Magnetic Nanoparticles Coated with (R)-9-Acetoxystearic Acid for Biomedical Applications.

The well-known ability to selectively drive nanomagnetic materials coated with anticancer drugs into tumor cells suggested the synthesis and the characterization of magnetic nanoparticles (MNPs) functionalized with (R)-9-acetoxystearic acid, the acetic ester of (R)-9-hydroxystearic acid (9-HSA), an antiproliferative agent active against different cancer cells. The acyl chloride of (R)-9-acetoxystearic acid, synthesized in two steps from 9-HSA, was reacted with (3-aminopropyl)triethoxysilane, chosen as a linker between MNPs and the stearyl moiety. In the last step, the novel amide was bound to magnetite NPs by reaction with silyl groups. A detailed structural, chemical, and magnetic characterization of the obtained material proved that it possesses properties in agreement with the requirements for drug delivery, opening the possibility to further insights focused on the 9-HSA biomedical applications.

Introduction

The growing interest in magnetic nanoparticles (MNPs) is mainly due to their versatility in a wide number of applicative fields, such as removal of toxic elements from industrial wastes,[1−3] magnetic resonance imaging (MRI) techniques for cancer diagnosis, and cancer therapy.[4−8] Integration of imaging-diagnostic systems based on positron emission tomography (PET) and MRI in a single diagnostic device PET/MRI (up to now the more advanced medical diagnostic instrumentation) moreover requires an effort on advanced material, instrumentation studies, and quality control.[9−12] The main advantage of using MNPs in biomedical field is due to the possibility to guide the drug to the target by means of an external magnetic field. In this context, particular interest is on nanometer-sized particles of iron oxide that allow combination of cancer therapy with their in vivo degradation into non-toxic iron ions.[7] MNPs showing superparamagnetic (SPM) behavior have indeed demonstrated their potential in anticancer drug delivery.[13−18]

Magnetite (Fe3O4) is a promising candidate as drug delivery medium owing to low toxicity and biocompatibility. The preparation of magnetite, aiming the drug release to the target, is a challenging task as different parameters to control are involved, including the size optimization and surface properties. Low toxicity and the capability to reach the target are connected with the MNP dimension. In fact, too small particles with diameter lower than 10 nm are, most of the time, rapidly removed from the body. On the other hand, particles larger than 200 nm are retained by the spleen. The optimal dimension to fulfill the therapy requirements ranges between 10 and 100 nm.[19−22]

The need to control the MNPs by magnetic fields requires that they be in a SPM state. In the range 10–100 nm, the magnetite is often monodomain,[23] so it behaves as a SPM material as a function of temperature, size, and magnetic interactions. For drug delivery, the SPM behavior is significant at room temperature, and this, requires to control dimensions, magnetic interactions, and size distribution of the MNPs. In addition, the functionalization can modify the magnetic behavior. The coating of MNPs with a drug, for example, can decrease particle interactions and agglomeration, modifying SPM behavior in the whole. MNPs can be derivatized by coating the iron oxide core surface with organic or inorganic molecules through a chemical bond thus obtaining magnetically controlled drug carrier for locoregional cancer treatment.

