The Physico-Chemical Characterization of Mesoporous Sulfated Zirconia Nanoparticles Prepared under Structure-Directing-Free for n -Hexane Isomerization

This article describes the physico-chemical characterization of the sulfated zirconia catalysts prepared from zirconyl chloride, acetic acid and ammonium persulfate system under structure-directing-free and calcined at 650˚C. The catalysts were characterized via an array of characterization techniques such as surface acidity and texture measurements, X-ray diffraction (XRD), ultraviolet-visible spectroscopy (UV-VIS), scanning electron microscopy (SEM) equipped with energy dispersive X-ray spectroscopy (EDXS), high resolution transmission electron microscopy (HRTEM), X-ray photoelectron spectroscopy (XPS), infrared spectroscopy (IR), thermogravimetric measurement (TG) coupled with a quadrupole mass spectrometer (MS), inductively coupled plasma-atomic emission spectroscopy (ICP-AES) and/or mass spectrometry (ICP-MS). It is clear from TG-MS, ICP-AES, and IR analyses that the precursor of the catalyst is a sulphur species-doped zirconium oxy-hydroxyl acetate complex. The presence of zirconium-bound sulfate groups results in the superacidity of the catalyst and hence high activity in n-hexane isomerization. It is shown from nitrogen adsorption and desorption, FESEM, and HRTEM measurements that the materials exhibit mesoporous and nanocrystalline structure.


Introduction
High surface area, nanostructured, crystalline metal oxides are a very interesting class of materials due to their great potential in various applications [1]. Environmental concerns have promoted legislation to limit the amount of aromatics in gasoline. However, reduction of aromatics has a negative impact on gasoline octane number that has to be compensated by other approaches. Alkanes are environmentally more acceptable than aromatics, and the branched hydrocarbons have higher octane numbers than linear alkane. The octane numbers are 26 and 93 for n-hexane and 2,2-dimethylbutane, respectively. The skeletal isomerization of n-alkanes plays an important role in the production of branched, high-octane hydrocarbons as a replacement of traditional tetra-ethyl lead additives. Isomerization of normal hexane (n-C 6 ) has been recognized to be one of the most economical units to boost octane level especially for the lower boiling gasoline. The process is typically catalyzed by bifunctional Pt/H-mordenite catalysts [2]. Recently, zirconia has been reported as a popular support for various reactions because of its high thermal stability, acid-base properties, and redox surface properties. As for supported catalysts, the catalytic activity is greatly dependent on the morphology, porosity, and surface area of the catalyst support. In our work, mesoporous monometallic Pd-promoted sulfated zirconia was used for n-hexane isomerization [3]. Herein, we describe the physico-chemical characterization of the sulfated zirconia catalysts prepared from zirconyl chloride, acetic acid and ammonium persulfate system under structure-directing-free and calcined at 650˚C, showing their high acidity, mesoporous and nanocrystalline structure.

