Core–Shell Pluronic-Organosilica Nanoparticles with Controlled Polarity and Oxygen Permeability

pubs.acs.org/Langmuir Article Core−Shell Pluronic-Organosilica Nanoparticles with Controlled Polarity and Oxygen Permeability Cristina De La Encarnacion Bermudez, Elahe Haddadi, Enrico Rampazzo, Luca Petrizza, Luca Prodi, and Damiano Genovese* Cite This: Langmuir 2021, 37, 4802−4809 Downloaded via 191.96.226.18 on September 4, 2021 at 00:40:42 (UTC). See https://pubs.acs.org/sharingguidelines for options on how to legitimately share published articles. ACCESS Metrics & More Read Online Article Recommendations sı Supporting Information * ABSTRACT: Nanostructured systems constitute versatile carriers with multiple functions engineered in a nanometric space. Yet, such multimodality often requires adapting the chemistry of the nanostructure to the properties of the hosted functional molecules. Here, we show the preparation of core−shell Pluronic-organosilica “PluOS” nanoparticles with the use of a library of organosilane precursors. The precursors are obtained via a fast and quantitative click reaction, starting from cost-effective reagents such as diamines and an isocyanate silane derivative, and they condensate in building blocks characterized by a balance between hydrophobic and Hbond-rich domains. As nanoscopic probes for local polarity, oxygen permeability, and solvating properties, we use, respectively, solvatochromic, phosphorescent, and excimer-forming dyes covalently linked to the organosilica matrix during synthesis. The results obtained here clearly show that the use of these organosilane precursors allows for finely tuning polarity, oxygen permeability, and solvating properties of the resulting organosilica core, expanding the toolbox for precise engineering of the particle properties. potential to modify the network of silica nanostructures for this purpose.15−17 Besides controlling the hosting ability of nanocarriers, a pre-requirement for the design of successful nanostructures for nanomedicine is their colloidal stability,18 also in biological fluidsthus in the presence of large protein concentration.12,19 The well-known preparation of core−shell Pluronic-silica “PluS” nanoparticles20,21 has recently demonstrated to yield small, monodisperse, and colloidally and photophysically stable nanoparticles, also in vivo. This type of silica nanoparticles grows templated by micelles of Pluronic F127a triblock copolymer composed of poly(ethylene glycol) (PEG) and poly(propylene glycol) (PPO)in acidic water at 30 °C, and exhibits a silica core diameter of ca. 10 nm and a hydrodynamic diameter of ca. 25 nm, which corresponds to the PEG blocks of Pluronic surfactant, which remain as brushes on the silica surface. Their very small size and the shielding PEG surface are responsible for long circulation time, low accumulation rate, and enhanced targeting ability.13,21 INTRODUCTION Functional nanoarchitectures, defined as materials engineered at the nanoscale to perform specific functions,1 have revealed in the last decades an enormous potential for transversal application in science and technology,2,3 owing to their versatility and to their small scale, which allows us to easily and creatively interface them with biological structures.4−6 In the field of drug delivery, the production of carriers with high load, fast dissolution rate, and specific targeting ability has been of capital importance to maximize the action of many pharmaceuticals. An additional advantage of this sought specificity is the drastic reduction of the amount of drug that, after unnecessary contact with nontargeted biological tissues and organs, will be largely dispersed in the environment when not causing adverse effects.7 To reach this goal, various formulation strategies have been developed with the main aims of optimizing pharmacokinetics and of properly matching the polarity of the specific drugs. Nowadays, the emergence of nanomedicine8,9 with the strategic design of nanocarriers endowed with multiple functions, including targeting, yearns for transferring this knowledge to the nanoscale.10−14 An efficient nanocarrier is required to host high loads of the drug molecule, which largely depends on matching its solvating nanoenvironment to the chemistry of the drug itself. The possibility to tune the chemistry of the nanocarrier is therefore of utmost importance, and organosilanes22−24 have the ■ © 2021 The Authors. Published by American Chemical Society Received: December 11, 2020 Revised: March 26, 2021 Published: April 14, 2021 4802 https://doi.org/10.1021/acs.langmuir.0c03531 