Sihuai
Chen
a,
Valeriu
Mereacre
*a,
Christopher E.
Anson
a and
Annie K.
Powell
*ab
aInstitute of Inorganic Chemistry, Karlsruhe Institute of Technology, Engesserstrasse 15, 76131 Karlsruhe, Germany. E-mail: valeriu.mereacre@kit.edu; annie.powell@kit.edu
bInstitute of Nanotechnology, Karlsruhe Institute of Technology, Hermann-von-Helmholtz Platz 1, 76344 Eggenstein-Leopoldshafen, Germany
First published on 4th November 2015
Two series of heterometallic FeIII–LnIII compounds, [FeIII4LnIII2(μ3-OH)2(mdea)4(m-NO2C6H4COO)8]·3MeCN where Ln = Y (1) and Dy (2) and [FeIII6LnIII3(μ4-O)3(μ3-O)(mdea)5(m-NO2C6H4COO)9]·3MeCN where Ln = Y (3) and Dy (4), were synthesized. Compounds 1 and 2 were obtained under ambient conditions, whereas 3 and 4 were obtained via a solvothermal transformation process by heating 1 or 2 at 120 °C in MeCN. The magnetic properties of all four compounds have been measured and show that compounds 2 and 4 containing DyIII ions exhibit slow relaxation of magnetization characteristic of Single Molecule Magnetic (SMM) behaviour.
In this search, ligands bearing alkoxy groups, which are capable of both chelating and bridging between metal centres, such as the N-substituted diethanolamines, and which are known to lead to polynuclear FeIII and 4f CCs,5,6 have been found to be ideal for stabilising 3d–4f CCs7 due to the fact that the hard-donor oxygens are likely to bind to the oxophilic lanthanide ions, leaving the softer donor nitrogen to act as the central tripodal ligand binding the softer transition metal ions and providing the anchor point for the 3d/4f coordination cluster. Thus the deprotonated alcohol arms provide chelating and bridging capabilities and facilitate the formation of high nuclearity 3d–4f CCs.
From a synthetic point of view, CCs are metastable species produced by solvolysis of metal ions and are prevented from reaching the thermodynamic continuous phase end-point through the availability of encapsulating ligand species.1b Whereas ambient conditions have been successfully applied to produce a large variety of CCs, hydro- and solvo-thermal synthesis often leads to coordination polymers and MOFs with continuous rather than finite 0D structures. However, careful control of the conditions has been shown to lead to the production of finite CC systems.8a,b This approach appears to be particularly promising for systems incorporating 4f ions. In this technique high temperatures are applied to the reactions in solvents with low boiling points. The resulting compounds produced under solvothermal conditions may exhibit structural diversity and unique properties.9 For example, we recently reported two FeIII4DyIII4 clusters obtained via a solvothermal treatment of two different FeIII–DyIII compounds produced from reactions conducted under normal conditions.8a
In this paper, we present the synthesis, structures and magnetic properties of two sets of FeIII–LnIII compounds formulated as [FeIII4LnIII2(μ3-OH)2(mdea)4(m-NO2C6H4COO)8] where Ln = Y (1) and Dy (2) and [FeIII6LnIII3(μ4-O)3(μ3-O)(mdea)5(m-NO2C6H4COO)9] where Ln = Y (3) and Dy (4), among which compounds 3 and 4 were synthesised via a transformation process by heating 1 or 2 in MeCN under solvothermal conditions, respectively.
