Open access peer-reviewed chapter

The Reactivity of Anatase TiO2 (211) Surface and the Bond- Charge Counting Model

Written By

Jing Xu, Li-Fang Xu, Jian-Tao Wang and Annabella Selloni

Submitted: November 17th, 2016 Reviewed: April 11th, 2017 Published: July 26th, 2017

DOI: 10.5772/intechopen.69141

Chapter metrics overview

1,888 Chapter Downloads

View Full Metrics


In this chapter, we intend to present a generic understanding of surface reactivity and water dissociation on TiO2 surfaces through a study of anatase TiO2 (211) surface—an idea model surface containing both four-coordinated Ti atom (Ti4) and five-coordinated Ti atom (Ti5). Our first-principles calculations show that the (211) surface is a high reactivity surface and reveal that water molecule can be easily dissociated on a Ti4 site while it hardly dissociates on Ti5 site. Furthermore, we introduce bond-charge counting model to clarify the mechanism. More generally, after an intensive investigation of literature, we found that the bond-charge counting model is applicable to all anatase and rutile TiO2 surfaces including step edges and vacancies where the reactivity of surfaces enable to dissociate water attribute to the existence of Ti4 atom or equivalent Ti4 atom.


  • TiO2 surfaces
  • surface reactivity
  • water dissociation
  • first-principles calculations
  • bond-charge counting model

1. Introduction

Titanium dioxide is a semiconductor-based heterogeneous photocatalysis material which received more and more interest. In nature, TiO2 crystallizes in three different structures: rutile, anatase, and brookite, all formed by TiO6 octahedra connected by shared edges and/or corners; rutile is the thermodynamically most stable bulk phase, while anatase is very common and stable in nanomaterials. As a major polymorph of TiO2, anatase TiO2 is the most widely studied phase and is extensively used in many industrial applications such as photovoltaic cells, photo and electrochromics, photocatalysis, photonic crystals, smart surface coatings, and sensors [19]. In all applications, the surface structure plays a key role, as the surface reactivity and physicochemical properties depend strongly on the exposed crystallographic facet. Therefore, the search for high reactivity TiO2 surfaces is a topic of great interest and an area of intense activity.

The rutile (110) surface has been investigated early [1012]. Anatase is less stable than rutile, but more efficient than rutile for applications. Many studies of the anatase TiO2 surface focus on the (001) and (101) surfaces [1320]. Theoretical studies [1317] show that the (101) surface is the thermodynamically most stable surface with a small surface energy of 0.49 J/m2, while the (001) surface is the highest reactivity surface with a high surface energy of 0.98 J/m2. More recently, using different dopants, adsorbates, or solvated species, anatase TiO2 nanocrystals exposing various crystalline facets have been prepared, including low-index facets such as (001) facets [18, 19], (100) [2124], (010) [25, 26], (101) [2732], (110) [33], and (111) [34], and high-index facets such as (103), (105), (106), (201), (301), and (401) [3539]. Besides, many researchers have made extensive investigation on surface defects since those defects, e.g., step edges [4042] and O vacancy [43, 44] are intrinsic on the surfaces of crystalline materials, which strongly influence the surface chemistry.

Since the discovery of photocatalytic splitting of water on a TiO2 electrode in 1972 [1], the interaction of TiO2 surfaces with water is of special interest. The structure of the hydrated surfaces is important not only because water is always present on TiO2 surfaces, but also because it can help understand and control the catalytic and (photo) electrochemical properties of this material. In fact, different water adsorption states have been found; for example, water favors molecular adsorption on the anatase (101) surface and dissociative adsorption on the (001) surface [13].

There is still controversy for water adsorption on the TiO2 surface based only on the DFT total energy calculations, e.g., on rutile (110). Despite numerous studies on this topic in literature, the mechanism of water dissociation on TiO2 surfaces remains to be clarified. Moreover, there is still a lack of a generic understanding of different surfaces including surfaces with steps and vacancies.

Due to a recent experiment, a large percentage of exposed (211) facet has been prepared and it is found that the (211) surface can effectively improve the photocatalytic activity of TiO2 for water dissociation reactions [45, 46]. Since the surface exposes both Ti4 and Ti5 atoms, the anatase (211) surface is studied in this work as an ideal model surface to illustrate the mechanism of water dissociation on TiO2 surface [47]. The Ti4 atom plays a critical role for splitting water molecule. Furthermore, we introduce a bond-charge counting model according to TiO2 structure and conclude that two unsaturated Ti bonds are the necessary conditions for splitting water on the surface. Then, we examine as much as possible TiO2 surfaces and find the model is applicable to all surfaces.

The paper is organized as follows: the reactivity of anatase TiO2 (211) surface is briefly reviewed in Section 2; then, we propose the bond-charge counting model and give some typical examples in Section 3; finally, we present conclusion remakes in Section 4.


2. The reactivity of anatase TiO2 (211) surface

2.1. Surface structure and stability

We begin with the experimental result. Recently, a large percentage of exposed (211) facet has been identified by X-ray diffraction (XRD) on N-doped TiO2 film deposited using RF magnetron sputtering [45]. N-doped TiO2 films were deposited on quartz glass substrates (2 cm × 4 cm) by RF reactive magnetron sputtering. The crystalline structure of the as-deposited N-doped TiO2 films was identified by X-ray diffraction (XRD). Figure 1 shows the XRD patterns of N-doped TiO2 film. Diffraction peaks observed at 2θ = 25.28°, 36.95°, 37.88°, 38.55°, 48.05°, 54.09°, 54.88°, 62.67°, and 68.76°correspond well with (101), (103), (004), (112), (200), (105), (211), (204), and (116) planes of anatase phase of TiO2. It can be seen that N-doping can greatly influence the growth orientation of anatase TiO2 particles. As shown in Figure 1, the intensities of the (004), (112), (200), and especially (211) peaks become stronger, while (101) peak become weaker for the N-doped TiO2 film, compared with those of the undoped TiO2 film. Especially, the increase of exposed (211) facets can effectively improve the photocatalytic activity of TiO2 for water dissociation reactions [46], showing the high reactivity of exposed (211) facets.