9-Hydroxystearic acid (9-HSA) is an endogenous cellular lipid able to inhibit the cell growth in a series of cancer cell lines. It has been demonstrated that it acts as an inhibitor of HDAC1 activity at micromolar concentrations; in HT29, human colorectal adenocarcinoma cells, the inhibitory effect of 9-HSA is mediated by an arrest in the G0/G1 phase cell cycle.[24,25] Molecular docking studies have shown a favorable formation energy of the HDAC1–9-HSA complex, and the complex with (R)-9-HSA became more stable than that with the opposite enantiomer.[26] This prediction was fulfilled after separately administering of both enantiomers.[27] Despite a clinical advantage, the use of (R)-9-HSA shows some limitations, such as the extremely poor water solubility and the need to administer relatively high doses in order to have a pharmacological effect. Recently, we focused our efforts on the search of efficient delivering modes of (R)-9-HSA, and we were able to load it in biocompatible keratin nanoparticles[28] and to insert it in hydroxyapatite nanocrystals[29,30] for possible applications in bone cancer. Now, in order to find a more general and versatile method to target the action of (R)-9-HSA toward local treatment sites and considering that the anchoring amido group, as well as the ester group, may be “in situ” hydrolyzed by cellular lipases and amidases thus permitting the release of the organic molecule, we planned to coat (R)-9-HSA to MNPs through (3-aminopropyl)triethoxysilane (NH2(CH2)3Si(OC2H5)3 (APTES), known for its ability to combine with biomolecules, drugs, and metals.[31] In the present study, we report the synthesis and a detailed structural, magnetic, and chemical characterization of this novel material.

Results and Discussion

Magnetite Nanoparticles Preparation and Functionalization

The synthetic strategy designed to functionalize magnetite nanoparticles with (R)-9-HSA implied his connection to APTES through an amide bond, followed by the anchoring to magnetite exploiting the reaction between the silyl group of the obtained amide and the magnetite hydroxy groups. A well-known and efficient synthetic route to amides is the reaction between an amine and an acyl chloride; in current case, taking into account the presence, on the (R)-9-HSA, of a hydroxy- and a carboxy-functionality, the hydroxy group needed to be protected prior the formation of the acyl chloride, to avoid the occurrence of undesired reactions. The synthetic sequence is shown in Scheme .

Scheme 1

Synthesis of Amide 4 from APTES and (R) 9-Hydroxystearic Acid

(R)-9-HSA (1) was enzymatically transformed into (R)-9-acetyl-HSA (2) and then treated with oxalyl chloride to produce the corresponding acyl chloride 3. The latter was reacted with APTES under Schotten–Baumann type conditions[32] to give the amide 4. The reactions (and related work-up procedures) of the second and third step (shown in Scheme ) have been carried out under inert atmosphere, to avoid hydrolysis, and compounds 3 and 4 were used without purification.

It has to be noted that the usually reported way to coat MNPs with an organic moiety through APTES bridge is realized by reacting MNPs with APTES and then by linking the organic moiety to the amino group of APTES-coated MNPs. In the current case, we first prepared the amide 4 between APTES and (R)-9-acetoxystearic acid by monitoring the reaction course through 1H NMR spectroscopy (Supporting Information file, Figures S1–S6). Once the reaction resulted to be complete, we reacted the crude 4 with magnetite nanoparticles (B-magnetite), in turn prepared via co-precipitation of iron sulphate salts in basic media.[33] The material was washed with anhydrous toluene to remove the eventually unreacted organic compound 4. The functionalization of magnetite nanoparticles with compound 4 must be carried out under strictly anhydrous conditions to avoid secondary hydrolysis of 4 by traces of water prior its bonding with magnetite nanoparticles with consequent formation of undesired byproducts. For this reason, we chose anhydrous toluene as solvent because other possible polar non protic solvents, such as DMSO or DMF, are afflicted by high hygroscopicity and/or high boiling point that make their complete removal difficult.

The IR spectrum of the novel final material was compared with that of B-magnetite (see spectra in Supporting Information, Figure S7) and showed bands at 2927.7 cm–1 because of aliphatic CH bonds, 1735.2 and 1031.7 cm–1 belonging to the ester group, and 1659.8 cm–1, typical of the amide group, thus confirming the successful derivatization with the organic compound 4. The novel material was indicated as MAGOR (Scheme ).

