催化学报  2016, Vol. 37 Issue (5): 637-643   PDF (550 KB)    
扩展功能
加入收藏夹
复制引文信息
加入引用管理器
Email Alert
RSS
本文作者相关文章
李会香
张宗超
Far reaching potentials of far infrared spectroscopy in catalysis research
Huixiang Li, Z. Conrad Zhang     
State Key Laboratory of Catalysis, Dalian National Laboratory for Clean Energy, Dalian Institute of Chemical Physics, Chinese Academy of Sciences, Dalian 116023, Liaoning, China
© 2016, Dalian Institute of Chemical Physics, Chinese Academy of Sciences.
Published by Elsevier B.V. All rights reserved.
远红外光谱在催化领域的应用前景
李会香a,b, 张宗超a     
a 中国科学院大连化学物理研究所, 催化基础国家重点实验室, 洁净能源国家实验室(筹), 辽宁大连 116023;
b 中国科学院大学, 北京 100049
摘要:中红外光谱是催化领域的重要技术之一, 已被广泛应用于催化过程的研究, 而远红外光谱 (FIR) 的应用相对而言并不成熟. FIR 可用于分析催化过程中较低能量的振动模式, 如氢键、芳烃骨架振动、重原子间的伸缩振动、气体分子的转动等, 从而可弥补中红外光谱的应用. 在本文中, 我们综述了有关 FIR 在催化领域的应用, FIR 可以用来表征金属有机化合物类、金属原子簇类、不同晶相的氧化铝等催化剂的结构. 在研究气体在催化剂表面上的吸附过程中 FIR 展现出独特的优势: 直接检测到气体 (如 CO) 与不同类型载体 (如 MOx) 的成键 M-C, 分析两者的相互作用强度, 进而表征催化剂载体表面的性质. 如 CO 在载体 M-ZSM-5 (M = Li, Na, K, Rb, Cs) 上的吸附强度ν(M-C) 和交换离子 M 的 1/r2 成正比 (r 是 M 的半径), 且 CO 在 ZnO 上的吸附强度 (ν(Zn-C) = 215 cm-1) 相对于在 M-ZSM-5 的吸附较强 (ν(M-C) = 85-150 cm-1), 因 ZnO 载体的电负性较碱金属强, 对于 CO 的吸附作用更强. 另外原位 FIR 可通过分析金属物与多种底物的相互作用强度、反应过程中催化剂的结构、浓度的变化趋势等, 为催化机理的分析提供理论支持. 在最新的研究成果中, 我们借助原位远红外光谱研究了多种金属氯化物催化葡萄糖异构化过程的机理, 经分析得知活性最高的催化剂 CrCl3 与底物葡萄糖分子中的羰基、羟基、乙二醇等结构配位较弱, 而与葡萄糖分子中的活性部位羟基乙醛结构作用较强. 而其他的金属氯化物如 VCl3 和 FeCl3 不仅与羟基乙醛结构配位较强, 与底物和产物分子中的羰基或羟基的作用也较强, 这对于其选择性地异构化葡萄糖不利. 综上所述远红外光谱在催化领域的应用展现了广阔的前景, 我们期待远红外光谱在催化研究中得到更广泛的运用.
关键词催化     远红外光谱     表征     原位分析     低能振动模式    

1. Introduction

Fourier transform infrared (FTIR) spectroscopy has played an important role in identifying molecular finger prints of reactants,products and intermediates,in elucidating the mechanisms of a broad range of reactions,and in probing the fundamental nature of active sites of many catalysts by both in-situ and ex-situ measurements [1, 2]. Specifically,FTIR spectroscopy measures the absorption of chemical bonds or groups in the 10-12500 cm-1 spectral region. The study of FTIR is commonly performed in three spectral segments,near infrared (NIR,4000-12500 cm-1),middle infrared (MIR,400-4000 cm-1),and far infrared (FIR,10-400 cm-1) (Fig. 1). MIR spectroscopy has been well established and most widely applied to study various bonds among C,H,O,N,S,B,X (halides). MIR application covers a wide range of fields [3, 4, 5, 6],including chemicals,food safety,environmental monitoring,materials,etc. The application of MIR in catalysis is relatively mature in following the transformation of chemical bonds and groups involved in reactions and over catalyst surfaces.