Motivated by the above experimental findings, in a recent theoretical work [47], we have made a systematic study of the surface reactivity and water adsorption on anatase (211) using ab initiocalculations. Calculations have been performed by the Vienna ab initio simulation package (VASP) [4850] with all-electron projector augmented wave (PAW) method [51]. The generalized gradient approximation (GGA-PW91) [52] is set as the exchange and correlation functional. The valence states 3d24s2 for Ti, 2s22p4 for O, and 1s1 for H are used with an energy cutoff of 500 eV for the plane wave basis set. The calculated lattice constants for bulk anatase TiO2 are used to construct the diverse facets listed in Table 1. The anatase (211) surface was modeled by a slab of six layers with a unit surface cell of 7.706 Å × 5.501Å × 27.677Å (γ = 101.44°) comprising a total of 54 atoms separated by a vacuum region of 12 Å. The Monkhorst-Pack scheme [53] was adopted for the Brillouin zone integration with a 6 × 6 × 1 k-point mesh. All atoms are relaxed during geometry optimizations with the given surface cell. Convergence criteria employed for both the electronic self-consistent relaxation and the ionic relaxation were set to 10−6 eV and 0.01 eV/Å for the total energy and Hellmann-Feynman force, respectively.

FacetNatE (J/m2)n(Ti5) (10−2Å−2)n(Ti4) (10−2Å−2)n(O2) (10−2Å−2)

Table 1.

Calculated surface energies (E in J/m2) and surface densities Ti5, Ti4, and oxygen O2 atoms [n(Ti5), n(Ti4), and n(O2)]. Nat is the total number of atoms in the slab.

Figure 1.

The X-ray diffraction (XRD) on N-doped TiO2 film.

We firstly discuss the surface stability. The stoichiometric unrelaxed termination of the (211) surface is shown in Figure 2(a) There are five under-coordinated and four fully-coordinated atoms exposed to the vacuum. The five under-coordinated atoms include three inequivalent twofold-coordinated oxygen atoms denoted by O21, O22, and O23, a fourfold-coordinated Ti4 and a fivefold-coordinated Ti5, respectively. The four fully-coordinated atoms are O31, O32, O33, and Ti6 [see Figure 2(a)]. Different from (001) and (101) surfaces [12], fourfold-coordinated Ti4 atoms are present on the (211) surface. Figure 2(b) shows the optimized anatase (211) surface. After relaxation, the (211) surface shows a very corrugated structure, with a characteristic, saw tooth-like profile along the [131] direction. All under-coordinated oxygen (O2i) atoms are displaced outward, while the under-coordinated Ti4 and Ti5 atoms are relaxed inward. Both angles ∠Ti4−O22−Ti5 and ∠Ti5−O31−Ti6 become smaller, 100.3° and 147.7°, respectively. The largest relaxations are those of the fully-coordinated oxygen O31, which relaxes outward by approximately 0.35 Å, and O32, which relaxes inward by approximately 0.34 Å. Meanwhile, the surface atoms form four-membered-ring (O-Ti-O-Ti) structures on the surface. These O-Ti-O-Ti rings are slightly deformed and the distances between oxygen atoms in these rings increased from the bulk value of 2.458 Å to 2.492–2.515 Å.

Figure 2.

Structures of the unrelaxed (a) and relaxed (b) anatase (211) surfaces. The O and Ti atoms are in red and grey spheres, respectively, indicated with different coordination numbers.

To investigate the surface stability, we calculated the electronic density of states (DOS) for bare anatase (211) surface after relaxation. The result is shown in Figure 3 in comparison with the bulk TiO2. There is a big gap, as large as in bulk, in the DOS of relaxed bare anatase (211) surface, which indicates the chemical stability of the (211) surface.

Figure 3.

Electronic density of states for the bulk TiO2 and bare anatase (211) surface after relaxation. The Fermi level is set at 0 eV.

2.2. Surface energetics

The surface energies for (101), (001), and (211) are estimated using the expression, E =(Etot–nEbulk)/A, where Etotis the total energy of the slab and Ebulkis the energy of TiO2 unit in the bulk, nis the number of TiO2 units in the slab, Ais the total surface area of the slab, including both sides of the slab. The calculated surface energies are listed in Table 1. The surface energy of the (001) surface is estimated to be 1.08 J/m2, which is nearly twice that of the most stable anatase (101) surface (0.52 J/m2), in agreement with previous theoretical studies [14]. Similarly, the (211) surface has a high surface energy of 0.97 J/m2, close to that of the (001) surface.

The value of the surface energy is known to be strongly correlated to the presence of under-coordinated Ti atoms on the surface [14]. The (001) surface energy is large because of the high surface density of Ti5 (see Table 1). However, the surface energy of anatase (211) is large even though the total density of under-coordinated Ti4 and Ti5 atoms is smaller than that on the (001) surface [even smaller than on (101)]. This result already suggests that Ti4 atoms, with two unsaturated bonds, have a higher reactivity than Ti5 atoms with one unsaturated bond. A similar behavior was found also for the anatase (110) and (103)s surfaces [14].

From the above calculation results in subsections 2.1 and 2.2, we can see that the (211) surface has a large electronic band gap and high surface energy. It shows those two surface properties, stability and reactivity, seem contradictory, could uniformly hold on the (211) surface.

2.3. Water adsorption

We next present a detailed picture for the adsorption of water on the TiO2 (211) surface by considering one, two and three adsorbed water molecules corresponding to various coverages θ = 1/3, 2/3 and 1 ML per surface unit cell, respectively.

For a single water molecule (1/3 ML), there are four possible adsorption modes, corresponding to different adsorption positions (Ti4 or Ti5) and different (molecular or dissociative) adsorption conformations. For molecular water adsorption on Ti5site[see Figure 4(a)], the oxygen of water bonds to Ti5 with bond length of 2.226 Å, and two surface oxygen atoms via Ti5 form two bond angles ∠Owater−Ti5−O22 = 99.85° and ∠Owater−Ti5−O31 = 77.18°, close to the bulk angles of 101.90° and 78.10°, respectively. Upon water adsorption, the Ti5 site becomes sixfold-coordinated: the Ti atom has six Ti-O bonds with their orientations similar to those in the bulk. At the same time, the two hydrogen atoms of water form H-bonds (HBs) with two neighboring surface under-coordinated oxygen atoms, O21 and O23, with bond lengths 2.339 and 1.873 Å, respectively. As a result, the computed molecular adsorption energy on the Ti5 site is 0.784 eV. For dissociative water adsorption on Ti5 site, the water molecule is dissociated into hydroxyl (OH) and H fragments. The OH group bonds to Ti5 with a length of 1.857 Å and then further bonds to O23 with a weak HB. The H fragment forms a new OH moiety with a nearby O21. As a result, the adsorption energy for a dissociated water on Ti5 site is 0.77 eV, which is slightly smaller than that of molecular adsorption. Thus, molecular adsorption is preferred on Ti5 site.

