Octa-coordinated alkaline earth metal–dinitrogen complexes M(N2)8 (M=Ca, Sr, Ba)

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Abstract

We report the isolation and spectroscopic identification of the eight-coordinated alkaline earth metal–dinitrogen complexes M(N2)8 (M=Ca, Sr, Ba) possessing cubic (Oh) symmetry in a low-temperature neon matrix. The analysis of the electronic structure reveals that the metal-N2 bonds are mainly due to [M(dπ)]→(N2)8 π backdonation, which explains the observed large red-shift in N-N stretching frequencies. The adducts M(N2)8 have a triplet (3A1g) electronic ground state and exhibit typical bonding features of transition metal complexes obeying the 18-electron rule. We also report the isolation and bonding analysis of the charged dinitrogen complexes [M(N2)8]+ (M=Ca, Sr).

Introduction

The chemical conversion of dinitrogen to commercially useful commodities is one of the most important reactions in chemical industry, which has long been the subject of extensive research1. Activating the strong triple bond in N2 is a challenge for inventive chemists, who tried in the past various transition metals for binding the molecule as ligand in molecular complexes. Dinitrogen is a poorly binding donor due to its comparatively weak donor–acceptor interactions in transition metal complexes1,2. Metal–ligand bonds of N2 are usually much weaker than those of isoelectronic CO. Braunschweig and coworkers recently reported that boron compounds may also be utilized for fixation of dinitrogen3,4.

Very recently, we reported the isolation and spectroscopic identification of the eight-coordinated carbonyl complexes M(CO)8 of the alkaline earth atoms M=Ca, Sr, Ba possessing cubic (Oh) symmetry in a low-temperature matrix5. The analysis of the electronic structure showed that the classical main-group metals M bind the CO ligands via donor–acceptor interactions through their (n)d atomic orbitals thus mimicking transition metals. Now we found that the alkaline earth atoms may also bind N2 in octa-coordinated complexes M(N2)8 (M=Ca, Sr, Ba) whereby the loss of one N2 ligand has surprisingly only a slightly smaller bond dissociation energy than the dissociation of one carbonyl ligand from M(CO)8. Homoleptic dinitrogen complexes of genuine transition metals, such as tetra-coordinated Ni(N2)4, hexa-coordinated vanadium, and chromium complexes M(N2)6, have been synthesized and spectroscopically characterized in low-temperature matrices6,7,8,9. Mass spectrometric and infrared photodissociation spectroscopic investigations in the gas phase revealed that the Ti+, V+, and Nb+ cations form six-coordinated dinitrogen complexes10,11,12, while the Y+, La+, and Ce+ cations gave the octa-coordinated dinitrogen complexes13. There is only one theoretical report on neutral octa-coordinated dinitrogen complexes by Kovacs, who calculated the lanthanum species La(N2)n (n = 1–8)14. The finding that heavier alkaline earth atoms may bind eight N2 ligands in forming the neutral M(N2)8 complexes is unprecedented.

Results

Experimental studies

Figure 1 shows the spectra in the terminal N–N stretching frequency region from the experiment using a barium target and a 0.5% N2/Ne sample. The spectra were recorded after (a) 30 min of sample deposition at 4 K, (b) after annealing at 12 K, (c) after 15 min of visible light irradiation, and (d) after 15 min of UV-visible light irradiation. Only two bands at 2118.0 and 2237.6 cm−1 were observed. The 2237.6 cm−1 band is metal independent and can be assigned to the antisymmetric stretching vibration of the linear N4+ cation based on the literature data15. The 2118.0 cm−1 band increases tremendously under UV-visible light irradiation. The weak band at 2141 cm−1 is due to trace of CO impurity absorption.

