2.1. The synthesis of the Binary Precursor and the Novel Compound 1
The synthesis of the novel compound was carried out according to the usual strategy followed by our research group. The chelating compound is always available in its acid form, which applies to various first-row transition metals (Mn-Zn) or post-transition metals (Cd, Pb), with more or less success. For Cu(II) azurite type (bluish) or malachite type (greenish) could be used, upon the assumption that the Cu2CO3(OH)2 (mw 221.1) formula is reasonable in practice for the calculation of the quantity of the copper(II) sources. This strategy is founded in the idea that the reaction of the copper hydroxy-carbonate with the acid form of the chelator (amino-polycarboxylic acids, amino acids, small peptides, etc.) will yield CO2 as an easily removable by-product (stirring and heating the reaction mixture, as well as applying controlled vacuum environment, usually working in aqueous medium). Two relevant comments need to be added regarding this work (and closely related ones): (1) The use of bluish copper hydroxy-carbonate can yield to unreacted dark CuO, whereas malachite only leaves unreacted apple green residue. (2) It is convenient to remove the small amount of unreacted material by careful filtration prior to adding other(s) coligands(s) to the binary complex solution This general strategy has the advantage of avoiding undesired by-products (i.e., alkaline salts). At the same time, it seems to favor good crystallizations. Moreover, when the amounts of reagents used do not match the stoichiometry of the final product according to molecular recognition criteria, it´s because the mother liquors can retain the excess of a free-ligand.
Our experiment, reported in the experimental section of this work, illustrates a case-study where the use of a significant excess of Hdap prevents the initial crystallization of the novel compound 1, though with a less practical yield.
2.2. Molecular and Supramolecular Structures in the Crystal
The structure established in the crystallographic study, with a single crystal, runs into the difficulty that the uncoordinated water molecules are highly disordered, which is why they are not taken into account in determining the molecular structure of the compound. Furthermore, the
Figure 2a reveals that one of the EGTA chelating ligands shows some disorder in an ethylene unit. This circumstance is of minor importance in relation to the molecular recognition between the Cu
2(EGTA) chelate and the Hdap nucleobase, although it must somehow influence the fact that the four metal centers of the tetranuclear molecule are non-equivalent (
Figure 2b). The data in
Table 1 indicate that the crystallographic quality is quite good.
Table 2 provides the data of bond distances and relevant trans angles in the coordination environments. Briefly, each µ-EGTA bridging chelator generates an elongated octahedral environment (4+2 type) and a penta-coordinate environment (4+1 type). Thus, there is an EGTA-1 with the Cu1 (4+1) and Cu4 (4+2) centers; and on the other hand, EGTA-2 has the Cu2 (4+1) and Cu3 (4+2) centers. Both the 4+1 and 4+2 environments contain the H(N3)dap N7 or N9 donors (with conventional notation for purines). The tetranuclear nature of the compound
1 is essentially due to the bridging mode of the H(N3)dap ligands. This means that compound
1 is formed from the bridging mode of molecular recognition of the Hdap ligands, instead of having obtained a different compound where the Cu
2(µ-EGTA) chelate coordinated an Hdap ligand to each metal center. The formation of the tetranuclear molecule is made possible by the tautomerization of the 2,6-diaminourine proton from its more basic donor (N9) to its less basic heterocyclic donor (N3). Therefore, tautomerization efficiently contributes to the molecular recognition mode in the investigated compound.
Table 3 shows the data of the distances and angles in the hydrogen bonds that were determined in this crystallographic study. Evidently, it includes N3-H···O and N6-H···O-type interactions between the Hdap ligands and coordinated oxygen atoms of EGTA.
The crystallographic study further reveals a
supramolecular recognition that is illustrated in the most simplified way in
Figure 3, despite the uncoordinated water delocalization and the disorder in an EGTA chelator. For this reason, locating the uncoordinated water was sacrificed in order to achieve a high structural resolution (SQUEEZE).
Figure 3 shows the involvement of the H(N3)dap ligands in stacking interactions that affect their 5- and 6-atom aromatic rings, but in such a way that two 5-atom rings of the Hdap ligand interact with each other at one end, and in the other something similar happens with the 6-atom rings. The aforementioned stacking interactions are shown in the figure by dashed lines that join the centroids of the rings involved.