Experimental
Details of the material preparation have been reported elsewhere by the authors [3]. In the present article, the materials were examined via an array of characterization techniques, as mentioned above, for a complete chemical and structural description.
X-ray diffraction (XRD) data were collected by using Bruker-AXS D8 Advance diffractometer or Rigaku D/max-2550/pc XRD. The XRD pattern was recorded by scanning it over a 2θ range of 20˚ -90˚ at a scan speed of 0.2 s/step with an increment 0.02˚/step and utilizing CuK α radiation at 40 kV and 40 mA.
The mean crystallite size was determined by applying the well-known Scherrer equation or Rietveld method.
The diffused reflectance UV-Vis spectra of the sulfated zirconia were recorded on a Varian Cary 5000 UV-VIS-NIR spectrophotometer equipped with an integrating sphere attachment. The computer processing of the absorption spectrum was done with Cary I-E software that allowed calculation of the Kubelka-Munk G. Y. Guo et al. function F(R) from the absorbance data. The band gap energy (Eg) for an allowed transition was determined by finding the intercept of the straight line in a plot of [F(R) × hυ] 2 versus hυ, where hυ is the incident photon energy. Or, the absorption edge energy was determined for the spectrum by a linear extrapolation to zero absorption.
Scanning electron microscopy (SEM) images were captured with a Nova Nano SEM 230 filed-emission microscope operated at 30 KV. Energy dispersive X-ray (EDX) analyses were performed using X-MAX 80 EDS on Nova Nano SEM 230. Samples for SEM were dusted on an adhesive conductive carbon disk attached to an aluminium mount.
TEM observations were performed in an instrument equipped with a fieldemission gun operating at 200 KV (JEOL-2100F) and a point-to-point resolution of 2.3 Å. High-resolution TEM micrographs were recorded using a slow scan CCD camera. The sample powders were sonicated for 5 min in absolute ethanol. A drop of the resulting suspension was then put on a carbon-coated copper grid and dried at room temperature prior to the measurement. The dimensions of the particles were measured from micrographs, taken with a transmission electron microscope.
XPS analysis was performed on a Kratos Axis Ultra DLD spectrometer (Kratos Analytical, Manchester, UK) equipped with a monochromatized aluminum X-ray source (powered at 10 mA and 15 kV) and an eight channeltron detector at room temperature under ca.10 −6 Pa vacuum. Powder samples were pressed on indium supports to provide a flat surface and decrease charging effect. The pass energy was set at 160 eV for the survey scan and 40 eV for individual spectra. The scan was conducted with a step size of 0.1 eV. Binding energy (BE) calibration was based on C1s at 284.6 eV. The acquired spectra were fitted using the Levenberg-Marquardt optimization algorithm, and peak shapes were modelled using an asymmetric Lorentzian line shape convolved with a Gaussian function, using the CACA-XPS processing software. The Ι (Zr3d 5/2 )/Ι (Zr3d 3/2 ) intensity ratio was fixed at 1.5 with an energy difference of 2.43 eV, which is in agreement with the handbook [4].
Fourier-transform infrared spectra for the pristine complex and catalysts were recorded on a Nicolet 6700 FTIR spectrophotometer (Thermo Scientific) in wavenumber 4000 -400 cm −1 range, with a resolution of 4 cm −1 and a scan number of 16. The infrared spectra of samples were studied as powder dispersed in a KBr pellet.
The thermogravimetric (TG) measurement was coupled with a quadrupole mass spectrometer (MS) to identify the species evolved from the sample during the thermogravimetric experiment, i.e., calcination process, and thus to better explain the catalytic behaviour of our sample. The measurement mode used in our work was multiple ion detection (MID), it is possible to scan only selected ions. The time dwelled at a given ion with MID mode may be much longer than with a full scanning method, thus improving its selectivity. The signals for masses 17

Acidity
Acidity is the most important function of sulfated zirconia and it is evidently could explain the small metal particle size (as will be corroborated later by the FETEM observations), since the presence of acidic groups increases the hydrophilic character of the support and favors the diffusion of the metal precursor [6].
Pyridine is widely used to identify the concentration and nature of acid sites on the surface of sulfated zirconia. The interaction of pyridine nitrogen with acidic sites gives rise to two different frequencies of bending vibration. Adsorption of pyridine on Brønsted acid sites forms a pyridinium ion, giving rise to infrared bands at ca. 1540, 1611, and 1638 cm −1 ; pyridine adsorption on Lewis acid sites yields covalently bound species, giving characteristic bands at ca. 1445, 1480 and 1575 cm −1 . The band around 1486 cm −1 is attributed to a combination band associated with both Brønsted and Lewis acid sites.
It is evident that the band area calculated from the integrated IR bands attributed to Brønsted and Lewis acid sites indicates the strength of Brønsted and Lewis acidities. It may be noted from Table 1 and Table 2 that with increasing temperature from room temperature to 300˚C, which is higher than the temperature required for hydrocarbon hydroisomerization reaction, the Brønsted and Lewis acidities of the catalysts studied remain with considerable intensity. In addition, it is worth pointing out that the typical Brønsted acidities (1540 and 1638 cm −1 ) for the monometallic Pd-promoted sulfated zirconia ( Table 2) can be interesting strengthened by raising temperature, leading to a high catalytic activity in n-hexane isomerization.

