How Are Eigenstates Determined for a Given Hamiltonian Matrix?

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SUMMARY

The discussion focuses on determining eigenstates for a Hamiltonian matrix defined in a Hilbert space with basis vectors \left| 1 \right\rangle, \left| 2 \right\rangle, and \left| 3 \right\rangle. The Hamiltonian is represented as H=\hbar J\left( \begin{matrix} 0 & 1 & 1 \\ 1 & 0 & 1 \\ 1 & 1 & 0 \\ \end{matrix} \right). The eigenstates are expressed as linear combinations \left| {{\psi }^{\left( k \right)}} \right\rangle =\sum\nolimits_{n=1}^{3}{c_{n}^{\left( k \right)}\left| n \right\rangle }, where c_{n}^{\left( k \right)}={{e}^{in\cdot 2\pi k/3}}/\sqrt{3}. The example provided for k=1 demonstrates that H\left| {{\psi }^{\left( 1 \right)}} \right\rangle results in an eigenvalue equation confirming \left| {{\psi }^{\left( 1 \right)}} \right\rangle as an eigenstate.

PREREQUISITES
  • Understanding of Hilbert spaces and basis vectors
  • Familiarity with Hamiltonian mechanics
  • Knowledge of eigenvalues and eigenstates in quantum mechanics
  • Basic proficiency in complex numbers and exponential functions
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  • Study the derivation of eigenstates from Hamiltonians in quantum mechanics
  • Learn about the significance of the constant J in quantum systems
  • Explore the implications of linear combinations of states in quantum mechanics
  • Investigate the role of symmetry in determining eigenstates
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Denver Dang
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Homework Statement


Assume a Hilbert space with the basis vectors \left| 1 \right\rangle, \left| 2 \right\rangle and \left| 3 \right\rangle, and a Hamiltonian, which is described by the chosen basis as:
H=\hbar J\left( \begin{matrix}<br /> 0 &amp; 1 &amp; 1 \\<br /> 1 &amp; 0 &amp; 1 \\<br /> 1 &amp; 1 &amp; 0 \\<br /> \end{matrix} \right),<br />
where J is a constant.

Now, show that the linear combination \left| {{\psi }^{\left( k \right)}} \right\rangle =\sum\nolimits_{n=1}^{3}{c_{n}^{\left( k \right)}\left| n \right\rangle }, where c_{n}^{\left( k \right)}={{e}^{in\cdot 2\pi k/3}}/\sqrt{3} with k = 1,2,3, is eigenstates for H.

Homework Equations

The Attempt at a Solution


I've been told that for k = 1, as an example, I should get:
H\left| {{\psi }^{\left( 1 \right)}} \right\rangle =\hbar J\left( \begin{matrix}<br /> 0 &amp; 1 &amp; 1 \\<br /> 1 &amp; 0 &amp; 1 \\<br /> 1 &amp; 1 &amp; 0 \\<br /> \end{matrix} \right)\left( \begin{matrix}<br /> {{e}^{2\pi i/3}} \\<br /> {{e}^{4\pi i/3}} \\<br /> 1 \\<br /> \end{matrix} \right)\frac{1}{\sqrt{3}}<br />
And from this you see that it is an actual eigenstate, since I end up with:
H\left| {{\psi }^{\left( 1 \right)}} \right\rangle =-\hbar J\left| {{\psi }^{\left( 1 \right)}} \right\rangle

My question is, how did the guy, which I got this from, come up with the vector for \left| {{\psi }^{\left( 1 \right)}} \right\rangle.
I can't seem to figure that out :/Thanks in advance.
 
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Denver Dang said:
My question is, how did the guy, which I got this from, come up with the vector for \left| {{\psi }^{\left( 1 \right)}} \right\rangle.
I can't seem to figure that out :/Thanks in advance.

The expression for \left| {{\psi }^{\left( 1 \right)}} \right\rangle just comes from letting ##k=1## in \left| {{\psi }^{\left( k \right)}} \right\rangle =\sum\nolimits_{n=1}^{3}{c_{n}^{\left( k \right)}\left| n \right\rangle }

Did you try writing that out explicitly and then interpreting as a column matrix?
 
I just figured it out :)

Thank you.
 

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