Langmuir 2021, 37, 4802−4809 Langmuir pubs.acs.org/Langmuir Article Figure 1. PluOS NP synthesis: organosilane precursors OS1−4, here schematized with two trivalent silane moieties and an organic linker, were mixed with TEOS to obtain Pluronic-organosilica nanoparticles PluOS NPs, doped with one of the luminescent probes PYS, DSS, or RBS. Scheme 1. Chemical Structures of Organosilanes OS1−4, Obtained via Reaction of Diamines 1−4 and Triethoxysylilpropylisocyanate, and of the Silanized Reporter Dyes PYS, DSS, or RBS (c) In this context, and starting from the robust synthetic protocol of PluS NPs, we explore here the possibility to modify this reliable preparation method with the use of organosilane precursors produced in situ with a fast and quantitative click reaction. The templating action of Pluronic F127 and the mild conditions can allow us to obtain nanoparticles with small size and high colloidal stability, but with a chemical network different from silica, characterized by a balance between hydrophobic and H-bond rich domains that allows for finely tuning polarity and oxygen permeability of the resulting nanoarchitectures. In addition, we explore the nanoenvironment of the resulting organosilica matrix by means of three luminescent probes that provide information on local polarity, permeability to oxygen, and ability to solubilize hydrophobic molecules. ■ MATERIALS AND METHODS All reagents and solvents were used as received without further purification. Nonionic surfactant Pluronic F127, tetraethoxysilane (TEOS, 99.99%), trimethylsilylchloride TMSCl (≥98%), tetramethoxysilane (TMOS), acetic acid (≥99.8%), reagent-grade dimethylformamide (DMF), 1-pyrenemethylamine hydrochloride (95%), 5(dimethylamino)naphthalene-1-sulfonyl chloride (dansyl chloride, ≥99.0%), hexamethylenediamine (98%), ethylenediamine (≥99.5%), p-phenylendiamine (98%) and N,N′-diphenylethylenediamine (98%) were purchased from Sigma-Aldrich. Triethylamine (≥99.5%), 3(triethoxysilyl)propyl isocyanate (≥95%), and NaCl were purchased from Fluka. The luminophores dansyl sulfonamide triethoxysilane (DSS),25 pyrene triethoxysilane (PYS),26 and Ru(bpy)32+ triethoxysilane derivative (RBS)27 were prepared as previously reported. A Milli-Q Millipore system was used for the purification of water (resistivity ≥18 MΩ). 4803 https://doi.org/10.1021/acs.langmuir.0c03531 Langmuir 2021, 37, 4802−4809 Langmuir pubs.acs.org/Langmuir Article Figure 2. (a−c) Hydrodynamic diameter distribution of RBS-doped PluOS with 50, 25, and 12.5% organosilane 1 as obtained by DLS measurement (distribution by intensity). (d) Average hydrodynamic diameter dH with relative error bars of all NPsprepared with the three fluorescent probeswith decreasing organosilane content and with or without end-capping agent TMSCl (from DLS). TEM micrographs of some organosilica NPs end-capped with TMSCl, scale bar = 20 nm: (e) RBS-doped PluOS with 25% organosilane OS1 (core diameter dC = 11 ± 3 nm), (f) RBS-doped PluOS with 12.5% organosilane OS1 (core diameter dC = 12 ± 2 nm). The organoethoxysilane derivatives OS1−4 were synthesized by click reactions between the corresponding diamine (i−iv) and (3isocyanatopropyl)triethoxysilane. In a typical preparation, 0.2 mmol of a diamine was dissolved in 0.1 mL of dimethylformamide (DMF) and 0.4 mmol of (3-isocyanatopropyl)triethoxysilane was added. This mixture was vortexed for 1 min and then stirred for 30 min at room temperature. Each synthesis was performed prior to the preparation of nanoparticles and their product used without further purification. Nanoparticles synthesis: to prepare core−shell organosilica nanoparticles (PluOS NPs), desired amounts of organosilane derivative (OS1−4), triethoxysilane dye derivative (in 0.1 mL DMF), and tetraethylorthosilicate (TEOS) were added under magnetic stirring at room temperature (25 °C) to an acidic aqueous solution (acetic acid 1 M, 1.6 mL) containing Pluronic F127 (100 mg) and NaCl (67 mg). Detailed information on the exact quantities can be found in Table S1 in the Supporting Information. After 3 h, the capping agent trimethylsilylchloride (TMSCL, 10 μL, 0.08 mmol) was then added and the solution was stirred overnight. Nanoparticle suspensions were purified via dialysis versus ultrapure water for 3 days (RC membrane, 12 KDa cutoff), and finally diluted to a total volume of 5 mL with water. started with a click reaction in DMF between a set of diamines and 3-(triethoxysilyl)propyl isocyanate to yield organosilane precursors OS1−4 (Scheme 1). The reaction is fast and quantitative, as it results from NMR