Scheme 2

Sketch of the Procedure Adopted in Current Work for the Synthesis of MAGOR

X-ray Diffraction Measurements

The X-ray diffraction (XRD) patterns of B-magnetite and MAGOR are reported in Figure . In particular, diffraction peaks of Figure a can be attributed to the magnetite (Fe3O4) phase (“International Centre for Diffraction Data”—ICDD card no. 19-0629); but because of very similar XRD patterns, the presence of the maghemite (γ-Fe2O3) phase cannot be excluded (ICDD card no. 39-1346).[34] Direct comparison between diffraction patterns of Figure a,b shows that MAGOR is composed of the same crystalline phase detected in B-magnetite. Furthermore, no significant variation indicating the presence of amorphous material or reflection broadening is observed, suggesting that the crystallinity of starting iron oxides is maintained after the functionalization with the organic moiety. The mean dimension of the crystalline domains was calculated by the Scherrer equation applied to the XRD patterns. The same value of ∼17 nm was obtained for B-magnetite and MAGOR inside the experimental error.

Figure 1

XRD patterns of (a) B-magnetite and (b) MAGOR nanoparticles.

For quantification of the organic material associated to inorganic magnetite in MAGOR, thermogravimetric (TGA) analyses were performed both on B-magnetite and on MAGOR. The two thermogravimetric profiles differ because of complete decomposition of the organic moiety between 150 and 600 °C (Figure ). Evaluation of the difference between the total weight loss of MAGOR and that of B-magnetite allows us to determine organic moiety content, which amounts to ∼9 wt %.

Figure 2

TGA plots of (a) bare nanoparticles (B-magnetite) and (b) coated nanoparticles (MAGOR).

Transmission Electron Microscopy Observations

Transmission electron microscopy (TEM) observations were performed to further investigate the MNP structure. Both B-magnetite and functionalized MAGOR were investigated. In particular, Figure a shows a general view of B-magnetite. The MNPs appear widely size-distributed and disorderly arranged on the carbon film of the TEM grid. The shape of the particles is approximately spherical with diameter ranging from 10 to 40 nm. It must be stressed that although the particle size is inhomogeneous, their diameters are fully comprised inside the interval recommended for drug delivery particles (between 10 and 100 nm). Selected area electron diffraction (SAED) measurements were performed to investigate the crystallinity and composition of the MNPs. Figure b is the SAED pattern of the particles visible in Figure a. It is composed of well-defined diffraction rings which indicate the random orientation of the particles and their good crystallinity degree. The diffraction rings in the SAED pattern correspond to the following interplanar distances: d1 = (0.483 ± 0.003) nm, d2 = (0.296 ± 0.003) nm, d3 = (0.253 ± 0.002) nm, d4 = (0.210 ± 0.002) nm, d5 = (0.171 ± 0.002) nm, d6 = (0.161 ± 0.001) nm, and d7 = (0.149 ± 0.001) nm. These values are in good agreement with diffraction data reported for magnetite/maghemite (ICDD card no. 19-0629/ICDD card no. 39-1346: d1(111); d2(220); d3(311); d4(400); d5(422); d6(511), and d7(440)). It is important to stress that no other phases were detected by SAED measurements performed on other groups of particles, and the same results, just reported, were also found for MAGOR, indicating that the upload of the organic material does not influence size, composition, and crystallinity of the MNPs.

Figure 3

(a–d) TEM analysis: (a) general view of B-magnetite nanoparticles; (b) corresponding SAED pattern; (c) high-resolution image of a B-magnetite nanoparticle; and (d) high-resolution image of a MAGOR nanoparticle.

High-resolution TEM (HRTEM) observations reveal that the MNPs are single crystals and so the mean dimension of crystalline domains obtained by XRD (∼17 nm) coincides with the average size of the MNPs. In particular, Figure c,d shows the inner structure of two typical nanoparticles. The atomic planes are clearly visible and extend with continuity from one side to the other of the particles. In more detail, Figure c shows an as-built MNP, while Figure d shows an MNP covered with the organic moiety (MAGOR). Actually, looking at the exterior of this last nanoparticle, it is possible to observe an amorphous layer (red lines) that can be associated to the organic coating of the particle surface. The same layer is not revealed on the as-built MNP surface, and the visible “orange peel” contrast at the exterior of the particle of Figure c is due to the amorphous carbon film over the TEM grid. TEM observations performed on other MAGOR nanoparticles always reveal the presence of a quite uniform amorphous layer on them, suggesting a homogeneous distribution of the organic coating around the nanoparticles (Figure S8 in Supporting Information).

