Marina A.
Uvarova
*a,
Fedor M.
Dolgushin
a,
Konstantin A.
Babeshkin
a,
Nikolay N.
Efimov
a,
Claudio
Pettinari
b,
Igor L.
Eremenko
a and
Sergey E.
Nefedov
a
aN.S. Kurnakov Institute of General and Inorganic Chemistry of the Russian Academy of Sciences, Leninsky Prosp. 31, 119991 GSP-1, Moscow, Russian Federation. E-mail: yak_marin@mail.ru
bChemistry Interdisciplinary Project (ChIP), School of Pharmacy, University of Camerino, Via Madonna delle Carceri, 62032 Camerino, Italy
First published on 27th June 2025
Novel mononuclear complexes [M((CF3)2pz)2((CH3)2pzH)2] (M = Zn (1), CoII (2), and CuII (3)) and binuclear complexes [Cu2(μ-(CF3)pz)2((CH3)2pzH)2(OOCBut)2] (4) were prepared by different simple synthetic methods and characterized by single crystal X-ray diffraction analysis. Compounds 1 and 2 have a similar structure with a tetrahedral metal environment, unlike compound 3, in which copper is in a square-planar environment. A copper square planar environment is also found in 4. The structures of the complexes are stabilized by intermolecular (1, 2, and 4) and intramolecular (3) hydrogen bonds. 1 was additionally characterized in solution by 1H NMR. The study of thermal behavior indicated the transformation of 2 into the pyrazolate bridging polymer [Co((CH3)2pz)2]n at 330 °C. Magnetic susceptibility measurements in the ac-magnetic field show the presence of slow field-induced (Hdc = 2500 Oe) magnetic relaxation behavior for the Co-based complex 2.
In most of the cases, the pyrazolate anion is coordinated in the bidentate form, giving pyrazolate-bridging complexes up to pyrazolate bridging polymers.20–28 The formation of mononuclear pyrazolate complexes is not common. The Deacon group managed to obtain homoleptic pyrazolates of La and Ce [La((CH3)2pz)3]n, in which pyrazolate anions are bound to metals featuring six different coordination modes,29,30 forming polymer chains. Only a few mononuclear complexes of d-metals where the anionic pyrazolate is bound in a monodentate form are known.19,31–34 Just one zinc complex {[Zn(tBu2pz)2(tBu2pzH)2]} has been obtained from a protolysis reaction of ZnEt232 and for this reason one of our goals is to define a clear procedure to obtain mononuclear complexes of 3-d metals containing only pyrazole-based ligands acting as anionic and ancillary donors.
Here we describe some methods for the synthesis of new uncommon mononuclear mixed pyrazolate–pyrazole complexes [M((CF3)2pz)2((CH3)2pzH)2] M = Zn (1), CoII (2), and CuII (3) (Scheme 1). When copper, zinc or cobalt acetate is mixed in acetonitrile with both (CF3)2pzH and (CH3)2pzH, the acetates are replaced by the acid fluorinated pyrazolate anions, whereas the more basic 3,5-dimethylpyrazole coordinates the metal center in the neutral form. An alternative method for obtaining 1 and 2 is the reaction of bridged binuclear complexes [M2(μ-(CH3)2pz)2((CH3)2pzH)2(OOCBut)2] (M = Zn and Co) with an excess of (CF3)2pzH. In the case of the copper compound, the reaction leads to the binuclear complex [Cu2(μ-(CF3)pz)2((CH3)2pzH)2(OOCBut)2] (4). The structures of all the compounds obtained were investigated by single-crystal X-ray diffraction analysis. The stability of the Zn compound was studied by solution 1H NMR. Magnetic susceptibility and thermal properties are investigated for the cobalt complex.
Complexes 1 and 2 are also prepared through the interaction of the previously described pyrazolate-bridging complexes [M2(μ-(CH3)2pz)2(CH3)2pzH)2(OOCBut)2] (M = Zn,35 M = Co36) with an excess of (CF3)2pzH in dichloromethane at room temperature. The formation of the zinc and cobalt complexes is likely accompanied by transfer of H+ from (CF3)2pzH followed by displacement of both (CH3)2pzH and HOOCBut.
