Julian
Opel†
ab,
Lisa-Catherine
Rosenbaum†
c,
Julian
Brunner
a,
Anne
Staiger
ac,
Ramon
Zimmermanns
a,
Matthias
Kellermeier
d,
Tanja
Gaich
c,
Helmut
Cölfen
*a and
Juan-Manuel
García-Ruiz
*b
aPhysical Chemistry, University of Konstanz, Universitätsstrasse 10, D-78457 Konstanz, Germany. E-mail: helmut.coelfen@uni-konstanz.de; Fax: +49 7531 88 3139; Tel: +49 7531 88 4063
bLaboratorio de Estudios Cristalográficos, Instituto Andaluz de Ciencias de la Tierra (CSIC-UGR), Avenida de las Palmeras No. 4, E-18100 Armilla, Granada, Spain. E-mail: juanmanuel.garcia@csic.es; Fax: +34 958 552620; Tel: +34 958 230000
cOrganic Chemistry, University of Konstanz, Universitätsstrasse 10, D-78457 Konstanz, Germany. E-mail: Tanja.Gaich@uni-konstanz.de
dMaterial Physics, BASF SE, GMC/O – G201, Carl-Bosch-Strasse 38, D-67056 Ludwigshafen, Germany. E-mail: matthias.kellermeier@basf.com; Fax: +49 621 66 43388; Tel: +49 621 60 43388
First published on 20th May 2020
Microcarriers with the ability to release and catch substances are highly desired metamaterials and difficult to obtain. Herein, we report a straightforward strategy to synthesize these materials by combining silica-biomorphs with mesocrystals. An easy access to microcarrier hulls with covalently bound spiropyrans as light-switchable anchor points is presented.
Fig. 1 Scanning electron micrographs of a biomorph worm (left) and a biomorph helix (right) decorated with magnetite mesocrystals (highlighted in red) at the globular apex of the structures. |
In order to create further functionality, the structures must be equipped with an additional responding unit that allows addressing of a switchable anchor point for controlled compound load/release. Previous studies employed post-functionalization by the use of silane coupling chemistry.9,15
The incorporation of light-switchable molecules into various systems and the development of so-called dynamic materials came into the focus of attention during the last decades. Not only the synthesis of materials for data storage,16 electronic devices17 or sensors18 but also the biological applications of photo-responsive compounds, e.g. in photopharmacology,19–21 have been investigated. Photo-switchable molecules show reversible transformation between at least two different thermodynamically stable isomers induced by irradiation with light of a particular wavelength. Among the wide range of photo-switches, spiropyrans achieved a privileged status since they enable the production of materials that are responsive to multiple external stimuli in an orthogonal fashion. The two isomeric structures of a spiropyran show vastly different properties, which results in an isomerization process that is not only induced by irradiation with light but also by several other external stimuli including temperature, solvent and pH-value.22 In addition, the covalent attachment of spiropyran units to a solid support results in numerous advantages compared to the non-immobilized counterparts, including an improved fatigue resistance,23,24 and the possibility to obtain biocompatible photoresponsive materials.25,26
The incorporation of silane-containing switchable molecules like spiropyrans is a desired method to obtain new metamaterials.22,27
The typical structural formula of a spiroindolinopyran (SP) is shown in Fig. 2, consisting of an indoline and a chromene moiety, which are connected via a spiro-center. The isomeric merocyanine (MC) is accessible by heterolytic cleavage of the Cspiro–O bond induced by irradiation with UV-light. The population of the excited state is followed by an intersystem crossing process to the corresponding triplet state in which the ring opening takes place.28 Internal rotation in the ground state to the cis- and trans-isomers is in most cases followed by a thermal isomerization to the trans-isomer. The open-ring isomer exists as either zwitterionic (2) or quinoidal species (3).
Merocyanine often shows strong fluorescence and exhibits a remarkably higher affinity to different chemical structures,29 a property that is caused by the additional free oxygen acting as a donor function. The zwitterionic merocyanine has already been described as a ligand for (divalent) metal ions30–32 whereas the neutral spiropyran is a rather unfavorable donor. Utilizing the huge differences in the properties of the isomers, multi-fluorescent hybrid particles,33 traps for ions34 and small molecules35 are prepared, the hydrophobicity of solid surfaces36 can be tuned reversibly, and the electrochemical properties of a surface37 are controlled. Reverse isomerization to the initial spiro-compound is possible by either thermal relaxation or irradiation with visible light. These properties made the spiropyran–merocyanine system to be the focus of our interest with regard to the design of a magnetized biomorphic microcarrier system.
1H-NMR (400 MHz, DMSO): δ [ppm] = 12.24 (bs, 1H), 8.24 (d, 3JHH = 2.8 Hz, 1H), 8.03 (dd, 3JHH = 2.8′, 9.0 Hz, 1H), 7.24 (d, 3JHH = 10.3 Hz, 1H), 7.17–7.13 (m, 2H), 6.88 (d, 3JHH = 9.0 Hz, 1H), 6.83 (t, 3JHH = 7.5 Hz, 1H), 6.69 (d, 3JHH = 7.8 Hz, 1H), 6.03 (d, 3JHH = 10.3 Hz, 1H), 3.57–3.39 (m, 2H), 2.64–2.44 (m, 2H), 1.21 (s, 3H), 1.10 (s, 3H).