and MS characterizations (see Supporting Information), thus allowing us to use the precursors without further purification. Analogous reactions were previously used to functionalize the surface of nanomaterials for catalytic purposes30,31 or to modify mesoporous nanoparticles for drug delivery.32 OS precursors are then cocondensated with tetraethoxysilane (TEOS) to tune the chemical nanoenvironment of the resulting organosilica matrix. Substituting half or more of the TEOS reagent in a typical synthesis of PluS NPs with an organosilane precursor results in the formation of nanoparticles of comparable size and morphology as PluS NPs, as witnessed by transmission electron microscopy (TEM) (Figure SI2) and by the main peak of the distribution obtained by dynamic light scattering (DLS) (distribution by intensity, Figure 2a). Yet, reduced colloidal stability is observed: aggregation is indeed confirmed by DLS analysis, which shows the presence of large sedimenting aggregates. However, by reducing the fraction of the organosilane precursors to 25 or 12.5%, we observed enhanced colloidal stability of the resulting PluOS NPs (Figure 2b−d). Plotting the dispersion of diameters measured with DLS (distribution by intensity, Figure 2d) also clearly shows the importance of the capping agent TMSCl to obtain the sought colloidal stability in water of core−shell organosilica nanoparticles.33 The average hydrodynamic diameter of PluOS NPs with 25 or 12.5% organosilanes, end-capped with TMSCl, ranges between 20 and 50 nm (Table 1). TEM reveals that in all cases, the organosilica core features a highly monodispersed diameter of 15 ± 5 nm, suggesting thatas in the synthesis of PluS NPs also in the presence of the organosilane precursor, the final core size is determined by the template action of the Pluronic F127 micelles (Figures 2e−f, S9 and S11). RESULTS AND DISCUSSION In a typical preparation of previously reported core−shell Pluronic-silica “PluS” nanoparticles,28 TEOS was added to a micellar solution of Pluronic F127 in water containing 1 M acetic acid; after condensation, trimethylsilylchloride (TMSCL) was added as an end-capping agent to promote long-term colloidal stability. Finally, a dialysis-based workup led to the isolation of monodispersed nanoparticles having a silica core of 11 ± 1 nm and hydrodynamic diameter of 25 ± 5 nm, well characterized in terms of concentration of nanoparticles, surface chemistry, and resulting photophysical properties when doped with suitable dyes.29 Starting from this method, we investigated the possibility to mix TEOS and an organosilane precursor to produce colloidally stable, long shelf-life, small core−shell organosilica-PEG nanoparticles (Pluronic-organosilica nanoparticles, here abbreviated as PluOS NPs, Figure 1). The preparation ■ 4804 https://doi.org/10.1021/acs.langmuir.0c03531 Langmuir 2021, 37, 4802−4809 Langmuir pubs.acs.org/Langmuir 25 ± 5 nm) and feature satisfactory stability against aggregation. After morphological characterization via TEM and DLS, we have investigated relevant physicochemical properties of the so-modified nanoparticle core using specific dyes, derivatized with silane moieties to be covalently linked within the organosilica network. Specifically, we have used a solvatochromic dye (dansyl silane, DSS) as a reporter of the local polarity,35−37 an excimer-forming dye (pyrene silane, PYS) to monitor the ability of the core to solubilize hydrophobic molecules,38 and an oxygen-sensitive phosphorescent dye (Ru(bpy)32+ silane, RBS) to report on the O2 permeability of the organosilane core.39,40 Three sets of organosilica NPs end-capped with TMSCl were synthesized, in three different organosilane: TEOS ratios (50, 25, and 12.5% organosilane molar fraction), for each silanized dye. The nominal dye doping degree was 1% for DSS and RBS and 0.2% for PYS, expressed in moles vs moles of silane moieties. The solvatochromic DSS dyes provide information on the micropolarity of the organosilica core, in which they are entrapped owing to their covalent silane link.36,37,41 Doping the organosilica matrix during its formation with a small amount of DSS indicates that the polarity of the nanostructured environment can be tuned by tuning the chemistry of the diamine (1−4), i.e., of the organosilane linker (OS1−4). Indeed, as shown in Figure 3a,b, the emission peak progressively shifts to a higher energy (hypsochromic shift) with increasing the number of carbon atoms in the aliphatic chain and the number of phenyl rings of the diamine, following the expected polarity scale diethylamine > hexanediamine > phenylenediamine > diphenylethylenediamine. Interestingly, the “reference” silica network formed by TEOS features intermediate polarity, suggesting that the organosilanes have a “double-sided” role on the overall polarity: while the diamine all-carbon chain linker contributes to make the silica network more hydrophobic, the urea groups formed by the reaction of amine and isocyanate provide local H-bond-rich, hydrophilic spots. The balance between the hydrophilicity of the urea groups and the lipophilicity of aliphatic and aromatic linkers results in a fine-tuning of the overall micropolarity of the organosilica nanoparticles. The comparison of the emission maxima of PluOS NPs and of DSS in different solvents, as plotted in Figure 3b, provides evidence of the magnitude of nanopolarity variations obtained by substituting TEOS with OS1−4, which ranges from a similar environment to ethanol with OS1 to a polarity lower than dichloromethane with OS4. The emission anisotropy of DSS dyes are very high for all PluOS NPs (0.25 < r < 0.35), and the monoexponential fluorescence lifetimes and high quantum yields are comparable to or higher than those of the monomeric DSS dye (Table S2 in Supporting Information), indicating that the dyes are well dispersed inside the rigid organosilica matrices and do not suffer from aggregation or self-quenching. Besides altering the average polarity of the chemical nanoenvironment within the nanoparticles, the introduction of organosilane groups may introduce different permeabilities of the network to relevant chemical species such as O2. It is important to note, at this point, that the tuning of oxygen permeability can be an interesting option to address specific applications. In fact, while a low permeability is desired for having a high luminescence intensity and photostability, a high permeability can allow the use of the nanoparticles as Table 1. Morphological and Photophysical Parameters of Dye-Doped Organosilica NPs dye DSS % OSa 0% 50% 25% 12.5% RBS 0% 50% 25% 12.5% PYS 0% 50% 25% 12.5% OS dH/nmb ndyec [dye] % mol/molTEOS only TEOS 1 2 3 4 1 2 3 4 1 2 3 4 only TEOS 1 2 3 4 1 2 3 4 1 2 3 4 only TEOS 1 2 3 4 1 2 3 4 1 2 3 4 32 14.4 0.180 0.66 57 39 66 114 38 34 60 48 21 27 44 40 37 1.9 8.3 0.7 4.8 4.2 7.5 15.8 8.1 8.2 10.3 17.9 12.6 7.4 0.024 0.104 0.009 0.060 0.053 0.094 0.200 0.101 0.103 0.129 0.224 0.158 0.093 0.74e 0.92e 0.71d,e 0.89d,e 0.66e 0.56e 0.09d,e 0.24d,e 0.56e 0.61e 0.10d,e 0.22d,e 0.070 88 74 40 172 24 36 47 55 32 40 46 44 29 0.28 0.57 0.74 0.62 3.2 3.9 6.2 4.2 7.7 6.9 10.4 7.9 7.03 0.004 0.007 0.009 0.008 0.040 0.049 0.078 0.053 0.096 0.086 0.130 0.099 0.088 0.090 0.072 0.072 0.058 0.061 0.070 0.072 0.053 0.059 0.35 144 30 54 93 77 47 38 42 31 28 44 36 3.65 7.22 0.92 3.37 4.00 4.08 5.27 3.87 5.40 5.31 5.82 4.49 0.046 0.090 0.012 0.042 0.050 0.051 0.066 0.048 0.068 0.066 0.073 0.056 0.38 0.36 0.07 0.28 0.47 0.52 0.025 0.26 0.50 0.51 0.026 0.26 Article PLQY f 0.080 f a Percentage of organosilane precursor with respect to TEOS. Hydrodynamic diameter in nanometers, average value, distribution by intensity, from DLS measurements. cAverage number of dyes per PluOS NP, obtained from absorbance spectra and assuming constant NP concentration from synthesis as in previous work.34 dThe photoluminescence quantum yields (PLQYs) are estimated excluding an energy transfer contribution from the organosilane matrix (see excitation spectra in Figures S1). eScattering is excluded from PLQY calculation, but it still introduces a significant error due to low absorption and high scattering at the excitation wavelength. fThe PLQY could not be measured. b As a general trend, the increase of the TEOS/organosilane ratio leads to an increased monodispersity in the hydrodynamic radius, suggesting that the organosilanes introduce some instability in the colloidal system. DLS shows that TMSCl end-capped PluOS NPs with equal to or less than 50% organosilane precursor converges to PluS morphology (dH = 4805 https://doi.org/10.1021/acs.langmuir.0c03531 Langmuir 2021, 37, 4802−4809 Langmuir pubs.acs.org/Langmuir Article Figure 3. (a) Emission spectra of DSS-doped PluOS NPs obtained with 50% OS 1−4 and of PluS NPs obtained with TEOS or TMOS as silane precursors. (b) Trends of the emission peak wavelength of DSS-doped PluOS NPs as a function of OS precursor and of its concentration. The emission peak wavelengths of PluS NPs obtained with TEOS or TMOS as silane precursors are marked in gray dashed line for reference. The emission peak wavelengths of DSS dye dissolved in different solvents are marked with colored lines