International Journal of Photoenergy

Volume 2012 (2012), Article ID 269654, 10 pages

doi:10.1155/2012/269654

Review Article

Nitrogen Incorporation in TiO₂: Does It Make a Visible Light Photo-Active Material?

B. Viswanathan and K. R. Krishanmurthy

National Centre for Catalysis Research, Indian Institute of Technology Madras, Chennai 600 036, India

Received 18 January 2012; Revised 11 April 2012; Accepted 26 April 2012

Academic Editor: Xuxu Wang

Copyright © 2012 B. Viswanathan and K. R. Krishanmurthy. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

Abstract.

The possibility of hydrogen production by photo-catalytic decomposition of water on titania has provided the incentive for intense research. Titania is the preferred semiconductor for this process, in spite of its large band gap (~3.2 eV) that restricts its utility only in the UV region. Various sensitization methodologies have been adopted to make titania to be active in the visible region. Doping of TiO₂ with nitrogen is one such method. The purpose of this presentation is to examine the state and location of nitrogen introduced in TiO₂ lattice and how far the shift of optical response to visible radiation can be beneficial for the observed photo-catalysis. The specific aspects that are discussed in this article are: (i) N-doped titania surface adopts a non-native configuration, though the bulk material is still in the native configuration of pure TiO₂ (ii) Though the nitrogen doped materials showed optical response in the visible region, the changes/improvements in photo-catalytic activity are only marginal in most of the cases. (iii) The exact chemical nature/state of the introduced nitrogen, and its location in titania lattice, substitutional and/or interstitial, is still unclear (iv) Is there a limit to the incorporation of nitrogen in the lattice of TiO₂?

1. Introduction

In titanium-dioxide-promoted photocatalysis or photoelectrochemical applications, the primary objective appears to be “how to make this system respond to visible radiation?” This aspect can be generally termed as sensitization of the semiconductor either intrinsically (conventionally termed as doping even though this may not be the correct connotation when the dopant concentration exceeds a certain limit) or by using visible light absorbing materials (usually dyes or some complex species) [1]. These studies have given rise to many spin offs like understanding of the defect chemistry of the materials, new synthesis strategies for generating these useful semiconducting oxides, and above all the understanding of the physics of the alternate energy levels that are induced by the incorporation of dopants in the original semiconductor. It should be remarked that the efforts to push the photoactive range of these materials to visible region (so that solar spectrum could be effectively utilized) have been the prime motive. It is therefore natural that a variety of synthesis methods for incorporation of nitrogen in TiO₂ have been reported in literature [2, 3].

2. Role of Heteroatoms in Titania

In recent times, there are many reports dealing with heteroatom, (typically, S, C, F, P, B, etc.) substituted (doped or implanted) materials examined as catalysts. The driving force for these studies is the possibility of generating extra allowed energy levels in the wide band gap (e.g., TiO₂) of the semiconductors. These additional allowed energy levels in the band gap of the semiconductor will not only promote absorption of visible light photons but also bring in alternate pathways for the electron-hole recombination, thus altering their life times which are essential for an effective photocatalyst. Such electronic structure alterations could be induced by these heteroatoms. Though the analysis of such effects may be interesting, this aspect is not considered in this presentation. The scope of this presentation is therefore restricted to considering incorporation of nitrogen in TiO₂ especially from the points of view of:

(i)what is the exact chemical nature of the substituted and interstitial nitrogen?(ii)what is the net effect observed in shifting the absorption edge of the semiconductor, and if it does, is there any relationship with the extent of substitution?(iii)the net changes that have been observed in the photocatalytic activity of substituted systems(iv)are there any qualitative correlations that can be derived from these observations?

The reason for this self-imposed restriction is that there is considerable literature already available on these systems. In the last five years alone, a simple search with “Nitrogen doped TiO₂” search term in Web of Knowledge returned 940 articles with 93 proceedings and 25 reviews published. Publications, year wise, indicate continued interest in the topic, with 123 in 2007, 146 in 2008, 138 in 2009, 174 in 2010, and 153 in 2011. Proper evaluation of these systems may provide some directions on catalysis promoted by these systems, especially for important reactions like the photo-catalytic decomposition of water or the photo-catalytic reduction of carbon dioxide. However, most of the investigations pertain to applications for degradation of organic pollutants in aqueous streams, model compounds therein, and typical dye chemicals.

