Tailored Lewis Acid Sites for High-Temperature Supported Single-Molecule Magnetism

Generating or even retaining slow magnetic relaxation in surface immobilized single-molecule magnets (SMMs) from promising molecular precursors remains a great challenge. Illustrative examples are organolanthanide compounds that show promising SMM properties in molecular systems, though surface immobilization generally diminishes their magnetic performance. Here, we show how tailored Lewis acidic Al(III) sites on a silica surface enable generation of a material with SMM characteristics via chemisorption of (Cpttt)2DyCl ((Cpttt)− = 1,2,4-tri(tert-butyl)-cyclopentadienide). Detailed studies of this system and its diamagnetic Y analogue indicate that the interaction of the metal chloride with surface Al sites results in a change of the coordination sphere around the metal center inducing for the dysprosium-containing material slow magnetic relaxation up to 51 K with hysteresis up to 8 K and an effective energy barrier (Ueff) of 449 cm–1, the highest reported thus far for a supported SMM.

S ingle-molecule magnets (SMMs), compounds exhibiting slow magnetic relaxation in the absence of an external magnetic field, are anticipated to be used for data storage, quantum computing, and/or spintronics. 1−4 Such applications require magnetic centers to be isolated on solid supports, where every site can be individually addressed. 5,6 To date, several methodologies of SMM surface immobilization have been explored, 7−13 focusing mostly on minimizing changes in coordination environment to avoid a decrease or loss of SMM properties. 14 Other approaches take advantage of the direct interaction between the metal center and the surface to induce or improve SMM properties. 15−19 A key challenge in generating magnetic remanence in supported SMMs is the multitude of possible interactions between the magnetic center and the surface, which can induce fast relaxation of the magnetic moment, 6,14,20 and thus so far, the performances of surface deposited SMMs lag far behind molecular systems. Among such molecular systems, dysprosocenium cations� Dy(III) ions sandwiched between two substituted cyclopentadienyl moieties (Cp R ) − �combine the high intrinsic magnetic moment of the lanthanide ion with a strong axial crystal field, 21−23 resulting in high magnetic anisotropy and positioning these molecular compounds among the best SMMs. 5,24−28 These cationic species are synthesized by the abstraction of an anionic X − ligand from a neutral precursor, i.e. [(Cp R ) 2 DyX] (Figure 1a, with X − = Cl − , I − , BH 4 − ). 24−28 This abstraction induces a shorter distance between Dy and (Cp R ) − , a wider Cp centroid −Dy−Cp centroid angle (ω), and consequently a stronger axial crystal field leading to better SMM properties compared to its neutral precursor. Alternatively, SMM properties can also be improved by weakening the equatorial crystal fields. 29−33 In seeking a surface-immobilized analogue to high-performing dysprosocenium complexes, one can draw a parallel with supported polymerization catalysts based on metallocenes. 34 A longstanding objective in the latter field has been the generation of highly active cationic metal surface sites by abstraction of one anionic ligand of the precursor by surface Lewis acid sites in the support, 35−37 e.g. low (tri-) coordinated Al(III) centers ( Figure 1b). These low-coordinate Al have been proposed to be accessible via several methods: dehydroxylation of γ-alumina 35,36 or incorporation of aluminum sites in a rigid framework (zeolites). 38,39 However, in many instance, neutral species are also formed due to the competitive reactions of the molecular precursor with surface OH groups. 34,40 Supports including alkylaluminum species mitigate these problems, 41,42 but lead to rather complex surface chemistry and the formation of multiple sites.
Herein, we report an alternative strategy by selectively generating strong Lewis acidic aluminum sites on silica while maintaining a surface largely free of OH groups. Chemisorption of (Cp ttt ) 2 DyCl ((Cp ttt ) − = 1,2,4-tri(tert-butyl)cyclopentadienide)�a molecular precursor having poor SMM properties (with no magnetic hysteresis observed at 2 K), 24,43 �at these low coordinate Al sites generates a material that exhibits slow magnetic relaxation up to 51 K with an effective energy barrier of U eff = 449 cm −1 . Detailed chemical and computational analyses of the material and its diamagnetic Y analogue 44 indicate a change in the coordination environment around the metal center resulting from a Lewis acid−base interaction between the surface Al sites and the chloride ligand. This interaction leads to a stronger axial crystal field, and consequently slower magnetic relaxation behavior for the Dy containing material.
