While zinc μ4-oxido-centered complexes are widely used as versatile precursors and building units of functional materials, the synthesis of their analogues based on other transition metals is highly underdeveloped. Herein, we present the first efficient systematic approach for the synthesis of homometallic [M4(μ4-O)L6]-type clusters incorporating divalent transition-metal centers, coated by bridging monoanionic organic ligands. As a proof of concept, we prepared a series of charge-neutral metal-oxido benzamidates, [M4(μ4-O) (NHCOPh)6] (M = Fe, Co, Zn), including iron(II) and cobalt(II) clusters not accessible before. The resulting complexes were characterized using elemental analysis, FTIR spectroscopy, magnetic measurements, and single-crystal X-ray diffraction. Detailed structural analysis showed interesting self-assembly of the tetrahedral clusters into 2D honeycomb-like supramolecular layers driven by hydrogen bonds in the proximal secondary coordination sphere. Moreover, we modeled the magnetic properties of new iron (II) and cobalt (II) clusters, which display a general tendency for antiferromagnetic coupling of the μ4-O/μ-benzamidate-bridged metal centers. The developed synthetic procedure is potentially easily extensible to other M(II)-oxido systems, which will likely pave the way to new oxido clusters with interesting optoelectronic and self-assembly properties and, as a result, will allow for the development of new functional materials not achievable before.
While zinc μ4-oxido-centered complexes are widely used as versatile precursors and building units of functional materials, the synthesis of their analogues based on other transition metals is highly underdeveloped. Herein, we present the first efficient systematic approach for the synthesis of homometallic [M4(μ4-O)L6]-type clusters incorporating divalent transition-metal centers, coated by bridging monoanionic organic ligands. As a proof of concept, we prepared a series of charge-neutral metal-oxido benzamidates, [M4(μ4-O) (NHCOPh)6] (M = Fe, Co, Zn), including iron(II) and cobalt(II) clusters not accessible before. The resulting complexes were characterized using elemental analysis, FTIR spectroscopy, magnetic measurements, and single-crystal X-ray diffraction. Detailed structural analysis showed interesting self-assembly of the tetrahedral clusters into 2D honeycomb-like supramolecular layers driven by hydrogen bonds in the proximal secondary coordination sphere. Moreover, we modeled the magnetic properties of new iron (II) and cobalt (II) clusters, which display a general tendency for antiferromagnetic coupling of the μ4-O/μ-benzamidate-bridged metal centers. The developed synthetic procedure is potentially easily extensible to other M(II)-oxido systems, which will likely pave the way to new oxido clusters with interesting optoelectronic and self-assembly properties and, as a result, will allow for the development of new functional materials not achievable before.
Molecular metal-oxido
clusters have gained attention as versatile
building units of a wide variety of functional materials based on
both coordination[1,2] and noncovalent supramolecular
networks.[3,4] The most prominent subsets of metal-oxido
clusters include trinuclear μ3-oxido-centered complexes,
tetranuclear μ4-oxido clusters, and multinuclear
polyoxidometalates (POMs) (Figure a). Among them, clusters comprising a highly symmetrical
tetrahedral [M4(μ4-O)]6+ core
(M = divalent metal) stabilized by six monoanionic bidentate organic
ligands are of particular interest due to their multifaceted chemistry
arising from the presence of several spots of structural tailorability,
including divalent metal centers in the tetrahedral core, the character
of anchoring groups, and the organic backbone of ligands in the secondary
coordination sphere (Figure b).[5,6] Such diversity of structural features results
in tuneable optoelectronic and coordination properties, which turns
μ4-oxido compounds into suitable candidates for magnetic,[7] luminescent,[8−10] and catalytic[11−15] materials. Moreover, [M4(μ4-O)L6]-type complexes can be regarded as discrete soluble intermediates
between simple monomers and polymeric lattices of various hybrid organic–inorganic
architectures. As such, they are widely used as model systems for
studying properties of more complex systems including MOFs[16,17] and hybrid metal oxide nanoparticles,[18,19] as well as
effective precursors of functional materials.[5,6,20−26] Nevertheless, the development of materials containing the [M4(μ4-O)] structural motif beyond zinc clusters
is hampered by the lack of facile access to this class of complexes
comprising metal centers of desired optoelectronic, catalytic, or
magnetic properties. For instance, access to homometallic isoreticular
MOF-5 analogues based on metals other than zinc is still very limited.