3. Status on Nitrogen-Incorporated Titania

The doped nitrogen assuming substituting anionic positions in (this is already an assumption!) titanium dioxide has attracted attention due to its possible photo-catalytic activity in the visible region [4]. Even though the visible light response of anion doped TiO₂ has been reported as early as 1986 by Sato [5], the recent work by Asahi et al. [6] have reopened the interest in this system. In the recent past, few innovative preparation methods have been evolved in literature for N, S, P, F, and B doped TiO₂ catalysts [7–10]. Simultaneously, there are also attempts to rationalize the observed results from theoretical calculations on this system [11–18]. The complexities involved in N-doped titania, especially with respect to the type of N species, their effects on visible light absorption, and the moderate influence on photocatalytic activity have been covered by Emeline et al. [19]. The current review addresses some of the issues that have emerged from the earlier presentation.

Besides, it is also observed that the state of N in titania and its effectiveness in extending the light absorption edge depend upon the way it is introduced through several preparation methods/techniques. Since this presentation mainly deals with nitrogen introduction in TiO₂, it is appropriate to list the typical preparation methods employed in literature, for incorporation of nitrogen in titania and look for possible correlations between nature of N introduced and preparation methods.

4. Preparation Methods for Incorporation of Nitrogen in

A number of preparative procedures have been adopted for introduction of nitrogen in TiO₂ lattice, which are briefly considered below.

(1)Synthesis from solution phase (sol gel method): [20, 21] Titanium isopropoxide (Ti(OPr)₄) was dissolved in ethanol with dodecylamine and refluxed to get a clear solution. After cooling the solution is neutralized with acetic acid followed by hydrolysis by water. This method has also been followed for multilayer formation of porous TiO₂ by dip coating method and then treated with nitrogen source. The preformed TiO₂ films were usually annealed in the presence of nitrogen precursors (e.g., NH₃) [22].(2)Reaction with ammonia or other N-containing organic substrates like urea, guanidine hydrochloride, or guanidine carbonate: [23, 24]. A dried commercial TiO₂ powder was treated in a flow of dry air or inert gas mixtures containing nearly 50% ammonia or other nitrogen containing substrates and, the sample is heated to 500–700°C. (3)Preparation by plasma treatment [25]: the solid is fixed to a quartz disk and placed in a plasma chamber with heating (400°C). Purified nitrogen was metered and introduced into the chamber, and the plasma treatment was carried out for a definite time period (of the order of 10 minutes).(4)Oxidation of TiN [26–29]: thin film of TiNx was deposited using DC magnetron sputtering (PVD) and then the film was oxidized. Instead, TiO₂ is first sputtered and then annealed in nitrogen. If suitable chemicals are chosen then TiO₂ was coated on a substrate and it is then treated with suitable nitrogen source like ammonia.(5)Electrochemical anodization [30] of titanium foils with suitable nitrogen source has also shown to be a method for controlled incorporation.(6)Low ion implantation method [31] has also been used to introduce nitrogen in TiO₂ single crystals.

It is not clear as to which of the methods give substituted N and which other methods result in interstitial N. According to one report [32], plasma-enhanced chemical vapor deposition yields substitutional nitrogen, while sol-gel method, annealing in NH₃ and chemical methods in general produced predominantly interstitial nitrogen.

None of the methods mentioned above could, however, give clear clues regarding the state of substituted nitrogen. This has to be elucidated by other structural techniques. In most of these studies the amount of nitrogen incorporated is small and hence the X-ray patterns for doped samples resembled that of pure titanium dioxide, and no clear cut changes in the structure could be discerned.

5. The Chemical Nature of Substituted Nitrogen in

The primary motive for nitrogen substitution in TiO₂ is to increase the visible light absorption by the semiconductor [33, 34]. In this sense, the reduction in band gap value with attendant increase in photo-catalytic activity has been reported [4–6, 10, 35–38]. This could have arisen due to either mixing of the nitrogen p states with oxygen 2p states on the top of the valence band or by the creation of N-induced mid gap levels as proposed by Asahi et al. [6] (Figure 1). Though these are the generally stated conceptual alterations in the energy states of the doped semiconductor, it is necessary to see the extent of validity of these postulates. However, it must be realized that the possibility of nitrogen substitution in TiO₂ provides opportunities for other applications hitherto not examined, namely, oxidation of CO, ethanol, acetaldehyde, and NO removal at room temperature [6, 39, 40]. These newer possibilities may have some far reaching implications.