as reference for polarity. Peak wavelengths are obtained with an error <0.5 nm. Figure 4. (a) Average lifetime of RBS-doped PluOS NPs at 0% (only TEOS), 12.5, and 25% OS molar ratios, for nanoparticles obtained using OS1−OS4 as organosilane precursors. (b) Plot of the short (τ1, squares) and long (τ2, circles) components of the phosphorescence decay of RBSdoped PluOS NPs 12.5% (red) and 25% OS molar ratio (black), for nanoparticles obtained using OS1−OS4 as organosilane precursors. In deareated solution (after purging with N2), the decays are monoexponential and close to the τ2 of the corresponding aerated solution (empty circles, red and black for 12.5 and 25% OS molar ratios, respectively). The short lifetime of RBS-doped PluS NPs (only TEOS) is 510 ns and is represented by the gray dashed line. sensitizers for photodynamic therapy. Finally, if chemosensors for molecular oxygen are desired, different oxygen permeation can tune the effective working range for pO2 measurements. We select RBS dye as a dopant of PluOS NPs to shine light on this aspect, due to the dependence of its phosphorescence lifetime on the diffusion of molecular oxygen. Indeed, the quenching rate of its triplet emissive state increases by increasing the concentration and diffusion rate of O2.42,43 Compared to the pure silica network, which forms an almost impenetrable matrix for oxygen, the core−shell organosilica NPs feature a shorter emission lifetime, indicating a higher local concentration and diffusion of molecular oxygen (Figure 4c). The lifetime shortening becomes more evident when the organosilane content of PluOS NPs is higher, highlighting the direct correlation between the presence of an organic counterpart in the organosilica network and the resulting oxygen permeability of the structure. In addition, the most apolar organosilane 4 appears to confer the highest oxygen permeability to the organosilane matrix. This trend is confirmed both when looking at the average lifetime (Figure 4a) or at the shortlifetime component τ1, i.e., the one that reports more accurately on the quenching from O2 (Figure 4b). In addition, the long-lifetime component τ2, which reports on the nonquenched fraction of RBS dyes, is comparable for all PluOS samples, indicating that (i) a fraction of RBS dyes is still not accessible to O2 and that (ii) RBS dyes are not quenched by the PluOS matrix. The observed quenching of RBS dyes is therefore only due to O2 diffusion. A conclusive proof of this statement is provided by the reversibility of the emission lifetime in the absence of O2, removed by purging PluOS NPs solutions with N2: the lifetime becomes monoexponential and matches at approximately 1.1 μs the long component of the decays acquired in the presence of O2, proving that also the quenched RBS dyes can reach the long phosphorescence lifetime of the fraction of RBS dyes which are not reached by 4806 https://doi.org/10.1021/acs.langmuir.0c03531 Langmuir 2021, 37, 4802−4809 Langmuir pubs.acs.org/Langmuir Article the preparation of organosilica matrices with finely tuned polarity, due to the balance between hydrophobic and H-bondrich domains. Silanized derivatives of fluorescent probes for polarity (Dansyl), oxygen permeability (Ru(bpy)32+), and solvating properties (Pyrene) were employed to test the nanoparticle matrices, yielding clear indication of the broad range of chemical nanoenvironments featured by the different organosilica nanoparticles. O2. Emission lifetimes measured for PluOS NPs with 50% OS were considered not reliable, due to the relatively high degree of aggregation that may substantially affect oxygen permeation. Finally, pyrene dyes are very sensitive to local solubility, with ready formation of dimers and excimers in unfavorable conditions that can be sensitively detected owing to their characteristic broad emission band centered at 480 nm.44,45 Emission from excimers is observed when pyrene dyes can come in contact during the lifetime of the excited state, which is possible either for diffusing species at high concentration or for static (nondiffusing) pyrene dyes when they are located very close to one another. In the last case, which is the case of rigid nanoenvironments, excimeric emission greatly depends on two factors: the local concentration of pyrene moieties and the ability of the solvating environment to stabilize the pyrene dyes, keeping them isolated from one another.46,47 We have observed, at a rather constant local pyrene concentration, the appearance of a strong excimeric emission from organosilica NPs containing organosilane OS1 (Figure 