Open Access Article
J.
Cichos
and
M.
Karbowiak
*
University of Wrocław, Faculty of Chemistry, ul. F. Joliot-Curie 14, 50-383 Wroclaw, Poland. E-mail: miroslaw.karbowiak@chem.uni.wroc.pl
First published on 14th November 2013
Here we report a method for coating of hydrophobic nanocrystals (NCs) with a thin silica layer. By using this approach 11 nm NaGdF4 NCs were coated with a mesoporous silica shell thinner than 20 nm resulting in highly monodisperse core–shell nanocomposite particles smaller than 50 nm. The synthetic protocol used here is based on the two-phase system that ensures high repeatability of the nanoparticle morphology and can be conveniently adapted for large-scale production. The use of an organic solvent as a diluent for tetraethoxysilane allows us to control not only the thickness, but also the porosity of the uniform silica shell. This procedure can be applied for coating NCs of various sizes and can be generalized to encapsulate other nanocrystals, e.g. semi-conductor quantum dots, into silica spheres. Furthermore, it allows facile surface modification with –NH2 groups that can be then used to conjugate biomolecules to the nanoparticle surface, as well as straightforward incorporation of various organic molecules (e.g. dyes or drugs) into the silica shell during its growth. To demonstrate potential applications up-converting NaGd0.80Yb0.18Er0.02F4 NCs were used as cores and zinc phthalocyanine was incorporated into the silica shell as a photosensitizer. Under irradiation with a 980 nm laser diode efficient generation of singlet oxygen was observed indicating that such nanocomposite particles have the capability to be used for photodynamic therapy.
To render NaYF4 NCs hydrophilic a number of compounds were tested as bio-compatible ligands for surface modification, e.g. PEG phosphate,4 mercaptopropionic acid,5,6 diphosphonic acid,7 phospholipids8 as well as polymer molecules such as poly(acrylic acid),9 poly(allylamine),10 polyethylenimine,11 polyvinylpyrrolidone12 and amorphous silica.12–16 The latter appears as the most widely accepted approach. Silica coating provides shielding of NCs from the water environment, thereby preventing emission quenching. At the same time silica facilitates introduction of reactive groups onto the nanoparticle (NP) surface for further bio-functionalization using well-established protocols. The most popular reagents used for surface modification are (3-aminopropyl)triethoxysilane (APTES) and (3-mercaptopropyl)trimethoxysilane (MPTES) which introduce NH2 and SH groups, respectively, enabling the covalent binding of biological molecules to the surface of NPs.
The two most common methods in the literature for coating of nanofluoride NCs are analogous to those widely used for preparation of monodisperse colloidal silica particles, i.e. the Stöber approach and the microemulsion based method. The first group of methods originates from the procedure described in 1968 by Stöber17 including its subsequent various modifications. There are numerous examples of using this method for silica coating of various NCs, for example Fe3O4,18 NaYF4:Ln3+,13,15,19 or LnF3.20 The main limitation of the Stöber method is that it can be employed for NCs forming colloidal solutions in water–alcohol media, whereas the vast majority of synthetic methods yields NCs with a hydrophobic surface which enables them to be suspended in chloroform or toluene, but not in water or ethanol. Moreover, the Stöber method, which was originally devised for preparation of colloidal silica nanoparticles, is very efficient in the synthesis of monodisperse silica spheres with diameters larger than 200–250 nm. Even though it is possible to obtain much smaller particles (<30 nm), their polydispersity typically exceeds 20%.21 Consequently, the silica shells obtained on NCs by Stöber related methods are relatively thick and achievement of thin uniform layers with controllable thickness is still quite challenging.
