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Article

Rare Nuclearities and Unprecedented Structural Motifs in Manganese Cluster Chemistry from the Combined Use of Di-2-Pyridyl Ketone with Selected Diols †

by
Katerina Skordi
1,
Dimitris I. Alexandropoulos
1,
Adeline D. Fournet
2,‡,
Nikos Panagiotou
1,
Eleni E. Moushi
3,
Constantina Papatriantafyllopoulou
1,§,
George Christou
2 and
Anastasios J. Tasiopoulos
1,*
1
Department of Chemistry, University of Cyprus, 1678 Nicosia, Cyprus
2
Department of Chemistry, University of Florida, Gainesville, FL 32611, USA
3
Department of Life Sciences, School of Science, European University Cyprus, 1516 Nicosia, Cyprus
*
Author to whom correspondence should be addressed.
Dedicated to Professor Spyros P. Perlepes, an excellent scientist, great teacher, valuable collaborator, and dear friend, on the occasion of his 70th birthday.
Current address: Intel Corporation, Hillsboro, OR 97124, USA.
§
Current address: School of Biological and Chemical Sciences, College of Science and Engineering, University of Galway, University Road, H91 TK33 Galway, Ireland.
Chemistry 2023, 5(3), 1681-1695; https://doi.org/10.3390/chemistry5030115
Submission received: 3 July 2023 / Revised: 25 July 2023 / Accepted: 27 July 2023 / Published: 1 August 2023

Abstract

:
The combined use of di-2-pyridyl ketone ((py)2CO) with various diols in Mn cluster chemistry has afforded five new compounds, namely, [Mn11O2(OH)2{(py)2CO2}5(pd)(MeCO2)3(N3)3(NO3)2(DMF)4](NO3)∙2DMF∙H2O (1∙2DMF∙H2O), [Mn11O2(OH)2{(py)2CO2}5(mpd)(MeCO2)3(N3)3(NO3)2(DMF)4](NO3) (2), [Mn12O4(OH)2{(py)2CO2}4(mpd)2(Me3CCO2)4(NO3)4(H2O)6](NO3)2∙2MeCN (3∙2MeCN), [Mn4(OMe)2{(py)2C(OMe)O}2(2-hp)2(NO3)2(DMF)2] (4), and [Mn7{(py)2CO2}4(2-hp)4(NO3)2(DMF)2](ClO4)∙DMF (5∙DMF) ((py)2CO22− and (py)2C(OMe)O = gem-diol and hemiketal derivatives of di-2-pyridyl ketone, pdH2 = 1,3-propanediol, mpdH2 = 2-metly-1,3-propanediol, 2-hpH2 = 2-(hydroxymethyl)phenol). Complexes 1 and 2 are isostructural, possessing an asymmetric [MnIII5MnII64-O)(μ3-O)(μ3-OH)(μ-OH)(μ3-OR)2(μ-OR)10(μ-N3)]8+ core. Compound 3 is based on a multilayer [MnIII8MnII44-O)23-O)23-OH)2(μ-OR)12]10+ core, while complex 4 comprises a defective dicubane core. The crystal structure of 5 reveals that it is based on an unusual non-planar [MnIII5MnII2(μ-OR)12]7+ core with a serpentine-like topology. Direct current (dc) magnetic susceptibility studies revealed the presence of dominant antiferromagnetic exchange interactions in complex 3, while ferromagnetic coupling between the Mn ions was detected in the case of compound 5. Fitting of the magnetic data for complex 4 revealed weak antiferromagnetic interactions along the peripheral MnII∙∙∙MnIII ions (Jwb = −0.33 (1) cm−1) and ferromagnetic interactions between the central MnIII∙∙∙MnIII ions (Jbb = 6.28 (1) cm−1).