5), while pyrene ■ ASSOCIATED CONTENT sı Supporting Information * The Supporting Information is available free of charge at https://pubs.acs.org/doi/10.1021/acs.langmuir.0c03531. Details on synthesis; NMR spectra; characterization methods; photophysical data; additional TEM images; spectra of absorbance, emission, excitation, and emission anisotropy; luminescence decays curves; and fitting results (PDF) ■ AUTHOR INFORMATION Corresponding Author Damiano Genovese − Dipartimento di Chimica “Giacomo Ciamician”, Università di Bologna, 40126 Bologna, Italy; orcid.org/0000-0002-4389-7247; Email: damiano.genovese2@unibo.it Authors Cristina De La Encarnacion Bermudez − Dipartimento di Chimica “Giacomo Ciamician”, Università di Bologna, 40126 Bologna, Italy Elahe Haddadi − Dipartimento di Chimica “Giacomo Ciamician”, Università di Bologna, 40126 Bologna, Italy; Department of Chemistry, College of Sciences, Shiraz University, Shiraz 71454, Iran Enrico Rampazzo − Dipartimento di Chimica “Giacomo Ciamician”, Università di Bologna, 40126 Bologna, Italy Luca Petrizza − Dipartimento di Chimica “Giacomo Ciamician”, Università di Bologna, 40126 Bologna, Italy Luca Prodi − Dipartimento di Chimica “Giacomo Ciamician”, Università di Bologna, 40126 Bologna, Italy; orcid.org/ 0000-0002-1630-8291 Complete contact information is available at: https://pubs.acs.org/10.1021/acs.langmuir.0c03531 Figure 5. (a) Normalized emission spectra of PYS-doped PluOS NPs at increasing concentration of OS1. (b) Normalized emission spectra of PYS-doped PluOS NPs prepared with 25% organosilanes OS1−4. Normalized emission spectrum of PYS-doped PluS NPs (prepared only with TEOS, blue line) is shown for comparison. Note that emission spectra in the presence of organosilane 3 (green spectra) are relative to residual emission due to heavy quenching from the PluOS matrix (PLQY = 0.025). results quenched in formulations containing organosilane 3 (in which residual excimeric emission can be observed), possibly due to an electronic interaction with the N-phenyl units (Table 1). From these observations, we can conclude that the urea groups play the most relevant role in destabilizing the pyrene dyes, resulting in the observation of excimer-like emission, while pure silica (formed by TEOS) and organosilica with bulkier organic moieties provide a favorable environment to separate the pyrene dyes from one another. Author Contributions C.E.B and E.H. contributed equally to the work. The manuscript was written through the contributions of all authors. All authors have approved the final version of the manuscript. Funding D.G. and L.P. are grateful to the Università di Bologna ( AL M A I D E A g r a n t ) an d M I U R ( P R I N P r o j ec t 2017EKCS35), respectively, for funding. C.E.B. acknowledges the Erasmus+ fellowship. CONCLUSIONS In conclusion, a new synthetic route is investigated that broadens the potential of the Pluronic-silica (PluS) nanoparticle preparation technique. Organosilane precursors are used to prepare core−shell organosilica nanoparticles PluOS with homogeneous morphology (10−15 nm core size, 20−50 nm hydrodynamic diameter) but with cores featuring different chemical environments. A click reaction among cost-effective reagents such as diamines and an isocyanate silane derivative is here proven useful to synthesize a broad set of precursors for ■ Notes The authors declare no competing financial interest. ABBREVIATIONS USED OS, organosilane; NP, nanoparticle; PluS, pluronic-silica; PluOS, pluronic-organosilica; PLQY, photoluminescence quantum yield; TEOS, tetraethoxysilane; TMOS, tetramethoxysilane; TMSCl, trimethylsylilchloride ■ 4807 https://doi.org/10.1021/acs.langmuir.0c03531 Langmuir 2021, 37, 4802−4809 Langmuir ■ pubs.acs.org/Langmuir Article Extending the Frontiers of Brightness. Angew. Chem., Int. Ed. 2011, 50, 4056−4066. (21) Rampazzo, E.; Voltan, R.; Petrizza, L.; Zaccheroni, N.; Prodi, L.; Casciano, F.; Zauli, G.; Secchiero, P. Proper Design of Silica Nanoparticles Combines High Brightness, Lack of Cytotoxicity and Efficient Cell Endocytosis. Nanoscale 2013, 5, 7897−7905. (22) Rahmani, S.; Akrout, A.; Budimir, J.; Aggad, D.; Daurat, M.; Godefroy, A.; Nguyen, C.; Largot, H.; Gary-Bobo, M.; Raehm, L.; et al. Hollow Organosilica Nanoparticles for Drug Delivery. ChemistrySelect 2018, 3, 10439−10442. (23) Kalantari, M.; Yu, M.; Jambhrunkar, M.; Liu, Y.; Yang, Y.; Huang, X.; Yu, C. Designed Synthesis of Organosilica Nanoparticles for Enzymatic Biodiesel Production. Mater. Chem. Front. 