Fig. 1. The regions of infrared spectra.

However,for structural investigation of chemical bonds involving heavier elements,particularly those in inorganic compounds such as metal oxides or salts,spectroscopy in the MIR and NIR regions is not applicable,because the vibration energies of these bonds fall in the FIR spectral region. Therefore,FIR spectroscopy can be used for the characterization of some inorganic compounds [7, 8] and some metal coordination complexes [9, 10] that may be catalytically active. FIR in the low spectral energy region has been shown to be well suited to study lattice vibrations [11],hydrogen bonds [12],as well as the skeleton vibration of aromatic molecules [13]. It should be emphasized that FIR remains much under developed and the least applied infrared tool,especially in the study of catalytic mechanisms. This mini review is therefore intended to draw attentions to the potential applications of FIR in catalysis research by discussing some important features of early studies and of some recent literatures. Potential future directions are suggested in the development of FIR for catalysis studies.

2. FIR characterization of catalyst structures

Catalysts are commonly categorized according to their physical state in corresponding reaction systems. Homogeneous catalysts refer to those that are fully miscible and disperse molecular level,while heterogeneous catalysts refer to those in which only surfaces contribute to catalytic activity. When organometallic complexes are used as homogeneous catalysts in solvent media in which reactions take place,such complexes and the reactants are both dissolved in the solvents. Although enzymes as catalysts are also homogeneous in aqueous reaction media together with reaction substrates,absorption bands by water in the IR spectral region (both MIR and FIR) is so intense that IR is not a suitable tool for such systems. Inorganic solid catalysts are mostly present as a heterogeneous phase in either liquid or gaseous reaction phase. Bonds among heavier elements,mostly metals in metallic or higher oxidation states often play major roles during catalysis. Techniques such as extended X-ray absorption fine structure (EXAFS),X-ray crystallography,mass spectrometry,nuclear magnetic resonance (NMR),UV-Vis spectroscopy,X-ray powder diffraction (XRD),X-ray photoelectron spectroscopy (XPS) and other specialized methods are often used for characterization of homogeneous catalysts or heterogeneous catalyst [14, 15]. These techniques have been proven versatile and informative pertaining to obtain critical mechanistic insights on the role of the catalysts in catalyzing reactions of interest. However,it should be noted that some of these tools are only available in specialized laboratories that are not readily accessible to many researchers. Even though FIR has not been widely applied as a catalyst characterization tool,like other IR tools,it is simple to operate,and is suited for the characterization of a wide variety of solid catalysts and organometallic complexes. As an underdeveloped spectroscopic tool,FIR offers the potentials to become a low-cost technology to provide structural information related to catalyst functions.

FIR is suited to study organometallic structural configurations. FIR studies of square planar trialkylphosphine complexes of the types cis and trans MX2L2 (M = Pd,Pt; X = Cl,Br,I; L = Me3P,Et3P) have shown that metal-phosphorus stretching frequencies v(M-P) occur in the narrow range 400-440 cm-1 [16]. Metal-halogen v(M-X) frequencies however,are found in a wider frequency range and are markedly dependent on the cis or trans geometry of the complex [17]. Boorman et al. [18] studied tetrahedral and square planar adducts of nickel (II) halides with tertiary phosphines and di-phosphines with FIR. Correlations of v(Ni-X) and v(Ni-P) with stereo-chemistry indicate that FIR is a useful technique to distinguish tetrahedral from cis or trans square planar complexes.

Metal clusters consisting of several metal atoms show spectra unique for each cluster size and exhibit fingerprints of the cluster’s structure [19, 20, 21]. Fielicke et al investigated the FIR spectra of neutral and cationic niobium clusters of Nb50/+ to Nb90/+. The experimental spectra were recorded in the 85-600 cm−1 region that covered the structure-specific vibrational finger-print range for these metal clusters. A comparison of the experimental and calculated Far-IR spectra allows for the identification of the cluster structures. The comparison with theory revealed that the overall geometries for the cations and neutrals are very similar [21].