To the best of our knowledge, three Co(II) pyrazolate frameworks are
the only examples of such materials obtained via direct
synthesis from inorganic salts.[27−29] Strikingly, this approach failed
in the case of isoreticular frameworks based on dicarboxylate linkers.
We also note that MOF-5(Co) and MOF-5(Be) were obtained from well-defined
metal-oxido precursors using the controlled SBU approach,[20] and cobalt (II) MOF-5 analogues were obtained
by a post-synthetic transmetalation.[17,30] However, the
latter process was not effective for other metal ions.
Figure 1
(a) Main families of
metal-oxido compounds. (b) Multifaceted chemistry
of tetrahedral μ4-oxido [M4(μ4-O)L6]-type complexes.
(a) Main families of
metal-oxido compounds. (b) Multifaceted chemistry
of tetrahedral μ4-oxido [M4(μ4-O)L6]-type complexes.To date, readily accessible zinc μ4-oxido clusters
have been the subject of the most extensive investigations. For example,
the most common zinc-oxido carboxylates are easily prepared by either
thermal decomposition of zinc carboxylates via elimination
of the corresponding anhydride[31] or in
alkaline solutions of zinc salts with water acting as a source of
the O2– ion.[10,32,33] An increased control over the process of zinc-oxido carboxylates
formation was achieved by using homoleptic zinc carbamates as well-defined
precursors acting simultaneously as water deprotonation agents (Figure a).[34−37] Another approach based on well-defined precursors utilizes diorganozinc
species, which are reacted with the appropriate proligand, and then
are exposed to dioxygen[38−40] or undergo hydrolysis by addition
of a stoichiometric amount of water (Figure b).[3,5,6,16,18,19,21,41−44] In the hydrolytic transformation, the high Brønsted
basicity of alkylzinc moieties is not only used to generate O2– ions but also facilitates initial deprotonation of
the proligand. This approach enabled the synthesis of μ4-oxido complexes incorporating a wide range of organic ligands,
namely, carboxylates,[5,16,21] phosphinates,[18,19,42] amidates,[23] amidinates,[6,26,41,43] and guanidinates.[44] Despite the wide
scope of applied [Zn4(μ4-O)]6+ core coating ligands, this relatively universal approach for Zn–oxido
complexes is essentially non-transferable to the related transition-metal
systems.
Figure 2
Controlled synthesis of metal μ4-oxido [M4(μ4-O)L6]-type clusters from well-defined
precursors: (a) carbamate approach, (b) organometallic approach, and
(c) one-pot transmetalation/hydrolysis approach.
Controlled synthesis of metal μ4-oxido [M4(μ4-O)L6]-type clusters from well-defined
precursors: (a) carbamate approach, (b) organometallic approach, and
(c) one-pot transmetalation/hydrolysis approach.In contrast to zinc–oxido complexes, tetrahedral open-shell
transition metal–oxido complexes were mostly obtained serendipitously,
seldom by design.[45] For example, Mn(II),
Fe(II), and Co(II) μ4-oxido clusters stabilized by N,N′-bidentate ligands were isolated
from reactions of inorganic metal salts with lithiated ligands.[46−48] In all cases, contamination by atmospheric oxygen or moisture was
indicated as the source of the O2– ions. Similarly,
a 3,5-dimethylpyrazolate cobalt-oxido cluster was obtained unexpectedly
during attempts to synthesize the mixed cobalt/zinc [Co1/3Zn2/3(Hdmpz)2] (Hdmpz = 3,5-dimethylpyrazole)
complex.[49] Furthermore, to the best of
our knowledge, the carbamate cluster [Co4(μ4-O) (OOCNC9H18)6], obtained via the insertion of a TEMPO radical into Co2(CO)8[7,50] is the only [M4(μ4-O)L6] system characterized magnetically. Therefore,
we believe that the application potential of tetrahedral oxido-centered
clusters as functional materials cannot be fully revealed without
a reliable synthesis method applicable to metal centers of various
characters.Herein, we present a novel one-pot transmetalation/hydrolysis
procedure
for the synthesis of homometallic oxido clusters incorporating various
divalent metal centers (Figure c). The efficiency of the developed approach was demonstrated
by the preparation of an amide-stabilized zinc-oxido complex [Zn4(μ4-O)(NHCOPh)6] (1-Zn) and its hitherto inaccessible iron (II) and cobalt (II) analogues
(1-Fe and 1-Co). The structural characterization
of 1-Fe, 1-Co, and 1-Zn revealed
that they all exhibit similar self-assembly properties resulting in
a honeycomb-like supramolecular motif. Furthermore, magnetic characterization
of 1-Fe and 1-Co shows strong antiferromagnetic
interactions between the metal centers within the [M4(μ4-O)] core likely mediated by the tetrahedral O2– bridges.
