silverwhale
- 78
- 2
In the book "Wachter, relativistic quantum mechanics", in page 5, the KG eq. is introduced as follows:
[tex]-\hbar^2 \frac{\partial^2 \phi(x)}{\partial t^2} = (-c^2 \hbar^2 \nabla^2 + m^2_0 c^4) \phi(x).[/tex]
Now I tried to solve this equation using the separation ansatz (product ansatz).
I get:
[tex]\phi (ct) = exp [\pm \frac{ i p_0 ct}{\hbar} ],[/tex]
and
[tex]\psi (x) = exp[\pm \frac{i \vec{p} \cdot \vec{x}}{\hbar}].[/tex]
Where the usual relativistic four-momentum conservation equation holds.
Now, this amounts to four combinations of solutions. But in the book, only two are written, namely:
[tex]\phi^{(1)}_p= e^{-i (c p_0 t - \vec{p} \cdot \vec{x})/ \hbar},[/tex]
[tex]\phi^{(2)}_p= e^{+i (c p_0 t - \vec{p} \cdot \vec{x})/ \hbar}.[/tex]
I really, really want to solve the equation; I feel a little bit frustrated because I don't get only the two solutions. Basically I am halfway there but I don't know what to do next.
So any help would be greatly appreciated!
[tex]-\hbar^2 \frac{\partial^2 \phi(x)}{\partial t^2} = (-c^2 \hbar^2 \nabla^2 + m^2_0 c^4) \phi(x).[/tex]
Now I tried to solve this equation using the separation ansatz (product ansatz).
I get:
[tex]\phi (ct) = exp [\pm \frac{ i p_0 ct}{\hbar} ],[/tex]
and
[tex]\psi (x) = exp[\pm \frac{i \vec{p} \cdot \vec{x}}{\hbar}].[/tex]
Where the usual relativistic four-momentum conservation equation holds.
Now, this amounts to four combinations of solutions. But in the book, only two are written, namely:
[tex]\phi^{(1)}_p= e^{-i (c p_0 t - \vec{p} \cdot \vec{x})/ \hbar},[/tex]
[tex]\phi^{(2)}_p= e^{+i (c p_0 t - \vec{p} \cdot \vec{x})/ \hbar}.[/tex]
I really, really want to solve the equation; I feel a little bit frustrated because I don't get only the two solutions. Basically I am halfway there but I don't know what to do next.
So any help would be greatly appreciated!