- #1
andresordonez
- 68
- 0
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.