The coordination of the H(N3)dap tautomer has been provided by five compounds prior to the present study. The available data are collected in the
Table 4 emphasizing two aspects: the molecular or polymeric nature of the compound and, where available, the formation of hydrogen bonds N3-H···O and N6-H··· O by cooperating with M-N9 or M-N7 coordinate bonds (M is transition metal). The very limited data available suggest the existence of known analogous compounds with copper, zinc or cobalt. Of a molecular nature, they are only available from data on the MULCED compound [
23], while the other compounds are polymers (1D or 2D) or metal organic frameworks (MOF) (3D). Available data indicates that the style of molecular recognition of compound
1 and its analogues is feasible regardless of the molecular or polymeric nature of the known compounds.
2.3. Physical properties
The physical properties studies are the thermal, spectral and magnetic stability which are described in detail below.
For comparison purposes,
Figure S1 (Supplementary file) shows the
FT-IR spectra of the binary compound [Cu
2(µ-EGTA)(H
2O)
2]·2H
2O (without Hdap) and of compound 1, [Cu
4(µ-EGTA)
2(µ-Hdap)
2(H
2O)
2]·7H
2O.
It can be observed that above 3000 cm-1 the spectrum of compound 1 permits us to determine different absorptions due to antisymmetric and symmetric water stretching modes and the primary amino group, in addition to two bands at 3194 and 3139 cm-1 due to N-H group stretching modes. Within this region of the spectrum we can determine the presence of water in the compound, as well as the presence of two non-equivalent N-H groups that correspond to the N3-H group of the two slightly different tautomers of H(N3)dap present in the crystal. On the other hand, a broad band is observed between 1650 and 1620 cm-1 due to the scissor’s deformation of the water molecules and the hexocyclic amino groups of Hdap. This band also includes the antisymmetric stretching of the EGTA carboxylate groups.
Of particular diagnostic value is a weak band at 1534 cm-1 that indicates the deformation in the plane of the N3-H group, δ (N-H). This band appears in a region where few other absorptions take place. At 1372 cm-1 the symmetric stretching of the carboxylate groups is observed. Two other interesting bands are observed at 1114 and 850 cm-1 corresponding to the antisymmetric and symmetric stretchings of the C-O-C group. These bands are normally observed at 1300-1000 and 890-820 cm-1; while in the binary compound, they’re observed at 1088 and 856 cm-1. The aromatic CHs of Hdap gives a deformation band out-of-plane π-CH at 850 cm-1. This band is always very defined and appears between 900-860 cm-1, which is a normal range, especially in hydrocarbons.
Figure 4 shows the
TGA (in air) and
DSC (in N
2 atmosphere)
curves. As is often the case, the seven (uncoordinated) water molecules and the two distal aqua ligands are lost in an overlapping process that corresponds to steps 1 and 2 indicated in
Table 5.
These processes occur within three thermal decomposition stages that produce carbon dioxide, carbon monoxide, water and the three oxides of nitrogen normally observed (N2O, NO, NO2) with traces of methane at 520 degrees, an oxide of copper is obtained with an experimental value higher than what was calculated, with the difference of these values being lesser than 1%. The decomposition of N2O in the atmosphere clearly shows the dynamics of heat absorption that essentially corresponds to the coordinated or uncoordinated loss of water between 30 degrees and 180 degrees, reflecting that the overlapping loss of the uncoordinated and the coordinated is a global and complex process. Above 180 degrees, a reasonable compensation of the absorption and heat loss processes occurs, as corresponds to the thermal decomposition of the organic ligands. It is important to note that complete loss of water initiates thermal decomposition above approximately 200 degrees in order to generate copper oxide at 520 degrees.
The
electronic spectrum, obtained by diffuse reflectance, shows an asymmetric d-d band with maximum absorption at 685 nm (see
Figure 5). The barycenter of intensity of this band is located at 735 nm, a value that is below the maximum absorption of the corresponding electronic spectrum of hexaaqua-cation (~800 nm) [
29]. In short, this comparison reflects that the metal environment in compound
1 has a stronger ligand field than the aqua-cation.
