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Multiple local σ-aromaticity of nonagermanide clusters

Nikolay V. Tkachenko and Alexander I. Boldyrev*
Department of Chemistry and Biochemistry, Utah State University, 0300 Old Main Hill, Logan, UT 84322-0300, USA. E-mail: a.i.boldyrev@usu.edu

Received 22nd February 2019 , Accepted 25th April 2019

First published on 29th April 2019


Nonagermanide clusters are widely used in inorganic synthesis and are actively studied by experimentalists and theoreticians. However, chemical bonding of such versatile species is still not completely understood. In our work we deciphered a bonding pattern for various experimentally obtained nonagermanide species. We localized the electron density via the AdNDP algorithm for the model structures ([Ge9]4−, [Ge9{P(NH2)2}3], Cu[Ge9{P(NH2)2}3] and Cu(NHC)[Ge9{P(NH2)2}3]) and obtained a simple and chemically intuitive bonding pattern which can explain the variety of active sites and the existence of both D3h and C4v geometries for such clusters. Moreover, the [Ge9]4− core is found to be a unique example of an inorganic Zintl cluster with multiple local σ-aromaticity.


Introduction

The concept of aromaticity has long gone beyond the classical Hückel organic structures.1,2 Today, the terms π- and σ-aromaticity are well used for a variety of compounds, including complex inorganic structures.3 In these cases, the delocalized bonding well describes the formation of highly symmetric stable compounds. Numerous planar boron clusters,4–7 metal clusters,3,7–13 and metallabenzenes14–18 fit well into the concept of aromaticity. Along with π- and σ-aromaticity, multiple local π aromaticity is found to be a useful tool to describe complex conjugate systems such as graphene.19–21 This concept has been accepted up to a point. In our work we showed that the concept of multiple local σ-aromaticity could be applied in chemistry. It should be noted that the analysis of completely delocalized canonical MOs cannot lead to a reliable picture of chemical bonding in such clusters,22,23 since there is a mixture of electron lone pairs (an element that does not participate in chemical bonding interactions) with bonding elements of the cluster. Thus, to analyse aromaticity, firstly we need to localize all classical elements (such as 1c–2e lone pairs and 2c–2e Lewis bonds). The adaptive natural density partitioning algorithm (AdNDP) can be very useful for this purpose.

Homoatomic clusters of type [M9]z− (M = Si, Ge, Sn, and Pb) have been investigated both experimentally and theoretically.24,25 The structures of most such clusters confirm the predictions from Wade's rules.26,27 Interestingly, the expectation of the geometry of [M9]4− species with 2n+4 (n = 9) skeletal electrons leads us to a nido nine-vertex polyhedron (C4v capped square antiprism).

An isolated [Ge9]4− cluster has been experimentally obtained in the solid state in the form of alkali metal salts (K4Ge9,28 Cs4Ge9 and Rb4Ge9 (ref. 29)). The geometry of these clusters (except Rb4Ge9) was found by X-ray crystallography and it was slightly distorted from the ideal C4v capped square antiprism, confirming Wade's rules.24 However, various DFT calculations (Table 1) suggest that the global minimum structure for [Ge9]4− is a tricapped trigonal prism (D3h symmetry).23,30 In turn, the C4v symmetric structure has one imaginary frequency. A similar picture could be found, for instance, in a biphenyl system (twisted geometry in the gaseous phase and completely planar in the solid state). D3h and C4v structures transform from one to another through the diamond square process (Fig. 1).31,32

Table 1 Relative energies with ZPE corrections (kcal mol−1) of D3h and C4v [Ge9]4− structures at various levels of theory
Structure PBE0 B3LYP
LANL2DZ Aug-cc-pvdz Aug-cc-pvtz LANDL2DZ Aug-cc-pvdz Aug-cc-pvtz
a Structure is a first order stationary point.
D3h [Ge9]4− 0.0 0.0 0.0 0.0 0.0 0.0
C4v [Ge9]4− 0.0 1.6a 10.2a 0.0 0.4a 9.1a



image file: c9sc00929a-f1.tif
Fig. 1 Side and top views of a (a) tricapped trigonal prism (D3h symmetry) and (b) capped square antiprism (C4v symmetry).

