Geometric and electronic surface reconstructions determine the physical and chemical properties of surfaces and, consequently, their functionality in applications. The reconstruction of a surface minimizes its surface free energy in otherwise thermodynamically unstable situations, typically caused by dangling bonds, lattice stress, or a divergent surface potential, and it is achieved by a cooperative modification of the atomic and electronic structure. Here, we combined first-principles calculations and surface techniques (scanning tunneling microscopy, non-contact atomic force microscopy, scanning tunneling spectroscopy) to report that the repulsion between negatively charged polaronic quasiparticles, formed by the interaction between excess electrons and the lattice phonon field, plays a key role in surface reconstructions. As a paradigmatic example, we explain the (1 × 1) to (1 × 2) transition in rutile TiO2ð110Þ.
Reticcioli, M., Setvin, M., Hao, X., Flauger, P., Kresse, G., Schmid, M., et al. (2017). Polaron-driven surface reconstructions. PHYSICAL REVIEW. X, 7(3), 1-10 [10.1103/PhysRevX.7.031053].
Polaron-driven surface reconstructions
Franchini, Cesare
Writing – Review & Editing
2017
Abstract
Geometric and electronic surface reconstructions determine the physical and chemical properties of surfaces and, consequently, their functionality in applications. The reconstruction of a surface minimizes its surface free energy in otherwise thermodynamically unstable situations, typically caused by dangling bonds, lattice stress, or a divergent surface potential, and it is achieved by a cooperative modification of the atomic and electronic structure. Here, we combined first-principles calculations and surface techniques (scanning tunneling microscopy, non-contact atomic force microscopy, scanning tunneling spectroscopy) to report that the repulsion between negatively charged polaronic quasiparticles, formed by the interaction between excess electrons and the lattice phonon field, plays a key role in surface reconstructions. As a paradigmatic example, we explain the (1 × 1) to (1 × 2) transition in rutile TiO2ð110Þ.| File | Dimensione | Formato | |
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PUBLISHED_PhysRevX.7.031053.pdf
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supplementary_11585_657053.pdf
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