Magnetic Measurements

MNP structures and size (d) play a significant role in determine their magnetic behavior. In particular, XRD and TEM analyses reveal that “d” ranges from 10 to 40 nm, with an average value of about 17 nm. These values are well below the limit for the magnetite magnetic monodomain dimension (i.e., often d ≈ 100 nm), suggesting that each nanoparticle is a single magnetic domain.[35,36] Zero-field cooled (ZFC) and field cooled (FC) curves show complex behavior because of the particle size distribution (Figure a). The mean blocking temperature is established over 350 K for both samples. In the low temperature regime, a rapid slope variation is detectable. The kink at about 20 K in both samples can be due to a spin glass (SG) like behavior. The phenomenon responsible of the SG like behavior can be identified into the dipolar interactions because the grain surface appears quite ordered, as revealed by HRTEM observations. However, this does not completely exclude surface-core spin interaction because of magnetic energy minimization.[37,38] For the MAGOR sample, it is possible to detect a second kink at about 90 K. This can be the signature of a Verwey transition, which is not detectable in B-magnetite NPs (Figure a). The differences between the two samples can be ascribed to the organic functionalization of the MAGOR NPs surface, which slightly modifies the surface and increases the interparticle distance, thus decreasing their mutual interactions.

Figure 4

(a) ZFC and FC curves for the B-magnetite and MAGOR samples. Empty symbols are ZFC and the filled symbols are FC. (b) Derivative d(MZFC)/dT for the B-magnetite and MAGOR samples.

More insight can be extracted from the derivative d(MZFC)/dT plot shown in Figure b. A peak at low temperature (about 10–20 K) is present in both samples. This confirms the presence of a SG like transition which can be ascribed to the collective behavior because of dipolar coupling between different particles.[39] Moreover, at about 80–90 K, in MAGOR sample, a possibly Verwey transition can be detected. The Verwey transition was reported in literature to be observed even for d < 50 nm at about Tv = 90 K. In fact, the increased surface/volume ratio can modify the Fe2+/Fe3+ ratio through partial oxidation inducing a decreasing of the bulk transition temperature Tv = 120 K.[39] B-magnetite does not present evidence of Verwey transition which, in this sample, can be hindered by dipolar interactions. d(MZFC)/dT measurements confirm the behavior outlined by ZFC–FC, putting in evidence a slight difference at low temperatures because of the organic materials at the surface. The observed small differences are due to the fact that the particles are relatively large to observe a significant coating effect. At higher temperatures, there is a distribution of blocking temperature (TB) because of the size dispersion. In fact, the temperature TB is a function of the particle volume and can be valued by eq (40)where EA is the barrier energy, K is the anisotropy constant, V the volume, and kB the Boltzmann constant. For T > TB the particle is “unblocked”, that is, the thermal energy will overcome the anisotropy energy (EA), so the magnetization direction of the particle begins to fluctuate in the direction allowed by the easy axis. From the FC–ZFC measurements, the irreversibility is reached over 350 K, so to better understand the magnetic behavior, especially at high temperature, it is necessary to evaluate the hysteresis loops for both the samples. In Figure a,b are plotted the loops at different temperatures.

Figure 5

(a) Hysteresis loops for B-magnetite. Measurements are taken at different temperatures. (b) Hysteresis loops for MAGOR. Measurements are taken at different temperatures.