Graphical Abstract

1. Introduction

Polynuclear coordination complexes of paramagnetic 3d metal ions have become the focus of intense investigation over the last few decades since they often possess interesting physical properties and fascinating structural features [1,2,3,4,5]. Among other 3d metals, manganese-containing compounds have been of great interest due to the ability of Mn ions to adopt a variety of oxidation states (i.e., II, III, and IV) and form high nuclearity metal-oxo clusters that can find applications in different research fields, including bioinorganic chemistry [6,7,8,9], materials science [10,11,12], and molecular magnetism [13,14,15]. In the latter case, Mn clusters hold a special place since they often possess a large number of unpaired electrons, and, in the presence of ferromagnetic exchange interactions, they can act as high spin molecules and/or magnetic refrigerants [16,17,18]. In addition, the combination of high spin ground state values (S) with significant uniaxial magnetic anisotropy (D), which in the case of Mn compounds is usually the result of Jahn–Teller (JT) axial elongation of MnIII ions in octahedral environments, can lead to single-molecule magnetism (SMM) behaviour [19,20,21]. SMMs are discrete species that can exhibit the properties of bulk magnets, but at the molecular level. Thus, SMMs display slow magnetic relaxation below a characteristic blocking temperature (TB) due to a significant energy barrier (Ueff) to reversal of the magnetization vector [22]. However, reorientation of magnetization cannot occur only by overcoming the Ueff barrier, but also through the barrier via quantum tunnelling of the magnetization (QTM) [23]. As a result of the coexistence of classical and quantum natures in such individual molecules, SMMs have been proposed for a variety of potential applications including high-density memory storage devices [24,25], quantum computing [23,26,27,28], and spintronics [29,30,31,32].
The synthesis of several Mn SMMs, including the first one [Mn12O12(OAc)16(H2O)4] [33,34], triggered interest in this area, and led to several new clusters and many synthetic strategies. As a result, Mn clusters with enhanced magnetic properties and impressive crystal structures have been reported, including the giant [Mn84] [35,36] and [Mn70] [36,37] torus-like complexes, which are the highest nuclearity 3d SMMs, and the [Mn49] aggregate [38], possessing a highly symmetric cuboctahedral core. These results demonstrate the special role of manganese in nanoscience and molecular magnetism, and to some extent explain why synthetic efforts are still focusing on the isolation of new Mn clusters. For these reasons, our group has had a continuing interest in the synthesis of polynuclear Mn complexes with novel structural characteristics, including large size, high nuclearities, highly symmetric metal cores, and interesting magnetic properties. To that end, we have employed several organic chelating/bridging ligands with different functionalities like (poly)alcohols [39,40,41,42] or oximates as primary organic ligands or combinations of them, following a mixed ligand approach [43,44,45]. Recently, these efforts were extended towards the combined use of another well-known chelate with a fruitful coordination chemistry, (py)2CO, with various aliphatic diols. This ligand has afforded numerous metal clusters, mainly because of the ability of its carbonyl group to undergo metal-assisted hydrolysis or alcoholysis (ROH; R = Me, Et), forming the anionic (py)2CO22− (gem-diol form) and (py)2C(OR)O (hemiketal form) groups displaying unique bridging capabilities, as illustrated by a series of studies, several of which were reported by S. P. Perlepes and coworkers [46,47,48,49]. Thus, studies from our group have shown that the combination of (py)2CO with aliphatic diols has led to the isolation of a new family of [Mn4M2] (M = Mn or Dy, Gd, Tb) complexes, possessing an uncommon cross-shaped core [50], and the highly symmetric [Mn24] and [Mn23] supertetrahedral T4 aggregates [51].
Herein, we report five new compounds obtained from reactions involving the combination of (py)2CO with selected diols in Mn cluster chemistry. In particular, the combination of (py)2CO and 1,3-propanediol (pdH2) or 2-methly-1,3-propanediol (mpdH2) afforded complexes [Mn11O2(OH)2{(py)2CO2}5((m)pd)(MeCO2)3(N3)3(NO3)2(DMF)4](NO3) (1 and 2) and [Mn12O4(OH)2{(py)2CO2}4(mpd)2(Me3CCO2)4(NO3)4(H2O)6](NO3)2∙2MeCN (3∙2MeCN), whereas the use of (py)2CO in conjunction with the aromatic diol 2-(hydroxymethyl)phenol (2-hpH2) led to [Mn4(OMe)2{(py)2C(OMe)O}2(2-hp)2(NO3)2(DMF)2] (4) and [Mn7{(py)2CO2}4(2-hp)4(NO3)2(DMF)2](ClO4)∙DMF (5∙DMF). Interestingly, complexes 1, 2, 3, and 5 possess uncommon metal cores which, to our knowledge, are reported for the first time in Mn cluster chemistry. The magnetic properties of compounds 35 were investigated through direct current (dc) magnetic susceptibility measurements, revealing the presence of dominant antiferromagnetic exchange interactions in complexes 3 and 4, and ferromagnetic ones in 5.

2. Materials and Methods

2.1. Materials, Physical and Spectroscopic Measurements

All manipulations were performed under aerobic conditions using materials (reagent grade) and solvents as received. Caution: Although no such behaviour was observed during the present work, perchlorate, nitrate, and azide salts are potentially explosive; they should be synthesized and used in small quantities and treated with care. Elemental analysis (C, H, and N) was performed by the in-house facilities of the University of Cyprus, Chemistry Department. IR spectra were recorded on ATR in the 4000–400 cm−1 range using a Shimadzu Prestige—21 spectrometer. Variable-temperature dc and ac magnetic susceptibility data were collected at the University of Florida using a Quantum Design MPMS-XL SQUID magnetometer equipped with a 7 T magnet and operating in the 1.8–400 K range. Samples were embedded in solid eicosane to prevent torquing. The ac magnetic susceptibility measurements were performed in an oscillating ac field of 3.5 G and a zero dc field. The oscillation frequencies were in the 5–1488 Hz range. Pascal’s constants [52] were used to estimate the diamagnetic corrections, which were subtracted from the experimental susceptibilities to give the molar paramagnetic susceptibility (χM). The program PHI [53] was used to fit the magnetic data.

