Author Affiliations
1Public Health and Management School, Hubei University of Medicine, Shiyan 442000, China2Hubei Biomedical Detection Sharing Platform in Water Source Area of South to North Water Diversion Project, Shiyan 442000, Chinashow less
Fig. 1. Crystal structure of monolayer TiO2(a) top view; (b) side view; (c) K point path.
Fig. 2. Phonon spectrum of monolayer TiO2.
Fig. 3. Molecular dynamics simulation of monolayer TiO2.
Fig. 4. Polar coordinates for Young's modulus (left/blue line) and Poisson's ratio (right/red line)
is the angle with respect to the
a-direction.
Fig. 5. Energy band structure (left) and density of states (right) of (a) monolayer P-6M2 TiO2, (b) monolayer rutile TiO2, (c) monolayer anatase TiO2.
Fig. 6. The differential charge density of monolayer TiO2.
Fig. 7. (a) The relation between total energy and the applied strain
along the
a/
b directions of monolayer TiO
2. The quadratic data fitting gives the in-plane stiffness of 2D structures. Black and red curves show the in-plane stiffness along the
a and
b directions of monolayer TiO
2. The shift of VBMs and CBMs for (b-c) monolayer TiO
2 with respect to the vacuum energy, as a function of the applied strain along either the
a and
b direction. The linear fit of the data yields the deformation potential constant.
Fig. 8. Band gap of monolayer TiO2 under uniaxial/biaxial strain, calculated using the HSE06 functional.
Fig. 9. Schematic diagram of monolayer TiO2 photocatalysis under uniaxial/biaxial strain.
Fig. 10. Optical properties: (a) virtual part of dielectric function; (b) absorption coefficient.
Material | a/b/Å
| ${\theta _1}$![]() /(
$^ \circ $![]() )
| ${\theta _2}$![]() /(
$^ \circ $![]() )
| l/Å
| $\sigma $![]() /Å
| Ef/eV
| TiO2 | 2.89 | 91.66 | 68.16 | 2.01 | 2.26 | –8.11 | MoS2 | 3.18 | 82.58 | 80.74 | 2.41 | 3.14 | –7.35 |
|
Table 1. Structure constants and binding energy of monolayer TiO2.
二维TiO2的结构常数和结合能
Carrier type | $m_a^ * $![]() /
${m_{\rm{e}}}$![]() ![]() | $m_b^ * $![]() /
${m_{\rm{e}}}$![]() ![]() | $m_l^ * $![]() /
${m_{\rm{e}}}$![]() ![]() | $\left| {{E_{la}}} \right|$![]() / eV
| $\left| {{E_{lb}}} \right|$![]() / eV
| $C_a^{2{\rm{D}}}$![]() / N·m–1 | $C_b^{{\rm{2 D}}}$![]() / N·m–1 | $\mu _a^{2{\rm{D}}}$![]() / cm2·V–1·s–1 | $\mu _b^{2{\rm{D}}}$![]() / cm2·V–1·s–1 | Electrons | 3.21 | 1.39 | 2.11 | 3.43 | 3.38 | 21.27 | 21.28 | 12.92 | 30.75 | Holes | 4.73 | 4.12 | 4.41 | 1.26 | 1.25 | 21.27 | 21.28 | 31.09 | 36.29 |
|
Table 2. Calculated effective mass
, deformation potential constant
, elastic modulus
, and carrier mobility
for monolayer TiO
2 along the
a (
) and
b (
) directions, where
represents the position of the valence band top and the conduction band bottom.