2018, 2, 1334−1342. (24) Koike, N.; Ikuno, T.; Okubo, T.; Shimojima, A. Synthesis of Monodisperse Organosilica Nanoparticles with Hollow Interiors and Porous Shells Using Silica Nanospheres as Templates. Chem. Commun. 2013, 49, 4998−5000. (25) Brasola, E.; Mancin, F.; Rampazzo, E.; Tecilla, P.; Tonellato, U. A Fluorescence Nanosensor for Cu2+ on Silica Particles. Chem. Commun. 2003, 24, 3026−3027. (26) Rampazzo, E.; Bonacchi, S.; Montalti, M.; Prodi, L.; Zaccheroni, N. Self-Organizing Core−Shell Nanostructures: Spontaneous Accumulation of Dye in the Core of Doped Silica Nanoparticles. J. Am. Chem. Soc. 2007, 129, 14251−14256. (27) Zanarini, S.; Rampazzo, E.; Ciana, L. D.; Marcaccio, M.; Marzocchi, E.; Montalti, M.; Paolucci, F.; Prodi, L. Ru(Bpy)3 Covalently Doped Silica Nanoparticles as Multicenter Tunable Structures for Electrochemiluminescence Amplification. J. Am. Chem. Soc. 2009, 131, 2260−2267. (28) Genovese, D.; Rampazzo, E.; Bonacchi, S.; Montalti, M.; Zaccheroni, N.; Prodi, L. Energy Transfer Processes in Dye-Doped Nanostructures Yield Cooperative and Versatile Fluorescent Probes. Nanoscale 2014, 6, 3022−3036. (29) Genovese, D.; Bonacchi, S.; Juris, R.; Montalti, M.; Prodi, L.; Rampazzo, E.; Zaccheroni, N. Prevention of Self-Quenching in Fluorescent Silica Nanoparticles by Efficient Energy Transfer. Angew. Chem., Int. Ed. 2013, 52, 5965−5968. (30) Rohani, S.; Mohammadi Ziarani, G.; Badiei, A.; Ziarati, A.; Jafari, M.; Shayesteh, A. Palladium-Anchored Multidentate SBA-15/ Di-Urea Nanoreactor: A Highly Active Catalyst for Suzuki Coupling Reaction. Appl. Organomet. Chem. 2018, 32, No. e4397. (31) Baghery, S.; Zolfigol, M. A.; Schirhagl, R.; Hasani, M.; Stuart, M. C. A.; Nagl, A. Synthesis of Novel Magnetic Nanoparticles with Urea or Urethane Moieties: Applications as Catalysts in the Strecker Synthesis of α-Aminonitriles. Appl. Organomet. Chem. 2017, 31, No. e3883. (32) Parambadath, S.; Rana, V. K.; Zhao, D.; Ha, C. S. N,N′Diureylenepiperazine-Bridged Periodic Mesoporous Organosilica for Controlled Drug Delivery. Microporous Mesoporous Mater. 2011, 141, 94−101. (33) Suratwala, T. I.; Hanna, M. L.; Miller, E. L.; Whitman, P. K.; Thomas, I. M.; Ehrmann, P. R.; Maxwell, R. S.; Burnham, A. K. Surface Chemistry and Trimethylsilyl Functionalization of Stöber Silica Sols. J. Non-Cryst. Solids 2003, 316, 349−363. (34) Rampazzo, E.; Bonacchi, S.; Juris, R.; Montalti, M.; Genovese, D.; Zaccheroni, N.; Prodi, L.; Rambaldi, D. C.; Zattoni, A.; Reschiglian, P. Energy Transfer from Silica Core-Surfactant Shell Nanoparticles to Hosted Molecular Fluorophores. J. Phys. Chem. B 2010, 114, 14605−14613. (35) Rottman, C.; Grader, G.; Avnir, D. Polarities of Sol-GelDerived Ormosils and of Their Interfaces with Solvents. Chem. Mater. 2001, 13, 3631−3634. (36) Palomba, F.; Genovese, D.; Petrizza, L.; Rampazzo, E.; Zaccheroni, N.; Prodi, L. Mapping Heterogeneous Polarity in Multicompartment Nanoparticles. Sci. Rep. 2018, 8, No. 17095. (37) Krasnowska, E. K.; Gratton, E.; Parasassi, T. Prodan as a Membrane Surface Fluorescence Probe: Partitioning between Water and Phospholipid Phases. Biophys. J. 1998, 74, 1984−1993. REFERENCES (1) Pan, D. Theranostic Nanomedicine with Functional Nanoarchitecture. Mol. Pharmaceutics 2013, 10, 781−782. (2) Saleh, Y. E.; Gepreel, M. A.; Allam, N. K. Functional Nanoarchitectures For Enhanced Drug Eluting Stents. Sci. Rep. 2017, 7, No. 40291. (3) Kim, J.; Young, C.; Lee, J.; Heo, Y.-U.; Park, M.-S.; Hossain, M. S. A.; Yamauchi, Y.; Kim, J. H. Nanoarchitecture of MOF-Derived Nanoporous Functional Composites for Hybrid Supercapacitors. J. Mater. Chem. A 2017, 5, 15065−15072. (4) Moyano, D. F.; Rotello, V. M. Nano Meets Biology: Structure and Function at the Nanoparticle Interface. Langmuir 2011, 27, 10376−10385. (5) Guleria, A.; Meher, M. K.; Prasad, N.; Poluri, K. M.; Kumar, D. Physicochemical Transformations of ZnO Nanoparticles Dispersed in Peritoneal Dialysis Fluid: Insights into Nano−Bio Interface Interactions. J. Phys. Chem. C 2017, 121, 18598−18607. (6) Wilder, L. M.; Fies, W. A.; Rabin, C.; Webb, L. J.; Crooks, R. M. Conjugation of an α-Helical Peptide to the Surface of Gold Nanoparticles. Langmuir 2019, 35, 3363−3371. (7) Rautio, J.; Meanwell, N. A.; Di, L.; Hageman, M. J. The Expanding Role of Prodrugs in Contemporary Drug Design and Development. Nat. Rev. Drug Discovery 2018, 17, 559−587. (8) Sun, Q.; Barz, M.; De Geest, B. G.; Diken, M.; Hennink, W. E.; Kiessling, F.; Lammers, T.; Shi, Y. Nanomedicine and Macroscale Materials in Immuno-Oncology. Chem. Soc. Rev. 2019, 48, 351−381. (9) Cabral, H.; Miyata, K.; Osada, K.; Kataoka, K. Block Copolymer Micelles in Nanomedicine Applications. Chem. Rev. 2018, 118, 6844− 6892. (10) Rahmani, S.; Akrout, A.; Budimir, J.; Aggad, D.; Daurat, M.; Godefroy, A.; Nguyen, C.; Largot, H.; Gary-Bobo, M.; Raehm, L.; et al. Hollow Organosilica Nanoparticles for Drug Delivery. ChemistrySelect 2018, 3, 10439−10442. (11) Lin, C.