An alternative route for synthesis of small silica nanoparticles (<50 nm) with better polydispersity is the microemulsion approach.22 Microemulsion based methods have been employed for fabrication of silica shells in various NCs (quantum dots,23 noble metals,24,25 FexOy,26 NaYF4 nanofluorides,12,14,27 and many others) yielding, in general, superior results compared to the Stöber method. However, the distinct disadvantage of microemulsion methods is the use of large amounts of surfactants, which require extensive washing, as well as problems with obtainment and sustainment during the synthesis of uniform micelles.21,28 Moreover, these methods allow obtaining silica layer with thickness that is rather discrete than variable in a continuous range.29 The efficacy and repeatability of the microemulsion method is strongly conditioned by controlling many strictly defined parameters of the process, such as the temperature and concentration of water, catalysts, SiO2 precursors, coated nanoparticles as well as surfactants and co-surfactants. Deviation from optimal conditions makes the control of silica shell thickness significantly more difficult and results, in a most fortunate case, in agglomeration and/or embodying of many cores into one silica shell.30 Another important limitation results from the fact that microemulsion methods cannot be conveniently adapted for large-scale production.
For some applications, such as photodynamic therapy (PDT), it is important to be able to obtain the mesoporous structure of the silica layer and to control the porosity degree. Most of the methods hitherto reported in the literature require additional steps in the synthesis procedure to achieve the desired porosity.31,32 Moreover, photosensitization of NPs usually entails a separate procedure of chemical attachment of photosensitizing molecules to the surface of modified (e.g. using (3-aminopropyl)triethoxysilane NH2(CH2)3Si(OC2H5)3) silica. The simple impregnation of NPs in the solution of photosensitizer usually leads to agglomeration and leakage of the dye outside NPs during PDT treatment.
The demonstrated disadvantages of Stöber and microemulsion methods indicate that coating of hydrophobic NaLnF4 NCs with a thin and uniform silica layer with controllable degree of porosity still remains quite challenging. Despite recent advances the morphology and monodispersity of silica coated NCs synthesized using existing protocols are still far from ideal. The important breakthrough in synthesis of monodisperse silica particles with sizes below 50 nm was made by Yokoi et al.33,34 who carried out hydrolysis and polycondensation of TEOS in the two-phase system in the presence of an amino acid (lysine or arginine) as a base catalyst. Under such conditions, silicate species are slowly delivered from an organic to an aqueous phase, whereas buffering properties of the amino acid keep the pH value constant (pH = 9–10) during the synthesis. Modification of the method of Yokoi et al. enabled Hartlen et al.21 to obtain silica particles with the controllable size ranging from 15 to 200 nm. We used these approaches which proved to be the most efficient in the synthesis of silica spheres as a starting point for exploiting the synthetic route for coating of nanocrystals with silica shells.
Herein, we report a novel, versatile and universal procedure for direct coating of hydrophobic nanocrystals with a uniform mesoporous silica layer resulting in monodisperse NC@mSiO2 core–shell nanocomposite particles smaller than 60 nm. The coating is carried out in a biphasic system in which TEOS is delivered heterogeneously from a top organic layer to the bottom aqueous layer containing CTAB stabilized NCs and L-arginine as a catalyst, which ensures high repeatability of NP morphology. The method can be used for coating of various kinds of NCs, such as nanofluorides (e.g. NaGdF4) or quantum dots (e.g. PbS). Coating of hydrophobic NCs with a layer of silica makes them dispersible in water and other polar solvents. Furthermore, the proposed procedure allows facile surface modification with various functional groups (e.g., amine, thiol, carboxyl) which can be then used to conjugate biomolecules to the NP surface using some well established protocols. The synthetic parameters allowing control of the porosity and thickness of the silica layer are also indicated and discussed. The method is particularly suitable for straightforward incorporation of dyes (e.g. photosensitizers) or other organic molecules into the silica layer during its growth. If photon up-converting NCs, e.g. NaLnF4:Er3+,Yb3+, are used as cores, the incorporated photosensitizer can be excited with radiation in the NIR region.
:
1 v/v) was added. The suspension was heated to 110 °C and degassed using a vacuum pump at 110–130 °C for 60 min with periodic Ar refills. Afterwards the flask was placed in a salt bath composed of NaNO3 and KNO3 (1
:
1 wt) preheated to 355 °C, kept in it for 30 min and subsequently cooled down by addition of 15 ml of ODE. Nanocrystals were precipitated with ethanol and centrifuged. The product was washed by dissolution in toluene and precipitation with ethanol 5 times and then dried in a N2 stream and stored in a tightly closed vial. The nanocrystals were redispersed in chloroform before use.