Important to heterogeneous catalysts,FIR was shown to be able to differentiate structures of solid state catalysts [22, 23, 24]. For examples,the alumina phases,boehmite,diaspore,gibbsite and bayerite,can be distinguished by FIR spectroscopy because the low-frequency modes of FIR are generally the most sensitive to the changes of AlO4 units. Boehmite has two characteristic FIR bands at 366 and 323 cm−1,while diaspore has five bonds at 354,331,250,199 and 158 cm−1. Gibbsite shows three characteristic FIR bands at 371,279 and 246 cm−1,whereas bayerite shows six bonds at 383,345,326,296,252 and 62 cm−1 [22]. Thus FIR allows for the study and the differentiation of the stretching of AlO4 units to characterize these four alumina phases in bauxites.

Microporous materials,particularly zeolites,are widely used as selective adsorbents for separations and as heterogeneous catalysts for catalytic processes. IR spectroscopy of adsorbed probe molecules is a widely used technique for zeolite characterization [25]. CO is the most frequently used molecule to probe zeolite structural and surface properties by monitoring the variation of its IR absorption wavenumber in reference to that of CO in gas phase. Otero Areán et al. [26] studied the stretching vibration of weak M+∙∙∙CO bond (M = Li,Na,K,Rb,Cs) formed upon CO adsorption in different alkali-metal exchanged zeolites at 77K. As shown in Fig. 2,the wavenumber of the cation-carbon bond vibration ν(M-C) increases linearly with increasing the inverse of the square of the cation radius. The absorption wavenumber of CO on an alkali ion does not vary appreciably in different zeolites,such as ZSM-5,Y,X and FER. The largest Na-CO vibration wavenumber is 141 cm-1. The high sensitivity of the ν(M+-CO) to the metal ions (M = Li,Na,K,Rb,Cs) in the FIR region suggests that it would be possible to quantitatively determine the relative abundance of these metal ions in zeolites.

Fig. 2. Plot of the wavenumber of the cation-carbon stretching vibration versus the inverse of the square of the cation radius. Reproduced with permission from Ref. [26].

For CO adsorbed (at 210 K) on ZnO,Saussey et al. [27] reported the ν(Zn-CO) fundamental stretching at 215 cm-1. The higher wavenumber of the cation-carbon bond ν(M-C) observed for the CO/ZnO system than the CO/alkali-metal exchanged zeolites can be explained by the stronger Zn-CO bond strength due to the higher electric charge density of the Zn2+ ion. Thus FIR spectroscopy of appropriate probe molecules may reveal structural details of surface sites by accurately measuring the low energy modes. Furthermore,Engström and Ryberg [28] compared the vibrational properties of the low-energy modes of a molecular and an atomic adsorbate: CO and O on Pt(111) surface by far infrared spectroscopy. For oxygen atoms an antiabsorption dip associated with the frustrated translation was observed,while in contrast,no such dip was observed for the frustrated rotations of CO. Obviously,MIR,FIR spectroscopies become complementary in studying gas adsorption process in catalysis [25, 26]. They can be used to study a wide range of energy from 10 to 4000 cm-1 and to track light variations of the molecular vibration of adsorbent interaction with the substrate through the whole adsorption process.

3. In-situ FIR study in catalysis

In-situ IR has been widely used for catalyst characterization to gether information about catalyst structure,concentration of reactants,intermediates and products. In-situ FIR could lift,to some extent,limitations in the region of middle infrared spectrum to allow for characterization of some catalytic reactions. For example,MIR only follows the changes in reactants,intermediates and products by monitoring the specific chemical bonds or structures in reactions catalyzed by homogeneous catalysts,while FIR may be suited to study the interactions between the catalysts and the reactants,intermediates and products. The FIR spectroscopy may therefore provide rich information for understanding the catalytic mechanism.