Although Wade's rules can give us a prediction of the cluster structure, we still do not have a comprehensive picture of the chemical bonding for such species. In this paper, we presented a new description of bonding in [Ge9]4− clusters, based on the local σ-aromaticity concept. The obtained bonding pattern explains both the presence of active sites and the existence of C4v and D3h geometries for these compounds.

Computational methods

All structures were optimized at the PBE0/aug-cc-pvdz33,34 level of theory. Frequency calculations were performed using the harmonic approximation. To understand the chemical bonding pattern, matrix representation of the first order reduced density operator in the NAO basis set was analysed by the adaptive natural density partitioning (AdNDP) algorithm35 as implemented in the AdNDP 2.0 code36 at the PBE0/cc-pvdz level of theory. In the AdNDP method, we followed general ideas of the NBO analysis proposed by Weinhold.37 It represents a chemical bonding structure in terms of nc–2e bonds following the concept of electron pairs and 2c–2e classical bonds. To assess the aromaticity of each aromatic fragment, nucleus-independent chemical shift (NICS)38,39 calculations were performed at the PBE0/aug-cc-pvtz level. The ChemCraft 1.8 software was used to visualize chemical bonding patterns and geometries of the investigated compounds.

Results and discussion

To understand the stability of both D3h and C4v isomers, we conducted AdNDP analysis of the first order reduced NAO density matrix for C4v and D3h [Ge9]4− clusters. We found that the C4v structure has nine classical Lewis lone pairs on germanium atoms with occupation numbers (ONs) 1.91–1.90 |e|. The remaining electron density forms eleven delocalized σ-bonds with ON = 2.00–1.90 |e| (Fig. 2). These delocalized σ-type fragments bind three areas of the germanium cluster. The first area is the cap of the square antiprism (Fig. 2b–d) and consists of three 5c–2e bonds with ON = 2.00–1.95 |e|. The shape of these elements as well as the number of electrons (6 electrons fit the 4n+2 Hückel's rule) indicates σ-aromaticity in the Ge5 cap fragment. Next three 8c–2e σ-bonds with ON = 2.00 |e| bind the bottom square fragment (Fig. 2e–g). The contribution of this Ge4 fragment into the 8c–2e bonds is ∼99.0% for the bond shown in Fig. 2e and ∼81.9% for bonds shown in Fig. 2f and g. The whole Ge8 square antiprism fragment is bound by five 8c–2e σ-bonds with ON = 2.00–1.90 |e|. The shapes of 8c–2e and 5c–2e bonds (one bond without a nodal plane, two bonds with one nodal plane, etc.) and 4n+2 electrons (n = 1,2) on each area render these fragments σ-aromatic. Therefore, the stability of the C4v structure can be explained by the existence of three σ-aromatic areas: the Ge5 cap fragment, Ge4 bottom square fragment and Ge8 square antiprism fragment.
image file: c9sc00929a-f2.tif
Fig. 2 Overall chemical bonding picture obtained for the C4v capped square antiprism [Ge9]4− cluster. ON denotes the occupation number (equal to 2.00 |e| in an ideal case). Lines between atoms help in visualization and do not represent 2c–2e bonds here and elsewhere.

An equally interesting picture of chemical bonding was found for the D3h [Ge9]4− cluster (Fig. 3). According to AdNDP analysis, the 40 valence electrons in [Ge9]4− can be localized into nine classical 1c–2e lone pairs on Ge atoms, two 3c–2e sigma bonds with ON = 1.97 |e|, and nine delocalized 5c–2e bonds. These nine 5c–2e bonds with ON = 1.98–1.89 |e| are responsible for binding interactions inside each Ge5 cap fragment (rectangular pyramids built on the sides of a trigonal prism). Three σ-bonds per cap constitute σ-aromaticity. It should be mentioned that the 3c–2e bonds could be also considered σ-aromatic since the number of electrons fits well in Hückel's rule (n = 0). Thus, the chemical bonding pattern for the D3h [Ge9]4− cluster includes nine lone pairs, two 3c–2e σ-aromatic bonds and three symmetric Ge5 σ-aromatic areas with 5c–2e σ-bonds, which explains the stability and the variety of active sites for such a structure.


image file: c9sc00929a-f3.tif
Fig. 3 Overall chemical bonding picture obtained for the D3h tricapped trigonal prism [Ge9]4− cluster.