Experimental Section
General Considerations
All manipulations were conducted
under a dry, oxygen-free argon atmosphere either using standard Schlenk
techniques or in a glovebox. All reagents were purchased from commercial
vendors: benzamide (Sigma), KH (Sigma), cobalt (II) chloride (ABCR),
iron (II) chloride (ABCR), zinc chloride and used as received. Solvents
were purified using an MBraun SPS-5 system.
General Procedure for the
Synthesis of 1-Fe, 1-Co, and 1-Zn
Equimolar amounts of
benzamide (0.969 g, 8.00 mmol) and KH (0.320 g, 8 mmol) were placed
in a Schlenk flask cooled to 0 °C and dispersed in THF (30 mL).
After a few minutes, the reaction mixture was allowed to gradually
warm to room temperature and stirred for 24 h. Then, FeCl2 (0.507 g, 4 mmol), CoCl2 (0.519 g, 4 mmol), or ZnCl2 (0.545 g, 4 mmol) was added. After another 8 h of stirring,
18 μL (1 mmol) of Millipore water and 10 mL of dimethylformamide
(DMF) were added and the reaction mixture was stirred for another
24 h. The product was isolated as red-brown (1-Fe), dark
blue (1-Co), or colorless (1-Zn) crystals
after filtration and crystallization in the presence of hexane vapor
at room temperature (yield = 71%, 755 mg (1-Fe); 79%,
859 mg (1-Co); 75%, 830 mg (1-Zn)).
Characterization
FTIR spectra were measured with a
Bruker Tensor II spectrometer using the ATR technique. Elemental analyses
were performed using a UNICUBE elemental analyzer (Elementar Analysensysteme
GmbH). Powder XRD data were collected on a PANalytical Empyrean diffractometer
with Ni-filtered Cu Kα radiation (λ = 1.5406 Å) or
Bruker D8 Advance diffractometer with V-filtered Cr Kα radiation
(λ = 2.2897 Å). The sample was spread on a surface of a
silicon plate fixed to the sample holder and sealed by a Capton tape.