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1 wt) preheated to 310 °C. After the temperature of the reaction mixture reached 310 °C 1 cm3 of sulfur solution was injected. After 5 min of reaction time the black solution was cooled down by placing the flask in cold water and QDs were precipitated with ethanol and washed by dispersing in chloroform and precipitation with ethanol, repeatedly (5 cycles). The as prepared PbS was dispersed in CHCl3 for further application. The procedure used for silica coating of the obtained PbS@OA was in general the same as that for the NaGdF4 nanocrystals, except that the amount of PbS@OA NCs was 3 mg.
The emission and excitation spectra were recorded on the Edinburgh Instruments FLSP920 spectrometer equipped with a Xe900 xenon lamp (450 W).
Zeta potential measurements were performed with a Malvern Zetasizer Nano ZS90 instrument.
The difficulty in obtaining an aqueous solution of hydrophobic core NCs was an important problem which had to be tackled. Fortunately, it has been previously demonstrated that hydrophobic NCs can be successfully transferred to an aqueous solution using an appropriate surfactant, e.g. CTAB.38,39 Following this approach Kim et al.40,41 transferred hydrophobic Fe3O4@OA NCs to an aqueous phase and coated them with a mesoporous silica (mSiO2) shell, using TEOS as a silica precursor and NaOH as a base catalyst. Using this approach in the next step of our procedure a microemulsion of NGF@OA NCs in water was prepared. To transfer hydrophobic NCs from a nonpolar solvent (chloroform) to an aqueous phase CTAB, Tween 80, SDS (sodium dodecyl sulfate), Triton X-100 and Igepal-CO 520 surfactants were tested. Among them only CTAB and SDS allowed us to obtain stable O/W microemulsions with good repeatability. Evaporation of chloroform from O/W microemulsion droplets yields a transparent colloidal solution of NGF@OA/CTAB (NGF@OA/SDS) NCs in water.
NGF@OA/CTAB NCs were coated with a mesoporous silica layer using the biphasic system – the bottom water phase and the top organic phase. The latter was composed of ethyl acetate or cyclohexane in which TEOS was dissolved as the silica precursor. The water phase contained dispersed NGF@OA/CTAB (NGF@OA/SDS) NCs and L-arginine (L-Arg) as a base catalyst. Such a biphasic system slows down the TEOS hydrolysis, since it is delivered with restricted rate from the organic phase to the aqueous phase where it hydrolyzes.21 In several trials it was found that the coating process proceeded much better for the CTAB stabilized microemulsion. In the case of using SDS as the surfactant only highly agglomerated, multi-core and shapeless agglutinations were observed after coating. Besides stabilizing hydrophobic NGF@OA NCs in the aqueous phase, the CTAB surfactant serves also as a template enabling formation of a mesoporous silica layer.40,41
Washing with water and ethanol (5 times each) is sufficient for removal of all unreacted species and CTAB. In FTIR spectra (Fig. S2†) only very weak bands attributed to CH vibrations can be detected at about 2900 cm−1. Additional washing with HCl solution (pH = 1–2) or heating at 130 °C in air for 12 h decreases only slightly and to the same extent the intensity of CH bands, due to removal of residual ethoxy groups (resulting from partially hydrolyzed TEOS) and/or solvent molecules from pores. Then, the residual CH bands observed in the FTIR spectrum should be attributed to OA which was not completely replaced by hydrolyzed TEOS on the NGF@OA NCs' surface. The band of N(CH3)R+ expected at 2800–3200 cm−1 is not observed in FTIR spectra. Moreover, also in the EDX spectrum (Fig. S3†) no signal from Br was detected, which indicates that CTAB is absent in the obtained material. Therefore, in our synthetic protocol no additional steps, such as treatment with HCl solution41 or calcination at 500 °C,31 are required for removal of the surfactant.