Fig. 1
figure1

Infrared absorption spectra of barium dinitrogen complexes. Infrared absorption spectra in the 2300–1950 cm−1 region from co-deposition of laser-evaporated barium atoms with 0.5% N2 in neon. a 30 min of sample deposition at 4 K, b after annealing at 12 K, c after 15 min of visible light irradiation, and d after 15 min of UV-visible light irradiation. A weak band at 2141 cm−1 is due to trace of CO impurity absorption

Similar bands centered at 2070.0 and 2057.7 cm−1 were observed in the experiments using the strontium and calcium targets. The spectra of strontium and calcium are shown in Supplementary Figs. 1 and 2. Experiments were also performed using the isotopic-substituted 15N2 and the 14N2 + 15N2 1:1 mixture samples. The 2057.7, 2070.0, and 2118.0 cm−1 bands are shifted to 1991.0, 2002.7, and 2048.7 cm−1, respectively, in the experiments with 15N2. The isotopic shifts are appropriate for terminal N–N stretching vibrations. These bands are the only product absorptions in the spectra with high N2 concentrations, suggesting the assignment to the coordinatively saturated M(N2)8 complexes following the example of M(CO)85. The observation of only one N–N stretching band suggests that these neutral dinitrogen complexes have the highest cubic Oh symmetry. The isotopic splittings in the experiments with the 14N2 + 15N2 mixed sample cannot be resolved due to band overlap. The spectra of barium (Supplementary Fig. 3) show that two broad bands (2115.4 and 2047.1 cm−1) slightly red-shifted from those of pure isotopic counterparts are observed with the 14N2 + 15N2 mixed sample. This mixed isotopic spectral feature is consistent with the cubic structure assignment.

Besides the neutral complexes, the radical cations of the alkaline earth dinitrogen complexes were prepared in the gas phase using a pulsed laser vaporization/supersonic expansion ion source and studied by mass-selected infrared photodissociation spectroscopy in the terminal N–N stretching frequency region (see Supplementary Figs 46 for mass spectra)16. Each spectrum is composed of a progression of mass peaks that are attributed to the cation complexes [M(N2)n]+ (M = Ca, Sr, Ba) with n up to 10. The peaks corresponding to [Ca(N2)8]+ and [Sr(N2)8]+ are always the most intense peaks at different experimental conditions, suggesting that they are coordination saturated cation complexes. The higher coordinated complexes [M(N2)n]+ with n > 8 have dinitrogen ligands that are weakly bonded in a second coordination sphere to the [M(N2)8]+ core species. Both the [Ca(N2)8]+ and [Sr(N2)8]+ cation complexes dissociated by elimination of an N2 ligand using a focused IR laser (see Supplementary Fig. 7 for infrared photodissociation spectra). Both spectra feature a broad band centered at 2113 and 2144 cm−1, respectively, which are blue-shifted by 56 and 74 cm−1 relative to the corresponding neutrals observed in solid neon matrix. The intensities of the [Ba(N2)8]+ cation complexes are much lower than those of the Ca and Sr complexes. The n = 8–11 complexes are the most intense peaks in the mass spectrum of barium. We are not able to obtain an effective IR spectrum for the [Ba(N2)8]+ complex due to its low intensity.

Theoretical studies

We performed extensive quantum chemical calculations using density functional theory (DFT) at the M06-2X-D3 and B3LYP-D3 level using various basis set of TZ2P quality in conjunction with relativistic effective core potentials for Sr, and Ba. We also investigated the electronic structure with a modern charge- and energy decomposition analysis to gain insights into the nature of the metal–nitrogen bonds (see Supplementary Methods). Figure 2 shows the energetically lowest lying equilibrium geometries of the M(N2)8 complexes at the M06-2X-D3/def2-TZVPP level. The atomic coordinates and calculated energies are given in Supplementary Data 1. The molecules have cubic (Oh) symmetry and a triplet (3A1g) electronic ground state. The N–N distances in the complexes are slightly longer than in free N2 (1.086 Å). The geometry optimizations of the M(N2)8 species at the electronic singlet states led to Jahn–Teller distorted structures which have D4d (M = Ca, Sr) or D4h (M = Ba) symmetry (Supplementary Fig. 8). The singlet species are 8.4 kcal mol−1 (M = Ca, Sr) and 6.2 kcal mol−1 (M = Ba) higher in energy than the triplet complexes. A similar situation was found for the isoelectronic octa-carbonyls M(CO)8, which were calculated at the same level of theory5.

