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International Journal of Photoenergy
Volume 2012 (2012), Article ID 987606, 8 pages
Photosensitized Oxidation of 9,10-Dimethylanthracene on Dye-Doped Silica Composites
Laboratorio Catálisis y Materiales, ESIQIE Instituto Politécnico Nacional, Zacatenco, 07738 México City, DF, Mexico
Received 15 July 2011; Accepted 17 November 2011
Academic Editor: Shifu Chen
Copyright © 2012 Elim Albiter et al. 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.
A series of cationic dyes, methylene blue (MB), safranin O (SF), toluidine blue (TB), and neutral red (NR), were successfully incorporated into a silica matrix by using ultrasound irradiation during the Stöber process. Several analyses were performed, including scanning dynamic light scattering (DLS), electron microscopy (SEM), nitrogen physisorption, FTIR spectroscopy, UV-vis, and diffuse reflectance spectroscopy. The entrapped dyes on silica were evaluated in singlet oxygen (1O2) generation under visible light irradiation, by means of the photosensitized oxidation of 9,10-dimethylanthracene (DMA). According to the results, the photocatalytic performance of the silica composites was improved, and the leakage of the dye from the particles was suppressed. Among these four different types of dye-doped silica composites, the SiO2-SF composite showed the most efficient delivery of 1O2.
A photosensitized reaction is defined as the process leading to photochemical or photophysical changes in a substrate by means of the absorption of radiation by other entity called a photosensitizer . Since the 1960s, several fundamental works have been published related to photosensitization in presence of oxygen and have distinguished two competing mechanisms referred as Type I and Type II [2–5]. Type I photooxygenation involves the formation of a sensitizer triplet state (3S*) which interacts with a substrate (XH) giving rise to a pair of free radicals by electron-transfer or hydrogen-transfer mechanisms . These produced radicals react with oxygen to regenerate the sensitizer and to form peroxy or superoxide radicals. Type II mechanism implicates the direct interaction of the sensitizer excited state with oxygen, generating upon energy transfer singlet oxygen [1O2, ()] which reacts directly with numerous organic substrates .
In spite of many efforts and successful results in the study of photosensitized reactions in homogeneous media, there are some disadvantages by this route mainly due to the solubility of the sensitizers in the reaction solvent and their removal from the reaction mixture . These problems can be overcome by the immobilization of the sensitizer in appropriated solid carriers. For instance, the advantages of using a dye dispersed on a solid carrier are the oligomerization of the dye can be prevented, a higher photostability of the dye is obtained, a higher purity of the final products, and the reusability of the dye . Important applications, for example, fine chemical synthesis, wastewater treatment, and photodynamic processes, among others, have been found for photosensitized singlet oxygen production [7–14].
Although many solid carriers such as polymers, zeolites, semiconductors, glasses, silica gel, among others, have been used to support a variety of sensitizers , we are interested to develop a hybrid organic-inorganic systems made of dye-doped silica particles active under visible-light irradiation for fine chemical synthesis. Silica is a very attractive material for many industrial and medical applications because it is inexpensive, chemically inert, thermally stable, and biocompatible. In fact, silica particles have captured much attention over the past two decades for their application in catalysis, separation, biosensors, and adsorption . Silica particles can be tuned from 50 to 300 nm containing pore diameters between 2 and 10 nm allowing for different dyes loadings. Also, they have a high surface area (>700 m2/g) and large pore volume (>0.9 mL/g) allowing high loading of chemicals . The doping of organic dyes into a silica matrix is not an easy task due to the weak interaction between the organic-inorganic hybrid compound . Usually, the main problem to solve is the instability of the composites, and dye molecules with small size are easy to leak out from the matrix . Several approaches have been developed to incorporate organic dyes into a silica matrix, for instance, covalent coupling , reverse microemulsion , and electrostatic interaction (Stöber method) . However, there is still no effective method to control the dispersion of the dye molecules, since they are quickly and spontaneously accumulated into the silica particles .
Herein, we reported a simple and modified Stöber method to synthesize SiO2-dyes composites by employing ultrasound irradiation during the hydrolysis and condensation steps of the silica source and dye addition. It was found that the as-synthesized composites were well dispersed into the silica particles with high stability during the photooxidation of 9,10-dimethylanthracene under visible light.