Texture
Besides the acidity, the textural parameters such as specific surface area, pore diameter and volume of a catalyst also contribute to the catalyst activity. A higher specific surface area favours the spacing of the sulfate groups, leading to less dense, more accessible and a large number of total acid sites. The large pore diameter and volume can make the reaction more feasible due to easy diffusion of reactants and product molecules. The textural properties of a catalyst are largely determined by preparation method including the initial precursor used as well as the post-synthesis treatment, e.g., digestion, calcination temperature, and  impregnation. The catalytic properties of sulfated metal oxides depend strongly on subtle variation in the material. The preparation method determines the dispersion and nature of sulphur species on the surface. Usually, sulfated zirconia is prepared by first precipitating the hydroxide of zirconium which, after washing and drying, is treated with a solution of sulfuric acid or ammonium sulfate and followed by calcination. The initial precursor used for preparing sulfated zirconia plays a vital role in the final texture and performance of a catalyst. Use of various precursors alters both Lewis and Brønsted acidity substantially. The most frequently used precursor for sulfation is dilute sulfuric acid and ammonium sulfate. The sulfation treatment of amorphous zirconium hydroxide not only provides superacid sites but also creates reducible sulfate sites [7]. The conventional preparation method for sulfated zirconia (SZ) results in microporous material. The synthesis of mesoporous zirconia has been advanced largely by utilizing templates or surfactants [1]. In our work, however, mesoporous sulfated zirconia nanoparticles have been prepared under structure-directingfree at 650˚C from zirconyl chloride, acetic acid and ammonium persulfate system. Figure 1(a) and Figure 1(c) present nitrogen adsorption and desorption isotherms at 77 K for the sulfated zirconia and monometallic Pd-promoted sulfated zirconia, respectively. The shape and sharpness of the isotherm reveal the mesoporous feature of the catalyst. According to the IUPAC classification [8], the shape of the isotherm resembles the type IV isotherm with H 1 hysteresis loop at high relative pressure, which is a characteristic of the mesoporous material, indicating capillary condensation taking place in mesopores [1] [9]. Pronounced desorption hysteresis present in the isotherm is an indicative of the presence of large mesopores in the material.
The sulfated zirconia has a bimodal pore diameter distribution in the mesoporous range, the one between 6 and 58 nm is the major, along with minor at the diameter range around 4 nm, as shown in the BJH pore distribution Figure 1(b). The monometallic Pd-promoted sulfated zirconia only has a pore diameter distribution in the mesoporous range (5 to 58 nm), as shown in the BJH pore dis-  [13]. Ammonium persulfate is used for the precursor of sulfation, yielding a sufficient number of both Lewis and Brønsted types of acidity, as shown in Table 1 and  Table 2. Furthermore, the activity for alkane isomerization is correlated to the surface site density of sulfates, and the higher the surface sulfate coverage the higher the initial isomerization activity of sulfated zirconia, thereby showing the importance of persulfates for the initiation of the reaction. In addition to the initial precursor used, digestion, calcination temperature and impregnation have important effect on the texture properties of a catalyst. The process of digestion in the course of preparation leads to an extensive polymerization through the condensation of the hydroxyl groups in the hydrous zirconium acetate complex to form ordered three-dimensional porous structure. The catalytic performance of sulfated zirconia hinges upon the successful incorporation of sulphoxy functional groups into the zirconia framework. The presence of acetic acid in solution with sulfuric acid favours a higher sulphur content in the sample. The increase in the sulphur content favours the formation of some complex sulfates that could exhibit both Brønsted and Lewis acidities. The increased surface area may be due to the presence of bridging sulfate SO 2− 4 ions on the surface. The bridging sulfate ions replace hydroxyl species on the surface, resulting in a more rigid and stable structure. Furthermore, it has been reported that the bridging sulfate ions elongate the Zr-Zr separation from about 3.4 -4.3 Å, which facilitates the dispersion of oxide particles and accordingly, increases the surface area.
It is well known that the specific surface area decreases as the calcination temperature increases and the mean pore size follows the opposite trend. This is because of the crystallite growth and pore wall thickening. It is, however, worth pointing out that our sulfated zirconia samples were prepared at calcination temperature as high as 650˚C, still showing a high BET surface area (83 m 2 •g −1 ), mesopore (18 nm), and large total pore volume (0.42 cm 3 •g −1 ), as shown in Table   3. Compared to the properties of the recently published sulfated zirconia and other types of acid catalysts for n-hexane isomerization, it may be clear from Table 3 that the sulfated zirconia studied shows the best performance among different types of acid catalysts. The mesoporous sulfated zirconia was used for n-hexane isomerization, resulting in a high catalytic activity [3].
A higher sulphur content in the sulfated zirconia made the active tetragonal crystalline phase of zirconia to be stabilised by a contribution to the rigidity of the structure, leading to an elongation of the Zr-Zr bond distance, or by retarding the tetragonal-to-monoclinic transformation. As temperature increased, more crystalline tetragonal phases were developed without the appearance of the monoclinic phase until about 650˚C, as shown in Figure 2.
The organic components present in the zirconium oxy-hydroxy acetate-persulfate complex were partially or completely removed at high temperature, leading to a greater pore volume. After the sulfated zirconia was impregnated with heteropolyacid (e.g. an acidic solution of Pd), it was possible for the heteropolyacid to locate at the inner surface of the support pores, resulting in a decrease of pore diameter, as shown in Table 3.