Diffraction patterns were collected by scanning with a step of 0.02°.1-Fe: IR (ATR): ν/cm–1 3347
(w), 3065 (vw), 2951 (vw), 2862 (vw), 1667 (m), 1599 (s), 1540(vs),
1508 (w), 1438 (vs), 1220 (s), 1117 (m), 1030 (w), 933 (w), 699 (vs),
668 (s), 472 (vs). Elemental analysis: calcd (%) for 1-Fe·0.84 THF·0.58 DMF (C47.1H46.8N6.6O8.4Fe4) (1063.13): C, 53.21; H, 4.44;
N, 8.67. Found (%): C, 53.33; H, 4.32; N, 8.77.1-Co: IR (ATR): ν/cm–1 3348
(w), 3068 (vw), 2973 (vw), 2863 (vw), 1674 (m), 1599 (s), 1555(vs),
1506 (w), 1454 (vs), 1388 (w), 1234 (s), 1133 (m), 1030 (w), 701 (vs),
670 (s), 489 (vs). Elemental analysis: calcd (%) for 1-Co·0.93 THF·0.59 DMF (C47.5H47.5N6.6O8.5Co4) (1082.70): C, 52.68; H, 4.43;
N, 8.53. Found (%): C, 52.91; H, 4.19; N 8.72.1-Zn: 1H NMR (300 MHz, CDCl3): δ [ppm] 7.90–7.73
(m, 12H, Ph), 7.46–7.32
(m, 18H, Ph), 6.36 (s, 1.2H, NH), 6.24 (s, 2.4H, NH), 6.15 (s, 1.2H,
NH); 13C NMR (75 MHz, CDCl3): δ [ppm]
177.12 (NCO), 137.03 (IVCAr), 130.55 (CAr), 128.14 (CAr), 127.36 (CAr); IR (ATR):
ν/cm–1 3361 (w), 3063 (vw), 2976 (vw), 2863
(vw), 1672 (m), 1599 (s), 1557 (s), 1501 (m), 1449 (vs), 1388 (w),
1233 (s), 1131 (m), 1028 (w), 697 (vs), 674 (s), 488 (s). Elemental
analysis: calcd (%) for 1-Zn·0.68 THF·0.75
DMF (C47H47N6.75O8.43Zn4) (1102.16): C, 51.19; H, 4.27; N, 8.58. Found (%): C, 51.22;
H, 4.22; N, 8.61.
X-ray Structure Determination
The
data were collected
at 100(2) K on a Nonius Kappa CCD diffractometer[51] using graphite monochromated Mo Kα radiation (λ
= 0.71073 Å). The crystal was mounted in a nylon loop in a drop
of silicon oil to prevent the possibility of decay of the crystal
during data collection. The unit cell parameters were determined from
ten frames and then refined on all data. The data were processed with
DENZO and SCALEPACK (HKL2000 package).[52] The structure was solved by direct methods using the SHELXS-97 program
and was refined by full matrix least-squares on F2 using
the program SHELXL-97.[53] All non-hydrogen
atoms were refined with anisotropic displacement parameters. The hydrogen
atoms were introduced at geometrically idealized coordinates with
a fixed isotropic displacement parameter equal to 1.5 (methyl groups)
times the value of the equivalent isotropic displacement parameter
of the parent carbon. Crystallographic data (excluding structure factors)
for the structure reported in this paper have been deposited with
the Cambridge Crystallographic Data Centre as a supplementary publication.
Copies of the data can be obtained free of charge on application to
CCDC, 12 Union Road, Cambridge CB21EZ, UK (fax: (+44)1223-336-033;
e-mail: deposit@ccdc.cam.ac.uk). CCDC: 2122831 (1-Fe); 2122830 (1-Co); 2122832 (1-Zn).
Magnetic Measurements
Magnetic properties were determined
using a Quantum Design MPMS–5XL SQUID magnetometer for direct
current (dc) and alternating current (ac) measurements. Microcrystalline
samples of 1-Fe and 1-Co were compacted
and immobilized into cylindrical PTFE sample holders. Experimental
dc data were recorded at 0.1 T in the temperature range 2.0–290
K and at 2.0 K in the field range 0.1–5.0 T. Experimental ac
data were collected at a zero static bias field in the temperature
range 2.0–50 K and frequency range 3–1000 Hz using an
amplitude of Bac = 3 G. However, no relevant
out-of-phase signals were detected for either compound. All data were
corrected for the diamagnetic contributions of the sample holders
and the compound (χm,dia/10–4 cm3 mol–1 = −5.37 (1-Fe), −5.31 (1-Co)).