Figure 4.

Side (left) and top (right) views of the structures for water adsorption on the anatase TiO2 (211) surface. (a) Molecular water on a Ti5 site. (b) Dissociative water on a Ti4 site. (c) Mixed state with one dissociative H2O on Ti4 and one molecular H2O on Ti5 sites at 2/3 ML. (d) Mixed state on Ti4 and Ti5 sites at 1 ML coverage. The O atom of water is plotted in orange, the H atom is in blue, and the H-bond is indicated by a dashed line.

On the other hand, for molecular water on a Ti4 site, the oxygen atom of water binds to Ti4 with a bond length of 2.207 Å, and Ti4 is located at the position of one of the bulk Ti-O bonds indicating that there is one Ti bond left. The Ti4 adsorption site becomes fivefold-coordinated and the adsorption energy for molecular water on Ti4 site is estimated to be 0.99 eV. Finally, for dissociative water on Ti4site[see Figure 4(b)], the O atom of the OH group is strongly bonded to the Ti4 atom with a short bond length of 1.847 Å (as compared to the Ti-O bond length of 2.207 Å in the molecular adsorption case) so that the Ti4 adsorption site becomes fivefold-coordinated. It is worthwhile to point out that the adsorption position of the O atom of the OH group does not correspond to the position of a bulk Ti-O bond, but is in the middle of the two missing bulk Ti-O bonds, and the orientation of Ti4-OOH bond clearly deviates from its direction in the bulk, as shown by the two bond angles ∠OOH−Ti4−O33 = 130.86° and ∠OOH−Ti4−O32 = 119.91°. This adsorption geometry with short bond length and a middle position indicates that the dissociated water interacts with two unsaturated Ti4 bonds indeed. Furthermore, the hydrogen atom of OH forms a weak HB with a neighboring O23 atom of length 2.534 Å. The dissociated H from water interacts with a surface oxygen O23 forming a new OH moiety with a bond length of 1.013 Å and further forms an HB of 1.598 Å with O22. As a result, the adsorption energy for dissociated water on Ti4 site is estimated to be 1.28 eV, which is significantly larger than the value of 0.99 eV obtained for molecular adsorption.

To obtain further insight, we show the projected densities of states of the surface with a dissociative water on a Ti4 site and molecular water on Ti5 site in Figure 5. We can see that the O-2p orbitals in the OH group are extended to a wide range between −3.2 and −0.9 eV, indicating that the O atom of OH is strongly interacting with the substrate. On the other hand, for the case with a molecular water adsorption on a Ti5 site, all peaks from the water molecule are sharp and are simply superimposed on those of the bare surface, indicating that they interact weakly with the surface.

Figure 5.

Projected electronic density of states on anatase (211) surface (a) for O-2s,pin the OH group on Ti4 site; (b) for O-2s, pin water on Ti5 site; The Fermi level is set at 0 eV.

Combined together the above four calculation results: the adsorption energy, bond length, bond angle, and DOS, we can conclude that dissociative adsorption can easilyhappen at the Ti4 site while hardlyhappens on Ti5. In fact, these different behaviors can be understood in terms of a simple model based on the bond-charge distribution, which is the key issue in this paper and will be discussed in the next section.

Now, let us consider more water adsorption case. For two adsorbed H2O molecules (2/3 ML coverage), the first H2O prefers to adsorb at a Ti4 site in dissociative form according to the single water-adsorption results; next, another water molecule should adsorb on a Ti4 or Ti5 site. For the structure with one dissociated H2O on a Ti4site and one molecular H2O on a Ti5site[see Figure 4(c)], the O-Ti5 bond is 2.230 Å, while the O-Ti4 bond length is much shorter, 1.992 Å. The dissociated H combines with an O23 atom forming a new OH moiety and further forms a strong HB (1.590 Å) with an O22 atom. An additional HB between two water molecules forms with a bond length of 1.775 Å, which makes two water molecules closer and changes the values of the bond angles. In this mixed structure (c), the adsorption energy is 1.045 eV/mol, which is a little larger than the averaged value of 1.034 eV [(1.284 + 0.784)/2] for the single water adsorption on Ti4 and Ti5 sites due to the contribution of the new HB. On the contrary, for the structure with two dissociated H2O on Ti4 and Ti5 sites, the adsorption energy is estimated to be 0.991 eV/mol, which is about 0.036 eV smaller than the averaged value of 1.027 eV [(1.284 + 0.770)/2] for the single water adsorption and also 0.054 eV lower than that of the mixed configuration. These results confirm that molecular adsorption is preferred on Ti5 in the mixed structure. Moreover, for a structure with one dissociated H2O and one associated H2O on Ti4 sites and structure with two dissociated H2O on Ti4 sites, the adsorption energy is estimated to be 0.960 and 0.916 eV/mol, respectively. Those are clearly lower than 1.045 eV/mol for the mixed structure. Therefore, with increasing coverage, water molecules prefer to be adsorbed in a mixed form with one dissociated H2O on a Ti4 site and one molecular H2O on a Ti5 site.