XRD
The tetragonal and cubic phases of zirconia are of high technological interest in ceramics and catalyst fields. Many studies have shown that only a tetragonal Z r O 2 -based catalyst shows good activity for alkane isomerization, while a thermodynamically more stable monoclinic zirconia-based catalyst is completely inactive for alkane isomerization, because one of the necessary conditions for the formation of superacid sites is the existence of metastable tetragonal phase, which may improve the stability of acid sites and acid strength of solid superacids [7]. Many approaches have been reported in attempting to stabilize either of these phases at ambient conditions. Most of these approaches include doping with tri-, tetra-, and pentavalent metals or carbonaceous material leading to the formation of oxygen vacancies to achieve charge balance. Oxygen vacancies with trapped electrons favour initial nucleation of tetragonal zirconia, and control the tetragonal-to-monoclinic phase transformation on cooling. Therefore, oxygen ion vacancies are responsible for the stabilization of tetragonal structure of zirconia at low temperature. Recently, however, it has been demonstrated that the stabilization of tetragonal zirconia at low temperature can be achieved also without the addition of the above metals. In addition, it has been shown that precursor anions and OH groups in preparing zirconia can play a complex and important role in the low-temperature stabilization of the tetragonal phase. In the present case, the stabilization of the tetragonal zirconia is mainly controlled by the presence of anion additive such as sulfate.
It is well known that surface sites, which adsorb oxygen at low temperature, are responsible for causing the tetragonal phase to undergo monoclinic transformation at low temperature; in contrast, the incorporation of sulfate covers these sites, retards the formation of larger crystallites of zirconia due to sulfate ions strong effect to attract electrons, and stabilizes tetragonal crystalline phase by retarding the tetragonal-to-monoclinic transformation. It is, in the present case, obvious from Figure 2 that a predominantly tetragonal structure is stabilized by sulfate. The sulfated zirconia with 8 -10 nm crystallite is derived from a zirconium oxy-hydroxyl acetate doped by sulphur species at a temperature as high as 650˚C. The d-spacing associated with the diffraction peak at 2θ = 30.4˚ is 0.294 nm, which is in good agreement with the expected d-spacing of (111) tetragonal zirconia (d = 0.295 nm). The XRD pattern (see Figure S1 in Supporting Information) of the monome- XRD measurement of the spent catalyst (see Figure S2 in Supporting Information) doesn't reveal significant structural changes compared to diffraction pattern of the fresh catalyst, indicating that the composition and structural integrity of the catalyst are not disturbed during the isomerization runs and hence it can be repeatedly used in hexane isomerization.

UV-Vis
UV-Vis spectroscopy gives information about the electronic transitions in the different electronic orbitals of a material, and the lattice defects present in it. In addition, the band-gap of a material may be estimated by extrapolating from the UV-Vis absorption spectrum. The optical band gap of the tetragonal zirconia is approximately at 5.1 eV (226 nm), indicating the presence of many lattice defects, probably cation impurity and/or oxygen vacancy. The optical band gap of bulk monoclinic zirconia is at around 5.2 (240 nm) and 5.7 eV, indicating less defective lattice. Therefore, this observation is complementary to the XRD result where stabilization of tetragonal phase is observed.
The diffuse reflection spectrum shows a high reflection in the visible region and a strong absorption only in the UV part (i.e., <290 nm). The drop in the UV part of reflection curve represents the host lattice absorption from the valence to conduction bands. Zirconia is an insulator material which shows interband transition in the UV region (220 nm) of the electronic spectrum corresponding to the O 2− (2p) → Zr 4+ (4d) transition, i.e., ligand-to-metal charge transfer [14]. nm, as indicated above.