Figure 1: Schematic energy level diagram for nitrogen substituted TiO₂ [Bare semiconductor absorbs UV radiation while the localized energy levels of nitrogen above valence band facilitate the visible light absorption].

There seems to be no consensus among the reports on the state of doped nitrogen in N–TiO₂ even though it is considered to be in the anionic form [4, 6, 41]. XPS analyses of N–TiO2 show that the N 1s core level binding energy lies between 396 and 397 eV, and it has been claimed that the state of nitrogen to be either nitrogen anion [41] or atomic nitrogen atoms [6, 40]. Additional N 1s peaks on N–TiO2 observed at binding energies 400 and 402 eV have been attributed to chemisorbed molecular dinitrogen or adsorbed organic compounds [6, 42]. Sakthivel and Kisch [43] observed no anionic-like nitrogen species with binding energy around 396 eV but only observed nitrogen 1s peak at around 404 eV which has been assigned to hyponitrite type nitrogen species. Valentin et al. [35–37] recognized this controversy in the assignment of N 1s peak position. They observed N 1s core level at 400 eV and hinted at a lower valence state for N. Recently Chen and Burda [44] observed N 1s level at 401.3 eV from a detailed XPS investigations of nano-TiO₂ and suggested that there is N–Ti–O bond formation due to nitrogen doping and no oxidized nitrogen is present. Sathish et al. [45] have examined this system and attributed the observed N-1s-binding energy at 398.2 eV to be due to N–Ti–O type species present in the system. The observations of N-1s-binding energy >400 eV may be attributed to the possible O–N–Ti linkages or some surface oxidation. In a subsequent paper [46] the same authors have tried to substantiate the presence of different types of N species like Ti–N and O–Ti–N in N–TiO₂ system. It is clear that the XPS results reported on this system require a better understanding.

In order to comprehend the situation, especially the bonding of substituted nitrogen in TiO₂, it is necessary that one attempts to summarize the different results reported in literature on XPS studies. This technique probes the core level binding energies of the constituent species, and the value of the binding energy is a reflection of the valence state and charge density around each of the atoms. Since the objective of this presentation is to get clarity on the nature of the nitrogen species, the data on the binding energy of the 1s level of nitrogen in substituted TiO₂ are summarized in Table 1.

Table 1: Nitrogen-1s-binding energies in nitrogen substituted TiO₂.

S. No
Nitrogen-1s-binding energy in N-TiO₂ in eV
Assigned to species like
Reference

1
~397
T–N bonding IBAD
[12]

2
396, 400
Ti–N bond chemisorbed dinitrogen
[13]

3
396.2, 398.3, 400.4
Chemically bound, O–Ti–N, chemisorbed N₂
[47]

4
396.7, 398.5
N–Ti bonding; symmetric to asymmetric with % N₂
[15]

5
398.6, 401
N substituted for oxide, Ti–N–O, incorporated nitrogen
[48]

6
395.4, 400.5
Ti–O–N unreacted NH₃, adsorbed nitrogen
[49]

7
396, 400
Ti–N, adventitious N₂
[14]

8
396.5, 402
B–N (bonded to Ti) and molecular N₂
[50]

9
397.4 −403.7, 401.3, 396
O–Ti–N, chemically bound N
[44]

10
396, 400, 402
N⁻ species, chemisorbed N₂
[6]

11
396
Chemically bound N⁻
[51]

12
397
Ti–N concentration dependent
[52]

13
396, 400
O–Ti–N, (Ti)

14
398.2
Covalency of Ti–N bond, anionic N, N–Ti–O
[45]

15
396
β-N
[39]

16
396.7, 399.6
Bulk N in two states nitride species N₂-anions NHx species chemically bound to H
[41]

