A.
Martinez-Cuezva
,
S.
Valero-Moya
,
M.
Alajarin
and
J.
Berna
*
Departamento de Química Orgánica, Facultad de Química, Regional Campus of International Excellence “Campus Mare Nostrum”, Universidad de Murcia, E-30100, Murcia, Spain. E-mail: ppberna@um.es
First published on 6th August 2015
Novel mechanized silica nanoparticles incorporating a peptide-based molecular shuttle as a photo-responsive interlocked gatekeeper of nanocontainers are described including the uptake and delivery studies of a model cargo.
Among the [2]rotaxanes containing a benzylic amide macrocycle pioneered by Leigh,7b–e the subset of the peptide-based structures14–17 are considered excellent scaffolds for the building of a broad range of molecular shuttles,14 logic gates,15 information storage devices16 and enzymatic delivery systems of bioactive compounds.17
Herein, we describe the preparation of novel mechanized silica nanoparticles having a peptide-based molecular shuttle as a photocontrollable gatekeeper and MCM-41 as a mesoporous support aimed at the construction of light-operated nanocontainers. The loading and delivery of rhodamine B (RhB) as a model cargo through the mechanism depicted in Fig. 1 have also been reported.
![]() | ||
Fig. 1 (a) Uptake and release of dye cargo molecules (RhB) from the pores of a MCM-41 silica functionalized with a light-responsive peptide [2]rotaxane. The movable lid is a tetralactame which locates on the preferred station (fumaramide, red cylinder, or peptide, green cylinder) depending on its affinity order. (b) Relative distance of the silicon atom to the first HB acceptor of the stations that are connected by the thread, illustrating the feasibility of the RhB loading. Cross dimensions (in nm) of the sealing tetralactame (blue ring) and the RhB cargo molecule (purple block) showing up the size matching with the average diameter (ca. 2 nm) of nanopores of the silica support. Molecular modeling structures of the macrocycle and the RhB cation are shown. Distances values were obtained from the CCDC database (see ref. 20). |
Our system is based on the light-induced E/Z isomerization of a fumaramide-based binding site for shuttling the macrocycle along the thread of a bistable [2]rotaxane18 thus closing and opening a molecular gate on the surface of a mesoporous silica support. We placed a peptide station (green cylinder, Fig. 1a) near the silica surface and connected to a fumaramide station (red cylinder) by an alkyl chain. In the open-pore state, the tetralactame ring is located on the fumaramide station allowing the free diffusion of the cargo RhB molecules (purple blocks) toward the void of the pores. The photoisomerization of the olefin affording the maleamide derivative (pink cylinder) alters the binding affinity of the unsaturated station by several kilocalories per mole19 and promotes the ring translocation towards the peptide-based binding site for entrapping the cargo (Fig. 1a). A cis-to-trans olefin isomerization shuttles back the ring to the fumaramide station, thus opening the pores for enabling the release of the RhB molecules and allowing the reusability of these nanocontainers.
The matching of the porous mesostructure of the silica nanoparticles (ca. 100–200 nm diameter) containing hexagonally arranged pores (ca. 2 nm diameter) and the relative sizes20 of the model cargo (RhB: 1.0 × 1.5 nm) and the ring (benzylic tetralactame: 0.8 × 1.7 nm) supports the ability of the latter for keeping the cargo molecules inside the pores (Fig. 1b). In addition, the relative distance of each station of the [2]rotaxane with respect to the porous surface regulates the position of the moveable lid and, consequently, it determines the limiting cross-dimensions of the loading cargo molecules to be longer than 0.7 nm but shorter than 2.7 nm.
Tetraethylorthosilicate as the silicon source and cetyltrimethylammonium bromide (CTAB) as the template were used in a base-catalyzed sol–gel protocol21 for affording the mesostructured silica of the MCM-41 type (MSN-1). The size and the mesoporous structure of the nanoparticles were studied by scanning electron and transmission electron microscopy, respectively (see Fig. S1a and b, ESI†).