For the measurements of the
electronic spin resonance (ESR), X and Q band ESR measurements were carried out in the 5-300 K range. The X-band ESR spectra exhibit near axial symmetries, but a considerable rhombicity can be detected operating at Q-band (
Figure 6 and
Figure 7). With a computer program working at the second order of the perturbation theory, the spectra could be fitted with a unique g tensor. Therefore, the exchange interaction between copper ions is large enough to collapse the spectra of the magnetically non-equivalent sites [
30]. It is noteworthy to mention that the intensity of the ESR signal drastically decreases below 20 K, suggesting that the exchange interactions are mainly antiferromagnetic. The main components of the calculated g tensor are: g
1 = 2.235, g
2 = 2.071 and g
3 = 2.052 (g
II = 2.235; g
⊥ = 2.061). The G parameter, defined as G = (g
II-2)/(g
⊥-2), is 3.8, less than 4, confirming the existence of exchange interactions and a small misalignment between the main axes of the individual g tensors in compound
1 [
31]. In any case, the lowest g value indicates a d
x2-
y2 ground electronic for all the Cu(II) centers, as correspond to axially elongated 4+1 and 4+2 environments.
The thermal evolution of the magnetic molar susceptibility is shown in
Figure 8. As the temperature is lowered, the susceptibility increases until a maximum of 0.0369 cm
3/mol is reached at 23 K, which then rapidly decreases (0.003 cm
3/mol at 5 K). The χ
mT product lies practically constant (1.56 cm
3K/mol) between 300 and 100 K and decreases swiftly when cooling down to 5 K (0.016 cm
3K/mol). The high temperature data (T>50K) is well described by a Curie-Weiss law (χ
m = C
m/T-θ), with Cm = 1.62 cm
3K/mol and θ = -9.7 K (
Figure 8, right). The observed Curie constant (C
m) agrees well with the calculations for four non-interacting S = 1/2 ions, with the g value deduced from de ESR study (g = 2.12). The negative θ value and the overall appearance of the χ
mT vs. T curve indicate the predominance of short-range antiferromagnetic interactions between the Cu(II) ions leading to a S = 0 spin ground state.
Considering the tetranuclear nature of compound 1, different magnetic exchange pathways through the H(N3)dap and EGTA organic ligands must be taken into account: Cu1···Cu2 (5.783 Å), Cu3···Cu4 (5.676 Å), Cu1···Cu4 (7.453 Å) and Cu2···Cu3 (7.233 Å). Therefore, the following spin Hamiltonian should be used to analyze the magnetic properties, including only isotropic interactions and the Zeeman term:
(1)
However, due to the large number of adjustable parameters, fitting the magnetic curves using the above expression does not provide reliable values for the exchange coupling constants. Therefore, it is necessary to put some constraints to the J
ij and g parameters. In this sense, it has been considered that despite the small differences in the super-exchange pathway, the two interactions propagated by the EGTA ligand are similar (J
12 = J
34 = J
A), and the same is applicable for the two interactions propagated by the H(N3)dap ligand (J
14 = J
23 = J
B In addition, taking into account the ESR results, it was assumed that all the local g-values are equal. Under these conditions, the fit of the experimental susceptibility data using the full-matrix diagonalization PHI program [
32] provided the following set of parameters: J
A = -12.4 cm
-1, J
B = -0.33 cm
-1 and g = 2.102 with R = 1.3x10
-4. The calculated curve matches very well with the experimental data in the complete temperature range studied (
Figure 8, left). The smaller coupling constant can be unambiguously attributed to the interactions propagated through the EGTA ligand, since the magnetic orbitals (mainly d
x2-
y2) lie in planes parallel to each other and perpendicular to the exchange pathway. The overlap between the orbitals bearing the unpaired electrons is significantly better through the H(N3)dap ligands in this compound, hence the stronger antiferromagnetic couplings.
2.4. DFT calculations
In the solid state, compound
1 forms infinite 1D assemblies that propagate via two different π-stacking interactions (see
Figure 9a). One is established between the 2,6-diaminopurine bases that are coordinated to the pseudo-octahedral Cu-atoms (denoted as A···A in
Figure 9a) and the other binding mode involves the 2,6-diaminopurine rings that are coordinated to the square-pyramidal Cu-atoms (denoted as B···B). The theoretical study is devoted to the energetic analysis of both π-stacking modes and the characterization of some additional H-bonds that are formed in the A···A binding mode. In order to keep the model computationally approachable and to simplify the description and DFT analysis of both interaction modes, the tetranuclear complex has been divided in two halves by cutting the μ-EGTA chelate as indicated in
Figure 9b, resulting in two dinuclear complexes denoted as “
A” and “
B”, see
Figure 9b.