The saturation magnetization for both B-magnetite and MAGOR samples is reported in Table . Ms has been obtained extrapolating the magnetization measurements at the limit (1/H) → 0 by[39,41]

Table 1

Magnetization Saturation Ms for B-Magnetite and MAGOR at Different Temperatures

sample	temperature (K)	Ms (emu/g)
B-magnetite	10	87.9 ± 0.9
MAGOR	10	87.6 ± 0.9
B-magnetite	100	86.1 ± 0.9
MAGOR	100	85.9 ± 0.9
B-magnetite	300	76.4 ± 0.8
MAGOR	300	76.1 ± 0.8

The estimated saturation magnetization (Ms) is very high, taking into account that the bulk magnetite Ms is reported to be about 98 emu/g at low temperatures and about 84–88 at 300 K.[36,42,43] The Ms value for the two MNP samples is the same, inside the experimental error, and it reaches the 85% of the bulk Ms (see Table ). This result can be explained in terms of good crystallization of the particles and reduced surface disorder, as revealed by XRD measurements and TEM observations.[36,44−47] It is important to stress that Ms in maghemite is 20% lower with respect to magnetite one, for nanoparticles having same dimensions,[48] so it is reasonable to suppose that the main phase in our iron oxide nanoparticles is magnetite. The high saturation magnetization is a favorable characteristic of MAGOR nanoparticles that confirms their relevance for applications in drug delivery.[21]

Both samples show small hysteretic behavior: coercivity (Hc) and remanence (Mr) are reported in Tables and 3.

Table 2

Coercivity and Remanence at Different Temperatures for B-Magnetite

B-magnetite
temperature (K)	Hc (Oe)	Mr (emu/g)
10	16 (2)	3.7 (6)
100	7 (1)	1.5 (2)
300	1.1 (2)	0.19 (3)

Table 3

Coercivity and Remanence at Different Temperatures for MAGOR

MAGOR
temperature (K)	Hc (Oe)	Mr (emu/g)
10	63 (9)	11 (2)
100	27 (4)	5.1 (8)
300	2.4 (4)	0.50 (8)

The size distribution affects the behavior of the particles’ assembly. In fact, the SPM behavior is stated for particle size lower than 25–30 nm,[36] so not all the particles are in the SPM state as put in evidence by hysteresis loops measurements. On the other hand, even if all the particles are not in the SPM state, the values of Hc and Mr are very small, especially at high temperatures. These values are similar to Hc and Mr found for Fe3O4 particles in the literature,[36,42] where a SPM-like state is defined in order to underline the low interaction condition at room temperature. Therefore, it is important to stress that the agglomeration of some MNPs, visible in the TEM image of Figure a, is not due to the magnetic interaction among particles, which could be a problem for specific medical applications, but more likely to the surface tension of the solvent (used to prepare the samples for TEM observations) during evaporation.

Conclusions

MAGOR, a new nanomaterial containing (R)-9-acetoxystearic acid bound for the first time to magnetite nanoparticles was prepared. The organic coating was made through a synthetic sequence in which a key role was played by APTES, a bidentate linker that reacted with both (R)-9-acetoxystearic acid and nanomagnetite (through silyl groups). 9-HSA was bound to APTES via amide formation (Schotten–Baumann like) after protection as 9-acetoxy derivative. Magnetic iron oxide nanoparticles prior (B-magnetite) and after the coating (MAGOR) were characterized by suitable and complementary techniques. IR and TGA analyses have allowed to evidence the link between nanoparticle and the organic coating and to estimate the upload of the organic material (∼9 wt %).

XRD and TEM measurements have revealed that the upload of the organic material does not influence size, composition, and crystallinity of the MNPs, which are single crystals with dimensions ranging from 10 to 40 nm and a mean value of about 17 nm: apt for drug delivery applications.

Magnetic characterization has evidenced the suitability of the MAGOR nanoparticles for magnetic drug delivery because of (i) their monodomain structure and low magnetic interaction, able to prevent agglomeration at room temperature and (ii) their high magnetization saturation, important to guide the drug to the target site through an external magnetic field.