Fig. 1A and B show TEM images of the silica coated NGF@mSiO2 NPs obtained using ethyl acetate or cyclohexane, respectively, as the top organic layer. The resulting core–shell NGF@mSiO2 NPs are highly monodisperse, with empty or multicore particles being practically absent. No agglomeration is observed and the porous structure of the silica shell is clearly noticeable. The average size of particles obtained from ethyl acetate and cyclohexane is 72 and 61, whereas the shell thickness is 30 and 25 nm, respectively. NPs shown in Fig. 1 were synthesized using the procedure described in the Experimental section, which hereafter will be referred to as the standard procedure.
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| Fig. 1 Silica coated nanoparticles prepared with the use of ethyl acetate (A) or cyclohexane (B) as the diluent for TEOS. | ||
EDX maps confirm the core–shell structure of NGF@mSiO2 NPs. Fig. 2 proves that Gd and Na are only present in the core of NPs, whereas the shell is composed of Si and O. The HR-TEM image and SAED pattern indicate that the monocrystallinity of the core is retained after silica coating.
The synthesis of uniform NaYF4:Tm3+/Yb3+/Gd3+@mSiO2 nanocomposites with the shell thickness between 15 and 45 nm was reported by Liu et al.14 The authors used CTAB to transfer hydrophobic cores into an aqueous phase and then TEOS was hydrolyzed using NaOH as the catalyst in the mixture of water and ethyl acetate. Although the quality of NPs reported in ref. 14 and here seems to be comparable, our method presents significant advantages. First, the synthesis presented here is far more straightforward. In ref. 14 removal of an excess amount of CTAB surfactant by cooling the solution overnight in an ice bath at 0 °C was required. Moreover, to avoid aggregation the coating process had to be carried out under continuous ultrasonication (600 W, 53 kHz) at a temperature maintained precisely at 25 °C. In addition, to obtain a uniform silica layer TEOS was added at especially low rate of one drop every ten minutes using microsyringes. Here, we use an organic phase for controllable delivery of TEOS at a reduced rate, which is favorable in regard of process reproducibility. Second, our process allows us to control not only the thickness, but also the porosity of the shell. Third, our method, as we shall present below, can be easily adopted for coating of other NCs, for example PbS QDs, which would hydrolyze in aqueous solution under prolonged ultrasonic treatment. Fourth, our process is easier for scaling up to large scale production.
Since in the biphasic system used in the present study the process of TEOS hydrolysis and condensation runs at significantly slower rate as compared to the Stöber or microemulsion method, the synthesis is very controllable and repeatable. High repeatability has been confirmed by over 60 independent trials that yielded coated NPs with very similar monodispersity as well as porosity and thickness of the silica layer. Moreover, nanocrystals with different sizes and shapes can be effectively coated. For example, Fig. 3D presents 12 nm cores coated with a silica shell of about 32 nm, whereas Fig. 3E and F show 50 nm cores coated with silica shells of 12 and 35 nm, respectively. The process is not much sensitive to small changes in reaction conditions, but at the same time there are a number of parameters, as is discussed in more detail below, which can by altered to control and optimize the properties of obtained shells. Moreover, the relatively long reaction time enables straightforward and controllable dosage of some other species in the course of silica growth, which can be incorporated into the shell or used to modify its surface for further biofunctionalization.
Hence, the developed method provides the complete procedure for synthesis and coating of hydrophobic NCs with a mesoporous silica shell, biofunctionalization of the surface and/or incorporation of dye molecules, which can be completed under mild conditions in simple steps represented in Scheme 1.