Fig. 2
figure2

Calculated geometries and bond lengths. Calculated equilibrium structures and interatomic distances [Å] of M(N2)8 and [M(N2)8]+ (M = Ca, Sr, Ba) at the M06-2X-D3/def2-TZVPP level. Bond dissociation energies D0 [kcal mol−1] for loss of one N2 and (in parentheses) loss of eight N2

Figure 2 shows also the bond dissociation energies (BDEs) for loss of one N2 by forming the hepta-coordinated complexes M(N2)7. The latter species, like the isoelectronic carbonyl complexes5, have a triplet ground state and a geometry with C3v symmetry, except for Ca(N2)7 which is slightly distorted from a C3v symmetrical structure (Supplementary Fig. 9). The BDE for the reaction M(N2)8 → M(N2)7 + Nis between D0 = 7.0 kcal mol−1 (M = Ca) and 9.2 kcal mol−1 (M = Sr). Surprisingly, the values are only slightly smaller than for the loss of one CO from M(CO)8, which are between D0 = 9.1 kcal mol−1 (M = Ca) and 11.5 kcal mol−1 (M = Sr) at the same level of theory5. However, the total bond strength of eight N2 ligands to the alkaline earth atoms is much lower than for eight CO species (Fig. 2). The BDEs for loss of eight N2 from M(N2)8 are only between D0 = 15.2 kcal mol−1 (M = Sr) and 25.1 kcal mol−1 (M = Ba). The corresponding values for loss of eight CO from M(CO)8 are between D0 = 58.8 kcal mol−1 (M = Sr) and 63.3 kcal mol−1 (M = Ca)5. This indicates that the octa-coordinated complexes M(N2)8 possess a particular stability among the series M(N2)n, which may be due to a cooperative interaction of all eight ligands. Such cooperative ligand behavior has been reported for mono- and dicarbonyl ion complexes [M(CO)2]+ with M = Cu, Ag, Au17.

The BDEs of the eighth N2 are about one-half to one-third of the BDEs for loss of all eight N2. This indicates that the lower coordinated complexes M(N2)n (n < 8) are much more weakly bonded than M(N2)8. The calculations predict that the low coordinated adducts M(N2)n (n < 5) complexes are unstable with respect to the fragments M + n N2 in the electronic ground state, which explains the nearly complete absence of the signals. In the present study, some weak bands are observed in the experiments, which could be due to the appearance of lower coordinated M(N2)n complexes with n = 5–7, but a definitive assignment is not possible.

The calculated equilibrium geometries and BDEs for the loss of N2 of the radical cations [M(N2)8]+ are also given in Fig. 2. The molecules have D4d symmetry for M = Ca and Sr and D4h symmetry for M = Ba; the same symmetry was found for the isoelectronic octa-carbonyl cations [M(CO)8]+ 5. The BDEs for loss of one N2 of the cations [M(N2)8]+ have similar values as for the neutral complexes M(N2)8, but the total bond strength for the binding of eight N2 in the cations is much higher than for the neutral species. This explains why signals for nearly all species [M(N2)n]+ (n = 1–8) are observed in the mass spectra (Supplementary Figs 46) while the lower coordinated neutral dinitrogen complexes are not observed. The equilibrium geometries of [M(N2)7]+ are shown in Supplementary Fig. 10.

Table 1 shows also the computed N–N stretching frequencies and frequency shifts of the neutral and charged dinitrogen complexes. The calculations give in accordance with experiment a significant red-shift Δυ of the M(N2)8 complexes relative to free N2. The theoretical Δυ values are a bit smaller than the experimental data. We calculated the vibrational frequencies using different functionals and basis sets. The theoretical values at the B3LYP-D3(BJ)/def2-TZVPPD level result in a slightly larger red-shift of the N–N stretching mode than at the M06-2X-D3/def2-TZVPP level, but the corresponding values are still smaller than the experimental results. We think that the discrepancy is likely due to the harmonic approximation of the frequency calculations. Calculations with a different basis set and ECPs for all metal atoms at M06-2X-D3/cc-pCVTZ-pp level gave nearly the same values as the M06-2X-D3/def2-TZVPP calculations (Supplementary Tables 1, 2). The calculated isotope shifts ∆υ(15N2) shown in Table 1 are in excellent agreement with the recorded values. The experiments showed a single N–N-stretching signal for [Ca(N2)8]+ and [Sr(N2)8]+, which is less red-shifted than for the respective neutral complexes (Table 1). The calculations of [M(N2)8]+ suggest two IR-active stretching modes for N2, which are too close to be experimentally observed as separated bands. The calculated wave numbers of the radical cations indicate a smaller red-shift than for the neutral species, which agrees with the observed trend.

