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- Thread starter mkbh_10
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Gokul43201

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This equation is simply an application of eq. 8.39 to a 2-state system. C1 and C2 are the components of the wave function along each of the 2 basis states. H12 and H21 are the off-diagonal terms in the Hamiltonian.

[tex]

\mathcal{H} \equiv \left(

\begin{array}{cc}

H_{11} & H_{12}\\

H_{21} & H_{22}

\end{array}

\right)

[/tex]

[tex]

\mathcal{H} \equiv \left(

\begin{array}{cc}

H_{11} & H_{12}\\

H_{21} & H_{22}

\end{array}

\right)

[/tex]

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