z-logo
open-access-imgOpen Access
Linear and nonlinear optical properties for AA and AB stacking of carbon nitride polymorph (C3N4)
Author(s) -
A.H. Reshak,
Saleem Ayaz Khan,
S. Auluck
Publication year - 2014
Publication title -
rsc advances
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.746
H-Index - 148
ISSN - 2046-2069
DOI - 10.1039/c4ra00388h
Subject(s) - stacking , carbon nitride , nonlinear optical , density functional theory , nitride , computational chemistry , plane wave , nonlinear system , materials science , molecular physics , carbon fibers , crystallography , chemistry , nanotechnology , physics , optics , quantum mechanics , organic chemistry , layer (electronics) , composite material , photocatalysis , catalysis , composite number
The linear and nonlinear optical susceptibilities of AA and AB stacking of the carbon nitride polymorph were calculated using the all electron full potential linear augmented plane wave method based on density functional theory. The complex part of the dielectric function is calculated using the recently modified Becke and Johnson (mBJ) approximation which gives a better optical gap in comparison to the Ceperley–Alder (CA) local density approximation, the Perdew–Burke–Ernzerhof generalized gradient approximation, and the Engel–Vosko generalized gradient approximation. The complex dielectric function and other optical constants like refractive index, absorption coefficient, reflectivity and energy loss function are calculated and discussed in detail. The calculated uniaxial anisotropy (−1.06 and −1.04) gives a maximum value of birefringence (−0.89 and −0.87) which increases the suitability of both AA and AB stacking for a large second harmonic generation. The calculated second order susceptibility tensor components |χ(2)333(ω)| at the static limit are 19.4 pm V−1 and 59.6 pm V−1 for AA and AB stacking which increases to 34.2 pm V−1 and 106.7 pm V−1 at λ = 1064 nm. The first hyperpolarizability β333(ω) for AA and AB stacking C3N4 for the dominant component |χ(2)333(ω)| at the static limit are calculated to be (1.6 × 10−30 esu and 9.6 × 10−30 esu) respectively.

The content you want is available to Zendy users.

Already have an account? Click here to sign in.
Having issues? You can contact us here
Accelerating Research

Address

John Eccles House
Robert Robinson Avenue,
Oxford Science Park, Oxford
OX4 4GP, United Kingdom