Finally, we discuss the monolayer coverage where three water molecules are adsorbed per surface unit cell. Following the 2/3 ML result with one dissociated H2O on a Ti4 site and one molecular H2O on a Ti5 site, the third molecule would adsorb molecularly on a Ti4 site [see Figure 4(d)]. It is an O atom that binds to Ti4 with a bond length of 2.259 Å, while the two H atoms form HBs with nearby O atoms, where H-O21 is 2.156 Å and H-O22 is 1.907 Å. The bond length for molecular water on a Ti5 atom is 2.221 Å, while for dissociated water on Ti4 it is 1.934 Å. Two bond angles ∠OOH−Ti4−O33 and ∠Owater−Ti4−O32 are 100.69° and 79.00°, respectively. Thus, all Ti atoms are sixfold-coordinated with orientations similar to those of a bulk Ti atom. The dissociated H is captured by an O23 atom to form an OH moiety and further interacts with an O22 atom forming an HB of 1.835 Å. An additional HB of 1.652 Å also exists between these two adsorbed H2O. All surface atoms become saturated. The adsorption energy has a larger value of 0.946 eV/mol for this mixed configuration on Ti4 sites. For comparison, we also consider configuration with two dissociated water molecules on Ti4 sites and one molecular H2O on Ti5. Though all surface atoms are also saturated, its adsorption energy is 0.909 eV/mol, which is lower than that of the mixed configuration with one dissociative and one molecular adsorption on Ti4. Thus, molecular adsorption is favored on Ti4 for the second water molecule. Meanwhile, for structure with one intact water on Ti4 and two dissociated water molecules on Ti4 and Ti5 sites, the computed adsorption energy is 0.902 eV/mol; for structure with three dissociated water molecules on Ti4, Ti4, and Ti5 sites, the adsorption energy is 0.833 eV/mol (see Table 2). These results suggest that a mixed water configuration is formed at monolayer coverage, with one dissociated water on Ti4, one molecular water on Ti4, and one molecular water on Ti5.

θ (ML)StructureH2OH, OHΔH (eV)
1/3Figure 4(a)Ti50.784
Figure 4(b)Ti41.284
2/3Figure 4(c)Ti5Ti41.045
Ti4, Ti40.916
3/3Figure 4(d)Ti4,,Ti5Ti40.946
Ti5Ti4, Ti40.909
Ti4, Ti4,Ti50.883

Table 2.

Adsorption energy (ΔH in eV) per H2O molecule on anatase (211) at various water coverages θ = 1/3, 2/3, and 1 ML.

The adsorption states are shown as H2O = molecular and H, OH = dissociative on a Ti4 or Ti5 site.

Our results show that Ti4 is an only active site which can dissociate water. Once Ti4 is saturated with a water, there will be no more water can be dissociated. It corresponds well with the experimental observations that the dissociation does occur only at low coverages and the probability of H2O dissociation is decreased with increasing surface coverage. That is the purpose that we describe adsorption in detail from low water coverage to full coverage in this section.


3. The bond-charge counting model for TiO2 surfaces

3.1. The mechanism and a simple phenomenological model

According to the above results, the adsorption energies of water on a Ti4 site are always larger than those on a Ti5 site (see Table 2). Moreover, a water molecule can be easily dissociated on a Ti4 site while it hardly dissociates on Ti5. We use a word “hardly” here because there is still controversy for the adsorption of H2O on Ti5 site. In our case, the adsorption energy for a molecular adsorption on Ti5 site is only slightly higher than the dissociated one, which is not adequately to convince that water cannot be dissociated on Ti5. Actually, there are a lot of arguments on this issue in literature. Lindan et al. [12] suggested that dissociative adsorption happened on the rutile (110) surface, while Schaub’s result [43] is in contrast to that. However, there is an important case that water is indeed dissociated on anatase (001) surface with only Ti5 atom [13]. Therefore, whether Ti5 atom can dissociate water is still a matter for controversy on TiO2 surfaces.

Many research works are only concentrated on the total energy calculations in literature. DFT total energy calculations are a definitely powerful tool. But here there is a shortcoming that total energy calculations just tell the total energy of the system, not the local interaction energy. For example, in dissociative adsorption, the total energy includes the adsorption site of the dissociated H as well as H-bond energy at high coverage case. Thus, it is difficult to extract the onsite interaction energy and it is hard to obtain a clear conclusion just from the total energy. All those controversies come from the information of total energy and less considerations for the reaction mechanism. Therefore, it is necessary to think it over from the origin of physics and chemistry beyond total energy calculation.

The water dissociation on surface is a chemical adsorption, which can be regarded as a chemical reaction analogue to a chemical displacement reaction, e.g., 2Na + 2H2O = 2NaOH + H2↑. In this displacement reaction, the necessary condition is that more active metal atom can substitute the less active metal atom or hydrogen. Also, from a physical point of view, the O atom in water must gain more electrons that H atom provided so that such a dissociation process happens by losing an H atom. From these considerations, we propose a simple bond-charge counting model based on the charge distribution on Ti bond in TiO2.

In bulk TiO2, each Ti atom has six nearest neighboring O atoms and Ti atom has four outmost electrons, i.e., each Ti4+ ion is surrounded by an octahedron of six O2− ions. Thus, on an average, each Ti atom can offer 4/6 electron charge at each Ti-O bond. It holds for both rutile and anatase since they have the same TiO6 octahedra structure. Therefore, we could make a simple bond-charge counting for this system. When a Ti4 atom interacts with the oxygen atom of H2O, two unsaturated Ti bonds participate in the interaction and offer about 4/3 electron charge to this O atom by forming a strong bond [see Figure 4(b)]. Thus, it satisfies the reaction requirement and Ti4 is more active than H atom. Then, one H atom can be released from the water molecule on a Ti4 site. In fact, one H atom dissociates spontaneously from the water molecule as this adsorbs on a Ti4 atom. On the other hand, Ti5 can only provide about 2/3 electron charge to the water O atom, less than the charge contribution from an H atom. Therefore, Ti5 is less active than H atom and hardly causes dissociation of an H atom. Although there is very little difference in energy (0.014 eV) between molecular and dissociated structures, we can clearly judge that water favors molecular adsorption and is unfavorable on Ti5 site.

The essence of the model is qualitatively taking account of average charge on each Ti bond in TiO2 material. The model is phenomenological and does not intend to provide the precise value of charge transferred during interaction due to the complex of 3d orbitals of Ti atom in TiO6 octahedra. Nevertheless, the bond-charge counting model clarifies the intrinsic charge difference between Ti4 and Ti5 atoms on surfaces where Ti4 can provide more than one electron and Ti5 much less one electron. The necessary condition for water splitting is that the surface Ti atoms must provide more than one electron to O atom of water. The charge contributed from a single Ti bond is not sufficient for water dissociation. Therefore, two unsaturated Ti bonds satisfy the condition corresponding to the four-coordinated Ti4 atom that has chemical reactivity, while Ti5 atom not.