When a mixture of copper acetate hydrate and (CH3)2pzH is warmed at 140 °C for three hours, acetic acid is removed and a brick-red powder insoluble in organic solvents is formed. The addition of hexane and (CF3)2pzH yields [Cu((CF3)2pz)2((CH3)2pzH)2] (3).
The reaction of the [Cu((CH3)2pzH)2(OOCBut)2]37 complex with (CF3)2pzH in dichloromethane does not lead to mononuclear [M((CF3)2pz)2((CH3)2pzH)2] as in the case of cobalt and zinc, but leads to the binuclear complex [Cu2(μ-(CF3)pz)2((CH3)2pzH)2(OOCBut)2] (4) in 75% yield. During this exchange reaction, one pivalate anion is replaced by a fluorinated pyrazolate anion, which in 4 bridges two copper atoms forming a dimer in which the pivalate and the heterocyclic (CH3)2pzH are coordinated in a monodentate form in the axial position.
It is worth noting that mononuclear complexes [M((CF3)2pz)2((CH3)2pzH)2] 1–4 are unique in their kind, since the metal atoms are surrounded only by heterocyclic pyrazole and pyrazolate donors.
Complex/parameter | 1 | 2 | 3 | 4 |
---|---|---|---|---|
M–N (CF3)2Pz | 1.995(3) | 2.008(4) | 1.992(3) | 1.994(2) |
1.998(3) | 2.019(4) | 1.987(3) | 2.000(2) | |
M–N (CH3)2pzH | 2.000(3) | 2.019(4) | 1.985(4) | 1.963(2) |
2.001(3) | 2.023(4) | 1.983(4) | ||
M–O | 1.940(2) |
D | H | A | d(D–H)/Å | d(H–A)/Å | d(D–A)/Å | D–H–A/° | |
---|---|---|---|---|---|---|---|
a 1 − X, −Y, +Z. b −X, +Y, 1/2 − Z. | |||||||
1 | N6 | H6 | N2 | 0.82(5) | 2.08(5) | 2.793(6) | 146(4) |
N8 | H8 | N4 | 0.80(3) | 2.07(3) | 2.799(5) | 152(3) | |
2 | N6 | H6 | N4 | 0.94(4) | 1.98(4) | 2.812(6) | 146(4) |
N8 | H8 | N2 | 0.82(4) | 2.07(4) | 2.820(6) | 151(4) | |
3 | N6 | H6 | N4a | 0.87(7) | 2.05(7) | 2.913(5) | 170(7) |
N8 | H8 | N2a | 0.93(5) | 1.95(5) | 2.848(5) | 160(5) | |
4 | N4 | H4 | O2b | 0.91(3) | 1.83(3) | 2.733(3) | 172(3) |
The structure of complex 2 is very similar to that of compound 1. The cobalt atom is in a tetrahedral environment formed by four nitrogen atoms of two (CF3)2pz anions and two (CH3)2pzH molecules (Fig. 2). There is only a slight increase in bond lengths (Co–N 2.008(4) Å–2.023(4) Å). This is the first example of single-element pyrazolate coordination in cobalt compounds.
