TY - JOUR
T1 - Electronic and optical properties of two-dimensional heterostructures and heterojunctions between doped-graphene and C- And N-containing materials
AU - Bafekry, Asadollah
AU - Gogova, Daniela
AU - M. Fadlallah, Mohamed
AU - V. Chuong, Nguyen
AU - Ghergherehchi, Mitra
AU - Faraji, Mehrdad
AU - Feghhi, Seyed Amir Hossein
AU - Oskoeian, Mohamad
N1 - Publisher Copyright:
© the Owner Societies 2021.
PY - 2021/2/28
Y1 - 2021/2/28
N2 - The electronic and optical properties of vertical heterostructures (HTSs) and lateral heterojunctions (HTJs) between (B,N)-codoped graphene (dop@Gr) and graphene (Gr), C3N, BC3and h-BN monolayers are investigated using van der Waals density functional theory calculations. We have found that all the considered HTSs are energetically and thermally feasible at room temperature, and therefore they can be synthesized experimentally. The dop@Gr/Gr, BC3/dop@Gr and BN/dop@Gr HTSs are semiconductors with direct bandgaps of 0.1 eV, 80 meV and 1.23 eV, respectively, while the C3N/dop@Gr is a metal because of the strong interaction between dop@Gr and C3N layers. On the other hand, the dop@Gr-Gr and BN-dop@Gr HTJs are semiconductors, whereas the C3N-dop@Gr and BC3-dop@Gr HTJs are metals. The proposed HTSs can enhance the absorption of light in the whole wavelength range as compared to Gr and BN monolayers. The applied electric field or pressure strain changes the bandgaps of the HTSs and HTJs, indicating that these HTSs are highly promising for application in nanoscale multifunctional devices.
AB - The electronic and optical properties of vertical heterostructures (HTSs) and lateral heterojunctions (HTJs) between (B,N)-codoped graphene (dop@Gr) and graphene (Gr), C3N, BC3and h-BN monolayers are investigated using van der Waals density functional theory calculations. We have found that all the considered HTSs are energetically and thermally feasible at room temperature, and therefore they can be synthesized experimentally. The dop@Gr/Gr, BC3/dop@Gr and BN/dop@Gr HTSs are semiconductors with direct bandgaps of 0.1 eV, 80 meV and 1.23 eV, respectively, while the C3N/dop@Gr is a metal because of the strong interaction between dop@Gr and C3N layers. On the other hand, the dop@Gr-Gr and BN-dop@Gr HTJs are semiconductors, whereas the C3N-dop@Gr and BC3-dop@Gr HTJs are metals. The proposed HTSs can enhance the absorption of light in the whole wavelength range as compared to Gr and BN monolayers. The applied electric field or pressure strain changes the bandgaps of the HTSs and HTJs, indicating that these HTSs are highly promising for application in nanoscale multifunctional devices.
UR - https://www.scopus.com/pages/publications/85102402154
U2 - 10.1039/d0cp06213h
DO - 10.1039/d0cp06213h
M3 - Article
C2 - 33615321
AN - SCOPUS:85102402154
SN - 1463-9076
VL - 23
SP - 4865
EP - 4873
JO - Physical Chemistry Chemical Physics
JF - Physical Chemistry Chemical Physics
IS - 8
ER -