Dirac Notation frees up from having to pick a basis
Suppose we have momentum states
Then
where
We’ll show later that
Therefore by projecting:
So the momentum is the Fourier Transform of the position.
Dirac Notation frees up from having to pick a basis
Suppose we have momentum states
Then
where
We’ll show later that
Therefore by projecting:
So the momentum is the Fourier Transform of the position.