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| Scheme 1 Schematic representation of synthetic steps for NGF@mSiO2, NGF@mSiO2(Pc), NGF@mSiO2–NH2, NGF@mSiO2(Pc)–NH2, NGF@mSiO2–FITC or NGF@mSiO2(Pc)–FITC nanoparticles. | ||
Ethyl acetate, cyclohexane and amyl acetate were tested as suitable solvents for TEOS. However, only for the first two solvents formation of silica shells was observed. The solvent forming the top organic layer does not participate directly in hydrolysis and condensation of TEOS, which takes place in the water phase or at the W–O interface. Therefore, it is somewhat surprising that the composition of the organic layer has a pronounced effect on the porosity of the silica shell (Fig. 1). If ethyl acetate is used the surface of nanoparticles becomes golf ball like (inset in Fig. 1A). The wormhole-like mesopores of the silica shell are smaller, around 2–4 nm in diameter, and more spherical than in the case of cyclohexane. The usage of cyclohexane yields spiked-nanoparticles, with a more dendrimeric structure of the layer. The pores are very big, with diameters of around 6–10 nm, and extend from the core to the surface forming irregular channels (inset in Fig. 1B).
Besides larger porosity, also the growth rate of the silica layer is significantly faster if cyclohexane instead of ethyl acetate is used as a diluent for TEOS. As we shall discuss below, this effect may be attributed to a smaller decrease of pH in the course of synthesis, which drops from the initial pH = 10.5 to pH = 5.0 when using ethyl acetate, while remaining almost unchanged (pH ∼ 9) when using cyclohexane. Consequently, the coating process, which is typically carried out at 70 °C in the presence of ethyl acetate, proceeds at a sufficient rate even at room temperature (RT) with the use of cyclohexane. This makes the process of silica layer growth more controllable. If the coating process is carried out for 24 h at 70 °C, the cores are incorporated into homogeneous silica spheres of about 50–60 nm in diameter, regardless of whether ethyl acetate or cyclohexane is used. After 24 h of reaction with the use of ethyl acetate as the top layer (the standard procedure), the 12 nm cores are coated with a silica shell of 29 nm, resulting in NPs with the total diameter of 70 nm (Fig. 3A). The shell thickness can be further reduced by decreasing the amount of TEOS (Fig. 3B) and/or increasing the amount of NCs (Fig. 3C). In the case when cyclohexane is used as the diluent for TEOS the reaction time appears to be another parameter suitable for controlling the layer thickness. NPs with the thickness of silica shell and the total size practically the same as those shown in Fig. 3A (ethyl acetate, 24 h, 70 °C) can be produced using cyclohexane and carrying out the process at RT, provided that it is prolonged to 72 h (Fig. 3D). Shortening of the reaction time from 72 h to 24 h allows reduction of the thickness of the layer below 15 nm (Fig. 3E). The larger cores (50 nm) were used in this experiment; nevertheless, a comparison of NPs shown in Fig. 3D and F demonstrates that the core size exerts only minor influence on the layer thickness. Under the same conditions 50 nm and 12 nm cores were coated with the silica layers of about 32 and 35 nm, respectively. The presented results indicate that using cyclohexane instead of ethyl acetate as the top layer enables easier regulation of the shell thickness.
CTAB stabilizes NGF@OA NCs in the aqueous phase, and also acts as a template for the nanometer-sized pore formation in the silica structure. Hence, the pronounced effect of the solvent on the shell porosity may result from different pH values at which the process occurs depending on whether cyclohexane or ethyl acetate is used as the top layer. In the latter case the more acidic conditions, owing to hydrolysis of ethyl acetate during the process, may decrease the amount of CTAB present on the surface of NGF@OA/CTAB NCs resulting in formation of a less porous structure.
Since the influence of other synthetic parameters is similar regardless of whether cyclohexane or ethyl acetate constitutes the top layer, only NPs obtained with the use of the latter are discussed below.
