2014
DOI: 10.1007/s13391-013-3097-z
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Ab initio calculations of electronic and optical properties of BeO nanosheet

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Cited by 35 publications
(9 citation statements)
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“…With this knowledge, we can exploit the moiré pattern to determine the h-BeO lattice constant with greater accuracy: with a moiré periodicity of 3.2 nm and the known lattice constant of 2.89 Å for Ag(111), one can deduce a lattice constant of 2.65 ± 0.01 Å for the h-BeO. This calculated lattice constant is consistent with the atomic resolution measurements, displaying a reduction in BeO bond length compared to bulk wurtzite structure, as theoretically predicted. ,,, The decrease in lattice constant was previously theorized to stem from the graphitic Be–O bond having an increased covalent character, and as a result, the atoms move closer to increase the orbital overlap of nearest neighbors. ,, …”
Section: Resultssupporting
confidence: 83%
See 1 more Smart Citation
“…With this knowledge, we can exploit the moiré pattern to determine the h-BeO lattice constant with greater accuracy: with a moiré periodicity of 3.2 nm and the known lattice constant of 2.89 Å for Ag(111), one can deduce a lattice constant of 2.65 ± 0.01 Å for the h-BeO. This calculated lattice constant is consistent with the atomic resolution measurements, displaying a reduction in BeO bond length compared to bulk wurtzite structure, as theoretically predicted. ,,, The decrease in lattice constant was previously theorized to stem from the graphitic Be–O bond having an increased covalent character, and as a result, the atoms move closer to increase the orbital overlap of nearest neighbors. ,, …”
Section: Resultssupporting
confidence: 83%
“…We next utilize scanning tunneling spectroscopy to study the electronic structure of the h-BeO. The differential conductance (d I /d V ) spectroscopy, representing the local density of states (LDOS), is shown in Figure a with spectra spanning 5 orders of magnitude in dynamic range and displayed in logarithmic scale, acquired at a set bias of 4.1 V. With such a large dynamic range, we can assign the location of the CBM at 3.0 ± 0.2 eV and VBM at −3.0 ± 0.2 eV, corresponding to a band gap of ∼6 eV, similar to the value of previous theoretical calculations. ,, However, we note that it is difficult to assign the exact locations of the band edges with d I /d V spectroscopy alone. As discussed above, this explains why the layers resemble pristine Ag(111) at low sample bias (Figures b, b); within the band gap, the h-BeO does not contribute to the LDOS.…”
Section: Resultsmentioning
confidence: 99%
“…2(a) (light green arrow). We find that the properties of ε 2 for the BeO monolayer are completely different from the dielectric function for BeO bulk in wurtzite structure [37,38]. The difference between the monolayer and the wurtzite structure is due to differences in the Be-O hybridization.…”
Section: Nitrogen Doped Beo Monolayermentioning
confidence: 71%
“…The threshold energies and the peak positions tell us that the physical properties of pure BeO monolayer are different from the properties of BeO bulk in its wurtzite structure [20,44], which is due to the Be-O hybridization. In a BeO monolayer each atom (Be or O atoms) has three bonds with the nearest neighbor, but in the BeO wurtzite structure each atom is bonded with four other atoms.…”
Section: Optical Propertiesmentioning
confidence: 97%
“…x and an insulator for E ⊥ z. The optical spectra are anisotropic, and the static refractive index of the nanosheet structure is lower than that of the wurtzite structure [20]. The monolayer h-BeO exhibits a wide band gap due to the atomic electronegativity difference in the polar h-BeO.…”
Section: Introductionmentioning
confidence: 99%