Table 1 Experimental and calculated IR-active N–N stretching frequencies υ of M(N2)8 and [M(N2)8]+ (M = Ca, Sr, Ba) and frequency shifts ∆υ (cm−1)

Figure 3 shows the orbital correlation diagram M with a spd valence shell and the electron configuration (n−1)d2ns0np0 in the cubic (Oh) field of eight N2 ligands. It explains the paradoxical situation that only 16 valence electrons of the 18-electron species M(N2)8 (M=Ca, Sr, Ba) are used to fill the valence shell of the metals. The HOMO (highest occupied molecular orbital) is degenerate; the occupation by two electrons with the same spin gives a stable electron configuration like in the X3Σg electronic ground state of O2. Filling the eg HOMO with two more electrons gives the 20 valence electron system ML8, which fulfills the 18-electron rule. Examples of the latter system were recently reported by us in an experimental/theoretical study of [TM(CO)8] (TM=Sc, Y, La)18.

Fig. 3
figure3

Orbital correlation diagram. Orbital correlation diagram of the spd valence orbitals of an atom M with the configuration (n−1)d2(n)s0(n)p0 in an octa-coordinated cubic (Oh) field of eight N2 ligands and occupied valence orbitals of Ca(N2)8. Only the occupied valence orbitals that are relevant for the Ca–N2 interactions are shown

The orbital interaction of a metal with a spd valence shell and eight ligands L in a cubic (Oh) field gives valence orbitals that have a1g, t1u, t2g, a2u, and eg symmetry, which can be associated with specific valence AOs of the metal (Fig. 3). The strength of the pairwise orbital interactions may be estimated with the EDA-NOCV (Energy Decomposition Analysis in combination with Natural Orbitals for Chemical Valence) method. Details of the method and further examples have been described in the literature19,20. Table 2 gives the numerical results of the calculations of M(N2)8 (M=Ca, Sr, Ba) using the fragments M in the electronic triplet state with (n−1)d2ns0np0 electron configuration and (N2)8 in the singlet state.

Table 2 EDA-NOCV results for triplet M(N2)8 (M=Ca, Sr, Ba) complexes at the M06-2X/TZ2P//M06-2X-D3/def2-TZVPP level

The data in Table 2 show that the intrinsic interaction energies ΔEint of M(N2)8 between the metal atoms in the electronic reference state and the dinitrogen ligand cage are rather large. They are much larger than the bond dissociation energies, which are only between 15.2 kcal mol−1 for M=Sr and 25.1 kcal mol−1 for M=Ba. The BDE values give the energy difference between the complex and the fragments at the equilibrium geometries in the electronic ground state, whereas the interaction energies ΔEint refer to the energy difference between the complex and the fragments in the frozen geometry and the electronic reference state. The electronic reference state of the metal atoms is the excited triplet state with the electron configuration (n)s0(n−1)d2 and the electronic ground state is a singlet with the configuration (n)s2(n−1)d0. The excitation energies (n)s2(n−1)d0 → (n)s0(n−1)d2 of the alkaline earth atoms M are rather large for M=Ca, Sr and notably smaller for M=Ba (Table 3). This explains why Ba(N2)8 has a higher BDE than Ca(N2)8 and Sr(N2)8 although the interaction energy ΔEint of the former species is significantly weaker than those of the lighter homologs.