1H-NMR (400 MHz, DMSO): δ [ppm] = 8.20 (d, 3JHH = 2.8 Hz, 1H), 7.99 (dd, 3JHH = 2.8, 8.9 Hz, 1H), 7.86 (t, 3JHH = 5.5 Hz, 1H), 7.18 (d, 3JHH = 10.4 Hz, 1H), 7.14–7.09 (m, 2H), 6.85 (d, 3JHH = 9.0 Hz, 1H), 6.78 (dt, 3JHH = 7.4, 0.6 Hz, 1H), 6.65 (d, 3JHH = 7.7 Hz, 1H), 5.97 (d, 3JHH = 10.4 Hz, 1H), 3.70 (q, 3JHH = 7.0Hz, 6H), 3.49–3.29 (m, 2H), 3.01–2.87 (m, 2H), 2.43–2.27 (m, 2H), 1.41–1.33 (m, 2H), 1.18 (s, 3H), 1.12 (t, 3JHH = 7.0 Hz, 9H), 1.07 (s, 3H), 0.49–0.45 (m, 2H).
13C-NMR (101 MHz, DMSO): δ [ppm] = 170.1, 159.2, 146.4, 140.5, 135.6, 127.9, 127.5, 125.6, 122.7, 121.9, 121.6, 119.1, 118.9, 115.4, 106.7, 106.6, 57.6, 52.4, 41.3, 39.5, 34.9, 25.5, 22.7, 19.4, 18.2, 7.4.
IR (ATR): ṽ [cm−1] = 3307, 2973, 2928, 1740, 1639, 1611, 1511, 1479, 1334, 1273, 1075, 951, 919, 808, 787, 748.
HRMS: m/z calculated for C30H42N3O7Si+: 584.2787; found: 584.2785.
Silica-biomorphs were precipitated from barium-containing alkaline silica sol through continued CO2 diffusion into the sol. The structures remained in the mother sol for 16 h to reach the secondary precipitation stage, where an outer silica shell and additional witherite attach to the structures.9 A thicker silica layer around the structures is desirable to improve the stability once the inner core dissolves for an improved carrier capacity of the MCBCs. Selective secondary precipitation of witherite crystals around the tips of the structures is desired to induce the heterogeneous magnetite mesocrystal formation. The obtained solid from the biomorph synthesis was rinsed several times with deionized water and dried. The biomorph powder mainly consisted of worm-like braids and helicoidal structures, decorated with witherite crystals on the former globular tips of the biomorphs. The structures were transferred into a magnetite nanocube solution in THF containing a certain amount of oleic acid. The biomorphs act as substrates for the mesocrystal formation. Mesocrystals were formed through gas phase diffusion of the anti-solvent (ethanol) into the magnetite nanocube solution. The particle and the oleic acid concentrations were accurately chosen in order to generate mesocrystals in the range of the tip size (cf.Fig. 1). The decreased nanocube concentration leads to smaller mesocrystals and a lower total magnetite loading of the structures. The result is a different responding behaviour in the magnetic field. The decreased oleic acid concentration results in an increased number of smaller mesocrystals. The total magnetite loading remained constant.9 The obtained MCBCs allow a further post-functionalization treatment with synthesized compound 7 by incubation of the structures in a 1 wt% solution in ethanol/water (95:5) for several hours. The generated functionalized silica layer can be seen in Fig. 3B as a blue layer in the SP form. The UV-irradiation of the material induces the spiro-compound to switch to the MC form, which is indicated by the glowing green colored layer (Fig. 3B). As previously mentioned in the literature, the vastly different properties of the two isomers can be further used for selective catch and release of compounds.27
To prove the postulated scheme of the formation of light switchable MCBCs, laser scanning microscopy (LSM) was used. A selective switching of the SP by using the bleach mode was induced with a different wavelength. Therefore, the excitation and emission spectra of compound 7 were recorded and are shown in Fig. 4A. The black spectrum shows the excitation spectrum of the SP-form detecting the intensity of fluorescence at 625 nm while the excitation wavelength changes. The spectrum has a maximum at 555 nm and a shoulder at 520 nm. In addition, several emission spectra were recorded to elaborate the obtained fluorescence as the subject of the excitation wavelength. Using an excitation wavelength of 555 nm, the highest fluorescence intensity was obtained (green spectrum), while an excitation wavelength of 490 nm exhibited lower fluorescence yields (blue spectrum). Nevertheless, the excitation wavelength of 490 nm is the most important result due to the equipped analysing lasers on the LSM. For the fluorescence experiments on the LSM, the imaging was performed with a 488 nm laser (1% laser power, pin hole: 1 a.u.). Imaging the structures with visible light continuously decreased the obtained fluorescence. The degradation of fluorescence is worse with the 555 nm laser, which was additionally chosen in other experiments to turn off the fluorescence while switching the MC back to the SP form. To generate a high amount of fluorescent MCs on the surface, the structures were “bleached” in a region of interest (ROI) with a 405 nm laser (20% laser power, 4 scans). The result is shown in Fig. 4B. The bleaching of the ROI occurred after the first and every third following cycle, indicated by the bluish bars. The measured data originated from a programmed times series. A continuous decrease of the fluorescence intensity in the 3 steps after excitation to a level lower than before the bleaching explains the ongoing decrease of the overall fluorescence intensity. The effect becomes even clearer by considering several cycles. An example is shown in Fig. 4C, where 72 cycles are recorded in the same area. To visualize this effect, Fig. 4D shows a functionalized MCBC in its OFF state, before the frame was illuminated with 405 nm light. Fig. 4E shows the activated structure after excitation. It has to be mentioned that the pictures show a lower end of a functionalized biomorph worm, and the lowest part is in focus. The pin hole cuts off the fluorescent light emitted from the upper part, allowing for an improved image quality and spatial resolution. Therefore, LSM seems to be an appropriate method to prove the incorporation of the functional silane on the structures. This has also been shown in previous studies15 and demonstrates the suitability of spiropyrans as switchable anchor points on biomorph-based microcarriers.
Footnote |
† JO and LCR wrote the paper and have contributed equally to the work. |
This journal is © The Royal Society of Chemistry 2020 |