Position Operator: f(\hat{x})=f(x)? Effects on g(x)

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Homework Help Overview

The discussion revolves around the position operator in quantum mechanics, specifically the relationship between a function of the position operator, f(âx), and the function evaluated at the variable x, f(x). Participants explore the implications of applying such functions to another function g(x).

Discussion Character

  • Conceptual clarification, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants question the notation used, particularly the distinction between x and âx. There are attempts to clarify the conditions under which f(âx) equals f(x) and discussions about the implications of applying f(âx) to g(x). Some also raise concerns about the meaning of certain expressions involving the position operator.

Discussion Status

The discussion is ongoing, with participants seeking clarification on notations and definitions. Some guidance has been offered regarding the conditions under which the initial statement may hold true, but there is no explicit consensus on the broader implications or interpretations of the operator's behavior.

Contextual Notes

There are indications of missing information regarding the definitions of the operators and functions involved, as well as potential complexities related to series expansions and convergence in operator theory.

zhaiyujia
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is it true that: [tex]f(\hat{x})=f(x)[/tex]?
What will happen if [tex]f(\hat{x})=\frac{\hat{x}}{\hat{x}+1}[/tex] act on [tex]g(x)[/tex]?
 
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Can you first clarify your notations, and also show work done and relations you know of etc.
 
Who's "x" and who's [itex]\hat{x}[/itex] ?
 
I assume that x is the eigenvalue of a position operator [itex]\hat x[/itex].

If f is a function that only depends on the operator [itex]\hat x[/itex], then the statement is true, as can be seen by expanding [itex]f(\hat x)[/itex] in a series and acting it on a ket [itex]\left| x \right>[/itex].
In general this need not be true though, e.g.
[tex]f(\hat x, \hat p) = \hat x \hat p[/itex] will not give <i>x p</i>. <br /> <br /> For the last question, what is [itex]1/\hat x[/itex] supposed to mean?[/tex]
 
If [itex]\hat{x}[/itex] is the position operator in QM, then you might as well consider the Hilbert space as being [itex]L^{2}(\mathbb{R},dx)[/itex] and you will find that the Schwartz space [itex]S(\mathbb{R})[/itex] is not only a domain for essential selfadjointness of [itex]\hat{x}[/itex], but also a domain for any polynomial function of the operator "[itex]\hat{x}[/itex]". Now, series expansions of operators is a tricky business (due to convergence issues) and now I'm too tired to go there.
 

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