Results and Discussion
Synthesis
of [M4(μ4-O)(NHC(O)Ph)6] (M
= Fe, Co, Zn) Complexes
Metal μ4–oxido
complexes were prepared using a new synthetic procedure
that involves three main steps: (i) generation of a potassium salt
from the selected proligand L-H, (ii) transmetalation reaction with
M(II) salt, and (iii) stoichiometric hydrolysis of the received homoleptic
M(II) complex (Figure c). Benzamide-coated clusters were selected as model systems due
to their close resemblance to the SBUs of the archetypal MOFs. To
demonstrate the applicability of the proposed methodology, we first
performed the synthesis of the zinc–oxido complex (1-Zn). Subsequently, we prepared the Co(II)- and Fe(II)-based μ4–oxido complexes (1-Co and 1-Fe), as examples of the elusive homologues based on magnetically active
and redox-active elements.In a typical procedure, equimolar
amounts of KH and benzamide were placed in a Schlenk flask and dispersed
in THF. The reaction mixture was stirred overnight, and then, a 0.5
molar equivalent of MCl2 (M = Fe, Co, Zn) was added. After
another 12 h, the obtained red-brown (Fe), deep blue (Co), or white
(Zn) suspensions were hydrolyzed using the 1:4 H2O/M molar
ratio. To increase the solubility of the resulting metal–oxido
complexes, DMF was added to the reaction mixture, and the solution
was stirred overnight. Then, the KCl slurry was removed by filtration,
and the respective product was isolated as well-shaped red-brown (Fe),
deep blue (Co), or colorless (Zn) crystals (Figure S8) by slow diffusion of hexane vapor into the parent solution
(for systematic characterization of the resulting complexes vide infra).A key aspect of the developed process
is the highly efficient metathesis
transmetalation driven by the low solubility of KCl in the employed
organic solvent. The use of a potassium salt also allows to effectively
eliminate the incorporation of alkali ions into the final product,
which was reported to occur in the case of Li- or Zn-based salts used
in transmetalation processes.[22,39,43,54−56] Advantageously,
potassium salts of highly basic ligands like amides can be easily
generated in situ by the reaction of a selected proligand
L-H with KH, where the only side product is H2, which finally
enables a one-pot synthesis. Furthermore, the utilization of ligands
with sufficiently high basicity is a crucial factor for ensuring proper
reactivity of a homoleptic ML2 complex, which acts as both
(i) the source of M(II) ions and stabilizing ligands, as well as (ii)
the water-deprotonating agent. Overall, the transmetalation/hydrolysis
process leads to the desired product [M4(μ4-O)L6] in high purity, with the generation of three easy-to-separate
side products: (i) gaseous H2 leaving the reaction system,
(ii) KCl precipitate that can be removed by filtration, and (iii)
the starting proligand, which can be separated from the product by
crystallization and reused. Due to the above-mentioned qualities,
the developed methodology is potentially easily applicable to other
μ4-O systems based on various M(II) metal centers
and a wide range of organic ligands with high basicity such as amidinate,
ureate, or guanidinate anions.
Structural Characterization
Complexes 1-Fe, 1-Co, and 1-Zn were characterized spectroscopically
and by single-crystal X-ray diffraction and elemental analysis. Compound 1-Zn was previously obtained via the organometallic
synthesis,[23] and the current characteristics
(for details, see Experimental Section and Supporting Information) are consistent with the
previous results. The FTIR spectra of 1-Fe and 1-Co are analogous to 1-Zn indicating the presence
of monoanionic benzamide ligands along with the [M4(μ4-O)] core characterized by the M-O bands observed at 477,
487, and 488 cm–1 for iron, cobalt, and zinc cluster,
respectively (Figure S9). Analysis of the
crystal structures indicates that 1-Fe, 1-Co, and 1-Zn are isostructural and crystalize in the P3̅c1 space group as solvates with
THF and DMF. The elemental (see Experimental Section) and 1H NMR analysis (Figure S10) indicates the 1:THF/DMF stoichiometry as approximately
1:0.75:0.75; however, the solvent content can vary in bulk samples.The molecular structure of the complexes 1-Fe, 1-Co, and 1-Zn comprises a tetrahedral [M4(μ4-O)] core coated by six μ2 monoanionic benzamidate ligands (Figure ). The M–O bonds to the central O2– ion are in the range 1.973–1.974, 1.948–1.955,
and 1.941–1.961 Å for 1-Fe, 1-Co, and 1-Zn, respectively. These values are in line with
the M–O bond lengths observed in previously reported iron (II)
(1.952–1.955 Å),[46] cobalt (II)
(1.928–1.956 Å),[50] and zinc
(II) (1.935–1.966 Å)[5,6] tetrahedral oxido clusters.