The final MSN-E-6 system was assembled in a stepwise synthesis from the thermoactivated22 silica nanoparticles (Scheme 1). First, the spherical surface of MSN-1 was functionalized with nitrile functions affording MSN-2 by heating with 2-cyanoethyltriethoxysilane in toluene. Further refluxing with 50% sulfuric acid provided the surface-bound carboxylic acid MSN-3. Next, amide bond formation between the carboxy groups of MSN-3 with the glycylglycine building block S1 (see the ESI†) in the presence of N,N-dicyclohexylcarbodiimide afforded the corresponding phthalimide-functionalized particles MSN-4. Subsequent hydrazinolysis23 of the preceding silica provided the amino-functionalized MSN-5 which was completely separated from the phthalhydrazide byproduct by continuous extraction in a Soxhlet apparatus with hot ethanol. Finally, the nucleophilic substitution of the bulky 2,6-diphenyl-4-nitrophenoxy stopper17a of the fumaramide rotaxane S2 (see the ESI†) by the amino groups of the latter silica particles yielded the target MSN-E-6 with a surface gated with a two-station peptide [2]rotaxane (Scheme 1).
![]() | ||
Scheme 1 Synthesis of the mesoporous silica nanoparticles MSN-E-6 functionalized with a photocontrollable peptide [2]rotaxane. |
Non-mechanized nanoparticles MSN-7 bearing an identical linear fragment to that of MSN-E-6 were also prepared according to the synthetic route outlined in Scheme 2. In this regard, the amine 2 was prepared through a two consecutive amide coupling-Boc deprotection protocol for incorporating the fumaramide and peptide binding sites tethered by a dodecyl alkyl chain. Next, the carbodiimide-mediated amide formation between the acid-terminated surface of MSN-3 and the amine 2 led to silica nanoparticles MSN-7 which were used as non-threaded model materials, lacking the benzylic amide macrocycle.
![]() | ||
Scheme 2 Synthesis of the mesoporous silica nanoparticles MSN-7 functionalized with the two-binding site thread precursor 2. |
The structure determination and characterization of the compounds and materials shown in the Schemes 1 and 2 were accomplished by means of their analytical and spectral data (see the ESI†). Although intense bands of the Si–O–Si stretching and bending vibrations at 1080 and 800 cm−1 are present in the FTIR spectra of all the silica materials shown in these schemes (see Fig. S3 and S4, ESI†) the functional groups incorporated in each stage are also evidenced in these spectra. Thus, the spectrum of MSN-3 shows a weak band at 2953 cm−1 owing to the C–H stretching and a strong one at 1726 cm−1 corresponding to the CO stretching vibration of the carboxy group. At the end of the transformations outlined in Scheme 1, the FTIR spectrum of the interlocked MSN-E-6 shows two intense C
O bands at 1646 and 1540 cm−1 corresponding to the C
O stretching vibrations of the different amido groups of the gatekeeper, also displaying intense bands in the range of 2983 and 2894 cm−1 due to the methylene groups present in this motif. 29Si and 13C cross-polarization magic-angle spinning solid-state (SS) NMR spectroscopies were also used to examine the grafting and attachment of the different organic fragments into MCM-41. The 29Si SSNMR spectrum (see Fig. S5, ESI†) of the silica MSN-2 shows two T signals at −54.8 and −61.9 ppm corresponding to the silicon atoms directly connected to the organic fragments and a Q signal at −109.5 ppm ascribed to the rest of silicon atoms [Si(OSi)n(OH)4−n; n = 2–4]. The measurement of the 13C SSNMR spectrum of each of the new synthesized material confirmed the successive chemical transformations toward the final mechanized silica (see the ESI†). The spectrum of the targeted MSN-E-6 shows several sets of signals at different chemical shift ranges: at 174.1–163.3 ppm appear those corresponding to the carbon atoms of the carbonyl groups of the amide functions, at 144.8–116.4 ppm those of the aromatic carbon atoms and in the region between 70 and 10 ppm come out those of the aliphatic carbon atoms (see Fig. S7, ESI†). The comparison of this 13C SSNMR spectra with the one of the non-interlocked MSN-7 materials displays noticeable differences evidencing the lack of the tetralactame in this latter material (see Fig. S7, ESI†) further proving the functionalization of MSN-E-6. Finally, TGA and elemental analysis showed the rough estimation of the maximum amount of these interlocked motifs on the surface of MSN-E-6 to be approximately 0.30 mmol per gram of silica.
