andresordonez
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Hi, while reading the section about the parity operator from the QM book by Cohen-Tannoudji (complement F II, page 192), I found this:
"
Consider an arbitrary vector [tex]|\psi\rangle[/tex] of [tex]\mathcal{E}_\vec{r}[/tex]:
[tex]|\psi\rangle = \int d^3 r \psi(\vec{r})|\vec{r} \rangle[/tex]
If the variable change [tex]\vec{r'}=-\vec{r}[/tex] is performed, [tex]|\psi \rangle[/tex] can be written:
[tex]|\psi \rangle = \int d^3 r' \psi (-\vec{r'}) |-\vec{r'} \rangle[/tex]
"
But [tex]d^3 r = dx dy dz[/tex] and after the variable change I get [tex]d^3 r' = dx' dy' dz' = - dx dy dz[/tex], so I don't understand what happened to that minus sign. It should be:
[tex]|\psi \rangle = -\int d^3 r' \psi (-\vec{r'}) |-\vec{r'} \rangle[/tex]
right??
Someone told me it had to do something with the meaning of the differential volume, but I'm not sure about that.
Thanks.
"
Consider an arbitrary vector [tex]|\psi\rangle[/tex] of [tex]\mathcal{E}_\vec{r}[/tex]:
[tex]|\psi\rangle = \int d^3 r \psi(\vec{r})|\vec{r} \rangle[/tex]
If the variable change [tex]\vec{r'}=-\vec{r}[/tex] is performed, [tex]|\psi \rangle[/tex] can be written:
[tex]|\psi \rangle = \int d^3 r' \psi (-\vec{r'}) |-\vec{r'} \rangle[/tex]
"
But [tex]d^3 r = dx dy dz[/tex] and after the variable change I get [tex]d^3 r' = dx' dy' dz' = - dx dy dz[/tex], so I don't understand what happened to that minus sign. It should be:
[tex]|\psi \rangle = -\int d^3 r' \psi (-\vec{r'}) |-\vec{r'} \rangle[/tex]
right??
Someone told me it had to do something with the meaning of the differential volume, but I'm not sure about that.
Thanks.