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Understanding correlations and localization in the Hubbard model ...

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The <strong>Hubbard</strong> <strong>model</strong><br />

Breakdown of b<strong>and</strong> <strong>the</strong>ory: correlation<br />

Hamiltonian:<br />

H =<br />

hopp<strong>in</strong>g H t<br />

{ }} {<br />

−t ∑<br />

{c † i,σ c j,σ + H.c.} +<br />

〈i,j〉σ<br />

<strong>in</strong>teraction H<br />

{ }} { U<br />

U ∑ n i↑ n i↓<br />

i<br />

Limit<strong>in</strong>g cases: Mott metal-<strong>in</strong>sulator transition<br />

Exact solution known <strong>in</strong> 1D via Be<strong>the</strong> ansatz (Lieb<br />

<strong>and</strong> Wu, 1968): <strong>in</strong>sulator for f<strong>in</strong>ite U.<br />

High-T c superconductivity<br />

<strong>Underst<strong>and</strong><strong>in</strong>g</strong> <strong>correlations</strong> <strong>and</strong> <strong>localization</strong> <strong>in</strong> <strong>the</strong> <strong>Hubbard</strong> <strong>model</strong> from variational calculations – p. 4

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