2.2. Syntheses

[Mn11O2(OH)2{(py)2CO2}5(pd)(MeCO2)3(N3)3(NO3)2(DMF)4](NO3)∙2DMF∙H2O (1∙2DMF∙H2O). Solid Mn(NO3)2·4H2O (0.75 g, 2.99 mmol) was added to a stirred solution of pdH2 (0.30 mL, 0.32 g, 4.15 mmol) and NEt3 (0.28 mL, 0.20 g, 2.01 mmol) in DMF (20 mL). To this solution was then added solid (py)2CO (0.10 g, 0.54 mmol), MeCO2Na (0.08 g, 0.98 mmol), and NaN3 (0.07 g, 1.08 mmol) under continuous stirring. The resulting brown solution was stirred for 1 h, filtered, and the filtrate layered with Et2O (1:3 v/v). Slow mixing gave after 1 week dark red/brown crystals of 1, which were kept in mother liquor for X-ray analysis, or collected by filtration and dried under vacuum for other solid-state studies. Yield: ~5%. Anal. Calc. (found) for C82H101N28O38Mn11 (1·2DMF·H2O): C, 36.60 (36.36), H, 3.78 (3.92), N, 14.57 (14.39)%. Selected IR data (KBr, cm−1): 3352 (sb), 2982 (m), 2932 (m), 2886 (m), 2750 (w), 2706 (w), 2482 (w), 2425 (w), 2359 (w), 2342 (w), 2118 (w), 2070 (m), 1763 (w), 1663 (m), 1584 (s), 1477 (m), 1377 (s), 1240 (m), 1157 (w), 1074 (m), 1047 (m), 1015 (m), 928 (w), 814 (m), 758 (m), 694 (m), 644 (m), 629 (s), 575 (m), 513 (m), 411 (w).
[Mn11O2(OH)2{(py)2CO2}5(mpd)(MeCO2)3(N3)3(NO3)2(DMF)4](NO3) (2). This compound was prepared in the same manner as complex 1, but by using mpdH2 (0.30 mL, 0.30 g, 3.38 mmol) in place of pdH2. After 1 week, dark red/brown crystals of 2 had appeared, which were kept in mother liquor for X-ray analysis, or collected by filtration and dried under vacuum for other solid-state studies. Yield: ~5%. Anal. Calc. (found) for C77H87N26O35Mn11 (2): C, 36.40 (36.27), H, 3.45 (3.24), N, 14.33 (14.08)%. Selected IR data (KBr, cm−1): 3553 (s), 3414 (sb), 3136 (s), 2828 (m), 2779 (m), 2029 (w), 1780 (m), 1710 (s), 1639 (s), 1618 (s), 1402 (s), 1242 (w), 1117 (w), 1082 (w), 1057 (w), 835 (w), 766 (m), 613 (m), 530 (m), 478 (m).
[Mn12O4(OH)2{(py)2CO2}4(mpd)2(Me3CCO2)4(NO3)4(H2O)6](NO3)2∙2MeCN (3∙2MeCN). Solid Mn(NO3)2·4H2O (0.75 g, 2.99 mmol) was added to a stirred solution of mpdH2 (0.30 mL, 0.30 g, 3.38 mmol) and NEt3 (0.28 mL, 0.20 g, 2.01 mmol) in MeCN (20 mL). To this solution was then added solid (py)2CO (0.10 g, 0.54 mmol), and Me3CCO2Na (0.12 g, 0.97 mmol) under continuous stirring. The resulting brown solution was stirred for 1 h, filtered, and the filtrate left undisturbed at room temperature. After 2 weeks, dark brown crystals of 3 appeared, which were kept in mother liquor for X-ray analysis, or collected by filtration and dried under vacuum for other solid-state studies. Yield: ~59%. Anal. Calc. (found) for C76H104N16O50Mn12 (3·2MeCN): C, 33.80 (33.65), H, 3.88 (3.67), N, 8.30 (8.06)%. Selected IR data (KBr, cm−1): 3383 (mb), 2959 (m), 2874 (w), 2371 (w), 1765 (w), 1599 (m), 1560 (m), 1477 (m), 1437 (m), 1360 (s), 1298 (m), 1223 (m), 1155 (w), 1119 (m), 1078 (m), 1032 (s), 891 (w), 814 (w), 783 (m), 756 (w), 694 (m), 681 (m), 635 (m), 559 (m), 511 (w), 459 (w), 415 (w).
[Mn4(OMe)2{(py)2C(OMe)O}2(2-hp)2(NO3)2(DMF)2] (4). Solid Mn(NO3)2·4H2O (0.75 g, 2.99 mmol) was added to a stirred solution of 2-hpH2 (0.20 g, 1.61 mmol), (py)2CO (0.10 g, 0.54 mmol) and NEt3 (0.28 mL, 0.20 g, 2.01 mmol) in a mixture of MeOH/DMF (1/1; 20 mL). The resulting brown solution was stirred for 30 min, filtered, and the filtrate layered with Et2O (1:3 v/v). Slow mixing gave, after 1 week, dark brown crystals of 4, which were kept in mother liquor for X-ray analysis, or collected by filtration and dried under vacuum for other solid-state studies. Yield: ~47%. Anal. Calc. (found) for C46H54N8O18Mn4 (4): C, 45.04 (45.19), H, 4.44 (4.21), N, 9.13 (8.98)%. Selected IR data (KBr, cm−1): 3419 (sb), 3139 (sb), 2960 (m), 2926 (m), 2819 (m), 2426 (w), 1734 (w), 1661 (s), 1601 (m), 1569 (w), 1474 (s), 1448 (s), 1435 (s), 1385 (s), 1313 (w), 1274 (m), 1260 (w), 1232 (w), 1222 (w), 1154 (w), 1113 (w), 1048 (m), 1026 (m), 990 (w), 935 (w), 881 (w), 783 (w), 762 (w), 725 (w), 682 (w), 635 (w), 620 (m), 575 (m), 542 (w), 517 (w), 469 (w) 455 (w), 449 (w).
[Mn7{(py)2CO2}4(2-hp)4(NO3)2(DMF)2](ClO4)∙3DMF∙H2O (5∙DMF). This compound was prepared in the same manner as complex 4, but by adding extra NaClO4 (0.14 g, 1.0 mmol). After 1 week, dark brown crystals of 5 appeared, which were kept in mother liquor for X-ray analysis, or collected by filtration and dried under vacuum for other solid-state studies. Yield: ~33%. Anal. Calc. (found) for C81H77N13O29ClMn7 (5·DMF): C, 45.97 (45.74), H, 3.67 (3.42), N, 8.60 (8.35)%. Selected IR data (KBr, cm−1): 3414 (sb), 3150 (sb), 2828 (w), 2779 (w), 2033 (w), 1775 (w), 1709 (s), 1638 (s), 1616 (s), 1402 (s), 1256 (w), 1225 (w), 1159 (w), 1120 (w), 1082 (w), 1055 (w), 1001 (w), 957 (w), 877 (w), 854 (w), 821 (w), 766 (w), 729 (w), 689 (w), 629 (m), 532 (w), 476 (w), 420 (w).

2.3. Single-Crystal X-ray Crystallography

Data were collected on a Rigaku—Oxford Diffraction SuperNova A single crystal X-ray diffractometer equipped with a CCD area detector and a graphite monochromator utilizing Cu Kα radiation (λ = 1.54184 Å) or Mo Kα radiation (λ = 0.71073 Å). Selected crystals were attached to glass fiber with paratone-N oil and transferred to a goniostat for data collection. Empirical absorption corrections (multiscan based on symmetry-related measurements) were applied using CrysAlis RED software [54]. The structures were solved by direct methods using SIR92 [55], and refined on F2 using full-matrix least-squares using SHELXL97 [56], SHELXL-2014/7 [57], and SHELXT [58]. Software packages used: CrysAlisCCD [54] for data collection, CrysAlisRED [54] for cell refinement and data reduction, WINGX for geometric calculations [59], while MERCURY [60] and Diamond [61] were used for molecular graphics. The crystal structures of compounds 1, 2, 3, and 5 contain a small area of highly disordered solvent molecules. For this reason, the SQUEEZE [62] function of PLATON was employed to remove the electron density associated with these solvent molecules from the intensity data. The solvent-free model and intensity data were used for the results reported here. In order to limit the disorder of the terminal ligands or lattice solvent molecules, various restraints (SIMU, RIGU, DELU, DFIX, DANG, ISOR) have been applied in the refinement of the crystal structures. For all compounds, the non-H atoms were treated anisotropically, whereas the H atoms were placed in calculated, ideal positions and refined as riding on their respective C atoms. Unit cell parameters and structure solution and refinement data for complexes 15 are listed in Table S1.