FESEM
A role played by the morphology of the catalyst on catalytic conversion can't be totally excluded. It is, therefore, important to characterize the catalyst by FESEM. The SEM micrograph of the investigated catalyst at 50,000× magnification ( Figure 4) proves to be a porous structure of the catalyst, which consists of nanometer-size particles with identical morphology, especially quasi-spherical in shape and about 8 nm in size. These particles have aggregated each other, forming mesopores with the size of ca.18 and 12 nm. The value correlates well with the average pore size obtained from nitrogen adsorption data.

HRTEM
Microstructure control is a key issue in materials engineering, because almost all  The small particle size is advantageous due to shorter diffusion distances for both reaction substrates and products, which increases reaction rates. The high acidity of the sulfated zirconia support could explain the small metal particle size, since the presence of acidic groups increases the hydrophilic character of the support and favors the diffusion of the metal precursor [6]. A typical SAED pattern is shown in Figure 5(b). The SAED image confirms that the mesostructured walls are composed of tetragonal phase, displaying characteristic diffuse electron diffraction rings. The diffusive SAED pattern further proves the formation of nanocrystalline zirconia with a tetragonal structure because a good match is observed with tetragonal structure, i.e., the obtained tetragonal lattice value was 0.294 nm in agreement with XRD analysis.

XPS
XPS analyses were performed for the samples to verify the presence of sulfate species, determine surface composition especially the S/Z r final molar ratio at the surface and obtain information on the electronic states and chemical environment of carbon, zirconium, oxygen, and sulphur atoms in the catalysts. G. Y. Guo et al. corresponds to a thickness that does not exceed 5 nm. Thus, irrespective of the preparation variant, the value (sulphur to zirconium) obtained from XPS measurements exceeds that determined from chemical analysis. Table 4 presents the surface composition of the fresh and spent catalysts derived from XPS analysis.
The O 1s spectrum (Figure 6(b)) for fresh catalyst is the same as that for spent catalyst ( Figure S3 in supporting information), and mainly comprises the first peak at 530.43 eV (fresh) and 530.58 eV (spent), corresponding to the oxygen in the network of zirconia and the second one located at 532.16 eV (fresh) and 531.58 eV (spent) attributed to terminal hydroxyl and sulfate species, showing the binding energy with negligible shift between the fresh and the spent catalyst.
The high resolution scan of C1s region for fresh (Figure 6(a)) and spent catalysts ( Figure S3) shows carbons present in two different chemical environments, corresponding to SP 2 (C=C) at 284.61 eV (fresh) and 284.87 eV (spent), and the carbonyl (C=C) and alcoholic [C-(OH)] carbon at 287.23 eV (fresh) and 287.20 eV (spent).
Binding energies of sulphur ( Figure 6(c)) were recorded in the region corresponding to 2p energies. The S 2p peaks located around 169.30 and 170.69 eV for the fresh catalyst and at 169.71 eV for the spent catalyst ( Figure S3) correspond to a unique sulfated species, resulting in the remarkable acidity on the surface of the sulfated zirconia. Figure 6(e) depicts the curve fitting in the de-convolution of Zr 3d spectrum for the samples. The main peaks at 185 and 182.67 eV for the fresh catalyst correspond to the Zr 3d 3/2 and Zr 3d 5/2 , respectively, which agrees well with the values reported in the literature for ZrO 2 [4].
The accurate P d superficial concentration is not available due to its low loading and partial overlap of P d 3d 5/2 with Zr 3p 3/2 [14]. Only weak signal exists for the 0.5 wt% P d catalyst because of the low concentration of P d atoms [6] [15] [16].

