Literature DB >> 35971413

Constructing "Closed" and "Open" {Mn8} Clusters.

Thomais G Tziotzi1, Athanasios Mavromagoulos2, Mark Murrie2, Scott J Dalgarno3, Marco Evangelisti4, Euan K Brechin5, Constantinos J Milios1.   

Abstract

Use of the 1,3,5-tri(2-hydroxyethyl)-1,3,5-triazacyclohexane ligand, LH3, in manganese chemistry affords access to two structurally related {Mn8} clusters: a "closed" {MnIII 6MnII 2} puckered square wheel of formula [Mn8L2(LH)O3(OH)2(MeO)2Br(imH)(H2O)3](Br)3 (1; imH = imidazole) and an "open" {MnIII 8} rod of formula [MnΙΙΙ 8L2O4(aibH)2(aib)2(MeO)6(MeOH)2](NO3)2 (2, aibH = 2-amino-isobutyric acid). In each case the triaza ligands, L/LH, direct the formation of {Mn3} triangles with their N atoms preferentially bonding to the Jahn-Teller axes of the MnIII ions. Subsequent self-assembly is dependent on the anion of the Mn salt and the identity of the organic coligand employed-the terminally bonded imidazole and the chelating/bridging amino acid. The {Mn3} triangles fold up on themselves in 1, forming a wheel. However, the syn, syn-bridging carboxylates in 2 prevent this from happening, instead directing the formation of a linear rod. Magnetic susceptibility and magnetization measurements reveal competing ferro- and antiferromagnetic interactions in both complexes, the exchange being somewhat weaker in 1 due to the presence of MnII ions.
© 2022 The Authors. Published by American Chemical Society.

Entities:  

Year:  2022        PMID: 35971413      PMCID: PMC9374326          DOI: 10.1021/acs.cgd.2c00489

Source DB:  PubMed          Journal:  Cryst Growth Des        ISSN: 1528-7483            Impact factor:   4.010


Introduction

The chemistry of polymetallic manganese compounds constitutes a vibrant and growing area of research that has characterized species of nuclearities up to 84.[1] These aesthetically pleasing structures represent a breadth of metallic topologies constructed from both mono- and multimetallic building blocks.[2−4] Those of low nuclearity have been proposed as mimics for the active site of Photosystem II in which a pentanuclear [Mn4Ca] complex is responsible for the oxidative splitting of water to molecular oxygen, protons, and electrons, upon solar irradiation.[5−14] Manganese clusters of all nuclearities have also been at the heart of molecular magnetism, having provided the prototype single-molecule magnet, [Mn12], which gave rise to an exciting research area that persists to this day.[15−18] Given that the topology of a polymetallic cluster depends on the identity and oxidation state of the metal ion, the presence/absence of oxide/hydroxide ions, the coordination ability/directionality of the organic/inorganic ligands used, and subtle changes in the reaction conditions employed, exploring the coordination chemistry of newly designed ligands alongside physical characterization of the products made remains a key initial step. This remains fundamentally important for the development of magneto-structural correlations, which play a pivotal role in understanding the structural factors underpinning magnetic behavior, a prerequisite for any potential application.[19] Following this approach, we report the synthesis of two related octanuclear Mn clusters upon employment of the ethanolamine-containing ligand 1,3,5-tri(2-hydroxyethyl)-1,3,5-triazacyclohexane ligand, LH3, (Scheme ), as a means of further investigating and expanding the chemistry and coordination ability of this ligand.[20−22]
Scheme 1

Ligand 1,3,5-Tri(2-hydroxyethyl)-1,3,5-triazacyclohexane, LH3, and Its Coordination Modes Found in 1 and 2

Experimental Section

All synthetic procedures were performed under aerobic conditions using materials and solvents as received. LH3 was prepared as previously reported.[23]

[Mn8L2(LH)O3(OH)2(MeO)2Br(imH)(H2O)3](Br)3 (1)

MnBr2·4H2O (0.5 mmol, 143 mg), LH3 (0.5 mmol, 109 mg), NEt3 (1.5 mmol), and imidazole (imH, 0.5 mmol, 34 mg) were stirred in MeCN/MeOH (1:1, 20 mL), forming a pale olive-brown solution that was left stirring for 45 min at room temperature. The resulting dark brown solution was then filtered and left undisturbed to evaporate slowly at room temperature. Dark brown single crystals suitable for X-ray crystallography were formed after 4 d in 30–35% yield. Anal. Calcd for C32H71Br4Mn8N11O19 (1): C, 22.97; H, 4.28; N, 9.21%. Found: C, 23.09; H, 4.17; N 9.03%.

