Xiaoyun Yanga,
Sina Hea,
Yijin Shua,
Zhangping Shib,
Yulin Guoa,
Qingsheng Gao*a and
Yi Tangb
aDepartment of Chemistry, Jinan University, 510632, Guangzhou, China. E-mail: tqsgao@jnu.edu.cn
bDepartment of Chemistry, Shanghai Key Laboratory of Molecular Catalysis and Innovative Materials, Laboratory of Advanced Materials and Collaborative Innovation Center of Chemistry for Energy Materials, Fudan University, 200433, Shanghai, China
First published on 14th October 2015
The electron regulation on supports can vary metal-support interactions with loaded metals in heterogeneous catalysis. In this paper, a facile Sr2+-mediated ionothermal route was introduced to control the nitridation degree in tantalum (oxy)nitrides, resulting in varied electronic properties and optimized interactions with gold nanocatalysts. A new mechanism was proposed that the formation of SrTa4O11 intermediates facilitated the replacement of O by N in controlled nitridation, and more importantly avoided undesired over-nitridation. As expected, the TaON support with defined nitridation promoted electronic metal-support interactions to generate Auδ− species, which was highly active for the thermal hydrogenation of nitrobenzene due to the moderated adsorption and effective activation on Auδ− in Au/TaON. This work elucidated the optimized metal-support interactions achieved on controllably nitridated supports, opening up new opportunities for the development of efficient nanocatalysts.
Introducing N into metal oxides usually brings narrowed band-gap and increased Fermi level as a result of the synergetic effects of both alloying and electron-transfer,16,17 which indicates a facile electron-manipulation by controlled nitridation. In the case of tantalum (oxy)nitrides, the smaller band-gap energy (vs. Ta2O5) enables them as novel visible-light photocatalysts,17,18 and the rich defect and tunable valence state are further proved promising for nonphotocatalytic hydrogenation and oxidation.19–21 It's more important that tantalum (oxy)nitrides can be utilized as promising catalyst supports. Their increased Fermi level and tunable electron features would promote the electronic interactions with metals, showing advantages in comparison with Ta-oxides.22–24 To achieve the optimized metal-support interactions in efficient catalysis, the controlled nitridation in tantalum (oxy)nitrides is highly demanded, however, it suffers easy over-nitridation to by-products of Ta3N5, Ta4N5, and even TaN during high-temperature synthesis.25,26
Nitridation utilizing organic–inorganic hybrid precursors provides the tailored generation of nitrides.8,27 Herein, a facile Sr2+-mediated route is conducted to accomplish the controlled nitridation in tantalum (oxy)nitride nanoparticles, which are mono-dispersed, well-separated and mostly single crystalline. A new mechanism via tantalate intermediate is proposed for the controlled nitridation. The formation of SrTa4O11, in which Ta–O bonds are weakened by Sr2+, ensures the generation of pure TaON or Ta3N5 at mild temperature, and avoids over-reactions. This innovation can be extended to other ionothermal system utilizing a wide range of alkaline-earth-metal salts, and can well address the remaining puzzlements in the previous work. For example, the previous Ca2+-assisted mechanism associated with the controlled NH3-release from Ca2+-chelated urea is controversial,28 because urea decomposes much earlier than nitridation reactions upon heating. The new mechanism via tantalate intermediates makes an obvious progress in the understanding of essential effects of ionic solvents. More importantly, it is discovered for the first time that such controlled nitridation obviously varies the electronic properties of tantalum (oxy)nitrides to express electronic metal-support interactions with gold for catalytic hydrogenation. In the probe reaction of nitrobenzene (NB) reduction under thermal condition, remarkably improved activity and optimized aniline (AN) selectivity are achieved over Au/TaON, as compared with those on Au/Ta2O5 and Au/Ta3N5. This is ascribed to the suitable adsorption and effective activation of substrates by moderately negative Auδ− on TaON support.
Meanwhile, Ta2O5 nanoparticles used for control catalytic tests were synthesized via traditional reverse homogeneous precipitation. 0.360 g of TaCl5 was dissolved in 5 mL of methanol, and then, 15 mL of NH3·H2O (19%, aq.) was added. After stirring for 1 hour, the white precipitate was washed with water and ethanol. After heating at 750 °C for 5 h under air, Ta2O5 nanoparticles were received.
A typical deposition–precipitation procedure was employed to prepare Au/Ta2O5, Au/TaON, and Au/Ta3N5 catalysts. Briefly, Ta-based nanoparticles were dispersed with the aqueous solution of HAuCl4 (4.856 × 10−3 mol L−1), and pH was adjusted to 9.0 by dropwise addition of 0.25 M NH3·H2O (aq.). After stirring for 6 hours and aging for another 2 hours, the catalyst was washed with deionized water for five times and then dried at 50 °C overnight, followed by a careful reduction with a stream of 5 vol% H2/Ar at 300 °C for 2 hours.