E. g.,a considerable number of investigations have been focused on glucose catalytic conversion to 5- hydroxymethylfurfural (5-HMF) [29],a platform chemical that can be converted to various chemicals,biofuels and biomaterials [30].

A considerably large number of publications have appeared that reported results of the reaction mechanism with various analysis techniques [31, 32, 33] since the discovery of a new catalytic system (Scheme 1) that enabled the conversion of glucose to 5-HMF [34]. Typical techniques such as NMR,XRD,UV-Vis,MIR are not capable of revealing the catalytic mechanism for this complex system. Most recently,an in-situ FIR spectroscopy tool has been successfully applied to the study of the coordination chemistry of various metal chlorides in an ionic liquid,1-butyl-3methylimidazolium chloride,or [BMIM]Cl [10].

Scheme 1. The proposed pathway of glucose conversion to 5-HMF in 1-ethyl-3-methylimidazole chloride ([EMIM]Cl). Reproduced with permission from Ref. [29].
3.1. Important factors in FIR analysis

In-situ FIR spectroscopy has limitations for two reasons. (1) FIR spectroscopy has been recorded with a DTGS/Polyethylene detector,the sensitivity of which is much lower than that of the MIR spectral detector,and (2) the energy of light source is lower in FIR region,so that the spectral noise becomes greater. Furthermore,water vapor in air greatly impacts on the quality of the far-infrared spectra. Water vapor molecule has many rotating absorption peaks in the far infrared region. When the FIR absorption spectrum of the sample is weak,strong moisture absorption makes it difficult to clearly distinguish peaks due to absorption by the sample. Therefore,in measuring in-situ infrared spectroscopy,care must be taken to minimize the impact of water vapor from the absorption spectrum. For a non-vacuum FTIR spectrometer,dry air or nitrogen purge of the optical bench is critically important. In our experience,a customized sample compartment lid provides an efficient protective physical barrier by reducing the impact of ambient air on the samples under investigation. Care must be taken during sample transfer to minimize air exposure. It should be noted that spectral resolution and the water vapor spectrum are directly related. The number of rotational absorption peaks,the peak shape and peak position of water vapor molecules change with the resolution of the measurement: the higher the resolution,the larger the number of water vapor absorption bands is. An 8 cm-1 resolution may be sufficient for the routine study in FIR spectrum. For a small amount of sample,the absorbance measured could be very low. In this case,a resolution of 16 cm-1 could be used [35].

3.2. In-situ FIR study of the mechanism of metal chlorides catalyzed glucose conversion to 5-HMF

Four representative metal chlorides,CrCl3,VCl3,PtCl2,and FeCl3 were chosen based on their conversion,yield (Fig. 3) for glucose conversion to 5-HMF and studied by in-situ FIR in order to understand the distinctively different performance characteristics of the catalysts in correlation to their coordination chemistries.

Fig. 3. The catalytic characteristics of metal chlorides for glucose conversion to 5-HMF in [BMIM]Cl at 96 ℃. Reproduced with permission from Ref. [10].

Then in-situ FIR spectroscopy was employed to follow the trend of metal-Cl absorption band variation in the complexes in the process of the glucose conversion catalyzed by the metal chlorides in [BMIM]Cl (Figs. 4 and 5).

Fig. 4. The FIR spectra of metal chlorides/[BMIM]Cl/glucose recorded at 100 ℃. (a) CrCl3/[BMIM]Cl/glucose,about 30 min; (b) VCl3/[BMIM]Cl/glucose,about 60 min; (c) PtCl2/[BMIM]Cl/glucose,about 80 min; (d) FeCl3/[BMIM]Cl/glucose,about 60 min. The arrows indicate that intensity changes with time. Reproduced with permission from Ref. [10].

Fig. 5. The trend of the peak absorbance at 303 cm-1 (a) and 497 cm-1 (b) in the CrCl3/[BMIM]Cl/glucose reaction system. The spectra were recorded for 30 min after the reaction started for 30 min. The arrows indicate that intensity changes with time. Reproduced with permission from Ref. [10].