Table 3 Experimental excitation energies of the alkaline atoms M and ions M+ from the electronic ground state to the reference state in the complexes M(N2)8 and [M(N2)8]+ (M = Ca, Sr, Ba)

The attractive metal–ligand interactions ΔEint of M(N2)8 come mainly from the covalent (orbital) term ΔEorb. The breakdown of the latter term into pairwise orbital interactions ΔEorb(1)–ΔEorb(5) shows that the covalent bonding is dominated by the [M(d)]→(N2)8 π backdonation ΔEorb(1), which contributes 70–85% to the total orbital interactions. The rather diffuse (n−1)d orbitals give the alkaline earth elements Ca–Ba an unusual reactivity with a remarkable donor ability. This was previously noted in our study of the carbonyl cation complexes [Ba(CO)]+ where the metal cation Ba+ is a donor for the neutral CO ligand21. We are not aware of any other metal cations that donate electronic charge to a neutral acceptor.

Figure 3 shows also the occupied MOs of Ca(N2)8. Visual inspection of the orbital shapes suggests that the contribution of the d-AOs of Ca in the eg HOMO is much larger than those of the calcium orbitals in the other MOs. The dominant role of the d(π)-AOs of Ca comes to the fore by the deformation densities Δρ(1)-(5), which are associated with the pairwise orbital interactions ΔEorb(1)-(5) (Fig. 4). Note that the isosurface values for Δρ(2)-(5) are much smaller than for Δρ(1), because otherwise the small contributions of the metal AOs would not be visible. The relative size of the charge transfer is given by the eigenvalues of the deformation densities |υn|. It becomes obvious that the largest charge transfer occurs for the [M(d)]→(N2)8 π backdonation |υ1|. The color code for the charge transfer is red→blue. The shape of the deformation densities Δρ(2)-(5) indicates that the orbital interactions ΔEorb(2)-(5) include charge transfer (polarization) within the N2 ligands with ΔEorb(5) exclusively coming from polarization. The deformation densities Δρ(1)-(5) of the heavier complexes M(N2)8 (M = Sr, Ba) are shown in Supplementary Figs. 11 and 12.

Fig. 4
figure4

Shape of deformation densities. Shape of the deformation densities Δρ(1)-(5), which are associated with the orbital interactions ∆Eorb(1)-(5) in Ca(N2)8 (Table 2) and eigenvalues |νn of the charge flow. The isosurface values are 0.002 for Δρ(1) and 0.0006 for Δρ(2)-(5). The color code of the charge flow is red → blue

We also analyzed the nature of the metal–ligand interactions in the cations [M(N2)8]+ using M+ in the electronic reference state 2D with the electron configuration (n)s0(n−1)d1 and the ligand cage (N2)8 as interacting fragments. The numerical results are shown in Table 4. The calculated interaction energies ΔEint of the cations are much smaller than in the neutral molecules (Table 2). This could be expected, because the dominant orbital interaction in M(N2)8 comes from the [M(d)]→(N2)8 π backdonation of the doubly occupied eg MO (Fig. 3). There is only one valence electron in M+ which is also less inclined to π backdonation due to the positive charge of the metal. Table 4 shows that the contribution of the [M+(d)]→(N2)8 π backdonation is much weaker than the related term in the neutral molecules (Table 2). The lower symmetry of [M(N2)8]+ (D4d or D4h) leads to a splitting of the orbital terms. The sum of the two σ donations into the metal d-AOs [M(d)]+←(N2)8 is slightly higher than in the neutral complexes, but it does not compensate for the weaker π backdonation. The cations [M(N2)8]+ have a significantly higher BDE than the neutral complexes (Fig. 2), because the excitation energy into the 2D electronic reference state of M+ is much less than the promotion to the electronic reference state of the neutral atoms (Table 3). It is interesting to note that the 2D state with the configuration (n)s0(n−1)d1 is the first excited state of the metal ions M+. The deformation densities Δρ(1)-(7), which are associated with the pairwise orbital interactions ΔEorb(1)-(7) of the cations [M(N2)8]+ show the expected features of the charge flow. They are shown in Supplementary Figs 1315.

