Finding the Ground State of a Hamiltonian Operator

Matthollyw00d
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When given a Hamiltonian operator (in this case a 3x3 matrix), how do you go about find the ground state, when this operator is all that is given? By the SE when have H\Psi=E\Psi. I can easily solve for Eigenvalues/vectors, but which correspond to the ground state, or am I missing something?
 
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The ground state is the state with the lowest energy.
 
So I achieve eigenvalues of \{0,1,2\} (this is actually the eigenvalues I have for the problem), would the 0 or the 1 be the lowest state? I assumed 0, but can a ground state have 0 energy?
 
It depends on the potential. You can always add a constant to the potential without changing anything physically, which would shift the total energy by the same amount. What you can't really have is the kinetic energy being 0 because there should always be some motion even in the ground state.
 
Let H=\hbar\omega \[ \left( \begin{array}{ccc}<br /> 1 &amp; i &amp; 0 \\<br /> -i &amp; 1 &amp; 0 \\<br /> 0 &amp; 0 &amp; 1 \end{array} \right) \]
and let A =\hbar \left[ \begin{array}{ccc}<br /> 1 &amp; 0 &amp; i \\<br /> 0 &amp; 1 &amp; 0 \\<br /> -i &amp; 0 &amp; 1 \end{array} \right].

Calculate the uncertainty relation \sigma_E \sigma_a for a system in the energy ground state.

My problem is calculating \langle [H,A]\rangle.
The commutator [H,A]=\hbar^2\omega \left[ \begin{array}{ccc}<br /> 0 &amp; 0 &amp; 0 \\<br /> 0 &amp; 0 &amp; 1 \\<br /> 0 &amp; -1 &amp; 0 \end{array} \right]
And if relevant the eigenvalues of H are \hbar\omega \{0,1,2\}.
It says to calculate in the ground state, but I don't know the ground state, so how do I gather it from this data?
 
You have the eigenvalue for the ground state, now find the corresponding eigenvector. It will be a (non-zero) vector

v_0 = \begin{pmatrix} a \\ b \\ c \end{pmatrix}

satisfying

H v_0 = 0.
 
Yes, but \langle v_0|[H,A]|v_0 \rangle =0 which gives me a trivial inequality, which leads me to believe something is incorrect and hence why I posted here.
 
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