IR
The chemical bonding mode between carboxylic acid, persulfate groups and zirconium centres is elucidated by infrared spectroscopy among the most well-developed analytical techniques for the characterization of organometallic complexes. Figure 7 presents the infrared spectrum of the pristine complex. The infrared vibrations of the complex are assigned by using evidence from the literature.  The broad band centred around 3416 cm −1 is due to the -OH stretching vibration in the acetate and persulfate, and water molecules. The bands around 1552 and 1431 cm −1 are ascribed to the asymmetric and symmetric stretching vibrations of the carboxyl (-COO − ) for the acetate ion, respectively. The frequency separation Δυ between the asymmetric and symmetric carboxyl stretching vibrations of an acetate group is an indication of the coordination mode of the acetate ion coordinated to a metal cation [19]. In general, a bidentate bridging acetate complex exhibits a Δυ value less than, but close to, the free ionic value of 160 cm −1 . A bidentate chelating acetate complex has Δυ value significantly less than the ionic value, while unidentate coordination results in Δυ value much greater than the ionic value. In the present case, the frequency separation is 121 cm −1 , suggesting that acetic acid binds to the zirconium centre in a bidentate bridging or chelating fashion.
The infrared spectra of some known zirconium acetates and oxy-hydroxylacetates didn't contain any intense band in the stretching frequency region (900 -1100 cm −1 ) of most of the metal-oxygen double bonds [20], thereby indicating the absence of zirconyl group Zr=O in these acetates. The infrared spectrum of the complex under investigation does not exhibit any intense band in 900 -1100 cm −1 , and hence there is no formation of Zr=O bond in the complex. An ambiguous and weak band at 1051 cm −1 is observed and ascribed to CH 3 rocking [19] or S-O bond vibration [21]- [26] of S 2 O 2− fite ions coordinated to zirconium cation. The band at 1051 cm −1 remains present even in the complex calcined at 650˚C, and therefore should be attributed to S-O bond vibration of S 2 O 2− 7 . Further, the assignment for the band can be supported by taking into consideration that previous paper [20] that reported the stretching frequencies of metal-oxygen double bonds did not deal with zirconium and that several published works on some zirconium compounds have shown the stretching frequencies of the Zr=O bond at 877 [27] [28] and around 780 cm −1 [29] [30].
The bands at 1185 and 1124 cm −1 may be assigned to asymmetric and symmetric stretching frequencies of S=O and S-O bonds of S 2 O 2− 7 , in other words, are typical bands for chelating bidentate sulphate and sulphite ions coordinated to zirconium cation [22] [24] [26] [27].
On the basis of the infrared band assignments of zirconium acetate, oxy-hydroxyl acetate, related carboxylates, oxy-chloride, zirconia, and other metal carboxylates [19] [31], we associate the band at 615 and 647 cm −1 with a deformation mode of acetate group rather than sulfate ions. Sulfate anion can form strong complexes with zirconium ion, and the above bands may account for the presence of covalently bound sulfate ions. However, the above bands in the present study almost disappeared as soon as the complex was heated to 400˚C, and hence it is attributed to a deformation mode of acetate group rather than sulfate ions.
Overall, it can be assumed from the presence of these infrared bands that the complex is a sulphur species-doped zirconium oxy-hydroxyl acetate complex in which an acetate ion is directly bonded to the zirconium of zirconium tetramer mainly in a chelating bidentate coordination mode and the resulting tetramers are linked together by acetate or persulfate ions.
On the basis of the above infrared spectrum of the pristine complex, we can easily understand the infrared spectra of the sulfated zirconia, Pd-promoted sulfated zirconia and spent catalyst. As shown in Figure 8, a broad peak at 3427 cm −1 corresponds to the hydroxo-and aquo-OH stretching vibrations of hydroxyl groups, and adsorbed water is accompanied by the band at 1632 cm −1 [9] [32]. The weak bands at 2925 cm −1 can be assigned to the bending/scissoring and stretching vibration of C-H and CH 3 groups [9] [33] [34].
The surface sulphur species are present in sulfated zirconia most likely in the form of pyrosulphate species showing a characteristic IR band around 1401 cm −1 , which should be responsible for the high catalytic acidity in the acid-catalysed reactions. In the pyrosulphate species Zr atoms are directly coordinated to strongly electron-withdrawing SO x centres. This configuration shows the characteristic asymmetric and symmetric stretching frequencies of partially ionized S=O double bonds and S-O bonds in the region of 1200 -900 cm −1 , as shown in infrared spectra.
The peaks at 1140, 1052 cm −1 , characteristic of inorganic chelating bidentate sulfate ion coordinated to metal cations (Zr 4+ ), are assigned to asymmetric and symmetric stretching frequencies of S=O and S-O bonds, indicating that the impregnation of persulfate ions on the surface of zirconia was in bidentate fashion [9] [34] [35]. It is, therefore, obvious that the superacidity of the catalyst studied may be attributed to the presence of zirconium-bound sulfate groups. The IR bands at 749 and 589 cm −1 are attributed to Z r -O stretching modes, characteristic of crystalline zirconia. Finally, it can be clearly known from Figure 8 that the infrared spectrum of the spent catalyst is similar to that observed for the fresh catalyst.