To assess local σ-aromaticity in D3h and C4v structures, we calculated NICSzz and NICSiso indices at different points of the clusters (Fig. 4). The coordinates of chosen points can be found in the ESI (Table S2). Significantly negative values of NICS indices at the centers of aromatic fragments (points 1, 3, and 4 for C4v and points 1 and 4 for the D3h structure) corroborate our local σ-aromatic description of the bonding pattern for such clusters (Table 2).


image file: c9sc00929a-f4.tif
Fig. 4 Points that were chosen for the NICS indices calculation.
Table 2 NICSzz and NICSiso indices calculated at chosen points for D3h and C4v [Ge9]4− clusters
Point C4v [Ge9]4− D3h [Ge9]4−
NICSzz NICSiso NICSzz NICSiso
1 −152.42 −85.91 −62.91 −50.81
2 −102.32 −94.10 −90.53 −67.92
3 −99.76 −90.68 −90.47 −65.89
4 −97.46 −78.02 −87.71 −55.38
5 −55.43 −26.92 −68.37 −22.68


It should be noted that the described bonding pattern is not unique to germanium clusters and could be found in other isoelectronic species. To show that, we performed AdNDP analysis for [Si9]4− and [Sn9]4− clusters. The results are similar and can be found in the ESI (Fig. S4–S6).

The described chemical bonding pattern also could be found in other synthesized germanium clusters. Various derivatized nonagermanide systems were reported,40–51 including mono-, di- and tri-substituted species. Of all the series, threefold phosphine-functionalized nonagermanide clusters, synthesized in 2018 by Fässler and coworkers, are of particular interest due to their high reactivity and ease of synthesis.51 In these clusters, the geometry of the core Ge9 fragment is found to be slightly distorted from that of the tricapped D3h symmetric trigonal prism. In our model calculations of the [Ge9{P(NiPr2)2}3] cluster, we attached three P(NH2)2+ substituents to the three capping Ge atoms. The results are shown in Fig. 5. We found that the bonding pattern of the core Ge9 fragment remains the same as that of the D3h-[Ge9]4− cluster. The main difference in bonding is that three peripheral 1c–2e lone pairs on capping Ge atoms participate in the formation of new two-center classical bonds with phosphorus (ON = 1.97 |e|). The occupancy of the nine 5c–2e bonds, which are responsible for the local σ-aromaticity, remains almost the same (Fig. 5d–f). The –P(NH2)2 substituents exhibit a classical bonding pattern with 1c–2e lone pairs on P (ON = 1.94 |e|) and N atoms (ON = 1.91 |e|) and 2c–2e σ N–H (ON = 1.99 |e|) and σ N–P (ON = 1.99 |e|) bonds (Fig. S1).


image file: c9sc00929a-f5.tif
Fig. 5 Chemical bonding picture of the core Ge9 fragment obtained for the [Ge9{P(NH2)2}3] cluster.

