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First principles calculations of
electron mobility in
nanocrystalline TiO2
Suzanne Wallace and Dr. Keith Mckenna
Department of Physics, University of York, Heslington, York, UK
DFT+U for correlated systems
 Coulomb interaction of localised electrons
 electron density NOT uniform
 Employ DFT+U (UTi = 4.2 eV)
 Correct for SI error
 U: adjustable correcting potential
 4.2 eV: produces good agreement with spectroscopic data [1]
[1] Morgan, B. J., & Watson, G. W. (2009). J Phys Chem C, 113(110), 7322–7328.
Finitex-dimension
∆E = Es - Eb
Eb
Es
Localising electrons
 Initialise magnetic moment at the site
 Create a potential well by dilating bonds
 Increase U-parameter (if necessary)
Wallace, S. K., & McKenna, K. P. (2014). Grain Boundary
Controlled Electron Mobility in Polycrystalline Titanium
Dioxide. Advanced Materials Interfaces, n/a–n/a.
doi:10.1002/admi.201400078
TiO2 anatase grain boundary
Deep trap at GB relative
to bulk:
-0.46 eV
(c.f. rutile GB: -0.2 eV)
Nanoparticle surfaces
Low index rutile surfaces: (100), (001), (101), (110), (111)
∆E = Es - Eb
(110) surface
subsurface trap of -0.28 eV
(001) surface
surface trap of -0.4 eV
Repulsive surfaces
TiO2 rutile nanoparticles
(a) (b) (c) (d)
(110)
(101)
(001)
(100)
(110)
(001)
(101)
(101)(100)
a  equilibrium nanoparticle shape b  trapping shape
c  strongly repulsive shape d  weakly repulsive shape
K. Momma and F. Izumi, "VESTA 3 for three-dimensional visualization of crystal, volumetric and morphology data," J. Appl. Crystallogr., 44, 1272-
1276 (2011).
Correlation between trapping energy
and on-site electrostatic potential
(001) site 9
(111) site 13
Surface models
(110) (101) (100) (001) (111)
4-coordinated surface sites
Conclusion
[2] Barnard, a., & Zapol, P. (2004). Effects of particle morphology and surface hydrogenation on the phase stability of TiO2.
Physical Review B, 70(23), 235403. doi:10.1103/PhysRevB.70.235403
[3] Dinh, C., Nguyen, T., Kleitz, F., & Do, T. (2009). Shape-Controlled Synthesis of Highly Crystalline Titania Nanocrystals. ACS
Nano, 3(11), 3737–3743.
 Nanoparticle mostly composed of (110) and (101) surfaces
 (110)  strong subsurface trapping
 (101)  weakly repulsive
Reduce area of (110) relative to (101) for
improved electron transport
e.g. by surface hydrogenation [2]
or capping [3]

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UG masters project

  • 1. First principles calculations of electron mobility in nanocrystalline TiO2 Suzanne Wallace and Dr. Keith Mckenna Department of Physics, University of York, Heslington, York, UK
  • 2. DFT+U for correlated systems  Coulomb interaction of localised electrons  electron density NOT uniform  Employ DFT+U (UTi = 4.2 eV)  Correct for SI error  U: adjustable correcting potential  4.2 eV: produces good agreement with spectroscopic data [1] [1] Morgan, B. J., & Watson, G. W. (2009). J Phys Chem C, 113(110), 7322–7328.
  • 3. Finitex-dimension ∆E = Es - Eb Eb Es Localising electrons  Initialise magnetic moment at the site  Create a potential well by dilating bonds  Increase U-parameter (if necessary)
  • 4. Wallace, S. K., & McKenna, K. P. (2014). Grain Boundary Controlled Electron Mobility in Polycrystalline Titanium Dioxide. Advanced Materials Interfaces, n/a–n/a. doi:10.1002/admi.201400078
  • 5. TiO2 anatase grain boundary Deep trap at GB relative to bulk: -0.46 eV (c.f. rutile GB: -0.2 eV)
  • 6. Nanoparticle surfaces Low index rutile surfaces: (100), (001), (101), (110), (111) ∆E = Es - Eb
  • 7.
  • 11. TiO2 rutile nanoparticles (a) (b) (c) (d) (110) (101) (001) (100) (110) (001) (101) (101)(100) a  equilibrium nanoparticle shape b  trapping shape c  strongly repulsive shape d  weakly repulsive shape K. Momma and F. Izumi, "VESTA 3 for three-dimensional visualization of crystal, volumetric and morphology data," J. Appl. Crystallogr., 44, 1272- 1276 (2011).
  • 12. Correlation between trapping energy and on-site electrostatic potential (001) site 9 (111) site 13
  • 13. Surface models (110) (101) (100) (001) (111) 4-coordinated surface sites
  • 14. Conclusion [2] Barnard, a., & Zapol, P. (2004). Effects of particle morphology and surface hydrogenation on the phase stability of TiO2. Physical Review B, 70(23), 235403. doi:10.1103/PhysRevB.70.235403 [3] Dinh, C., Nguyen, T., Kleitz, F., & Do, T. (2009). Shape-Controlled Synthesis of Highly Crystalline Titania Nanocrystals. ACS Nano, 3(11), 3737–3743.  Nanoparticle mostly composed of (110) and (101) surfaces  (110)  strong subsurface trapping  (101)  weakly repulsive Reduce area of (110) relative to (101) for improved electron transport e.g. by surface hydrogenation [2] or capping [3]