The geometry of complex 3 differs from those of 1 and 2. In 3, the copper atom, in a square planar environment, is four-coordinated by nitrogen atoms from two (CF3)2pz-anions (Cu–N 1.992(3) Å, 1.987(3) Å) and two (CH3)2pzH molecules (Cu–N 1.985(4) Å, 1.983(4) Å) (Table 1 and Fig. 3a). A square-planar environment is typical for a copper atom due to the strong field of ligands that affects the electronic structure of the copper ion, forcing it to form bonds in one plane, unlike cobalt and zinc, which usually form a tetrahedral or octahedral environment. The nature of hydrogen bonds is quite different from those in 1 and 2. In 3, intermolecular hydrogen bonds between (CF3)2pz and (CH3)2pzH of neighboring molecules aggregate mononuclear complexes into dimers (Table 2 and Fig. 3b). Additionally, the dimers are stabilized by weak π–π interactions between pairwise adjacent (CH3)2pzH fragments with the shortest C–C distance of 3.386(8) Å and distances between the centroids of the pyrazole rings of 3.84 and 4.02 Å. The formation of similar H-linked dimers is observed for square planar pyrazolate Pd34 and Pt complexes.39
Complex 4 of composition [Cu2(μ-(CF3)pz)2((CH3)2pzH)2(OOCBut)2] crystallizes into the monoclinic space group C2/c with a solvate molecule of dichloromethane. Compound 4 is a binuclear complex in which two copper atoms positioned at a non-binding distance of 3.3063(7) Å and connected by two bridging (CF3)2pz− anions are coordinated by a monodentate-bound pivalate anion and (CH3)2pzH (Fig. 4). As a result, each copper atom is found in a square planar environment formed by three pyrazolic nitrogen atoms (Cu–N 1.9632(19)–1.9998(17) Å) and one oxygen atom of the carboxylic group (Cu–O 1.9402(16) Å). The structure of the complex is additionally stabilized by unusual “cross” intramolecular hydrogen bonds involving the oxygen atoms of the terminal pivalate anions of one copper atom and the hydrogen atom of the NH group of the (CH3)2pzH molecule coordinated to the other copper atom (Table 2). Analogous hydrogen bonds are found in the similar complex [Cu2(μ-(CH3)2pz)2((CH3)2pzH)2(OOCBut)2].37 The substitution of the bridging (CF3)2pz− anions in 4 with (CH3)2pz− in ref. 37 results in a shortening of the Cu⋯Cu distance to 3.2629(8) Å. It can also be noted that in 4 the bond lengths of copper with bridging (CF3)2pz− Cu–N(CF3)2pz (1.9998(17) Å–1.9942(17) Å) are longer than those in [Cu2(μ-(CH3)2pz)2((CH3)2pzH)2(OOCBut)2] containing a bridging (CH3)2pz− (Cu–N(CH3)2pz 1.952(8)Å–1.977(8)Å), while in 4 the bond lengths between the copper and terminal (CH3)2pzH ligands (Cu–N(CH3)2pzH 1.9632(19)Å) are shorter than those in [Cu2(μ-(CH3)2pz)2((CH3)2pzH)2(OOCBut)2] (Cu–N(CH3)2pzH 2.0041 (5)Å).
The molecular structures of complexes 1–4 are also confirmed by IR spectroscopy. Complexes 1–3, having very similar spectra, show very strong bands due to the valence fluctuations of CF3-groups at 1257 cm−1, 1222 cm−1, and 1117 cm−1 in 1 and at 1254 cm−1, 1218 cm−1, and 1117 cm−1 in 2 and 3. Bands at 2936–2940 cm−1 in 1–4 correspond to the vibrations of the CH3-groups of the heterocyclic pyrazole ligand. Aromatic C–H-stretching vibrations are characterized by the bands at 750–755 cm−1 and 1008–1058 cm−1 (ring fluctuations) in 1–4. In the spectrum of 4, it is also possible to distinguish the C–O vibrations due to the pivalate anions (1553 cm−1). The change in the coordination of the pyrazole ligand from the monodentate in compounds 1–3 to bridging in 4 leads to a slight shift of all characteristic absorption bands (see the ESI,† Fig. S3–S6).
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Fig. 5 Temperature dependences of magnetic susceptibility (χ) and χT under a 5000 Oe dc-magnetic field. |
The χT values decrease linearly up to 2.53 cm3 K mol−1 at 40 K, then a sharper drop in the χT magnitude follows reaching the minimum value of 1.08 cm3 K mol−1 at 2 K. This behavior can arise from the anisotropy of Co2+ ions and the Zeeman effect caused by the applied dc-magnetic field.40 The M(H) and M(H/T) dependences are given in Fig. S1 (ESI†).
Due to the active development of Co-based molecular magnets in recent years,41 the ac-magnetic susceptibility measurements were performed to determine the possibility of slow magnetic relaxation for complex 2.