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| Fig. 4 TEM images of NGF@mSiO2 nanoparticles obtained using the standard procedure (the same as that used for NPs shown in Fig. 1A) except that: (A) 1.95 cm3 of chloroform solution of NGF@OA was used (three times the number of NCs used for the particles shown in Fig. 1A and 3A); (B) L-Arg concentration was 0.17 mg cm−3; (C) 50 μl of TEOS was used; (D) 100 μl of TEOS was used; (E) CTAB concentration was 0.03 M; (F) CTAB concentration was 0.04 M. | ||
The presence of –NH2 groups was further confirmed by labeling NPs with FITC. This step illustrates also the possibility of biofunctionalization of NH2-modified NPs. FITC reacts with the primary amino groups on the surface of NPs to form stable conjugates through thiourea linkage. After washing out of the non-conjugated fluorescein the FITC-labeled NPs can be detected by fluorescence spectroscopy. PL and PLE spectra recorded for FITC-modified nanoparticles dispersed in PBS buffer (pH = 7.4) confirm that NPs were successfully modified with FITC (Fig. S5, ESI†). Under the UV lamp the strong green fluorescence of FITC-modified NPs is easily visible even with the naked eye (inset in Fig. S5, ESI†).
Favorably, a slow rate of the coating process enables controllable introduction of APTES at an appropriate stage of reaction. Addition of APTES in a mixture with TEOS at the beginning of the reaction leads to formation of voids around the cores. In some NPs these empty spaces extend from the core to the surface yielding cracked spheres (Fig. 5A). A considerable number of empty spheres are also formed. A similar TEM image is observed for NGF@mSiO2–NH2 NPs obtained with APTES added after 6 h of the reaction time, although the number of cracked or void containing NPs is smaller (Fig. 5B). The observed effect of APTES is analogous to that leading to obtainment of silica nanoparticles with a rough surface44 and results from the presence of aminopropyl groups which do not participate in polycondensation. Consequently, the defective sites are formed yielding an unperfected –O–Si–O– network, which can collapse and sink causing that NPs may locally shrink when C2H5OH and H2O molecules are removed due to drying. Interestingly, addition of APTES at the initial reaction stage exerts a pronounced effect also on the porosity of formed silica shells. The inset in Fig. 5B shows that the porosity of shells obtained with APTES added after 6 h of the reaction time is much smaller compared to those obtained with APTES added after 24 h (Fig. 5C). In the latter case the porosity is practically the same as that of NPs with the unmodified surface (synthesized in the absence of APTES, Fig. 1A). Hence, we can conclude that most suitably APTES should be added after 24 h of the reaction time that results in mesoporous NPs with the surface functionalized with NH2 groups, but at the same time without any noticeable influence of APTES on the NP morphology.
The method developed here presents great advantages in comparison with the soaking method.31 Using the soaking procedure it was observed that ZnPc could be released out of the silica layer in ethanol.31 In order to prove that in our case no release of ZnPc occurs, the ZnPc incorporated NPs were dispersed in ethanol under continuous stirring for 1 h. Then, after centrifugation of NPs the UV/vis absorption spectra of the supernatants were measured showing no absorption bands of ZnPc expected in the 590–680 nm range. Importantly, NPs preserve their favorable properties, such as monodispersity, regular shape and porosity, during the photosensitization procedure proposed here (Fig. 6A).
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| Fig. 6 TEM images of (A) NGF@mSiO2(Pc) nanoparticles with ZnPc incorporated during growth of the silica layer; (B) NGF@mSiO2 nanoparticles soaked in solution of ZnPc in pyridine. | ||
The efficiency of singlet oxygen generation was evaluated by using a photochemical method based on oxidation of 9,10-anthracenediylbis(methylene)dimalonic acid (ABDA)49 (Fig. S6, ESI†). In the presence of 1O2 the ABDA fluorescence is quenched, because it is oxidized to its nonfluorescent endoperoxide form (Fig. S6C and D†).
In a typical experiment 10 mg of NGF@mSiO2(Pc) nanoparticles was suspended in 1 ml of 20 μM ABDA solution in PBS or DI water and placed in a quartz cuvette. After irradiation with a 980 nm laser diode for a specific period of time, the fluorescence of ABDA was measured under excitation at 382 nm. Fig. 7 shows the changes in the ABDA fluorescence intensity (λex = 382 nm) as a function of exposure time of the sample to NIR laser radiation. Analogous dispersion of NGF@mSiO2 NPs (without a photosensitizer) was also employed as the control in the experiment. A continuous decrease of ABDA fluorescence intensity is observed in NGF@mSiO2(Pc) colloidal solution during the exposure time, which is indicative of singlet oxygen generation. The same results were obtained regardless of whether DI water or PBS solution was used as a dispersion medium. After 70 minutes of irradiation the ABDA fluorescence intensity drops to 60% of its initial value, whereas a decrease by less than 10% is observed in the control experiment.