In turn, the M–O and M–N metal-to-amidate bond lengths
(1-Fe: 1.972–2.023, 1-Co: 1.941–1.996, 1-Zn: 1.958–2.005 Å) are longer than typical M–O
(Fe–O: 1.936–1.978 Å,[57] Co–O: 1.929–1.950 Å,[50] Zn–O: 1.922–1.962 Å5) but shorter
than typical M–N (Fe–N: 2.044–2.070 Å,[46] Co–N: 2.000–2.059 Å,[46] Zn–N: 1.997–2.035 Å[6,46]) bond lengths in known oxido–metal clusters. This observation
indicates a disorder in the arrangement of N and O atoms in the crystal
structures of 1-Fe, 1-Co, and 1-Zn, which suggests the occurrence of the coordination position isomerism
in the benzamidate anions. Specifically, each of them may act either
as an (O,N)- or (N,O)-bidentate ligand, which overall gives four isomers
bearing metal centers with varying coordination environments: M(NNN)M(OON)M(OON)M(OON), M(NNN)M(OOO)M(OON)M(NNO), M(NNO)M(OOO)M(NNO)M(NNO), and
M(NNO)M(NOO)M(NNO)M(NOO) (Figure S5). Furthermore, each of these
isomers is chiral, which adds up to four pairs of possible enantiomers
occupying the same position in the crystal lattice. This coordination
position isomerism introduces differences in environments around N-bonded
protons, which explains the observed respective signal splitting in
the 1H NMR spectrum (Figure S10, for details see Supporting Information).
Figure 3
Molecular structure of
the isostructural complexes 1-Fe, 1-Co,
and 1-Zn; detailed information
regarding the structures are provided in the Supporting Information.
Molecular structure of
the isostructural complexes 1-Fe, 1-Co,
and 1-Zn; detailed information
regarding the structures are provided in the Supporting Information.Very recently, we have
demonstrated that the N-bonded hydrogen
atoms in the proximal secondary coordination sphere provide efficient
H-donor sites for hydrogen bonds which influence the self-assembly
of zinc-oxido clusters.[6] In this context,
we showed that complex 1-Zn, comprising both O and NH
groups in the anchoring group of stabilizing ligand, self-assembles
into 2D supramolecular honeycomb-like layers via pairs
of complementary intermolecular NH···O hydrogen bonds
(the N–H···O distance is 2.760 Å) supported
by π–π interactions in the distal secondary coordination
sphere (Figures and S4). The new complexes 1-Fe and 1-Co exhibit similar self-assembly properties with the corresponding
intermolecular O···HN distances of 2.662 and 2.783
Å, respectively (Table S10), as well
as analogous packing of molecules in the crystal structure. The 2D
honeycomb supramolecular layers are AA-type stacked, as a consequence
forming two types of closed voids: one in the environment of two [M4(μ4-O)] cores and another one within the
space limited by aromatic rings of 12 neighboring clusters (Figure f). These voids are
filled by disordered THF or DMF solvent molecules (1.5 solvent molecules
per oxido cluster). THF molecules enclosed in the voids of the former
type are partially oriented due to the formation of O···HN
hydrogen bonds involving the amidate NH groups.
Figure 4
Crystal structure motifs
of 1-Fe, 1-Co, and 1-Zn: (a,d)
hexagonal assembly of oxido clusters
driven by noncovalent interactions in the secondary coordination sphere;
(b,e) system of intermolecular hydrogen bonds between oxido clusters;
(c) schematic representation of the honeycomb-like supramolecular
structure; (f) solvent accessible surfaces of the two types (blue
and yellow) of closed voids between 2D supramolecular honeycomb-like
layers.
