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Article

Occurrence of Double Bond in π-Aromatic Rings: An Easy Way to Design Doubly Aromatic Carbon-Metal Structures

by
Nikolay V. Tkachenko
1,2,
Alvaro Muñoz-Castro
2 and
Alexander I. Boldyrev
1,*
1
Department of Chemistry and Biochemistry, Utah State University, 0300 Old Main Hill, Logan, UT 84322-0300, USA
2
Grupo de Química Inorgánica y Materiales Moleculares, Facultad de Ingeniería, Universidad Autonoma de Chile, El Llano Subercaseaux, Santiago 2801, Chile
*
Author to whom correspondence should be addressed.
Molecules 2021, 26(23), 7232; https://doi.org/10.3390/molecules26237232
Submission received: 7 November 2021 / Revised: 24 November 2021 / Accepted: 26 November 2021 / Published: 29 November 2021
(This article belongs to the Special Issue Chemical Bonding: A Commemorative Special Issue Honoring Professor Linus Pauling)
Browse Figures
Versions Notes

Abstract

:
A chemical bonding of several metallabenzenes and metallabenzynes was studied via an adaptive natural density partitioning (AdNDP) algorithm and the induced magnetic field analysis. A unique chemical bonding pattern was discovered where the M=C (M: Os, Re) double bond coexists with the delocalized 6c-2e π-bonding elements responsible for aromatic properties of the investigated complexes. In opposition to the previous description where 8 delocalized π-electrons were reported in metallabenzenes and metallabenzynes, we showed that only six delocalized π-electrons are present in those molecules. Thus, there is no deviation from Hückel’s aromaticity rule for metallabenzynes/metallabenzenes complexes. Based on the discovered bonding pattern, we propose two thermodynamically stable novel molecules that possess not only π-delocalization but also retain six σ-delocalized electrons, rendering them as doubly aromatic species. As a result, our investigation gives a new direction for the search for carbon-metal doubly aromatic molecules.

1. Introduction

Since the pioneering work of Thorn and Hoffmann investigating the delocalization in metallocycles [1], and a consequent isolation of osmebenzene by Roper et al. [2], a huge variety of metalla-aromatic structures have been discovered experimentally and studied computationally [3,4,5,6,7,8,9]. Those species can be described as usual aromatic compounds where one or several carbon atoms are replaced with a transition metal atom. Such a peculiar combination of a transition metal and a carbon-framework can produce a variety of interesting chemical bonding patterns. The study of metallocycles is important not only for the broad understanding of chemical bonding concepts and applicability of the aromaticity term but also as useful for synthetic organic chemistry [10,11,12,13].
One very important subgroup of metalla-aromatics is metallabenzenes (Figure 1a), metallacycle analogs to benzene. Chemists have managed to synthesize a huge variety of these complexes, incorporating various metals into the aromatic ring such as: osmium [14,15,16,17,18,19,20,21,22,23], rhenium [24,25,26], platinum [27,28,29,30], and iridium [31,32,33,34,35,36,37]. It was shown that metallabenzenes bear an appreciable aromatic character which is reflected in rather high aromatic stabilization energies [38,39,40,41] and negative nucleus-independent chemical shift values [42,43,44,45]. In the work of Thorn and Hoffmann, authors suggested that the metallabenzenes should have six π electrons, two of which come from the metal atom (dxz orbital), while the remaining 4 electrons come from the C5H5− fragment [1]. Martin et al. showed a cognate conclusion, noting a striking similarity between orbitals of benzene and metallabenzenes [44]. Interestingly, more recent studies do not share this point of view, introducing different numbers of delocalized π-electrons. Thus, Schleyer proposed that the dyz orbital is also participating in π-delocalization, and, thus, eight π-electrons are delocalized in the π-system [3]. This result contradicts with the Hückel [4n + 2] aromaticity rule; however, authors discussed that only two delocalized orbitals have the Hückel character, while another two orbitals (where the dyz orbital participates in delocalization) have the Möbius character [46] for which Hückel’s rule does not work. Later, Fernandez and Frenking proposed their interpretation of metallabenzenes aromaticity, showing the presence of ten π-electrons, where p-orbitals of in-plane ligands also participate in the π-delocalization [38,47]. All alternative interpretations were based on the analysis of canonical molecular orbitals (MOs) and studied the degree of stabilization that comes from the metal d-orbitals. In this work, we are trying to address this issue with the AdNDP localization technique that can explicitly show the degree of delocalization within the metallacycle.
Another quite intriguing subgroup of the metalla-aromatic compound is metallabenzynes (Figure 1b). Those complexes are of particular interest since they combine the double M=C bond and π-conjugated aromatic ring. Such a peculiar chemical bonding regime can help design new molecules with unprecedented physical and chemical properties.
In this study, we analyze the chemical bonding patterns of various model metallabenzene and metallabenzyne complexes (Figure 1c–e) which are analogues of experimentally synthesized complexes (Figure 1f–h) [14,48,49]. From the AdNDP analysis, only six π-electrons were found to participate in the delocalization in both metallabenzenes and metallabenzynes, agreeing with the Thorn and Hoffmann description. Based on the chemical bonding analysis of osmabenzyne and rhenabenzyne, two novel structures that possess doubly aromatic six-membered carbon-metal ring were designed.