Thus, the novel material possesses all the necessary properties for being used in magnetically-guided delivery of 9-HSA, a known antiproliferative agent acting selectively against cancer cells. This work paves now the way to biochemical studies on MAGOR delivery and effects, for example, in vitro or through local deposit.

Experimental Section

Materials

Iron(III) pentahydrate sulphate (Fe2(SO4)3·5H2O, 97%), ammonia (NH3, 28–30 wt %, d = 0.9 g/cm3), diethyl ether, ethyl acetate, dichloromethane, toluene, ethanol (95%), vinyl acetate, and lipase acrylic resin from Candida antarctica 10,000 U/g (Novozyme 435) were purchased from Sigma-Aldrich. CDCl3 was from Euriso-top (Saint-Aubin, France), iron(II) heptahydrate sulphate (Fe2SO4·7H2O, 95%) and triethylamine (TEA, 99%) were from Carlo Erba (Italy), and oxalyl chloride was from Alfa Aesar, Thermo Fisher Scientific (Karlsruhe, Germany). Ultrapure UPP water used for magnetite synthesis was obtained with a Milli-Q plus system (Millipore Co., resistivity 18MΩcm). (R)-9-Hydroxystearic acid was synthesized from Dimorphotheca sinuata L. seeds, as previously described.[27] CH2Cl2 was dried by distillation over P2O5 and stored under an argon atmosphere. Toluene was dehydrated by distillation under nitrogen on Na/K amalgam and stored under nitrogen on 4 Å molecular sieves.

Characterization Techniques

Nuclear Magnetic Resonance

The NMR spectra (1H, 13C, DEPT) were recorded on Varian spectrometers Gemini 300, Mercury 400 and Inova 600 (Varian, Palo Alto, USA). The frequencies are given in Hz, and the chemical shift is given in ppm using the chemical shift of the solvent CDCl3 as the reference (7.26 and 77.0 ppm for 1H and 13C NMR, respectively).

IR Spectra

IR spectra were recorded using a Fourier transform spectrophotometer PerkinElmer FT-IR spectrometer Spectrum Two in the 4000–500 cm–1 wavelength range, using a NaCl cell for liquid samples, whereas the spectra of solid samples were recorded using an Universal ATR accessory.

Mass Spectra

ESI-MS spectra were recorded on a mass spectrometry WATERS 2Q 4000.

pH Measurements

The pH-measures were carried out on a AMEL334-B, calibrated with standard solutions at pH = 7 and pH = 9.

Thermogravimetric Analyses

They were performed using a PerkinElmer TGA-7 with a heating ramp from 37 to 700 °C at a rate of 10 °C/min, under air flux.

X-ray Diffractometry

Powder X-ray diffractometry was carried out using a Panalytical X’Pert Pro (Cu Kα radiation, λ = 0.154 nm, 40 mA, 40 kV). The peak broadening was used to evaluate the crystal size (τ), which was calculated from the width at half maximum intensity (β1/2) using the Scherrer equation (eq )[33]where λ is the wavelength, θ the diffraction angle, and K a constant depending on crystal habit (chosen as 1). For crystal size calculation, the most intense reflection for magnetite was taken into consideration, that is, peak (311).

Transmission Electron Microscopy

The size and inner structure of the NPs were investigated by TEM techniques using a Philips CM200 microscope operating at 200 kV and equipped with a LaB6 filament. For TEM observations, a small quantity of NPs was dispersed in ethanol and subjected to ultrasonic agitation for approximately one min. A drop of the suspension was deposited on a commercial TEM grid covered with a thin carbon film; finally, the grid is kept in air until complete evaporation of the ethanol.

