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SUPPORTING INFORMATION
Gas Adsorption and Light Interaction Mechanism in
Phosphorene-Based Field-Effect Transistors
Manthila Rajapaksea, George Andersona, Congyan Zhanga, Rajib
Musaa, Jackson Walter b, Ming
Yua, Gamini Sumanasekeraa,b, Jacek B. Jasinskib*
a Department of Physics and Astronomy, University of Louisville,
Louisville, KY, 40292, USA
b Conn Center for Renewable Energy Research, University of
Louisville, Louisville, KY, 40292,
USA
* Corresponding author: E-mail: [email protected],
Phone: +1-502-852-6338
Electronic Supplementary Material (ESI) for Physical Chemistry
Chemical Physics.This journal is © the Owner Societies 2020
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Figure S1. (left) The band structures of the pristine
phosphorene and various gas molecules on the
top of phosphorene, respectively. The dash line is the Fermi
level and the red arrows indicate the
direct band gap at the Γ point. (right)The total (TDOS) and
partial (PDOS) of the densities of states
of the pristine phosphorene (a) and various gas molecules on the
top of phosphorene (b)-(d),
respectively, where the black curves denote the TDOS, the
red-dotted curves denote PDOS of
phosphorene, and the green-dashed curves denote the PDOS of gas
molecules. The Fermi energy
is shifted to zero.
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Figure S2. (a) Schematic illustration of the optimized structure
of phosphorene with its lattice
constants a and c. (b) the electronic band structure (left) and
densities of states (right) of the
optimized phosphorene with its direct band gap of 0.82 eV. The
blue line represents the fermi level
and the inset is the first Brillouin zone with high symmetry k
points.
a
c
Γ X S Γ Y S
Γ X y S
(a) (b)
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(a)
(b)
Figure S3. Relative resistance of phosphorene exposed to yellow
(a) and red (b) LEDs, for two
different biasing voltages.
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Figure S4. Curve fitting of the relative resistance ON and OFF
response during yellow (top) and
red (bottom) light illumination.