17
398.7, 400.1
C–N bonds, hyponitrite, O–Ti–N, C–Ti–O, Ti–O–N–C
[53]

18
396, 399.9
N⁻ substituted, chemisorbed N₂
[30]

19
396.8
β-N, substitution
[54]

20
397, 400, 403
Ti–N, chemisorbed N₂
[55]

21
396.2, 400.2
β-N and γ-N
[56]

22
396, 400
Incorporated, trapped N₂
[27]

23
395.6, 399.6
in TiN, Ti–N–O, Ti–O–N
[11]

24
396, 400
O–Ti–N
[57]

25
396, 398.8, 400.5
Substitution, molecular N₂
[20]

26
397–402
Substituted nitrogen
[23]

27
397.4, 400.3, 402.5
Ti–N–Ti, Ti–O–N–O/Ti–O–N–N
[58]

28
395.8, 400
β-N, N–O, N–C, N–N
[26]

29
396, 400
β-N, molecular N₂
[4]

30
396, 400, 402
β-N, others not assigned
[29]

31
396.1, 402
N–Ti–O, γ-N₂
[59]

32
396, 400
β-N, N–O, N–C, N–N
[24]

33
396, 399.5
β-N, chemisorbed N₂, interstitial O–N–Ti
[28]

34
396.2, 398.4, 400, 401.5
β-N, chemisorbed nitrogen
[46]

35
396, 400, 402
β-N (396 eV) and molecularly chemisorbed γ-N₂ (400 and 402 eV)
[6]

36
399.6, 396
Interstitial nitrogen and substituted nitrogen
[60]

37
400.5
No substitution nitrogen
[61]

38
399
Both substitution and interstitial nitrogen
[62]

39
399.6
Interstitial nitrogen doping at low levels and nitrogen doping at higher levels; the limit for this transition is 1.2 at%.
[63]

40
400
O–Ti–N bonding
[64]

41
399.2, 400.5
C=N–C, N–Csp2, –C=N
[65]

42
400, 402
Chemisorbed nitrogen
[25]

43
399.5
Valence state of nitrogen between −2 and −3
[66]

44
402, 399.5
Chemisorbed molecular nitrogen, interstitial nitrogen
[67]

The data presented in Table 1 give rise to a number of points, which are listed as follows.

It appears that there is some consensus on the state of nitrogen in substituted systems as Ti–N with nitrogen substituting for the anion. However, there is no definite information on the valence state of this substituted species. It has been assumed in some cases as N⁻ anion and in some of the other reports the valence state is not exactly mentioned except stating that there is Ti–N bonding. This can give rise to the following contemplations.

(a)If N⁻ is the species then the valence state of Ti has to be different from Ti⁴⁺, which has been recognized in some of the reports, but they have not exactly accounted for the valence state of Ti so that electro-neutrality is maintained.(b)It has been tacitly assumed that the N-1s-binding energy is around ~396-397 eV, and this peak is mostly present when the nitrogen content in substituted systems is very small. It is generally observed that with increasing nitrogen content the higher binding energy (~400 eV) peak appears which is normally considered to be due to chemisorbed molecular species or interstitial N or due to the nitrogen of the precursor species employed for N substitution in TiO₂.(c)The acceptable binding energy value of N 1s level in substituted systems is around 396-397 eV. If this were to be the 1s binding energy of the nitrogen species then the species cannot be either in positive or multiple negative valence states. If nitrogen were to assume anionic states (as is generally believed) then nitrogen-1s-binding energy should be around 394 eV. This ionic state can also be expected on the basis of electronegativity difference between that of titanium and nitrogen. If it were to be in cationic state, it should be around 400 eV which is less likely on the basis of size and charge. If on the other hand the Ti–N bond were to assume covalent character, the observed nitrogen-1s-binding energy can vary with extent of loading and possibly account for the variations in the binding energy values reported in literature. The literature is unfortunately silent on this aspect for some unknown reasons.(d)Another important aspect is that the type of species envisaged, namely, either Ti–N or Ti–O–N, could have been present mostly on the surface as they have been detected only in XPS measurements with no indications in the X-ray diffraction patterns, which are nearly the same as the starting TiO₂. This means that the surface layers have a non-native configuration as compared to the native configuration that is present in the bulk of the material. If this were to be true, then the reactivity (or even the photocatalytic consequences reported) of the surface should be different from what is generally observed on bare . Though this has been observed in many publications, they have not been assigned to the changes observed due to the nonnative configurations that may be present on the surfaces of substituted systems [68].(e)Even though there are reports on the changes in the intensity of the emission due to N 1s level in the substitution state (namely, around 396-397 eV), it is not clear from the available literature to what percentage the nitrogen substitution in anionic position will take place and when the signal due to molecularly chemisorbed nitrogen species starts to appear. The changes observed or expected in the optical spectrum are critically dependent on this parameter.(f)Observation of two XPS peaks at 396–398 eV and 400–402 eV possibly indicates the presence of substitutional as well as interstitial nitrogen, respectively, in titania lattice though the exact chemical nature is not clear.(g)Nitrogen incorporation in titanium dioxide has thus been claimed through a number of preparation methods [65, 69]. It is generally presumed that the visible light photo activity of the resultant material is due to incorporation of nitrogen in the lattice. An alternate postulate is that nitrogen precursors could give rise to light active molecular species on the surface (dye like) which function as sensitizers for the observed visible light photo-activity [70–73]. However, this concept cannot account wherein molecular nitrogen or other molecules, which on decomposition yield molecular nitrogen, are employed for the preparation of nitrogen substituted TiO₂.