2. Theoretical Methods

All structures were initially preoptimized using a PBE0 [50] DFT functional and LANL2DZ [51] basis set. Subsequent refinement of structural data was conducted using a large def2-TZVP [52] basis set. A chemical bonding analysis was performed using the AdNDP [53,54] algorithm as implemented in AdNDP 2.0 code. The AdNDP method can represent a chemical bonding pattern in terms of both Lewis bonding elements (lone pairs (1c–2e) and 2c–2e bonds) as well as delocalized bonding elements (such as nc-2e (n  >  2) bonds), allowing one to describe highly delocalized electrons associated with the concept of aromaticity. This technique is widely used in describing chemical bonding patterns of various metal-containing clusters [55,56,57,58,59,60], aromatic 2D-materials [61,62,63], and doubly aromatic metal systems [64,65]. All AdNDP calculations were performed at the PBE0/def2-TZVP level of theory. It was shown before that the PBE0 functional could overestimate electron delocalization and aromaticity in planar aromatic systems [66]. To avoid this problem, we reoptimized geometries and performed the AdNDP analysis using the CAM-B3LYP functional [67] that does not suffer from a delocalization error. We note that the obtained AdNDP results reproduce results obtained with the PBE0 functional showing that the found chemical bonding pattern is DFT-functionally independent. The frequency calculations were performed using the harmonic approximation, and all reported structures were confirmed to be minimal due to the absence of imaginary frequencies. To assess the aromaticity with a quantitative parameter, NICS [68] calculations were performed at the PBE0/def2-TZVP level. The ChemCraft 1.8 software was used to visualize chemical bonding patterns and geometries of investigated compounds. The Gaussian 16 software was used for all quantum chemical calculations described above [69].
The nucleus-independent shielding tensors (σij) [70,71,72] were calculated within the GIAO formalism by using the ADF2019 code [73], employing the hybrid PBE0 [50] functional and an all-electron STO-TZ2P basis set, placed in a three-dimensional grid in order to evaluate the induced field (Bind), upon an external magnetic field (Bext), related via Biind  =  −σijBjext [74,75,76]. For convenience, the i and j suffixes are related to the x-, y-, and z-axes of the molecule-fixed Cartesian system (i, j  =  x, y, z). The values of Bind are given in ppm in relation to Bext. Relativistic effects were considered through the ZORA Hamiltonian [77].

