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I guess it doesn't matter for this proof, but shouldn't there be an additional "h-bar" in the (i/2m) when you use the schrödinger equation to solve for the time derivative of the wave funkton? cause the hamiltonian is "H=( -h²/2m)+V"
How to find normalization constt? Write example on it .
dude read the book
I guess it doesn't matter for this proof, but shouldn't there be an additional "h-bar" in the (i/2m) when you use the schrödinger equation to solve for the time derivative of the wave funkton? cause the hamiltonian is "H=( -h²/2m)+V"
How to find normalization constt?
Write example on it .
dude read the book