1 | 2 | 3 | 4 | |
---|---|---|---|---|
Formula | C82H87N15O42Fe4Y2 | C82H87N15O42Fe4Dy2 | C94H100N17O50Fe6Y3 | C94H100N17O50Fe6Dy3 |
M r | 2355.88 | 2505.11 | 2868.91 | 3090.50 |
Crystal system | Monoclinic | Monoclinic | Triclinic | Triclinic |
Space group | C2/c | C2/c |
P![]() |
P![]() |
T (K) | 150(2) | 150(2) | 298(2) | 150(2) |
a (Å) | 31.177(4) | 31.1882 | 13.9126 | 13.8939(9) |
b (Å) | 15.660(2) | 15.6817 | 16.8878 | 16.7523(12) |
c (Å) | 20.673(3) | 20.7311 | 24.9901 | 24.8472(16) |
α (°) | 90 | 90 | 81.858 | 81.772(5) |
β (°) | 95.539(2) | 94.922 | 83.118 | 83.121(5) |
γ (°) | 90 | 90 | 86.085 | 85.507(5) |
V (Å3) | 10![]() |
10![]() |
5762.6 | 5671.5(7) |
Z | 4 | 4 | 2 | 2 |
D calc (g cm−3) | 1.558 | 1.810 | ||
F(000) | 4808 | 3074 | ||
μ (mm−1) | 1.129 | 2.794 | ||
λ (Å) | 0.80000 | 0.71073 | ||
Data collected | 57![]() |
53![]() |
||
Unique data | 11![]() |
20![]() |
||
R int | 0.0330 | 0.0992 | ||
Parameters | 553 | 1530 | ||
R 1 (I > 2σ(I)) | 0.0778 | 0.0604 | ||
wR2 (all data) | 0.2302 | 0.1545 | ||
S (all data) | 1.029 | 0.969 | ||
Max. diff. peak/hole (e Å−3) | +1.47/−0.93 | +1.98/−3.21 |
Crystallographic data (excluding structure factors) for the structures in this paper have been deposited with the Cambridge Crystallographic Data Centre as supplementary publication no. CCDC 1429780 and 1429781.
Powder X-ray measurements were made with a Stoe STADI-P diffractometer using Cu-Kα radiation.
The reactions of [FeIII3O(m-NO2C6H4COO)6(H2O)3]·(m-NO2C6H4COO)/Ln(NO3)3/mdeaH2 in the molar ratio 1:
1
:
8 in MeCN at room temperature afforded the hexanuclear compounds [Fe4Ln2(μ3-OH)2(mdea)4(m-NO2C6H4COO)8]·3MeCN, where Ln = Y (1) and Dy (2). Compounds [Fe6Ln3(μ4-O)3(μ3-O)(mdea)5(m-NO2C6H4COO)9]·3MeCN, where Ln = Y (3) and Dy (4), can be synthesised via a solvothermal transformation process by heating 1 or 2 in MeCN under solvothermal conditions for 72 hours, respectively (Scheme 1).
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Scheme 1 A schematic representation of the synthetic routes of compounds 1–4. Details are given in the Experimental section. |
Single-crystal X-ray analysis revealed that compound 1 crystallises in the monoclinic space group C2/c with Z = 4, while compound 4 crystallises in the triclinic space group P with Z = 2. Crystals of both 1 and 2 are small and weakly-diffracting, but it was possible to determine the structure of 1 using synchrotron radiation. Compounds 2 and 3 were shown to be isomorphous with 1 and 4, respectively, by comparison of their unit cells with those of compounds 1 and 4. Therefore, the structures for 1 and 4 are described here in detail as representative examples.
Compound 1 exhibits the identical {Fe4Y2} core unit to that previously reported for [Fe4Ln2(μ3-OH)2(nbdea)4((CH3)3CCO2)6(N3)2]13 and for [Fe4Dy2(μ3-OH)2(nbdea)4(C6H5CO2)8]·MeCN.8a In the hexanuclear core of compound 1 there is a butterfly shaped central {Fe2Y2} unit, in which the FeY2 triangles are each bridged by a single (μ3-OH)− ligand (O1 or O1′), a syn,syn-bridging benzoate and a doubly-deprotonated (mdea)2− ligand, with the two deprotonated oxygens (O4, O5 or O4′, O5′) forming alkoxo bridges along the Fe⋯Y edges. The remaining FeIII ions are linked to the tetranuclear core through two deprotonated oxygens (O2, O3 or O2′, O3′) from a doubly-deprotonated (mdea)2− ligand and a syn,syn-bridging benzoate, respectively (Fig. 1).