3. Results and Discussion

3.1. Hückel’s [4n+2] π-Aromaticity of Metallabenzenes and Metallabenzynes

To model the synthesized rhenium and osmium complexes (Figure 1f–h), we replaced bulky Ph3P- and PhMe2P- groups with a PH3- ligand, while we preserve all atoms in the aromatic rings as they are in the experimental structure. Such a substitution does not affect chemical bonding in the metallocycle itself and will reflect the delocalization pattern properly. The optimized geometries reproduce the M-C (M: Os, Re) and C-C distances within the aromatic ring with a good precision (bond lengths’ deviations from the experimental data are within the 0.1–0.01 Å range). The alternation of C-C inside the ring is not large, and all bonds have the same length within the ~0.03 Å for Os structures and ~0.05 Å for the Rhenium complex. To ensure that the constructed single-determinant singlet wavefunction can be applied in those cases, we checked the stability of the wave function (WF) showing the absence of any RKS to UKS instabilities. We also performed the optimization of the complexes in the triplet open-shell configuration and found the triplet states are appreciably higher in energy than the singlet states. Those facts show that the DFT approximation is valid in this case, and the singlet single-determinant WF could be used to describe the systems considered. For the sake of simplicity, we introduce the following notation for the investigated complexes: [Os(CO)I(PH3)2(C5H5)]-[Os]C5H5, [OsCl2(PH3)2(C5H4)]-[Os]C5H4, and [ReCl(PH3)3(C5H4)]-[Re]C5H4.
To analyze the chemical bonding in the investigated species, we performed an AdNDP analysis as implemented in AdNDP 2.0 code. We start our discussion with the chemical bonding of the osmabenzene. The [Os]C5H5 complex has 66 valence electrons that could be localized into 33 two-electron bonding elements. Following the idea of AdNDP analysis, the localization starts from the one-center two-electron (1c-2e) elements, or lone pairs. We found two s-type lone pairs on oxygen and iodine atoms with occupation numbers (ON) 2.00–1.98 |e|, two p-type lone pairs on iodine with ON = 1.99–1.93 |e|, and two d-type lone pairs (dyz and dx2-y2) on the Os-atom with ON = 1.78–1.75 |e| (Figure 2a). A consequent localization of 2c-2e bonding elements leads to a σ-bonding framework with sixteen C-O, C-C, C-H, and P-H 2c-2e bonds with ON = 2.00–1.97 |e|. The Osmium atom has a quasi-octahedral environment, and six Os-C, Os-P, and Os-I 2c-2e σ-bonds with ON = 1.98–1.93 |e| can be localized. Predictably, two 2c-2e π-bonds were found in the -C≡O ligand rendering the C-O bond as a triple bond. The remaining six valence electrons form π-delocalized 6c-2e bonds, resembling benzene 6c-2e delocalization (Figure 2a). The shape of those bonds and the number of electrons (in agreement with the Hückel’s [4n+2] rule) render this complex as π-aromatic. The complete bonding pattern of [Os]C5H5 can be found in the Supporting Information file (Figure S1), while the most significant bonding elements are shown in Figure 2a.
We want to note that this picture contradicts with some recent descriptions of metallabenzenes, where eight [3] and ten [38,47] π-electrons were meant to be delocalized in the metallocycle. It was discussed that not only the dxz orbital of the Os-atom participates in the formation of π-conjugation, but also the dyz orbital overlaps with the π-electrons of the carbon framework. However, this conclusion was made based on the canonical molecular orbital (MO) picture, which is delocalized in its nature. We believe that the picture obtained by the AdNDP is more chemically intuitive and more descriptive since it is based on the matrix representation of the first-order reduced density operator. We can definitely localize the dyz lone pair on the Os-atom which does not participate in delocalization in any significant manner, although it is formally of the same symmetry as some orbitals in the π-conjugated system. To show that, we localized this lone pair as a 6c-2e π-bond. The increase in ON was only 0.1 |e| showing a tiny degree of the delocalization of the dyz lone pair over the metallabenzene ring. Thus, we believe that the initial description proposed by Thorn and Hofmann is correct, and there is no deviation from Hückel’s aromaticity rule for metallabenzynes/metallabenzenes complexes.
A cognate chemical bonding was found for the [Os]C5H4 complex (Figure S2). The main difference in chemical bonding is the presence of a 2c-2e Os-C in-plane π-bond (Figure 2b), which is also reflected in the significant shortening of Os=C distance with respect to the Os-C single-bond (~0.27 Å difference). A similar chemical bonding pattern was found for rhenabenzyne (Figure S3). It is a very intriguing result, since, to the best of our knowledge, the coexistence of the in-plane π-bond with the π-aromatic system has never been described before in the realms of the AdNDP localization technique. The possibility of such a reconciliation opens up an opportunity to design quite unique structures with doubly aromatic metal-carbon rings that will be described in the next subsection.