The dissolved MClx (M = Cr,V,Pt,Fe; x = 2,3) were found to form new M complexes in the MClx/[BMIM]Cl/glucose reaction system under typical reaction conditions,as shown in Fig. 4. The absorbance of Cr-Cl band at 302 cm-1 decreased gradually at the beginning (Fig. 4(a)) and then showed a limited restoration (Fig. 5(a)) after an extended period of reaction,due to the consumption of glucose. Meanwhile,the peak intensity of Cr-O (from glucose) coordination bond at 497 cm-1 increased gradually (Fig. 4(a)) and then decreased slowly (Fig. 5(b)). Thus the FIR spectra indicate that Cr(Ⅲ) center coordinated with glucose first and catalyzed the isomerization of glucose to fructose. In addition,in-situ far-infrared spectra of the VCl3/[BMIM]Cl/ glucose system (Fig. 4(b)) indicate that the V-Cl bond absorbance at 287 cm-1 declined much more than the Cr-Cl bond absorbance in the CrCl3/[BMIM]Cl/glucose system with time, and with concomitant change in V-O bond FIR absorbance. It is possible that the vanadium ion coordinates with more than one glucose molecule,and can coordinate with the oxygen of a carbonyl group and a glycolaldehyde structure at the same time,resulting in increased side reactions dominated by humins. The spectra in Fig. 4(c) show the FIR features of the PtCl2/[BMIM]Cl/glucose system. Both the glucose absorption peak at 554 cm-1 and the Pt-Cl stretch vibration band at near 310 cm-1 showed a less pronounced change in 80 min compared to that in CrCl3/[BMIM]Cl/glucose (Fig. 4(a)). Evidently,replacement of Pt-Cl bond by Pt-O bond is not favored as indicated by the FIR spectra. As a result,PtCl2 displays rather low catalytic activity for glucose conversion (Fig. 3). In the FeCl3/[BMIM]Cl/glucose system,the absorbance of the anion [FeCl4]- at 381 cm-1 decreased sharply and the absorbance of [FeCl4]2- [36] at near 280 cm-1 increased gradually at the same time. Neither the absorbance at 381cm-1 or 280 cm-1 was restored,even after 2 h (Fig. 4(d)). Evidently the strong Fe-O bonds contribute to the non-selective catalytic performance of Fe(Ⅲ) catalyst due to the formation of dominantly humins.

3.3. In situ FIR study of the interaction strength between substrate and catalytic center

FIR spectroscopy was also applied to the study the coordination strength of metal chloride CrCl3 in [BMIM]Cl in the presence of model compounds with different oxygen sources. The results were correlated with the performance of CrCl3 for glucose conversion in the presence of the same model compounds [10].

The Cr-Cl bond in [CrCl6]3- complex absorbs at 302 cm-1. The intensity of this band decreased in response to the added model compounds,n-butanol (Fig. 6(a)),cyclohexanone (Fig. 6(b)),H2O (Fig. 6(c)). The intensities of these bands were able to gradually restore by evaporization of the model compound at 100 ℃. The coordination to Cr(Ⅲ) by the oxygens from n-butanol,cyclohexanone,or water is so weak that a temperature of 100 ℃ was sufficient to disrupt the Cr-Omodel compound coordination bond and to reverse fully to the stable [CrCl6]3- complex. However,when excess glycolaldehyde was added to the CrCl3/[BMIM]Cl system,the Cr-Cl bond absorbance at 302 cm-1 was decreased by nearly 1/2 (Fig. 6(d)),due to the formation of Cr-O (coming from glycolaldehyde) coordination bonds and Cr-Cl-Cr bridged bond [36]. Thus Cr(Ⅲ) center is strongly coordinated with glycolaldehyde. And the strong interaction with the glycoaldehyde competes with glucose coordination to the Cr(Ⅲ),resulted in a reduced glucose conversion and 5-HMF yield,as supported by the catalytic results in Fig. 7.