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Fig. 1 Molecular structure of the coordination cluster in [FeIII4YIII2(μ3-OH)2(mdea)4(m-NO2C6H4COO)8]·3MeCN (1). Organic H atoms have been omitted for clarity. |
The molecular structure of compound 4 consists of a core of six FeIII and three DyIII ions (Fig. 2). One of the μ4-O2− ligands, O1, bridges between Fe1 and three DyIII ions (Dy1, Dy2 and Dy3) to give a distorted tetrahedral {FeDy3(μ4-O)} unit. The Fe1 and Dy1 are further linked through two syn,syn-bridging benzoates, while Dy2 and Dy3 are each chelated by a benzoate ligand. The Fe1–O1 distance is 1.8714(1) Å, while the Dy–O1 bond lengths are in the range 2.2691(2)–2.3810(2) Å. The angles between Fe1 and the three Dy ions are 122.265(6)° for Fe1–O1–Dy1, 104.032(7)° for Fe1–O1–Dy2 and 103.445(7)° for Fe1–O1–Dy3, respectively, while the Dy–O1–Dy angles vary from 107.105(5)° to 110.147(4)°.
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Fig. 2 Molecular structure (left) and core (right) of the coordination cluster in [Fe6Dy3(μ4-O)3(μ3-O)(mdea)5(m-NO2C6H4COO)9]·3MeCN (4). Organic H atoms have been omitted for clarity. |
The Dy2⋯Dy3 edge is further bridged by a benzoate oxygen (O15) while the Dy1⋯Dy3 and Dy1⋯Dy2 edges are each further bridged by other μ4-O2− ligands with two further Fe centres: O2 bridges Dy1, Dy3, Fe2 and Fe3, and O3 bridges Dy1, Dy2, Fe2 and Fe4. Two peripheral benzoate ligands provide two syn,syn-bridges between Fe3 and Dy3 or Fe4 and Dy2, respectively. The only μ3-O2− ligand O4 bridges the central Fe2 to the final two FeIII ions (Fe5 and Fe6). Additionally, two further benzoate ligands form two syn,syn-bridges between Fe5 and Fe6. The remaining ten (mdea)2− oxygens each form a (μ-OR) bridge between the iron and a further metal centre, thus forming four Fe⋯Fe and six Fe⋯Dy bridges.
In contrast to the previously reported isostructural Fe4Ln2 clusters with benzoate8a or t-butylbenzoate13 ligands, the nitrobenzoate ligands in 1 offer additional possibilities for inter- and intermolecular interactions. Thus the molecular structure is now further stabilised by intramolecular C–H⋯ONO hydrogen bonds and electrostatic interactions between nitro N and O atoms of adjacent nitrobenzoate ligands. The overall crystal packing is also stabilised by a range of intermolecular C–H⋯ONO hydrogen bonds involving C–H bonds from either nitrobenzoate or diethanolamine ligands. Similar interactions are found in the structure of 4.
For compound 2, the χT product decreases on lowering the temperature, reaching a minimum value at 12 K, and then slightly increases until 32.6 cm3 K mol−1 at 1.8 K, which may result from the weak intramolecular ferromagnetic interactions within the complex (Fig. 3). Since the magnetic behaviour of 1 suggests that the FeIII–FeIII interactions are antiferromagnetic, a subtraction of the χT product of 1 from 2 was performed to estimate the magnetic interactions related to the DyIII ions (Fig. 3). The shape of the adjusted χT vs. T plot revealed that the interaction between the two central DyIII ions should be weakly ferromagnetic.
