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The TB Hamiltonian for the tetragonal lattice is $ \hat H_0 = -J\sum_{m,n} (\hat a_{m+1,n}^\dagger \hat a_{m,n}+\hat a_{m,n}^\dagger \hat a_{m,n+1}+h.c.) $

How can this be derived for the hexagonal lattice?

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    $\begingroup$ Your title talks about a tight-binding Hamiltonian but the body of your question talks about a Hubbard Hamiltonian, which has an extra on site term which does not appear in Hamiltonian you have written down. What are you actually after? $\endgroup$ – By Symmetry Jul 12 at 8:54
  • $\begingroup$ TB Hamiltonian. $\endgroup$ – John Typas Jul 13 at 1:52
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Graphene has two atoms per unit cell belonging to sublattices A and B. Nearest neighbor hopping takes place only between atoms of different sublattices:

$$ \hat{H} = -t \sum_j a^\dagger\left(\mathbf{r}_j\right) b\left(\mathbf{r}_j\right) + a^\dagger\left(\mathbf{r}_j\right) b\left(\mathbf{r}_j + \mathbf{d}_1\right) + a^\dagger\left(\mathbf{r}_j\right) b\left(\mathbf{r}_j + \mathbf{d}_2\right) + \mathrm{h.c.}\,. $$

The Hamiltonian tells you that for an A-sublattice atom inside the unit cell at $\mathbf{r}_j$, there are three nearest neighbors: one in the same unit cell and two more in the unit cells shifted by the lattice vectors $\mathbf{d}_1$ and $\mathbf{d}_2$. Write the Hamiltonian in the momentum space:

$$ \hat{H} = -t \sum_j \left[\frac{1}{\sqrt{N}}\sum_\mathbf{q} a^\dagger_\mathbf{q}e^{-i\mathbf{r}_j \cdot\mathbf{q}}\right] \left[\frac{1}{\sqrt{N}}\sum_{\mathbf{q}'} b_{\mathbf{q}'}e^{i\mathbf{r}_j \cdot\mathbf{q}'}\right] \\ -t \sum_j \left[\frac{1}{\sqrt{N}}\sum_\mathbf{q} a^\dagger_\mathbf{q}e^{-i\mathbf{r}_j \cdot\mathbf{q}}\right] \left[\frac{1}{\sqrt{N}}\sum_{\mathbf{q}'} b_{\mathbf{q}'}e^{i\left(\mathbf{r}_j+\mathbf{d}_1\right) \cdot\mathbf{q}'}\right] \\ -t \sum_j \left[\frac{1}{\sqrt{N}}\sum_\mathbf{q} a^\dagger_\mathbf{q}e^{-i\mathbf{r}_j \cdot\mathbf{q}}\right] \left[\frac{1}{\sqrt{N}}\sum_{\mathbf{q}'} b_{\mathbf{q}'}e^{i\left(\mathbf{r}_j+\mathbf{d}_2\right) \cdot\mathbf{q}'}\right] + \mathrm{h.c.}\,. $$

Here, $N$ is the number of unit cells in the system. Performing the summation over $j$ gives $N\delta_{\mathbf{qq}'}$ so that

$$ \hat{H} = -t \sum_\mathbf{q} a^\dagger_\mathbf{q} b_\mathbf{q} -t \sum_\mathbf{q} a^\dagger_\mathbf{q} b_\mathbf{q} e^{i \mathbf{d}_1 \cdot \mathbf{q}} -t \sum_\mathbf{q} a^\dagger_\mathbf{q}b_\mathbf{q}e^{i \mathbf{d}_2\cdot \mathbf{q}} + \mathrm{h.c.} \\ =-t\sum_\mathbf{q}a^\dagger_\mathbf{q}b_\mathbf{q} \left( 1 + e^{i\mathbf{d}_1\cdot\mathbf{q}} + e^{i\mathbf{d}_2\cdot\mathbf{q}} \right) + \mathrm{h.c.} \\ =-t\sum_\mathbf{q} \begin{pmatrix} a^\dagger_\mathbf{q} & b^\dagger_\mathbf{q} \end{pmatrix} \begin{pmatrix} 0&1 + e^{i\mathbf{d}_1\cdot\mathbf{q}} + e^{i\mathbf{d}_2\cdot\mathbf{q}} \\ 1 + e^{-i\mathbf{d}_1\cdot\mathbf{q}} + e^{-i\mathbf{d}_2\cdot\mathbf{q}} &0 \end{pmatrix} \begin{pmatrix} a_\mathbf{q} \\ b_\mathbf{q} \end{pmatrix}\,. $$

There you go!

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  • $\begingroup$ thank you al lot ! $\endgroup$ – John Typas Jul 30 at 13:51

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