Fig. 6. (a) FIR spectra of the Cr-Cl stretch vibration in the CrCl3/[BMIM]Cl/n-butanol system; (b) FIR spectra of the Cr-Cl stretch vibration in the CrCl3/[BMIM]Cl/cyclohexanone system; (c) FIR spectra of the Cr-Cl stretch vibration in the CrCl3/[BMIM]Cl/water system. (d) FIR spectra of the Cr-Cl stretch vibration in the CrCl3/[BMIM]Cl/glycolaldehyde system. The FIR spectra were recorded at 80 ℃; the arrows in (a),(b) and (c) represent the variation trend of the Cr-Cl coordination bond during evaporation of the model compound. The background spectra of CrCl3/[BMIM]Cl system were taken before the addition of the model compound. Reproduced with permission from Ref. [10].

Fig. 7. The effect of different probing model compounds on glucose conversion. (1) None; (2) Glycolaldehyde; (3) n-Butanol; (4) Cyclohexanone. Reproduced with permission from Ref. [10].
4. Conclusion and prospect

FIR spectroscopy is shown to be a convenient technique broadly applicable to characterize the catalyst structure,the process of gas adsorption on catalyst surface,and the determination of metal ions by using a probe molecule such as CO. The in-situ FIR technique is particularly suited to follow the progress of catalyst evolution and the products in catalytic reactions. The lattice vibration energies of metal clusters and metal oxides catalysts lie in FIR region,as well as the vibration energy of coordination complex catalysts. The force between adsorbent and adsorbate is typically weak so that it falls in the low energy mode within the FIR region. Furthermore,in-situ FIR spectroscopy could also track the changes of homogeneous catalyst in the course of catalytic reaction and explore the coordination strength between reagent and catalytic center. FIR spectroscopy could complement the application of MIR,NIR spectroscopy with the advantage of capable of measuring these low energy vibration modes accurately. In addition,there are various low energy vibration modes,such as hydrogen bonding,framework vibration of aromatics,and the rotation of the gas molecules. Thus FIR has a much far-reaching potentials in the study of catalysts and catalytic mechanisms. We expect much progress can be made by devoting efforts in expanding the potential scope and applications in the characterization of catalysts and in the mechanism study of catalytic processes.