First, the MEP surfaces of fragments
A and
B have been computed to explore the most electron rich and poor parts of the molecules, which are represented in
Figure 10. As expected, the minima are located at the noncoordinated atoms of the carboxylate groups (–75 and –63 kcal/mol in
A and
B, respectively) and the MEP maxima are located at the amino group bonded to C2 (ranging +54 to +60 kcal/mol). The MEP value at the H-atoms of the Cu-coordinated water molecules is similar (+53 kcal/mol), revealing that both the NH
2 groups and water molecules are strong H-bond donors. The MEP value at the available NH bond of the NH
2 group at C6 is also large and positive (+46 and +44 kcal/mol in
A and
B, respectively) but significantly smaller than those at the NH
2 groups due to the formation of the intramolecular NH···O H-bond in the former. The MEP is also positive at the –CH
2– groups of the chelate ligand (+26 kcal/mol) and over the six membered ring of the 2,6-diaminopurine.
The coordination by N7 and N9 in combination with the N3-H tautomer instead of the coordination via the more basic N1 or N3 in combination with the N9-H tautomer is likely due to the formation of extra H-bonds that compensate the different coordination ability of the six and five-membered ring N-atoms. This has been confirmed by performing QTAIM analysis. The distributions of bond critical points (CPs, fuchsia spheres) and bond paths of the Cu(II) complexes
A and
B are shown in
Figure 11, confirming the existence of the NH···O contacts (via N3H3 and N6H6). The interaction energies of these NH···O HBs derived from the potential energy density (Vr) measured at the bond CPs range from –6.06 kcal/mol to –9.07 kcal/mol, confirming the energetic relevance of these contacts. Interestingly, the QTAIM analysis also evidences the presence of a weaker CH···O contact in the Cu(II)-atom coordinated by N7 in both models, where a bond CP and bond path connects the C8–H bond of the imidazole ring to the Cu-coordinated O-atom of the carboxylate group. The energy associated to these contacts are weaker (–5.08 and –3.70 kcal/mol in
A and
B, respectively).
As commented above, two different π-stacking modes have been analyzed theoretically. They are shown in
Figure 12 along with the QTAIM and NCIplot analyses. The combined QTAIM and NCIplot representations are very useful to visualize NCIs in real space, including their attractive/repulsive nature (provided by the color of the isosurfaces). It can be observed that the self-assembled A···A dimer shown in
Figure 12a combines two strong and symmetrically equivalent OH···N interactions (established between the coordinated water molecules and the N1-atom of 2,6-diaminopurine) with an antiparallel π-stacking interaction. The latter is characterized by four bond CPs and bond paths interconnecting C and N atoms and includes the exocyclic NH
2 group. Moreover, a green (attractive) reduced density gradient (RDG) isosurface is located between the 2,6-diaminopurine moieties, further characterizing the π···π interaction. The dimerization energy is large and negative (–17.00 kcal/mol), confirming the importance of this assembly in the solid state of compound
2. The contribution of the HBs is –14.4 kcal/mol, thus supporting the strong nature of these HBs, in line with the blue RDG isosurfaces located between the OH groups and N1-atoms. This energetic analysis reveals that in fact the HBs dominate the formation of this dimer. The other stacking binding mode (B····B) that involves the 2,6-diaminopurine coordinated to the square-pyramidal Cu(II) metal centre is much complicated. The RDG isosurface is very extended and occupies most of the space between the monomers, disclosing a strong complementarity. Moreover, there is an intricate combination of interactions taking place, explaining the very large dimerization energy (–44.5 kcal/mol), more than twice the A···A. This is due to the existence of multiple CH··O contacts between the carboxylate groups and the CH bonds of the chelator. Moreover, two ancillary anion–π interactions (indicated as O···π in
Figure 12b) are also observed, characterized by a bond CP and bond path connecting one O-atom of the carboxylate group to the pyrimidine ring, in line with the MEP analysis that revealed the π-acidity of this ring. The large binding energy observed for the B···B dimer likely explains the pentacoordination of these Cu(II) in B since the formation of the B···B staking mode is able to compensate the stabilization that would be obtained by the coordination of the water molecules.