Establishing coherent momentum-space electronic states in locally ordered materials

Rich momentum-dependent electronic structure naturally arises in solids with long-range crystalline symmetry. Reliable and scalable quantum technologies rely on materials that are either not perfect crystals or non-crystalline, breaking translational symmetry. This poses the fundamental questions of whether coherent momentum-dependent electronic states can arise without long-range order, and how they can be characterized. Here we investigate Bi<sub>2</sub>Se<sub>3</sub>, which exists in crystalline, nanocrystalline, and amorphous forms, allowing direct comparisons between varying degrees of spatial ordering. Through angle-resolved photoemission spectroscopy, we show for the first time momentum-dependent band structure with Fermi surface repetitions in an amorphous solid. The experimental data is complemented by a model that accurately reproduces the vertical, dispersive features as well as the replication at higher momenta in the amorphous form. These results reveal that well-defined real-space length scales are sufficient to produce dispersive band structures, and that photoemission can expose the imprint of these length scales on the electronic structure.

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Publication Details

Journal
Nature Communications
Published
2024-09-17
DOI
https://doi.org/10.1038/s41467-024-51953-y
Citations
7
Primary Topic
Topological Materials and Phenomena
Type
article
Field-Weighted Citation Impact
2.03

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article

Establishing coherent momentum-space electronic states in locally ordered materials

Adolfo G. Grushin, Mary Scott, Samuel Ciocys, Paul Corbae et al.
7 citations
Nature Communications
Topological Materials and Phenomena
2.03
article

Establishing coherent momentum-space electronic states in locally ordered materials

Adolfo G. Grushin, Mary Scott, Samuel Ciocys, Paul Corbae, Ellis Kennedy, F. Hellman, Quentin Marsal, Dániel Varjas, Alessandra Lanzara
article en
7 citations

Abstract

Rich momentum-dependent electronic structure naturally arises in solids with long-range crystalline symmetry. Reliable and scalable quantum technologies rely on materials that are either not perfect crystals or non-crystalline, breaking translational symmetry. This poses the fundamental questions of whether coherent momentum-dependent electronic states can arise without long-range order, and how they can be characterized. Here we investigate Bi<sub>2</sub>Se<sub>3</sub>, which exists in crystalline, nanocrystalline, and amorphous forms, allowing direct comparisons between varying degrees of spatial ordering. Through angle-resolved photoemission spectroscopy, we show for the first time momentum-dependent band structure with Fermi surface repetitions in an amorphous solid. The experimental data is complemented by a model that accurately reproduces the vertical, dispersive features as well as the replication at higher momenta in the amorphous form. These results reveal that well-defined real-space length scales are sufficient to produce dispersive band structures, and that photoemission can expose the imprint of these length scales on the electronic structure.

Nature CommunicationsVol. 15(1)
Institut polytechnique de Grenoble (FR), Uppsala University (SE), Centre National de la Recherche Scientifique (FR), Lawrence Berkeley National Laboratory (US), Stockholm University (SE), Budapest University of Technology and Economics (HU), Leibniz Institute for Solid State and Materials Research (DE), Complexity, Topology and Dynamics in Quantum Matter (DE), Max Planck Institute for the Physics of Complex Systems (DE), AlbaNova (SE), Institut Néel (FR), Université Grenoble Alpes (FR), University of California, Berkeley (US)
U.S. Department of Energy, Gordon and Betty Moore Foundation, European Commission, Deutsche Forschungsgemeinschaft, Hungarian Scientific Research Fund, Office of Science, Horizon 2020 Framework Programme, National Research, Development and Innovation Office, Basic Energy Sciences
Climate action
Openalex Percentile: Top 15%
Topological Materials and Phenomena
2.03
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