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Charge Density Waves in 2D Materials Bogdan Guster PhD advisors: P. Ordejón E. Canadell M. Pruneda

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Page 1: Charge Density Waves in 2D Materialsphantomsfoundation.com/GRAPHENECONF/2018...Phonon instability at M 1Q phonon condensation → 2x1 CDW 3Q phonon condensation → 2x2 CDW ... (1

Charge Density Waves

in 2D Materials

Bogdan Guster

PhD advisors: P. Ordejón E. Canadell M. Pruneda

Page 2: Charge Density Waves in 2D Materialsphantomsfoundation.com/GRAPHENECONF/2018...Phonon instability at M 1Q phonon condensation → 2x1 CDW 3Q phonon condensation → 2x2 CDW ... (1

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Motivation

1T – TiSe2

Page 3: Charge Density Waves in 2D Materialsphantomsfoundation.com/GRAPHENECONF/2018...Phonon instability at M 1Q phonon condensation → 2x1 CDW 3Q phonon condensation → 2x2 CDW ... (1

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Contents

→ What is a charge density wave?

→ Electronic structure of TiSe2

→ Phonons’ role and the 2x2 CDW phase

→ Doping effect on the CDW phase

Page 4: Charge Density Waves in 2D Materialsphantomsfoundation.com/GRAPHENECONF/2018...Phonon instability at M 1Q phonon condensation → 2x1 CDW 3Q phonon condensation → 2x2 CDW ... (1

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What is a Charge Density Wave?

Half-filled electron band of the 1D atomic above (c), below (d) Tc

Real part of the Lindhard function for 1D, 2D and 3D free electron gas (e)

Phonon dispersion of 1D atomic chain at different temperatures (f)

Adv. Phys. X 2 3 622-640 (2017)

Page 5: Charge Density Waves in 2D Materialsphantomsfoundation.com/GRAPHENECONF/2018...Phonon instability at M 1Q phonon condensation → 2x1 CDW 3Q phonon condensation → 2x2 CDW ... (1

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TiSe2 – Intro

Semi-metallic (d0)

Phase transition at ~230 K

2x2 CDW modulated structure

Opens gap at Fermi level

Commensurate → Incommensurate with doping

Page 6: Charge Density Waves in 2D Materialsphantomsfoundation.com/GRAPHENECONF/2018...Phonon instability at M 1Q phonon condensation → 2x1 CDW 3Q phonon condensation → 2x2 CDW ... (1

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TiSe2 – Semi-metallic character

Electronic dispersion

BG et al 2018 2D Mater. 5 025024

Page 7: Charge Density Waves in 2D Materialsphantomsfoundation.com/GRAPHENECONF/2018...Phonon instability at M 1Q phonon condensation → 2x1 CDW 3Q phonon condensation → 2x2 CDW ... (1

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TiSe2 – Electrons and Phonons

Electronic dispersion

Phononic dispersion

Lindhard function mapping

Unstable

BG et al 2018 2D Mater. 5 025024

Page 8: Charge Density Waves in 2D Materialsphantomsfoundation.com/GRAPHENECONF/2018...Phonon instability at M 1Q phonon condensation → 2x1 CDW 3Q phonon condensation → 2x2 CDW ... (1

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TiSe2 – Phonons Behaviour

8 8 BG et al 2018 2D Mater. 5 025024

120°

120°

Page 9: Charge Density Waves in 2D Materialsphantomsfoundation.com/GRAPHENECONF/2018...Phonon instability at M 1Q phonon condensation → 2x1 CDW 3Q phonon condensation → 2x2 CDW ... (1

TiSe2 – 2x2 CDW phase

Page 10: Charge Density Waves in 2D Materialsphantomsfoundation.com/GRAPHENECONF/2018...Phonon instability at M 1Q phonon condensation → 2x1 CDW 3Q phonon condensation → 2x2 CDW ... (1

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TiSe2 – Doping effect

Page 11: Charge Density Waves in 2D Materialsphantomsfoundation.com/GRAPHENECONF/2018...Phonon instability at M 1Q phonon condensation → 2x1 CDW 3Q phonon condensation → 2x2 CDW ... (1

Electronic structure character

Phonon instability at M

1Q phonon condensation → 2x1 CDW

3Q phonon condensation → 2x2 CDW

Doping → Incommensurate CDW

Similar mechanism in single-layer TiTe2

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Conclusion