The data presented in Table 1 show that the nitrogen incorporated in TiO₂ is mostly in the substitution position for the anion conventionally designated as β-N species. Several investigations have reported peaks at 400–402 eV indicating presence of interstitial nitrogen as well. However, there is no clear cut statement on the valence state of the nitrogen. Is it a trivalent anion? Or at least an anion with negative charge on substituted nitrogen? The N substituted systems on further incorporation of nitrogen gives rise to molecularly chemisorbed species. This observation leads one to make an estimate of the possible extent of substitution in TiO₂. In any of the studies reported, this aspect has not been clearly stated. This could be deduced by the shift of the band gap value as a function of the extent of nitrogen substitution. A rough estimate of the data available in literature shows that the substituted nitrogen cannot exceed 10%. However, it is necessary to examine the band structure alterations that can take place by the substitution of anions in titanium dioxide by nitrogen anion.

6. N Substitution Theoretical Approaches

A few theoretical studies have been reported on this aspect on the basis of the calculation of the density of states (DOS). The salient points that emerge out of these theoretical studies are [12–15, 17, 18]

(1)the nitrogen 2p states give rise to allowed energy states just above the valence band of the semiconductor (Figure 1).(2)the 3d states of the metal provide allowed energy levels near the conduction band.(3)the transition from the allowed 2p states of nitrogen to the conduction band accounts for the visible light activity of these doped systems.(4)Asahi et al. [6] believe that the Nitrogen 2p and oxygen 2p states hybridize and thus account for the band gap narrowing. This statement has been substantiated by the calculations of Sakai et al. [13] and that of Li et al. [12] Shang et al. [14], and Sathish et al. [18]. The model calculations have been made on a typical cluster [Ti₅O₁₄H₈] (Figure 2).

Figure 2: Model of the cluster (Ti₅O₁₄H₈) [the position of the replaced oxygen is shown by an arrow].

The position of the substituted nitrogen in the place of oxygen atom is shown by arrow. This corresponds to an anionic position in the TiO₂ lattice. The density of states (DOS) calculation has shown the reduction in the band gap which is attributed to the orbital mixing of the hetero atom with oxygen 2p and Ti 3d states as stated earlier. It is presumed that the energetic considerations show that the nitrogen 2p states can mix with both the 2p state of oxide ions and also the 3d state of the titanium ions thus accounting for the reduction in the band gap with the possibility of visible light active nature of N-doped TiO₂. It has been shown that both the top of the valence band and the bottom of the conduction band are broadened due to nitrogen doping in TiO₂.

The points of relevance are

(i)does nitrogen doping in TiO₂ directly reduces the value of the band gap of TiO₂?(ii)does the substitution of nitrogen give rise to allowed energy states in the band gap of the semiconductor thus accounting for the visible light response of the doped semiconductor?(iii)how does the substitutional/interstitial nitrogen influence the activity?

