Gerenuk
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Hi,
I was wondering why the wave-function in quantum mechanics is complex. There are a lot of threads in the physics section and I've downloaded a lot of papers, but they seem quite technical. So I'd like to examine the following idea (sorry if I use sloppy terms ;) ):
I have an orthonormal basis of vectors/functions which can be labeled with two indices f_{E,k} and which are "two-dimensional". It's not just a column vector, but rather f_{E,k}(x,t). The vector algebra is undetermined (could be any linear algebra).
Now I have two conditions
k^2f_{E,k}+V(x,t)f_{E,k}=Ef_{E,k}
\forall a: f_{E,k}(x+Ea,t+ka)=f_{E,k}(x,t)
(btw, the second is in a way equivalent to E=mc^2)
Is it now possible to proof that the only orthonormal solution for this is a complex algebra with
f_{E,k}(x,t)=\exp(i(kx-Et))?
Please add definitions (for scalar product and so on) as appropriate!
Or which other definitions/conditions do I need to get that complex solution uniquely?
I was wondering why the wave-function in quantum mechanics is complex. There are a lot of threads in the physics section and I've downloaded a lot of papers, but they seem quite technical. So I'd like to examine the following idea (sorry if I use sloppy terms ;) ):
I have an orthonormal basis of vectors/functions which can be labeled with two indices f_{E,k} and which are "two-dimensional". It's not just a column vector, but rather f_{E,k}(x,t). The vector algebra is undetermined (could be any linear algebra).
Now I have two conditions
k^2f_{E,k}+V(x,t)f_{E,k}=Ef_{E,k}
\forall a: f_{E,k}(x+Ea,t+ka)=f_{E,k}(x,t)
(btw, the second is in a way equivalent to E=mc^2)
Is it now possible to proof that the only orthonormal solution for this is a complex algebra with
f_{E,k}(x,t)=\exp(i(kx-Et))?
Please add definitions (for scalar product and so on) as appropriate!
Or which other definitions/conditions do I need to get that complex solution uniquely?