2.1. Synthesis of SiO2-Dye Composites
Tetraethyl orthosilicate (TEOS), methylene blue (MB), safranin O (SF), toluidine blue (TB), neutral red (NR), and SiO2 nanopowder were purchased from Sigma-Aldrich and used without further purification. Ethanol (HPLC grade) was used as solvent; double distilled water and ammonium hydroxide (NH4OH) were also used during the synthesis. The molecular structure of the dyes can be seen in Figure 1.
The composites were synthesized by using a modified Stöber method where the dye was incorporated since the formation of the SiO2 particles. TEOS was used as silica source and NH4OH as catalyst, and the composites silica-dye were obtained in one-step process. Briefly, it was prepared two solutions, one containing TEOS and ethanol (solution 1) and another with NH4OH, water, and dye (solution 2). Solution 1 was poured drop by drop into solution 2, ultrasonic irradiation was applied during 10 min, and the samples were aged for 12 h under constant agitation. The obtained powders were completely dried under vacuum at 318 K. The molar ratios used in the preparation of the composites were 1/20/0.1/30 for TEOS/water/NH4OH/ethanol, and the nominal concentration of dye was or moles of dye/g of SiO2.
The dynamic light scattering (DLS) measurements were determined by a Zetasizer Nano instrument (Malvern), and ethanol was used as dispersant. A Quanta 3D FEG (Fei) scanning electron microscope (SEM) was used; the dry samples were deposited onto a carbon tape before analysis. The SiO2 and SiO2-MB samples were analyzed in an Asap 2405 (Micromeritics) automated gas sorption system to obtain the nitrogen adsorption isotherms at 77.4 K. The specific surface area was estimated with the Brunauer-Emmett-Teller (BET) model, and the pore size distribution was evaluated with the BJH model. All samples were outgassed at 373 K for 1 h prior to analysis. FTIR spectra in the region 4000–400 cm−1 were obtained with a Nexus 470 Spectrometer (Nicolet). The powders were mixed with KBr to form a pellet. UV-vis spectra were obtained on a Cintra 20 Spectrometer (GBC). The diffuse reflectance measurements were done using the lab sphere RSA-PE-20 accessory using BaSO4 as reference. In all cases the spectra were recorded in the 400–800 nm region.
2.3. Photocatalytic Evaluation
The photooxygenation of 9,10-dimethylanthracene (DMA) was carried out in acetonitrile (HPLC grade) using a Newport solar simulator (Model 67005) equipped with a 150 W Xe lamp with a maximum emission around 460 nm. It was used a 10 mL batch reactor for the evaluation of the SiO2-MB composites and an 80 mL batch reactor for the evaluation of the different SiO2-dye composites. The temperature was kept constant at 298 K, and the incident light was filtered in order to cut out light below 400 nm and eliminate any photochemical reaction of DMA. The initial concentration of DMA was 16 mg/L, and the composite loading was 1 g/L or 0.5 g/L. The reaction samples were analyzed using HPLC (GBC model 1120) equipped with a UV detector (λ = 254 nm), using a 70/30 acetonitrile/water mobile phase (1 mL/min) and a 15 cm column (Grace Prevail C18 5 μ). The samples were also analyzed using a GC-MS (Perkin-Elmer model TurboMass) using a 30 m capillary column (Alltech EC5).
3. Results and Discussion
3.1. Characterization Results of SiO2-MB Composites
The influence of the dye over the final particle size of the composite was determined by DLS. During the polymerization of TEOS through the formation of Si–O–Si bonds, the cationic part of MB molecule can interact with part of Si–O groups by electrostatic forces, increasing the stability of the hybrid system  and leading to an amount of the average size from 110 nm (as-prepared SiO2) to 141 and 185 nm by using and mol/g SiO2 MB concentration, respectively. The stability of the SiO2-MB composites was compared in a blank experiment, where a solution of MB in ethanol was mixed under stirring with the as-prepared SiO2 particles during 12 h and then dried under vacuum and 318 K. The resulting material was rinsed with ethanol, and the MB was completely washed out, causing a total decolorization. However, the SiO2-MB composite prepared by the modified Stöber method never exhibited this behavior. The remaining ethanol used in the SiO2-MB composite washes was analyzed by UV-vis, and the characteristic absorption bands of MB were not observed, confirming the high stability of the composite.
A SEM image of the SiO2-MB composite shows the morphology of the spheres in Figure 2. It can be seen spheres ranging from 100 to 200 nm in size, in some cases well dispersed but also forming particle agglomerates. The morphology of the silica spheres (not shown here) was similar than that of the composite.