3.2. Hückel’s [4n+2] σ- and π- Double Aromaticity of Novel Carbon-Metal Structures

The possibility to use the in-plane p-orbital of carbon and dx2-y2-orbital of the transition metal without the introduction of a huge strain (in comparison to the case of the planar benzyne C6H4 ring, where a highly strained C≡C bond is present) allows proposing possible metal-carbon structures that will employ delocalization not only in the π-fashion but also in the σ-regime. As illustrated in Figure 3, the combination of three carbon atoms and three transition metal atoms could potentially produce a stable doubly aromatic six-membered ring.
To test this hypothesis, we employed the [M] motifs ([M]: [OsCl2(PH3)2], [ReCl(PH3)3]) that were used in the first part of this work and combined them with three carbon atoms to form a six-membered ring. As a result, [{OsCl2(PH3)2}3C3] ([Os]3C3) and [{ReCl(PH3)3}3C3] ([Re]3C3) stoichiometries were obtained. The optimized structures are found to be a local minimum without possessing any imaginary frequencies. The WF was checked to be stable, and similar triplet species are significantly higher in energy than the singlet ones. The geometries of the proposed species are shown in Figure 4. Remarkably, both structures contain the M3C3 six-membered planar ring.
The AdNDP analysis reveals the cognate chemical bonding pattern as was found in metallabenzynes. The localized lone pairs and σ-bonding framework coincide (Figures S4 and S5). However, the remaining 12 electrons form three delocalized 6c-2e σ- and π-bonding elements (Figure 5). The shape of those elements agrees with the proposed model bonding depicted in Figure 3. We note that the occupation numbers of π-aromatic bonds are rather low (1.68–1.55 |e| for [Os]3C3 and 1.79–1.74 |e| for [Re]3C3); however, the occupancies could be increased up to 2.00–1.98 |e| values by including phosphorous atoms in the localization scheme (resulting in 12c-2e bonds). Thus, 6c-2e π-bonds show some delocalization character over -PH3 ligands. Previously, the presence of double aromaticity in metal systems was discussed for M42− molecules composed out of Al, Ga, and In atoms [64,65]. Moreover, recently, Saito and coworkers synthesized a molecule ([C6(SePh)6][SbF6]2) in an isolated form that possesses a double aromaticity arising from σ- and π-rings [78].
To assess the aromaticity of metallo-organic rings with a quantitative parameter, we calculated NICSzz(0) and NICSzz(1) indices (Table 1) at the center of the aromatic rings. The exact coordinates of the special points for each cluster can be found in the Supporting Information file (Table S2). The significantly low values of NICSzz(0) and NICSzz(1) indices inside of aromatic rings and the increasing of the NICSzz(0) values for [M]3C3 species are in agreement with the overall description of double aromaticity in the proposed structures and π-aromaticity of the metallabenzenes and metallabenzynes species.
We note that the difference in the trends for NICSzz(0) and NICSzz(1) for [M]C5H4 and [M]3C3 is due to the different types of aromaticity that are present in those systems. Since [M]C5H4 is a π-aromatic system, we observe that NICSzz(0) values are less negative than NICSzz(1) values (a similar trend can be found in π-aromatic benzene). In turn, [M]3C3 systems are doubly aromatic and possess σ-aromaticity in addition to π-aromaticity. For σ-aromatic systems, it was found before that NICSzz(0) is more negative than NICSzz(1) [79,80]. Thus, due to the presence of σ-aromaticity, [M]3C3 systems possess largely negative NICSzz(0). Such a trend could be vividly visualized using NICSzz-Scan plots (Figure S6). Slightly less negative values of NICSzz(1) of [M]3C3 in comparison with [M]C5H4 are due to the delocalization of π-electrons to the -PH3 ligands, which is also reflected in the ONs of π-delocalized bonds obtained from the AdNDP analysis.
To access the spatial distribution of the magnetic shielding parameters, the isosurface representation of the induced magnetic field (Bind) was calculated. It accounts for the characteristic patterns of the magnetic response at the molecular surroundings of the complexes, revealing the inherent characteristics given by the above discussed bonding pattern related to the Hückel’s [4n + 2] aromaticity on the studied metallobenzynes and metallabenzenes complexes. The isotropic term is related to the orientational averaged response owing to the molecular tumbling in solution, which is related to NICS given as an isosurface along the overall structure denoted as Iso (Figure 6), which shows a larger contribution from the M-C, M-Cl, and M-P bond (M=Os, Re). In addition, for [Os]C5H4 and [Re]C5H4, a shielding surface at the six membered MC5H4 ring indicates its aromatic character. In agreement to NICSzz(0) and NICSzz(1) values (Table 1), the related Bzind isosurface exhibits an enhanced shielding response with a complementary deshielding region along the ring backbone, denoting the shielding cone property from aromatic rings. The contour plot for Bzind supports this behavior, showing a shielding value of ~ −10 ppm nearby the center of the ring increasing along the z-axis, which is enhanced towards the C-C and C-M bonds (>−20 ppm).
For [Os]3C3 and [Re]3C3 rings, the NICSzz(0) values (Table 1) show an enhanced shielding denoting their double aromatic characteristics. Similarly, the isosurface and contour plot representation of Iso and Bzind denotes an enhanced shielding response at the center of the M3C3 ring, in comparison to the MC5H4 case, which is decreased along the z-axis as previously depicted by NICSzz(1). Moreover, nearby the M center, a deshielding contribution is found, suggesting that besides the double aromatic character of the M3C3 ring, the NICSzz values are also affected by the contribution from the metal center, leading to a decrease in the shielding behavior nearby the center of the [Os]3C3 and [Re]3C3 rings, as shown from the side-view contour plot of Bzind from Figure 6, but clarified by the top-view from Figure 7. It is important to note that such an observation is exclusive for metal-containing rings in contrast to hydrocarbons or other light element structures because of the contribution from core electrons [81].
Furthermore, the contribution from the metal center to the NICSzz and its related isosurface (Bzind) terms is explored in terms of diamagnetic (diaBzind), paramagnetic (paraBzind), and spin–orbit (SOBzind) contributions within the two components’ ZORA/GIAO formalism [82].
Bzind = diaBzind + paraBzind + SOBzind
The diamagnetic contribution involves an unperturbed electron density and is largely affected by the number of core electrons, thus increasing according to the atomic number (Z) of the involved metal centers [82]. The paramagnetic term (paraBzind) involves the mixing of ground and excited states upon the external magnetic field, and is mainly affected by the frontier orbital structure, and thus accounting for the classical electron counting consideration, such as Hückel’s rule. Lastly, the spatial contribution from the spin-orbit coupling is accounted by the SOBzind term [83].
From Figure 7, the strong shielding behavior at the center of the Os3C3 ring is contributed from the paramagnetic term, i.e., accounting for the favorable double aromatic character, as depicted by the bonding pattern fulfilling both in-plane and out-of-plane Hückel circuits. Interestingly, the diamagnetic contribution shows a large deshielding contribution originated at each M center, with a small SOBzind contribution. Hence, the contribution from core electrons from M decreases the long range characteristics of the shielding cone property [84] of the Os3C3 ring. Similar results were obtained for [Re]3C3 (Figure S7).

