TABLE OF CONTENTS
Content |
Page |
Chapter 1: Introduction |
1 |
1-1) Nanomaterials |
2 |
1-2) TiO2 Compounds |
3 |
1-3) Doping |
4 |
1-3-1) Cation-Doped TiO2 |
6 |
1-3-2) Anion-Doped TiO2 |
7 |
1-4) Objectives of the Present Thesis |
8 |
Chapter 2:Literature Review |
10 |
Chapter 3:Theoretical Background |
15 |
3-1) Density Functional Theory (DFT) |
16 |
3-2) Hybrid Functionals |
17 |
3-2-1) B3LYP Methods |
17 |
3-3) Basis Sets |
18 |
3-3-1) Double Zeta Basis Set |
18 |
3-3-2) Polarization Basis Functions |
19 |
3-3-3) Basis Set Superposition Errors (BSSEs) |
20 |
3-4) Theory of Atoms in Molecules (AIM) |
22 |
3-5) Natural Bond Orbitals (NBO) |
25 |
3-6) Density of State |
26 |
3-7) Computational Details of the Present Research |
27 |
Chapter 4:Results and Discussion |
29 |
4-1) (TiO2)n n=5,6 Nanoclusters |
30 |
4-1-1) Structural Optimization |
30 |
4-1-2) Formation Energy |
36 |
4-1-3) Electronic Structures of Doped (TiO2)n n=5,6 |
38 |
4-2) Interaction of (TiO2)n n=5,6 Nanoclusters with Hydrogen Peroxide |
47 |
4-2-1) Geometrical Structures |
47 |
4-2-2) Interaction Energies of the Complexes |
55 |
4-2-3) Atoms in Molecules Topological Parameters of the Complexes |
58 |
4-2-4) Natural Bond Orbital (NBO) Analysis |
62 |
4-3) Conclusions |
65 |
References |
67 |
Appendix |
83 |
Abstract and Title page in Persian |
LIST OF TABLES
Content |
Page |
Table 4.1 Structural data of doped (TiO2)5 nanoclusters;spin multiplicity, dipole moment and average bond lengths (dav) |
33 |
Table 4.2 Structural data of doped (TiO2)6 nanoclusters;spin multiplicity, dipole moment and Average bond lengths (dav) |
33 |
Table 4.3Formation energy of (TiO2)n n=5,6 for different positionof dopant atoms. ( eV) |
37 |
Table 4.4 HOMO and LUMO energies of pure and doped nanoclusters, HOMO-LUMO energy gap (Eg), Fermi energy (Efermi) |
40 |
Table 4.5 Bond length between titanium and oxygen of H2O2 (dTi-O), oxygen of cluster and hydrogen of H2O2 (dO-H), oxygen and oxygen in H2O2 (dO-O), bond angles of oxygen-hydrogen-oxygen (∠OHO), and dihedral angle of H2O2 in most stable complexes as well as isolate H2O2 |
54 |
Table 4.6 Adsorption energies (DEad) as well as thecounterpoise corrected interaction energies (DEcorr) and the BSSEvalues for most stable complexes (all values are in kcal mol-1 ) |
56 |
Table 4.7 Calculated adsorption energies for N-, Fe-doped and undoped (TiO2)n n=5,6 nanoclusters. (kcal mol-1) |
57 |
Table 4.8Topological parameters at BCP of O…M (M= Fe,Ti) and H…X (X= O,N ). Parameters: ρ ( r ),electron density; Ñ2 ρ ( r ), Laplacian; H ( r ), electron energy density; and – , ratio of potential to kinetic electron energy density. (au) |
59 |
Table 4.9Correlation between electron density and Ti…O and H…O bonds which has created in adsorption site |
60 |
Table 4.10 Charge transfer (CT, e) and NBO second-order interaction energy (E2, kcal mol-1) for the corresponding donor-acceptor orbital interactions of H2O2 adsorption on N-doped (TiO2)n n=5,6 nanoclusters |
64 |
Table 4.11 Charge transfer (CT, e) and NBO second-order interaction energy (E2, kcal mol-1) for the corresponding donor-acceptor orbital interactions of H2O2 adsorption on Fe-doped (TiO2)n n=5,6 nanoclusters |
64 |
LIST OF FIGURES
Content |
Page |
Fig4-1) Different position for doping in pure (TiO2)n n=5,6nano-clusters. The letters b, t, and f denote bridge, terminal andfront sites, respectively |
32 |
Fig 4-2) Optimized geometries of Fe- and N-doped (TiO2)5 nanoclusters. The blue atom belong to nitrogen, green for iron, grey for titanium and red for oxygen |
34 |
Fig 4-3) Optimized geometries of Fe- and N-doped (TiO2)6 nanoclusters. The blue atom belong to nitrogen, green for iron, grey for titanium and red for oxygen |
35 |
Fig 4-4)Variation of formation energy forpure and doped (TiO2)n n=5,6 nanoclusters |
37 |
Fig 4-5) The schematic digram of the mechanism of the N- and Fe-doped (TiO2)n n=5,6 nanoclusters. e and h refer to electron and hole, respectively |
40 |
Fig 4-6)HOMO visualization (left) and total density of states (right) of (TiO2)n n=5,6 nanostructures. The dashed line represents the position of the Fermi level. The DOS of undoped cluster,N-dopedandFe-doped are shown by Black, blue and red curves, respectively |
44 |
Fig 4-7)Natural charge distribution of the undoped and Fe-doped (TiO2)n n=5,6 nanoclusters |
46 |
Fig 4-8)Most stable optimized geometries for the interaction of Fe-doped (TiO2)5 and pure nanoclusters with H2O2 |
50 |
Fig 4-9)Most stable optimized geometries for the interaction of N-doped (TiO2)5 and pure nanoclusters with H2O2 |
51 |
Fig 4.10)Most stable optimized geometries for the interaction of Fe-doped (TiO2)6 and pure nanoclusters with H2O2 |
52 |
Fig 4.11)Most stable optimized geometries for the interaction ofN-doped (TiO2)6 and pure nanoclusters with H2O2 |
53 |
Fig 4.12)Relationship of the electron density with Ti…O and H…O bond distance |
60 |