Observation of competing, correlated ground states in the flat band of rhombohedral graphite

Zoltán Tajkov

Nanostructures Department, Centre for Energy Research,

Department of Biological Physics, Eötvös Loránd University

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Electrons in solids  - Band theory

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\left[ -\frac{\hbar^2}{2m}\nabla^2 + U\left( \mathbf{r} \right) \right] \psi\left( \mathbf{r} \right) = \varepsilon \psi\left( \mathbf{r} \right)

averaged potential

Electrons in solids  - Band theory

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\left[ -\frac{\hbar^2}{2m}\nabla^2 + U\left( \mathbf{r} \right) \right] \psi\left( \mathbf{r} \right) = \varepsilon \psi\left( \mathbf{r} \right)

Why do we use it?

  • electrical resistivity
  • optical absorption
  • foundation of solid-state electronics

It explains...

Electrons in solids  -  Beyond band theory

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Why do we use it?

Because we can.

An example: methane

1 carbon atom + 4 hydrogen atoms = 10 electrons

30 independent coordinates

100 points per coordinate

 \( 100^{30}=10^{60} \) complex number

1 complex number in every atom

We can store the wave function in \( 10^{30} m^3 \)

Strongly correlated electron systems

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  • Colossal magnetoresistance
  • High-temperature superconductivity
  • VO\( _2 \)

Elbio Dagotto, Science 309, 257 (2005)

Rhombohedral Graphite

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E(\mathbf{q}) \propto |\mathbf{q}|^N

SSH chain

Rhombohedral Graphite

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What does the experiment say? STM results

Rhombohedral Graphite

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DMRG - Beyond meanfield

Theory

Degenerate ground state!

Rhombohedral Graphite

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Experiments

Rhombohedral Graphite

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The team

Oroszlányi László

Koltai János

Hagymási Imre

Nemes-Incze Péter

Péter Vancsó

András Pálinkás

Levente Tapasztó

Rhombohedral Graphite

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\( \mu_1 \approx 10^{-2} \mu_\mathrm{Bohr} \)

LDA+U vs LDA, meanfield

Possible explanations I.

Rhombohedral Graphite

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External electric field

Possible explanations II.

E-field strength 0.05 V/Å

Rhombohedral Graphite

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Quantum confinement

Possible explanations III.

Rhombohedral Graphite

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Experiments - one more thing

Symmetry breaking