3. Results and Discussion

3.1. Synthetic Comments

For the last several years, our group has been investigating reactions involving the combination of two different organic chelating/bridging ligands. Our first attempts focused on the combination of phenolic oximes with various diols in Mn coordination chemistry and produced high nuclearity complexes with aesthetically pleasing structures. These included a [Mn32] double-decker wheel [43], which is the largest Mn/oxime SMM, a 1-D coordination polymer containing an [Mn40] octagonal superstructure [44], and a [Mn18Na6] wheel [45], consisting of repeating [Mn3] triangular units linked through Na+ cations. Recently, this synthetic methodology was extended towards the combination of (py)2CO with various aliphatic diols in Mn and Mn/4f cluster chemistry, which has led to the isolation of a new series of heterometallic [Mn4Ln2] (Ln = Dy, Gd, Tb) complexes and their homometallic [Mn6] analogues, all based on an uncommon cross-shaped core [50]. Notably, in the homometallic and heterometallic compounds, derived from the use of phenolic oximes/diols or (py)2CO/diols blend, respectively, the diols are not participating in the final structures even though they are initially used in the reaction mixture. However, reactions in the absence of the diol ligands did not produce the same results, demonstrating that although the mechanism of cluster formation is difficult to predict or explain, the presence of diols is essential for the formation of the above structures. Attempts to combine both (py)2CO and other aliphatic diols in the same structure were also successful and produced [Mn24] and [Mn23] supertetrahedral T4 clusters, incorporating both the gem-diol form of di-2-pyridyl ketone ((py)2CO22−) and 1,3-propanediol, and featuring SMM properties [51].
In the present work, we report five new Mn complexes that extend the body of results obtained from the concomitant use of (py)2CO with various diols, in this case (m)pdH2 or 2-hpH2, and emphasize the ability of this synthetic strategy to yield new Mn clusters exhibiting unprecedented metal core topologies.
In particular, compound 1 was isolated from the investigation of reactions of the (py)2CO/pdH2 “blend” under basic conditions in the presence of azide (N3) ions. Thus, the reaction of Mn(NO3)2·4H2O, (py)2CO, and pdH2 in the presence of NEt3, MeCO2Na, and NaN3 in a molar ratio of ~1:0.2:1.4:0.7:0.3:0.4 in DMF resulted a brown solution which was layered with Et2O to afford, after 1 week, dark red/brown crystals of 1 in ~5% yield. The same reaction was repeated, but using mpdH2 in place of pdH2, which yielded red/brown crystals of the isostructural complex 2 in similar yield (~5%). The formation of compounds 1 and 2 is summarized in the general Equation (1):
11   Mn ( NO 3 ) 2 + 5   ( py ) 2 CO + ( m ) pdH 2 + 3   MeCO 2 Na + 3   NaN 3 + 1.25   O 2 + 6.5 H 2 O + 4   DMF   DMF [ Mn 11 O 2 ( OH ) 2 { ( py ) 2 CO 2 } 5 ( ( m ) pd ) ( MeCO 2 ) 3 ( N 3 ) 3 ( NO 3 ) 2 ( DMF ) 4 ] ( NO 3 ) + 6 NaNO 3 + 13   HNO 3
Various modifications were performed to the above-described reaction, aiming to investigate the role of the ligands employed in the synthetic route affording 1 and 2. One of these modifications which involved the removal of N3 ligand from the reaction mixture, since 1 and 2 contained only three of them in their structure, two of which are terminally bound to Mn ions, afforded a new dodecanuclear Mn complex. Thus, the reaction of Mn(NO3)2·4H2O with (py)2CO and mpdH2, in the presence of NEt3 and Me3CCO2Na in a ~1:0.2:1.1:0.7:0.3 molar ratio in MeCN, afforded dark brown crystals of compound 3, in ~59% yield. Equation (2) summarizes the formation of 3:
12   Mn ( NO 3 ) 2 + 4   ( py ) 2 CO + 2   mpdH 2 + 4   Me 3 CCO 2 Na + 2   O 2 + 12   H 2 O   MeCN [ Mn 12 O 4 ( OH ) 2 { ( py ) 2 CO 2 } 4 ( mpd ) 2 ( Me 3 CCO 2 ) 4 ( NO 3 ) 4 ( H 2 O ) 6 ] ( NO 3 ) 2 + 4   NaNO 3 + 14   HNO 3
The extension of these studies to the use of aromatic polyols in the ligand “blend” together with (py)2CO was investigated using the diol—type ligand 2-hpH2. Thus, the reaction of Mn(NO3)2·4H2O, (py)2CO, 2-hpH2, and NEt3 in a molar ratio of ~1:0.2:0.5:0.7 in a mixture of MeOH/DMF (1/1) solvents resulted a brown solution which was layered with Et2O to afford, after 1 week, dark brown crystals of 4 in ~47% yield. The formation of compound 4 is summarized in Equation (3):
4   Mn ( NO 3 ) 2 + 2   ( py ) 2 CO + 2   2 - hpH 2 + 0.5   O 2 + 4   MeOH + 2   DMF   MeOH / DMF [ Mn 4 ( OMe ) 2 { ( py ) 2 C ( OMe ) O } 2 ( 2 - hp ) 2 ( NO 3 ) 2 ( DMF ) 2 ] + H 2 O + 6   HNO 3
The same reaction that led to the isolation of 4 was repeated in the presence of NaClO4 (0.3 equivalents), and complex 5 was produced as dark brown crystals, from slow evaporation of the solutions, in ~33% yield. The formation of compound 5 is summarized in Equation (4):
7   Mn ( NO 3 ) 2 + 4   ( py ) 2 CO + 4   2 - hpH 2 + NaClO 4 + 1.25   O 2 + 1.5   H 2 O + 2   DMF MeOH / DMF   [ Mn 7 { ( py ) 2 CO 2 } 4 ( 2 - hp ) 4 ( NO 3 ) 2 ( DMF ) 2 ] ( ClO 4 ) + NaNO 3 + 11   HNO 3
The chemical and structural identities of all the reported compounds were confirmed by single-crystal X-ray crystallography, elemental analyses (C, H, N), and IR spectroscopy.

