Abstract
Two-dimensional (2D) atomically thin boron layers designated as borophene or boraphene, attract great interest as promising post-graphene 2D materials. The borophene layer phonon structure has not yet been clarified by experimentation in spite of its importance for application for possible superconduction and thermal technologies. For this work we measured, by experimentation, the phonon dispersion of an incommensurate three-domain ${\ensuremath{\chi}}_{3}$-borophene formed on Ag(111) using high-resolution electron energy loss spectroscopy. Measured phonons were analyzed using first-principles theoretical calculations. Because the phonon band of the substrate Ag(111) lies in a low-energy region, the borophene phonon is well separated from the substrate. For our calculations, a commensurate slab supercell model was adopted, the periodicity of which was Ag(111) $3\ifmmode\times\else\texttimes\fi{}3$. The lattice parameter of the model was determined using experimentally obtained phonon data. The highest frequency phonon of an isolated borophene layer was fitted to the data as a function of the electronic charge in it. The best fitted lattice parameter was used in the supercell model. The model well reproduced the experimentally observed phonon dispersion. No marked anomaly was found in the phonon structure.
Highlights
Since the beginning of the 21st century, two-dimensional (2D) materials of one or several atomic thickness have become a main stream both in fundamental and application research fields
The following can be performed in the preparation chamber: reflection high-energy electron diffraction (RHEED), Auger electron spectroscopy (AES), Kr+ ion bombardment, Ag deposition from a Knudsen cell (K-cell, EF 40C1; PREVAC) with a pyrolytic boron nitride (PBN) crucible, and B deposition from an electron-heated evaporator (EFM 3; Scienta Omicron, Inc.)
Even though the lattice parameter of Ag(111) (aAg(111) = 288.4 pm [42]) is smaller (−8.7%) than that of NbC(111) (aNbC(111) = 315.9 pm [35]), deposition of Ag at room temperature caused in the epitaxial growth for which the relationship was (111)Ag (111)NbC and [110]Ag [110]NbC
Summary
Since the beginning of the 21st century, two-dimensional (2D) materials of one or several atomic thickness have become a main stream both in fundamental and application research fields. Following the amazing success of graphene, atomically thin elemental materials designated as “Xenes” have been explored extensively in anticipation of various applications: silicene (Si), germanene (Ge), stanene (Sn), phosphorene (P), borophene or boraphene (B), and so on [1]. Among these Xenes, borophene is most interesting because of its characteristic properties [2,3,4,5,6] and many promising applications for gas sensors, hydrogen storage in fuel cells, superconductors, electrodes in alkaline metal batteries, catalysts for hydrogen evolution or oxygen reduction [7,8], and biomedical devices [9]. Several theoretical works explained its mechanisms [11,12,13]
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