Table 4 EDA-NOCV results for doublet [M(N2)8]+ (M = Ca, Sr, Ba) complexes at the M06-2X/TZ2P-ZORA//M06-2X-D3/def2-TZVPP level

One referee noted reservation against the use of the 18 valence electron rule for the systems, saying that the coordination number 8 is very favorable for the heavier alkaline earth atoms. We want to point out that this refers to compounds in the solid state, where the alkaline earth atoms are found as isolated M2+ cations, which are stabilized by the ligand cage of the solid. Isolated molecules do not possess ionic bonds but polar covalent bonds. Diatomic CaO has a bond length of 1.821 Å22, whereas solid CaO has a Ca–O distance of 2.42 Å23. The latter value agrees with an ionic bond, whereas the former data comes from a polar covalent double bond. The atomic partial charges at the metal atom calculated by the NBO 6.0 method24 are 1.25 (Ca), 1.24 (Sr), and 1.05 (Ba), which also indicate polar covalent bonds rather ionic bonds. The electrostatic attraction in ionic solids comes from the mutual attraction of the separated ions, whereas the electrostatic component in the EDA-NOCV calculations comes from interpenetrating charges. We want to emphasize that the data in Table 2 consider the metal–ligand interactions in terms of M←L σ donation and M→L π backdonation between the fragments in the electronic reference state prior to bond formation, which agrees with the Dewar–Chatt–Duncanson (DCD) model25,26,27. We think that the bonding situation in the isolated molecules is best described in terms of polar covalent bonds due to dative interactions that can be described with the DCD model and which agree with the 18-electron rule.

In summary, we report the first octa-coordinated heavy alkaline earth metal–dinitrogen complexes M(N2)8 (M = Ca, Sr, Ba) that feature strong red-shift in the N–N stretching frequencies and also obey the 18-electron rule. We also report the molecular ions [M(N2)8]+ and provide a detailed analysis of the bonding situation in the complexes. The results suggest new perspectives for the topic of dinitrogen activation.

Methods

The alkaline earth metal–dinitrogen complexes were prepared via the reactions of pulsed laser-evaporated alkaline earth metal atoms and dinitrogen molecules in solid neon. The product species were detected by infrared absorption spectroscopy employing a Bruker Vertex 80 V spectrometer at 0.5 cm−1 resolution using a liquid-nitrogen cooled mercury cadmium telluride (MCT) detector. The experiments were carried out with a wide range of dinitrogen concentrations (from 0.02 to 2% relative to Ne on the basis of volume). No obvious product absorptions were observed in the experiments with very low N2 concentrations (<0.05%). Further details have been described before28.

Data availability

All the studied data are presented in the manuscript and supplementary materials. Additional raw data that support the findings of this study are available from thecorresponding authors upon reasonable request.

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Acknowledgements

The experimental work was supported by the National Natural Science Foundation of China (grant numbers 21688102 and 21433005). L.Z. and G.F. acknowledge financial support from Nanjing Tech University (grant numbers 39837123 and 39837132) and SICAM Fellowship from Jiangsu National Synergetic Innovation Center for Advanced Materials, Natural Science Foundation of Jiangsu Province for Youth (grant number BK20170964), National Natural Science Foundation of China (grant number 21703099). S.P. thanks Nanjing Tech University for a postdoctoral fellowship and the high performance center of Nanjing Tech University for the computational resources. G.F. and S.P. are grateful to the Deutsche Forschungsgemeinschaft for financial support.

Author information

S.P. carried out the quantum chemical calculations. L.Z. and G.F. analyzed the theoretical data and wrote the theoretical part of the paper. Q.W., G.D., and G.W. did the matrix isolation experiments, S.L. and J.J. did the gas phase infrared photodissociation experiments. M.Z. analyzed the experimental data and wrote the experimental part of the paper. M.Z. and G.F. supervised the experimental and theoretical work. Q.W. and S.P. contributed equally to this work.

Correspondence to Mingfei Zhou or Gernot Frenking.

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Peer review information: Nature Communications thanks Ingo Krossing and other anonymous reviewers for their contribution to the peer review of this work.

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