Furthermore, the SEM investigation shows that all the products are in form of well-defined nanoparticles (Fig. S2 in ESI†). Representatively, Fig. 2a and b display the SEM images of TaON and Ta3N5, which are obtained with a typical RU/Ta of 2.0 and 7.0, respectively. They are about 20–30 nm in diameter. In the TEM images (Fig. 2c and d), TaON can be distinguished by the clear (110) and (200) lattice fringes, while Ta3N5 is confirmed by the (110) and (402). The EDS obtained on the both of above nanoparticles confirm the complete removal of SrCl2 by a treatment with 1 M HCl (Fig. S3 in ESI†). Additionally, such TaON and Ta3N5 exhibit a surface area of 21.3 and 25.6 m2 g−1, respectively (Table S1 in ESI†).
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Fig. 2 (a and b) SEM and (c and d) TEM images of (a and c) TaON and (b and d) Ta3N5 NPs, harvested at RU/Ta = 2.0 and 7.0, respectively. |
XPS analysis further gives clear evidence about TaON and Ta3N5 with varied electronic structures (Fig. 3). With the introduction of N, TaON presents the obviously shifted peaks of Ta 4f7/2 and 4f5/2 at the lower binding energies of 26.0 and 27.7 eV, respectively, as compared with those located at 26.9 and 28.7 eV in Ta2O5.29 This is associated with the lower electronegativity of N than that of O, as well as the consequently favored electron transfer from N to Ta. In this way, Ta3N5 displays the further decreased binding energy of 25.1 and 26.9 eV for Ta 4f7/2 and 4f5/2, respectively. Meanwhile, the red-shifted absorption bands of TaON and Ta3N5 nanoparticles in UV/vis DRS (Fig. S4a in ESI†), in comparison with those for Ta2O5, indicate the narrowed band-gap due to nitridation. According to previous reports,29 the valence band in tantalum (oxy)nitrides, mainly contributed by O 2p and N 2p orbitals, ascends from −7.93 eV in Ta2O5, to −6.6 eV in TaON and −6.02 eV in Ta3N5, bringing about obviously increased Fermi level with the increased nitridation degree (Fig. S4b in ESI†).
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Fig. 4 XRD patterns of products obtained in the absence of Sr2+ with the varied RU/Ta ratio from 1.0 to 8.0. |
As the ionothermal processes were conducted at lower temperature (550 °C) or with a lower flow rate of carrier N2 (100 mL min−1) than that for a typical procedure (700 °C and 500 mL min−1), in which nitridation reactions were depressed,31 the intermediate of SrTa4O11 (ICDD no. 01-083-0608) was received (Fig. S5 in ESI†). This observation indicates the strong interactions between Sr and Ta in the form of strontium tantalate during ionothermal synthesis. According to the crystalline data of SrTa4O11 and Ta2O5 (Fig. S6 in ESI†), some weakened Ta–O bonds in SrTa4O11 are suggested by the extended length in a wider range (1.839–2.478 Å) than that in Ta2O5 (1.839–2.126 Å). This predicts the easier breaking of Ta–O in strontum tantalate under nitridation, and the promoted replacement of O atoms by N, as verified by the following thermal analysis.
The TGA/DSC analysis under N2 atmosphere was conducted on the similar gel precursors with and without Sr2+, which were denoted as SrTa/U and Ta/U, respectively (Fig. S7 in ESI†). The same RU/Ta of 2.0 was adopted. To elucidate the nitridation reactions, we focus on the evolution in TGA/DSC over 500 °C (Fig. 5a). Noticeably, the nitrogen source at such high temperature is CNx derived from urea,20,32 whose presence has been verified by IR spectra (Fig. S8 in ESI†). The SrTa/U precursor shows a weight loss and an endothermic peak around 626 °C, and another evolution near 765 °C. The samples taken from TGA/DSC at 650 and 800 °C respectively exhibit the typical absorption band-edges of TaON (490 nm) and Ta3N5 (600 nm) in UV-vis DRS (Fig. 5b). It is indicated that the reactions around 626 °C in TGA/DSC would be associated with the nitridation to TaON, at which point the further reaction to Ta3N5 requiring higher temperature of 765 °C is avoided. However, Ta/U without Sr2+ only presents a drastic weight loss and an obvious endothermic peak around 742 °C, consistent with the synthetic procedure requiring calcination at 775 °C (Fig. S9 in ESI†). And the sample taken from TGA/DSC at 800 °C displays an intensive absorption from 600 nm in UV-vis DRS (Fig. 5b), corresponding with the uncontrolled nitridation to TaON and Ta3N5 mixtures (Fig. 4). Similar situation is also observed in the case with a RU/Ta of 7.0 (Fig. S8 in ESI†). SrTa/U (RU/Ta = 7.0) obviously displays the accelerated nitridation at lower temperature than that of Ta/U due to the mediation of SrTa4O11. This effectively restricts the over-nitridation to TaN that is usually observed in the absence of Sr2+ (Fig. 4).