Crystal structure motifs
of 1-Fe, 1-Co, and 1-Zn: (a,d)
hexagonal assembly of oxido clusters
driven by noncovalent interactions in the secondary coordination sphere;
(b,e) system of intermolecular hydrogen bonds between oxido clusters;
(c) schematic representation of the honeycomb-like supramolecular
structure; (f) solvent accessible surfaces of the two types (blue
and yellow) of closed voids between 2D supramolecular honeycomb-like
layers.
Magnetic Characterization
Comprehensive characterization
of physicochemical properties of molecular building blocks is crucial
for designing new functional supramolecular assemblies. Notably, the
exploration of regular [M4(μ4-O)L6]-type magnetic systems with uniform exchange pathways (i.e.,
coupling patterns) between all spin centers has been impeded by the
inaccessibility of well-defined model complexes. To the best of our
knowledge, the carbamate cluster [Co4(μ4-O)(OOCNC9H18)6] is the only system
of this type characterized magnetically, albeit on a purely phenomenological
level indicating antiferromagnetic interaction between the cobalt
ions.[7] However, tetranuclear Cu(II) cluster
[Cu4(μ4-O)(OOCCF3)6(q)4] (q = quinoline) can be described as a farther-related
analogue of such regular systems, based on pentacoordinate, trigonal
bipyramidal metal centers.[58] Its magnetic
properties were extensively studied experimentally and theoretically
indicating exceptionally ferromagnetic interactions within the [M4(μ4-O)] core. All other works on the magnetic
properties of μ4-oxido-centered complexes involve
more distorted systems with less uniform ligand spheres, commonly
including monoatomic chalcogenide or alkoxide bridges prone to the
mediation of strong antiferromagnetic interactions.[59−62] Taking this into account, we
performed magnetic characterization of the new complexes 1-Fe and 1-Co. The magnetic data indicates predominantly
antiferromagnetic exchange interactions between four M(II) centers
within the [M4(μ4-O)] core for both Co(II)
and Fe(II) systems. This is reflected by the shape of the χmT versus T plot, the rather
low value of χmT at 290 K, and the
almost vanishing values of χmT and Mm at 2.0 K representing an effective total spin
value of Stotal = 0 (Figures and 6, see Supporting Information for a detailed
discussion). These observations are consistent with the previous magnetic
study for [Co4(μ4-O)(OOCNC9H18)6], which leads to the general conclusion
that the tetrahedral oxido-bridges in [M4(μ4-O)] systems tend to mediate strong antiferromagnetic coupling. This
phenomenon is often linked to the high M–O–M bond angles,[63,64] which in 1-Fe and 1-Co fall in the range
106.3–112.4°. We also analyzed the magnetic properties
of 1-Fe and 1-Co using an effective isotropic
spin model, which here represents a reasonable approximation since
tetrahedrally coordinated 3d6 and 3d7 centers
are characterized by 5E and 4A2 ground
terms, respectively. In contrast, due to the larger spin–orbit
coupling of both centers, the ground terms are usually split, leading
to temperature-dependent behavior of χmT below 30 K. However, this feature can be neglected for 1-Co as a relevant splitting of the A2 ground term requires
a strong distortion from the tetrahedral ligand field, which is not
the case for the molecular structure of 1-Co. For 1-Fe; however, the quintet E term is significantly split in
any case. Therefore, the χmT versus T data for both compounds were simultaneously fitted at
both 0.1 and 1.0 T, restricted to the temperature interval of 10–290
K and subsequently the values at lower temperatures were calculated.
Based on the single-crystal X-ray structures, we model the M4 cluster as a trigonal pyramid, with the apex defined by threefold
N-coordinated metal, since the distance from the central O here slightly
differs from the other centers (as shown in Figure ). Accordingly, we define the spin connectivity
by two different exchange parameters: Jb, between the metal centers of the base (denoted by indices 2–4)
and Jt, between a metal center of the
base and the apical (top) metal center (index 1). Thus, the corresponding
effective Hamiltonian is
Figure 5
Temperature dependence of χmT at 0.1 (black) and 1.0 T (green circles) of 1-Fe; inset:
molar magnetization Mm vs magnetic field B at 2.0 K; red lines represent the least-squares fit (above
10 K) to the effective spin model described in the text.
Figure 6
Temperature dependence of χmT at
0.1 (black) and 1.0 T (green circles) of 1-Co; inset:
molar magnetization Mm vs magnetic field B at 2.0 K; red lines represent the least-squares fit to
the effective spin model described in the text.