[MnΙΙΙ8L2O4(aibH)2(aib)2(MeO)6(MeOH)2](NO3)2 (2)

Mn(NO3)2·6H2O (0.5 mmol, 143 mg), LH3 (0.5 mmol, 109 mg), 2-amino-isobutyric acid (aibH, 0.25 mmol, 25.7 mg), and NEt3 (1.5 mmol) were added in MeOH (20 mL), and the resulting dark brown solution was left to stir for 45 min. The solution was then filtered and left undisturbed to evaporate at room temperature. Dark brown single crystals suitable for X-ray crystallography were formed after 5 d in 35–40% yield. Anal. Calcd for C42H96Mn8N12O32 (2): C, 29.32; H, 5.62; N, 9.77%. Found: C, 29.20; H, 5.51; N 9.86%.

Physical Methods

Elemental analyses (C, H, N) were performed by the University of Ioannina microanalysis service. Variable-temperature, solid-state direct current (dc) magnetic susceptibility data were collected on a Quantum Design MPMS-XL magnetometer at the University of Zaragoza and a Quantum Design MPMS3 magnetometer at the University of Glasgow. Diamagnetic corrections were applied to the observed paramagnetic susceptibilities using Pascal’s constants. Powder X-ray diffraction (PXRD) measurements were collected on freshly prepared samples of the complexes on a PANanalytical X’Pert Pro MPD diffractometer at the University of Crete.

Single-Crystal X-ray Diffraction

Diffraction data for 1 and 2 were collected on a Bruker D8 Venture diffractometer (University of Crete), equipped with a PHOTION II CPAD detector at 210 and 200 K, respectively. Hydrogen atoms were modeled in idealized geometries, except those of waters of crystallization, which were located in the Fourier maps. Data collection parameters and structure solution and refinement details are presented in Table S1, while full crystallographic details may be found in the Supporting Information (CIF files with CCDC reference numbers 2159430 and 2159431 correspond to 1 and 2, respectively).

Results and Discussion

Synthesis

The 1:1 reaction of MnBr2·4H2O with LH3 in a basic MeOH/MeCN solution, and in the presence of imidazole, imH, leads to the formation of black crystals of [MnIII6MnII2L2(LH)O3(OH)2(MeO)2Br(imH)(H2O)3](Br)3 (1) after 4 d in good yield. Complex 1 is a mixed-valent octanuclear complex. Base-assisted aerial oxidation of the Mn(II) ions occurs readily, even in the presence of the mildly reducing Br– ions. Interestingly, attempts to change the identity of the product and the MnIII/MnII ratio by changing reaction conditions and reactant stoichiometry failed. Indeed compound 1 was isolated in all cases, as evidenced by a PXRD comparison between 1 and the crystalline materials obtained, perhaps highlighting the stability of the structure. Analogous reactions under solvothermal conditions led to amorphous (pale brown) powders and/or the dissociation of the LH3 ligand to its component parts.[24] This appears to be a common theme in the chemistry of LH3, and it may be attributed to the reducing environment created by the high-pressure/temperature conditions in the autoclave. With the identity and structure of 1 established (vide infra) the next step was to attempt to replace the terminally bonded imidazole ligand with a bridging ligand, in this case 2-amino-isobutyric acid, to examine how this would affect the self-assembly process. Thus, the reaction between Mn(NO3)2·6H2O, LH3, and aibH in a basic MeOH solution affords the octanuclear complex [MnΙΙΙ8L2O4(aibH)2(aib)2(MeO)6(MeOH)2](NO3)2 (2). The Mn ions in 2 are all in the 3+ oxidation state, and the triaza ligands are now fully deprotonated, with the cluster adopting a different topology to that seen in 1, in which analogous building blocks have self-assembled in a different manner. As with complex 1, changing reaction conditions and reactant stoichiometry did not lead to the isolation of any other crystalline species.