3.2. Typical examples

In order to verify this model, we have made an intensive investigation for TiO2 surface as much as we could find in literature including steps and vacancies. We found that all reactive surfaces splitting water are associated with Ti4 atom or equivalent Ti4 atom without any exception. We are not able to exhaust all surfaces here, rather list typical and important surfaces in different geometric categories as follows.

3.2.1. Surfaces with Ti4 atom

We start the survey from the TiO2 surfaces with Ti4 atoms. At anatase surfaces, the (110) and (103)scontain Ti4 atoms. Therefore, their surface energies are 1.15 and 0.99 J/m2, respectively [14]. Those rather high values indicate that the surfaces have a very high reactivity contributed from Ti4 atoms.

3.2.2. Surface with only Ti5 atom

The surfaces with only Ti5 atom are more interesting. Whether the surfaces can dissociate water is controversy. We will see it strongly depends on its surface energy. As anatase (001) surface, the surface energy has a rather high value of 0.98 J/m2 indicating a high reactivity. Thus, it is clearly pointed out in Ref. [13] that the structure of the dissociated state (in Figure 6(a) same as in Figure 3(a) in Ref. [13]) is characterized by the breaking of the bond between the bridging 2c oxygen and the Ti5 atoms involved in the adsorption, i.e., the Ti5 atom actually becomes fourfold-coordinated after breaking its bond to a bridging O atom. Therefore, the dissociative water is absorbed on an equivalent Ti4 site. It is expected that such phenomenon of Ti5 atom breaking bond with neighboring oxygen becomes an effective Ti4 atom which would be held for the anatase (103)fsurface with the high surface energy of 0.9 J/m2.

Figure 6.

(Figure 3in Ref. [13]) Atomic structure (side view) for adsorbed water molecule(s) on anatase (001). (a) Dissociated state. (b) Molecular state. (c) Mixed state. Gray lines in (b) and (c) indicate hydrogen bonds. Bond lengths are in Å.

However, for the other surfaces only containing Ti5 atoms, their surface energies are very small. The values are 0.49 and 0.58, and 0.35 J/m2 for anatase (101) and (100), and rutile (110), respectively. Note that the rutile (110) surface has smallest surface energy. Thus, the anatase (101) [13] and rutile (110) [11] are thermodynamically most stable structures. We can rule out the possibility of water dissociation on those surfaces [10].

Combined with the surface energy, we may estimate which surface with only Ti5 atom can dissociate water by breaking a Ti bond. According to calculations, the surface energy should approach to ~1 J/m2. For the high reactive surfaces with only Ti5, the Ti5 atoms eventually become too effective Ti4 atoms during the interaction.

3.2.3. Surfaces with steps

Step edges are the most common intrinsic defects on the surface. In this subsection, we give two examples of steps on two most stable surfaces, anatase (101) and rutile (110) surface.

Gong et al. [40] have made an intensive investigation on anatase (101) surface. The structure models of step edges they studied are shown in Figure 7. We can divide those surface step structures into two categories with Ti4 (in Figure 7(a), (d), (e), (f), and (h)) and without Ti4 atoms (in Figure 7(b), (c), and (g)). Then, we recapitulate their surface energy calculation results γ (θ) in unit 10-2eV/Å2 and rearrange in an order of containing Ti4 and Ti5 atoms as follows:

Figure 7.

Structure models of step edges A–E on anatase (101) (Figure 2in Ref. [40]).

AI(Figure 7(a))5.364.684.34Ti4
CI(Figure 7(e))5.494.814.46Ti4
CII(Figure 7(f))
E(Figure 7(h))6.825.865.34Ti4
AII(Figure 7(b))4.604.244.06Ti5
BI(Figure 7(c))3.663.59Ti5
D(Figure 7(g))4.524.113.94Ti5

We omit the labels of vicinal surfaces here for simplicity. The surface energies with Ti4 are larger than that with Ti5 in each column. Gong et al. further studied water adsorption on D, BI, and AII with Ti5 atom (see Supplementary Information in Ref. [40]). On D-type step edge, both molecular and dissociative H2O adsorption can occur, but energy difference is much smaller than on flat TiO2 (101). For BI step, the adsorption energies are smaller than that on the (101) surface. Note BI has the smallest surface energy among all step structures. On the least stable AII with the highest surface energy among steps containing Ti5 atom, the water adsorption is found to be similar to the anatase (001) surface where water is dissociatively adsorbed with adsorption energy 1.28 eV. Again, here surface Ti5 atom becomes Ti4 by breaking a bond with neighboring oxygen.

Hong et al. [41] investigated water adsorption behavior step edges on rutile TiO2 (110) surface using DFT calculations. They found that the < 1-10 > edge exhibits significantly enhanced water adsorption, especially dissociative adsorption, as compared to the pristine (110) surface and < 001 > step edge due to the existence of fourfold coordinated Ti4 atoms at the < 1-10 > step edge, which lead to charge transfer to adsorbates more easily than fivefold coordinated Ti5 atoms on the (110) surface and < 001 > step edge.

Later, Zheng et al. [42] studied the associative and dissociative adsorption of water molecules on rutile TiO2 (110) surface with step defects by DFT calculations. The step structures were created by removing the TiO2 unit along the < 1-11 > direction and exposing the Ti4 atoms (terminating the Ti rows of the upper terrace) and the Ti5 atoms (see Figure 1(a), (b) in Ref. [42]). They only considered the case of Ti bonds fully saturated. Their results show that the molecular and dissociative adsorptions of H2O can both be observed on Ti4 sites and the molecularly absorbed water is more favorable on the Ti5 sites. The lowest energy corresponds to the configuration where water molecule on Ti5 site and one dissociated and one molecular water on Ti4 site, same as our result for anatase (211) surface [47].

Thus, dissociative adsorption is also attributed to the existence of Ti4 atoms and/or equivalent Ti4 atoms exposing at step edges on anatase (101) and rutile (110) surfaces.

3.2.4. Surfaces with O vacancy

Oxygen vacancy is also one of the most common defects on the surface. Again, in this subsection, we give two examples of O vacancy on two most stable surfaces, rutile (110) and anatase (101).

