x)\) in detail.
USEFUL FOR

Quantum physicists, students of quantum mechanics, and researchers exploring the mathematical foundations of quantum theory will benefit from this discussion.

maser
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I'd like to show that if there exists some operator [itex]\overset {\wedge}{x}[/itex] which satisfies [itex]\overset {-}{x} = <\psi|\overset {\wedge}{x}|\psi>[/itex], [itex]\overset {\wedge}{x}|x> = x|x>[/itex] be correct.

[itex]\overset {-}{x} = \int <\psi|x> (\int<x|\overset {\wedge}{x}|x'><x'|\psi> dx')dx = \int <\psi|x> (x<x|\psi>)dx = \int <\psi|x> (x\int<x|x'><x'|\psi> dx')dx[/itex]

So I concluded that [itex]<x|\overset {\wedge}{x}|x'> = x<x|x'>[/itex] and if we factor out x' I can get [itex]<x|\overset {\wedge}{x} = x<x|[/itex] but not [itex]\overset {\wedge}{x}|x> = x|x>.[/itex]

However, fortunately I could find a book saying,

"[itex]<x|\overset {\wedge}{x}|x'> = x\delta(x-x')[/itex] where [itex]\delta(x-x') = <x'|x>[/itex]. Then you can work out the result that [itex]\overset {\wedge}{x}|x> = x|x>.[/itex]"

I was confused by the definition of delta function in this book and confirmed [itex]\delta(x-x') = <x|x'>[/itex] in some documents on the internet. But I cannot convince myself that the definition [itex]\delta(x-x') = <x'|x>[/itex] is an error of the book, because the definition is used in the book many times. Furthermore the book don't have any ideas of hermitian operators.

Here, I come to have two questions.

1. [itex]\delta(x-x') = <x|x'> or <x'|x> ?[/itex] Which is correct answer?
2. How to prove [itex]\overset {\wedge}{x}|x> = x|x>[/itex] from [itex]<x|\overset {\wedge}{x}|x'> = x\delta(x-x')[/itex] without the properties of hermitian operator?
 
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What is the relation between [itex]\delta(x-x')[/itex] and [itex]\delta(x'-x)[/itex]?
 

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