Physics Asked on December 26, 2020
My notes state that the spectral decomposition formula is of the form:
$$ hat{A} = hat{A}hat{1} = sum{hat{A} } |A_iranglelangle A_i | = sum{A_i } |A_iranglelangle A_i | $$
Now consider the Hamiltonian as
$$ hat{H} = begin{bmatrix}E&KK*&Eend{bmatrix}$$
It would be easy to show that the eigenvalues are $$E_+ = E+|K|$$ and$$E_- = E-|K| $$and the eigenstates are as follows:
$$ |+rangle = frac{1}{sqrt{2}}
begin{pmatrix}
frac{k}{|k|}
1
end{pmatrix} $$
$$ |-rangle = frac{1}{sqrt{2}}
begin{pmatrix}
frac{-k}{|k|}
1
end{pmatrix} $$
I was expected then to show that the unitary operator $$hat{U}(t) = e ^{ithat{H}/hbar}$$ can be defined as follows:
$$hat{U}(t)=e^{-ihat{H}t/hbar}=
e^{-iEt/hbar}begin{pmatrix}
cos(|K|t/hbar) & -ifrac{K}{|K|}sin(|K|t/hbar)
-ifrac{K^*}{|K|}sin(|K|t/hbar) & cos(|K|t/hbar)
end{pmatrix}$$
According to my notes the appropriate application of the spectral decomposition formula to do so is
$$ hat{U}(t) = e ^{it{hat{H}}/hbar} = e ^{it{E_+}/hbar} |+ranglelangle +| + e ^{it{E_-}/hbar} |-ranglelangle -| $$
However if we recall the spectral decomposition formula as:
$$ hat{U} = hat{U}hat{1} = sum{hat{U} } |U_iranglelangle U_i | = sum{U_i } |U_iranglelangle U_i | $$
My question therefore is why is it appropriate to use the $|+rangle$ and $|-rangle$ states when they are the eigenstates of the $hat{H}$ operator and not the $hat{U}(t)$ one?
My question therefore is why is it appropriate to use the $|+rangle$ and $|-rangle$ states when they are the eigenstates of the $H$ operator and not the $U(t)$ one?
The eigenvectors $|+rangle$ and $|-rangle$ of $hat{H}$ are also eigenvectors of $hat{U}(t)$, because
$$begin{align} hat{U}(t) |+rangle &=e^{ithat{H}/hbar} |+rangle &=sum_{n=0}^infty frac{1}{n!}left(frac{ithat{H}}{hbar}right)^n |+rangle &=sum_{n=0}^infty frac{1}{n!}left(frac{itE_+}{hbar}right)^n |+rangle &=e^{itE_+/hbar} |+rangle end{align}$$
and similarly $$hat{U}(t) |-rangle =e^{itE_-/hbar} |-rangle$$
This justifies the spectral decomposition of $hat{U}(t)$: $$hat{U}(t) = e ^{it{E_+}/hbar} |+ranglelangle +| + e ^{it{E_-}/hbar} |-ranglelangle -|$$
Correct answer by Thomas Fritsch on December 26, 2020
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