3.2. Description of Structures

For complexes 15, the Mn oxidation states and the protonation level of O atoms were determined by charge-balance considerations, inspection of the metric parameters, BVS calculations [63,64] (Table S2), and the observation of Jahn–Teller distortions for the octahedral MnIII ions, which take the form of axial elongation.
Since compounds 1 and 2 exhibit very similar structures, with their main difference being the presence in 2 of the ligand mpd2− (instead of pd2−), only the structure of 1 will be described in detail. Representations of the molecular structure and the structural core of 1 and 2 are shown in Figure 1 and Figure S1, respectively. The coordination modes of the ligands are illustrated in Schemes S1 and S2. Complex 1 crystallizes in the orthorhombic space group Pbca. Its molecular structure consists of a [Mn11O2(OH)2{(py)2CO2}5(pd)(MeCO2)3(N3)3(NO3)2(DMF)4]+ cation, one NO3 counter-ion, as well as two DMF and one water solvent molecules. The cation of 1 features the unusual, asymmetric, mixed-valence [MnIII5MnII64-O)(μ3-O)(μ3-OH)(μ-OH)(μ3-OR)2(μ-OR)10(μ-N3)]8+ core in which the 11 Mn ions are held together by one of each of the following ligands, μ4-O2−, μ3-O2−, μ3-OH, μ-OH, and one bridging end-on N3 group. Further bridging is provided by the doubly deprotonated alkoxido arms of one η223 pd2− ligand and five (py)2CO22− groups. Four of the latter bridge four metal ions, either in a η12214 mode (three (py)2CO22− anions) or in a η13114 (one of them), and the remaining one five Mn ions in a η13215 coordination mode. Additional ligation is provided by three bridging carboxylates, connecting either two or three Mn ions and adopting the syn,syn-η11:μ, syn,anti-η11:μ and η213 coordination modes, two chelating nitrates, two terminal azides, and four terminal DMF molecules. All Mn ions are six-coordinate with distorted octahedral geometries, except for Mn1, which is seven-coordinate in a distorted pentagonal bipyramidal geometry, and Mn3, which is five-coordinate, possessing a distorted square pyramidal geometry (τ = 0.20).
A close examination of the structure of 1 revealed the presence of strong intramolecular hydrogen-bonding interactions involving the H2O and DMF solvent molecules and the bridging OH ligands (Figure S2). However, there is no evidence for direct hydrogen-bonding interactions between neighbouring cations of 1, which are fairly well separated, as shown from the shortest Mn···Mn separation between neighbouring [Mn11] units, which is 8.919 Å (Mn1···Mn5).
Complex 3 crystallizes in the monoclinic space group C2/c and its molecular structure contains a cationic cluster based on a [MnIII8MnII44-O)23-O)23-OH)2(μ-OR)12]10+ core (Figure 2). The unit cell of 3 also contains two MeCN solvent molecules, and two nitrate ions that counter-balance the change of the cationic cluster. The latter could be conveniently dissected into three parts: a central [MnIII4MnII2O4(OH)2(OR)4]2+ unit and two [MnIII2MnII] trinuclear subunits located above and below the hexanuclear one. The central [MnIII4MnII2] unit consists of four edge-sharing triangles in a rod-like conformation, with all Mn ions being at the same plane. The two similar [MnIII2MnII(OR)4]4+ subunits comprise an MnII and two MnIII ions bridged by four alkoxido O atoms in a “V-shaped” arrangement. The three parts of the core are linked together by O16 and O18 atoms corresponding to μ4- and μ3-O2− bridges. The 12 μ-OR bridges of the structural core of the cation of 3 are provided by four η12214 (py)2CO22− and two η223 mpd2− ligands (Scheme S3), while peripheral ligation is provided by four syn,syn11:μ Me3CCO2 groups, four chelating nitrate anions, and six terminal H2O molecules. All Mn ions are six-coordinate with distorted octahedral geometries, except for Mn3, which is seven-coordinate in a distorted pentagonal bipyramidal geometry. A close inspection of the structure of 3 revealed that the neighbouring [Mn12] cations are well separated, as shown from the fairly long closest intermolecular Mn···Mn separation of 7.374 Å.
Complex 4 crystallizes in the triclinic space group P 1 ¯ and its asymmetric unit consists of one half of the [Mn4(OMe)2((py)2C(OMe)O)2(2-hp)2(NO3)2(DMF)2] molecule (Figure 3).
It possesses a defective dicubane metallic skeleton, consisting of two edge-sharing MnIII2MnII triangular units. The four Mn ions are bridged by the alkoxido O atoms of two μ3-OMe anions (O9), two η121:μ (py)2C(OMe)O (O2), and two η12:μ 2-hp2− (O4) ligands (Scheme S4), yielding an overall [MnIII2MnII23-OMe)2(μ-OR)4]4+ core. The coordination sphere of the Mn ions, which are all six-coordinate in distorted octahedral geometry, is completed by two terminal NO3 ions and two DMF solvent molecules. A close inspection of the crystal packing of 4 reveals the presence of non-covalent short contacts between neighbouring [Mn4] compounds. More specifically, the coordinated DMF molecules are involved in intermolecular CH3-π interactions with the pyridyl rings of the (py)2C(OMe)O ligands, while T-shaped π-π stacking is observed between the pyridyl rings of (py)2C(OMe)O ligand and the phenolic rings of 2-hp2−. The distance between the pyridyl C4 and the centroid of phenolic ring was found to be 3.555(9) Å (C4…C7C8C9C10C11C12) (Figure S3). The shortest Mn···Mn separation between adjacent neighbouring tetranuclear clusters of 4 is 9.544 Å.
Complex 5 crystallizes in the monoclinic space group P21/c and its asymmetric unit contains a [Mn7{(py)2CO2}4(2-hp)4(NO3)2(DMF)2]+ cationic cluster, one perchlorate counterion, and one DMF solvent molecule. The structure of the cation of 5 consists of 6 vertex-sharing [Mn2(μ-OR)2] rhombic units that form an unusual non-planar [MnIII5MnII2(μ-OR)12]7+ core with a serpentine-like topology (Figure 4). The metal ions are bridged by 12 alkoxido O atoms, provided by four η12214 (py)2CO22− groups and four η12:μ 2-hp2− ligands (Scheme S5). The peripheral ligation is completed by two terminal NO3 ions and two DMF solvent molecules. All Mn ions are six-coordinate in distorted octahedral coordination environment, except for Mn1 and Mn7, which are five-coordinate, possessing a distorted square pyramidal geometry (τ = 0.18 and 0.25 for Mn1 and Mn7, respectively).
Close inspection of the crystal structure of 5 reveals that there are intermolecular π-π stacking interactions involving the pyridyl rings of (py)2CO22− and the phenolic rings of 2-hp2−, with distances ranging between 3.745 (9) and 3.868 (9) Å (Figure S4). The shortest Mn···Mn separation between adjacent neighbouring [Mn7] clusters of 5 is 8.344 Å.
The reported compounds display several novel structural features, with some of them exhibiting unprecedented asymmetric Mn/O cores. In particular, complexes 1 and 2 possess a [MnIII5MnII64-O)(μ3-O)(μ3-OH)(μ-OH)(μ3-OR)2(μ-OR)10(μ-N3)]8+ core that appears for the first time in Mn carboxylate chemistry, display a rare nuclearity [65], and a unique oxidation state level of Mn ions for undecanuclear complexes. Similarly, complex 3 is based on a multilayer [MnIII8MnII44-O)23-O)23-OH)2(μ-OR)12]10+ core consisting of a central rod-like unit in which two “V-shaped” subunits are attached, while complex 5 possesses an unusual non-planar [MnIII5MnII2(μ-OR)12]7+ core with a serpentine-like arrangement. In addition, compound 4, despite the fact that it comprises a core that has been previously seen in coordination chemistry of 3d metal ions, [66,67,68,69,70,71,72] is the second example of an Mn defective dicubane structure containing a derivative of (py)2CO as ligand, the other one being the complex [Mn4((py)2CO(OH))2((py)2CO(OCH3))2(N3)4] [73].

