Is the More Operator Correct for \langle x'|\hat{p} \hat{x} | x \rangle?

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BeauGeste
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Consider
[tex]\langle x'|\hat{p} \hat{x} | x \rangle[/tex].
Are these steps correct?
1. [tex]\hat{x}[/tex] operates on the x eigenstate to get
[tex]\langle x'|\hat{p} x | x \rangle[/tex].
2. x is a c-number so can be pulled out to get
[tex]x \langle x'|\hat{p} | x \rangle[/tex].
3. [tex]x \langle x'|\hat{p} | x \rangle = x \frac{\partial}{\partial x'}\delta (x'-x)[/tex]

The part I'm most wary on is 2 where I pulled x out. It seems like the p operator is acting on it so I shouln't be able to do that.

Alternatively, could I do the following:
1. have p operate on [tex]\hat{x}[/tex] first to get
[tex]\frac{\partial}{\partial x'}x' \delta (x'-x)[/tex]
2. Which becomes
[tex]\delta (x'-x) + x' \delta'(x'-x)[/tex]

Is one of these two routes incorrect?
 
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BeauGeste said:
2. x is a c-number so can be pulled out

Yes, you can do that. Operators do not act on c-numbers.

Eugene.
 
Both are correct (except you dropped a factor of -i*hbar in line 3, but you also dropped it in the 2nd part). You can check that your two final expressions are equal by integrating them against a test funtion of either x or x'.
 
Won't you get the same thing for
[tex]\langle x'|\hat{x} \hat{p} | x \rangle[/tex]
though? That would imply the two operators commute.
 
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BeauGeste said:
The part I'm most wary on is 2 where I pulled x out. It seems like the p operator is acting on it so I shouln't be able to do that.
It's not a problem because [itex]\hat{p}[/itex] is not a differential operator: [itex]\hat{p}[/itex] is a linear operator acting on states. Because it's linear, it commutes with all complex numbers.


[itex]\hat{p}[/itex] only turns into a differential operator when everything's written out in the position representation -- in that case, you would have

[tex] \langle x' | \hat{p} \hat{x} | x \rangle<br /> =<br /> \int_{-\infty}^{+\infty} \delta(x' - \xi) \left(-i \hbar \frac{\partial}{\partial \xi} \right)<br /> \xi \delta(x - \xi) \, d\xi[/tex]

and now it's differently obvious, since x clearly commutes with [itex]\partial / \partial \xi[/itex].
 
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