Figure 3 shows the nitrogen adsorption-desorption isotherm of the SiO2 and the SiO2-MB composite. The shape corresponds to a type IV isotherm according to the IUPAC classification . The hysteresis loop (H3/H4 types) can be attributed to the presence of slit-shaped pores and open pores where no condensation was evident. According to these results, the pore size varies between 10 and 100 nm diameter (see Figure 3(a)). The corresponding surface area was 91 m2/g for SiO2 and 23 m2/g for the SiO2-MB composite. Note that slight changes in the composite adsorption-desorption isotherm (Figure 3(b)) caused a dramatic decrease in specific surface area and a bimodal behavior of pore size distribution with an important amount of macropores. These results could be indicative that MB was incorporated, probably of irregular form, into the silica matrix modifying the shape and size of the pores.
FT-IR spectra of MB, SiO2, and SiO2-MB composite ( mol/g SiO2) are presented in Figure 4. The main absorption bands of MB at 1610, 1505, 1405, and 1355 cm−1 are assigned to the = N+ cation, the heterocyclic skeleton, and to the −CH3 symmetric and asymmetric bending vibrations, respectively [23, 24] (Figure 4(a)). The obtained spectrum of SiO2 (Figure 4(b)) reproduces the general features often reported for this compound [24, 25]. It is worth noting that bands at 1200, 1100, 800, and 460 cm−1 are attributed to Si–O–Si vibrations and band at 960 cm−1 corresponds to the Si–OH vibration. The spectrum also presented a broad band located between 3750 and 3000 cm−1; this can be generated by the hydration of the solid (bands located at 3350 and 1630 ) or by the presence of SiO–H vibrations . The FT-IR spectrum of the SiO2-MB composite was quite similar than that of SiO2, which can be attributed to the low concentration of MB in the material, so that the main absorption bands of MB overlap with SiO2 bands (Figure 4(c)). Note that a slight deformation of Si–O–Si bands at 1200 cm−1 and 3000–3750 cm−1 is detected in the composite which can be indicative of a bonding interaction between the organic dye and SiO2 .
The visible light absorption spectra of SiO2-MB composites and a mechanical mixture (MB + commercial SiO2) are compared in Figure 5. In the mechanical mixture sample, a strong band appears at 670 nm and one shoulder at 610 nm (Figure 5(b)). The main band is associated to free molecules of MB (monomer, see Table 1), and the shoulder is assigned to the formation of the so-called H-aggregates (dimers) [26, 27]. In the diffuse reflectance spectrum of SiO2-MB composite [MB] = mol/g SiO2 (Figure 5(a)), a wide band appears with a maximum at around 610 nm indicating that the predominant species was MB dimers. If the concentration of MB is increased to mol/g SiO2, the maximum of absorption is shifted to around 590 nm, which is interpreted as the formation of trimers and higher aggregates .
The visible light absorption spectra of the different SiO2-dye composites prepared by the modified Stöber method and the mechanical mixture preparations are shown in Figure 6. In general, each kind of preparations presented different optical properties. For instance, the composites prepared by the modified Stöber method showed a better band definition compared with the wide and irregular profile of the mechanical mixture bands. Note that a broad absorption band with a maximum at 490 nm was observed for commercial SiO2 + SF (Figure 6(d)); in comparison with the SiO2-SF composite, a sharper absorption band appeared at 515 nm (Figure 6(a)). These results indicated that, in the first case, dye aggregates were the predominant species meanwhile; in the second case there were more monomeric dye species incorporated into the silica matrix [28, 29]. The SiO2-NR composite and its mechanical mixture are shown in Figures 6(b) and 6(e). In the mechanical mixture, a broad absorption band from 400 to 650 nm, with a maximum centered at 505 nm, was previously assigned to the absorption of H-aggregates (dimers) of the dye . When the dye was incorporated since the formation of the SiO2 matrix, a solvatochromical shift in the absorption maximum to 535 nm was absorbed, and a slight shoulder at 480 nm was also observed. The absorption band associated to the free molecules of NR is located around 535 nm [29–31], and the absorption associated with the uncharged form of NR is located around 450–460 nm in methanol [30, 32]. Hence, the predominant species in the SiO2-NR composite was the free molecules of the dye although the neutral form (pKa = 6.8 ) could be present, due to basic media used in the preparation of the materials, causing the observed shoulder. In the case of TB, the mechanical mixture with commercial SiO2 (Figure 6(f)), the absorption spectrum presented an ill-defined band with a maximum centered at 585 nm, produced by the presence of TB dimers [33, 34]. When TB was incorporated into the SiO2 composites (Figure 6(c)), a well-defined band appeared in the absorption spectrum centered at 615 nm and a slight shoulder also appeared at 495 nm. The absorption at 615 nm was produced by the presence of TB monomers in the composite.