Description of Structures

Complex 1 crystallizes in the orthorhombic space group P212121. The metallic skeleton (Figure ) of the cluster describes a wheel of vertex-sharing {Mn3} triangles or, alternatively, a “closed”, puckered, square [MnIII6MnII2] wheel, with the two divalent Mn ions (Mn8 and Mn4) located on opposite sides of the square. Its metal–oxygen core consists of a twisted, asymmetric {MnIII6MnII2(μ3-O)3(μ3-OH)(μ-ΟΗ)(μ-OMe)2(μ-OR)6}6+ unit in which the Mn ions forming the square [MnIII6MnII2] core are bridged by a combination of oxide, hydroxide, and alkoxide groups. More specifically, in the upper and lower corners of the square wheel, the two groups of three MnIII centers (Mn1, Mn2, Mn3 and Mn5, Mn6, Mn7) are bridged by one μ3-O2– (O4 and O13, respectively), one μ-OMe (O5 and O14, respectively), and one μ-OR (O6 and O8, respectively). In the left corner of the square wheel, consisting of Mn5, Mn3, and Mn8, the Mn centers are bridged by one μ3-OH– (O16), one μ-OH– (O15), and two μ-OR groups. The right corner of the square wheel, consisting of Mn1, Mn4, and Mn7, is held together by one μ3-O2– (O9) and two μ-OR (O1, O12) bridges. The ligand is found in its fully deprotonated L3– and partially deprotonated LH2– forms, adopting the η2:η2:η1:η1:η1:η1:μ5 coordination mode in both cases. The assignment of the Mn oxidation states was performed on the basis of bond valence sum (BVS) calculations (Table S2) and the appearance of Jahn–Teller (JT) axes for the six-coordinate trivalent metal ions. Αll the Mn ions are six-coordinate, with the exception of Mn8, which is five-coordinate, adopting a trigonal bipyramidal geometry. The coordination sphere of Mn8 is completed by the presence of one terminal Br– anion and one terminal imH ligand. The structure of 1 displays two very interesting features: (i) the N atoms of the L3–/LH2– ligands prefer bonding to the JT positions of the MnIII ions, creating triangular building blocks, as has been previously reported,[20−22] which self-assemble via vertex sharing, and (ii) the metallic skeleton of 1 describes half the metallic skeleton of the recently reported complex [MnIII12MnII6(O)6(OH)2(OMe)6(L)4(LH)2Br12][22] (Figure S1) likely due to the presence of the terminal imH/Br– ligands on Mn8 blocking the dimerization.
Figure 1

Molecular structure of the trication of 1 (left) and its metal–oxygen core (right). Color code: MnIII = purple, MnII = orange, O = red, N = blue, C = gray, Br = yellow. H atoms are omitted for clarity.

Molecular structure of the trication of 1 (left) and its metal–oxygen core (right). Color code: MnIII = purple, MnII = orange, O = red, N = blue, C = gray, Br = yellow. H atoms are omitted for clarity. The terminal bonded H2O ligand and the monodentate O arm of the LH ligand on Mn6 are H-bonded to the equivalent atoms on Mn2 on neighboring clusters (O(H)···O, ∼2.6 Å), with the former also being H-bonded to the Br counteranions (O(H)···Br, ∼2.6 Å). The result is the formation of H-bonded zigzag chains of clusters running along the b-axis of the cell in the extended structure (Figure S2). Complex 2 crystallizes in the triclinic space group P1̅. Its metallic skeleton (Figure ) describes six edge-sharing triangles arranged in an “open” or rod-like fashion and possessing a {MnIII8(μ3-O)4(μ3-OMe)2(μ-OR)2(μ-OMe)2} core. The ligand is found in its fully deprotonated form, L3–, adopting an η2:η1:η1:η1:η1:η1:μ4 bonding mode, “capping” a metallic {Mn3} triangle via the three N atoms and two monodentate arms, and further bridging to a central Mn ion through the remaining arm. Two of the amino acid ligands are found in the zwitterionic form, aibH, adopting an η1:η1:μ coordination mode, while the remaining two ligands are in the monoanionic form, aib–, and bonding in chelate fashion forming a five-membered ring via the amino group and one Ocarboxylate atom. All the Mn ions are in the 3+ oxidation state (Table S2), six-coordinate, and in distorted octahedral geometries, with their JT axes being approximately coparallel, lying perpendicular to the mean plane of the {Mn8} rod. As in 1, the N atoms of the L3– ligand display a preference for occupying solely the JT positions on the MnIII ions, creating [Mn3] triangular building blocks. However, on this occasion they self-assemble in a linear fashion rather than “wrapping up” to form a wheel, as illustrated in Figure . Given the similarity of the reactions, this suggests the process is governed to a large extent by the nature and bonding preferences of the different organic coligands employed. For example, the presence of the syn, syn-bridging carboxylates in 2 may favor the assembly of a more linear cluster through a promotion of edge-sharing rather than vertex-sharing triangles, preventing cyclization (Figure ).
Figure 2

