nomadreid
Gold Member
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I am not sure if I should be posting this under QM or under Linear Algebra, since it appears to be an algebraic step that I do not see, and am asking the wonderful people on this forum to spell it out for me. In John Baez's derivation of the Energy-time Uncertainty relation,
http://math.ucr.edu/home/baez/uncertainty.html
there is the following step, which first I will quote and then state my question:Selecting an observable A which does not commute with H,
"< [H,A] > = <ψ, [H,A] ψ>
is i\hbar times the time derivative at t = 0 of <ψ, A ψ>, as you can see if you note that the solution to the Schrödinger equation can be written in the form
U(t) ψ = exp(-itH/\hbar) ψ
Thus
<[H, A]> = i\hbar d<A>/dt"
If he is using the commutator [H,A] as the operator U(t), then I do not see how to get from
<[H, A]> =<ψ, exp(-itH/\hbar) ψ>
to
i\hbar d<A>/dt
(i.e., i\hbar d<ψ, Aψ>/dt)
If he is not using the commutator as the operator, then I am lost even worse.
I would be very grateful for anyone showing me this step more explicitly. ("Derivation for Dummies")
http://math.ucr.edu/home/baez/uncertainty.html
there is the following step, which first I will quote and then state my question:Selecting an observable A which does not commute with H,
"< [H,A] > = <ψ, [H,A] ψ>
is i\hbar times the time derivative at t = 0 of <ψ, A ψ>, as you can see if you note that the solution to the Schrödinger equation can be written in the form
U(t) ψ = exp(-itH/\hbar) ψ
Thus
<[H, A]> = i\hbar d<A>/dt"
If he is using the commutator [H,A] as the operator U(t), then I do not see how to get from
<[H, A]> =<ψ, exp(-itH/\hbar) ψ>
to
i\hbar d<A>/dt
(i.e., i\hbar d<ψ, Aψ>/dt)
If he is not using the commutator as the operator, then I am lost even worse.
I would be very grateful for anyone showing me this step more explicitly. ("Derivation for Dummies")