Schaub et al. [43] investigated the O vacancy on rutile (110) through both experiments and DFT calculation and determined the O vacancies as active sites responsible for the dissociation of water molecules. Their DFT calculation results show that the dissociation of water is only at oxygen vacancies with an adsorption energy of 0.94, while on the perfect (100) surface, water molecule binds to the surface by 0.56 eV and the dissociation of water is even endothermic by 0.23 eV. The dissociative adsorption is unfavorable on the perfect (100) surface. They explained that the large reactivity of the vacancies is associated with the high-energy defect and water dissociation is simply to refill the coordination shell of Ti underneath the vacancy. However, there will be something more than that. Note that the twoTi6 atoms underneath the vacancy become Ti5 atoms when O leaves the surface. Thus, when O atom of water is to refill the O vacancy, the twoTi5 atoms interact with O of water simultaneously. Then, in this case, we should count two Ti bonds participating in interaction. Therefore, the dissociation of water is due to the combined contribution of two unsaturated Ti atoms.

On the anatase (101) surface, dissociation of water close to the oxygen vacancy is energetically favored compared to molecular adsorption. Tilocca and Selloni [44] have done a detailed calculation of energy barrier between the molecular and dissociated states. When a surface O atom is removed, the Ti6 and Ti5 atoms bridging this O atom tune into Ti5 and Ti4, respectively. Water oxygen bonds to Ti4 and then dissociates through a dissociation pathway. Thus, the dissociation of water on O vacancy of anatase (101) is also attributed to that Ti4 atom.

3.2.5. Surfaces with Ti3 atom

Recently, the three-coordinated Ti atom (Ti3) are found on the (111) anatase TiO2 surfaces. Xu et al [34] reported that they prepared anatase TiO2 single crystals exposed (111) facet. Their DFT calculations showed that the (111) facet has a much higher surface energy of 1.61 J/m2, which is attributed to the large percentage of under-coordinated atoms. They also found that this material has much higher photocatalytic activity than other surfaces. Here, there are Ti3 and Ti5 atoms with the ratio 1:3 on the (111) surface. According to our model, the Ti3 atom could contribute two electrons participating interaction. Thus, it is expected that two water molecules could be dissociated on a single Ti3 site. It could explain the (111) surface has much higher photocatalytic activity than other surfaces.


4. Conclusions

In conclusion, we use the anatase (211) surface as an idea model surface, containing one Ti4 and one Ti5 under-coordinated atoms in unit cell, to investigate their distinct properties. Our ab initiocalculations show that the (211) surface is indeed a high reactivity surface with a high surface energy of 0.97 J/m2. In addition, the four-coordinated Ti4 atoms with two unsaturated bonds have a stronger chemical reactivity in comparison to the Ti5 atoms with one unsaturated bond. Studies of water adsorption suggest two distinct states of adsorbed water on the (211) surface, one related to molecular water on Ti5 sites and the other to dissociated water on Ti4 sites. These results indicate that the Ti4 atoms will play a critical role in water decomposition. According to TiO2 structure, we propose a simple bond-charge counting model where each unsaturated Ti bond contributes 2/3 charge in average. As a necessary requirement of chemical reaction, the dissociation of water only occurs when Ti atoms provide more electrons to oxygen in water than H atom. Then, we reach to a conclusion that only Ti4 atom or equivalent Ti4 can dissociate water. The controversy about whether Ti5 can dissociate water is resolved that Ti5 atom will eventually become Ti4 by breaking bond to neighboring O atom at surface with high surface energy while the dissociation will not happen for surface with low surface energy. Besides traditional DFT total energy calculation, this model is considered in a fundamental way. We can also declare that the bond charge offered by surface Ti atoms is the mechanism for water dissociation on TiO2 surface. Furthermore, the model is generic and applicable to both rutile and anatase surfaces including defects, e.g., step edges and vacancies.



We acknowledge the useful discussions with Y.G. Cao. This work was supported by the National Science Foundation of China (Grants No. 10774177, No. 10634070, and No.11174297), and the National Basic Research Project (Grants No. 2010CB923002 and No. 2011CB922204), and the Fundamental Research Funds for the Central Universities, and the Research Funds of Renmin University of China.


