gitano
- 11
- 0
Hi,
At one point in Chapter 1 of Sakurai he is deriving the momentum operator in the position basis - I just don't see how he makes some of the mathematical leaps (at least leaps for me) between the following expressions
[tex] \int dx' |x' + \Delta x'> < x' | \alpha > = \int dx' | x' > < x' - \Delta x' | \alpha >[/tex]
[tex]= \int dx' | x' > \left ( < x' | \alpha > - \Delta x' \frac{\partial}{\partial x'} < x' | \alpha > \right )[/tex]
I guess I kind of see that the [tex]|x' + \Delta x' >[/tex] acting on the position wavefunction of alpha is the same as translating the position wavefunction to the right by [tex]\Delta x'[/tex]. Is this the logic here or is there a more mathematical way of showing it.
Now, the transition to the last equality is even less intuitive for me.
At one point in Chapter 1 of Sakurai he is deriving the momentum operator in the position basis - I just don't see how he makes some of the mathematical leaps (at least leaps for me) between the following expressions
[tex] \int dx' |x' + \Delta x'> < x' | \alpha > = \int dx' | x' > < x' - \Delta x' | \alpha >[/tex]
[tex]= \int dx' | x' > \left ( < x' | \alpha > - \Delta x' \frac{\partial}{\partial x'} < x' | \alpha > \right )[/tex]
I guess I kind of see that the [tex]|x' + \Delta x' >[/tex] acting on the position wavefunction of alpha is the same as translating the position wavefunction to the right by [tex]\Delta x'[/tex]. Is this the logic here or is there a more mathematical way of showing it.
Now, the transition to the last equality is even less intuitive for me.