-W.; Lu, K. Y.; Wang, S. Y.; Sung, H. W.; Mi, F. L. CD44-Specific Nanoparticles for Redox-Triggered Reactive Oxygen Species Production and Doxorubicin Release. Acta Biomater. 2016, 35, 280−292. (12) Nichols, J. W.; Bae, Y. H. Odyssey of a Cancer Nanoparticle: From Injection Site to Site of Action. Nano Today 2012, 7, 606−618. (13) Soster, M.; Juris, R.; Bonacchi, S.; Genovese, D.; Montalti, M.; Rampazzo, E.; Zaccheroni, N.; Garagnani, P.; Bussolino, F.; Prodi, L.; et al. Targeted Dual-Color Silica Nanoparticles Provide Univocal Identification of Micrometastases in Preclinical Models of Colorectal Cancer. Int. J. Nanomed. 2012, 7, 4797−4807. (14) Helle, M.; Rampazzo, E.; Monchanin, M.; Marchal, F.; Guillemin, F.; Bonacchi, S.; Salis, F.; Prodi, L.; Bezdetnaya, L. Surface Chemistry Architecture of Silica Nanoparticles Determine the Efficiency of in Vivo Fluorescence Lymph Node Mapping. ACS Nano 2013, 7, 8645−8657. (15) Guimarães, R. S.; Rodrigues, C. F.; Moreira, A. F.; Correia, I. J. Overview of Stimuli-Responsive Mesoporous Organosilica Nanocarriers for Drug Delivery. Pharmacol. Res. 2020, 155, No. 104742. (16) Yu, L.; Chen, Y.; Lin, H.; Du, W.; Chen, H.; Shi, J. Ultrasmall Mesoporous Organosilica Nanoparticles: Morphology Modulations and Redox-Responsive Biodegradability for Tumor-Specific Drug Delivery. Biomaterials 2018, 161, 292−305. (17) Li, J.-L.; Cheng, Y.-J.; Zhang, C.; Cheng, H.; Feng, J.; Zhuo, R.X.; Zeng, X.; Zhang, X.-Z. Dual Drug Delivery System Based on Biodegradable Organosilica Core−Shell Architectures. ACS Appl. Mater. Interfaces 2018, 10, 5287−5295. (18) Chakraborty, A.; Dalal, C.; Jana, N. R. Colloidal Nanobioconjugate with Complementary Surface Chemistry for Cellular and Subcellular Targeting. Langmuir 2018, 34, 13461−13471. (19) De Crozals, G.; Bonnet, R.; Farre, C.; Chaix, C. Nanoparticles with Multiple Properties for Biomedical Applications: A Strategic Guide. Nano Today 2016, 11, 435−463. (20) Bonacchi, S.; Genovese, D.; Juris, R.; Montalti, M.; Prodi, L.; Rampazzo, E.; Zaccheroni, N. Luminescent Silica Nanoparticles: 4808 https://doi.org/10.1021/acs.langmuir.0c03531 Langmuir 2021, 37, 4802−4809 Langmuir pubs.acs.org/Langmuir Article (38) Nizri, G.; Magdassi, S. Solubilization of Hydrophobic Molecules in Nanoparticles Formed by Polymer-Surfactant Interactions. J. Colloid Interface Sci. 2005, 291, 169−174. (39) Messaggi, F.; Ruggeri, I.; Genovese, D.; Zaccheroni, N.; Arbizzani, C.; Soavi, F. Oxygen Redox Reaction in Lithium-Based Electrolytes: From Salt-in-Solvent to Solvent-in-Salt. Electrochim. Acta 2017, 245, 296−302. (40) Barrett, S. M.; Wang, C.; Lin, W. Oxygen Sensing via Phosphorescence Quenching of Doped Metal−Organic Frameworks. J. Mater. Chem. 2012, 22, 10329−10334. (41) Klymchenko, A. S.; Duportail, G.; Demchenko, A. P.; Mély, Y. Bimodal Distribution and Fluorescence Response of EnvironmentSensitive Probes in Lipid Bilayers. Biophys. J. 2004, 86, 2929−2941. (42) Ji, S.; Wu, W.; Wu, W.; Song, P.; Han, K.; Wang, Z.; Liu, S.; Guo, H.; Zhao, J. Tuning the Luminescence Lifetimes of Ruthenium(Ii) Polypyridine Complexes and Its Application in Luminescent Oxygen Sensing. J. Mater. Chem. 2010, 20, 1953−1963. (43) Morris, K. J.; Roach, M. S.; Xu, W.; Demas, J. N.; DeGraff, B. A. Luminescence Lifetime Standards for the Nanosecond to Microsecond Range and Oxygen Quenching of Ruthenium(II) Complexes. Anal. Chem. 2007, 79, 9310−9314. (44) Masseroni, D.; Biavardi, E.; Genovese, D.; Rampazzo, E.; Prodi, L.; Dalcanale, E. A Fluorescent Probe for Ecstasy. Chem. Commun. 2015, 51, 12799−12802. (45) Prado, E. A.; Yamaki, S. B.; Atvars, T. D. Z.; Zimerman, O. E.; Weiss, R. G. Static and Dynamic Fluorescence of Pyrene as Probes of Site Polarity and Morphology in Ethylene-Co-(Vinyl Acetate) (Eva) Films. J. Phys. Chem. B 2000, 104, 5905−5914. (46) Avis, P.; Porter, G. Effect of Concentration on the Absorption and Fluorescence Spectra of Pyrene in a Solid Solution of Poly(Methyl Methacrylate). J. Chem. Soc., Faraday Trans. 2 1974, 70, 1057−1065. (47) Hammarström, P.; Kalman, B.; Jonsson, B.-H.; Carlsson, U. Pyrene Excimer Fluorescence as a Proximity Probe for Investigation of Residual Structure in the Unfolded State of Human Carbonic Anhydrase II. FEBS Lett. 1997, 420, 63−68. 4809 https://doi.org/10.1021/acs.langmuir.0c03531 Langmuir 2021, 37, 4802−4809