4. Conclusions

In this research we showed that metallobenzynes and metallabenzenes complexes possess Hückel’s [4n + 2] classical π-aromatic conjugated system. We showed that the previous assignment of eight and ten delocalized π-electrons does not agree with the AdNDP localization picture, and the dyz lone pair of a transition metal has an appreciable occupation number and cannot be considered as a delocalized 6c-2e bond. By analyzing chemical bonding of metallabenzynes, we firstly described an in-plane π-bond coexisting with π-aromaticity in realms on the AdNDP analysis. It allowed us to construct two novel molecules ([Os]3C3 and [Re]3C3) with doubly aromatic six-membered ring, denoting the contribution from the metal core electrons to the magnetic characteristics of the overall structure. We believe these findings will help in the development and understanding of chemical bonding in metallocycles and open a possibility to discover a novel class of doubly aromatic carbon-metal species.

Supplementary Materials

Figure S1: Chemical bonding pattern of [Os]C5H5, Figure S2: Chemical bonding pattern of [Os]C5H4, Figure S3: Chemical bonding pattern of [Re]C5H4, Figure S4: Chemical bonding pattern of [Os]3C3, Figure S5: Chemical bonding pattern of [Re]3C3, Figure S6: The NICSzz values calculated at different distances from the ring center, Figure S7: The induced magnetic field for investigated complexes, Table S1: Optimized structures of investigated complexes, Table S2: Coordinates of chosen points for NICS calculation.

Author Contributions

Conceptualization, N.V.T., A.M.-C. and A.I.B.; methodology, N.V.T., A.M.-C. and A.I.B.; writing—original draft preparation, N.V.T., A.M.-C. and A.I.B.; writing—review and editing, N.V.T., A.M.-C. and A.I.B.; visualization, N.V.T., A.M.-C. and A.I.B.; supervision, A.I.B.; All authors have read and agreed to the published version of the manuscript.

Funding

The research was funded by the R. Gaurth Hansen Professorship fund to A.I.B.; A.M.-C. acknowledges financial support from the FONDECYT/ANID grant 1180683.

Institutional Review Board Statement

Not applicable.

Informed Consent Statement

Not applicable.

Data Availability Statement

The data that support the findings of this study are available from the corresponding authors on a reasonable request.

Acknowledgments

The support and resources from the Centre for High Performance Computing at the University of Utah are gratefully acknowledged.