Molecular structure of the dication of 2 highlighting the capping mode of the L3– ligand (top) and its metallic skeleton (bottom). Color code: MnIII = purple, MnII = orange, O = red, N = blue, C = gray. H atoms are omitted for clarity.

Figure 3

A comparison of the “wrapped” vs “linear” octametallic cores of 1 (left) and 2 (right).

Molecular structure of the dication of 2 highlighting the capping mode of the L3– ligand (top) and its metallic skeleton (bottom). Color code: MnIII = purple, MnII = orange, O = red, N = blue, C = gray. H atoms are omitted for clarity. A comparison of the “wrapped” vs “linear” octametallic cores of 1 (left) and 2 (right). The NH3+ moiety of the zwitterionic, bridging aibH ligand is H-bonded to the terminally bonded O arm of the chelating aib ligand in the same molecule (N(H)···O, ∼2.9 Å). They are also H-bonded to the MeOH molecules of crystallization (N(H)···O, ∼2.9 Å) and to the non-coordinating carboxylate O atom of an aibH ligand on a neighboring molecule (N(H)···O, ∼2.8 Å). The latter results in the formation of staggered chains of clusters in the extended structure of 2 (Figure S3).

Magnetic Properties

Variable-temperature dc magnetic susceptibility data were collected for microcrystalline samples of 1 and 2 in the temperature range 2–300 K under an applied magnetic field of 0.1 T and are plotted as the χT product versus T in Figure . The purity of the samples were confirmed by means of PXRD comparison with the simulated data from the single-crystal structures (Figure S4). For both complexes, the room-temperature values of χT (1, 23.08 cm3 K mol–1, 2: 19.31 cm3 K mol–1) are slightly lower than the theoretical values expected for non-interacting [MnIII6MnII2] (26.75 cm3 K mol–1) and [MnIII8] (24.00 cm3 K mol–1) units, respectively, assuming g = 2.00. Both complexes show similar variable-temperature behavior: when cooled, χT decreases steadily before it plateaus between 50 and 10 K for 1 at 14.5 cm3 mol–1 K and between 100 and 10 K for 2 at ∼13.4 cm3 K mol–1. Below 10 K, χT decreases rapidly to values of ∼12.4 cm3 K mol–1 (1) and ∼11.6 (2) cm3 K mol–1. This behavior suggests the dominance of relatively strong antiferromagnetic exchange interactions in both 1 and 2 with the plateaus attributed to competing ferro- and antiferromagnetic interactions within the clusters. The exchange appears to be weaker in 1 than 2, which is likely due to the presence of the MnII ions, which are known to mediate rather weak nearest-neighbor exchange coupling.[25,26]
Figure 4

Temperature dependence of the χT product, where χ is the dc molar magnetic susceptibility, for 1 and 2, as labeled, collected in an applied magnetic field of B = 0.1 T.

Temperature dependence of the χT product, where χ is the dc molar magnetic susceptibility, for 1 and 2, as labeled, collected in an applied magnetic field of B = 0.1 T. Low-temperature, variable-temperature, and variable-field magnetization data were measured for both clusters in the temperature range 2–10 K and in magnetic fields up to 5 T (Figure ). At the lowest temperature and highest field measured, M reaches values of ∼15.2 and ∼7.7 μB for 1 and 2, respectively. This is indicative of the presence of dominant antiferromagnetic exchange and relatively small spin ground states, in agreement with the susceptibility data and previous magneto-structural correlations of alkoxide-bridged [MnIII2] dimers with parallel JT axes oriented perpendicular to the bridging plane (Type I dimers)[27,28] and related complexes.[29,30] The large nuclearity and complicated topology/structure of the two compounds precludes any quantitative analysis of the data. No out-of-phase ac susceptibility signals were detected under zero-applied dc fields for either complex.
Figure 5

Isothermal molar magnetization M vs applied magnetic field data for 1 (left) and 2 (right), collected for T = 2, 5, and 10 K, as labeled.

