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

Join the discussion
Registration is free. Ask a follow-up in this thread, or start your own.
4 replies · 6K views
zhaiyujia
Messages
6
Reaction score
0
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]?
 
Physics news on Phys.org
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.