These issues have not yet been resolved.

7. The Nature of Titanium Species in N-Substituted

Having seen that the exact chemical nature of nitrogen in N-substituted TiO₂ is subject to controversy, it is natural to expect some changes in the 2p3/2 binding energy of Ti. This is required since nitrogen can either take up the position of the oxide ions or can also replace the cations. In addition, since the difference in the values of the electronegativity of nitrogen and titanium is 1.5 as against the value of 1.9 for Ti and oxygen, one can expect even if nitrogen were to take up the anionic position, the bonding may involve in some covalent character and hence the 2p3/2-binding energy of titanium can be different from what is observed for Ti⁴⁺.

The reported XPS results on the binding energy of Ti 2p3/2 in nitrogen-substituted TiO₂ are given in Table 2.

Table 2: 2p3/2 binding energy values for Ti in N-substituted TiO₂.

S. No
Binding energy of 2p3/2 level of Ti In N–TiO₂ (in eV)
Assigned as
Reference

1
458
Ti in 4+ oxidation state
[27]

2
459.3, 458.5
Electronic interaction is different, covalency
[45]

3
<459.1
Substitution of N Multiple oxidation states +3+2
[52]

4
+0.9 and +2.1 with respect TiO₂
Intrinsic defects implanted nitrogen
[31]

5
458
Same as in TiO₂
[27]

6
458.6, 456.2
Ti in +3 and +4 states
[59]

7
458.2
Shifted to lower value, electron density increases, covalency
[26, 53]

8
459.2, 456.1
Decrease by 05–02 eV with respect to TiO₂, N–Ti–N or O–Ti–N, N–Ti–N, O–Ti–N
[58]

9
458.1, 463.8
Ti–N bonds shifts to lower values
[23]

10
457.5
Ti–N
[20]

Though most of the studies on the N-substituted TiO₂ systems have clearly dealt with the XPS of N 1s level, they are not making any significant comment of the corresponding features of the Ti 2p XP spectra. This study could have given some information on the state of nitrogen in the substituted systems. If nitrogen incorporation were to take place similar to TiN-like species then Ti could have been present in +3 oxidation state and the covalency of the bond could have increased, and it could have resulted in the decrease in the binding energy of 2p3/2 level of Ti present in N–TiO2. However, most of the studies have not reported explicitly this observation and also in some of the studies, they have not observed the shift to lower binding energy values with respect to what is observed in TiO₂, which possibly implies that nitrogen is not either substituted for oxygen or the species generated are not like TiN.

8. Nitrogen in Interstitial Sites in Titania

According to Asahi et al. [6] only substitutional type of N doping is possible. This leads to mixing of the 2p states of oxygen from titania with the 2p states of N and results in intra band states which in turn can effectively narrow down the band gap, thereby facilitating visible light. Interstitial type N doping was found to be ineffective.

In contrast, Valentin et al. [35–37] propose that incorporation of nitrogen in substitutional state is more effective in the formation of localized levels within the band gap and conclude that both substitutional and interstitial nitrogen may exist with energy levels as shown in (Figure 1) and depending on the preparation (oxygen partial pressure) conditions. According to Valentin et al. [35–37], substitutional nitrogen states lie just above valence band, by 0.14 eV, and interstitial nitrogen states lie higher in the gap at 0.73 eV. Two N1s XPS peaks, one observed at 396 eV (substitutional) and the other at 400 eV (interstitial) nitrogen species lend credence to this theory. It is also known that nitrogen can substitute the Ti site in TiO₂.

Hence, at present, it is not clear in what state nitrogen is introduced in TiO₂. No correlations exist between the method adopted for N incorporation and the type of N in the lattice, substitutional, or interstitial. In the absence of clear understanding of the state of nitrogen introduced in titanium dioxide, it is difficult to interpret the photo-catalytic activity observed with these systems since the creation of new adsorption centers could also be one of the reasons for the observed photo-catalytic effect even though the photon absorption range could have shifted to visible range.

9. Photo-Catalytic Studies on Nitrogen-Introduced

It is known that the primary reason for substitution of nitrogen in TIO₂ is to extend the photon absorption range to visible region. Even though, this expectation is mostly fulfilled, as substantiated from the optical response of a typical system reproduced in Figure 3, its effects on photocatalytic activity are yet to be realized in expected terms.