3.2. Photosensitized Oxidation of DMA
In photosensitized reactions, the photosensitizer molecule absorbs the energy of a photon () of ultraviolet or visible radiation to become an excited singlet state which rapidly converts into an excited triple state. The lifetime of the triplet is longer (microseconds) than that of the singlet (nanoseconds) so that energy transfer from the triplet to dissolved oxygen molecule to form singlet oxygen (1O2) is possible. The amount of singlet oxygen generated by a photosensitizer is determined by the rate of absorption of photons, the triplet quantum yield, and the efficiency of the energy transfer process . After singlet oxygen is generated, it either reacts with a substrate or losses its excitation energy as heat or light emission (phosphorescence). Scheme 1 shows a reaction scheme considering the visible light irradiation of a SiO2-dye composite in presence of oxygen, ethanol, and the main substrate DMA.
Scheme 1 (reaction scheme of the photosensitized oxidation of DMA on dye-doped silica composites). where is the light intensity, is a rate constant for the quenching of excited SiO2-dye by triplet oxygen to produce singlet oxygen, is the rate constant of chemical quenching of singlet oxygen in presence of DMA; however, singlet oxygen also decays to the ground state by energy transfer to the solvent or with other species in solution with a rate constant . A rough estimation of the rate constant in (3) can be obtained by considering that an excess of singlet oxygen is produced compared with the initial concentration of DMA and then a pseudofirst-order reaction is proposed (5)–(8): where The concentration profiles of DMA, during the photooxidation in presence of SiO2-MB, are shown in Figure 7. Note that raw data fit well to a first-order reaction at two concentrations of MB, with values of 0.0762 and 0.0154 min−1 for and moles of dye/g of SiO2, respectively.
As shown in Figure 8, the conversion of DMA followed a similar behavior (first order kinetics) with the different SiO2-dye composites. However, the rate constants had different values, and it is clearly seen that SiO2-MB is not a good photocatalyst for this reaction. Note that the values had the following increasing order depending of the dye used in the photooxidation of DMA (Figure 9): SF > TB > NR > MB. These results revealed that the singlet oxygen generation depended on the type of composite used. Therefore, in the particular case of SiO2-SF composite instead of presenting almost the same absorption properties than MB, it presented a rate constant one order of magnitude higher compared with MB which should be interpreted as SF dye was homogenously dispersed on the silica matrix, as indicated by the UV-vis spectra results (Figures 5 and 6), where the SiO2-SF composite presented a sharper absorption band at 515 nm, mainly as a consequence of the presence of monomeric species of SF in the material. Further studies are in progress in our lab in order to know in detail the properties and behavior of the SiO2-SF composites for fine chemical synthesis under visible light irradiation.
Finally, a reaction path scheme showing the formation of DMA endoperoxide and two unidentified byproducts (V and VI), which were found with all series of dye-doped silica particles, is presented in Figure 10. As mentioned before, the main product was the DMA endoperoxide; however, the two unidentified byproducts were detected by HPLC and GC-MS (supplementary information). As is well known, the endoperoxides are highly instable compounds so that easily decompose to other oxygenated compounds following a parallel path forming stable products as the unidentified V and VI byproducts.
In this study, a novel procedure (modified Stöber method) to obtain stable and active SiO2-dye composites for the photosensitized oxidation of 9,10-dimethylanthracene was developed. We found important differences in the mechanical mixtures and Stöber’s method preparations of our four dye-doped silica composites than can be attributed to the higher electrostatic interaction and dispersion of the dye into the silica matrix by the second procedure. According to the results, all dyes had a larger affinity to the matrix and can be easily incorporated. These findings agreed with the photocatalytic behavior, and the SiO2-SF composite showed the most efficient delivery of 1O2. Two byproducts were also detected during the photooxidation of DMA which are probably assigned to the decomposition of the endoperoxide.
This work was financially supported by the National Council of Science and Technology (Conacyt) Projects: 106891 and 153356. The authors also acknowledge the support of COFAA-IPN. E. Albiter thanks Conacyt for the scholarship support.
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