In the zero dc-magnetic field, the out-of-phase (χ′′) values of magnetic susceptibility in comparison to in-phase (χ′) values for complex 2 are negligible at 2 K in the ac-frequency range from 10 to 10000 Hz (Fig. 6). The absence of considerable χ′′(ν) signals for complex 2 most likely is attributed to the significant contribution from the quantum tunneling of the magnetization (QTM), resulting in fast relaxation. To minimize the effect of QTM, non-zero dc-fields of up to 5000 Oe have been applied, resulting in the appearance of significant out-of-phase signals on the χ′′(ν) dependences for complex 2. The optimal value of the dc-field strength, corresponding to the minimal relaxation rate, equals 2500 Oe for complex 2 (Fig. S2, ESI†).
The χ′′(ν) isotherms measured under a 2500 Oe dc-field were approximated using the generalized Debye model. The resulting temperature dependence of relaxation time (τ vs. 1/T) is shown in Fig. 7.
In the high-temperature range of 3.9–4.1 K, for complex 2 the τ(1/T) dependence was fitted using the Arrhenius equation (τ = τ0·exp{Δeff/kBT}) corresponding to the Orbach relaxation mechanism, where τ0 and Δeff/kB are the shortest relaxation time and demagnetization energy barrier, respectively. The resulting relaxation parameters for complex 2 in the high-temperature range were calculated as follows: Δeff/kB = 44 (±1) K and τ0 = 3 × 10−10 (± 1 × 10−10) s.
The τ vs. 1/T dependence in the whole temperature range of 2–4.1 K for complex 2 was approximated using the sum of Orbach, Raman (τ−1 = CRamanTnRaman) and QTM (τ−1 = BQTM) relaxation mechanisms with the following set of parameters: Δeff/kB = 44 (fixed) K, τ0 = 3 × 10−10 (fixed), CRaman = 0.08 (±0.04) s−1 K−nRaman, nRaman = 7.8 (±0.6) and BQTM = 156 (±3) s−1. The Orbach relaxation parameter values were set to the values obtained from the high-temperature range approximation to avoid over-parametrization.
The main mass loss of 64% corresponds to the removal of two (CF3)2pzH molecules (theoretical value: 62%), which are obtained by protonation of the fluorinated pyrazolate anion, and is accompanied by the formation of a residue (practical value: 35%, theoretical value: 38%).42 The formation of a pyrazolate-bridged polymer is accompanied by an exothermic effect at a temperature of 331 °C. The composition of the residue is confirmed by the elemental analysis data. Such proton exchange between pyrazole fragments is associated with a higher volatility of (CF3)2pzH compared to (CH3)2pzH. Beyond 370 °C, a slow decrease in mass is observed without thermal effects, which indicates the destruction of the pyrazolate anion without the formation of a new phase. The formation of a pyrazolate-bridged copper polymer, [Cu(μ-(CH3)2pz)2]n, has been previously described in ref. 37.
IR spectra were recorded in the 400–4000 cm−1 region using a Spectrum-65 PerkinElmer FT-IR spectrometer.
Microprobe analyses were carried out using a Carlo Erba EA 1108 Series CHN elemental analyzer (Center of Collective Use of IGIC RAS).
X-ray diffraction analysis of 1–4 was carried out on a Bruker Apex II diffractometer (MoKα, λ = 0.71073 Å, graphite monochromator, CCD detector). The absorption correction was applied semiempirically using the SADABS program.43 The structures were solved by direct methods using the ShelXS-97 program44 and refined by the full-matrix least-squares method using the ShelXL program45 in the anisotropic approximation for non-hydrogen atoms. Some of the CF3 groups in structures 1 and 2, as well as the tert-butyl group in 4, are positionally disordered over two positions (refinement of disordered groups was carried out using standard DFIX, DANG, and EADP constraints). The hydrogen atoms of the NH groups were located from the difference Fourier maps and included in the refinement in the isotropic approximation without constraints; the positions of other hydrogen atoms were calculated geometrically, and they all were refined in the isotropic approximation in the riding model with Uiso(H) = 1.5Uequiv(C) for methyl groups and Uiso(H) = 1.2Uequiv(C) for other hydrogen atoms. The main crystallographic data and refinement parameters for compounds 1–4 are given in Table S1 (ESI†).