Based on the above results, we propose a new mechanism associated with crucial strontium-tantalate intermediates for controlled nitridation (Scheme 1). In the intermediate of SrTa4O11, parts of Ta–O bonds are weakened. This benefits the replacement of O by N for generating TaON with a low RU/Ta, and more importantly avoids over-nitridation to Ta3N5 because the residual Ta–O bonds are not affected by Sr2+. In the case with a high RU/Ta, the promoted nitridation at T < 700 °C also prevents products from over-reacting to TaN. Thus, the controlled nitridation is successfully achieved. In this way, the Sr/Ta ratio controlling the intermediates of tantalates makes obvious influence the generation of TaON and Ta3N5 (Fig. S10 in ESI†).
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Scheme 1 Proposed mechanism via a vital strontium-tantalate intermediate for controlled nitridation. |
This mechanism is universal for ionothermal processes using other alkaline-earth metal ions. In the presence of Ba2+, TaON and Ta3N5 phases are obtained as RU/Ta = 2.0 and 5.0, respectively (Fig. S11 in ESI†). Similar pure Ta3N5 is fabricated at RU/Ta = 5.0 with Ca2+ or Mg2+, however, the intermediates of Ca2Ta2O7 and MgTa2O6 still remain at the low RU/Ta of 1.0–3.0 (Fig. S12 and S13 in ESI†), whose decomposition usually requires complete nitridation with high temperature (>775 °C) and flow rate (>1.0 L min−1).28 Such difference is probably related to their diverse ionic radius (Mg2+ 89 pm; Ca2+ 112 pm; Sr2+ 126 pm; Ba2+ 142 pm).33 Owing to the toxicity of Ba2+ and the difficult decomposition of Ca2+ and Mg2+-based tantalates, the Sr2+-mediated route is suitable for the environment-friendly and facile synthesis of nitrides.
We believe that this explanation would make a progress in discovering the essential effects of ionic solvents. Ionothermal routes were ever conducted to fabricate ternary metal oxynitrides, e.g., MTaO2N (M = Ca, Sr or Ba), MNbO2N (M = Sr or Ba), however, their functions in controlled nitridation were unfortunately ignored.34 In our previous work,28 the indispensable effect of Ca2+ in the controlled synthesis of TaON and Ta3N5 was ascribed to the chelation between Ca2+ and urea, which slowed down the release of NH3 from urea decomposition to control nitride generation. However, it cannot elucidate how the urea decomposition at low temperature (<400 °C) affects nitridation at high temperature (∼775 °C). Herein, tantalate intermediates are found in the ionothermal routes with a wide range of alkaline-earth-metal salts (e.g., Mg2+, Ca2+, Sr2+ and Ba2+), which are indispensable to achieve the well-defined tantalum (oxy)nitrides. The controlled nitridation due to the weakened Ta–O bonds of tantalates successfully protects the desired generations of TaON and Ta3N5 from over-reactions, opening new mind in the understanding of ionothermal synthesis.
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Fig. 6 TEM images of (a) 0.9% Au/Ta2O5, (c) 0.8% Au/TaON, (e) 0.9% Au/Ta3N5, and the corresponding size distribution of Au on (b) Ta2O5, (d) TaON, (f) Ta3N5. |
H2-TPR and XPS analysis were further conducted on the above catalysts. In H2-TPR results (Fig. 7a), the strong metal-support interactions in Au/TaON and Au/Ta3N5 are suggested by the lower reduction temperature of Au3+ species in comparison with Au/Ta2O5, all of which possess the consistent size-distribution of Au (Fig. 6). Although parallel reductions peaking at 121–122 °C are both detected, the onset temperature of 72 °C in Au/Ta3N5 is lower than that in Au/TaON (97 °C). Such interactions are further affirmed by XPS (Fig. 7b). The sample of Au/Ta2O5 displays the Au 4f7/2 and 4f5/2 peaks located at 87.6 and 83.9 eV, which are coincident with those for metallic gold.36 With the nitridation of Ta-based supports, these peaks are respectively shifted to the lower binding energies of 87.4 and 83.7 eV in Au/TaON, indicating negatively charged Au species (Auδ−). This observation should be attributed to the increased Fermi level in nitridated supports (Fig. S4b in ESI†), which promotes electron transfer from supports to Au.37–39 In Au/Ta3N5, the corresponding ones with an obvious red-shift to 87.1 and 83.4 eV suggest that electrons are further accumulated on Auδ− surface due to the highly nitridated Ta3N5 supports. Such metal-support interactions varied by the nitridation of Ta-based supports are expected to make obvious influence on the catalytic performance of gold.40,41