Temperature dependence of χmT at 0.1 (black) and 1.0 T (green circles) of 1-Fe; inset:
molar magnetization Mm vs magnetic field B at 2.0 K; red lines represent the least-squares fit (above
10 K) to the effective spin model described in the text.Temperature dependence of χmT at
0.1 (black) and 1.0 T (green circles) of 1-Co; inset:
molar magnetization Mm vs magnetic field B at 2.0 K; red lines represent the least-squares fit to
the effective spin model described in the text.The data of 1-Fe indicate a small level of paramagnetic
impurities, which was accounted for in the analysis of the data. For 1-Co, we neglected such contributions, since the measurements
point to a negligible level, that is, within the error margin of the
fitting model. For 1-Fe, consisting of effective S = 2 centers, the least-squares fit yields Jt = (−18.6 ± 0.1) cm–1, Jb = (−15.7 ± 0.2) cm–1, and geff = 2.21 ± 0.02, and a
paramagnetic impurity level corresponding to 0.0964 FeII centers per formula unit. For 1-Co (effective S = 3/2 centers), we find Jt = (−24.5 ± 0.1) cm–1, Jb = (−19.6 ± 0.1) cm–1,
and geff = 2.56 ± 0.02. In both cases,
the exchange interactions are antiferromagnetic, and the ground state
of the respective compound can be characterized by an effective total
spin Stotal of 0. For each 1-Fe and 1-Co, the obtained two J values
correspond to the geometric differences, in particular the M–(μ4-O)–M angles. Furthermore, the J values
for the FeII and CoII systems are very comparable
when considering the different spin quantum numbers that enter the
effective spin Hamiltonian as S2. The
effective g factors are fully in line with tetrahedrally
coordinated FeII and CoII centers.
Conclusions
We have developed a new efficient one-pot synthetic approach for
tetrahedral μ4–oxido complexes of various
divalent metal centers stabilized by monoanionic bridging O,N-ligands.
The new synthetic procedure relies on simple stoichiometric hydrolysis
of the homoleptic [ML2] complex generated in situ in a transmetalation reaction. To prove the usefulness of the developed
approach, we have synthesized and characterized a series of M(II)
(M = Fe, Co, Zn) oxido benzamidates. All complexes exhibit analogous
honeycomb-like supramolecular structures in their crystal lattices,
which indicates that their self-assembly properties are dominated
by cooperative noncovalent interactions in the secondary coordination
sphere and likely unaffected by the specific character of the metal
center. Moreover, we have characterized the magnetic properties of
the new Fe(II) and Co(II) complexes, utilizing effective spin models
that underscore a general tendency for antiferromagnetic coupling
of μ4-bridged metal centers in [M4(μ4-O)]-type systems.The reported procedure is potentially
easily extensible to other
M(II)–oxido systems stabilized by a vast array of organic ligands.
These findings will likely pave the way to new oxido clusters with
interesting optoelectronic and novel molecular building units and,
as a result, will allow for the development of new, as of yet elusive
functional materials.
Authors: D Prochowicz; K Sokołowski; I Justyniak; A Kornowicz; D Fairen-Jimenez; T Friščić; J Lewiński Journal: Chem Commun (Camb) Date: 2015-03-07 Impact factor: 6.222
Authors: Jan Nawrocki; Daniel Prochowicz; Iwona Justyniak; Jan van Leusen; Arkadiusz Kornowicz; Paul Kögerler; Janusz Lewiński Journal: Dalton Trans Date: 2019-08-15 Impact factor: 4.390
Authors: Daniel Prochowicz; Jan Nawrocki; Michał Terlecki; Wojciech Marynowski; Janusz Lewiński Journal: Inorg Chem Date: 2018-10-08 Impact factor: 5.165