Qian et al.31 obtained NaGdF4:Yb3+,Er3+ up-converting NPs coated with porous silica using the microemulsion method and then incorporated ZnPc into the silica layer by soaking. The decrease of ABDA fluorescence intensity after exposure to NIR laser radiation was comparable to that observed in our case (for details see the ESI†). The major important difference is, however, that in the procedure reported here the photosensitizer is incorporated into the silica layer during its growth. This prevents its leakage even if NPs are dispersed in a solvent (e.g., ethanol) in which the photosensitizer dissolves. Qian et al.31 observed that when ZnPc is loaded by soaking nanoparticles in a solution of the photosensitizer in pyridine, ZnPc could be released out from silica in ethanol within 1 hour. Obviously, the photosensitizer was not released in DI water or PBS buffer, since ZnPc does not dissolve in these solvents.
For comparison of two methods of photosensitizer incorporation, we prepared NPs loaded with ZnPc, employing the same protocol as in ref. 31 (however, using 10 mg instead of 100 mg of NGF@mSiO2 to preserve comparability with our results obtained for NGF@mSiO2(Pc)), which includes soaking of NPs in a solution of ZnPc in pyridine (1 ml, 0.5 mg ml−1) for 24 h at room temperature, centrifuging and washing with PBS solution. Apparently, a larger load of ZnPc into nanoparticles can be obtained in this way. Fig. 7 shows that such soaked NPs generate 1O2 more efficiently than those with ZnPc incorporated during silica growth.
However, even simple visual observation of the stability of NP colloidal suspension demonstrates obviously that soaking in ZnPc solution followed by several washings with PBS leads to a considerable agglomeration of NPs. After centrifugation a thin layer of pyridine solution of ZnPc stays on the surface of NPs causing their aggregation in PBS buffer. This is owing to the insolubility of ZnPc in PBS since a similar effect was observed if some diluted pyridine solution of ZnPc was added to the PBS buffer – just a gentle centrifugation (2000 rpm, 318g) was sufficient to separate the ZnPc from the solution. TEM images prove these visual observations. Incorporation of ZnPc during growth of the silica layer yields monodisperse NPs (Fig. 6A), forming stable colloidal solutions. In contrast, strongly agglomerated NPs, with ZnPc present between grains, are observed if a soaking protocol was employed (Fig. 6B). Then, in spite of the higher efficiency of 1O2 generation, formation of NP aggregates excludes application of soaked NPs in PDT.
The preliminary results show that even a larger amount of 1O2 is produced by NGF@mSiO2(Pc) NPs obtained with the use of cyclohexane, which can be attributed to their higher porosity. Quantitative results and more detailed studies of the kinetics of 1O2 generation (Fig. S7†) as a function of NP porosity will be presented in a forthcoming communication.
Further optimization of the procedure should enable obtainment of thinner shells, with a reduced number of empty or multicore NPs. The influence of various synthetic parameters on the morphology and optical properties of silica coated QDs will be discussed in more detail in one of our forthcoming papers. Here we can conclude that the presented results demonstrate the large versatility of our procedure. It is likely that it can be applied for incorporation of other hydrophobic nanoparticles, such as magnetic oxides (Fe2O3) or metal nanocrystals (Au), into mesoporous silica spheres.
Footnote |
| † Electronic supplementary information (ESI) available: Figures presenting additional TEM images, FTIR, EDX, PL and PLE spectra, schematic representation of singlet-oxygen generation under irradiation of NPs with a NIR laser diode, quenching of the ABDA fluorescence in the presence of 1O2 and kinetics of singlet oxygen generation. See DOI: 10.1039/c3tb21442g |
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