Conflicts of Interest

The authors declare no conflict of interest.

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Molecules 26 07232 g001 550
Figure 1. Structures of metallabenzenes and metallabenzynes. Structures (a) and (b) are general structures of metallabenzenes and metallabenzynes, respectively. Structures (c–e) are considered in this study and are model structures for previously synthesized complexes (f–h).
Figure 1. Structures of metallabenzenes and metallabenzynes. Structures (a) and (b) are general structures of metallabenzenes and metallabenzynes, respectively. Structures (c–e) are considered in this study and are model structures for previously synthesized complexes (f–h).
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Molecules 26 07232 g002 550
Figure 2. Results of the AdNDP analysis for [Os(CO)I(PH3)2(C5H5)] (a) and [OsCl2(PH3)2(C5H4)] (b). Only selected bonding elements are shown.
Figure 2. Results of the AdNDP analysis for [Os(CO)I(PH3)2(C5H5)] (a) and [OsCl2(PH3)2(C5H4)] (b). Only selected bonding elements are shown.
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Molecules 26 07232 g003 550
Figure 3. Proposed structure of doubly aromatic metal-carbon ring and orbitals’ representation of conjugated π- and σ- electrons.
Figure 3. Proposed structure of doubly aromatic metal-carbon ring and orbitals’ representation of conjugated π- and σ- electrons.
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Molecules 26 07232 g004 550
Figure 4. Optimized structures of proposed doubly aromatic complexes: [Os]3C3 (a) and [Re]3C3 (b).
Figure 4. Optimized structures of proposed doubly aromatic complexes: [Os]3C3 (a) and [Re]3C3 (b).
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Molecules 26 07232 g005 550
Figure 5. Results of the AdNDP analysis for [Os]3C3. Only σ- and π- delocalized bonding elements are shown. The cognate pattern was found for [Re]3C3.
Figure 5. Results of the AdNDP analysis for [Os]3C3. Only σ- and π- delocalized bonding elements are shown. The cognate pattern was found for [Re]3C3.
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Molecules 26 07232 g006 550
Figure 6. The induced magnetic field for [Os]C5H4, [Re]C5H4, [Os]3C3, and [Re]3C3, given as isosurface (±5 ppm, Blue: Shielding; Red: Deshielding) and contour plot (Side-view; Negative values: Shielding; positive: Deshielding).
Figure 6. The induced magnetic field for [Os]C5H4, [Re]C5H4, [Os]3C3, and [Re]3C3, given as isosurface (±5 ppm, Blue: Shielding; Red: Deshielding) and contour plot (Side-view; Negative values: Shielding; positive: Deshielding).
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Molecules 26 07232 g007 550
Figure 7. The induced magnetic field for [Os]3C3, given as contour plot and its contribution from diamagnetic (diaBzind), paramagnetic (paraBzind), and spin–orbit (SOBzind) terms.
Figure 7. The induced magnetic field for [Os]3C3, given as contour plot and its contribution from diamagnetic (diaBzind), paramagnetic (paraBzind), and spin–orbit (SOBzind) terms.
Molecules 26 07232 g007
Table
Table 1. NICSzz(0) and NICSzz(1) indices calculated for complexes investigated in this work.
Table 1. NICSzz(0) and NICSzz(1) indices calculated for complexes investigated in this work.
ComplexNICSzz(0)NICSzz(1)
[Os]C5H4−9.2−15.0
[Re]C5H4−9.9−14.2
[Os]3C3−23.5−2.8
[Re]3C3−29.5−6.3
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Tkachenko, N.V.; Muñoz-Castro, A.; Boldyrev, A.I. Occurrence of Double Bond in π-Aromatic Rings: An Easy Way to Design Doubly Aromatic Carbon-Metal Structures. Molecules 2021, 26, 7232. https://doi.org/10.3390/molecules26237232

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Tkachenko NV, Muñoz-Castro A, Boldyrev AI. Occurrence of Double Bond in π-Aromatic Rings: An Easy Way to Design Doubly Aromatic Carbon-Metal Structures. Molecules. 2021; 26(23):7232. https://doi.org/10.3390/molecules26237232

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Tkachenko, Nikolay V., Alvaro Muñoz-Castro, and Alexander I. Boldyrev. 2021. "Occurrence of Double Bond in π-Aromatic Rings: An Easy Way to Design Doubly Aromatic Carbon-Metal Structures" Molecules 26, no. 23: 7232. https://doi.org/10.3390/molecules26237232

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