The field dependence of magnetization for 1 at 2 K confirmed the presence of the dominant antiferromagnetic interactions between the FeIII ions, in which the magnetization only reaches 0.05μB even up to 70 kOe (Fig. S1,† top-left). For 2, the magnetization increases with increasing field at low temperature (2 K, 3 K and 5 K), reaching about 12μB without saturation even at 70 kOe (Fig. S1,† top-right). The lack of saturation indicates the presence of magnetic anisotropy and/or low-lying excited states in this system. Since compound 2 contains two antiferromagnetically coupled Fe2 units for which the magnetization at low temperature is close to zero, the value of 12μB at 70 kOe is contributed by the weak ferromagnetically coupled Dy2 unit, in which the value for the single DyIII ion in polycrystalline compounds is expected to be ∼5–6μB.
For 3 and 4, the χT value at 300 K is much lower than the expected value for six high-spin FeIII (S = 5/2, g = 2) and three DyIII non-interacting ions (see Table S1†), respectively, which indicates strong antiferromagnetic interactions within the complexes. Upon cooling, χT values for both compounds continuously decrease until 1.8 K, confirming the dominant antiferromagnetic interactions within both complexes (Fig. 4, left). For compound 3 containing diamagnetic YIII ions, the χT value of 0.75 cm3 K mol−1 at 1.8 K revealed that at low temperature the interactions within the five bottom FeIII ions as well as the interaction between the FeIII pentamer and the single FeIII ion (Fe1) are antiferromagnetic. The shape of the adjusted χT vs. T plot for compound 4 with the data of compound 3 subtracted suggested that the interactions between the three central DyIII ions should also be antiferromagnetic (Fig. 4, left). Furthermore, the discrepancy between the χT values for 3 and 4 at 300 K is 42.7 cm3 K mol−1. This value is in good agreement with the expected value (42.5 cm3 K mol−1) for three non-interacting DyIII ions.
The field dependence of the magnetization at low temperature for 3 increases steadily and reaches 6.6μB at 2 K and 70 Oe (Fig. S1,† bottom). This value is much lower than the expected saturation value of 10μB for the parallel alignment of the single FeIII ion (Fe1) (S = 5/2) spin and the resulting spin state of the five antiferromagnetically coupled iron ions in the FeIII pentamer (S = 5/2). This shows that in spite of the absence of direct exchange pathways between these spin sources, they still experience each other and this results in weak antiferromagnetic interaction, leading to a lower magnetic moment of 6.6μB than the expected 10μB.
The M vs. H data for compound 4 show that the magnetization increases with an increase in applied field in two steps at 2 K (Fig. 4, right). First, the magnetization increases sharply, reaching a step at about 10.1μB at a field of 10 kOe. With a further increase in applied field, the magnetization increases rapidly again and approaches a value of 22.0μB at 70 kOe. Such a behaviour indicates the stepwise alignment of spins under the applied field and the progressive population of the low-lying excited states. The value 22.0μB is in good agreement with the value expected for three Dy ions in polycrystalline compounds (∼15μB) and 6.6μB from the (Fe5 + Fe) unit. The lack of saturation indicates the presence of magnetic anisotropy and/or the low-lying excited states in this system.
The orientation of the main magnetic axes for all three DyIII centers in 4 can be determined by using the program Magellan.15Fig. 5 shows that the axes for Dy2 and Dy3 point towards the Dy1 while the axis for Dy1 points to the center of the Dy3 triangle. Such an orientation leads to an incomplete cancellation of magnetic spins, resulting in a magnetic ground state for the Dy3 triangle. The type of inflection observed at about 10 kOe is usually observed when the applied magnetic field overwhelms weak antiferromagnetic interactions and dictates the orientation of these spins. However, the presence of very anisotropic Dy ions in this compound makes it difficult to determine the magnitude of the magnetic exchange interaction and to determine which magnetic spins are involved in this. Another factor here is that the Dy3 triangle in 4 does not necessarily have a nonmagnetic ground state, although the structural details suggest this given our previous results on triangles with very similar structural features. Thus, although at small fields (0–10 kOe) its magnetization shows a similar behaviour to that seen for the prototype Dy3,16 the non-magnetic state can be excluded since the χT of 4 at 1.8 K is far from zero (see Fig. 4, left), indicating a magnetic ground state for the Dy3 triangle. We would need more information concerning the relative magnitudes of the exchange between Dy–Dy and Dy–Fe ions to elucidate the origin of the observed inflection.