The thermal behavior of the complexes was studied using the simultaneous thermal analysis (STA) technique for parallel recording of TG (thermogravimetry) and DSC (differential scanning calorimetry) curves. The study was performed using an STA 449 F1 Jupiter instrument (“NETZSCH”) in Al-crucibles under a lid with a hole to ensure a vapor pressure of 1 atm during the thermal decomposition of the samples. The rate of heating to 500 °C was 10 °C min−1 under an argon atmosphere (Ar content > 99.998%, O2 < 0.0002%, N2 < 0.001%, water vapor < 0.0003%, and CH4 < 0.0001%).
1H NMR spectra were recorded in CDCl3 at ambient temperature using Bruker AVANCE 300 and 400 spectrometers at 300.1 and 400.1 MHz, respectively, using a solvent as the internal standard (CDCl3, 7.26 ppm; CD3OD, 3.31 ppm). Chemical shifts (δ) and coupling constants (J) are given in ppm and in Hz, respectively. The peak patterns are indicated as follows: (s, singlet; d, doublet; t, triplet; q, quartet; o, octet; m, multiplet; and br., broad).
Magnetic susceptibility measurements were performed using a Quantum Design PPMS-9 susceptometer. For dc susceptibility measurements, a magnetic field of 5000 Oe was applied, and the corresponding measurements were performed in the 2–300 K range. For ac susceptibility measurements of all samples, oscillating ac fields of 5 Oe, 3 Oe and 1 Oe in the frequency ranges of 10–100, 100–1000 and 1000–10000 Hz, respectively, were applied. These settings allowed one both to avoid sample heating at low temperatures (which may occur when the modulation amplitude and frequency are high) and to obtain the best signal-to-noise ratio. All magnetic measurements were performed on polycrystalline samples sealed in polyethylene bags and covered with mineral oil in order to prevent field-induced orientation of crystallites. The paramagnetic components of the magnetic susceptibility χ were determined taking into account both the diamagnetic contribution evaluated from Pascal's constants and the contributions of the sample holder and mineral oil.
Anal. calc. ZnC20H18N8F12: C 36.18, H 2.73, N 16.88. Found: C 36.87, H 2.56, N 16.11. FT-IR (ATR), ν cm−1: 3435 m, 3139 w, 2934 w, 1576 m, 1547 m, 1530 m, 1502 m, 1423 w, 1376 m, 1352 m, 1296 s, 1224 s, 1259 s, 1194 w, 1157 s, 1128 s, 1080 w, 1050 m, 1014 s, 983 w, 813 s, 750 w, 733 w, 577 w, 428 w. 1H NMR (CDCl3, 400 MHz, 294 K) 2.51 (s, 12 H, (CH3)2pzH), 5.92 (s, 2H, (CF3)2pz), 6.79 (s, 2H, (CH3)2pzH, 14.7 (s, 2H, NH–(CH3)2pzH).
Anal. calc. CuC20H18N8F12: C 36.29, H 2.74, N 16.92. Found: C 36.59, H 2.55, N 17.11. FT-IR (ATR), ν/cm−1: 3199 w, 3102 w, 2940 m, 2785 w, 1595 s, 1545 m, 1528 w, 1501 w, 1422 m, 1348 m, 1308 m, 1254 s, 1217 s, 1173 w, 1111 s, 1079 m, 1058 w, 1025 m, 1008 s, 978 w, 810 s, 755 m, 733 w, 617 m.
Anal. calc. Cu2C30H36F12N8O4: C 38.84, H 3.91, N 12.08. Found: C 39.11, H 4.16, N 12.34. FT-IR (ATR), ν cm−1: 3423 s, 2964 m, 2931 m, 1634 m, 1556 s, 1553 s, 1500 w, 1483 m, 1411 w, 1371 s, 1265 s, 1225 w, 1137 s, 1055 w, 1028 s, 810 w, 760 s, 618 w, 433 w.
Footnote |
† Electronic supplementary information (ESI) available. CCDC 2430824–2430827. For ESI and crystallographic data in CIF or other electronic format see DOI: https://doi.org/10.1039/d5nj02001h |
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