3.3. Solid-State Magnetic Susceptibility Studies

Solid-state, variable-temperature direct current (dc) magnetic susceptibility measurements were performed on powdered polycrystalline samples of 35 in a 0.1 T field and in the 5.0–300 K range; the low synthesis yields of 1 and 2 did not allow us to perform magnetic measurements on these compounds. The χMT versus T plots for all complexes are depicted in Figure 5.
For complex 3, the χΜT steadily decreases from 29.70 cm3mol−1K at 300 K to 24.70 cm3mol−1K at 50 K, and then it rapidly drops to a minimum of 9.75 cm3mol−1K at 5.0 K. The χΜT at 300 K is smaller than the spin-only (g = 2) value of 41.50 cm3mol−1K for four MnII and eight MnIII non-interacting ions, indicating the presence of dominant antiferromagnetic exchange interactions. The χΜT at 5.0 K suggests a non-zero spin ground state value of ST = 3 or 4.
In the case of 4, the χΜT at 300 K is 14.85 cm3mol−1K, remains almost stable up to 50 K, and then decreases rapidly to a minimum of 5.26 cm3mol−1K at 5.0 K. The χΜT value at 300 K is in agreement with the spin-only (g = 2) value of 14.75 cm3mol−1K for 2 MnII and 2 MnIII non-interacting ions. The shape of the curve indicates the existence of dominant antiferromagnetic exchange interactions and a small spin ground state (possibly ST = 1). In order to quantify the strength of the intramolecular magnetic exchange interactions, the magnetic susceptibility data for compound 4 were fit using program PHI [53]. The system was modeled by using two exchange parameters (Figure S5), Jwb and Jbb, accounting for the peripheral MnII···MnIII and the central MnIII···MnIII interactions, respectively. The spin Hamiltonian used is shown in Equation (5).
H ^ = 2 J w b ( S 1 S 2 + S 2 S 3 + S 3 S 4 + S 4 S 1 ) 2 J b b S 1 S 3 + μ B g ( i = 1 4 S i ) H
The fit gave the following parameters: Jwb = −0.33(1) cm−1, Jbb = 6.28(1) cm−1, and g = 1.98(1), revealing weak antiferromagnetic interactions along the peripheral MnII∙∙∙MnIII ions and ferromagnetic interactions between the central MnIII∙∙∙MnIII ions, and suggesting a spin ground state ST = 1. The obtained coupling constants and g values are within the range reported for other Mn4 clusters with similar structural core, in the majority of which the metal ions are ferromagnetically coupled [66,67,68,69,70,71,72]. However, there are cases reporting antiferromagnetic exchange interactions between the Mn ions of such tetranuclear clusters [74,75].
For complex 5, the experimental χΜT value at 300 K (20.48 cm3mol−1K) is slightly lower than the spin-only (g = 2) value for 2 MnII and 5 MnIII non-interacting ions (23.75 cm3mol−1K). Upon cooling, the χΜT decreases slightly to 19.38 cm3mol−1K at 50 K and then it increases rapidly to reach a maximum of 25.20 cm3mol−1K at 5.0 K. This low temperature increase of the χMT is indicative of the presence of dominant ferromagnetic exchange interactions in complex 5, while the maximum χMT value at 5 K suggests a spin ground state of ST = 6 or 7.
To obtain additional information about the spin ground states, ST, and the potential presence of slow relaxation of magnetization (indicative of SMM behaviour) in complexes 35, alternating current (ac) magnetic susceptibility studies were performed. Data were collected using a 3.5 G ac field and a 1000 Hz oscillation frequency over the temperature range 1.8–15 K. In the case of complex 3, the in-phase signal (plotted as χMT vs. T) decreases from 19.00 cm3mol−1K at 15.0 K to 5.87 cm3mol−1K at 1.8 K (Figure S6, left). The decrease of χMT with decreasing T is suggestive of the presence of low-lying excited states with S greater than the ground state, as expected for a system with dominant antiferromagnetic exchange interactions. Extrapolation of the χMT data from above ∼6.0 K to 0 K gives a value of ∼6 cm3mol−1K, which is indicative of a spin ground state ST∼3 for g = 2.0. These findings are consistent with the results obtained from the dc data. Additionally, no out-of-phase χM signals were observed for complex 3 (Figure S6, right), indicating that this compound does not exhibit SMM behaviour.
In the case of complex 4, the in-phase χMT signal (Figure S7, left) displayed an almost linear decrease from ∼12.40 cm3mol−1K at 15 K to ∼2.73 cm3mol−1K at 1.8 K. Extrapolation of the χMT data from above ∼6.0 K to 0 K gives a value of ∼2.0 cm3mol−1K, suggestive of a spin ground state ST∼1 (for g = 2.0), in agreement with the conclusion from the dc studies. Complex 4 does not show any frequency-dependent out-of-phase (χM) ac signals down to 1.8 K (Figure S7, right), possibly due to its small ST value.
The χMT vs. T plot for complex 5 (Figure S8, left) shows a steep increase with decreasing T from 23.71 cm3mol−1K at 15 K to a plateau value of ∼27 cm3mol−1K at ∼5 K. This behaviour indicates a spin ground state ST∼7, in line with the conclusions from the dc studies. The drop of χMT at lower T may be due to the existence of weak intermolecular interactions. Below ∼2.5 K, there is a drop in χMT accompanied by an increase in the χ′’M vs. T (Figure S8, right). However, the signal is very weak, and no peak maxima were observed, indicating that 5 may display slow magnetic relaxation, but below 1.8 K, the operating limit of our SQUID magnetometer.