Previously, an intriguing reactivity was found for such threefold phosphine-functionalized nonagermanide clusters.51 The reaction of [Ge9{P(NiPr2)2}3] and NHCDippCuCl leads to the formation of a (NHCDippCu)[Ge9{P(NiPr2)2}3] compound, containing the D3h symmetric Ge9 fragment. For understanding the bonding pattern within the copper containing structure, we started our analysis from the model molecule – (Cu)[Ge9{P(NH2)2}3]. The results are shown in Fig. S2. We found that the Cu atom keeps five 1c–2e d-type lone pairs with an occupation number of 1.99–1.96 |e|. The bonding pattern of the [Ge9{P(NH2)2}3] part remains almost the same, except one 3c–2e σ-aromatic fragment on the top of the trigonal prism that transforms into a 4c–2e Ge3Cu σ-bond with ON = 1.97 |e|. The contribution of the Ge3 triangle fragment into the 4c–2e bond is found to be ∼83.7%. Even though this model molecule is a good object for studying bonding patterns, the optimized geometry noticeably differs from the experimentally obtained structure. For instance, the Ge–Ge distance in the upper triangle of the trigonal prism is 3.17 Å (experimental value is 2.87 Å). That is why we decided to include the NHC ligand attached to the Cu atom, which models the NHCDipp ligand.

The geometry of the optimized structure with the NHC ligand attached to the Cu atom corroborates with the experimental data. So, the Ge–Ge distance in the upper triangle and the distance between capped germanium and germanium in the upper triangle of the prism is 2.93 Å and 2.50 Å, respectively (experimental data are 2.87 Å and 2.50 Å, respectively). It should be mentioned that the attachment of the second [Ge9{P(NH2)2}3] fragment to the (Cu)[Ge9{P(NH2)2}3] molecule also leads to Ge–Ge distances similar to the experimental ones (Table S1, {[Ge9{P(NH2)2}3]Cu[Ge9{P(NH2)2}3]} structure). By conducting AdNDP analysis we found that the bonding pattern of the core Ge9 fragment remains the same (Fig. S3). It consists of six s-type 1c–2e lone pairs on Ge atoms, three local σ-aromatic Ge5 fragments, one 3c–2e σ-aromatic bond at the bottom, and one 4c–2e CuGe4 σ-bond at the top of the prism. The binding interactions of the Cu atom are illustrated in Fig. 6. The new 2c–2e σ Cu–C bond with ON = 1.95 |e| appears due to the attachment of the NHC ligand. The contribution of the carbon atom into the Cu–C bond is assessed to be ∼85.3%, indicating the donor–acceptor type of the sigma bond.


image file: c9sc00929a-f6.tif
Fig. 6 Chemical bonding of the Cu atom in the Cu(NHC)[Ge9{P(NH2)2}3] cluster.

Conclusions

In summary, we performed a chemical bonding analysis for five nonagermanide species. The stability of both D3h and C4v structures of the Ge94− cluster could be well described via the concept of multiple local σ-aromaticity. We are not aware of such a chemical bonding in the literature. On the basis of AdNDP analysis we can separate the electron density in locally aromatic regions: the Ge5 cap, Ge8 antiprism, and Ge4 square fragments for C4v [Ge9]4−, and then three Ge5 caps, and two 3c–2e triangular fragments for D3h [Ge9]4−. We found a similar bonding pattern for the core Ge9 fragment for previously synthesized trisubstituted [Ge9{P(NR2)2}3] clusters. The –P(NH2)2 groups are bound with the tricapped trigonal prism core via classical 2c–2e Ge–P σ-bonds.

A variety of active sites are well described with the obtained bonding picture. Thus, it was found that the copper atom in Cu[Ge9{P(NH2)2}3] and Cu(NHC)[Ge9{P(NH2)2}3] clusters interacts with the 3c–2e σ-bond of the Ge9 core to form a 4c–2e bond. Therefore, the described picture is indeed in good agreement with the experimental reactivity of such compounds. The same chemical bonding was also found in isoelectronic [Si9]4− and [Sn9]4− clusters. We hope that the new obtained bonding pattern with locally σ-aromatic fragments could be an important step to build a coherent bonding structure of Ge-family clusters and congener species. It will also help in the development and understanding of chemical bonding for complicated cases in inorganic chemistry.

Conflicts of interest

There are no conflicts to declare.

Acknowledgements

This work was supported by the USA National Science Foundation (Grant CHE-1664379 to A. I. B).

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Footnote

Electronic supplementary information (ESI) available. See DOI: 10.1039/c9sc00929a

This journal is © The Royal Society of Chemistry 2019