Isothermal molar magnetization M vs applied magnetic field data for 1 (left) and 2 (right), collected for T = 2, 5, and 10 K, as labeled.

Conclusions

Replacing imH with aibH in the reaction between a MnII salt and LH3 leads to the formation of a linear [Mn8] “rod” rather than a [Mn8] “wheel”. The building blocks in each case are {MnIII3} triangles directed by the L/LH ligands, which preferentially bond to the JT axes of the MnIII ions. The subsequent self-assembly process is then dictated by the anion of the Mn salt (Br– vs NO3–) and the organic coligands employed, with the latter clearly having a huge influence on topology. While the Br– and imH ligands are monodentate, allowing the {Mn3} triangles to self-assemble via vertex sharing into a wheel, the syn, syn-bridging aib and chelating aibH ligands direct the formation of a linear or rod-like structure containing edge-sharing {Mn3} triangles. The presence of the aibH coligand also leads to an increased oxidation state level in 2 ([MnIII8]) versus 1 ([MnIII6MnII2]) and an increased oxide content. The magnetic behavior of the two complexes is, perhaps unsurprisingly, rather similar but with the MnII ions in 1 leading to a weaker antiferromagnetic exchange than that present in 2. The structural similarity of 1 and 2 with previously published structures of LH3[20−22] highlights the dominant topological role played by the ligand, which makes understanding and exploiting self-assembly processes somewhat simpler. In turn, this should allow for the synthesis of more targeted species.
  23 in total

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5.  What Controls the Magnetic Exchange and Anisotropy in a Family of Tetranuclear {Mn2IIMn2III} Single-Molecule Magnets?

Authors:  Kuduva R Vignesh; Stuart K Langley; Christopher J Gartshore; Boujemaa Moubaraki; Keith S Murray; Gopalan Rajaraman
Journal:  Inorg Chem       Date:  2017-02-03       Impact factor: 5.165

6.  A [Mn18] wheel-of-wheels.

Authors:  Marco Coletta; Thomais G Tziotzi; Mark Gray; Gary S Nichol; Mukesh K Singh; Constantinos J Milios; Euan K Brechin
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7.  What controls the magnetic interaction in bis-μ-alkoxo Mn(III) dimers? A combined experimental and theoretical exploration.

Authors:  Nelly Berg; Thayalan Rajeshkumar; Stephanie M Taylor; Euan K Brechin; Gopalan Rajaraman; Leigh F Jones
Journal:  Chemistry       Date:  2012-03-29       Impact factor: 5.236

8.  A family of manganese rods: syntheses, structures, and magnetic properties.

Authors:  Gopalan Rajaraman; Muralee Murugesu; E Carolina Sañudo; Monica Soler; Wolfgang Wernsdorfer; Madeleine Helliwell; Chris Muryn; Jim Raftery; Simon J Teat; George Christou; Euan K Brechin
Journal:  J Am Chem Soc       Date:  2004-12-01       Impact factor: 15.419

9.  Emissive {Mn4(III)Ca} clusters with square pyramidal topologies: syntheses and structural, spectroscopic, and physicochemical characterization.

Authors:  Alysha A Alaimo; Daisuke Takahashi; Luís Cunha-Silva; George Christou; Theocharis C Stamatatos
Journal:  Inorg Chem       Date:  2014-12-05       Impact factor: 5.165

10.  The first amino acid bound manganese-calcium clusters: a {[MnCa]2} methylalanine complex, and a [MnCa] trigonal prism.

Authors:  Thomais G Tziotzi; Evangelos K Andreou; Eirini Tzanetou; Dimitris A Kalofolias; Daniel J Cutler; Marek Weselski; Milosz Siczek; Tadeusz Lis; Euan K Brechin; Constantinos J Milios
Journal:  Dalton Trans       Date:  2020-07-22       Impact factor: 4.390

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