References
[1] T. Lear, R. Marshall, J. A. Lopez-Sanchez, S. D. Jackson, T. M. Klapotke, M. Baumer, G. Rupprechter, H. J. Freund, D. Lennon.. J. Chem. Phys., 2005, 123, 174706/1-174706/13.
[2] L. MacAleese, P. Maitre.. Mass Spectrom. Rev., 2007, 26, 583-605.
[3] Z. Z. Wu, E. B. Xu, J. Long, Y. J. Zhang, F. Wang, X. M. Xu, Z. Y. Jin, A. Q. Jiao.. Food Control, 2015, 50, 405-412.
[4] J. Lejeune, J. B. Brubach, P. Roy, A. Bleuzen.. C. R. Chim., 2014, 17, 534-540.
[5] S. Nasrazadani, T. Springfield.. Mater. Struct., 2013, 47, 1607-1615.
[6] T. C. Ruthenburg, P. C. Perlin, V. Liu, C. E. McDade, A. M. Dillner.. Atmos. Environ., 2014, 86, 47-57.
[7] S. Vahur, A. Teearu, I. Leito.. Spectrochim. Acta A, 2010, 75, 1061-1072.
[8] M. Zhang, T. Moxon.. Am. Miner., 2014, 99, 671-680.
[9] M. D. Hopkins, V. M. Miskowski, P. M. Killough, A. P. Sattelberger, W. H. Woodruff, H. B. Gray.. Inorg. Chem., 1992, 31, 5368-5374.
[10] H. X. Li, W. J. Xu, T. Y. Huang, S. Y Jia, Z. W. Xu, P. F. Yan, X. M. Liu, Z. C. Zhang.. ACS Catal., 2014, 4, 4446-4454.
[11] F. Keilmann.. Infrared Phys., 1991, 31, 373-380.
[12] K. Ohno, T. Shimoaka, N. Akai, Y. Katsumoto.. J. Phys. Chem. A, 2008, 112, 7342-7348.
[13] S. Huant, J. B. Robert, G. Chouteau, P. Bernier, C. Fabre, A. Rassat.. Phys. Rev. Lett., 1992, 69, 2666-2669.
[14] E. A. Pidko, V. Degirmenci, R. A. van Santen, E. J. M. Hensen.. Inorg. Chem., 2010, 49, 10081-10091.
[15] J. H. Baek, J. S. Kim, M. J. Moon, M. S. Lee.. J. Nanosci. Nanotechnol., 2015, 15, 5314-5317.
[16] M. J. Taylor, A. L. Odell, H. A. Raethel.. Spectrochim. Acta, 1968, 24, 1855-1861.
[17] E. Lasseuguette, A. Gandini, M. N. Belgacem, H. J. Timpe.. Polymer, 2005, 46, 5476-5483.
[18] P. M. Boorman, A. J. Carry.. Inorg. Nucl. Chem. Lett., 1968, 4, 101-105.
[19] A. Fielicke, G. von Helden, G. Meijer.. Eur. Phys. J. D, 2005, 34, 83-88.
[20] C. Ratsch, A. Fielicke, A. Kirilyuk, J. Behler, G. von Helden, G. Meijer, M. Scheffler.. J. Chem. Phys., 2005, 122, 124302/1-124302/15.
[21] A. Fielicke, C. Ratsch, G. von Helden, G. Meijer.. J. Chem. Phys., 2007, 127, 234306/1-234306/8.
[22] H. D. Ruan, R. L. Frost, J. T. Kloprogge, L. Duong.. Spectrochim. Acta, 2002, 58, 265-272.
[23] F. Windisch Jr... J. Appl. Phys., 2004, 95, 5435-5442.
[24] J. Pellicer-Porres, A. Segura, Ch. Ferrer-Roca, J. A. Sans, P. Dumas.. Phys. Conden. Matt., 2013, 25, 50592/1-50592/7.
[25] J. C. Lavalley.. Catal. Today, 1996, 27, 377-401.
[26] C. Otero Arean, G. Turnes Palomino, A. Zecchina, G. Spoto, S. Bordiga, P. Roy.. Phys. Chem. Chem. Phys., 1999, 1, 4139-4140.
[27] J. Saussey, T. Rais, J. C. Lavalley.. Bull. Soc. Chim. Fr., 1985, 305-312.
[28] U. Engström, R. Ryberg.. J. Chem. Phys., 2000, 112, 1959-1965.
[29] Z. C. Zhang.. Wiley Interdisciplinary Rev.: Energy Environ., 2013, 2, 655-672.
[30] R. J. van Putten, J. C. van der Waal, E. de Jong, C. B. Rasrendra, H. J. Heeres, J. G. de Vries.. Chem. Rev., 2013, 113, 1499-1597.
[31] E. A. Pidko, V. Degirmenci, R. A. van Santen, E. J. M. Hensen.. Angew. Chem. Int. Ed., 2010, 49, 2530-2534.
[32] J. Guan, Q. Cao, X. C. Guo, X. D. Mu.. Comput. Theor. Chem., 2011, 963, 453-462.
[33] R. W. Nagorski, J. P. Richard.. J. Am. Chem. Soc., 2001, 123, 794-802.
[34] H. B. Zhao, J. E. Holladay, H. Brown, Z. C. Zhang.. Science, 2007, 316, 1597-1600.
[35] S. P. Weng, Fourier Transform Infrared Spectrometry, 2nded., Chemical Industry Press.. Beijing, 2012, 12.
[36] J. S. Avery, C. D. Burbridge, D. M. Goodgame.. Spectrochim. Acta A, 1968, 24, 1721-1726.
[37] Y. M. Zhang, E. A. M. Pidko, E. J. Hensen.. Chem. Eur. J., 2011, 17, 5281-5288.