4.7 Article

Optoelectronic properties of new direct bandgap polymorphs of single-layered Germanium sulfide

Journal

CERAMICS INTERNATIONAL
Volume 45, Issue 14, Pages 18073-18078

Publisher

ELSEVIER SCI LTD
DOI: 10.1016/j.ceramint.2019.06.028

Keywords

Two-dimensional materials; Nanoscale optoelectronic and photovoltaics; Electronic structure calculations; Anisotrpic optical spectra; Large optical absorption

Funding

  1. Deanship of Scientific Research at King Khalid University through the Research Groups Program [R.G.P. 2./21/40]
  2. Research Center of the Female Scientific and Medical Colleges, Deanship of Scientific Research, King Saud University
  3. HEC [7435/Punjab/NRPU/RD/HEC/2017]

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The single-layered Germanium sulfide exhibits interesting optoelectronic properties however the indirect bandgap hinders its practical applications for nanoscale optoelectronic and photovoltaic devices. Herein, we report two direct bandgap polymorphs of single-layered GeS (delta-GeS and epsilon-GeS) and explore their optoelectronic properties using the density functional theory based computational approaches. The indirect bandgap of the intrinsic GeS monolayer (alpha-GeS) calculated in present study amounts to 0.76 eV, whereas the direct bandgap energies for delta- and epsilon-derivatives of GeS have been recorded as 1.93 and 2.10 eV respectively. The optical spectra of these monolayers demonstrated a high degree of anisotropy and significantly different optical absorption, reflection, and refraction coefficients were seen in the x- and y-directions. They exhibited different plasmons energies along x- and y-directions which reveal the GeS monolayers as potential polarizers of electromagnetic radiations. Moreover, these monolayers demonstrated exceptionally large optical absorption spanning over a wide range of electromagnetic spectrum. The absorption coefficients were recorded typically larger along y-axis than x-axis. The designed direct bandgap monolayers are believed to overcome the major hurdles of single-layered GeS for nanoscale optoelectronic applications.

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