  1. 1. Fujishima A, Honda K. Electrochemical photolysis of water at a semiconductor electrode. Nature (London). 1972;238: 37-38. DOI: 10.1038/238037a0
  2. 2. Regan BO, Grätzel M. A low-cast, high-efficiency solar-cell based on dye-sensitized colloidal TiO2 films. Nature. 1991;353: 737-740. DOI: 10.1038/353737a0
  3. 3. Linsebigler AL, Lu G, Yates JT. Photocatalysis on TiO2 surface principles, mechanisms, and selected results. Chemical Reviews. 1995;95: 735-758. DOI: 10.1021/cr00035a013
  4. 4. Grätzel M. Photoelectrochemical cells. Nature. 2001;414: 338-344. DOI: 10.1038/35104607
  5. 5. Fujishima A, Zhang X, Tryk DA. TiO2 photocatalysis and related surface phenomena—Review, Surface Science Reports. 2008;63: 515-582. DOI: 10.1016/j.surfrep.2008.10.001
  6. 6. Li Y, Somorjai GA. Nanoscale advances in catalysis and energy applications, Nano Letters. 2010;10: 2289-2295. DOI: 10.1021/nl101807g
  7. 7. Liu G, Yang HG, Pan J, Yang YQ, Lu GQ, Cheng HM. Titanium dioxide crystals with tailored facets, Chemical Reviews. 2014;114: 9559-9612. DOI: 10.1021/cr400621z
  8. 8. Fang WQ, Gong XQ, Yang HG. On the unusual properties of anatase TiO2 exposed by highly reactive facets, The Journal of Physical Chemistry Letters. 2011;2: 25-734. DOI: 10.1021/jz200117r
  9. 9. Hagfeldt A, Boschloo G, Sun L, Kloo L, Pettersson H. Dye-sensitized solar cells, Chemical Reviews. 2010;110: 6595-6663. DOI: 10.1021/cr900356p
  10. 10. Henderson MA. Structural sensitivity in the dissociation of water on TiO2 single-crystal surfaces, Langmuir. 1996;12: 5093-5098. DOI: 10.1021/la960360t
  11. 11. Charlton G, Howes PB, Nicklin CL, Steadman P, Taylor JSG, Muryn CA, Harte SP, Mercer J, McGrath R, Norman D. Relaxation of TiO2(110)-(1x1) using surface X-ray diffraction, Physical Review Letters. 1997;78: 495-498. DOI: 10.1103/PhysRevLett.78.495
  12. 12. Lindan, PJD, Harrison NM, Gillan MJ. Mixed dissociative and molecular adsorption of water on the rutile (110) surface, Physical Review Letters. 1998;80: 762-765. DOI: 10. 1103/PhysRevLett.80.762
  13. 13. Vittadini A, Selloni A, Rotzinger FP, Grätzel M. Structure and energetics of water adsorbed at TiO2 Anatase (101) and (001) surfaces, Physical Review Letters. 1998;81: 954-2957. DOI: 10.1103/PhysRevLett.81.2954
  14. 14. Lazzeri M, Vittadini A, Selloni A. Structure and energetics of stoichiometric TiO2 anatase surfaces, Physical Review B. 2001;63: 155409. DOI: 10.1103/PhysRevB.63.155409
  15. 15. Diebold U. The surface science of titanium dioxide. Surface Science Reports. 2003;48: 53-229. DOI: 10.1016/S0167-5729(02)00100-0
  16. 16. Gong XQ, Selloni A. Reactivity of anatase TiO2 nanoparticles: The role of the minority (001) surface, The Journal of Physical Chemistry B. 2005;109: 19560-19562. DOI: 10.1021/jp055311g
  17. 17. Gong XQ, Selloni A, Vittadini A. Density functional theory study of formic acid adsorption on anatase TiO2 (001): Geometries, energetics, and effects of coverage, hydration, and reconstruction, The Journal of Physical Chemistry B. 2006;110: 2804-2811. DOI: 10.1021/jp056572t
  18. 18. Yang HG, Sun CH, Qiao SZ, Zou J, Liu G, Smith SC, Cheng HM, Lu GQ. Anatase TiO2 single crystals with a large percentage of reactive facets, Nature (London). 2008;453: 638-641. DOI: 10.1038/nature06964
  19. 19. Selloni A. Crystal growth—Anatase shows its reactive side, Nature Materials. 2008;7: 613-615. DOI: 10.1038/nmat2241
  20. 20. Angelis FD, Valentin CD, Fantacci S, Vittadini A, Selloni A. Theoretical studies on anatase and less common TiO2 phases: Bulk, surfaces, and nanomaterials, Chemical Reviews. 2014;114: 9708-9753. DOI: 10.1021/cr500055q
  21. 21. Li JM, Cao K, Li Q, Xu DS. Tetragonal faceted-nanorods of anatase TiO2 with a large percentage of active {100} facets and their hierarchical structure. CrystEngComm. 2012;14: 83-85. DOI: 10.1039/c1ce06229h
  22. 22. Wu L, Yang BX, Yang XH, Chen ZG, Li Z, Zhao HJ, Gong XQ, Yang HG. On the synergistic effect of hydrohalic acids in the shape-controlled synthesis of anatase TiO2 single crystals, CrystEngComm 2013;15: 3252-3255. DOI: 10.1039/c2ce26744f
  23. 23. Lai ZC, Peng F, Wang Y, Wang HJ, Yu H, Liu P, Zhao HI. Low temperature solvothermal synthesis of anatase TiO2 single crystals with wholly {100} and {001} faceted surfaces, Journal of Materials Chemistry. 2012;22: 23906-23912. DOI: 10.1039/c2jm34880b
  24. 24. Li JM, Xu DS. Tetragonal faceted-nanorods of anatase TiO2 single crystals with a large percentage of active {100} facets, Chemical Communications (Cambridge). 2010;46: 2301-2303. DOI: 10.1039/b923755k
  25. 25. Ding XK, Ruan HC, Zheng C, Yang J, Wei MD. Synthesis of TiO2 nanoparticles with tunable dominant exposed facets (010), (001) and (106), CrystEngComm. 2013;15: 3040-3044 DOI: 10.1039/c3ce27097a
  26. 26. Wu BH, Guo CY, Zheng NF, Xie ZX, Stucky GD. Nonaqueous production of nanostructured anatase with high-energy facets {001} or {010} facets, Journal of the American Chemical Society. 2008;130: 17563-17567. DOI: 10.1021/ja8069715
  27. 27. Wu D, Gao Z, Xu F, Chang J, Gao S, Jiang K. Anatase TiO2 nanocrystals enclosed by well-defined crystal facets and their application in dye-sensitized solar cell, CrystEngComm. 2013;15: 516-523. DOI: 10.1039/c2ce26454d
  28. 28. Gordon TR, Cargnello M, Paik T, Mangolini F, Weber RT, Fornasiero P, Murray CB. Nonaqueous synthesis of TiO2 nanocrystals using TiF4 to engineer morphology, oxygen vacancy concentration, and photocatalytic activity. Journal of the American Chemical Society. 2012;134: 6751-6761. DOI: 10.1021/ja300823a
