Abstract
The first-principle calculation with many-body effects explore the electronic and optical properties of newly designed ‘graphyne with BP at hexagonal ring’ (labeled as BP-yne). Our calculations show that BP-yne surface is a direct band gap semiconductor having band gap greater than pristine graphyne and this band gap value is sufficient to overcome the endothermic character of water-splitting reaction and further indicates its possible photocatalytic activities. The Raman and IR spectra analysis indicates quite different feature compare to its structural analogous ‘graphyne with 3BN at ring’ which may help to identify it during synthesis. Its optical absorption can be tuned from near-infrared to UV region depending on the polarization of electric field vector. The optical band gap, as well as the strong absorption peak, lies in the near-infrared region (NIR) and this promising trait can be exploited in biomedical arena.
Highlights
The nanoscale two-dimensional (2D) membranes have stimulated intense interest due to their variety of applications in optoelectronics, spintronics, catalysts, sensors, capacitors, solar cells, batteries, and so on
The valence band maxima (VBM) is mainly contributed by bonding pzπ band of carbon and P atom, while antibonding pzπ∗ band attributed by B and C atom mainly contribute to conduction band minima (CBM) (Fig. 2(c–e))
In case of GW+Bethe-Salpeter equation (BSE) calculation, first strong peak is red-shifted compared to GW corrected one (Fig. 4b(ii)) and the band gap becomes 1.523 eV with significant e-h binding energy (0.337 eV), i.e. the strong peak is located in the near-infrared region (NIR), which points toward its possible use in biomedical application including photothermal therapy and low-power NIR laser irradiation,[53] as ideal photothermal agent should exhibit strong absorbance in NIR region, which is a transparency window for biological tissues.[54]
Summary
The nanoscale two-dimensional (2D) membranes have stimulated intense interest due to their variety of applications in optoelectronics, spintronics, catalysts, sensors, capacitors, solar cells, batteries, and so on. The DFT-band gap is found to be 0.814 eV which is larger than graphyne,[18] but smaller than BN- yne sheet.[18,19] The VBM is mainly contributed by bonding pzπ band of carbon and P atom, while antibonding pzπ∗ band attributed by B and C atom mainly contribute to CBM (Fig. 2(c–e)).
Full Text
Topics from this Paper
Hexagonal Ring
Direct Band Gap Semiconductor
Pristine Graphyne
Strong Absorption Peak
Band Gap
+ Show 5 more
Create a personalized feed of these topics
Get StartedTalk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Similar Papers
Applied Surface Science
Nov 1, 2019
Electrochemical Society Meeting Abstracts
Sep 1, 2016
Crystals
Jul 13, 2023
Physical Chemistry Chemical Physics
Jan 1, 2015
Journal of Solid State Chemistry
Jan 1, 2022
Combustion and Flame
Sep 1, 2022
Chemical Physics
Nov 1, 2015
Materials Today Communications
Mar 1, 2021
Journal of Physics and Chemistry of Solids
Apr 1, 2019
AIP Advances
Aug 1, 2011
International Nano Letters
Oct 13, 2020
Inorganic Chemistry
Jun 1, 2003
Radiation Effects and Defects in Solids
Aug 1, 2013
Radiation Physics and Chemistry
Apr 1, 2014
Structural Chemistry
May 28, 2014
AIP Advances
AIP Advances
Nov 1, 2023
AIP Advances
Nov 1, 2023
AIP Advances
Nov 1, 2023
AIP Advances
Nov 1, 2023
AIP Advances
Nov 1, 2023
AIP Advances
Nov 1, 2023
AIP Advances
Nov 1, 2023
AIP Advances
Nov 1, 2023
AIP Advances
Nov 1, 2023
AIP Advances
Nov 1, 2023