We first synthesized the silica-based materials containing surface Al(III) sites via a two-step process. The first step involves grafting of a bulky trismesitylaluminum (Al(Mes) 3 ) on the isolated OH groups of partially dehydroxylated amorphous silica, yielding well-defined surface (Mes) 2 Al-(OSi�) sites. In the second step, the resulting material is heated at 450°C under high vacuum (10 −5 mbar) to provide Al@SiO 2 (Figures 2a and S1). This thermal treatment leads to a transfer of remaining mesityl groups from Al(III) to Si(IV) with simultaneous opening of adjacent siloxane bridges, which results in a tailored support containing isolated low-coordinate Al(III) sites in all-oxygen environments with only a minor amount of residual OH groups. This makes Al@SiO 2 a wellsuited platform for the selective abstraction of anionic ligands. Transmission Fourier-transform infrared spectroscopy (FT-IR) measurements indicate the consumption of isolated OH groups during the grafting process, which are not restored upon thermal treatment (Figure 2c). Mass balance analysis as well as 1 H, 13 C, and 29 Si solid-state nuclear magnetic resonance (NMR) spectroscopy (see SI for more details, Figures S4, S5, and S10) data confirm the formation of a monografted surface species, (Mes) 2 Al(OSi�), before heat treatment. The heattreated material contains primarily Al(OSi�) 3 sites along with a small amount (around 10%) of remaining mesityl-aluminum moieties. Wideline solid-state 27 Al NMR spectra (Figure 3a) of Al@SiO 2 indicate the presence of two main Al(III) sites, each exhibiting different quadrupolar coupling constants (C Q ) of ca. 14 (site I, violet) and 22 MHz (site II, green), which are assigned to two types of surface Al sites in distorted, tetrahedral oxidic environments. The presence of strong Lewis acid sites on the support is established by exposing the material to 15 N pyridine and recording its solid-state 15 N{ 1 H} CP-MAS spectrum ( Figure S6) which displays an intense signal at 252 ppm along with a weaker signal at 216 ppm, consistent with the presence of strong Lewis acid sites along with a small amount of residual acidic silanols (not observed by IR). Notably, the 27 Al NMR spectrum of this  material (Figure 3b) indicates that site I is not affected by adsorption of pyridine, while site II shows a strong decrease of C Q from 22 to 15 MHz, indicating that only site II is prone to coordinate Lewis bases, suggesting that it is a highly distorted tetrahedral site consistent with its large C Q value.