  29. 29. Wu N, Wang J, Tafen DN, Wang H, Zheng J-G, Lewis JP, Liu X, Leonard SS, Manivannan A. Shape enhanced photocatalytic activity of single-crystalline anatase TiO2 (101) nanobelts, Journal of the American Chemical Society. 2010;132: 6679-6685. DOI: 10.1021/ja909456f
  30. 30. Chen C, Hu R, Mai K, Ren Z, Wang H, Qian G, Wang Z. Shape evolution of highly crystalline anatase TiO2 nanobipyramids {001} and {101} facets, Crystal Growth & Design. 2011;11: 5221-5226. DOI: 10.1021/cg200457g
  31. 31. Pan JH, Han G, Zhou R, Zhao XS. Hierarchical N-doped TiO2 hollow microspheres consisting of nanothorns with exposed anatase {101} facets, Chemical Communications (Cambridge). 2011;47: 6942-6944. DOI: 10.1039/c1cc11796c
  32. 32. Horvat B, Rečnik A, Dražić G. The growth of anatase bipyramidal crystals during hydrothermal synthesis, Journal of Crystal Growth. 2012;347: 19-24. DOI: 10.1016/j.jcrysgro.2012.03.027
  33. 33. Liu M, Piao L, Zhao L, Ju S, Yan Z, He T, Zhou C, Wang W. J. Anatase TiO2 single crystals with exposed {001} and {110} facets: Facile synthesis and enhanced photocatalysis, Chemical Communications (Cambridge). 2010;46: 1664-1666. DOI: 10.1039/b924172h
  34. 34. Xu H, Reunchan P, Ouyang SX, Tong H, Umezawa N, Kako T, Ye JH. Anatase TiO2 single crystals exposed with high-reactive {111} facets toward efficient H2 evolution, Chemistry of Materials. 2013;25: 405-411. DOI: 10.1021/cm303502b
  35. 35. Yang WG, Xu YY, Tang Y, Wang C, Hu YJ, Huang L, Liu J, Luo J, Guo HB, Chen YG, Shi WM, Wang YL. Three-dimensional self-branching anatase TiO2 nanorods: Morphology control, growth mechanism and dye-sensitized solar cell application, Journal of Materials Chemistry A. 2014;2: 16030-16038. DOI: 10.1039/c4ta02761b.
  36. 36. Jiang HB, Cuan Q, Wen CZ, Xing J, Wu D, Gong X-Q, Li C, Yang HG. Anatase TiO2 crystals with exposed high-index facets (105), Angewandte Chemie International Edition. Ed. 2011;50: 3764-3768. DOI: 10.1002/anie.201007771.
  37. 37. Wu L, Jiang HB, Tian F, Chen Z, Sun C, Yang HG. Ti0.89Si0.11O2 single crystals bound by high-index {201} facets showing enhanced visible-light photocatalytic hydrogen evolution, Chemical Communications (Cambridge). 2013;49: 2016-2018. DOI: 10.1039/c3cc38105f
  38. 38. Yang MH, Chen PC, Tsai MC, Chen TT, Chang IC, Chiu HT, Lee CY. Alkali metal ion assisted synthesis of faceted anatase TiO2 {101} and {301} exposed were synthesized, CrystEngComm. 2013;15: 2966-2971. DOI: 10.1039/c3ce26965e
  39. 39. Wu HB, Chen JS, Lou XW, Hng HH. Asymmetric anatase TiO2 nanocrystals with exposed high-index facets and their excellent lithium storage properties. Nanoscale. 2011;3: 4082-4084. DOI: 10.1039/c1nr10854a
  40. 40. Gong XQ, Selloni A, Batzill M, Diebold U. Steps on anatase TiO2 (101), Nature Materials.2006;5: 665-670. DOI: 10.1038/nmat1695
  41. 41. Hong F, Ni YH, Xu WJ, Yan YF. Origin of enhanced water adsorption at <1-10> step edge on rutile TiO2 (110) surface, The Journal of Chemical Physics. 2012;137: 114707. DOI: 10.1063/1.4753951
  42. 42. Zheng T, Wu C, Chen MJ, Zhang Y, Chummings PT. A DFT study of water adsorption on rutile TiO2 (110) surface: The effects of surface steps, The Journal of Chemical Physics. 2016;145: 044702. DOI: 10.1063/1.4958969
  43. 43. Schaub R, Thostrup P, Lopez N, Lægsgaard E, Stensgaard I, Nørskov JK, Besenbacher F. Oxygen vacancies as active sites for water dissociation on rutile TiO2 (110), Physical Review Letters. 2001;87: 266104. DOI: 10.1103/PhysRevLett. 87. 266104
  44. 44. Tilocca A, Selloni A. Reaction pathway and free energy barrier for defect-induced water dissociation on the (101) surface of TiO2-anatase, The Journal of Chemical Physics. 2003;119: 7445. DOI: 10.1063/1.1607306
  45. 45. Wang C, Hu QQ, Huang JQ, Wu L, Deng ZH, Liu ZG, Liu Y, Cao YG. Efficient hydrogen production by photocatalytic water splitting using N-doped TiO2 film. Applied Surface Science. 2013;283: 188-192. DOI: 10.1016/j.apsusc.2013.06.080
  46. 46. Wang C, Hu QQ, Huang JQ, Deng ZH, Shi HL, Wu L, Liu ZG, Cao YG. Effective water splitting using N-doped TiO2 films: Role of preferred orientation on hydrogen production, International Journal of Hydrogen Energy. 2014;39: 1967-1971. DOI: 10.1016/j.ijhydene.2013.11.097
  47. 47. Xu J, Xu LF, Li ZZ, Wang JT, Lin ZS, Liu K, Cao YG, Selloni A.Ab Initiostudy of water adsorption and reactivity on the (211) surface of anatase TiO2, Physical Review Applied. 2016;5: 064001. DOI: 10.1103/PhysRevApplied.5.064001
  48. 48. Kresse G, Hafner J.Ab initiomolecular dynamics for liquid metals, Physical Review B. 1993;47: 558-561. DOI: 10.1103/PhysRevB.47.558
  49. 49. Kresse G, Furthmüller J. Efficiency ofab-initiototal energy calculations for metals and semiconductors using a plane-wave basis set, Computational Materials Science. 1996;6: 15-50. DOI: 10.1016/0927-0256(96)00008-0
  50. 50. Kresse G, Furthmüller J. Efficient iterative schemes forab initiototal-energy calculations using a plane-wave basis set, Physical Review B. 1996;54: 11169-11186. DOI: 10.1103/PhysRevB.54.11169
  51. 51. Blöchl PE. Projector augmented-wave method. Physical Review B. 1994;50: 17953-17979. DOI: 10.1103/PhysRevB.50.17953
  52. 52. Wang Y, Perdew JP. Correlation hole of the spin polarized electron gas, with exact small-wave-vector and high-density scaling, Physical Review B. 1991;44: 13298-13307. DOI: 10.1103/PhysRevB.44.13298
  53. 53. Monkhorst HJ, Pack JD. Special points for Brillouin zone integrations, Physical Review B. 1976;13: 5188-5192. DOI: 10.1103/PhysRevB.13.5188

Written By

Jing Xu, Li-Fang Xu, Jian-Tao Wang and Annabella Selloni

Submitted: November 17th, 2016 Reviewed: April 11th, 2017 Published: July 26th, 2017