Magnetic Measurements

Magnetic measurements were performed by means of a Quantum Design PPMS ac/dc Magnetometry System (ACMS). The measurements are based on the mutual-inductance technique using the ACMS coil set and electronics. Magnetization data as a function of temperature have been measured till 30 kOe. ZFC and FC protocols have been applied to evaluate the temperature dependence of the magnetization.[35,41] The ZFC–FC magnetization measurements have been performed at first by cooling the sample starting from room temperature to 2 K in zero magnetic field. A small static magnetic field of 100 Oe was then applied, and the ZFC measurement was performed during the warmup from 2 to 350 K. The FC measurement was recorded, as a function of the temperature, while the sample was cooled down to 2 K. Hysteresis loops have been performed at 10, 100, and 300 K till 10 kOe to evaluate the coercivity and remanence as a function of the temperature.

Synthesis of the Organic Coating

Synthesis of (R)-9-Acetoxyoctadecanoic Acid (2)

To a mixture of (R)-9-hydroxystearic acid (0.60 g, 2.0 mmol) and vinyl acetate (10 mL), diethyl ether was added until dissolution of the solid (about 20 mL). Novozyme 435 (0.630 g) was added, and the mixture was stirred at 30 °C for 5 days. The suspension was filtered through a Gooch funnel, and the enzyme was washed with diethyl ether and ethyl acetate. Evaporation of the combined organic phases afforded acetylated product (0.66 g, 1.9 mmol, 97% yield). 1H NMR (600 MHz, CDCl3, 298 K): δ, ppm: 4.85 (qt, J = 5.8 Hz, 1H, CHOH), 2.34 (t, J = 7.4 Hz, 2H, CH2COOH), 2.04 (s, 3H, CH3CO), 1.63 (qt, J = 7.3 Hz, 2H, CH2CH2COOH), 1.55–1.45 (m, 4H), 1.37–1.20 (m, 22H, remaining CH2 chain), 0.88 (t, J = 6.9 Hz, 3H, CH3); 13C NMR (150.8 MHz, CDCl3, 298 K): δ, ppm: 179.6, 171.0, 74.4, 34.1, 34.03, 33.9, 31.8, 29.5 (2 signals overlapped), 29.26 (2 signals overlapped), 29.1, 28.9, 25.20, 25.19, 24.6, 22.7, 21.3, 14.1; ESI-MS+ (m/z): 365 [M + Na]+, 381 [M + K]+; ESI-MS– (m/z): 341 [M – H]−; IR (ν, cm–1): 3428, 2958, 2925, 2856, 1735, 1705, 1646, 1462, 1373, 1242, 1027.

Synthesis of (R)-1-Chloro-1-oxooctadecan-9-yl Acetate (3)

Into a three-necked round-bottom flask and under an argon atmosphere, (R)-9-acetoxyoctadecanoic acid (300 mg, 0.00088 mol) was dissolved in anhydrous CH2Cl2 (10 mL). Oxalyl chloride (0.077 mL, 0.00088 mol) was added to the solution, and the mixture was stirred for 24 h at room temperature. The reaction course was monitored by 1H NMR spectroscopy. When it resulted complete, the solvent was removed and the oil obtained was used without purification. 1H NMR (400 MHz, CDCl3, 298 K): δ, ppm: 4.85 (qt, J = 5.9 Hz, 1H, CHOH), 2.88 (t, J = 7.3 Hz, 2H, CH2COOH), 2.04 (s, 3H, CH3CO), 1.70 (qt, J = 7.4 Hz, 2H, CH2CH2COOH), 1.55–1.45 (m, 4 H), 1.39–1.19 (m, 22 H), 0.88 (t, J = 7.0 Hz, 3H, CH3); 13C NMR (100.5 MHz, CDCl3, 298 K): δ, ppm: 173.8, 171.0, 74.3, 53.4, 47.1, 34.1, 34.0, 31.9, 29.5 (2 signals overlapped), 29.3, 29.2, 28.9, 28.3, 25.3, 25.2, 25.0, 22.7, 21.3, 14.1; IR (ν, cm–1, neat): 2928, 2858, 1791, 1721, 1378, 1266, 1019.