4. Conclusions

The syntheses, crystal structures, and magnetic properties of five new Mn clusters (15) are reported. They were derived from a synthetic strategy that involves the concomitant use of (py)2CO and selected diols in Mn cluster chemistry. The reported compounds display novel structural features and some of them unprecedented structural cores (13 and 5). Magnetism studies indicated the presence of dominant antiferromagnetic exchange interactions in compounds 3 and 4, and ferromagnetic ones in 5. The latter also exhibits weak out-of-phase ac signals at low T, suggesting that it might be a weak SMM. This work extends the body of results obtained from the concomitant use of (py)2CO with various diols in Mn cluster chemistry and emphasizes the ability of this synthetic strategy to yield compounds possessing novel structural features. This possibly happens because of the exceptional bridging capability of (py)2CO’s derivatives and polyols, which are able to afford high nuclearity Mn clusters with aesthetically pleasing structures. Future studies will involve the use of additional diol ligands, including pyridyl diols, in conjunction with (py)2CO in Mn cluster chemistry.

Supplementary Materials

The following supporting information can be downloaded at: https://www.mdpi.com/article/10.3390/chemistry5030115/s1. Table S1. Crystal data and structural refinement parameters for compounds 1∙2DMF∙H2O, 2, 3∙2MeCN, 4 and 5∙DMF. Table S2. Bond valence sum (BVS) calculations for Mn ions in 15. Figure S1. Ball and stick representation of the complete structure of 2. H atoms are omitted for clarity. Colour code: MnII, cyan; MnIII, blue; N, green; O, red; C, black. Figure S2. Hydrogen bonding in 1, including interactions of a lattice H2O (O38) molecule with a bridging OH (O32) anion (O38···O32 = 2.672 (2) Å) and an O atom of a lattice DMF molecule (O36) with a bridging OH (O29) anion (O36···O29 = 2.756 (4) Å). Colour code: MnII, cyan; MnIII, blue; N, green; O, red; C, black. H atoms are omitted for clarity. Figure S3. Intermolecular CH3-π interactions between a coordinated DMF (C16) molecule with a pyridyl ring (C17C18C19C20C21N4) of the (py)2C(OMe)O ligand (C16…C17C18C19C20C21N4 = 3.677 (9) Å), and T-shaped π-π stacking between a pyridyl ring (C4) of (py)2C(OMe)O ligand and a phenolic ring (C7C8C9C10C11C12) of 2-hp2− anion (C4…C7C8C9C10C11C12 = 3.555 (9) Å) in 4. Colour code: MnII, cyan; MnIII, blue; N, green; O, red; C, black. H atoms are omitted for clarity. Figure S4. Intermolecular π-π stacking in 5, including interactions (left) of the pyridyl rings (C45C46C47C48C49N8) of (py)2CO22− anions (C45C46C47C48C49N8…C45C46C47C48C49N8 = 3.745 (9) Å), and (right) of a pyridyl ring (C13) of (py)2CO22− and a phenolic ring (C1C2C3C4C5C6) of 2-hp2− anions (C13…C1C2C3C4C5C6 = 3.868 (9) Å) of two adjacent cations of 5. Colour code: MnII, cyan; MnIII, blue; N, green; O, red; C, black. H atoms are omitted for clarity. Figure S5. J-coupling scheme employed for the elucidation of magnetic exchange interactions in 4. Figure S6. Temperature dependence of the in-phase χMT product (left) and out-of-phase χM (right) ac susceptibility signal of 3 in a 3.5 G field oscillating at 1000 Hz frequency. Figure S7. Temperature dependence of the in-phase χMT product (left) and out-of-phase χM (right) ac susceptibility signal of 4 in a 3.5 G field oscillating at 1000 Hz frequency. Figure S8. Temperature dependence of the in-phase χMT product (left) and out-of-phase χM (right) ac susceptibility signal of 5 in a 3.5 G field oscillating at 1000 Hz frequency. Scheme S1. Schematic representation of the coordination modes of (py)2CO22 and pd2 ligands in complex 1. Scheme S2. Schematic representation of the coordination modes of (py)2CO22 and pd2 ligands in complex 2. Scheme S3. Schematic representation of the coordination modes of (py)2CO22 and mpd2 ligands in complex 3. Scheme S4. Schematic representation of the coordination modes of (py)2C(OMe)O and 2-hp2 ligands in complex 4. Scheme S5. Schematic representation of the coordination modes of (py)2CO22 and 2-hp2 ligands in complex 5.