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Fig. 5 Orientation of the anisotropy axes as determined using the Magellan15 program for the DyIII centres (Dy1, Dy2 and Dy3) in 4. |
Due to the magnetic anisotropy present in both sets of compounds, ac susceptibility measurements were performed under zero dc fields. There is no out-of-phase signal shown above 1.8 K for compounds 1 and 3. However, in the case of compound 2, both temperature- and frequency-dependent in-phase, χ′, and out-of-phase, χ′′, signals are detected, indicating slow relaxation of its magnetisation. The temperature-dependent χ′′ signals showed no maximum, but some shoulders were observed, indicating the presence of quantum tunnelling effects with more than one relaxation process involved in this system (Fig. S2†). However, clear maxima were observed in the frequency-dependent χ′′ signals (Fig. 6) and the Cole–Cole plots (Fig. S3†) can be fitted to a generalised Debye function resulting in α = 0.05–0.16, demonstrating that there is only one relaxation process in this system. Fitting the frequency-dependent ac susceptibility data of 2 with an Arrhenius law leads to the characteristic SMM energy barrier, Ueff, of 7.1 K and the relaxation time, τ0, of 6.4 × 10−6 s (Fig. S4†).
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Fig. 6 Frequency dependence of the in-phase (χ′) (left) and out-of-phase (χ′′) (right) ac susceptibility components at the indicated temperatures in zero dc field for 2. |
In order to further study this system and check for any quantum tunnelling effect above 1.8 K, the frequency dependence of the ac susceptibility was measured under different applied dc fields at 1.8 K. As shown in Fig. S5,† the maximum value in the frequency dependent out-of-phase plot increases from 110 Hz at 500 Oe to a value of 884 Hz at 2000 Oe and then slightly decreases. This observation suggests that the magnetic relaxation can be slowed down by the application of the external dc fields. Thus, ac data were collected with an applied dc field of 500 Oe and clear maxima were detected on both χ′′ vs. T (Fig. S6†) and χ′′ vs. v (Fig. 7) data. The characteristic relaxation times (τ) were determined from the frequency dependence of the out-of-phase susceptibility. Fitting the data by an Arrhenius law leads to an estimation of the energy gap Ueff = 18.4 K and the relaxation time τ0 = 2.0 × 10−7 s (Fig. S7†), which further confirmed that a small external dc field slowed down the relaxation time by suppressing quantum tunnelling of magnetization.
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Fig. 7 Frequency dependence of the in-phase (χ′) (left) and out-of-phase (χ′′) (right) ac susceptibility components at the indicated temperatures under 500 Oe dc field for 2. |
The ac susceptibility measurement for 4 in zero dc field shows very weak out-of-phase ac signals. However, under a dc field of 1000 Oe, a clear maximum is detected on the χ′′ vs. ν plot (Fig. 8). Fitting the data by an Arrhenius law leads to an estimation of the energy gap Ueff = 17.1 K and the relaxation time τ0 = 7.4 × 10−8 s (Fig. S8†).
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Fig. 8 Frequency dependence of the in-phase (χ′) (left) and out-of-phase (χ′′) (right) ac susceptibility components at the indicated temperatures under 1000 Oe dc field for 4. |
We acknowledge the Synchrotron Light Source ANKA for provision of instruments at the SCD beamline for the structural determination of compound 1, and we would like to thank Dr Gernot Buth for assistance in using the beamline.
Footnote |
† Electronic supplementary information (ESI) available. CCDC 1429780 and 1429781. For ESI and crystallographic data in CIF or other electronic format see DOI: 10.1039/c5dt03909f |
This journal is © The Royal Society of Chemistry 2016 |