Synthesis of (R)-1-Oxo-1-((3-(triethoxysilyl)propyl)amino)octadecan-9-yl Acetate (4)

Triethylamine (0.122 mL, 0.00088 mol) and APTES (0.20 mL, 0.00088 mol) were added to a solution of 3 (0.00088 mol) in CH2Cl2 (10 mL), and the mixture was stirred for 3 h at room temperature. The reaction was monitored by 1H NMR spectroscopy until it resulted complete. The solvent was removed under inert atmosphere to avoid exposure to air, the solvent was removed, and the residue was used without purification. 1H NMR (600 MHz, CDCl3, 298 K): δ, ppm: 4.76 (qt, J = 6.03 Hz, 1H, CHOH), 3.73 (q, J = 7.1 Hz, 6H, CH2OSi), 3.16 (q, J = 6.4 Hz, 2H, CH2NH), 2.08 (t, J = 7.6 Hz, 2H, CH2COOH), 1.90 (s, 3H, CH3CO), 1.57–1.46 (m, 2 H), 1.47–1.37 (m, 4 H), 1.22–1.10 (m + t, 24H + 9H, aliphatic chain + CH3CH2OSi), 0.77 (t, J = 7.0 Hz, 3H, CH3), 0.53 (t, J = 8.1 Hz, 2H, CH2Si); 13C NMR (150.8 Hz, CDCl3, 298 K): δ, ppm: 172.9, 170.8, 74.2, 58.2, 45.6, 41.6, 36.6, 33.92, 33.87, 31.7, 29.3 (2 signals overlapped), 29.10, 29.08, 29.01 25.6, 25.11, 25.06, 22.7, 22.5, 21.1, 18.1, 13.9, 8.5; ESI-MS+ (m/z): 568 [M + Na]+, 584 [M + K]+; IR (ν, cm–1, neat): 3448, 2930, 2859, 2416, 2248, 2212, 1717, 1662, 1520, 1465, 1387, 1371, 1261, 1103, 1077.

Preparation of Bare Magnetite (Fe3O4) Nanoparticles (B-Magnetite)

The synthesis of bare magnetite nanoparticles was carried out following a previous protocol.[33,49] Into a three-necked round-bottom flask, FeSO4·7H2O (2.788 g, 0.010 mol) and Fe2(SO4)3·5H2O (5.131 g, 0.010 mol) were dissolved in 100 mL of water Milli-Q purity grade, and the solution was degassed with three vacuum/nitrogen purging cycles. An excess of ammonia (13.0 mL, 0.200 mol) was added dropwise monitoring the pH of the mixture until to pH = 10.4. The black suspension was stirred for 2 h at 60 °C and cooled and allowed to stand. MNPs were separated from the supernatant solution using an external magnetic bar and thoroughly washed with water and ethanol, dried at 60 °C, and kept under vacuum for 12 h at 50 °C. The final product (2.220 g, 96% yield) was stored under an argon atmosphere.

Functionalization of B-Magnetite with 4

Dry toluene (10 mL), MNPs (B-magnetite, 205 mg, 0.88 mmol), and Et3N (10 μL, 0.072 mmol) were added to the crude amide 4 (0.88 mmol). The suspension was vigorously stirred for 24 h at 60 °C and then maintained at 100 °C for 1 h. The solvent was removed using Magnetic bar’s technique described for the synthesis of MNPs (sub-section 4.3.4), and then, the product was washed with dry toluene. (R)-1-Oxo-1-((3-(triethoxysilyl)propyl)amino)octadecan-9-yl acetate-coated MNPs, hereinafter indicated as MAGOR, were first dried in an oven for 12 h (70 °C) and then kept under vacuum for 12 h. IR analysis confirmed the presence of characteristic bands of organic groups: IR (ν, cm–1): 2930.4, 1735.2, 1659.8, 1478.8, 1121.4, and 1031.7.