Next the light-responsive gating behavior of MSN-E-6 was investigated. The diffusion of the RhB cargo into the pores of this light-responsive silica was carried out by soaking the mechanized nanoparticles in a stirred aqueous solution of the guest compound for 24 h. The surface-adsorbed excess of the cargo was thoroughly washed and the resulting material was carefully dried. Then the pores of the material were sealed by means of a trans-to-cis photoisomerization of the olefin station14c,18,24 by irradiation at 254 nm promoting the shifting of the tetralactame ring toward the peptide station close to the surface of the nanoparticulate silica. This operation kinetically entraps the guest molecules into the MSN-Z-6 container and, then, the RhB loaded silica is thoroughly washed and dried. Although the accessibility of the cargo to the pores of MSN-1 decreased after its functionalization with the rotaxane, as it was confirmed by the TEM observation (see Fig. S14, ESI†); the openings of the gated material still permitted the entrance of enough RhB for carrying out the study of its controlled release.
The delivery of RhB from the nanopores of MSN-Z-6 was investigated in two different solvents, dichloromethane and water. For closely related interlocked systems18 it is known that the polarity of the solvent affects the position of the ring over the peptide binding site. Thus, whereas in non-disrupting hydrogen bond solvents such as dichloromethane the ring is mainly located on the peptide station, in polar solvents the alkyl chain would act as a second solvophobic station.18 For this purpose, a stirred suspension of RhB-loaded MSN-Z-6 was irradiated at 365 nm for promoting the cis-to-trans isomerization which triggers the ring translocation to the most energetically favorable binding site that, in this case, is the resulting fumaramide station far away from the surface of the nanoparticulate silica. Consequently, this latter irradiation promotes the opening of the pores and the release of RhB, which was monitored by measuring the absorbance spectrum at different times (Fig. 2, inset). The obtained profile for the light-driven opening of the gatekeepers of this silica in dichloromethane shows a progressive delivery of the cargo reaching 50% of the maximum delivery in 50 min and needing 30 min more to reach a liberation of 80% of the cargo (Fig. 2a). Using Beer–Lambert's law, the RhB loading was calculated revealing that, for 3 mg of RhB-loaded MSN-Z-6, 0.175 μmol (2.8 wt%) of the cargo was released (see ESI†).
When the release experiment was carried out in water, the discharge of half the load lasted 200 min and the release profile of the rest is extended for more than 5 h (Fig. 2b). Consequently the remarkable positional integrity of the ring after photoisomerization of the maleamide binding site to its trans isomer promotes the expected release of the cargo in dichloromethane, and less quickly in water due to the decrease of the ring discrimination. At this point it is convenient to remark that slow dynamics release profiles as that shown in Fig. 2b are desirable in therapeutic treatments as they allow a moderated liberation of potent (and/or short half-life) drugs.2,3
It should also be noted that the interlocked nanogates of this container prevent significant premature release of the cargo dye molecules as revealed by the flat region (0–10 min) of the profiles in both solvents (Fig. 2a and b). We also carried out control experiments by monitoring the absorbance of RhB-loaded MSN-Z-6 in the absence of light in both studied solvents (Fig. 2c and d), showing the absence of leaking processes under such conditions. Incidentally, these latter results also give an idea of the positional integrity of the ring over the peptide-based binding site in MSN-Z-6 (see ESI†). Release control experiments with the non-mechanized material RhB-loaded MSN-7 disclosed a quick leaking of the guest molecules into solution confirming the key role of the benzylic amide macrocycle as the interlocked gatekeeper of MSN-6 (see ESI†).
In summary, we have demonstrated the feasibility of building mechanized silica nanoparticles using a peptide-based molecular shuttle and MCM-41 as a mesoporous support. We have shown the efficiency of this particular functionalization in actuating as gatekeepers upon exposure to visible light irradiation displaying different dosages depending on the working conditions. The unprecedented integration of a benzylic tetralactame as a movable lid allows a proficient uptake and release of RhB employed as the model cargo. This mechanized material must be included in the yet scarce number of described light-operated molecular nanovalves and opens stimulating opportunities for the development of a novel generation of smart nanocontainers by anchoring amide-based interlocked compounds, which could be used as controlled delivery systems.
This work was supported by the MINECO (CTQ2009-12216/BQU and CTQ2014-56887-P) and the Fundacion Seneca-CARM (Project 19240/PI/14). A.M.-C. thanks the Marie Curie COFUND/U-IMPACT programs and the MINECO for postdoctoral contracts. We also thank Prof. José M. González and Dr Almudena Torres of the National Center for Electron Microscopy (UCM, Madrid) for their helpful assistance with the TEM observations.
Footnote |
† Electronic supplementary information (ESI) available: Synthetic procedures, experimental details and characterization. See DOI: 10.1039/c5cc04365d |
This journal is © The Royal Society of Chemistry 2015 |