Author Contributions

Conceptualization, A.J.T.; methodology, K.S., E.E.M. and C.P.; software, K.S., A.D.F., N.P. and D.I.A.; validation, A.J.T. and G.C.; formal analysis, K.S., A.D.F., N.P. and D.I.A.; investigation, K.S. and A.D.F.; resources, A.J.T.; data curation, K.S., A.D.F., N.P. and D.I.A.; writing—original draft preparation, D.I.A.; writing—review and editing, D.I.A., G.C. and A.J.T.; visualization, D.I.A. and A.D.F.; supervision, A.J.T.; project administration, A.J.T.; funding acquisition, A.J.T. All authors have read and agreed to the published version of the manuscript.

Funding

This research was funded by the Cyprus Research and Innovation Foundation Research Grant “EXCELLENCE/0421/399”, which is co-funded by the Republic of Cyprus and the European Regional Development Fund. G.C. thanks the US National Science Foundation for support (CHE-1900321) and the University of Florida.

Data Availability Statement

The crystallographic data for complexes 15 have been deposited in the Cambridge Structural Database and assigned the following numbers CCDC 2278744-2278748.

Conflicts of Interest

The authors declare no conflict of interest.

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Figure 1. Ball and stick representations of (top) the complete structure and (bottom) the partially- labelled core of 1. H atoms are omitted for clarity. Colour code: MnII, cyan; MnIII, blue; N, green; O, red; C, black.
Figure 1. Ball and stick representations of (top) the complete structure and (bottom) the partially- labelled core of 1. H atoms are omitted for clarity. Colour code: MnII, cyan; MnIII, blue; N, green; O, red; C, black.
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Figure 2. Ball and stick representations of (left) the complete structure and (right) the partially-labelled core of 3. H atoms are omitted for clarity. Colour code: MnII, cyan; MnIII, blue; N, green; O, red; C, black.
Figure 2. Ball and stick representations of (left) the complete structure and (right) the partially-labelled core of 3. H atoms are omitted for clarity. Colour code: MnII, cyan; MnIII, blue; N, green; O, red; C, black.
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Figure 3. Ball and stick representations of (left) the complete structure and (right) the partially-labelled core of 4. H atoms are omitted for clarity. Colour code: MnII, cyan; MnIII, blue; N, green; O, red; C, black.
Figure 3. Ball and stick representations of (left) the complete structure and (right) the partially-labelled core of 4. H atoms are omitted for clarity. Colour code: MnII, cyan; MnIII, blue; N, green; O, red; C, black.
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Figure 4. Ball and stick representations of (top) the complete structure and (bottom) the partially-labelled core of 5. H atoms are omitted for clarity. Colour code: MnII, cyan; MnIII, blue; N, green; O, red; C, black.
Figure 4. Ball and stick representations of (top) the complete structure and (bottom) the partially-labelled core of 5. H atoms are omitted for clarity. Colour code: MnII, cyan; MnIII, blue; N, green; O, red; C, black.
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Figure 5. Temperature dependence of χMT for complexes 3, 4, and 5 in a field of 0.1 T. The solid black line represents the fit of the experimental data obtained for complex 4.
Figure 5. Temperature dependence of χMT for complexes 3, 4, and 5 in a field of 0.1 T. The solid black line represents the fit of the experimental data obtained for complex 4.
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MDPI and ACS Style

Skordi, K.; Alexandropoulos, D.I.; Fournet, A.D.; Panagiotou, N.; Moushi, E.E.; Papatriantafyllopoulou, C.; Christou, G.; Tasiopoulos, A.J. Rare Nuclearities and Unprecedented Structural Motifs in Manganese Cluster Chemistry from the Combined Use of Di-2-Pyridyl Ketone with Selected Diols. Chemistry 2023, 5, 1681-1695. https://doi.org/10.3390/chemistry5030115

AMA Style

Skordi K, Alexandropoulos DI, Fournet AD, Panagiotou N, Moushi EE, Papatriantafyllopoulou C, Christou G, Tasiopoulos AJ. Rare Nuclearities and Unprecedented Structural Motifs in Manganese Cluster Chemistry from the Combined Use of Di-2-Pyridyl Ketone with Selected Diols. Chemistry. 2023; 5(3):1681-1695. https://doi.org/10.3390/chemistry5030115

Chicago/Turabian Style

Skordi, Katerina, Dimitris I. Alexandropoulos, Adeline D. Fournet, Nikos Panagiotou, Eleni E. Moushi, Constantina Papatriantafyllopoulou, George Christou, and Anastasios J. Tasiopoulos. 2023. "Rare Nuclearities and Unprecedented Structural Motifs in Manganese Cluster Chemistry from the Combined Use of Di-2-Pyridyl Ketone with Selected Diols" Chemistry 5, no. 3: 1681-1695. https://doi.org/10.3390/chemistry5030115

APA Style

Skordi, K., Alexandropoulos, D. I., Fournet, A. D., Panagiotou, N., Moushi, E. E., Papatriantafyllopoulou, C., Christou, G., & Tasiopoulos, A. J. (2023). Rare Nuclearities and Unprecedented Structural Motifs in Manganese Cluster Chemistry from the Combined Use of Di-2-Pyridyl Ketone with Selected Diols. Chemistry, 5(3), 1681-1695. https://doi.org/10.3390/chemistry5030115

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