Next, Al@SiO 2 was combined with (Cp ttt ) 2 DyCl or its diamagnetic analogue (Cp ttt ) 2 YCl to yield the corresponding materials Dy-Al@SiO 2 and Y-Al@SiO 2 (Figure 2b). FT-IR measurements of these materials (Figures 2c and S7) show an increase of the relative intensity and a changed intensity distribution of C−H stretching modes (3050−2850 cm −1 ) compared to the rare-earth free material with features that are in line with those of the molecular precursors. 24,25 The IR data and the low M/Al molar ratios (ca. 0.25) for Dy-Al@SiO 2 and Y-Al@SiO 2 suggest a successful surface deposition of the precursor most likely via interaction of the chloride ligand with the most reactive Lewis acidic sites. In order to understand the nature of the precursor−support interaction, we investigated Y-Al@SiO 2 via solid-state 1 H and 13 C magic-angle-spinning (MAS) NMR. The data confirm the presence of (Cp ttt ) − and mesityl moieties supporting a successful surface deposition of the precursor (Figures S8 and S9). Furthermore, 27 Al NMR shows that the C Q value of Al site II decreases from 22 to 19 MHz upon reaction with (Cp ttt ) 2 YCl (Figure 3c), pointing to an interaction of Al site II with the Y precursor while site I remains unperturbed, paralleling the observations upon pyridine adsorption. This interaction is corroborated by solid-state 89 Y{ 1 H} CP NMR spectra acquired with sensitivity enhanced by dynamic nuclear polarization (DNP), 46 The magnetic properties of Dy-Al@SiO 2 were evaluated using alternating current (AC) and direct current (DC) experiments. The out-of-phase (χ′′(ν), with ν denoting the oscillating field frequency) component of the AC magnetic susceptibility exhibits maxima between 2 and 51 K (Figure 4a) under an oscillating field in the absence of an applied static magnetic field. Over the whole measured range, χ′′ shows a temperature dependence visualized by the shift of the maxima upon increasing temperatures. In contrast, (Cp ttt ) 2 DyCl does not exhibit slow relaxation characteristics under these conditions. 24 To gain more insights into the specific relaxation times and mechanisms, the AC susceptibility data in the 2 to 49 K range were fitted using the extended Debye model showing a wide distribution of relaxation times with an α max of 0.56 (Table S1) resulting from a distribution of magnetic sites on the surface, consistent with the 89 Y NMR data and other reports on surface deposited SMMs. 17,19 The extracted specific relaxation times τ for each temperature can be expressed with the two component fit of τ −1 = τ 0  (over an effective energy barrier U eff , k B representing the Boltzmann constant) and the second term describes the Raman process (C is the Raman coefficient and n the Raman exponent). To the best of our knowledge, Dy-Al@SiO 2 not only shows slow relaxation at the highest reported temperature but also has the highest reported U eff = 449 cm −1 (τ 0 = 5.24 × 10 −9 s, C = 9.3 × 10 −2 s −1 K −n and n = 1.75) for an immobilized SMM (see Supporting Information (SI) for more details, Figure S13 and Table S2). The field-dependency of the magnetization was investigated in the range of an applied field between −20 to +20 kOe using a field sweep rate of 16 Oe s −1 between 2 and 8 K (Figure 4c). Under these conditions, the hysteresis loops remain open up to 8 K. At 2 K a remnant magnetization of 0.9 Nβ and a coercive field of 354 Oe was found, further demonstrating the SMM character of Dy-Al@SiO 2 . The opening of the hysteresis loop supports the hypothesis that the interaction of (Cp ttt ) 2 DyCl with Al@SiO 2 induces SMM behavior.
To further corroborate these results, the dependence of magnetic properties of model structures as a function of the Dy−Cl distance were investigated computationally using an ab initio CASSCF/RASSI-SO/SINGLE_ANISO approach (see SI for more details). As expected, the energy splitting between the two lowest Kramers doublets is driven by the Dy−Cl bond length, with longer bonds yielding higher energy spacings. Note that elongation of the Dy−Cl bond leads to wider ω angle and shorter Dy−Cp centroid distance consistent with the improved SMM properties (see SI, Figures S16−S22 and Tables S3−S6). Comparison of the calculated χT and magnetization curves at 2 K (Figures S14 and S15) of all the model structures with the measured data suggest an increase in Dy−Cl bond length from 2.54 Å in (Cp ttt ) 2 DyCl to around 2.6−3.1 Å in Dy-Al@SiO 2 .
In conclusion, this work shows that selectively formed Lewis acidic Al(III) surface sites can be used to immobilize (Cp ttt ) 2    . Magnetic characterization of Dy-Al@SiO 2 : (a) frequency dependence of the out-of-phase component of the AC susceptibility measured in zero external DC field between 2 and 51 K using a 3 Oe amplitude, (b) temperature dependence of the relaxation time between 2 and 49 K where the red line is the best fit using the parameters in the text, and (c) hysteresis curves recorded between 2 and 8 K with 16 Oe s −1 field sweep rate. Inset shows a zoom of the zero-field region.