TG-MS
Investigation of the thermal behaviour of the complex may be conducive in clarifying the composition and structure of the complex synthesized by the present process. Thermogravimetric (TG), differential scanning calorimetry (DSC) and elemental analyses were used to obtain information about the thermal behaviour of the complex when it was heated in air.
When the complex was heated up to 800˚C in air, the TG and DSC traces are shown in Figure 9. It can be seen that a one-to-one correlation exists between the DSC and TG traces, indicating that the thermal effects are accompanied by weight losses. The complex is found to decompose to zirconia in three steps, as shown in the DSC curve: one endothermic and two exothermic decomposition analysis is not sensitive to the determination of non-metals, and that metals may be more accurately determined by ICP-IES than by EDXS. Therefore, based on the clue given by the EDXS analysis, we have quantitatively determined the metal and non-metals by ICP-AES and by elemental analysis and X-ray fluorescence spectroscopy, respectively, yielding (wt%) Zr (51.85), S (2.388), H (3.15), N (0), and Cl (0). Combined with the data derived from the thermal gravimetric and elemental analyses, the pristine complex can be represented by an empirical formula: Zr 4 (S 2 O 7 ) 0.25 O 2 (OH) 5 (CH 3 COO) 6 •H 2 O. Figure 10 shows the ion current curve for evolved gases in the TG-MS measurement of the catalyst. As shown in Figure 10, water vapor is the evolved gas from 90˚C to 350˚C. Carbon dioxide, carbon monoxide, and methyl oxide (CH 3 O) occur over ~380˚C, 450˚C, and 400˚C, respectively. No evolution of SO, SO 2 and SO 3 is found during the evolved gas analysis, suggesting a good thermal stability of the sulfated zirconia catalyst. The weight loss below 620˚C from TG  analysis is attributed to elimination of adsorbed water and oxidation of carbon, It is, therefore, clear, from the IR and TG-MS data that the superacidity of the catalyst studied may be attributed to the presence of stable zirconium-bound sulfate groups.

Conclusions
This article elucidates the reason why mesoporous sulfated zirconia can be prepared under structure-directing-free at 650˚C from zirconyl chloride, acetic acid and ammonium persulfate system.
According to the acidity measurement, it is worth pointing out that the typical Brønsted acidities (1540 and 1638 cm −1 ) for the catalyst, i.e., monometallic Pdpromoted sulphated zirconia (Table 2) can be interesting strengthened by raising temperature, leading to a high catalytic activity in n-hexane isomerization. It is shown from nitrogen adsorption and desorption measurement that pronounced desorption hysteresis is present in the isotherm, indicating the presence of large mesopores in the catalyst.
The XRD patterns demonstrate that the Pd-promoted sulfated zirconia is a nearly pure tetragonal zirconia with 8 -10 nm crystallite, which is supported by UV-VIS spectroscopy.
HRTEM images show that particles are faceted single crystals with not exactly a spherical but much more of a polygonal shape and with clear lattice fringes corresponding to crystallographic planes of the tetragonal zirconia, due to the interplanar spacing (0.294 nm) being in agreement with the d-spacing (0.295 nm) of the (111) plane of tetragonal zirconia.
XPS analyses were performed for the samples to verify the presence of sulfate species, determine surface composition especially the S/Z r final molar ratio at the surface and obtain information on the electronic states and chemical environment of carbon, zirconium, oxygen, and sulphur atoms in the catalysts. It is clear from TG-MS, ICP-AES, and IR analyses that the precursor of the catalyst is a sulphur species-doped zirconium oxy-hydroxyl acetate complex. The superacidity of the catalyst studied may be associated with the presence of zirconium-bound sulfate groups. The sulfated zirconia catalyst possesses a good thermal stability.