Figure 3: UV-vis reflectance spectra of (a) TiO₂, (b) P-25, (c) undoped hollow TiO₂ sphere, and (d) N-doped hollow TiO₂ sphere [74].

Cho et al. [74] have studied the photo-catalytic activity of nitrogen-doped TiO₂ hollow nanospheres and concluded that the activity under visible light was superior to that of pure TiO₂ or Degussa P-25.

A compilation of the photocatalytic activity studies on N-doped titania is presented in Table 3.

Table 3: Typical photocatalytic studies reported on N-substituted TiO₂.

S. No
Photo-catalytic studies on N–TiO₂
Reference

1
Photo-activity using stearic acid, no visible-light-induced activity
[27]

2
Photo degradation of Phenol N–TiO₂, anatase is higher
[55]

3
Degradation of methylene blue, no specific trend with respect to nitrogen substitution
[30, 39, 45, 46]

4
Photo-degradation of methyl orange
[48, 53, 58]

5
Photodecomposition of isopropyl alcohol
[52, 75]

6
Photo-electrochemical decomposition of water
[52]

7
Degradation of ethylene glycol
[76]

8
Decomposition of 2-chlorophenol
[14, 23]

9
Decomposition of VOC and Rhodamine B
[29]

10
Decomposition of acetaldehyde
[6]

It is surprising to note that the photo-catalytic activity of N–TiO2 has been restricted to the same type of reactions (namely decomposition of organic substrates), and considerable increase in the reactivity is not observed for visible light irradiation. This casts doubt on the attempts that are made for shifting the absorption to visible range by sensitizing the semiconductor with the hope that more of the solar radiation can be utilized. This postulate is not established till now. It appears that one has to re-examine the methodology for the selection of materials for photo/photo-electrochemical decomposition of water where one is searching for a semiconductor which can be photo active in the visible range.

Photo-catalytic decomposition of volatile organic compounds and decontamination of water, though, may be relevant from environmental control point of view the photo-catalytic decomposition of water for the production of fuel (namely, hydrogen) may be of greater relevance and importance. The studies so far reported in literature on nitrogen-doped TiO₂ have not shown considerable enhancement of the decomposition of water by increasing absorption in the visible range. Besides Kitano et al. [77] observed that N-doped titania film after photo electrolysis of water under visible irradiation showed a decrease in N concentration at surface layer indicating that the surface was oxidized during electrolysis. Such stability issues [77, 78] with N-doped titania usage need to be addressed and improved.

10. Conclusions

(1)It is not clear from the results reported in literature that nitrogen introduction in TiO₂ lattice can promote the phase transformation from anatase to rutile. It is known that anatase to rutile phase transformation is either inhibited or promoted by the addition of substances like K₂O, P₂O₅, Li₂O and carbon in the former three cases the transformation was inhibited while in the case of carbon it is accelerated [79–81]. However, the available reported literature is not clear if introduction of nitrogen in TiO₂ lattice can alter or promote the phase transformation from anatase to rutile. This can be considered as an indirect evidence for nitrogen not incorporated in the lattice.(2)Interrelationships between the methods adopted for N introduction and chemical nature and location of N in TiO₂ lattice are yet to be understood.(3)Maximum/optimum doping of N that could be achieved, and its effect on photoactivity is another aspect that needs further study. (4)If the X-ray diffraction patterns for N-doped TiO₂ remain the same as that of pure TiO₂, then the effect of N introduction should have been minimal and hence the surface configuration could be different from that of the bulk native structure. If this architecture is possible, then optical absorption changes observed could have arisen out of the surface layers and hence only the adsorptive properties could have altered, accounting for the increased photo-catalytic oxidation of organic substrates.(5)Stability of the N-doped titanium dioxide under irradiation during photo-electrolysis of water [78] is a challenge to be addressed.

Acknowledgments

Grateful thanks are due to Department of Science and Technology, Government of India for the generous support of the National Centre for Catalysis Research, at IIT Madras. The authors also wish to thank one of the reviewers for his remarks for the improvement of the paper.

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