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Fig. 7 (a) H2-TPR profiles and (b) Au 4f XPS spectra of 0.9% Au/Ta2O5, 0.8% Au/TaON, and 0.9% Au/Ta3N5. |
Entry | Catalyst | Conv. (%) | Sel. (%) | |
---|---|---|---|---|
PHA | AN | |||
a Typical conditions: NB (0.5 mmol), catalysts (40 mg), FA (6.0 mmol), EtOH (5.0 mL), H2O (5.0 mL), N2 (0.5 MPa), 80 °C, 2.5 hours.b H2 (0.5 MPa) was used as the reductant. | ||||
1 | Ta2O5a | 33 | >99 | 0 |
2 | TaONa | 30 | >99 | 0 |
3 | Ta3N5a | 35 | >99 | 0 |
4 | 0.9% Au/Ta2O5a | 52 | 92 | 8 |
5 | 0.8% Au/TaONa | >99 | 49 | 51 |
6 | 0.9% Au/Ta3N5a | 73 | 60 | 40 |
7 | 0.8% Au/SiO2a | 74 | 83 | 17 |
8 | 0.9% Au/Ta2O5b | 52 | >99 | 0 |
9 | 0.8% Au/TaONb | 65 | >99 | 0 |
10 | 0.9% Au/Ta3N5b | 58 | >99 | 0 |
11 | 0.5% Au/TaONa | 39 | 85 | 15 |
12 | 1.3% Au/TaONa | >99 | 29 | 71 |
13 | 1.7% Au/TaONa | >99 | 27 | 73 |
Considering the similar catalytic FA decomposition to CO2 and H2 over Au/Ta2O5, Au/TaON and Au/Ta3N5 (Table S3 in ESI†), the different performance for NB reduction by FA should be contributed by the reduction steps of NB. Further test in the direct hydrogenation of PHA exhibits the negligible difference (Table S4 in ESI†), suggesting the varied activity in the first step from NB to PHA. The intrinsic properties of Au in the above catalysts are believed as a key factor for NB hydrogenation, regarding the similarities in surface area, Au particle size and active-site amount already confirmed by N2 sorption analysis, TEM investigation and CO uptake experiment, respectively (Table S1 in ESI† and Fig. 6).
Typically, the adsorption of NB substrate on Au is the key in NB reduction.44,45 According to the Balandin-type volcano plots, the moderate adsorption on metals is demanded for efficient catalytic conversion because a weak adsorption cannot effectively activate substrates and a strong adsorption precludes product desorption.46,47 Negatively charged Auδ− over TaON resulting from electronic metal-support interactions38,39 (cf. XPS in Fig. 7b) would promote the adsorption of polar –Nδ+–Oδ− bonds in NB,42,46,47 as compared with the neutral Au on Ta2O5, which presents optimized activity and selectivity (Scheme 2). As for Au/Ta3N5, the further negatively charged Auδ− on Ta3N5 would make NB and even as-formed PHA adsorption so strong that the following steps are hindered.46 And thus, the reduced activity and AN selectivity are observed. Obviously, an appropriate nitridation level of supports is critical for optimizing metal-support interactions with gold nanocatalysts.
Another test under light irradiation, showing further affected charge-distribution on Au by photo-excited electrons, can serve as an important evidence for the above conclusion in nonphotocatalytic condition. In view of the different band-gap energy of Ta2O5, TaON and Ta3N5, UV (λ > 200 nm) and visible (λ = 400–800 nm) light was employed for Au/Ta2O5 and the both of Au/TaON and Au/Ta3N5, respectively. The increased activity is observed on Au/Ta2O5, while the decreased one is presented by Au/TaON and Au/Ta3N5, in contrast with that without irradiation (Fig. 8). Thanks to the excited electron from Ta2O5 to Au, the as-formed Auδ− accelerates NB reduction by enhanced adsorption. However, too strong NB and PHA adsorption on excessively charged Auδ−, strengthened by photo-excitation, would block the following reactions and thus reduce the activity on Au/TaON and Au/Ta3N5. Additionally, the test under visible light (λ = 400–800 nm) was also conducted on Au/Ta2O5. The performance similar to that without irradiation, but lower than that with UV, should be ascribed to the failure to excite wide-band-gap Ta2O5 (3.9 eV) by visible light. This test eliminates the influence from the visible-light plasmonic effects of Au.
Footnote |
† Electronic supplementary information (ESI) available: Additional characterization of SEM, TEM, XRD, TGA/DSC, IR, N2 isothermal sorption and CO uptake. See DOI: 10.1039/c5ra19644b |
This journal is © The Royal Society of Chemistry 2015 |