Triggering a global density wave instability in graphene via local symmetry-breaking
Science Advances, 8, eabm5180 (2022) Two-dimensional quantum materials offer a robust platform for investigating the emergence of symmetry-broken ordered phases owing to the high tuneability of their electronic properties. For instance, the ability to create new electronic band structures in graphen...
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Main Authors: | , , , , , , , , , , , |
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Format: | Journal Article |
Language: | English |
Published: |
23-04-2022
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Subjects: | |
Online Access: | Get full text |
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Summary: | Science Advances, 8, eabm5180 (2022) Two-dimensional quantum materials offer a robust platform for investigating
the emergence of symmetry-broken ordered phases owing to the high tuneability
of their electronic properties. For instance, the ability to create new
electronic band structures in graphene through moir\'e superlattices from
stacked and twisted structures has led to the discovery of several correlated
and topological phases. Here we report an alternative method to induce an
incipient symmetry-broken phase in graphene at the millimetre scale. We show
that an extremely dilute concentration ($<\!0.3\% $) of surface adatoms can
self-assemble and trigger the collapse of the graphene atomic lattice into a
distinct Kekul\'e bond density wave phase, whereby the carbon C-C bond symmetry
is broken globally. Using complementary momentum-resolved techniques such as
angle-resolved photoemission spectroscopy (ARPES) and low-energy electron
diffraction (LEED), we directly probe the presence of this density wave phase
and confirm the opening of an energy gap at the Dirac point. We further show
that this Kekul\'e density wave phase occurs for various Fermi surface sizes
and shapes, suggesting that this lattice instability is driven by strong
electron-lattice interactions. Our results demonstrate that dilute
concentrations of self-assembled adsorbed atoms offer an attractive alternative
route towards designing novel quantum phases in two-dimensional materials. |
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DOI: | 10.48550/arxiv.2204.10999 |